|Publication number||USRE40900 E1|
|Application number||US 11/541,516|
|Publication date||Sep 1, 2009|
|Filing date||May 17, 2000|
|Priority date||May 22, 1999|
|Also published as||CA2371593A1, CA2371595A1, CN1364336A, CN1365537A, DE60001940D1, DE60001940T2, DE60003925D1, DE60003925T2, EP1186097A1, EP1186097B1, EP1188231A1, EP1188231B1, US6480062, US6799027, WO2000072439A1, WO2000072440A1|
|Publication number||11541516, 541516, PCT/2000/1895, PCT/GB/0/001895, PCT/GB/0/01895, PCT/GB/2000/001895, PCT/GB/2000/01895, PCT/GB0/001895, PCT/GB0/01895, PCT/GB0001895, PCT/GB001895, PCT/GB2000/001895, PCT/GB2000/01895, PCT/GB2000001895, PCT/GB200001895, US RE40900 E1, US RE40900E1, US-E1-RE40900, USRE40900 E1, USRE40900E1|
|Inventors||Ian J. Forster|
|Original Assignee||Forster Ian J|
|Export Citation||BiBTeX, EndNote, RefMan|
|Patent Citations (27), Classifications (12), Legal Events (3)|
|External Links: USPTO, USPTO Assignment, Espacenet|
This invention relates to an amplifier circuit, in particular but not exclusively to an amplifier circuit for providing bandpass amplification at intermediate frequencies in radio receivers.
Amplifiers are widely used in the prior art for amplifying input signals applied thereto to provide amplified output signals. This is particularly important in radio receivers in which radiation received thereat generates corresponding antenna received signals which typically have an amplitude of microvolts. The radio receivers employ amplifiers therein to amplify such received signals to an amplitude in the order of multivolts to volts, for example to drive a loudspeaker. Since it is difficult to prevent amplifiers designed to amplify at radio frequencies from spontaneously oscillating, especially if they comprise cascaded gain providing stages, it is customary to heterodyne the received signals to lower intermediate frequencies whereat it is easier to provide a high degree of amplification and also provide more selective bandpass signal filtration.
In prior art radio receivers, it is therefore customary to provide a majority of signal amplification required at intermediate frequencies, namely frequencies lying intermediate between that of the radiation received and audio or video frequencies. For example, a radio receiver receives radiation at a frequency of 500 MHz and generates a corresponding antenna received signal also at 500 MHz. The receiver heterodynes the received signal to generate an intermediate frequency signal in a frequency range around 10.7 MHz which is then amplified and filtered, and finally demodulates the amplified intermediate frequency signal to generate a corresponding audio output signal having signal components in a frequency range of 100 Hz to 5 kHz.
Recently, because the radio frequency spectrum is becoming increasingly congested, there is a trend to use an ultra high frequency (UHF) range in contemporary communications systems, namely around 500 MHz; transmission at microwave frequencies, for example 1 GHz to 30 GHz is now also employed. Associated with this is a trend in modern radio receiver design to employ intermediate frequency amplification at several tens of MHz or greater, this is done in order to obtain adequate ghost image rejection associated with using heterodyne processes.
In modem modern mobile phones, most signal amplification is provided in intermediate frequency amplifier circuits incorporated therein. These circuits comprise transmission amplifiers and associated surface acoustic wave (SAW) or ceramic filters to provide a narrow bandpass signal amplification characteristic; the circuits and their associated filters are conventionally referred to collectively as an “intermediate frequency strip”. Such transmission amplifiers consume significant power in operation, for example intermediate frequency amplifier circuits employed in mobile telephones typically consume between several hundred microamperes and several mA of current when operational.
In order to provide modern mobile telephones with extended operating time from their associated batteries, new types of battery have been researched and developed which provide enhanced charge storage to weight performance, for example rechargeable metal hydride and lithium batteries.
The inventor has appreciated, rather than concentrating on improving battery technology, that reduction in current consumption of intermediate frequency amplifier circuits in radio receivers is desirable to provide extended operating time from batteries. The invention has therefore been made in a endeavour to provide an alternative type of amplifier circuit, for example a circuit especially suitable for use at intermediate frequencies in radio receivers which is capable of requiring less power to operate.
