Reducing spontaneous emission in circuit quantum electrodynamics by a combined readout and filter technique
US-2016329896-A1 · Nov 10, 2016 · US
US2018226975A1 · US · A1
| Field | Value |
|---|---|
| Publication number | US-2018226975-A1 |
| Application number | US-201715425989-A |
| Country | US |
| Kind code | A1 |
| Filing date | Feb 6, 2017 |
| Priority date | Feb 6, 2017 |
| Publication date | Aug 9, 2018 |
| Grant date | — |
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Superconducting devices with enforced directionality and related methods are provided. In one example, a device including a first Josephson junction transmission line (JTL) for propagating a first set of quantum signals in a first direction and a second JTL for propagating a second set of quantum signals in the first direction is provided. The device may include a logic gate having a first input terminal for receiving the first set of quantum signals via the first JTL, and a second input terminal. The device may include a unidirectional buffer having a first input terminal for receiving the second set of quantum signals via the second JTL and an output terminal for coupling the second set of quantum signals to the second input terminal of the logic gate, where the unidirectional buffer may be configured to propagate quantum signals in only the first direction.
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1 . A device comprising: a first Josephson junction transmission line (JTL) for propagating a first set of quantum signals in a first direction; a second Josephson junction transmission line (JTL) for propagating a second set of quantum signals in the first direction; a logic gate comprising a plurality of Josephson junctions, wherein the logic gate having a first input terminal for receiving the first set of quantum signals via the first JTL, and a second input terminal; and at least one unidirectional buffer having a first input terminal for receiving the second set of quantum signals via the second JTL and an output terminal for coupling the second set of quantum signals to the second input terminal of the at least one logic gate, wherein the unidirectional buffer is configured to propagate quantum signals in only the first direction. 2 . The device of claim 1 , wherein the unidirectional buffer comprising: a first inductive element coupled between a first terminal and a second terminal; a first Josephson junction coupled between the second terminal and a ground terminal; a second inductive element coupled between the second terminal and a third terminal; and a second Josephson junction coupled between the third terminal and the ground terminal, wherein the second inductive element is configured to form an inductive loop comprising the first Josephson junction, the second inductive element, and the second Josephson junction. 3 . The device of claim 2 , wherein the inductive loop is configured to store a current in the inductive loop. 4 . The device of claim 3 , wherein the unidirectional buffer is configured to receive power via a clock signal comprising a plurality of phases, and wherein the clock signal is configured to provide a bias current to at least the second Josephson junction. 5 . The device of claim 4 , wherein the unidirectional buffer is configured to propagate a quantum signal in the first direction when a sum of the bias current and the current stored by the inductive loop is sufficient to trigger the second Josephson junction. 6 . The device of claim 1 , wherein the quantum signals comprise single-flux quantum (SFQ) pulses. 7 . The device of claim 6 , wherein the SFQ pulses comprise positive SFQ pulses and negative SFQ pulses. 8 . The device of claim 2 , wherein the first Josephson junction has a corresponding first critical current value and the second Josephson junction has a corresponding second critical current value, and wherein the first critical current value is approximately 1.1 to 1.4 times the second critical current value. 9 . A unidirectional buffer comprising: an input terminal for receiving quantum signals via a Josephson transmission line (JTL) configured to propagate signals in a first direction, wherein the unidirectional buffer is configured to propagate quantum signals in only the first direction and not in a second direction opposite to the first direction. 10 . The unidirectional buffer of claim 9 further comprising: a first inductive element coupled between the input terminal and a second terminal; a first Josephson junction coupled between the second terminal and a ground terminal; a second inductive element coupled between the second terminal and a third terminal; and a second Josephson junction coupled between the third terminal and the ground terminal, wherein the second inductive element is configured to form an inductive loop comprising the first Josephson junction, the second inductive element, and the second Josephson junction. 11 . The unidirectional buffer of claim 10 , wherein the inductive loop is configured to store a current in the inductive loop. 12 . The unidirectional buffer of claim 11 , wherein the unidirectional buffer is further configured to receive power via a clock signal comprising a plurality of phases, and wherein the clock signal is configured to provide a bias current to at least the second Josephson junction. 13 . The unidirectional buffer of claim 12 , wherein the unidirectional buffer is further configured to propagate a quantum signal in the first direction when a sum of the bias current and the current stored by the inductive loop is sufficient to trigger the second Josephson junction. 14 . The unidirectional buffer of claim 10 , wherein the quantum signals comprise single-flux quantum (SFQ) pulses. 15 . The unidirectional buffer of claim 14 , wherein the SFQ pulses comprise positive SFQ pulses and negative SFQ pulses. 16 . The unidirectional buffer of claim 10 , wherein the first Josephson junction has a corresponding first critical current value and the second Josephson junction has a corresponding second critical current value, and wherein the first critical current value is approximately 1.1 to 1.4 times the second critical current value. 17 . A device comprising: a logic gate comprising a plurality of Josephson junctions, wherein the logic gate having a first input terminal for receiving quantum signals and a second input terminal for receiving quantum signals; and a first unidirectional buffer having a first input terminal for receiving the quantum signals and an output terminal for coupling the quantum signals to the first input terminal of the at least one logic gate, wherein the unidirectional buffer is configured to propagate quantum signals in only the first direction; and a second unidirectional buffer having a first input terminal for receiving the quantum signals and an output terminal for coupling the quantum signals to the first input terminal of the at least one logic gate, wherein the unidirectional buffer is configured to propagate quantum signals in only the first direction. 18 . The device of claim 17 , wherein the first unidirectional buffer comprises a first inductive loop and wherein the second unidirectional buffer comprises a second inductive loop, and wherein each of the first inductive loop and the second inductive loop is configured to store a current. 19 . The device of claim 18 , wherein each of the first unidirectional buffer and the second unidirectional buffer is configured to propagate the quantum signals in only the first direction when a sum of any stored current in a corresponding inductive loop and any bias current received via a clock signal exceeds a threshold. 20 . The device of claim 17 , wherein the quantum signals comprise single-flux quantum (SFQ) pulses and wherein the SFQ pulses comprise positive SFQ pulses and negative SFQ pulses.
using super-conductive elements · CPC title
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using superconductive devices · CPC title
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