CA2208576A1 - Semiconductor gamma-ray camera and medical imaging system - Google Patents

Semiconductor gamma-ray camera and medical imaging system

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Publication number
CA2208576A1
CA2208576A1 CA002208576A CA2208576A CA2208576A1 CA 2208576 A1 CA2208576 A1 CA 2208576A1 CA 002208576 A CA002208576 A CA 002208576A CA 2208576 A CA2208576 A CA 2208576A CA 2208576 A1 CA2208576 A1 CA 2208576A1
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CA
Canada
Prior art keywords
detection
imaging system
event
channel
coupled
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Abandoned
Application number
CA002208576A
Other languages
French (fr)
Inventor
Clinton L. Lingren
Stanley J. Friesenhahn
Jack F. Butler
F. Patrick Doty
William L. Ashburn
Richard L. Conwell
Frank L. Augustine
Boris Apotovsky
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Digirad Corp
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Individual
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Application filed by Individual filed Critical Individual
Publication of CA2208576A1 publication Critical patent/CA2208576A1/en
Abandoned legal-status Critical Current

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Classifications

    • GPHYSICS
    • G01MEASURING; TESTING
    • G01TMEASUREMENT OF NUCLEAR OR X-RADIATION
    • G01T1/00Measuring X-radiation, gamma radiation, corpuscular radiation, or cosmic radiation
    • G01T1/16Measuring radiation intensity
    • G01T1/161Applications in the field of nuclear medicine, e.g. in vivo counting
    • AHUMAN NECESSITIES
    • A61MEDICAL OR VETERINARY SCIENCE; HYGIENE
    • A61BDIAGNOSIS; SURGERY; IDENTIFICATION
    • A61B6/00Apparatus for radiation diagnosis, e.g. combined with radiation therapy equipment
    • A61B6/42Apparatus for radiation diagnosis, e.g. combined with radiation therapy equipment with arrangements for detecting radiation specially adapted for radiation diagnosis
    • A61B6/4208Apparatus for radiation diagnosis, e.g. combined with radiation therapy equipment with arrangements for detecting radiation specially adapted for radiation diagnosis characterised by using a particular type of detector
    • A61B6/4258Apparatus for radiation diagnosis, e.g. combined with radiation therapy equipment with arrangements for detecting radiation specially adapted for radiation diagnosis characterised by using a particular type of detector for detecting non x-ray radiation, e.g. gamma radiation
    • GPHYSICS
    • G01MEASURING; TESTING
    • G01TMEASUREMENT OF NUCLEAR OR X-RADIATION
    • G01T1/00Measuring X-radiation, gamma radiation, corpuscular radiation, or cosmic radiation
    • G01T1/16Measuring radiation intensity
    • G01T1/161Applications in the field of nuclear medicine, e.g. in vivo counting
    • G01T1/164Scintigraphy
    • G01T1/1641Static instruments for imaging the distribution of radioactivity in one or two dimensions using one or several scintillating elements; Radio-isotope cameras
    • G01T1/1642Static instruments for imaging the distribution of radioactivity in one or two dimensions using one or several scintillating elements; Radio-isotope cameras using a scintillation crystal and position sensing photodetector arrays, e.g. ANGER cameras
    • GPHYSICS
    • G01MEASURING; TESTING
    • G01TMEASUREMENT OF NUCLEAR OR X-RADIATION
    • G01T1/00Measuring X-radiation, gamma radiation, corpuscular radiation, or cosmic radiation
    • G01T1/16Measuring radiation intensity
    • G01T1/24Measuring radiation intensity with semiconductor detectors
    • G01T1/243Modular detectors, e.g. arrays formed from self contained units
    • GPHYSICS
    • G01MEASURING; TESTING
    • G01TMEASUREMENT OF NUCLEAR OR X-RADIATION
    • G01T1/00Measuring X-radiation, gamma radiation, corpuscular radiation, or cosmic radiation
    • G01T1/16Measuring radiation intensity
    • G01T1/24Measuring radiation intensity with semiconductor detectors
    • G01T1/247Detector read-out circuitry
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01LSEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
    • H01L27/00Devices consisting of a plurality of semiconductor or other solid-state components formed in or on a common substrate
    • H01L27/14Devices consisting of a plurality of semiconductor or other solid-state components formed in or on a common substrate including semiconductor components sensitive to infrared radiation, light, electromagnetic radiation of shorter wavelength or corpuscular radiation and specially adapted either for the conversion of the energy of such radiation into electrical energy or for the control of electrical energy by such radiation
    • H01L27/144Devices controlled by radiation
    • H01L27/146Imager structures
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01LSEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
    • H01L27/00Devices consisting of a plurality of semiconductor or other solid-state components formed in or on a common substrate
    • H01L27/14Devices consisting of a plurality of semiconductor or other solid-state components formed in or on a common substrate including semiconductor components sensitive to infrared radiation, light, electromagnetic radiation of shorter wavelength or corpuscular radiation and specially adapted either for the conversion of the energy of such radiation into electrical energy or for the control of electrical energy by such radiation
    • H01L27/144Devices controlled by radiation
    • H01L27/146Imager structures
    • H01L27/14643Photodiode arrays; MOS imagers
    • H01L27/14658X-ray, gamma-ray or corpuscular radiation imagers
    • HELECTRICITY
    • H04ELECTRIC COMMUNICATION TECHNIQUE
    • H04NPICTORIAL COMMUNICATION, e.g. TELEVISION
    • H04N23/00Cameras or camera modules comprising electronic image sensors; Control thereof
    • H04N23/30Cameras or camera modules comprising electronic image sensors; Control thereof for generating image signals from X-rays
    • AHUMAN NECESSITIES
    • A61MEDICAL OR VETERINARY SCIENCE; HYGIENE
    • A61BDIAGNOSIS; SURGERY; IDENTIFICATION
    • A61B6/00Apparatus for radiation diagnosis, e.g. combined with radiation therapy equipment
    • A61B6/02Devices for diagnosis sequentially in different planes; Stereoscopic radiation diagnosis
    • A61B6/03Computerised tomographs
    • A61B6/037Emission tomography
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01LSEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
    • H01L27/00Devices consisting of a plurality of semiconductor or other solid-state components formed in or on a common substrate
    • H01L27/14Devices consisting of a plurality of semiconductor or other solid-state components formed in or on a common substrate including semiconductor components sensitive to infrared radiation, light, electromagnetic radiation of shorter wavelength or corpuscular radiation and specially adapted either for the conversion of the energy of such radiation into electrical energy or for the control of electrical energy by such radiation
    • H01L27/144Devices controlled by radiation
    • H01L27/146Imager structures
    • H01L27/14665Imagers using a photoconductor layer
    • H01L27/14676X-ray, gamma-ray or corpuscular radiation imagers
    • HELECTRICITY
    • H04ELECTRIC COMMUNICATION TECHNIQUE
    • H04NPICTORIAL COMMUNICATION, e.g. TELEVISION
    • H04N5/00Details of television systems
    • H04N5/30Transforming light or analogous information into electric information
    • H04N5/32Transforming X-rays

Abstract

An imaging system including an imaging head, a signal processor, a data acquisition system, and an image processing computer is disclosed. The imaging head includes a detector and an aperture for directing the radiation to the detector. The detector comprises a plurality of closely-packed detection modules (206) comprising a plurality of detection elements (212) mounted to a circuit carrier (214) which includes channels for conditioning and preprocessing the electrical pulses produced when a detection element absorbs radiation. The amplitude of the pulse is indicative of the magnitude of the radiation absorbed. The detection modules employ a fall-through circuit to automatically find valid events, i.e., only those detection elements having a stored amplitude exceeding a predetermined threshold.

Description

SE~CONDUCTOR GAMMA-RAY CAMERA
AND MEDICAL IMAGlNG SYSTEM

BACKGROUND OF T~ INVENl~ON

1. Field of the Invennon 5 This invention relates to the general field of radiation ;, n~ with ~mph~is on medical applie~hon~ in radiology and esper;.~lly in nuclear me~i~in~o. In parhcular the invention provides an improved ~alalus and method for detecting radiation and constructing an image colrl ~onding to the spatial distribution of its source for nuclear medicine and other applic~hon~

10 2. Description of Related Art Medical ~ anos~ic im~eine began with the discovery of x rays by W. C. Roentgen in 1895 and today includes radiography, nuclear medicine im~g,ina, ulLlasOulld im~aine, co~uled tomographic im~ein~, and magnetic reson~ce im~gine. In general the goal of each type of me~ic~l im~ine is to provide a spatial mapping of a parameter, feature, 15 or process within a patient.

ID radiology and co~ uLed tomography, a source of x rays is beamed through the patient onto a suitable detector such as a film or a plate. The detector measures the ill~c.~iLy distribution of the inrid~nt beam of x rays and provides an image 1~ ples~ ..t;l-a the ;on of the radiation resulting from the absorption and sc~ e within the 20 patient's body.

Nuclear me~iicine involves injection of a radiopk~ JI;cal into a patient and me~u~ ,llc,lt of the intellsiLy distribution of gamrna radiation e_itted from t~h-e patient's W O96/20412 PCTrUS9~116911 body. Radioph~ c~ ~l;c~ls are formed by ~ll;.r ~ g a r~ oactive tracer to a ph~ r~,.
tical that is known to ~.ef~ ~ially ~rcllm~ te in the organ of interest. Thus, the radiation pattern is a measure of blood fiow, metabolism, or recc~lor density within the organ of interest and provides ~., . ,~3t;on about the fimrtion of the organ. Either a single S projection image of the radiation pattern may be taken (planar im~inp) or many projection images may be acquired from different directions and used to coml ~Le the three ~im~n~ional emission distribunon (single photon emission co~ cd tomography, or SPECT). Radiation-im~ginP systerns used in nuclear m~icine are often referred to as "gamma" carneras.

Pioneer nuclear medicine im~ainP systems used sC~nnin~a~ methods to generate images.
Such pioneer systems generally used a srint~ tion-type gamma-ray detector equipped with a focusing collimator which moved continuously in selçcted coor lil~ate directions, i.e., in a series of parallel sweeps, to scan regions of interest. A disadvantage of these early im~ginP systems was the lengthy exposure t~nes that were required to derive an irnage of the system or organ under test. In ~jnon, dynamic studies of such organs were often dif Eicult to obtain.

Another type of prior art r~ tion ~etrction system utilizes an "Anger" type gamma scintillation camera (narned after its inventor H.O. Anger, see "A ~ew Ins~ument for Mapping ('T~mm~ Ray Ernitters," Biology and Medicine Quarterly Report, U.C.R.L.-3653, 1957), for ~te. ".i~;n,, the r~ tion pattem emitted from a patient's body. These nuclear medicine imagers use large sodium iodide scinhll~tin,a, crystals in conjunction with a banlc of photomnltlrlier tubes (PMTs). A collim~tinP a~c~Lule in front ofthe scin-tillation crystal focuses the garnrna rays on the crystal, and g~mma rays ~om a radio~h~ reutical injected into the patient produce light flashes (scintillations) in the crystal which are converted into electrical signals by the PMTs. High density shielding material, typically lead, is used to cover the sides and back of the radiation detection assembly to prevent radiation from ent~ring the detector by any path other than through W O96/20412 PCTrUS95/16911 t_e collim~tor. A co~l,ul", locates each flash from the relative m~ des of the PMT
signals. Crystals are typically 200 to 400 s~uare i~ches in area T imit~tions in the Anger camera stem from the process of converting srintill~tions into electri~l signals. Sources of distortion in~lu~le: l) variation ofthe acce~ ce field-of-5 view angle ofthe PM tubes with ~ict~nre from the scintill~tion event, 2) refraction andlight guiding due to index of refi~r,tion micm~trhrs, 3) unavoidable dead regions between PMTs, 4) higher effective density (hence, heavier weighting) of distant PMTs, 5) non-ullifollll spatial ~ ,ollse of individual PMTs, 6) variation in le~l,ollse from one PMT to another, 7) te~pol~l variation of PMT response, and 8) an unavoidable dead margin 10 several c~Li~cters wide around the perimeter related to the inability of ~ ",lin;l.g positions outside the rniddle of the outer PMTs. Other errors stem from instabilities in the PMTs and the fragility and hy~uscopic nature of the srintill~tiQn crystal.

Disadvantageously, because of the large size of the detection assembly that results from the combination of srintill~tor, light pipe, and photomnltirlier tubes, the lead shielding 15 dramatically increases the weight and cost of Anger c~me~ Furthermore, the non-sensitive (dead) margin around the p. . ;- - ~t?tF I of the Anger camera makes it difficult to adequately image small organs and some body parts (the breast, for example). In addition, the large size of the Anger ca_era and its weight prevent it from being used effectively in locations such as in o~ g rooms, intensive care units, or at the patient's 20 bedside.

Inherent to the Anger camera design, the scin~ tor detection element is formed in a plane. There could be sigIlificant advantage for some applications of formina the detection elements in a shape that conforms more closely to that of an object to be imaged.

PCTrUS95/16911 Sernicon~lurtor detector-array i~age~ have been proposed for solving problems with Anger c~rne~c e.g., see U.S. Patent No. 4,292,645; U.S. Patent No. 5,132,542; EEE
Tr~n~açtionc onNuclear Science, Vol. NS-27, No. 3, June 1980, "Semicon~ ctor Gamma C~m~ in Nuclear Medicine;" and EEE Tr~ne~rtion~ on Nuclear Science, Vol. NS-25, S No. 1, Feb 1978, "Two-Detector, SI2-F.I~m~ nt Hig~ Purit,v C.,~dl~i~ Camera Proto-type." It has long been recognized that semicon~ rtor detector arrays are potentially attractive for nuclear medicine im~ing because of their very small size and weight, excellent spatial resolution, direct conversion of gamma photons into electrical signals, capability of on-board signal procPs~ing~ high stability, and reliability. Using this 10 technique, gamma-ray rarii~tion absorbed in a semicon~ o~ detector produces holes and electrons within the detector m~t~on~l which, due to the influence of a bias voltage, se~ and move toward opposite surfaces ofthe slomicondllctQr m~t~ri~l in accordance with their L~ e~ e electrical charge polarities. The electron and hole ~ LL~ are then ~mplified and conditioned by electronic CLL''~iLI~ to produce electrical signals which are 15 plocessed to in~icate the location and iLLtl .~iLy ofthe corresponding inci(lent ga~na-ray radiation.

