|Publication number||US20050213627 A1|
|Application number||US 11/061,726|
|Publication date||Sep 29, 2005|
|Filing date||Feb 22, 2005|
|Priority date||Feb 20, 2004|
|Also published as||DE102004009531A1, DE102004009531B4, US7848376, US20090034570|
|Publication number||061726, 11061726, US 2005/0213627 A1, US 2005/213627 A1, US 20050213627 A1, US 20050213627A1, US 2005213627 A1, US 2005213627A1, US-A1-20050213627, US-A1-2005213627, US2005/0213627A1, US2005/213627A1, US20050213627 A1, US20050213627A1, US2005213627 A1, US2005213627A1|
|Inventors||William Masselink, Sebastian Dressler, Mykhaylo Semtsiv, Nikolai Georgiev, Manfred Helm, Thomas Dekorsy, Mathias Ziegler|
|Original Assignee||Humboldt-Universtaet Zu Berlin, Forschungszentrum Rossendorf E.V.|
|Export Citation||BiBTeX, EndNote, RefMan|
|Patent Citations (4), Referenced by (28), Classifications (13), Legal Events (1)|
|External Links: USPTO, USPTO Assignment, Espacenet|
The present invention relates to a quantum cascade laser structure, especially a quantum cascade laser structure that enables the production of quantum cascade lasers on the basis of intersubband transitions which can emit laser radiation with a wavelength of about 4 μm at room temperature (approx. 300 K). The invention furthermore relates to a quantum cascade laser (QCL).
The presence and the concentration of a number of molecules, such as CO2, can be detected by measuring the absorption of infrared radiation with wavelength of approx. 4 μm. Furthermore, the atmosphere is permeable for radiation in a wave length spectrum of 2.9 μm to 5.3 μm. In particular it is possible to detect and define the concentration of a number of air-polluting gases, industrial chemicals, and biological emission relevant for medical diagnoses in this way. However, measuring the absorption spectra requires intensive sources of radiation, such as a laser emitting in the suitable wave length spectrum, as well as suitable detectors.
There are several classes of lasers that are capable of emitting radiation in the appropriate wavelength spectrum. A first class of lasers is the so-called lead-salt lasers, which, however, require cooling to a low temperature in their operation. A second class is the so-called antimonide diode laser, which also require cooling to a low temperature, and for which it has not been proven to date that they can emit radiation in the wave length spectrum around approximately 4 μm. A third class of lasers is the so-called “Class-B lasers” such as OPOs (Optic Parametric Oscillator) and DFG laser (Difference Frequency Generation Laser), which are both based on a frequency conversion of laser radiation emitted in the near infrared range by means of non-linear generation of difference energies. However, the optical components required in Class B lasers require a much higher effort and are more expensive than the optical components of lasers that emit the laser radiation directly in the suitable wave length spectrum.
An attractive alternative to the aforementioned lasers is the quantum cascade laser. A quantum cascade laser (QCL) comprises as a core component a number of so-called cascades, each of which has a number of quantum wells and a number of barrier layers, which are arranged alternately and are comprised of semiconductor materials. Typically, a quantum cascade laser comprises approximately 20 to 100 of these cascades. The principle structure of a quantum cascade laser is described, for example, in the article by J. Faist et al., Science, Vol. 264, 22 April 1994. An overview of various approaches for quantum cascade lasers is found in J. Faist et al., IEEE Journal of Quantum Electronics, Vol. 38, No. 6, July 2002.
For a better comprehension of the structure and the mode of operation of quantum cascade lasers, some of the properties of semiconductor materials are described briefly in the following.
The electrical behavior of a semiconductor material can be described with the so-called band model, which states that various energy ranges, the so-called energy bands, are available to the electrons of the semiconductor material, and that the electrons of the semiconductor material can essentially take on any energy value within said energy bands. Various bands may be separated from one another by a band gap, i.e., an energy band with energy values the electrons cannot possess. If an electron changes from a higher energy band to an energy band in a lower energy range, energy corresponding to the difference of the energy values of the electron before and after the change, which is also called “transition”, is released. The energy difference can be released in form of photons. The band with the highest energy level, which is fully filled with electrons at a temperature of 0 Kelvin, i.e., the so-called valence band, and the conduction band that is energetically above the valence band, which is unfilled at 0 Kelvin, as well as the band gap between them are of special significance for a semiconductor material.
