METHOD AND APPARATUS FOR JOSEPHSON DISTRIBUTED OUTPUT AMPLIFIER |
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申请号 | US12186465 | 申请日 | 2008-08-05 | 公开(公告)号 | US20100033252A1 | 公开(公告)日 | 2010-02-11 |
申请人 | Quentin P. Herr; Donald Lynn Miller; John Xavier Przybysz; | 发明人 | Quentin P. Herr; Donald Lynn Miller; John Xavier Przybysz; | ||||
摘要 | The disclosure generally relates to a method and apparatus for providing high-speed, low signal power amplification. In an exemplary embodiment, the disclosure relates to a method for providing a wideband amplification of a signal by forming a first transmission line in parallel with a second transmission line, each of the first transmission line and the second transmission line having a plurality of superconducting transmission elements, each transmission line having a transmission line delay; interposing a plurality of amplification stages between the first transmission line and the second transmission line, each amplification stage having an resonant circuit with a resonant circuit delay; and substantially matching the resonant circuit delay for at least one of the plurality of amplification stages with the transmission line delay of at least one of the superconducting transmission lines. | ||||||
权利要求 | What is claimed is: |
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说明书全文 | 1. Field of the Invention The disclosure generally relates to wideband distributed amplifiers. More specifically, the disclosure relates to a method and apparatus for providing high-speed, low signal power amplification using superconducting technology. 2. Description of Related Art A well-known wideband amplifier known as a distributed amplifier amplifies the incoming signal to an output signal commensurate with the desired amplification level. Distributed amplifier architecture introduces delay to achieve wideband characteristics. Conventional distributed amplifiers include a pair of transmission lines, each having a characteristic impedance, for independently connecting the inputs and outputs of several active devices. The gain of the distributed amplifier is additive rather than multiplicative. The gain is determined, in part, by the number of stages. This property enables the distributed amplifier to provide a gain at frequencies beyond that of the unity-gain frequency of any individual stage. The delays of the input transmission line 110 and the output transmission line 120 can be made equal through the selection of propagation constants and line lengths to ensure that the output signals from each individual device sums in phase. Both input and output lines must be resistively terminated, by resistors 130 and 140. A major drawback of the conventional distributed amplifier is poor efficiency because power matching and phasing cannot be achieved at the same time. A conventional distributed amplifier is also inoperable with high-speed superconducting systems. Superconductor digital circuits feature high clock rates (i.e., 10-40 GHz) and extremely low signal power levels (i.e., 2-8 nW). Superconductor circuits are ideally suited for mixed-signal applications such as analog to digital conversion due to high sample rates and quantum accurate feedback distributed amplifiers, which use the same operating principles as the metrological voltage standard. However, because signal levels are so low and data rates are so high, establishing data links to conventional electronics, at low bit error rate, has been proved difficult. Therefore, there is a need for a method and apparatus to provide a distributed amplifier adapted to high clock rates and low signal power. In one embodiment, the disclosure relates to a method for providing a wideband amplification of a signal, the method comprising: forming a first transmission line in parallel with a second transmission line, each of the first transmission line and the second transmission line having a plurality of superconducting transmission elements, each transmission line having a transmission line delay; interposing a plurality of amplification stages between the first transmission line and the second transmission line, each amplification stage having an resonant circuit with a resonant circuit delay; and substantially matching the resonant circuit delay for at least one of the plurality of amplification stages with the transmission line delay of at least one of the superconducting transmission lines to provide a wideband amplification of an input signal. In another embodiment, the disclosure relates to a distributed amplifier circuit comprising: a first transmission line and a second transmission line, each of the first transmission line and the second transmission line having a plurality of Josephson Transmission lines (“JTLs”), each JTL having a Josephson transmission delay; a plurality of resonant circuits connected in series and including a voltage source controlled with at least one of the first transmission line or the second transmission line, one of the plurality of the resonant circuits having a resonant transmission delay; wherein the resonant transmission delay is substantially matched to the Josephson transmission delay of at least one of the plurality of JTLs. In still another embodiment, the disclosure relates to a superconductor driver for high throughput data amplification, comprising: a first amplification