Plololy~e semiconductor detector-array cameras embodying these princirles have been developed with varying degrees of s~ccess. For example, alL~ L~ at using two-~im~oncional detector arrays of cryogenically-cooled-germanium ~etectQrs and room-20 t~ f ~ e HgI2 detectr,rs have generally been lirnited to the sci~ntific laboldtul ~ due tothè problems associated with cryogenic cooling and practical difficulties with HgI~
technology. An early feasibility study of an im~ging system based on a rotating linear array of cadmium telluride (CdTe) ~ietectors has similarly not proven to be a satisfactory solution and has a~aLe~lly been ab~n~one~l 25 One exarnple of a prior art serniconductor garnma camera is described in U.S. Pat. No.
4,292,645, to S~lossP~, et al. Schlosser teaches an improved technique for providing the n~cess~ry electrical contact to doped regions of a semiconductor garnrna detector PCTnUS9S/16911 S

principally compnced of geTTn~nil~m A layer of resistive m~tf~1 makes contact with conductive strips on the detector s~lrfarç, and two readout contacts at the sides of the resistive layer, parallel to the strips and co.~.-f~ d to two ampLifiersl allow identification of the strip where a gamma ray is absorbed. The o~osi~ side of the ~f tf ctor is arranged 5 the same except that the strips are orthogonal to those on the top. The spatial position of an event is the ;l~tf..se~l ;on ofthe iderltified orthogonal strips. Two arnplifiers for the top surface and two amplifiers for the bottom surface handle all events in the entire imager.
Though this keeps the electronic colllpollent count small, it is a disadvantage to use the entire crystal for detectiorl of each gamma ray. As a result of this, the resolution gets 10 worse and the achievable count rate decreases as the size of the detector is increased.

Another example of a prior-art gamma-ray-im~gina system using a semiconductor ~t~Pctor array is described in ~ri~lc Research Society Syrnposil~m Procee~ling~, Vol.
302 (hl~tPri~c Research Society, Pi~ LLgll, 1993), pp. 43-54, "Multi-~ement MercuTy Iodide Detector Systems for X-Ray and (~mm~-Ray Tm~ging," by Bradley E. Patt. Patt 15 teaches the use of orthogonal strips on opposite sides of the sernicon~ tor crystal to define the serniconductor detector array pixels, with one amplifier being used for each strip. The coincidton.~e of signals from orthogonal strips is used to define the position at which a gamma ray is absorbed within the crystal. Disadvantageously, as the area of the detector gets larger and the length of the strips iacL~ases, the c~p~cit~n~e associated with 20 the strip and the leakage current in the strip from the ~letect~r ~ClC;dSe. Both c~p~it~n~e and leakage current reduce the pulse energy resolution which degrades the imagerp~r~

The prior art lacks a semicon~-lctor detector array that is large enough to satisfy nuclear medicine applications or that op~ .dLes at room te~ c~dL-ILe. Therefore, there is a need for 25 a detector which overcomes the disadvantages of the Anger camera, has an active area ap~loyl;ate for medical im~gin~ application, has negligible dead region around the WO 96t20412 PCT/US95/16911 p. . ;~ r, and Op~dl~ ~ at room te.ll~ ~e. There is a need for a cost-effective mean~
of m~nl~f~chlring such de~ u~ for nuclear mP~icine and other applic~tion~

A sPmi~on~ ctor detector array may be realized by combining together many individual detector ~l~nPnt~ However, when the individual detPctor cle,~ are made sllfficiPntly S small to meet spatial resolution l~lUil CllL-.llL ~, the number of amplifiers needed to amplify the signals becoLucs very large. For infrared and lo~v-eL.. .~y x-ray applications, prior art focal-plane arrays and silicon-strip detectors combine amplifiers for each element and a multiplexer that provides a single output for the large nurnber of inputs (see Nuclear InsLlul~t~t~ and Methods in Physics Research, Vol. 226, 1984, pp. 200-203; and EEE
transactions on Nuclear Science, Vol. NS-32, No. 1, February 1985, p 417). These prior art readout circuits are not adequate for h~n~llinE signals produced by gamma-ray d~ ol~ such as CZT detector arrays required for nuclear merlicine im~ging In addition, because of variations in response between individuaI detector elements and bet~veen individual amplifiers, a need exists for a method to norm~li7~o the gain and 15 efficiency of each ~etechon çlement and its associated amplifier.

The present invention provides such a semiconductor gamrna-ray camera and im~ging system wherein both planar images and SPECT images may be obtained. The im~ging system includes a ~1etector for sensing radiation emitted from a subject under test, electronics for conrlitioning and processing the detected radiation ~i~n~l~ a CO~yult,r for 20 controlling the detection process and of forming and displaying images based upon the signals ge ~e.~ted by the detectors, and output devices for displaying the images and providing data to a user.
S~lblM~RY OF 1~ INVENl~ON

An im~gin~ system inclll~ing an im~in~ head, a signal processor, a data acquisition system and an irnage processin~ coml,~t~. is described. The im~in~ head preferably incllldf s an x-ray or gamma-ray detector and an e.lL~ce a~ ure such as a collimator or 5 pinhole for directing the rays to the detector. I~ the p~r,,.l~;1 embodiment, the detector compricfs a plurality of closely-paclced detection modules. Each detection module compri~Ps a plurality of detection elements mounted to a circ ut carner. The detection elements produce electrical pulses having ~mplihlde5 indicative of the m~gnih~e of radiation absorbed by the detection f lemf ntc In the plefe.~1 embo~iment, the detection 10 eleTnent$ are coupled to a circuit carrier contained withill the im~ging head. The circuit carrier includes ci.c~iL,y for conditioning and processing the signals generated by the detection elf mf ntc and for plep~lL~g the processed signals for further procf~csing by the signal processor. Each ~etection el~ ment has a collesluonding conditioning and procf c$in~ ~h~nnf l The clf tection e1L ..~ plcr~Lably comrrice c~millm-zinc-telluride 15 m~teri~l In accoLd~ce with the present invention, each conditioning and processing channel stores the amplitudes of the detection f If' ~ Ilf.- It electrical pulses which exceed a predetf rmined threshold. When a df tection f'lf ~ . lf.~ l~ absorbs sllfficipnt radiation to produce an electrical pulse having an ~mplitll~e which ~;~cee~s the threshold, the rh~nnf,l associated with the 20 detection elemfnt records a valid detection ~ll ~Il~lt "event". The detection modules employ a falI-through circuitwhich ~ulo.~ l;e~lly finds only those detection elemf ntc that have recorded a valid hit. When ylul~pted by the signal processor, the fall-through circu~t searches for the next detection clemc.~t and associated channel having a valid event.
Upon finding the next recorded event, the detection module produces the address of the 25 element and the arnplitude of the electrical pulse which produced the valid event. The address of each detection element and p~se amplitude is provided to the signal processor for further procescing CA 02208~76 1997-06-23 W O 96t20412 PCTnUS95/16911 The signal ~ùce~s~r ac.lLLu~s data from the con~ oning and proc~ccing rh~nnPlc, no~n~li7Ps and formats the data, and stores it in memory bloclcs for access by the data acquisition CU111~Ut~ L. In addition, the signal processor provides a bias voltage for the detector and provides the event threshold voltage that is used by the detection modules 5 for riicl;.;"~ g valid events. The signal processor pe rùllllc diagnostics, gain no~n~li7~tion, and re."uûrlse efficiency norrn~li7~tion fi~nrtionc The data acquisition system includes hardware and software which co..".,l",i~t~ with the signal processor and the image l,lucessi~lg co",~.ul~ system. The data acquisition system controls acquisition and processing of data received from the conditioning and processing 10 ch~nn~c, produces image data based upon the event data in a format that is compatible with existing im~ing ca~n~,.aS, and l~, --'.--liL~; the data to the im ge processing computer.
The data acquisition system also provides a mt~fh~;c... for ...~;..I; ;.~;~g detectjon elem~nt event histograms and pulse-height distribution data. The data acquisition sy tem can produce images in a ~L~d~d format to allow images to be displayed using co~n~Lcially 15 available im~ging systems.

The image ~loc~;llg co~u~. . displays images based upon the signals generated by the detection elem~ntc The image ~Locess;.-g cou~ulc~ form~ t~s irnages based upon the processed signals and displays the formlll~t~ images on a display device. The image processing coL~puh~ provides an int~rf~re with an o~.aLor, controls data acquisition 20 modes, receives image data from the data acquisition system, displays i ages in real tirne on a display device, and col~icates with display and other readout devices. The image processing colll~ule. also provides a mech~nicm for ad~usting operational parameters used within the im~ging system.

The details of the preferred embodiment of the present invention are set forth in the 25 acco~ ying drawings and the description below. Once the details of the invention are known, IlUll~. .uus ~d~ihon~l ~o~ions and c]-~ ~g~ ~ will be~o~c ob~ious to one skilled in the art.

BRIEF DESCRIPTIO~ OF T~IE DRAWINGS

FIGURE 1 shows the camera and im~in~ system of the present invention.

FIGURE 2 shows the camera and im~E~in~ system of FIGURE 1, showing the detector,signal p,ocessol, data acquisition system, and image processing col~yu~ system of the 5 present invention.

FIGURE 3a shows an exploded ~ ec~ive view of a detection module used in the detector shown in FIGURE 2.

FIGURE 3b shows an exploded pc.:,~e~ e view of an altemative embodiment of the detection module shown in FIGURE 2.

10 FIGURE 4 shows a block diagram ofthe detection module board shown in FIGURE 2.

FIGURE 5a is a block ~ gr~m of the detection modules used in the detection module board shown in FIGI)RE 4 showing the il,t~rconn~c';on of signals between analog and digital ASICs used to implement the detection module functions.

FIGURE Sb is a simplified bloclc diagram of a fall-through circuit used to read valid 15 events recorded in the detection tolt-m~ont conditioning and p~oces~ g ch~nnçlc of the present invention.

FIGURE 6 shows a bloclc diagram of the analog ASIC shown in FIGURE Sa.

FIGURE 7 shows a block diagram of the digital ASIC shown in FIGURE Sa FIGURE 8 shows a fim~l n~l block ~iagr~rn of the signal ~.~,ce~so~ shown in FIGURE
2.

FIGURE 9 shows additional details of the signal ~OCeSSOI of FIGURE 8.

Like ~ef ~ nce numbers and ~esi~T ~tions in the various drawings refer to Iike e~ ont.~.

W O 96/20412 PCTrUS95/16911 DETAILED DESCRIPTION OF THE INVENlION

Throughout this description, the ~Lcfell~d embodiment and examples shown should be considered as exemplars, rather t~lar as limit~tion~ on the present invention. The following d~s~ption ~esr~ib~s ~etection of gamma rays, however, the detection of x rays 5 can be equally con~id~red. Many x-ray applications would require dirr~.e.lt ~im~n~ions of the sub-coLuponc~L~.

The semicon~ctor-based garnrna-ray camera and m~lic~l im~ging system of the present invention, he.e;~LI~ referred to as a "camera," is shown in FIGURE 1 and referred to by ~cf~ ce nnm~l 100. Reft ~ing simlllt~n~-ously to FIGURES I and 2, the camera 100 10 ofthe present invention compri~ps a gamrna-ray detector 200, an entrance apelLulc such as a colIimator or pinhole 205 for directing the gamrna rays to the detector, a signal processor 300, a data acquisition COLU~U~,r 400, an irnage proc~s~ing co~ uLel system 450, and a gantry 500 for positioning the camera adjacent to a patient7 an organ, or other object 102. The ~letPctor 200 is used to sense r~ rion e_itted from the object 102. The signals ge .~ rd by the detector 200 are ~ d to the signal processor 300 using any convenient means, preferably a digital communications link 202.

As shown in FIGURE 2, the camera 100 also preferably int~ s a pluTality of input/output devices for 1.,~ ...;LI;.~g and displaying derived images of the object 102 to both on-site and remote users ofthe present invention. For example, the present camera 20 100 preferably includes, at a minimum, an input from a device such as an ele~;hoca~ liograph and a display device 604 for displaying images ofthe object 102 to on-site users (not shown). However, images can also be tr~n~m~ to off-site or remote users via a teleco., l. "u.~ic~ions L~. .wo~h 616 using a f~c~imile m~chine 600 or a modem 602 or direct digital r.elwu~k (not shown). The camera 100 can produce "hard copies" of 25 images using a plurality of paper display de~ices. For example, the camera 100 can include a laser printer 606, a dot-matrix printer 608, and a plotter 610 for providing paper PCT~US95/16911 or filrn copies of an irnage. The carnera 100 can also store ~igiti7~d irnages of the object 102 in a magnetic data storage device 614 and/or an optical data storage device 612.

Both planar and single photon ernission coLu~uLed tomographic (SPECI ) irnages of the ernission of radiation from radioisotopes are obtainable using the present camera 100.
5 The camera 100 is ~ci~ne~l to provide images of areas that are difflcult to access and image using COll~ ;on~l garnma cameras. The camera 100 is also r~ecign~rl to provide images that are coLI~nLionally obtained in nuclear medicine. As shown in FIGURE 2, the gamma-ray detector 200 preferably comrric~s an array 204 of detection modules 206 mounted upon a module board 208. The module board 208 transmits the signals 10 generated by the detection modules to the signal processor 300 for procescing. As described in more detail below with leftl~ nce to FIGURES 3-4, each of the detection modules 206 includes detection elem~ont array 212 which comprise semiconductor m~t~ri~l that can detect gamma radiation with acceptable p~lrullllance at room t~LU~ld-ture. In addition, each tletec~ion module 206 includes ulL~dted circuits (ICs) in a carrier 214, o~ Livdy coupled to the detection elements 212, that amplify, condition, and process the electrical signals g~ ,,t~d by the detection elements for tr~ncmiccion to the sig~al processor 300. The sig~al processor 300 ac.luu~ the signals from the gamma-ray detector 200, makes corrections to the data, and places the data into memory for use by the data acquisition coLul.uL~ 400 for fu- 111 ;n~ images of the object 102. The irnages are displayed on the display 604 and stored, printed, or LI~L liLLed using the other output devices shown in FIGURE 2. The sig~ificant coLu~olle,.L~ of the camera 100 are described below in respective sub-sections.