In the cascades of quantum cascade lasers, the semiconductor materials for the barrier layers and the quantum wells are selected such that the lower conduction band edge of the barrier material lies higher in energy than the lower conduction band edge of the quantum well material. The lower conduction band edge represents the lowest energy value that an electron can assume within the conduction band. The energy difference between the energy of the lower conduction band edge of the barrier material and the lower conduction band edge of the quantum well material is also called the conduction band discontinuity. As a result of this selection, the electrons of the quantum wells cannot readily penetrate the barrier layers and are therefore enclosed in the quantum wells. The can only “tunnel” through a barrier layer into an adjacent quantum well in a quantum-mechanical process, with the probability of the occurrence of a tunneling process depending on the height of the conduction band discontinuity and the thickness of the barrier layer between the two quantum wells.
In the quantum well, the behavior of the electrons enclosed in said well are determined by quantum mechanics effects due to the small thickness of the layer (only a few nanometers). An essential effect is that the electrons in an energy band of the quantum well can no longer assume any energy value within the energy range of the band, but rather are confined to the energy values of specific energy levels, i.e., so-called sub-bands. The energetic differences between the individual sub-bands are particularly high if the quantum well is very thin and the conduction band discontinuity is high. The electron energy does not change continuously, but rather jumps from one sub-band to the next. The electron can change from one energy level to the other energy level only if the energy increase or the energy decrease suffered by an electron corresponds precisely to the difference of the energy values of two sub-bands. Transitions from one energy level to another energy level within one and the same band are called intersubband transitions. In the cascades of the quantum cascade laser, the emission of laser radiation occurs at these intersubband transitions.
J. Faist et al., IEEE Journal of Quantum Electronics, Vol. 38, No. 6, July 2002, describes a quantum cascade laser that can emit laser radiation with a wave length of 5.3 μm at room temperature. The cascades of the quantum cascade laser described in the aforementioned article are applied to an InP (indium phosphide) substrate. Its quantum wells are comprised of In0.6Ga0.4As (indium-gallium-arsenide with 60% indium and 40% gallium) and its barrier layers are comprised of In0,44Al0,56As (indium-aluminum-arsenide with 44% indium and 56% gallium). Because of the ratio between the indium and gallium composition in the quantum wells and/or the ratios between the indium and aluminum composition in the barrier layers, the materials of said layers, all of which have a crystalline structure, have other lattice constants than the InP substrate (the lattice constant can be considered as a measure of how far the atoms in a crystalline material, where atoms are essentially arranged at the junctions of an intended lattice, are distanced from one another). When preparing a layer structure for the cascades of the quantum cascade laser, the layers will adapt to InP substrate, taking on its planar constant in the plane parallel to the surface, which leads to strain due to the different lattice constants. Thus, the adaptation can be maintained only up to a specific critical thickness of the layer structure if the strain is not compensated. To compensate for the strain created in the layers within one cascade, the parts of the constituents in the In0,6Ga0,4As quantum wells are selected so that compression strain is created in said layers, whereas the parts of the constituents in the In0,44Al0,56As barrier layers are selected so that tensile strain is created in said layers. Furthermore, the thicknesses of the individual layers are coordinated with respect to one another so that the compression- and the tensile strains are largely compensated within a cascade (so-called strain compensation).
Although it was possible to emit laser radiation in a wave length spectrum of 3.5 to 100 μm with intersubband transitions in quantum cascade lasers, it was not possible to date to achieve an emission of radiation in the wave length spectrum below 4.6 μm at room temperature.
The problem to be solved by the present invention is to provide a quantum cascade laser structure with intersubband transitions that allow the production of quantum cascade lasers which can emit radiation in the wave length spectrum of 2.9-5.3 μm, especially in a spectrum of 3.1 to 4.6 μm, at room temperature, i.e., at approximately 300 K.
Another object to be attained by the invention is to provide an improved quantum cascade laser.
The first object of the invention is attained with a quantum cascade laser structure in accordance with claim 1 and the second object is attained with a quantum cascade laser in accordance with claim 15. The dependent claims include advantageous modifications of the invention.
