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Superconducting non-destructive readout circuits

專利號
US10868540B2
公開日期
2020-12-15
申請人
Anna Y. Herr; Quentin P. Herr; Ryan Edward Clarke; Harold Clifton Hearne, III; Alexander Louis Braun; Randall M. Burnett; Timothy Chi-Chao Lee(US VA Falls Church)
發(fā)明人
Anna Y. Herr; Quentin P. Herr; Ryan Edward Clarke; Harold Clifton Hearne, III; Alexander Louis Braun; Randall M. Burnett; Timothy Chi-Chao Lee
IPC分類
H03K19/195; G11C11/44; H03K3/38; G06N10/00
技術(shù)領(lǐng)域
josephson,ndro,rql,junction,lclk,input,circuit,tail,j2,logical
地域: MD MD Ellicott City

摘要

Non-destructive read out (NDRO) circuits are provided for use in reciprocal quantum logic (RQL) superconducting systems. Each NDRO circuit includes a “body” circuit that provides a single or multi-state sub-critical bias current to one or many independent “tail” circuitries. Each “tail” has minimal effect on the “body” thereby preventing any interference or destruction to the state of the “body” circuitry. The circuits reduce device count and thereby increase circuit density, simplify and reduce the cost of fabrication, and provide functionality not available in existing designs, such as the ability to write a state and read it in the same operation cycle. The NDRO circuits provide more compact unit cells useful in memory or logic arrays, demanding fewer resources with increased functionality. The circuits also provide compact cells for AND, AND-OR, A-NOT-B, inverter, multiplexer, and demultiplexer gates.

說明書

In single-read RQL D-register circuit 700, Josephson junction J2 junction triggers when the logical lock input LCLK goes “high” (i.e., when a positive SFQ pulse is provided on the logical clock input LCLK to assert the logical clock input), bringing the superconducting phase of Josephson junction J2 to 2π radians (“high”). The phase of Josephson junction J2 remains “high” if the data input DI is asserted (i.e., with a positive SFQ pulse introduced to data input DI) upon the falling edge of the logical clock signal provided on input LCLK. Josephson junction J2 will “flip back” (i.e., its phase will return to 0 radians, “l(fā)ow”) if data input DI is unasserted (“l(fā)ow”) during this time. Consequently, the superconducting phase of Josephson junction J2 determines the internal state of the body 702 of RQL D-register circuit 700. Thus, for example, Josephson junction J2 having a 2π radian superconducting phase can correspond to a stored “1” (logical “high”) value, whereas Josephson junction J2 having a 0 radian superconducting phase can correspond to a stored “0” (logical “l(fā)ow”). In particular, the stored state corresponds to the phase of state-storing Josephson junction J2 during the latter half of an operation cycle, as can be noted in timing diagram 1000, particularly during “write 0” operations.

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