G~mm~-Rav Detector The gamma-ray detector 200 of the present invention comprises an array of closely-packed detecion modules 206 mounted upon the module board 208. The module board 208 routes the signals generated by the detection modules 206 to the signal processor 300.
The detector 200 preferably includes an 8X8 array of detection modules 206. For -PCTrUS95/16911 conve~ience of ples~ AI ;on, FIGURE 2 shows a 4xj array of ~tection mod~es 206.
The ~etection modules 206 are preferably ~im~n~ion~ 1-inch by 1-inch square.
Therefore, the ~efe,L~d embodiment of the gamma-ray detector 200 has an "active"sensing area of 64 square inches.

5 Another embodiment of the present invention mounts the detection modules 206 in a shape other than a plane to form a detectinn surface that is more a~pro~liate for imAging some objects. Also, although the illustrated embodiments desrribe a detector 200 having detection modules 206 arranged in an array format, the present invention con~ plates detectors 200 including detection modules 206 a~Tanged in other configurations. For 10 example, the modules 206 can be arranged linearly, or in a circle, or in any other convenient configuration.

The module board 208 and the ~tection modules 206 of the ~etector 200 are housedwithin a light-tight housing. Shi~l~ing mAt~ri~l preferably lead, is positioned behind and on the sides of the module board 208 and detection modules 206 to prevent stray rArliAtion 15 fiom adversely affecting the acquired image. The shields are Al~ A~;~/ely made of tungsten carbide or other high-density m~tPriAI and have sufficient mass to block ullw~Llt~d stray r~iAtion from reaching the detection ~ --f .I~'i and thereby degrading the quality of the images produced by the camera 100. The housing (not shown) also preferably includes a thin ~ lll window which is positioned over the face of the20 detection modules 206. The window prote~ the detection modules from light andphysical damage yet allows gamma rays emitted from the object 102 under test to penetrate the window and to be absorbed in the detection elements 212. Alternatively, the window can be made from any low Z mAt~riAI which does not absorb an appreciable amount of the radiation being imaged.

The housing is secured around the module board 208, detection elements 206, and shielding mAt~ri~l using screws or other ~llArh",~ ~I means. The digital co~ ications W O 96/20412 PCTrUS95/16911 link 202 enters the housing L~o~ a hole or slot (not shown) formed at one end. The slot a~d the housing edges are preferably made light-tight. The housing is preferably su~polled to the gantry 500 using vibration isolation techniques. In one l~cf~ dembo-limPnt the t~ e within the housing is controlled by a cooling system which S removes heat from the housing.

The dead region around the active surface at the detector is small. It is made up of the 5hiPlrling m~te~i~l on the sides of the detector and the support housing, and it is typically less than 0.5 inch.

Detection Modules~0 FIGURE 3a shows an exploded pe ~ .e~ e view of one detection module 206 of the Sc~ll invention. As depicted in FIGURE 3a, the detection module 206 c~.,.l,. ;~es an il,tc~ated circuit mounted within a l-inch square ceramic or plastic carrier. The semiconductor ~etection m~tPri~l, sub-com~o~1c.lt 210, of the detection module 206 incln~s an array of detection çlPm~ntc 212. The detrction elements 212 are preferably 15 configured in an 8x8 array. In the prcfc.,cd embodiment of the present invention, the detection elements 212 comrriee a plurality of c~l~iu~-zinc-telluride (CZT) garnma-ray detection areas formed on the lower surface of sub-colllpo~ent 210. The crystals can ~ltprn~tively c~mrrieP c~millm tell-lrid~P, mercuric iodide, g~ .., silicon, or other x-ray or gamma-ray se~lsi~vc m~teri~le As is known in the art, CZT crystals provide 20 good energy and spatial resolution, can operate at room tc~. ~al~c, and can be m~nllf~r-tured in large volurnes in a variety of ~imeneions. The CZT crystals convert gamma rays received from an object under test 102 (FIGURE 1) into electrical charge pulses. The ~mplit~ ç ofthe electrical pulses are indicative ofthe energy ofthe gamma rays absorbed.

The clet~ection modules 206 shown in FIGURE 3a is assembled with thin plates positioned 25 on both the top and bottom s~lrf~res of the sub-component 210. The upper plate (not sho~,vn) provides a means for applying a bias voltage to the detection modules 206, WO 96~ 12 in~ tl-s the bias voltage from the detector housing, and provides physical prol~clion for the CZT crystals. The upper plate is d~ci~n~d to allow the gamma rays ernitted from the object 102 to ~ ' h~t~ the plate and to be absorbed in the detection Clt .~.lt~ 212. In the y~fi ~l~d embo-iimtont the plates are made from 0.5 rnm thick ~lumin~ ~It~m~tively, the 5 upper and/or lower plates are made from glass epoxy circuit board or other inc~ tin~
m~tPri~l A lower plate 230 provides the means for con~ g the detection çl~ 212 to the circuit carrier 214. The lower plate 230 includes a plu~ality of contact pads 232 which co.l~y.~ud in position to the positions ofthe detection elements 212. The plurality of contact pads 232 provide electrical connection for each detection element to a 10 coll~yo~ g input contact pad on the top surface of the circuit carrier 214. The contact pads 232 are electricalIy isolated from each other.

The circuit carrier 214 houses the ICs and passive co,~ o~ ;, and provides illL~;u~ec-tions from the ICs to the detection elements 212 and to the module board 300. The circuit carrier 214 preferably comrricçs ceramic or plastic. In the preferred embodiment, thick-15 film resistors and ~ p~cil~ in the circuit carrier ~ 14 couple the signals from the detectionelements 212 to the inputs ofthe ICs and shunt detector leakage current to ground.

In the ~le~ ;d embodirnent of the present invention, the electrodes of sub-coll~onent 210 are formed by a gold layer on the CZT. ~lt~ tively, pl~tinllm, carbon, or other conductive m~teri~lc can be used. The rl~tection ~ om~ontc 212 are formed by an array of 20 electrodes on the lower surface of the sub-component 210. The spatial resolution of the gamma-ray detector 200 (FIGURE 1) is det~ d in large part by the size of the detection elements 212. ~e. r~ e and long-term stability are enhanced by passivating the areas of CZT crystal between the electrodes.

In an ~It~n~tive enviru--, ., It, the array of detection elpm~tc 212 fo~ned in the detection 25 module 206 compric.oc sep~ CZT cIystals, shown in FIGURE 3a as four CZT crystals 218, 220, 222, and 224. The cryst Is shown are preferably 12.7 mit~imeters by 12.7 WO 96/20412 PCItUS95tl6911 millimet~r_ by 3 millim~t.ors thick, comrncing spec~al grade CZT. Gold contact films or layers are affixed to top and bottom ~uLf~es of each crystal 218-224. The electrodes on the bottom surface of each crystal form a pattern of gold squares, one square for each detection ele n~nt In the ~ d emborlimpnt~ the gold squares are approximately 3 S millimeters on a side. The lines of separation 216 h .~. n the squares are preferably passivated, thereby, producing greater than 100 megohms isolation between detection el.om~ntc In the pl~f~.led embodiment, conductive epoxy is used to bond the electrodes of the det~ c~on ~1~ ml~ntc 212 to the contact pads ofthe lower plate and the co~ of the lower 10 plate to the input contact pads of the circuit carrier 214. ~ ItPrn~tively, other conductive bonding means may be uced such as indium-bump bonding.

Thus, the detector inputs are conn~cte~ to the ICs in the circuit carrier 214 via the upper surface of the carrier 214. Other inputs and outputs are connected to the ICs via a plurality of pins 240 on the bottom surface ofthe circuit carrier 214. The plurality of pins 15 240 are ~eci~n~ ~ to mate with insertion or socket CQ.~I-P~ aff~xed to the module board 208 (FTGURE 2). As described above, prior art assemblies of semiCon~ r~tQr radiation dclcclol~ typically ;--~t;, r~re with conrli~oning electronic circuits in a manner that allows the assemblies to be butted on, at most, three sides. The configuration of the detection module 206 shown in FIGURE 2 advantageously allows the detection module 206 to be 20 butted on all four sides. Th~.efole, the present detection module 206 advantageously provides a modular el~rn~nt which can be combined in a number of ways with otherdetection modules 206 to produce a nuclear medicine imager having a desired configura-tion.

",.I;~ely, FIGURE 3b depicts the same detection module 206 but with the array of25 semiconductor de~ection elements 213 formed by orthogonal strips on the upper and lower ~". r~ s of sub-co.llpone.lt 210. An advantage of using orthogonal strips is that the nurnber of ~h~....~lC of signal con~itioning is less for the same spatial resolution or the spatial resolution can be made finer with the same number of ~h~nnt~lc of signalcon~ oning In this embodiment, the signals from the upper surface are cQ....~cl~d to the inputs of the ;.~ d circuits via a capacitor and resistor network. The ~ e 5 embodiment shown in FIGURE 3b preferably has 32 upper strips and 32 lower strips on 1 mm centers in a module that has outer ~im~ncions of a~lo~ cly 32 mrn by 34 mm.The module has a small dead space at only one edge and is constructed to ~ i7e that dead space to allow the module to be fully buttable on 3 sides and buttable on 4 sides with a small dead space on only one side. The semiconductor m~tt~ri~l is made up of one or 10 more elements with strips formed on the ~... ri~ es and ~t~.co...~l-cte~l as required to form the total array.

CZT crystals have been comm~rcially available from Aurora Technologies Col~olalion of San Diego, C~lifomi~ since the late 1980's and from eV Products of SaYonburg,Pe~sylv~ia since 1993. Cadmiurn telluride is available from vendors in the U.S.A., 15 Asia, and Europe.

Pasaiv~tion of CZT Dclcclula In the prcf~lcd embodiment of the present invention, the areas of passivation on the ~ r~ s ofthe CZT su~co~ on~ ~l 210 are created by for~ung an insulating film on the CZT. In the plcf~"~d embodiment, a native oxide film is grown from a substrate of 20 cadmium zinc telluride after the metal layer has been deposited upon the substrate ~ ri1c~s Growing a native oxide film provides a means for ~oncl-ring that the resict~nce between metal pads or lines formed in the sub-ct~t~ is increased and m~int~in~(l at a high value.

The inclll~ting film layer 216 (FIGURE 2) is formed in a CZT surface by treating the CZT
25 surface with a hydrogen peroxide solution at low te~l.pe.~ cs. After the metal layer is deposited, a native oxide layer is grown by subjecting the CZT substrate to an aqueous PCTrUS95/16911 hy~oge.l peroxide solution of aE~lu~ ely 3% to 30% conce.lL aLiorl at te~ dLu~S
of ap~l~x;. ~ ly 20 ~C to 60 ~C for a~l.lu~ rly tvvo secon~c to an hour depending upon e. For example, the CZT ~etec~ion t?lern~nt array is preferably first m~t~lli7~dand ~ ;l before being c~ osed to the aqueous hydrogen peroxide solution.
S Typically, the CZT sub-co~ollent 210 is placed in an aqueous hydrogen peroxidesolution of a~p~u~ately ;% conc~ontr~tion for a~lu~ately 30 mim~tes at 60~C.
However, the Lr~ ~ ~p~ ~1l l l. e may vary depending upon the desired depth of the ûxide layer and the speed at which the oxide layer is to be grown. After exposing the CZT substrate as described, a black, highly-resistive oxide film is produced upon the surface of the CZT
10 substrate which sllbst~n~i~lly decleases surface leakage ~ le~lts between the detection elements 212. The leakage current can be further decreased by baking the passivated detection elements 212 in an oxygen-nitrogen en~ u~ cnt at relatively low te~ .dlul. s.
For e~mple, the passivdted detection elementc are typically baked in air for approxi-mately 30 " li-,~ s at a t. ,llp~dlure of appro~cim~tely 60~C.

The oxide film 216 between the detection elem~ntc 212 is soluble in hydrogen chloride solutions. The film may also be dissolved in an acidic aqueous HAuC14 electrolytic plating solution typically used for contact metallization. It is i~luoll~t to be able to dissolve the oxide fiIm when the CZT detectors are fabricated by pas~iva~ing the CZT
wafers before m~t~lli7~tion. In addition, dissolving the oxide fiLm is helpful when 20 selectively removing the oxide layer for metal deposition, and in a combined oxide-etch/metal plating process.

The present method of passivating the surface of the CZT detection crystals resolves known problems associaL~d with photûlithography for a number of reasons. Monolithic array structures produced by phûtolithography suffer frûm low surface re~ nre between 25 metallized contacts, a~patenLly due to an alteration of the stoichiometry and other chemical effects. Surface effects produced by photolithography are troublesome in monolithic array devices. Also, passivation of the edges enhances the capability of a PCTrUS95/16911 single c1~ detector or of an array detector to operate at high voltages, and de~ lcases leakage .;u..~ . The problems produced by photolithography are alleviated by thechernical passivalion method dçscribe~ above. By l~hPmi~11y passivating the CZT
surface, the present invention offers signific~nt ad/~es over the prior art. For5 exarnple, a native grown in~ ting layer elimin~tl-s the problems associated with depositing an oxide layer upon the CZT substrate. In addition, CZT crystals having a native oxide layer can be easily and iue~e~iv~ely m~n~1f~ct lred. The oxide layers provide high resistivity and decreased surface leakage c~rent between the detection elements 212. In addition, the native oxide is chemically co...~ ;ble with the CZT
I 0 substrate.