The quantum cascade laser structure in accordance with the invention comprises a number of cascades, i.e., at least two cascades and preferably 20 to 50 cascades, each of which comprise a number of alternately arranged quantum wells and barrier layers. The material of at least one quantum well as well as the material of at least one barrier layer are under mechanical strain, with the respective strains in particular may being tensile strains or compression strains. The quantum wells and barrier layers are coordinated such in the quantum cascade laser structure in accordance with the invention that any strain is largely compensated within one cascade. Largely compensated should be understood to mean that the compensation does not necessarily need to be complete, but only to such an extent that there is no strain that would make pseudo-morphological growth impossible. One skilled in the art understands pseudo-morphological growth to be a growth where an adsorbed crystalline layer having a different crystalline structure and/or a different lattice constant than the substrate accepts the crystalline structure and the lattice constant of the substrate. In the quantum cascade laser structure in accordance with the invention, the material of the quantum wells has only one respective constituent material and the material of at least one of the barrier layers has at least two constituents materials, with the two constituent materials may having different constituents or the same constituents in various quantity ratios. The constituent materials of a layer may comprise, for example, the elements Al (aluminum), Ga (gallium), As (Arsenic) or In (Indium) as constituents. In the following, the term constituent material is used for materials having only one constituent material synonymously for the material of the respective layers.
Compared to the quantum cascade laser structures with strain compensation, as described in the state of the art, the quantum cascade laser structure in accordance with the invention is more flexible in the adjustment of the band structure, the so-called “band structure engineering.” Important parameters in the engineering of the band structure are the size of the conduction band discontinuity, the thickness of the quantum wells and the probability of an electron penetrating the barrier layer, i.e., the so-called tunnel probability. In the strain-compensated quantum cascade laser structures in accordance with the state of the art, the size of the conduction band discontinuity depends on the relative ratios of the constituents in the constituent materials used in the barrier layers and quantum wells. The tunnel probability, however, depends on the size of the conduction band discontinuity, i.e., the relative compositions of the constituents, as well as on the thickness of the barriers. Thus, for the band structure engineering, there are only two largely independently variable parameters available in the strain-compensated quantum cascade laser structures in accordance with the state of the art for engineering the barrier thickness, the conduction band discontinuity and the tunnel probability. If, for example, the relative ratios of the constituents in the constituent materials are used to engineer the conduction band discontinuity, and the thickness of the layers is then adapted for strain compensation, this also already determines the tunnel probability. In particular, it is not possible to simultaneously maximize the conduction band discontinuity and realize a good strain compensation because the tunnel probability is an important parameter for the laser process, i.e., for the emission of the laser radiation.
Furthermore, the quantum cascade laser structure in accordance with the invention also offers the composition of at least one barrier layer with two constituent materials as a variable parameter. For example, it is possible to select one of the constituent materials of said barrier layer such that the size of the conduction band discontinuity is engineered to a desired value—for example maximized—whereas the barrier thickness is selected such that the tunnel probability reaches the desired value for the engineered value of the conduction band discontinuity. The relative ratios of the constituents in the second constituent material of the barrier layer can then be selected so that the strain is compensated by the already determined barrier thickness.
To realize strain compensation, it is in particular possible to select the relative ratio between the constituents of the constituent material and/or the thickness of at least one of the quantum wells such that the strain in at least one of the barrier layers is compensated by a strain in the essentially same amount as the strain of at least one barrier layer, but with an inverted sign.
In the quantum cascade laser structure in accordance with the invention, the cascade may comprise an injection zone, a extraction zone and an active zone arranged in-between said zones, where the actual emission of the laser radiation occurs, with each zone comprising at least one barrier layer and at least one of the barrier layers in the active zone and/or the injection zone comprising at least two constituent materials. If said barrier layer is the barrier layer of the active zone adjacent to the injection zone, i.e., the so-called injection barrier, quantum cascade lasers can be realized by appropriately engineering the thickness of the injection barrier and thus also the tunnel probability through the injection barrier, and said quantum cascade lasers can be operated optionally so as to emit laser radiation with multiple wave lengths (multiple wave length emission) or laser radiation with only one wave length (single wave length emission).
