Author Affiliations
1Department of Electronic Information Engineering, Nanchang University, Nanchang 330031, China2State Key Laboratory of Low-Dimensional Quantum Physics, Department of Physics, Tsinghua Universtiy, Beijing 100084, China3Institute for Advanced Study, Nanchang University, Nanchang 330031, Chinashow less
Fig. 1. Schematic diagram of the nanomechanical resonator coupled with a qubit.NAMR-量子比特系统的物理模型图
Fig. 2. Schematic energy-level diagram explaining the occurrence of the phonon blockade by the driving field satisfying the resonance condition: (a) Energy-level diagram when Eqs. (8) are satisfied, where
and
; (b) energy-level diagram when Eqs. (9) are satisfied, where
and
.
外加驱动场共振的情况下声子阻塞现象的能级图 (a)满足(8)式时的能级图, 其中
和
; (b)满足(9)式时的能级图, 其中
和
Fig. 3. Logarithmic plot (of base e) of the zero-delay-time second-order correlation functions
as a function of
for different
with
: (a)
,
,
; (b)
,
,
.
在不同的
关系下, 二阶关联函数
与
的关系图 (a)
,
,
,
; (b)
,
,
,
Fig. 4. Schematic energy-level diagram of unconventional phonon blockade.UPNB能级图
Fig. 5. Different parameter range for the CPNB, the UPNB, and the present scheme.本文方案与CPNB和UPNB的区别
Fig. 6. The logarithmic plot (of base e) of the zero-delay-time second-order correlation functions
and average photon numberN: (a) and (b)
,
; (c) and (d)
,
,
. The shared parameters:
.
二阶关联函数
和平均声子数
的对数图像 (a), (b)
,
; (c), (d)
,
,
. 其他参数为
.
Fig. 7. The logarithmic plot (of base e) of the zero-delay-time second-order correlation functions
as a function of
. The shared parameters:
,
. Other parameters: (a)
,
(our scheme),
(UPNB); (b)
,
(our scheme),
(CPNB).
二阶关联函数
(对数)与
的关系图, 其中
,
(a)
,
(本文方案),
(UPNB); (b)
,
(本文方案),
(CPNB)
Fig. 8. The logarithmic plot (of base e) of the zero-delay-time second-order correlation functions
as a function of
:
,
,
. Other parameters: (a)
,
,
(our scheme),
(UPNB); (b)
,
,
(our scheme),
(CPNB).
二阶关联函数
(对数)与
的关系图,
,
,
(a)
,
,
(本文方案),
(UPNB); (b)
,
,
(本文方案),
(CPNB)
Fig. 9. The detecting model of the statistical properties of the phonons.声子统计特性探测模型