Detection Module Board FIGURE 4 shows a block ~ ~ m of the ~etPction module board 208 shown in FIGURE
2. The detection module board co~La~s an array of socket con"~clol~ into which each detection module 206 shown in FIGURE 2 is inserted. ~1t~m~tively, the modules can be 15 soldered into the module board. FIGURE 4 shows the illh.co~uection of the detection module input/output pins. In one embodirnent, the gamma-ray detector 200co~lises35 detection modules arranged in a 5x7 array. However, the array size used in the ill~L aLed embodiment is exemplary only, and should not be taken as a limitation of the present invention. The gamma-ray detector 200 of the present invention may comprise 20 X detection modules 206, arranged as an NxM array or as any shape or size. The only dif~erence between such an NxM array camera and the ill~hdtt;d embodiment example is the way the modules are mapped in the image and the number of address lines required.
For example, in one embodiment, six address lines specify the location of sixty-four detection modules 206 ~ ged in a square pattem. The same sixty-four elements could 25 also be arranged in any other desired shape, such as rectangular, circular, as an angular ring or a cross. In an embodiment having a 16X16 array of detection modules, eight active lines are required on the module address bus 256.

WO 96t20412 PCTIUS95/16911 Each ~etec~ion moduIe 206 shown in FIGURE 4 is mated to a co~ ,o~ding socket co~e~ilor (not shown) soldered or otherwise affixed and electrically coupled to the moduIe board 208. The sockets are closely packed together on the moduIe board 208 with the detection modules 206 butted against each other on all four sides when the 5 modules are fulIy engaged and mated with the 5O~ PtC The module board preferably includes "push holes" (not shown) at each module location which allow a technician to instalI or remove the modules 206 from the sockets without damage during testing and servicing.

Both digit 1 and analog signals are routed in a known fashion to each socket via traces in 10 the module board 208 as s~h~o~n~tically shown in FIGURE 4. The digital signals and supply lines are provided to the module board 208 via input and output ports that are co.-nP~-~e~l to the digital cou~u~cations link 202 (FIGURE 2). As shown in FIGURE
2 and described below in more detail with refe ~ --ce to FIGURE 8, the digital commllniç~-tions link 202 is connected to the signal processor 300. The analog sign~lc, output by each detection module 206, are bussed together on the module board 208 and routed via linear buffers 250, 252 to the signal processor 300 (FIGURE 2) via an analog link 203, preferably a twin-axial cable. The cross-talk between the analog and digital signals is thereby greatly reduced by conditioning and chiekling the analog output signals and by L~ g the analog and digital signals over s~&dte cornrnunication Links 202, 203.

20 In the embodiment shown in FIGURE 4, the detection modules have a plurality of input/output pins 240 (FIGURE 3a) which mate with corresponding insertion connectors in the module sockets affixed to the module board 208. The pin-fimction list for each module socket of the illustrated embodiment is given below in Table 1. Pins and functions listed below have co~le~olldi.lg integrated circuit inputloutput fimctionality as - 25 is described below with .~r. ~ nce to FIGURE 4.

PCTrUS95/16911 Ground co... ~l ;onc~ bias signals, and supply voltages are routed to the detection m~ s 206 via internal layers of the ~letection module board 208. Power pins are col---e~-led to bypass capacitors (not shown) which bypass the power supplies to les~c.,Li~e ground planes. Digital and linear signals are l,u~ d on both the module board 208 and on the 5 signal processor 300 (FIGURE 2). Table 2 shows the pin function list for the digital cc~ tionc ~nk202 which couples the module board 208 with the si~ processor 300.

P~ NCTION
¦ INPUT/OUTPUT ¦
1-6 Element Address Output 7 FallIn Input 8 FalI Out Output 9 Valid Output Address Enable Output I l Advarlce Input 12 Linear Reference Output 13 Linear Ou~:put Output 14 Threshold Input Threshold Re~.e.lce Input 16 Analog Power #1 n/a 17 Analog Ground #l n/a 18 AnalogPower#2 n/a 19 Analog Ground #2 n/a Digital Power #2 nla 21 Digital Ground #2 n/a 22 Test Signal (Linear) Input 23 Test Shift Register CLK Input 24 Test Shift Register Data In Input Test Shift Register Data Out Output TABLE 1 - Detection Module Pinout Function List PCTrUS95/16911 F~CTION INPUT/OUTP-1-6F.lemen~ Address Output 7-14Module Address Output Valid Output 16 Advance Input 17 Threshold I~put 18Bias Voltage n/a 19Analog Power n/a 20Analog Ground n/a 21Digital Power n/a 22Digital Ground n/a 23Buffer Power n/a 24Buffer Power n/a 25Buffer Ground n/a 26Chassis Ground n/a 27Test Signal input 28 Test Data input 29Shift Register ~1 input 30Shift Register t~2 input TABLE 2 - Wire List for Link 202 In the plef;,l~1 embodiment, tne signals provided from the signal ~lucesso~ 300 to the detection module board 208 include voltage and ground refere~ces and the "advance"
signal. As desrnbe~ below in more detail, the address and "valid" signals and the analog outputs are provided from the detecion module board 208 to the signal processor 300 S when a fall-through addressing id~nhfi~s a valid event in a detection el~mPnt 212. These signals are bussed to every detection module 206 on the module board 208. For eY~mrle all of the valid lines of the detection modules 206 are bussed together on line 260. The bias voltage (preferably 200-500 volts) is connPcted to the top surface of each detection module and excites the detection elements 212 during camera operation.
10 Both module and element addresses are supplied to the signal processor 300 via comrnon address lines 256, 262 co~ ected from each detection module location on the module board 208. The module address bus 256 and the elem~nt address bus 262 are logically combined to create an n-bit wide address bus. In the p.c;f:_,.ed embodiment, the address bus I ~ to the signal processor 300 is l~bits wide. In the ~refe~.~d embo~lim~?nt, the module address lines 256 are treated by the signal processor 300 as the most-signifi-cant-address bits, and the element address lines 262 are treated as the least-significant-address bits. The address busses 256, 262 are driven by tri-state buffers at each detection module loc~non Only one detection module 206 asserts an address on the address busses 256, 262 at a given time.

20 In the ~lcfe,l~d embodiment, the module address of each detection module 206 is "hard-wired" into a tri-state ~scei~er located at each module on the module board 208. That is, the binary address for each module socket is pre-wired by connecting the apyl~pliate bits to digital ground and power. As described below in more detail with reference to FIGURES 5-7, when the fall-through addressing arrives at a detection module with valid 25 data, that module outputs an analog signal (via a linear signal out line 270), a "valid"
signal, an "address enable" signal, and the address which uniquely id~nt-ifi~s the detection ~l~m~nt 212. The digital IC in the detection module 206 asserts the detection element WO 96/20412 PCI~/US95/16911 address on the address bus 256, and a tri-state address buffer at that module location asserts the detection module address on the bus 262 when an "address enable" signal is asserted true. The detection modules 206 are the.efo,e ~esign~ to be completely interchangeable. The detection modules 206 the.~fc"~c are not "addressed" by the data S acquisition co~uull-~ 400 in a conventional sense. Rather, as described below in more detail with lcf~ ce to FIGIJRES 5-~, the modules 206 initiate the address when an event occurs. As shown in FIGURE 4, the detection modules 206 are linked together in a"daisy-chain" configuration by couplLng the "fall-out" output signal from one module (e.g., fall-out signal 280) to the "fall-in" input signal of a successive module (e.g., fall-in 10 signal 282). As described below, the "fall-in" and "fall-out" signals are used to implement the "fall-throu~h" data scheme of the present Lnvention.

As ~esrribed below in more detail, when a detection module 206 asserts a valid signal on line 260, the signal processor 300 reads and plocesses that detection element's address on the "address" lines and analog signal on the "linear output" line. The signal p~cessor 300 15 then re-init.~tt s the fall-through adL~s~g and data acquisition process by generating and s~n~linP an "advance" signal overthe digital c~.. ,.. "ications link202.

~etection Modules ~ o~ ection of the An~log ~nd Di~ital Tnt~rated Circuits The circuit carrier 214 preferably co~ c three ;..t~.,.t~ ci~ two identical analog application specific integrated circuits (ASICs) and one digital ASIC. The two analog 20 ASICs arnplify and shape the analog signals for processing by the digital ASIC. The digital ASIC co~, es the analog signals ge .~ ~r~ by the analog ASICs with a reference or threshold voltage. If the signal is greater than the threshold (a "valid hit"), a latch is set which causes the analog value to be stored in a peak detection circuit. When enabled by a fall-through signal, the digital ASIC generates a "valid" signal and an "address 25 enable" signal. L~ ,conl~;~ions within the detection module 206 between the two analog ASICs 700 and a digital ASIC 800 are shown in the block tli~ m of FIGURE ja. The64 signals from the detection elements 212 are connPctPd to the inputs of the analog W O 96/20412 PCTrUS95/16911 ASICs via thick-film r~ JIS in camer 214. The leakage current from each ~letection ele~c.lL 212 is routed to ground via thick-film resistors so litho~Qph~d on the carrier 214.

Although the present invention is shown having t~vo analog ASICs 700 in each detection module 206, one skilled in the art will ay~fe-e;ate that the signal conditioning functions p~,lru~ ed by the analog ASICs 700 can be irnplemented in an QltemQtive embodiment within one ASIC 700 and that the number of analog chan-lels in one ASIC 700 couId be either greater or less than 32. Further, the present invention co~Lc;.,lplates combining the analog and digital processing fiml~hon~ on a single ~te~ated circuit.

Because the detection elem~ntc 212 produce low Qmplit~ e electrical pulses when irr~-liQtç~ any noise created during the proc~csing of these signals can adversely affect the resultant image. The present invention ~ignifiçQntly reduces crosstaLk and noise by se~Lil~g the analog and digital ciLc~iL~ y into sep~ nte ASICs.

Some prior art imQging devices use ASICs that re~uire that the preQmplifier associated with each detechon element 212 be reset periodically to coLu~e~sale for detector and ~mrlifiPr input ~ . This resetting is typically acco. . ,pli~h~d with an analog switch co~lne~;t~d across the preQmplifier fee~bQ~k path. The operation of the switch causes large, spurious signals and mo."P .I~. ;ly in~QpacitQtes the amplifier. Passive fee~lbQck n~ olks are difficult to implement bec~.~se high re~i~tQnce values must be used to effectively reduce the noise levels. The pro~llction of such high-value resistors is not c~ ly possible. As shown in FIGURE 5a, the present invention el;lll;l~tes the detector current portion of this problem by placing a resistor/capacitor network 702 be~veen an input port 704 and its associated input pad 706 on each input of the an~og ASIC 700.
The resistorlcQrQcitor ne~wulh702 shunts leakage current from the ~etec~ion element 212 to ~ anlog ground 712 on the module board 208 before the leakage current enters the analog ASIC 700. Typical values for the resistor 708 and the capacitor 710 of the WO 96/20412 PCTrUS95/16911 ~eji~Lol/c~p~--iLo. n~.w~lL 702 are 200MQ and 100 pF, re~,uc~;Li~ely. The amplifier input current is co~ ed by using a high output iu~pcdallce arnplifier as the feedb~rk element around the preamplifier. Each detection el~mtont 212 of the 8x8 array of each detection module 206 iS electrically coupled to an input port 704 on the circuit carrier 214. The signals g~ ~d by the ~1P ~ch~n elf~fn~8ntc 2l2 and t~ .c.~.iLll~d to the 64 input ports 704 are relatively low-level signals ranging in values from 6000 to 60,000 electrorls.

Assertion of the valid line 260 by one of the detection modules 206 indicates that at least one of its detection elements 212 has received a hit that ~ uucs processing and that it was selected by the fall-through addressing. Following a valid hit and after waiting a short time period which is sufficient to allow the linear signal to stabilize within the peak detector, the digital ASIC 800 enables an intf m~l gate and waits to be enabled by a fall-through signal which is described below in more detail. Valid hits can be con.;ul~ y stored for all detection elements 212 in the ~f~tecrion module 206 by the digital ASIC.
After a detection element 212 receives a valid hit, it waits to be enabled by a fall-through signal. The ASIC 800 then asserts a "valid" signal on output line 260 and an address enable signal on output pad 831. As described above and shown in FIGURE 4, the valid lines 260 of all of the detection modules 206 are electrically coupled together and the valid signal is ~ ed to the signal processor 300 over the digital coll~ullica~ons link 202.

Thus, if any of the ~etech~n ek ~ ; in the gamma-ray detector 200 produce a valid hit, the valid and address enable signals are asserted for that detection element when it is enabled by the fall-through signal. A peak detector in each ch~nnf l of the digital ASIC
800 stores the amplitude ofthe charge pulse received from the detection çl~m~nt 212 until it is read by the signal ~lucessor 300. As shown in FIGURE ~a, the stored analog signal is provided to the signal ulucesso~ 300 through an analog pad 817 which is coupled with the linear bus 270. The hit is held within the digital ASIC 800 untiI it is read, processed, and cleared by an advance signal 258 produced by the signal processor 300. Each peak W O96/20412 PCTrUS9~/16911 detector within the digital ASIC 800 stores the ~mplit~lde of the highest amplitude of sl~ccessive hits generated by a detection el~m~nt 212 until it is reset by the signal processor 300. The "hold droop" of the peak detector is preferably apl,lo~ately no greater than 0.0001 % per microsecond.