In the quantum cascade laser structure in accordance with the invention, not all barrier layers must comprise at least two constituent materials to achieve the aforementioned advantages. In one realization, the material of at least one of the barrier layers therefore has only one constituent material. In a modification of said realization, the constituent material of the barrier layers comprising only one constituent material is selected such that the conduction band discontinuity is maximized in the cascade. A large conduction band discontinuity is in particular advantageous if the laser is intended for use at room temperature.
The thicknesses and the constituents of the constituent materials of the quantum wells and the barrier layers as well as the composition of the material of at least one barrier layer having at least two constituent materials may be selected such in the quantum cascade laser structure in accordance with the invention that the laser wave length spectrum is 2.9 to 5.3 μm, preferably 3.5 to 4.5 μm, and in particular 3.7 to 4.2 μm. In addition to the detection of molecules, said wave length spectrum is also of significance for the transmission of communication, for collision monitoring radar systems, for automated steering systems, for medical diagnosis, for the target acquisition in the military as well as in the civilian area, and for the dazzling of infrared detectors and infrared cameras. With the proper selection of the temperature at which it is operated and/or the strength of the current flowing through the laser, the quantum cascade laser in accordance with the invention in particular facilitates the variation of the emission wave length within the stated range. A so-called external cavity or a different tuning strategy can also be used to engineer the wave length.
The following constituent materials, which include Al, As, Ga and In as constituents, are especially suitable for use in the quantum cascade laser structure in accordance with the invention:
The constituent materials need not necessarily be present in pure form. Rather, they may also contain small amounts of other materials such as Sb (antimony) or P (phosphorus) in parts by molar composition of not more than approximately 5%. Even if InxGa1−xAs, In0,73Ga0,27As, InyAl1−yAs, In0,55Al0,45As, InzAl1−zAs, AlAs or other constituent materials or materials are mentioned in the scope of this description, this is also always intended to comprise the case that said constituent materials and/or materials include small amounts of other constituents.
With the aforementioned constituent materials, it is in particular possible to obtain a very large conduction band discontinuity between the AlAs of the barriers and the InGaAs in the quantum wells, with a possible emission of laser radiation with a wave length between 2.9 and 5.3 μm, in particular between 3.5 and 4.5 μm and especially in a wave length between 3.8 and 4.2 μm, at room temperatures.
The thicknesses of the quantum wells and/or the thicknesses of the barrier layers and/or the composition of at least one barrier layer having two constituent materials may be selected such in the quantum cascade laser structure in accordance with the invention, in particular in the active zone of the structure, that the laser-active transition from a number of energetically closely adjacent higher conditions to energetically lower condition or into a number of energetically lower conditions and energetically closely adjacent conditions occurs so that multiple wave length emission occurs. In particular by varying the ratio of the InyAl1−yAs constituent material relative to the InzAl1−zAs-consitutent material in the injection barrier, the subband structure in the adjacent quantum well of the active zone, where the emission process occurs, can be engineered so that multiple wavelength emission as well as single wave length emission is possible.
Multiple wavelength emission can be obtained in particular if the injection barrier is less than approx. 4 to 5 nm thick, in particular less than 4.5 nm thick and especially less than 4 nm thick.
In the quantum cascade laser structure, a cascade may in particular have the following layers with the stated constituent materials and layer thicknesses in the stated order:
For the n-doping, Si may be introduced into the respective layers, for example.
Instead of InAlAs and/or AlAs, the quantum cascade laser structure in accordance with the invention may comprise InAlAsSb (indium-aluminum-arsenic-antimony) or AlAsSb (aluminum-arsenic antimonide) as constituent material of at least one barrier layer with at least two constituent materials and/or as constituent material of the remaining barrier layers.
A quantum cascade laser in accordance with the invention comprises a lower waveguide layer, an upper waveguide layer and a quantum cascade laser structure in accordance with the invention arranged between said two waveguide layers. In particular, a quantum cascade laser in accordance with the invention may have a quantum cascade laser structure that can emit the laser radiation in several wave lengths and it may be equipped with a means to select the wave length of the emitted laser light. A potential means for selecting the wave length, for example, may be a so-called external cavity or a grating. A combination of external cavity and grating is also possible.
