TY - JOUR
T1 - W states fusion via polarization-dependent beam splitter
AU - Li, Ke
AU - Zheng, Dongliang
AU - Xu, Wangqiong
AU - Mao, Huibing
AU - Wang, Jiqing
N1 - Publisher Copyright:
© 2020, Springer Science+Business Media, LLC, part of Springer Nature.
PY - 2020/11
Y1 - 2020/11
N2 - Based on the polarization-dependent beam splitter (PDBS), we propose an optical scheme to fuse small-size polarization entangled W states into a large-scale W states. With the present scheme, two Wm+n+t-2 states can be created from an n-qubit W state, an m-qubit W state and a t-qubit W state, and two Wm+n+t+q-3 states can be generated from Wm, Wn, Wt and Wq states. In the previous fusion schemes, only one particle from each initial W state is allowed to enter the fusion mechanism, but with the progress of experimental technology, two particles can be extracted. In this case, the W states fusion of our scheme will be realized without any ancillary particles and controlled quantum gate. In addition, compared with the one target W state obtained in previous preparation schemes, our scheme can generate two large-scale W states, which effectively improve the success rate of generating target W state. The ability to generate two target W states makes our scheme have a distinct advantage in preparing W states with larger particle numbers. This preparation mechanism also can be generalized to the case of fusing more different or same particles W states.
AB - Based on the polarization-dependent beam splitter (PDBS), we propose an optical scheme to fuse small-size polarization entangled W states into a large-scale W states. With the present scheme, two Wm+n+t-2 states can be created from an n-qubit W state, an m-qubit W state and a t-qubit W state, and two Wm+n+t+q-3 states can be generated from Wm, Wn, Wt and Wq states. In the previous fusion schemes, only one particle from each initial W state is allowed to enter the fusion mechanism, but with the progress of experimental technology, two particles can be extracted. In this case, the W states fusion of our scheme will be realized without any ancillary particles and controlled quantum gate. In addition, compared with the one target W state obtained in previous preparation schemes, our scheme can generate two large-scale W states, which effectively improve the success rate of generating target W state. The ability to generate two target W states makes our scheme have a distinct advantage in preparing W states with larger particle numbers. This preparation mechanism also can be generalized to the case of fusing more different or same particles W states.
KW - Polarization-dependent beam splitter
KW - State fusion
KW - W state
UR - https://www.scopus.com/pages/publications/85095971431
U2 - 10.1007/s11128-020-02898-w
DO - 10.1007/s11128-020-02898-w
M3 - 文章
AN - SCOPUS:85095971431
SN - 1570-0755
VL - 19
JO - Quantum Information Processing
JF - Quantum Information Processing
IS - 11
M1 - 412
ER -