5 When the signal processor 300 completes processing the event, it asserts an "advance"
signal on advance signal line 258. As shown in FIGURE 4, the advance signal line 258 of each module 206 is electrically coupled together. When the advance line 258 is asserted true, the active detection module 206 (i.e., the detection module which ~lesellLly has control of the address busses 256, 262 and the linear bus 270) clears the active output 10 lines (valid line, address lines, and linear signals) and allows the fall-through signal to advance to the next latched detection elt?mPnS

Fall-shrollph Circuit A fall-throug_ circuit is included in ASIC 800 for each detection element. A simplified block diagram of the fall-through circuit is shown in FIGURE 5b as a series of logical 15 "AND" and "OR" gates coupled together. This depiction of the fall-through circuit is given simply to describe its function. Each detection elt m~ns 212 has a colL~onding latch within the ASIC 800 for storing valid hits received by the detection element 212.
For example, as shown in FIGURE 5b, latch 808 stores a hit received by the firstdetection çll nl ,l (DE 0), latch 810 stores a hit received by the second detection ele~nPnt 20 in the 8x8 ~Tay (DE 1), and so on. The latch outputs are coupled to co~ onding fall-through blocks 812, 814. Block 812 has a first input of its OR gate 816 coupled to the fall-in signal line 282. The fall-in and fall-out signal lines of the detec~ion modules 266 on the board 208 are "daisy-chained" together (FIGURE 4). For example, the fall-out signal line 280 of detection module 266 is coupled to the fall-in input 282 of the next detection module 268. The last detection module 284 of the a~ray of detection modules 206 has its fall-out line 280 coupled to a NOR gate 286. The output of the NOR gate 286 is coupled to the fall-in input 282 of the first detection module 266.

Therefore, the fall-through circuits within each detection module 206 of the garnma-ray detector 200 are a~l tied together, forrnin~ one circular fall-through loop. The NOR gate 286 allows the fall-through system to be initi~li7~1 during a power-up sequence. For example, at power up, a PWR UP signal 288 is asserted high which causes a one-shot multivibrator 290 to de-assert a logical 0 pulse on the fall-in signal line 282 of the first detection module 266. Refi ~ring again to FIGURE 5b, if the first detection element latch 808 of the first detection module 266 is not set (i.e., the first detection element 212 associated with the latch 808 has not received a valid hit), the OR gate 816 will output a logical low value. The logical low is input into an OR gate 818 of the next fall-through block 814 which is associated with the next detection element 212 of the 8x8 array of detection elements 212 (e.g., "DE 1 "). If the next detection element latch 810 is not set (i.e., the second detection element 212 associated with the latch 810 has not received a valid hit), the OR gate 818 will also output a logical low value. The subsequent fall-through blocks will similarly continue to produce a logical low value which progresses through the chain of fall-through blocks until a detection element is found which has received a hit and has thereby set its colfe~onding latch. If no detection element 212 within a ~etection module 266 received a valid hit, that is, if the digital ASIC 800 of detection module 266 does not have a latch set, the detection module outputs a logical low from its fall-out signal line 280. The low value is input to the fall-in input line 282 of the next module 268. Thus, the logical low progresses through the OR gates of each sl.fcee~;..g module until an el~-m.ont that has an event ready for procPs~ing is encou~ ~d or the signal passes out of the last module and back into the first.

A logical high input to any OR gate (i.e., OR gates 816, 818, and so on) stops the fall-through process. When an event is found, the digital ASIC 800 activates tri-state buffers 25 (not shown) which allows the ASIC to take control of both the digital address busses 256, 262 and the linear signal line 270 (FIGURE 4). The address of the detection element 212 which received the hit and which subsequently caused the fall-through circuit to halt is output onto the element address bus lines 262 by the ASIC 800. The address of the ASIC's detection module 206 is also ass~ d from the ~ ccciver onto the module - address lines 256 by the address enable line 832. As described above, the module address is hard-wired on the module board 208 into an 8-bit ha~sceiver that is enabled by the address enable signal. The analog signal ofthe detection Pl.oment 212 which caused the 5 fall-~.,~ process to halt is sPlected using the ~etPction element address output 262 of the digital ASIC 800.

The valid signal resulting from a hit causes the signal processor 300 to read and process the address and the analog signal. No other detection module can access the bus lines because the fall-through configuration ensures that only one detection module 206 is 10 enabled at a time. The fall-through process remains halted until the signal processor 300 completes proce~sing the event and asserts an "advance" signal over the advance signal line 258 which is shared by every detPction module. When the active ~letection module receives the advance signal, it ~l r~.".,~ the following functions in se~lu~lce: resets the peak detector which is ~;u~ Lly addressed; it de-asserts the valid signal causing the valid 15 signal line 260 to assume a logical low value; it de-asserts the address enable signal; it disables its tri-state buffers, thereby, relP~ing the address and signal busses; and it asserts a logical low pulse over its fall-out line. The fall-through process resumes with the next fall-through bloclc in the digital ASIC 800.

Because the fall-through scheme scans detection element~ in a sequential manner, one 20 Ple ~ at a time, ~etection r.l~ . "~. ,t i 212 that receive a valid hit cannot affect or illh.~ ulJt the sc~nning of other detec~ion elPmPnt~ All elements are "1atched-out" or inhibited until they are read during a subsequent fall-through scan. Thus, each detection element 212 of each module 206 is given an e~ual oppo~ ~u.~y to be serviced by the signal processor 300.

W O 96/20412 PCTnUS95/16911 Tn~ d~c:d cirr~litc acs) FIGURE 6 shows a block diagram of t_e analog ASIC 700 of FIGURE Sa. Preferably, each analog ASIC 700 in~ os thirty-two ch~nnelc Each ~h~nnçl preferably has an input pad 706 for rece;v~g and con~litioning the analog signal produced by its associated 5 detection elernent 212 when a garnrna-ray is absorbed. Each ~h~nnel includes a charge amplifier 718 and a ch~ping arnplifier 720. The prearnplifier inco~ dLes a current-sourcing ~mp1ifier (inrli~tl d by resistor 738 in FIGURE 6) to m~int~in the DC stability of the circuit. The rise and fall times of the shaping amplifier are set via resistors external to the ASIC 700.

10 The ~lef~ d value of the c~p~citor 740 is selecte~l to provide a desired delay time. The amplifiers 718 are ~ecign~l to amplify the pulses g~ 1led by the detection ~ e..~ 212 to levels which can trigger CO-~p~o~la within the digital ASIC 800. Preferably, the ~mplifierc 718 amplif,v the ~nalog signals to levels ~p~o~ately equal to one volt.

The peaking and fall times of the ch~ring ~mplifier 720 is chosen to . .~ white and 15 1/F noise contributions and to obtain good b~celinP recovery. Preferably the peaking time is 0.1 to 1.0 microsecond with fall times of 1 to 10 microseco~1c~ The outputs of the shaping amplifiers 720 are coupled to the inputs of col~,J~onding peak deteclola in the digital ASIC 800.

As shown in FIGURE 7, the digital ASIC 800 preferably includes sixty-four parallel 20 çh~nnelc coll~Jl,onding to the sixty-four detection elPmentc 212 asso~ d with each detec~ion module 206. Each channel includes a peak detector 820, a colllpdldlor 822, an event latch 824, AND gates 826, 828, a fall-through block 830, and an address encoder 832.

As described above with reference to FIGURE 5a, the peak detectors 820 p.,lrO~ an 25 analog peak detection function by storing the highest of successive pulses gen~.dted by the detection elements 212 until a valid signal "locks out" any subsequently generated pulses. The ~ubse~ Lly g~ tr~l pulses are "locked out" untiI the peak value is read.
The switch 814 allows the analog signal from the selected peak ~et~ctor to be t~ d to the signal processor 300 via the linear out sig line 817 when that detection element 5 address is valid.

As shown in FIGURE 7, the peak detectors 820 include control lines 833 coupled from the fall-through blocks (830,836, 838) to the ~wit~,hcs 814. The switches 814 couple the OUtpUt of a s~lected peak detector 820 to the signal buffer 812 when act~l~ted by a control line 833. The an~log voltage stored by any one peak detector 820 is reset by the advance 10 signal 842 if and only if the address of that element is enabled. That is, when a switch 814 is activated by a fall-through block (e.g., 830), the peak detector connected to the activated switch 814 is reset when the advance signal 842 is asserted. Thus, after the signal processor 300 processes an event stored by a peak detector, it clears the selected peak detector 820 to allow it to begin ~c~ ting subsequent hits.

The buffer/driver 812 is coupled to switch 810. The switch 810 is controlled by an address valid signal line 848. The address valid signal line 848 is described below in more detail with ~efe~nce to the fall-through blocks enable signals. The output of the buffer/driver 812 is coupled to the out sig output pad 817 which is connected to the signal processor 300 via the Linear out signal Line 270 (FIGURES 4 and 5).

20 As shown in FIGURE 7, a first input to the co~pdldtor 822 is provided via the input pad 802. A second input to the co~ d~atur 822 is provided via a threshold voltage (V~ input line 804 which is cornmon to all modules in the system. If the detection element signal arnplitude has a voltage that is lower than the threshold voltage, the event is not recorded.
However, if the detection-element-signal amplitude is greater than the threshold (V~, 2~ the co~paLator 822 asserts its output (preferably by asserting a logical high value at its output) to set the co~ ,onding latch 824. The signal remains recorded in the event latch CA 02208576 l997-06-23 W O96/20412 PCTrUS95/16911 824 until it is processed and reset by t_e signal processor 300 as ~esrnbed below in more detail.

The AND gates 826,828 serve two di~ t timing functions. The AND gate 826iS usedto ensure t_at the pulse g. ..~ .aLed by a detection elemçnt 212is allowed to stabilize within S t_e peak detector 820 (FIGURE 7)~ccori~t~1 with that detection element 212 before t_e valid signal is gene~aLed. The logical one is inverted before it is input to the AND gate 826, which causes the output of the AND gate to transition to a logical low value. The AND gate 826 output will co.,~ .o to be m~ .;n~d at a logical low value until the pulse received by the input 802 transitions below the threshold voltage. The AND gate 826 the,c:folc pl~ the output of the event latch 824 from passing though it to the AND
gate 828 input until the pulse returns to a level below the threshold voltage. This delay ensures that the peak detector 820iS allowed to stabilize before a hit is passed on to the fall-through block 830. This ensures that the analog signal ~ e~l by the peak dotector 820 via out_sig pad 817 co~ o~lds to the peak arnplitude of the pulse.

The AND gate 828iS used in conjunction with the fall-through block 830 to facilitate the fall-through scheme described above. As described below in more detail, the AND gate 828 prevents a detection element 212 which .eceives a hit from i~L~-u~L~g the fall-through process until the detection el~m~ont is sc~nnçd by the fall-through circuit. The AND gate 828, together with the fall-through blocks, ensures that every event latch 824 issc~nnP(l in se~ù~Lial order and that every detection element has an equal op~olluui to be serv-iced by the signal processor 300.

As described above with reference to FIGURE Sa when the "advance" signal 258 iS
asserted on advance input pad 842, the sc~nn~od event latch 824iS reset via reset line 844.
As shown in FIGURE 7, the reset line 844 of the enabled latch 824iS coupled to the priorit,v-select/fall-through block 830. When a selected block 830 receives an advance sigIlal 842, the block 830 resets the latch 824 via the reset line 844.

W O96/20412 PCTrUS9S/16911 The fall-through blocks include "enable" outputs which are coupled to a plurality of address en- odPrs (i.e., 832, $70, 890, etc.). AI1 enable output of a selected fall-through block is asserted ~l~e.~ . the event latch 824 which is coupled to the sPlectPcl priority select block co~ an event and the selected priority select block is ~ Lly being 5 sc~ (i.e., the fall-through process has reached the s~le~Lecl priority select block). The enable outputs thereby cause one of the address encoders (e.g., 832) to present an address on an internal address bus 846 which is indicative of the selected detecion elPment 212 co."i.,.,;.,g a valid hit. A valid address signal 848 is then as~c.lc~d which causes an analog switch 850 to close. The detection elemPnt address is then asserted on the detection element address bus 262 and LL~ I;LIe~-1 to the signal processor 300.

As described above with reference to FIGURES 5-7, each ~etechon module 206 has an analog ASIC 700 which ~mplifies the analog sign~s produced by the detection ele.~eu 212 and which CO111~LC3 the analog signals with an event threshold voltage which is commc)~ to all of the detection modules 206. The event threshold voltage is preferably 15 established above noise level. When the analog signal produced by a detection element 212 PYI~ee~1s the event threshold voltage and that detection element is "addressed" via the fall-through scheme as described above, the digital ASIC 800 g~,dtes a valid signal 260 which infnrmc the cOlll~u~, signal plocess()r 300 that at least one detection ele,lle.lt 212 has lcceivcd a hit ~. 4u~ g p~cej~;r-g The digital ASIC 800 takes control of the linear 20 and address busses and outputs both the address of the detection elPmPn~ 212 and the m~gnit~ e of the amplified signal. The ASICs 700, 800 clear the flag and the linear signal produced by the addressed detection ele..lc.lt 212 once the signal processor reads and processes the event. As described below in more detail, the signal processor 300 inflic~teS when it has ~,cessed an event by assc. Ling the "advance" signal via the advance 25 signal line 258.

Ihus, the gamrna-ray detector 200 and, more specific~lly, the module board 208 appears to the signal processor 300 as a very simple analog/digital input device compn~ing an array of det~tJ., which produce pulse-height and address ;.lru....AI;on and which store this ;- fU- . I-A~ ;on until a read completion acknowledgement (via the adv~ce sig~al 258) is provided by the signal pluccssor 300. When the signal processûr 300 has comple~cl plOC~;"g a ~etec~ on çl~mPnt's address and reading the elc.llc.lL's linear signal, the 5 system g. ..l ,.t. ', an advance signal 258, thus allowing the next pending ~letPct on cl( mYnt to be addressed. The next ell~mPnt in the ~etection module array which has a hit pending will g. ~ e its address, its analog signal, and a valid flag. The signal processor 300 is thereby freed ofthe tirne-intensive task of polling each detection element 212, including detPCt;OnCIL~ which do not have pending hits. In fact, using the fall-through scheme 10 described above with reference to FIGURES 5-î, the addressing of detection el~m~n occurs indepen~Pntly ofthe proc~ing p~ rO. ",rtl by the signal processor 300. The signal processor 300 simply pulses its advance signal line 258 when it has read the detection element event data. As shown in FIGURE 2, the signal plocessor 300 is housed on a circuit board that ;llt~ . r;~L~S with the data acquisition co~ ,uL., 400. All co~ llullication b~,lwcc~ the signal processor 300 and the detector 200 occurs through the co.. ~-.. ;c~tion~ links 202 and 203.