It is known in the art, as described in a Japanese patent application no. JP 55137707, to cascade reflection amplifiers in series and interpose filters therebetween to prevent higher harmonic components generated in preceding stages from propagating to successive stages. The filters are not operable to inhibit signal propagation in a reverse direction along the cascaded series of amplifiers to prevent the occurrence of spontaneous oscillation.
According to the present invention, there is provided an amplifier circuit for receiving an input signal and providing a corresponding amplified output signal, the circuit characterised in that it comprises:
This provides the advantage that interposition of the filters between the amplifiers is capable of isolating each amplifier from its neighbouring amplifiers, thereby hindering signal propagation in the reverse direction along the path; incorporation of the modulating means enables the input signal propagating through each amplifier to be converted between a carrier and a sideband signal, thereby enabling it to propagate through the filters in the forward direction along the path.
The circuit provides the benefit that is capable of providing signal amplification and consuming less current during operation compared to prior art amplifier circuits.
One skilled in the art would not expect it to be practicable to connect a plurality of reflection amplifiers together and obtain stable amplification therefrom because of spontaneous interfering oscillations which would arise during operation. The circuit addresses this problem by incorporating the connecting means which promotes intended signal amplification in the circuit and counteracts signal amplification giving rise to spontaneous oscillation therein.
Spontaneous oscillation is defined as self induced oscillation arising along a signal path providing amplification as a consequence of feedback occurring around or within the signal path.
Conveniently, the filters are arranged in series along the signal path, the filters alternating between sideband transmissive filters and sideband rejective filters along the path, and the modulating means is arranged to convert the input signal as it propagates along the signal path alternately between a corresponding carrier signal transmissible substantially through the sideband rejective filters only and a corresponding sideband signal transmissible substantially through the sideband transmissive filters only, thereby promoting input signal propagation in the forward direction along the path and hindering signal propagation in the reverse direction therealong.
In another aspect, the invention provides a method of amplifying an input signal and providing a corresponding amplified output signal, the method characterised in that it includes the steps of:
The method provides the advantage that, during amplification, the signal is selectively directed from amplifier to amplifier in a forward direction along the signal path, thereby counteracting any of the amplifiers reamplifying the input signal and hence preventing any feedback loops being established in which spontaneous oscillation can arise.
An embodiment of the invention will now be described, by way of example only, with reference to the following diagrams in which:
The filters 610, 630 are identical and employ surface acoustic wave (SAW), bulk acoustic wave (BAW) or ceramic filter components. Each of filters 610, 630 provides a bandpass transmission characteristic for signals propagating between its terminals H1, H2. The characteristic comprises a single transmission peak centred at a frequency f0 having upper and lower −3 dB cut off frequencies of f0+f1 and f0−f1 respectively. In the circuit 600, f0 is 100 MHz and f1 is 50 KHz.
The filter 620 also employs SAW, BAW or ceramic filter components. It provides a double peak transmission characteristic for signals propagating between its terminals H3, H4. The double peak characteristic comprises two transmission peaks, a first peak centred at a frequency f0+f2 and a second peak centred at a frequency f0−f2. The first peak has −3 dB upper and lower cut off frequencies of f0+f2+f1 and f0+f2−f1 respectively. Likewise, the second peak has −3 dB upper and lower cut off frequencies of f0−f2+f1 and f0−f2−f1 respectively.
The biphase switches 650, 660 are identical and each incorporates three terminals, namely signal terminals J1, J2 and an input terminal K as described above. The switch 650 incorporates an inductor and a varactor, also known in the art as a varicap diode; control signals applied to the terminal K of the switch 650 are operative to control a potential applied to the varactor therein, thereby changing its tuning and affecting a phase shift imparted to signals propagating through the switch 650 between its terminals J1, J2. When the control signal from the switching oscillator 670 is in the logic state 0, the switches 650, 660 are operative to provide 0° phase shift; conversely, when the control signal is in the logic state 1, the switches 650, 660 are operative to provide 90° phase shift. Thus, in operation, signals propagating through and subsequently returning from switches 650, 660 via their terminals J1, J2 and amplified by associated reflection amplifiers 700, 710 are periodically switched in phase between 0° and 180°.
