Kono S, Masuyama Y, Ishikawa T, Tabuchi Y, Yamazaki R, Usami K, Koshino K, Nakamura Y
Research Center for Advanced Science and Technology (RCAST), The University of Tokyo, Meguro-ku, Tokyo 153-8904, Japan.
College of Liberal Arts and Sciences, Tokyo Medical and Dental University, Ichikawa, Chiba 272-0827, Japan.
Phys Rev Lett. 2017 Jul 14;119(2):023602. doi: 10.1103/PhysRevLett.119.023602. Epub 2017 Jul 13.
A superconducting qubit in the strong dispersive regime of circuit quantum electrodynamics is a powerful probe for microwave photons in a cavity mode. In this regime, a qubit excitation spectrum is split into multiple peaks, with each peak corresponding to an individual photon number in the cavity (discrete ac Stark shift). Here, we measure the qubit spectrum in a cavity that is driven continuously with a squeezed vacuum generated by a Josephson parametric amplifier. By fitting the obtained spectrum with a model which takes into account the finite qubit excitation power, we determine the photon number distribution, which reveals an even-odd photon number oscillation and quantitatively fulfills Klyshko's criterion for nonclassicality.
处于电路量子电动力学强色散 regime 中的超导量子比特是用于探测腔模中微波光子的强大探针。在该 regime 中,量子比特激发谱被分裂成多个峰,每个峰对应于腔中的单个光子数(离散交流斯塔克位移)。在此,我们测量了一个由约瑟夫森参量放大器产生的压缩真空连续驱动的腔中的量子比特谱。通过用一个考虑了有限量子比特激发功率的模型对获得的谱进行拟合,我们确定了光子数分布,该分布揭示了奇偶光子数振荡并定量地满足了 Klyshko 的非经典性判据。