Sun~l Processor 300 The signal pl~ce~or 300 ac.luilcs data from the gamma-ray detector 200, norrn~li7Ps and fo----AI~ the data, and stores it in IllLJ~llol~ blocks for access by the data acquisition CO~ uk,, 400. In additio~, the signal p~cei~ol 300 provides the bias voltage for the ~letector 200 and provides the event threshold voltage that is used by the ~e~ction module 206 for fli~ ;..g valid gamma-ray pulses.

FIGURE 8 is a func~onal block diagrarn of the signal processor 300. The sigrlal ~lucessor 300 preferably compri~Ps a field pro?~,A",-"~ble gate aIray (FPGA) 302; a flash analog-to-digital cûn~ (ADC) 304; a fast digital-to-analog converter (DAC) 306 used for ga~n n~rm~li7~tion; a threshold DAC 316 for setting the event threshold voltage; an input/output port 318 for cu~ with the data ~~luisilion col~ul~ l 400; a gated Wo s6/20412 PCT~US95/16911 cc~ er 314; a digital window block 322, having a low port 324 and a high port 326;
a latch 328; a test signal ge~.f ~tol 370; a one-milli~econd clock 372; and a bias voltage supply 254. As described below in more detail, the signal processor 300 also includes random access memory (RAM) which is allocated into several blocks: a gain memoryS block 308, a h~lù~a~ Lu~,LIuly block 310, and a pulse-height distribution memorv block 312 which are named for the type of illfo~Lu~Lion stored therein. As described below in more detail with reference to FIGURE 9, the signal processor 300 also includes two "ping-pong" buffers 346,348, which store addresses used in the "~ d~g mode" of data storage.

10 All commnnir~tion signals and power b~ n the signal processor 300 and the module board are via c~...,...~...;cations links 202 and 203. For exarnple, as shown in FIGURE 8, the linear input line 270 is connecte~l to the linear outputs of all detection modules 206 via analog co.. ".. ;~ ;on~ link 203. The address inputs to the FPGA 302 are provided via address lines 256 and 262; the valid line is coupled to the valid signal line 260; the 15 advance signal is provided over the advance signal line 258; the threshold voltage is l"..l~lll;urA over the threshold signal line 272; the test signals are provided on test signal lines 274; and the bias voltage is provided over the bias signal line 254, all via the analog ~nk 203.

The FPGA 302 allows the fimrhom of the si~al processor 300 to be controllable via 20 sGn~e. Upon initi~l;7~hon~ the data ac~uisiLion co~,~ulcl 400 Ll~ iL~ configuIation inforrnation to the signal processor 300 via the parallel input/output port 318. This configuration information design~tes the mode of data acquisition. For example, the signal processor 300 can configure the FPGA 302 to store event data which exceeds a software controlled threshold voltage in the histogram memory block 310. ~lt.orn~tively, 2S several pulse-height windows can be specified and a St~dtt: histogram can be t~ in the histogram memûry blûck 310 for each window. Additionally, a pulse-height distribution or s~,e~ rece;~red from each detection element 212 can be stored WO 96t20412 PCr/US95/16911 in the pulse-height memory block 312. Each of these modes can be sepA._lely specified upon initiAIi7A~ion of the FPGA 302.

When the valid signal line 260 bf comt~s true, the detection elem~nt address is read from the address lines 256, 262. This address is used to address a ~e~uo. y location COII~A;I~ g 5 the gain n~trrnAli7Ation factor for the cle .\f ~-t This ir.fo. ,--AI;on is l-A--~ir . .~1 to the DAC
306 that outputs a voltage ~lO~OlL onal to the element gain. The voltage output by the DAC 306 is used by the ADC 304 in nt7rTnAIi7in~ and conver~ing the analog signalproduced by the selected proc~ccing chAnn~l and provided on line 270.

The element address is also used to map the pulse-height Amplitlldç into the histogram memory block 310 or, Alt~rnAtely, into the pulse-height distribution memory block 312.
During an initial measul.~ent, the gain nonnAli7Ation factors are set to unity and an isotopic source is used to measure the respollse-s of the individual elementc. These responces are then analyzed by the host col~ er to obtain the gain factors that will be used during imA~ing In this way vAriAnses in elem~nt ~es~ollses are eli~inA~ thus greatly improving image quality. When the event has been acquired, normAIi7~l and stored, an advance signal is gene,aLed on line 258 which Allows the garnma-ray detector 200 to advance to the next detection element that has a valid hit.

As described above, one important function ~ . rv.,.,to~l by the signal processor 300 is ~etection-element-gain nt rTnAIi7,ltion The sig~al processor uses the gain memory block 308 to p~.rO.~. this gain nonnAIi7Ation function. The gain memory block 308 cont~inc a gain normAli7Ation factor for each of the detection elements in the gamma-ray detector 200. In the ~ef. ,l~d embodiment, there are as many as 256 detection modules 206 and sixty-four detection elements 212 per module. Each pulse-height distribution comprises 128 chAnnels with a depth of two bytes. Therefore, in that example, the gain memory block 308 has 2S6x64 x 128 x 2, or 4,194,304 memory byte locations. When an event occurs, the gain memory 308 is addressed and the data is LLa~r~ d to the gain W O96/20412 PCTrUS9S/16911 norm~li7~tiQn DAC 306. This in turn controls the; ~ f~Ous full-scale range of the ADC 304. The output of the ADC 304 is thus "gain nl~lm~li7e~ The ADC "done"
signal 344 causes the data storage operation to proceed.

The gain nonn~li7~tion factors are initialIy obtained by first setting the factors to unity.
5 The signal ~ucessol 300 then accnm~ tes a pulse-height distribution of each ~çtection el~Tnf nt in the pulse-height ~elllol.~ block 312. The pulse-height distnbution is analyzed by the data acquisition co~ ul~i. 400 to obtain the relative gain for each element, a number l,iopollional to this value is stored as a gain no~li7~tion factor for each detection f~lP.,.~ ,I in the gain memory block 308. The gain norrn~li7~hon factors thereby 10 obtained are used to nt~ li7lo the analog signals subsequently received from each detection ~If m~nt 212 during data acqllicition In pulse-height mode, the element addresses and the ADC output are used to address the pulse-height memory block 312 via address lines 340 and output lines 338 in building a pulse-height ~ecchulll of each detection element 212. Thus, each el~m~nt address is 15 ~co~ with a 128-location histogram. The upper seven bits of the ADC specify the "adcllcs~e~" of these 128 loc~tionc Each location in the histog~arn is incrf mentf~d by one when its address appears on the ADC. More than one byte of memory at each location can be spe-ifi~l for improving st~ti~tiç~l accuracy. Thus, the pulse-height memory 312 ~ccl~m~ tes a pulse-height ~c~ llu~ for each of the detection elements 212 in the 20 gamma-ray ~-tecto- 200. This spe ~ Lu can be analyzed by the data ac.luisilion c~ u 400 by ~cf~ g the pulse-height memory 312.

In the image-collection modes, each detection f lf ment address is four bytes of memory deep and is incl~ "f .~tf ~1 by one each time that address is ~l~sP"ted on the address lines and the ADC output is of the proper amplitude. Thus, histograms of the incoming data 25 can be created accoldil~ to gamma-ray energy detecte~1 As shown in FIGURE 8, the addresses and the event ~mplihl~s are ~ d via the address signal lines 340 and 338 to the digital window block 322. The digital window block has a high port 326 and a low port 324. The data ac~lui~ilion col.~ 400 establishes the va~ues provided to these ports by wnting via the colll~ , bus 320 a low and high amplitude value into the low and high ports 324, 326. The output of the ADC 304 is cvm~ed with the value stored in the low and high ports 324, 326. If tbe value on the ~mpli~ldf~ lines 338 falls b~ L~
the low and bigh values stored in the digital window's low and high ports 324, 326, the ~ok~mf~nt address provided on address lines 340 is used to address the histogram memory 310. The value in the histogram memory 310 at the element address is incremente~ by one and ~ at that address.

In "list" mode, each event is "time-tagged." Address inforrnation is combined with the eight bits from the ADC and three bits from a clock and placed in one of a ping-pong memory buffer pair. These buffers are sized to allow eacy data L d.,sr~r at high rates of data acq~lici*on When a buffer fills, data transfer is switched to the other buffer and an i~ttlLU~l is generated which sets up a DMA ~re- of the full buffer to a hard disk optionally coupled to either the data acquisition colllpul~r 400 or the image proc~ossin~
com~ul~ system 450. An output from a port will force flushing of the buffers at the tf "~ ;on of data acql-icition For 256 mo~ s addressable via eight address lines in the gamma-ray detector 200, each image histograrn requires a block of 65,536 bytes of memory (256x64x4). The signal ~locessor employs dual-ported memo~y so that both the FPGA 302 and the data acquisition co.ll~utc~ 400 CPU can access the gain memory simnlt~neously.

Once the memories 310, 312 are written with detection element data, the FPGA 302asserts the advance signal over advance signal line 258 which allows the next event to be L~d on the event address lines 256, 262 and the linear input line 270. As described above with .~,ence to FIGURES 5-7, the detection modules 206 are se~uentially scanned until a module is found having a valid hit. The signaL processor 300 reads the W O 96/20412 PCT~US95/16911 valid hit address and linear data. In the ~rc,.l~d emboriimpnt~ it takes ~.o~alely 2.5 rnic~secol--ls to scan Lh~ugh all of the detçc~i~n modlllçs 206 when there is no valid hit, and it t~kes approxirnately 2 microsecon~ls to process each detector element hit. At a~p~o~;."A~ly 220,000 counts per second, the signal processor 300 will read an average S of one data point per entire scan, and its IIIA~C;III~I.II read rate is a~o~lely 500,000 counts per second.

The imA~in~ system 450 can produce live displays of g~mma-ray pulse-height distributions or histograrns of events which occur between pre-defined pulse-height levels. In addition, the data acquisition cO~ . 400 can pe.ro~ iAgnostic functions based on the data in the memory blocks 310, 312. For example, in a prelim;n~rv ~e~u~ ent, the imager is exposed to a ....; rO. ", field of r~iAtion from the isotope to be used in the imA~ing The data rate is recorded for each element in the system, and the relative count rate in each çlem~nt iS used to obtain a detection efficiency factor for that element. Subsequent analysis of the image employs these factors to correct incidental 15 vA~Ances in el~rnent detection efficiencies.

As shown in FIGURE 8, the signal processor 300 also includes a threshold DAC 316which allows the threshold voltage provided to the detection modules 206 over threshold voltage line 272 to be adjusted under software control. The input to the threshold DAC
316 is provided via the CCil~ul~,- bus 320.

20 In the plefe.l~d embodiment, the signal ~locejsor 300 also includes the blocks shown in FIGURE 9. The signal processor 300 includes two memory address buffers 346, 348, a buffer pointer 350, and a 1-m~ econ~l clock 352. Using the haldw~e shown in FIGURE
9, the signal processor 300 can store address information in the memory address buffers 346, 348, in addition to creating histograms and storing histograrn data in the histo~ram 25 memory block 310 as described above. The address information is stored within the memory address buffers 346,348 together with timing i.~Çul 11 lA~iOn geric._~d by the clock W O 96/20412 PCTrUS95/16911 352. When the first memory buffer 346 becomes full, the addresses are routed by the buffer pointer 350 to the second memory buffer 348. When the first buffer 346 becomes full, the buffer pointer 3SO also g. .1~ .al~s a disk write i~L~luyL signal to the data acquisi-tion computer 400 via the control line 362. As shown in FIGURE 9, tne control line 362 S is coupled with the COLU~Uh~ bus 320. When the buffer pointer asserts the l-lh.~ u~t signal on the control line 362, the data acquisition COulyulc~ 400 begins ~xec~ g a first Luh ~uyL routine to tTansfer the data from the first memory buffer 346 to a data disk (e.g., data storage device 614,FIGURE 1). When the second memory buffer 348 becomes full, the buffer pointer 350 g~on~r~t~oS a second disk write i~ yt which causes the data 10 acquisition COLUYUL~400 to execute a second ~L.~l u~t routine to transfer the data from the second buffer 348 to the data disk. Address infor nation is subsequently loaded into the first buffer 346. This ''~L c;,~,,,;l~g mode" of storage of address and tirning information is controlled by the data acquisition COLuyuLe~ 400 via software ~ g on the CPU.

To synchronize the address and data with the occurrence of ext~rn~l events, the signal 15 processor 300 f~cilit~t~s tagging the event with the address inform~tion stored in the memor,v address buffers 346,348. For example, to s~--c~onize the addresses stored in the memory buffers 346,348 with an event such as a heart colllLacLion~ an input signal from a heart mo~itoring sensor is provided. The logic level input signal is provided over signal line 364. When an ~rn~l event occurs, the signal line 364 is asserted, which 20 causes a special tag to be i~ d within the address data stream input into the buffers 346,348. For elc~rnrl~, an event can cause one of the address bits to be set or cleared and can thus be used as a flag. When the data is processed into time divisions, the tag time events will allow the data to be subdivided into phased time slices. In an alternative embo-iim~nt, memory buffers 346,348 shown in FIGURE 9 can accommodate address, 25 pulse-height data, and timing info.",~tion Such streaming data can then be read back f~om the hard disk and sorted into time bins related to the e~ct~rn~l event flag. Thus it is possible to form a time historv of the contractions of the heart or other l~ LiLive oc"~ nces. /~lL~ l~n~;vGly~ the clock ;nro. I..nl;on can be l~,laced with pulses from an PytPm~l position encoder that wilI aIlow position-d~PpPn-lPnt images to be accnml-l~tpd for tomographic applications.

The DAC 356 works together with the regulator 358 and the DC/DC conv~llG. 360 toprovide a regulated voltage source for the bias voltage 254. The input to the DAC 356 is provided via sonwal~ control over the COl~ bus 320. A fraction of the converter output voltage is used as a co~ya~ison input to a high-gain operational amplifier. The amplifier controls the drive signal to the converter to m~int~in the ope.~Lil g bias at the desired value.