Operation of the circuit 600 will now be described with reference to
The filter 610 receives an input signal Sin at its terminal H1 input. The signal Sin is for example, generated in a preceding stage (not shown) which heterodynes a received signal to generate the signal Sin as an intermediate frequency signal including signal components in a frequency range of f0−f1 to f0+f1. The signal Sin is transmitted through the filter 610 from the terminal H1 to the terminal H2 thereof because its signal components are within the frequency range of the peak 850 of the filter 610. When the signal Sin propagates from the terminal H2, it is unable to pass through the filter 620 because it is not transmissive at frequencies of the signal components; the signal Sin thus propagates from the terminal H2 to the terminal J1 of the switch 650 and becomes phase modulated therein to emerge at the terminal J2 as a first modulated signal Sm1. The modulated signal Sm1 propagates to a port T3 of the amplifier 700 which reflectively amplifiers amplifies the signal Sm1, to provide a second amplified modulated signal S2 Sm2. The signal Sm2 propagates from the port T3 of the amplifier 700 back through the switch 650 whereat it is further phase modulated to provide a third modulated signal Sm3 which is output at the terminal J1.
The signal Sm3 is phase modulated and comprises two sidebands including signal components in the frequency range of peaks 860, 870. The sidebands in the signal Sm3 are prevented from propagating back through the filter 610 because it is non-transmissive at the frequencies of these sidebands. The signal Sm3 thus propagates from the terminal H3 of the filter 620 to the terminal H4 thereof because the sidebands are within the frequency range of the peaks 860, 870 of the filter 620.
The signal Sm3 propagates from the terminal H4 of the filter 620 to the terminal J1 of the switch 660. The filter 630 is unable to transmit the signal Sm3 because it is not transmissive at the frequency ranges of the sidebands of the signal. The signal Sm3 thus propagates through the switch 660 from its terminal J1 to its terminal J2 to emerge therefrom as a fourth signal Sm4. Because the switch 660 provides phase modulation at the frequency f2, the sidebands in the signal Sm3 am heterodyned to generate a signal component in the signal Sm4 in a frequency range of the peak 850. The signal Sm4 propagates from the terminal J2 of the switch 660 to a port T3 of the amplifier 710 wherein it is reflectively amplified to provide an amplified signal Sm5. The signal Sm5 propagates from the port T3 of the amplifier 710 back through the switch 660 whereat it is further phase modulated to emerge as a sixth signal Sm6 at the terminal J1 of the switch 660. The signal Sm6 includes, from the signal Sm5, signal components in the frequency range of the peak 850 after amplification thereof.
Because the filter 620 is untransmissive to signals including signal components within the frequency range of the peak 850, especially at its H4 terminal, the signal Sm6 is prevented from being transmitted back through the filter 620. The signal Sm6 thus propagates through the filter 630 from its terminal H1 to its terminal H2 to propagate therefrom as the signal Sout. The signal Sout incorporates signal components present in the signal Sin which have been amplified by the circuit 600.
In broad overview, the circuit 600 alternately converts from stage to stage the signal Sin to be amplified from carrier frequency, namely within the frequency range of the peak 850, to sidebands, namely within the frequency range of the peaks 860, 870. Thus, the switches 650, 660 in combination with the filters 610, 620, 630 are effective at counteracting signal propagation back in a reverse direction along a path from the output Sout to the input Sin; this isolates the amplifiers 700, 710 thereby enabling greater signal amplification to be achieved in the circuit 600 without spontaneous oscillations arising. Hence, the circuit 600 is capable of providing high signal amplification approaching 50 dB for low current consumption in the order of a few tens of microamperes on account of employing reflection amplifiers.
If the reflection amplifiers 700, 710 were merely cascaded together without the switches 650, 660 and the filters 610, 620, 630, severe spontaneous oscillation problems would be encountered which would hinder intended input signal amplification from being achieved.
The circuit 600 can be modified to include more amplification stages, each stage incorporating a reflection amplifier and being isolated from its neighbouring stages by a filter like the filter 610 in a first direction along the signal path, and by a filter like the filter 620 in a second direction along the signal path, said directions being mutually opposite. This enables higher gain to be achieved on account of incorporating more amplifier stages than illustrated in FIG. 1.
The filters 610, 620, 630 can be one or more of SAW filters, ceramic filters or tuned inductance/capacitance filters. For high frequency operation, bulk acoustic wave filters can also be employed.
The amplifiers 700, 710 can be connected to a bias controller arranged to control transistor currents within the amplifiers 700, 710 thereby enabling dynamic control of their gain, for example where automatic gain control (AGC) is required to cater for a relatively large dynamic range of signals applied at Sin.
