Superconducting quantum circuit to simulate the dynamical Casimir effect in a double cavity

被引:0
|
作者
Sanso, Jean Paul Louys [1 ,2 ]
Del Grosso, Nicolas F. [1 ,3 ]
Lombardo, Fernando C. [1 ,3 ]
Villar, Paula I. [1 ,3 ]
机构
[1] FCEyN UBA, Fac Ciencias Exactas & Nat, Dept Fis Juan Jose Giambiagi, Ciudad Univ,Pabellon 1, RA-1428 Buenos Aires, Argentina
[2] Univ Innsbruck, Inst Expt Phys, Technikerstr 25, A-6020 Innsbruck, Austria
[3] IFIBA CONICET UBA, Fac Ciencias Exactas & Nat, Ciudad Univ,Pabellon 1, RA-1428 Buenos Aires, Argentina
基金
奥地利科学基金会;
关键词
MOVING MIRROR; RADIATION; CREATION; PHOTONS; VACUUM; TIME;
D O I
10.1103/PhysRevA.111.013714
中图分类号
O43 [光学];
学科分类号
070207 ; 0803 ;
摘要
In this work we study simulations of photon generation due to the dynamical Casimir effect (DCE) in a onedimensional (1 + 1) double superconducting cavity. To achieve this, we propose the use of a superconducting quantum circuit so as to be able to experimentally perform quantum simulations of the DCE. The simulated cavity consists of two perfectly conducting mirrors and a dielectric membrane of infinitesimal depth that effectively couples two cavities. The total length of the double cavity L, the difference in length between the two cavities AL, and the electric susceptibility chi and conductivity v of the dielectric membrane are tunable parameters. All four parameters are treated as independent and are allowed to be tuned at the same time, even with different frequencies. We analyze the cavity's energy spectra under different conditions, finding a transition between two distinct regimes that is accurately described by kc= root v/chi. In particular, a lowest-energy mode is forbidden in one of the regimes while it is allowed in the other. We compare analytical approximations obtained through the multiple-scale analysis method with exact numerical solutions, obtaining the typical results when chi is not being tuned. However, when the susceptibility chi is tuned, different behaviors (such as oscillations in the number of photons of a cavity prepared in a vacuum state) can arise if the frequencies and amplitudes of all parameters are adequate. These oscillations might be considered as adiabatic shortcuts where all generated photons are eventually destroyed.
引用
收藏
页数:20
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