When an event occurs, the address of the detection element 212 which caused the event is used to address the gain memory block 308 via the gain address bus lines 332. In the ill--ctr~ted embodiment, the FPGA 302 combines the module address bus 356 with the ~etect on çlPmPnt address bus 262 to produce the gain address bus 332. As described above, the FPGA 302 treats the module address as the most significant address bits and the element address as the least ciEnifi~nt address bits. When the gain memory block 308 is addressed by the FPGA 302 via the gain address lines 332, the pre-calculated gain nonn~li7~tion factor for the pending detection element 212 is yl~ sellt~d on the gain nn~n~ tion signal lines 334. The pre-stored gain noTTn~li7~tion factor for the pending ~et~Pction ~IPTnPnt 212 is then latched into the gain nor~n~1i7~tion latch 328. In the ~ ted embodiment, the signal processor 300 uses an 8-bit DAC 306 which accepts the 8-bit gain norm~li7~tion factor from the latch 328. When the selected gain norm~li7~tion factor is latched into the latch 328, an analog reference value is produced by the DAC 306 co.l~*,ondiug to the 8-bit gain nonn~li7~tion factor. The gain reference voltage is output on ~fe.~,lce voltage line 336, which is coupled to the flash ADC 304.
- 25 The l~f~ .~;nce output voltage produced by the DAC 306 is used as a lefe.ence to the flash ADC 304. The input voltage to the flash ADC 304 is provided ~om the linear output line 270 of the ~etection module board 208. Because the flash ADC 304 is a ratio-me~ic type W O 96/20412 PCTnUS95/16911 analog-to~igital converter, the output ofthe ADC 304 is l.lo~ollional to the ratio ofthe input signal ~ce;ved on the linear input line 2 î0 and the reference voltage provided by the DAC 306 via ~ef,.~.lce voltage line 336. Thus, the fiash ADC 304 produces a digital le~.cs~ ;on of the ~mplitu(1e of the linear input signal gen~ .~kd by the ~etechon S cl~ .l (which l~ c~;ved the hit) modified by the gain norrn~li7~tion factor stored in the gain memor,v 308 (for that clçtection ele. .~. ~ ~1 212). The ADC 304 therefore produces an 8-bit output on ~mplihl~ie line 338 which is independent of particular gain variations in each ofthe detection elemlontc 212 and v~n~tionc in the corresponding amplification and conditioning ci~;uilry.

The FPGA 302 waits a short time for the gating transient of the latch 328 and the DAC
306 output to settle before issuing a convert signal to the flash ADC 304. The convert signal is provided over convert signal line 342 and causes the flash ADC 304 to gene~ale a digital output on the amplitude line 338. The flash ADC 304 p. .r~l~s the analog-to-digital co~ ,aion in a~lo,~ ly 50 n~n~ secont1c or less, and the total conversion tirne from the assertion of the convert signal on signal line 342 to the gene.d~on of an output on amplitude lines 338 is ~plox;~ ly 300 n~noseconds. The flash ADC 304 asserts an ADC done signal over the signal line 344 to inform the FPGA 302 when the conversion is completP~ When the ADC done signal is asserted on signal line 344, the FPGA 302 asserts the advance signal on advance signal line 258 which frees the active c1etection module 206 to proceed with finding the next pending detection elçment event.
The histogram memory 310 can be llp-l~t~ while the processing of the next detection element event is ini~i~t~

Data Acquisition Co~ ul~, The data acquisition co~h. 400 incln~les h~dwi ~ e and software which coll~ Picate with the signal plocessor 300 and with the image processing co~~ . system 450. The data acquisition computer 400 controls acquisition and processing of data received from the array of detection mo~llles 206, produces irnage data based upon the event data in a format that is co."~ l;ble with f~ nE im~.Ein~ c ~ , c, and l~ -..iL~i tnat data to the irnage ~luCf j~ CO~ JI~ system 450. The data acquisition co.n~ r 400 also provides a m~chani~m for ~ ;"E ~etection element event histograms and pulse-height distri-bution data and can produce images in a standard forrnat to allow the irnages to be S displayed using coll,ule.~;ially available ;m~EinE systems for the image proc~ssinE
CO~u~ L~ 450. For ~yample~, in one plef~ ;d embo~iml~nt~ the data acquisition com~ul~
400 delivers i_age hi~lu~s to an image-processing co~uL.,. over a fast data link. In a second embodiment the relative location of each event and the signal amplitude are rtl to the image proc~os~;nE Colll~Ultl via a parallel link In this later embodiment 10 the image proces~ing cûm~ul~r would assume the task of producing histograms.

Images can be time-tagged at any desired rate that can be resolved by the clock. In one cfc~red embodirnent the data are tagged at a rate of 30 frames per second. Thc.e~ule, if data is collected at ay~lox;..,~tely 300,000 counts per second, each tirne-tagged frame conPins approximately 10,000 data points.

The data ac.l-.isiLion colll,uuL-,. 400, together with the signal processor 300, increases tne llexibility and reduces the cost of the rletector 200 by pc fi~ E detection-element-gain and ~et~ction ~ -f!ffioi~ncy n-~n,.li~ation functions. This benefit results from less stringent le~ue..lc~hL~ on the quality of the detection el~m~nt~ and from elimina*ng the need for rl l~t~ hiilg the gainc ofthe detection ~1~ . .f .~plification/peak~ietpction strings.

20 The data acquisition co~l~utl . 400 analyzes the relative ef~iciency of each detection element 212 and pc.rolms a no~.~nali7~tion function on the received data to ensure that a u~lirullll radiation exposure produces an image having a ullirUllll hltf;~ily (i.e., equally irradiated detection elements produce the same shade of gray for every pixel). Thus, after initializa*on, the signal processor 300 and data acquisition colll~u~ 400 ensure that, 25 when equally i~ liatf~l, each detection element 212 produces an identically displayed ~sponae which is independent ofthe actual lc;a~Jonâe produced by the detection element W O96/20412 PCTrUS95/16911 212. This nonnAIi7Ation feature reduces the costs associated with producing detect on Pk .,~ i 212 and detection modules 206 having !~..;fc.~ c~.~OLISc and gain çhA.~ , ;e-tics. This feature eI;III;IIA~S the need to adjust the gains of each detection element 212 and its Associ~rd AmrlifirAtion and signal conditioning Cucuilly. This feature also 5 allows i~loved energy r~sollltion of each detection el~ .t 212 and irnproved rejection of Compton-scALl~,ed events. It also improves the long term stability of the imAging system. These fc~Lu cs are achieved without a cignifis~nt reduction of data throughput:
total count rates of 500,000 counts per second can be processed by the present data acquisition co u~uk,- 400.

rhe signal processor 300 and data acquisitiosl col~uLcl 400 also provide increased flexibility by allowing fimrtione to be changed under software control, thereby avoiding costly board redesigne when a~litionAl functionality is required or desired.

Tm~e Proce~ein~ Co~ ,ul~ l SysteTn The image processing co~ UL~ system 450 provides an intrrf~re with the o~ Lor, 15 governs data acquisition modes, lec~ cs image data from the data acquisition col~yuL~.
400, displays images in real tirne on the display 604, and co.~ ..ic~tes with display and readout devices. It also provides a facility for adjustiIlg operational pa~..ct~rs~ such as, the gamma-ray energy bounds and calibration PA.AIII~ t. .s used by the system. The co~ irAt on with the data acquisition COLU~lL~,- 400 is via a standard i"l~. rAce such 20 as Fth~.ot or SCSI-2 using a data protocol plcrt:~Lcd by the particular image procee~ing computer system 450 being used. The image plOCeaaLIlg CoLupuLt~L system provides image display, rotation, slicing, region-of-interest highligh~in~, etc. under o~ Lol control.

As shown in FIGURE 2, the image proces~;-,g coll~uLc,. system 450 can also display images on any of the other display devices coupled to it. This system includes both 25 software and hardw~e to control the input and output devices shown in FIGURE 2.

Thus, a nuclear mr~irin~ im~ging system has been described wherein the im~gin~ system includes an im~ ing head 200, signal processor 300, and a data acquisition colll~uh.~ 400.
The im~in~ head inr~ çs an array of closely-packed ~etection morl-lles Each ~etection module comprices an array of semiconductor detection elements mounted to a circuit S carrier, wL~.~in the circuit carrier inrlu~s cil~.uiLl.y to condition and process the signals gellc.ated by the detection elements and to prepare the processed signals for further proceccing by the signal processor. The im~ing system form~ tes images based upon the processed signals and displays the formulated images on a display. The detection modules preferably comprise cadmium-~nc-telluride material. The address of each 10 detection module and element is provided to the signal processor when the cletection element absorbs a gam~na ray of energy greater that a threshold controlled by the signal processor (a valid hit). The detection modules employ a fall-through scheme to ~lltom~tir~lly read only those detection çlc "~ , in sequence, that have l~ceived a valid hit and to produce the address of those elements and the m~anit~lde of the absorbed 15 photon. The signal processorp. (;J".~C rli~gnostics~ gain nnrm~li7~tion, r~JlJonse efficien-cy norm~li7~tion, and data acquisition functions. The im~gin~ system displays images based upon the signals g- ll. ,dled by the detection elementc.

A number of embo~; . "~ of the present invention have been described. Nevertheless, it will be understood that various mo~lifir~tions may be made without departing from the 20 spirit and scope of the invention. For example, other buttable shapes could be used for the detection modules 206, such as triangular, rectangular or hexagonal. Similarly, the detection elementc 212 could have other shapes besides square. Also, as described above, the two analog ASICs of each detection module can be combined into a single ASIC.
Sirnilarly, both the digital and analog functions can be irnplernentP~ using one ASIC. In 25 addition, the method of gain norrn~li7~tion could be pc ~r~lllled completely in software after the analog values are converted to digital. Accordingly, it is to be understood that the invention is not to be limited by the specific illustrated embo~1imentc~ but only by the scope of the appended claims.

Claims (79)