To dissipate the heat created in the operation of the quantum cascade laser, a quantum cascade laser in accordance with the invention may be connected to a heat sink, which may be realized, for example, as a so-called buried hetero structure or as a so-called epilayer-down mounting. By dissipating excess heat into the heat sink, the performance of the quantum cascade laser can be improved in particular in the operation at temperatures in the 300 K range.
Other characteristics, properties and advantages of the present invention are shown in the following in the description of an realization with reference to enclosed figures.
A quantum cascade laser 10 in accordance with the invention is shown schematically in
The quantum cascade laser described in the realization can be operated in particular such that it emits in a pulsed operating modus at 20° C. laser radiation in the wave length spectrum of approx. 3.8 to approx. 4.2 μm with a power output of over 240 mW per facet, i.e., in two different and in particular opposite radiation directions of the laser. If the quantum cascade laser is operated at low temperatures (8 K), a peak power output of up to 8 watts per facet can be obtained in the pulsed operating mode.
The quantum cascade laser 10 is produced in form of a vertical layer stack 11 from semiconductor materials and comprises a substrate 20, which simultaneously represents the lower cladding layer of the quantum cascade laser 10. In the present realization, the substrate 20 is comprised of InP (indium phosphide) and is doped with Sn (tin) in a concentration of 2×1017 (doping means that atoms of another material, so-called foreign atoms or doping materials, are introduced into a semiconductor material in order to supply free electrons) and also functions as the lower electric contact of the laser.
The substrate 20 is topped by a lower waveguide layer 30 of In−0.52Ga0.48As, which is doped with Si (silicon) in a concentration of 5×1016 cm−3. The lower waveguide layer 30 has a higher index of refraction than the substrate 20 and a thickness of 220 nm. Together with a second, upper waveguide layer 40, which is also made of In0.52Ga0.48As and has a silicon doping in a concentration of 5×1016 cm−3 and a thickness of 220 nm, said waveguide layer 30 confines the photons generated in the quantum cascade laser structure 100. The quantum cascade laser structure 100 has 30 cascades and a thickness of 1400 nm and is arranged between the two waveguide layers 30, 40. It will be described in detail later with reference to
A so-called four-period graded superlattice 50, i.e., a layer where a lattice structure is superimposed on another lattice structure in a graded manner,caps the second waveguide layer. The superlattice 50 is produced of Si-doped In0.52Ga0.48As and Si-doped In0.52Al0.48As and has a thickness of 18 nm. Because of the different lattice constants of In0.52Ga0.48As and In0.52Al0.48As, the four-period superlattice 50 is formed in that the lattice positions of the two lattices render all four lattice periods congruent.
The superlattice 50 is followed by two top cladding layers 60, 70 with a total thickness of 3,300 nm, each of which is produced of InP and Si-doped, but with different Si concentrations. While the first top cladding layer 60 that directly follows the superlattice 50 has a thickness of 2,500 nm and a Si-concentration of 1×1017, the thickness of the second top cladding layer 70 is 800 nm and its Si concentration is 4×1018. Instead of InP, the top cladding layers 60, 70 may also be produced of other suitable materials, such as InAlAs or InGaAlAs (indium-gallium-aluminum-arsenide), for example.
The top layer of the quantum cascade laser 10 forms a contact layer 80 that is 130 nm thick and Si-doped with a concentration of 1×1019 cm−3 and forms the top electrical contact of the laser.
Each of the quantum wells 110 a to 110 j is produced of In0.73Ga0.27As as the only constituent material, with the quantum wells 110 b, 110 c and 110 d also being n-doped with a Si concentration of 5×1017. The thicknesses of the quantum wells 110 a to 110 j are in a range of 1.8 to 5.0 nm and can be found in the table below. However, the quantum wells 110 a to 110 j may not fall below a specific minimum thickness so that the energy levels of the sub bands are not pushed out of the quantum well.
Each of the barrier layers 105 a to 105 c and 15 g [TrNote: sic; 105 g?] to 105 j are produced of AlAs. Their thicknesses vary between 0.9 and 2.1 nm and are also listed in the table below. Unlike the barrier layers 105 a to 105 c and 15 g to 105 j, the barrier layers 105 d, 105 e and 105 f are each comprised of two constituent materials, i.e., of AlAs as first constituent material 111 a, 112 a, 113 a and In0.55Al0.45As as second constituent material 111 b, 112 b, 113 b. The constituent material 111 b of the barrier layer 105 d is also doped with Si in a concentration of 5×1017.