The amplifier circuit 600 incorporates a cascaded series of reflection amplifiers connected to form a signal path along which input signal amplification occurs. The reflection amplifiers are connected by switched devices, for example the switches 650, 660 and the filters 610, 620, 630, to facilitate signal propagation in a forward direction along the path for amplification and counteract signal propagation in a reverse direction along the path which can give rise to spontaneous oscillation. This enables higher amplification gains to be achieved for a lower current consumption which is less than required for prior art transmission amplifiers providing comparable gain.
The reflection amplifier circuit 1400 will now be further described with reference to FIG. 3. The circuit 1400 is included within a dotted line 1410 and comprises a silicon or gallium arsenide (GaAs) transistor indicated by 1420, a capacitor 1430 and a resistor 1440 forming a termination network for the transistor 1420, a feedback capacitor 1450, an inductor 1460 and a resistor 1470 forming a bias network, and a current source 1480. The circuit 1400 includes an input/output port T3 which is connected to a gate electrode 1420g of the transistor 1420 and to a first terminal of the capacitor 1450.
The circuit 1400 is connected to a power supply 1500 for supplying the circuit 1400 with power. The supply 1500 is connected to a drain electrode 1420d of the transistor 1420 and also to a first terminal of the capacitor 1430; a second terminal of the capacitor 1430 is connected to a signal ground. The capacitor 1450 provides a second terminal which is connected to a source electrode 1420s of the transistor 1420, to the resistor 1440 which is grounded, and through the inductor 1460 and the resistor 1470 in series to the source 1480, which is connected to the signal ground.
In operation of the circuit 1400, the gate electrode 1420g receives an incoming signal 6 applied through the port T3. The incoming signal causes a signal current corresponding to the incoming signal to flow between the source electrode 1420g and the drain electrode 1420d. The signal current is coupled through gate-drain and gate-source capacitances of the transistor 1420 and also through the capacitor 1450, thereby generating an outgoing signal at the gate electrode 1420g which is an amplified version of the incoming signal. The incoming signal is reflected at the gate electrode 1420g where it is combined with the outgoing signal which propagates out through the port T3.
On account of the circuit 1400 receiving the incoming signal and returning the combined signal via one terminal, namely the port T3, it behaves as a reflecting negative resistance. The circuit 1400 and its associated components shown within the dotted line 1410 are capable of providing a high power gain approaching +30 dB for a drain/source current through the transistor 1420 in the order of a few tens of microamperes. Such a high power gain is not achievable from a transmission amplifier operating on such a low supply current.
When incorporated into a mobile telephone as part of its intermediate frequency strip, the amplifier circuit 600 incorporating a plurality of the circuits 1400 is capable of providing an order of magnitude reduction in telephone current consumption associated with amplifying signals therein at intermediate frequencies compared to prior art. This is of considerable benefit which provides extended duration of telephone operation from power supplied from rechargeable batteries for example.
It will be appreciated by those skilled in the art that variations can be made to the circuit 600 without departing from the scope of the invention. Thus, alternative switching devices, or equivalent devices, can be used with reflection amplifiers provided they exhibit similar characteristics to the switches and filters in the circuit 600, namely for counteracting spurious oscillation from arising.
The circuit 600 can be incorporated into radio receivers, for example mobile telephones, to function as intermediate frequency strips therein. Moreover, when provided with a demodulator to convert signals output from the circuit 600, the circuit is capable of operating as an IF receiver.
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|JPS55105408A||Title not available|
|JPS55137707A||Title not available|
|JPS60127806A||Title not available|
|U.S. Classification||455/313, 455/341, 455/106, 330/287, 455/325, 455/311|
|International Classification||H03F3/46, H03F1/02, H04B1/26, H03F3/60|
|Feb 24, 2012||FPAY||Fee payment|
Year of fee payment: 8
|Oct 23, 2012||AS||Assignment|
Owner name: MINERAL LASSEN LLC, NEVADA
Free format text: ASSIGNMENT OF ASSIGNORS INTEREST;ASSIGNOR:MARCONI UK INTELLECTUAL PROPERTY LIMITED;REEL/FRAME:029173/0564
Effective date: 20050106
|Feb 23, 2016||FPAY||Fee payment|
Year of fee payment: 12