1. A nuclear imaging system, comprising:
a. a radiation guide structure comprising one of a collimator or pinhole; and b. an imaging detector positioned proximate the radiation guide structure, comprising:
(1) a plurality of detection modules, each having an exposure surface, a surfaceopposite the exposure surface, and a plurality of sides, the exposure surface being substantially covered with radiation detecting material, wherein each detection module is buttable on all sides with adjacent detection modules such that the imaging detector has substantially no dead regions between butted detection modules, and wherein each detection module further includes a plurality of semiconductor detection elements for producing electrical pulses having an amplitude indicative of the energy of radiation form high-energy photons impinging on the exposure surface, and (2) a conditioning circuit, operatively coupled to the detection elements, for conditioning the pulses, wherein the conditioning circuit provides low-noise amplification of the pulses.
2. The imaging system of claim 1, wherein the conditioning circuit further provides shaping of the pulses.
3. The imaging system of claim 2, wherein the imaging detector further comprises an event processor, operatively coupled to the conditioning circuit, for processing the pulses, wherein the event processor:
a. identifies valid events using amplitude discrimination; and b. generates event-addresses corresponding to valid events.
4. The imaging system of claim 3, wherein the event processor stores a voltage representative of the magnitude of incident-photon energy.
5. The imaging system of claim 3, further comprising:
a. a data processor, wherein the data processor responds to a valid event by:
(1) storing the address corresponding to the valid event;
(2) deriving a normalized event amplitude; and (3) storing the event in a selected memory bank.
6. The imaging system of claim 5, further comprising a computer imaging system, coupled to the data processor, wherein the computer imaging system accesses the data stored in the selected memory bank and controls the mode of imaging data, and wherein the computer imaging system formats the data into images and displays the images on display media.
7. The imaging system of claim 1, wherein the detection modules are configured in a non-rectangular shape.
8. The imaging system of claim 1, wherein the detection modules are configured to conform to a non-planar surface such as a head or breast.
9. The imaging system of claim 1, wherein the detection elements comprise at least one semiconductor wafer partitioned to form an array of detection elements.
10. The imaging system of claim 9, wherein a plurality of semiconductor wafers are tiled together.
11. The imaging system of claim 9, wherein each semiconductor wafer includes an electrode coupled to a side of the wafer which is exposed to high-energy photons and wherein each semiconductor wafer also includes an array of electrodes coupled to the opposite side of the wafer.
12. The imaging system of claim 11, wherein the semiconductor comprises cadmium-zinc-telluride (CZT) and the electrodes comprise a metal, and wherein the electrodes are deposited in a thin layer on the CZT wafer, and wherein a portion of the CZT wafer which is not covered by electrode metal is covered by a passivating layer formed upon the surface.
13. The imaging system of claim 12, wherein the passivating layer is formed by soaking the CZT wafer in an aqueous solution of hydrogen peroxide and baking the CZT wafer in air.
14. The imaging system of claim 12, wherein the passivating layer is formed by soaking the CZT wafer in a 3% by weight aqueous solution of hydrogen peroxide at a temperature of 60C C and baking the CZT wafer at 60° C in air for approximately 30 minutes.
15. The imaging system of claim 9, wherein the array of detection elements is an 8x8 square array.
16. The imaging system of claim 15, wherein the array of detection elements has an outside dimension of about 1 square inch.
17. The imaging system of claim 1, wherein the detection elements comprise at least one CZT
crystal tiled together, wherein the CZT crystals are patterned with areas of conductor which define separate detection elements, and wherein the conductor areas are separated by areas of passivation, and wherein the passivation areas are formed by treating areas between the conductor areas with a hydrogen peroxide solution.
18. The imaging system of claim 1, wherein the high-energy photons range from approximately 5 keV to 10 MeV.
19. The imaging system of claim 1, wherein the event processor comprises analog and digital integrated circuits.
20. The imaging system of claim 3, wherein the event processor comprises a peak detection circuit and a comparison circuit, and wherein the conditioning circuit is coupled to both the peak detection circuit and the comparison circuit, and wherein the event processor further comprises a plurality of latches coupled to the comparison circuit, and wherein the comparison circuit compares the amplitude of detection element pulses with a reference value, and wherein the comparison circuit sets a selected latch based upon the comparison.
21. The imaging system of claim 20, wherein the event processor utilizes a fall through method of processing the set latches, and wherein all of the set latches are read in a predetermined sequence.
22. The imaging system of claim 1, wherein a plurality of resistors and capacitors is operatively coupled between the detection elements and the conditioning circuit.
23. The imaging system of claim 22, wherein the resistors and capacitors utilize thin-film technology.
24. The imaging system of claim 22, wherein the resistors and capacitors utilize thin-film technology.
25. The imaging system of claim 12, wherein the detection modules further include a circuit carrier having a plurality of interconnections which couple the CZT wafer to theconditioning circuit.
26. The imaging system of claim 25, wherein the circuit carrier is a pin grid array.
27. The imaging system of claim 1, wherein the detection modules further include a circuit carrier, and wherein the material of the carrier has a thermal coefficient of expansion substantially equal to the coefficient of expansion of CZT.
28. The imaging system of claim l, wherein the imaging system is used to detect radiation emitted by a biological system or organ.
29. The imaging system of claim 28, wherein the imaging system is used for single-photon emission computed tomographic (SPECT) applications.
30. The imaging system of claim 9, wherein each semiconductor wafer is partitioned to form a first and a second set of parallel strips, wherein the first set of strips are positioned upon the exposure surface of the detection module, the second set of strips are positioned upon the surface opposite the exposure surface of the detection module, and the second set of strips are orthogonal to the first set of strips.
31. The imaging system of claim 30, wherein the detection elements are formed at the intersection of the first and second sets of orthogonal strips.
32. The imaging system of claim 74, wherein the detection elements comprise at least one semiconductor wafer partitioned to form an nxm array of detection elements.
33. The imaging system of claim 32, wherein a plurality of semiconductor wafers are tiled together.
34. The imaging system of claim 32, wherein each semiconductor wafer is partitioned to form a first and a second set of parallel strips, wherein the first set of strips are positioned upon the exposure surface of the detection module, the second set of strips are positioned upon the surface opposite the exposure surface of the detection module, and the second set of strips are orthogonal to the first set of strips.
35. The imaging system of claim 34, wherein the detection elements are formed at the intersection of the first and second sets of orthogonal strips.
36. The imaging system of claim 32, wherein each semiconductor wafer includes an electrode coupled to a side of the wafer which is exposed to high-energy photons and wherein each semiconductor wafer also includes an array of electrodes coupled to the opposite side of the wafer.
37. The imaging system of claim 36, wherein each semiconductor comprises cadmium-zinc-telluride (CZT) and the electrodes comprise a metal, and wherein the electrodes are deposited in a thin layer on the CZT wafer, and wherein a portion of the CZT wafer which is not covered by electrode metal is covered by a passivating oxide layer formed upon the surface.
38. The imaging system of claim 37, wherein the passivating oxide layer is formed by soaking the CZT wafer in an aqueous solution of hydrogen peroxide and baking the CZT wafer in air.
39. The imaging system of claim 37, wherein the passivating oxide layer is formed by soaking the CZT wafer in a 3% by weight aqueous solution of hydrogen peroxide at a temperature of 60° C and baking the CZT wafer at 60° C in air for 30 minutes.
40. The imaging system of claim 32, wherein the array of detection elements is an 8x8 square array.
41. The imaging system of claim 40, wherein the array of detection elements has an outside dimension of about 1 square inch.
42. a. A detection module comprising:
b. a semiconductor radiation detector having a top surface and a bottom surface,wherein the bottom surface is patterned into a plurality of detection elements defined by patterning selected portions of the surface with areas of conductor, and wherein each detection element produces an electrically-charged detection element pulse indicative of the magnitude of radiation received by each element, and wherein the detection element pulse is transmitted to an electrode coupled to the bottom surface of each element; and c. an electronic circuit carrier mechanically coupled to the detector, wherein the carrier contains circuits for processing the detection-element pulses, and wherein the circuits include at least one channel for conditioning and processing the detection-element pulses coupled to each detection element.
43. The detection module of claim 42, further comprising a circuit board, mounted between the detector and the carrier, wherein the circuit board couples the electrode from the bottom surface of each element to a conditioning and processing channel for each element.
44. The detection module of claim 42, further comprising a substantially thin plate mounted to and electrically coupled to the top surface of the detector.
45. The detection module of claim 42, further comprising a substantially thin plate mounted to the bottom surface of the detector.
46. The detection module of claims 44 and 45, wherein the plates comprise ceramic.
47. The detection module of claim 46, wherein the plates are less than 0.025 inch thick.
48. The detection module of claim 42, wherein the channel amplifies, conditions and processes the detection-element pulses, and wherein the conditioning and processing channel stores an amplitude and an address of the detection-element pulses which exceed a reference threshold.
49. The detection module of claim 48, wherein the channel transmits the stored amplitude and address when enabled by a fall-through means, and wherein the fall-through means enables the channel after processing an upstream channel.
50. The detection module of claim 48, wherein the conditioning and processing channel further includes leakage current compensation means, and wherein the compensation means compensates for substantially large and variable leakage currents generated by the detection elements.
51. A detection module comprising:
a. a semiconductor radiation detector having a top surface and a bottom surface, wherein the bottom surface is patterned into a plurality of detection elements, and wherein each detection element produces pulses indicative of the energy of an absorbed photon of radiation received by each element, and wherein the detection-element pulses are transmitted to an electrode coupled to the bottom surface of each element; and b. an electronic circuit carrier mechanically coupled to the detector, wherein the carrier contains electronic circuits for processing the detection-element pulses, and wherein the circuits include at least one processing channel for each detection element, and wherein the processing channel produces a flag whenever a detection-element pulse exceeds a reference threshold.
52. An electronic circuit for processing pulses received from a plurality of gamma-ray detection elements, comprising:
a. a plurality of analog channels each corresponding to a unique one of the detection elements, wherein each analog channel is coupled to the corresponding element, and wherein each analog channel amplifies, shapes, and integrates the pulses produced by the corresponding detection element;
b. a plurality of digital channels each corresponding to a unique one of the analog channels, wherein each digital channel is coupled to the corresponding analog channel, and wherein the digital channel compares the amplitude of the amplifiedpulses produced by the corresponding detection element with a threshold, and wherein the digital channel latches the result of the comparison and wherein thedigital channel provides the address of the corresponding detection element and the corresponding pulse amplitude for access by an imaging system.
53. The circuit of claim 52, wherein the electronic circuit comprises an integrated circuit.
54. The circuit of claim 52, wherein the analog and digital channels are physically separated to improve noise immunity and reduce cross-talk.
55. A semiconductor detector patterned with an array of conductor areas fonning an array of detection elements, wherein the semiconductor comprises CZT and conductor areas are passivated, such passivation is provided by treating the areas between the conductor areas with a solution of hydrogen peroxide.
56. A nuclear medicine imaging system for imaging radiation emitted by an object under test, comprising:
a. an imaging head comprised of a plurality of detection modules, each having anexposure surface, a surface opposite the exposure surface, and a plurality of sides, the exposure surface being substantially covered with radiation detecting material, wherein each detection module is buttable on all sides with adjacent detection modules such that the imaging detector has substantially no dead regions betweenbutted detection modules, and wherein each detection module further includes a plurality of semiconductor detection elements for producing electrical pulses indicative of the energy of radiation from high-energy photons impinging on the exposure surface, b. an event processor, mounted within the detection modules, for processing the pulses, wherein the event processor flags events corresponding to each detection element that produces a pulse exceeding a predetermined threshold;
c. a data processor, coupled to the event processor, for successively reading the flagged events; and d. a computer imaging system, coupled to the data processor, wherein the imagingsystem accesses the data processor to read the successive flagged events, and wherein the imaging system formats the pulses of the detection elements corresponding to the flagged events into images and displays the images on a display.
57. A camera for imaging radiation emitted by an object under test, comprising:
a. an imaging head comprised of a plurality of detection modules, wherein the detection modules are butted against one another in an array such that the imaging head has substantially no dead regions between butted detection modules, and wherein the detection modules include a plurality of semiconductor detection elements, and wherein the detection elements produce pulses indicative of the energy of high-energy radiation absorbed by the detection elements; and b. a processor, mounted within the detection modules, for processing the pulses,wherein the processor amplifies, conditions and processes the pulses, and wherein the processor stores processed pulses which exceed a threshold.
58. A fall-through event system for selecting events generated by a plurality of signal conditioning and processing channels, each channel coupled to a corresponding detection element, each channel conditioning and processing electrical pulses produced by the corresponding detection element, and each channel producing a valid event whenever the corresponding detection element produces a pulse exceeding a predeterrnined threshold, comprising:
a. means for scanning the channels, wherein the scanning means scans each channel in a predetermined sequence until finding a valid event, and, upon finding a valid event, enables the channel containing the valid event and awaits receipt of an advance signal before continuing to scan subsequent channels in the sequence.
59. The fall-through event system of claim 58, wherein each channel independently conditions and processes the electrical pulses produced by the corresponding detection element.
60. The fall-through event system of claim 58, wherein each channel receives the electrical pulses produced by the corresponding detection element at random times.
61. The fall-through event system of claim 58, wherein each channel produces a valid event based upon the amplitude of the electrical pulses produced by the corresponding detection element.
62. The fall-through event system of claim 58, wherein each channel stores the amplitude of the electrical pulses which exceed a predetermined threshold.
63. The fall-through event system of claim 62, wherein the channel enabled by the reading means generates a valid signal, outputs an address associated with the enabled channel, and outputs the amplitude stored by the enabled channel.
64. The fall-through event system of claim 63, wherein, upon receipt of the advance signal, the enabled channel ceases to output the valid signal, the associated address, and the amplitude, and wherein the enabled channel resets the amplitude stored by the enabled channel.
65. The fall-through event system of claim 63, wherein the enabled channel generates a digital representation of the amplitude stored by the enabled channel.
66. A signal processor for processing signals generated by a plurality of conditioning and processing channels, each channel operatively coupled to a corresponding detection element which produces electrical pulses indicative of the magnitllde of radiation absorbed by the detection element, each channel storing an amplitude of the electrical pulse exceeding a predetermined threshold, and each channel generating an event whenever the electrical pulse exceeds a predetermined threshold, comprising:
a. a means for sampling a stored amplitude of a channel generating an event;
b. means, operatively coupled with the sampling means, for normalizing gain introduced by the channel and the corresponding detection element, wherein the normalization means normalizes the sampled amplitude; and c. means, coupled with the normaization means, for storing the normalized amplitude.
67. The signal processor of claim 66, wherein each detection element has a unique address, and wherein each channel generating an event transmits an address of the corresponding detection element to the signal processor, and wherein the signal processor further includes means, coupled to the sampling means, for reading the transmitted address.
68. The signal processor of claim 67, wherein the signal processor generates an advance signal after storing the normalized amplitude.
69. The signal processor of claim 67, wherein the signal processor further includes means, coupled to the sampling means, for tagging the transmitted address and normalized amplitude with a time-tag, and wherein the address, amplitude and time tag are stored together on a storage device coupled to the signal processor.
70. The signal processor of claim 69, wherein the addresses, amplitudes and time tags stored on the storage device are sorted into time bins related to an external event flag.
71. The signal processor of claim 66, wherein the normalization means includes:
a. an analog-to-digital converter having a reference input and an analog input, wherein the analog input is coupled to the sampled amplitude; and b. means, coupled to the reference input, for storing a plurality of gain normalization factors, wherein each detection element has a corresponding pre-stored gain normalization factor, and wherein the storage means outputs a gain normalizationfactor of the detection element coupled to the channel generating the event to the reference input thereby causing the analog-to-digital converter to produce a normalized signal.
72. A method of nonmalizing signals generated by a plurality of conditioning and processing channels and a plurality of detection elements, each detection element producing electrical pulses indicative of the magnitude of radiation absorbed by the detection element, each channel operatively coupled to a unique one of the detection elements, comprising the steps of:
a. exposing the detection elements to mono-energetic photons;
b. generating a map of the amplitude of the pulses produced by each detection element;
c. normalizing the electrical signals produced by the channels based upon the amplitude map.
73. A method of normalizing electrical pulses generated by a plurality of detection elements, the electrical pulses indicative of the magnitude of radiation absorbed by the detection elements, comprising the steps of:
a. exposing the detection elements to a uniform radiation field;
b. generating a map of the efficiency of each detection element; and c. normalizing the electrical pulses produced by each detection element based upon the efficiency map.
74. An imaging system for obtaining an image of the location and intensity of radiation emitted by a source, comprising an imaging detector for sensing energy and position-of-incidence of radiation, comprising a plurality of detection modules, each having an exposure surface, a surface opposite the exposure surface, and a plurality of sides, the exposure surface being substantially covered with radiation detecting material, wherein the detection modules are configurable in an NxM array, and wherein each detection module is buttable on all sides with adjacent detection modules such that the imaging detector has substantially no dead regions between butted detection modules, and wherein each detection module further includes a plurality of semiconductor detection elements for producing electrical pulses indicative of the energy of radiation from high-energy photons impinging on the exposure surface.
75. The imaging system of claim 74, further including a support structure that provides me-chanical support, shielding from electrical noise, shielding from stray-photon radiation, and electrical interconnection for the detection modules.
76. The imaging system of claim 74, further including a conditioning circuit for processing a photon event, wherein the conditioning circuit is operatively coupled to the detection elements, and wherein the conditioning circuit provides low-noise amplification and shaping of the pulses produced by the detection elements.
77. The imaging system of claim 76, further including an event processor, operatively coupled to the conditioning circuit, for processing the conditioned photon events, wherein the event processor:
a. identifies valid events using amplitude discrimination; and b. generates event-addresses corresponding to valid events.
78. The imaging system of claim 77, wherein the event processor further stores a voltage representation of the magnitude of each incident-photon energy.
79. The imaging system of claim 77, further including a data processor, operatively coupled to the event processor, wherein the data processor responds to a valid event by:a. storing the event address of the valid event;
b. deriving a normalized event amplitude; and c. storing the event in a selected memory bank.
CA002208576A 1994-12-23 1995-12-21 Semiconductor gamma-ray camera and medical imaging system Abandoned CA2208576A1 (en)

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