Doping substance Reference Doping concentration Thickness Symbol Material substance [cm−3] [nm] 105 AlAs 0.75 110a In0.73Ga0.27As 3.4 105a AlAs 1.3 110b In0.73Ga0.27As Si 5 × 1017 3.0 105b AlAs 0.9 110c In0.73Ga0.27As Si 5 × 1017 2.6 105c AlAs 0.9 110d In0.73Ga0.27As Si 5 × 1017 2.2 105d 111b In0.55Al0.45As Si 5 × 1017 2.3 1.4 111a AlAs 0.9 110e In0.73Ga0.27As 2.0 105e 112b In0.55Al0.45As 2.3 1.4 112a AlAs 0.9 110f In0.73Ga0.27As 1.8 105f 113b In0.55Al0.45As 3.9 3.0 113a AlAs 0.9 110g In0.73Ga0.27As 1.8 105g AlAs 0.9 110h In0.73Ga0.27As 5.0 105h AlAs 1.7 110i In0.73Ga0.27As 4.2 105i AlAs 2.1 110j In0.73Ga0.27As 3.8 105j AlAs 0.75
The barrier layers 105 a to 105 c, 105 i, 105 j and quantum wells 110 a to 110 c, 110 i, 110 j form the so-called extraction zone, the barrier layers 105 f to 105 h and quantum wells 110 g and 110 h the so-called active zone and the barrier layers 105 d and 105 e and quantum wells 110 d to 110 f the so-called injection zone of the quantum cascade laser structure (see
In the quantum wells 110 a to 110 j, the conduction band edge K is energetically lower, whereas it is energetically higher in the barrier layers 105 a to 105 j. The use of AlAs in all barrier layers and InGaAs quantum wells maximizes the conduction band discontinuity, which reflects the energetic difference between conduction band edge K in the barrier layers 105 a to 105 j and the quantum wells 110 a to 110 j, in the entire cascade. When the quantum cascade laser structure is operated at room temperature, the large conduction band discontinuity in particular prevents electrons from overcoming the barrier layers 105 a to 105 j by having enough thermal energy to move unrestricted into the conduction band of the barrier material. Such transitions can lead to a so-called thermal depopulation of the energy level of a quantum well and as a result, the corresponding electrons are lost for the laser process. This thermal depopulation would inhibit a use of the laser at room temperature. Therefore, the large conduction band discontinuity of the quantum cascade laser structure in accordance with the invention makes it possible to emit laser radiation in a spectrum between 2.9 and 5.3 μm, especially in a spectrum of 3.5 and 4.5 μm and furthermore in particular in a spectrum of 3.7 to 4.2 μm at higher temperatures than would be possible with quantum cascade laser structures in accordance with the state of the art. In particular, the quantum cascade laser structure in accordance with the invention also allows an emission at room temperature.
Furthermore, the electrons can also transition from a higher energy level to a lower energy level. In doing so, they emit energy, for example in the form of photons, with the emitted energy corresponding to the energy difference between the two energy levels. In a transition of this type, i.e., in the transitioning from laser level 2 to laser level 1, the laser radiation is emitted. The wavelength of the emitted laser radiation is determined by the energy difference between the two laser levels 1, 2. Because said energy difference can be adjusted in particular by the width of the quantum wells 110 g and 110 h, the wavelength of the emitted laser radiation can be engineered in the production of the quantum cascade laser with the appropriate selection of said width. However, it is also possible to adjust the wave length of the emitted laser radiation in an already existing structure. The wavelength at which the emission of the laser radiation occurs can be varied, for example, with the appropriate adjustment of the temperature and/or the current strength of the current that flows through the quantum cascade laser and/or the electrical field.