stage having a first Josephson transmission line (JTL) and a second Josephson transmission line with a resonant circuit interposed therebetween, the first Josephson transmission line having a first transmission line delay and the second Josephson transmission line having a second transmission line delay, the resonant circuit configured to have a resonant circuit delay substantially matching the first transmission line delay. In yet another embodiment, the disclosure relates to a superconducting amplifier comprising: a first transmission line having a plurality of Josephson transmission lines (JTLs) connected in series, each JTL having a respective JTL delay; a plurality of voltage sources arranged in series with a plurality of resonant circuits, each of the plurality of voltage sources electro-magnetically communicating with at least one JTL; and wherein each voltage source defines a SQUID which is set and reset through an inductive coupling with one of the JTLs. These and other embodiments of the disclosure will be discussed with reference to the following exemplary and non-limiting illustrations, in which like elements are numbered similarly, and where: In Transmission lines 230 and 240 are formed in parallel and communicate set/reset signals to each amplification stage. In the embodiment of In one embodiment of the disclosure, transmission lines 230 and 240 are configured to have one or more Josephson transmission lines (“JTLs”) for transmitting the set/reset signals. Josephson transmission lines are advantageous for providing high clock rates and low signal power. Each JTL has a characteristic transmission delay. Referring to According to one embodiment of the disclosure, an amplification stage comprises two JTLs connected in parallel with a voltage source and a resonant circuit interposed therebetween. Referring to exemplary embodiment of The set signal 232 and reset signal 242 provide extremely small, single flux quantum (“SFQ”) voltage pulses to each amplification. An exemplary set/reset signal may be about 0.5 mV high and 4 pS wide, FWHM. The SFQ signals are distributed on the active JTLs and turn ON and OFF the voltage sources connected in series. In one embodiment, each JTL was built to provide about 6 pS delay. The resonant circuit was selected to have a resonant delay of about 6 pS, thereby matching the resonant delay of the JTLs. Thus, the resonant circuit delay was matched to a JTL delay of about 6 pS. The resonant circuit also provided 50 Ohm impedance and the circuit provided 20 GHz bandwidth, supporting 10 Gb/S NRZ data. The amplifier bandwidth-gain product was substantially higher than that of the conventional distributed amplifiers, and substantially higher than other amplifiers of SFQ input signals. Voltage sources 301, 302 . . . 312 include two Josephson junctions arranged in a superconducting-quantum-interference-device (“SQUID”). Each voltage source is set and reset through inductive coupling with transmission lines 330 and 340. SQUID 312 comprises Josephson junctions 315 and 316, as well as inductor 313 and shunt resistor 314. The shunt resistor in each SQUID (applied asymmetrically to the right junction, as shown) enforces the out-of-phase voltage mode required to reset the circuit. During operation, inductor 360 is energized by an SFQ Pulse from Set/Reset gates 332/342. The inductive coupling energizes inductor 313 of SQUID 312. Shunt resistor 314 provides out-of-phase voltage mode which enables resetting SQUID circuit 312. The application of shunt resistor 314 with SQUID 312 is exemplary and non-limiting. Other circuit configurations which enable resetting of the SQUID circuit can be used without departing from the principles disclosed herein. Similar to In one embodiment of the disclosure, the active Josephson transmission delay on the input is matched to lumped LC transmission line delay on the output. Thus, transmission delay through JTL 335 can be matched to transmission delay of lumped LC circuit 323. In another embodiment, transmission delay through JTL 345 can be matched to transmission delay of lumped LC circuit 323. In still another embodiment, each of JTLs 335, 345 is selected to have a transmission line delay matching that of lumped circuit 323. In still another embodiment, lump circuit 323 has a characteristic delay matching transmission line delay through JTL 333 or 343. Each voltage source shown in (50 Ω+50 Ω)/12=8 Ω (1) In one embodiment of In Transmission line 430 comprises a plurality of JTLs, with each JTL matched to an amplification stage such that a circuit with n amplification stages has n−1 JTLs. As discussed, each JTL has a characteristic delay associated therewith. In contrasts with circuits of As with flux-powered single-flux-quantum logic gates, such an amplifier configuration can avoid static power dissipation in the JTL by elimination of the associated bias resistors. Inductor 451 and capacitor 452 complete circuit 400 by forming a resonant circuit which communicates with voltage source 412. In one exemplary embodiment, resistor 455 was matched to resistor 453 and each was provided a 50 Ω resistance. While the principles of the disclosure have been illustrated in relation to the exemplary embodiments shown herein, the principles of the disclosure are not limited thereto and include any modification, variation or permutation thereof. |