发明名称 CONSTRUCTING AND PROGRAMMING QUANTUM HARDWARE FOR QUANTUM ANNEALING PROCESSES
摘要 Methods, systems, and apparatus, including computer programs encoded on computer storage media, for constructing and programming quantum hardware for quantum annealing processes.
申请公布号 US2016328659(A1) 申请公布日期 2016.11.10
申请号 US201415109600 申请日期 2014.12.31
申请人 Google Inc. 发明人 MOHSENI Masoud;NEVEN Hartmut
分类号 G06N99/00;H01L39/22;G06F15/82;H01L39/02 主分类号 G06N99/00
代理机构 代理人
主权项 1. An apparatus comprising: a first pair of logical superconducting units for use in computation, each logical superconducting unit being configured to have quantum states that can be spanned over Pauli operator σsji, where i=x, y, or z; a first pair of control superconducting units for use in assisting the computation without being a computational unit, each control superconducting unit being configured to have quantum states that can be spanned over Pauli operator σcki, where i=x, y, or z; a first coupler between a first logical superconducting unit and a second logical superconducting unit, wherein when a magnetic field is applied along a z direction, the first coupler couples a quantum operator σs1z of the first logical superconducting unit with a quantum operator σs2z of the second logical superconducting unit in a first coupling represented by σs1z σs2z; a second coupler between a first control logical superconducting unit and a control second superconducting unit, wherein when a magnetic field is applied along a z direction, the second coupler couples a quantum operator σc1z of the first control superconducting unit with a quantum operator σc2z of the second control superconducting unit in a second coupling represented by σc1z σc2z; a third coupler between the first logical superconducting unit and the second control superconducting unit, wherein when the magnetic field along the z direction is applied, the third coupler couples a quantum operator σs1z of the first superconducting unit with a quantum operator σc2z of the second superconducting unit in a third coupling represented by σs1xσc2z; and a fourth coupler between the second logical superconducting unit and the first control superconducting unit, wherein when the magnetic field along the z direction is applied, the fourth coupler couples a quantum operator σs2z of the first superconducting unit with a quantum operator σc1z of the second superconducting unit in a fourth coupling represented by σs2xσc1z.
地址 Mountain View CA US