A prototype of the described quantum cascade laser structure with lateral dimensions of 1.5 nm×34 μm emitted laser radiation with a wave length of approx. 4.005 μm (see
Also important for the emission of laser radiation is the degree of overlapping between the various energy levels of the mini-bands I and II and the laser levels 1 and/or 2 in the quantum wells 110 g and 110 h, which is linked closely to the tunnel probability. A high degree of overlapping means that a specific part of the laser radiation is not resulting from a transition from laser level to into laser level 1 but from a transition from one energy level of the mini-band II to the laser level 1 or in energy levels of the mini-band I. Likewise, in a large overlap, transitions from laser level 2 into an energy level of the mini-band I may occur. Because the energy levels of a mini-band differ slightly, the wave length of the laser radiation emitted at the corresponding transitions also differ slightly so that instead of radiation of a single wavelength, radiation in a wavelength spectrum is emitted. However, if the degree of overlapping between the various energy levels of the mini-bands I and II and the laser levels 1 and 2 in the quantum wells 110 g and 110 h is low, the transitions from one energy level of the mini-band II or into an energy level of the mini-band I are hardly significant in the emitting of the laser radiation and thus only laser radiation with a single wave length, which is determined by the energy difference between the laser level 2 and the laser level 1, is emitted.
In the quantum cascade laser structure in accordance with the invention, it is in particular possible to adjust the degree of overlapping between the various energy levels of the mini-bands I and II and the laser levels 1 and/or 2 in the quantum wells 110 g and 110 h by appropriately adjusting in particular the thickness of the barrier layer 105 f, which forms the injection barrier of the quantum cascade laser structure, i.e., the barrier through which the electrons are “injected” into the active zone of the cascade, as well as the relative parts of the constituent materials 113 a and 113 b in the barrier layer 105 f. Quantum cascade laser structures can be generated, which can be operated in multiple wave length emission modes as well as in single wave length emission mode. In particular thin barrier layers 105 f as in the present realization are suitable for the production of quantum cascade lasers that can be operated in the multiple wave length emission modus.
Some other experimentally determined performance data of the laser in accordance with the invention are described in the following with the FIGS. 6 to 8.
The experimentally determined power output determined with a quantum cascade laser as described in the realization is shown in
Also shown in
In the realization for the quantum cascade laser structure in accordance with the invention, the barrier layers are constructed with two constituent materials in such a manner that each of the constituent materials forms an independent partial layer. However, the two constituent materials can also be combined in other ways, for example to form a so-called superlattice pseudo alloy. Furthermore, the quantum cascade laser in accordance with the invention is not limited to the quantum cascade laser design described in the present realization. Rather, the quantum cascade laser structure in accordance with the invention can also be used in other quantum cascade laser designs. An overview of the various quantum cascade laser designs is shown in J. Faist et al., IEEE Journal of Quantum Electronics, Vol. 38, No. 6, July 2002.
|Cited Patent||Filing date||Publication date||Applicant||Title|
|US4999844 *||Apr 12, 1989||Mar 12, 1991||Omron Tateisi Electronics Co.||Semiconductor quantum well laser|
|US6023482 *||Jan 23, 1998||Feb 8, 2000||Lucent Technologies Inc.||Article comprising a strain-compensated QC laser|
|US6232624 *||Jul 12, 1999||May 15, 2001||Hughes Electronics Corporation||InPSb channel HEMT on InP for RF application|
|US6324199 *||Nov 18, 1998||Nov 27, 2001||Lucent Technologies Inc.||Intersubband light source with separate electron injector and reflector/extractor|
