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US Patent 10386229 Gated superconducting photon detector

Patent 10386229 was granted and assigned to PsiQuantum on August, 2019 by the United States Patent and Trademark Office.

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Patent
Patent

Patent attributes

Patent Applicant
PsiQuantum
PsiQuantum
Current Assignee
PsiQuantum
PsiQuantum
Patent Jurisdiction
United States Patent and Trademark Office
United States Patent and Trademark Office
Patent Number
10386229
Date of Patent
August 20, 2019
Patent Application Number
16028293
Date Filed
July 5, 2018
Patent Citations
‌
US Patent 10186858 Device for a current limiter and a current limiter comprising said device
‌
US Patent 10171086 Superconducting three-terminal device and logic gates
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US Patent 10103736 Four-input Josephson gates
Patent Citations Received
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US Patent 12119820 Superconducting field-programmable gate array
0
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US Patent 11475945 Superconductive memory cells and devices
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US Patent 12095462 Superconducting logic circuits
0
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US Patent 12107375 Methods and devices for impedance multiplication
0
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US Patent 11473974 Superconducting photon detector
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US Patent 11569816 Superconducting switch
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US Patent 10879905 Superconducting field-programmable gate array
‌
US Patent 10897235 Superconducting signal amplifier
...
Patent Primary Examiner
‌
Thanh Luu
Patent abstract

The various embodiments described herein include methods, devices, and systems for fabricating and operating photodetector circuitry. In one aspect, a photon detector system includes: (1) a first superconducting wire having a first threshold superconducting current; (2) a second superconducting wire having a second threshold superconducting current; (3) a resistor coupled to the first wire and the second wire; (4) current source(s) coupled to the first wire and configured to supply a current that is below the second threshold current; and (3) a second circuit coupled to the second wire. In response to receiving light at the first wire, the first wire transitions from a superconducting state to a non-superconducting state. In response to receiving light at the second wire while the first wire is in the non-superconducting state, the second wire transitions to a non-superconducting state, redirecting the first current to the second circuit.

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