|Citing Patent||Filing date||Publication date||Applicant||Title|
|US7424042||Sep 22, 2006||Sep 9, 2008||Daylight Solutions, Inc.||Extended tuning in external cavity quantum cascade lasers|
|US7466734||Sep 22, 2006||Dec 16, 2008||Daylight Solutions, Inc.||Compact external cavity mid-IR optical lasers|
|US7492806||Jun 15, 2005||Feb 17, 2009||Daylight Solutions, Inc.||Compact mid-IR laser|
|US7535936||Aug 5, 2005||May 19, 2009||Daylight Solutions, Inc.||External cavity tunable compact Mid-IR laser|
|US7732767||Aug 11, 2006||Jun 8, 2010||Lasermax, Inc.||Target marker having quantum cascade laser for thermally marking a target|
|US7796341||Apr 16, 2009||Sep 14, 2010||Daylight Solutions, Inc.||Lenses, optical sources, and their couplings|
|US7822089 *||Jul 20, 2007||Oct 26, 2010||Osram Opto Semiconductors Gmbh||Semiconductor layer structure with superlattice|
|US7826503||Sep 4, 2008||Nov 2, 2010||Daylight Solutions, Inc.||Extended tuning in external cavity quantum cascade lasers|
|US7848382||Jan 13, 2009||Dec 7, 2010||Daylight Solutions, Inc.||Laser source that generates a plurality of alternative wavelength output beams|
|US7873094||Jan 15, 2009||Jan 18, 2011||Daylight Solutions, Inc.||Compact Mid-IR laser|
|US7893424||Jul 20, 2007||Feb 22, 2011||Osram Opto Semiconductors Gmbh||Semiconductor layer structure with superlattice|
|US7920608||Mar 11, 2008||Apr 5, 2011||Daylight Solutions, Inc.||Quantum cascade laser suitable for portable applications|
|US8000367||Jan 18, 2008||Aug 16, 2011||Fraunhofer-Gesellschaft Zur Forderung Der Angewandten Forschung E.V.||High-efficiency unipolar quantum cascade laser|
|US8022392||Jul 20, 2007||Sep 20, 2011||Osram Opto Semiconductors Gmbh||Semiconductor layer structure with superlattice|
|US8067734||May 13, 2010||Nov 29, 2011||Lasermax, Inc.||Target marker having quantum cascade laser for thermally marking a target|
|US8168952||Sep 22, 2011||May 1, 2012||Lasermax, Inc.||Target marker having quantum cascade laser for thermally marking a target|
|US8189630||May 18, 2010||May 29, 2012||Daylight Solutions, Inc.||Quantum cascade laser suitable for portable applications|
|US8306077||Apr 21, 2009||Nov 6, 2012||Daylight Solutions, Inc.||High output, mid infrared laser source assembly|
|US8442081||Apr 25, 2012||May 14, 2013||Daylight Solutions, Inc.||Quantum cascade laser suitable for portable applications|
|US8471240||Jan 19, 2011||Jun 25, 2013||Osram Opto Semiconductors Gmbh||Semiconductor layer structure with superlattice|
|US8575595 *||Apr 12, 2010||Nov 5, 2013||Qinetiq Limited||P-type semiconductor devices|
|US8879590||Sep 27, 2012||Nov 4, 2014||Daylight Solutions, Inc.||High output, mid infrared laser source assembly|
|US8913637||Jan 4, 2013||Dec 16, 2014||Daylight Solutions, Inc.||Quantum cascade laser suitable for portable applications|
|US9042688||Jan 26, 2012||May 26, 2015||Daylight Solutions, Inc.||Multiple port, multiple state optical switch|
|US9059562||Jun 22, 2012||Jun 16, 2015||Daylight Solutions, Inc.||Control system for directing power to a laser assembly|
|US9093813||Oct 11, 2012||Jul 28, 2015||Daylight Solutions, Inc.||Mounting base for a laser system|
|US20120025170 *||Apr 12, 2010||Feb 2, 2012||Qinetiq Limited||P-type semiconductor devices|
|US20120207186 *||Feb 16, 2010||Aug 16, 2012||The Board Of Regents Of The University Of Texas System||Terahertz quantum cascade lasers (qcls)|
|International Classification||H01S5/024, H01S5/00, H01S5/343, H01S5/14, H01S5/34|
|Cooperative Classification||H01S5/141, H01S5/3406, H01S5/1096, H01S5/3402, B82Y20/00|
|European Classification||B82Y20/00, H01S5/34A2|
|Jun 6, 2005||AS||Assignment|
Owner name: HUMBOLDT-UNIVERSTAET ZU BERLIN, GERMANY
Free format text: ASSIGNMENT OF ASSIGNORS INTEREST;ASSIGNORS:MASSELINK, WILLIAM TED;DRESSLER, SEBASTIAN;SEMSTSIV, MYKHAYLO PETROVYCH;AND OTHERS;REEL/FRAME:016305/0894
Effective date: 20050512
Owner name: FORSCHUNGSZENTRUM ROSSENDORF E.V., GERMANY
Free format text: ASSIGNMENT OF ASSIGNORS INTEREST;ASSIGNORS:MASSELINK, WILLIAM TED;DRESSLER, SEBASTIAN;SEMSTSIV, MYKHAYLO PETROVYCH;AND OTHERS;REEL/FRAME:016305/0894
Effective date: 20050512