1) W state
W态
1.
Controlled quantum dialogue based on W state;
基于W态的控制量子对话(英文)
2.
Teleportation of an entangled state via the W states;
用W态作量子信道实现纠缠态的隐形传送
3.
Long-distance controlling for the non-classical characteristics of entangled atom in W state in double cavities;
W态纠缠实现双腔远程控制原子的非经典特性
2) W states
W态
1.
Probabilistic teleportation of an N-particle arbitrary and unknown state via W states;
信道为W态的N粒子任意未知态的概率传送
2.
We may make three-particle entanglement using the source of three-particle W states.
利用W态纠缠源可以产生三纠缠粒子,用这些相互纠缠的粒子作为量子信道,再辅以经典信道传送Bell基联合测量信息和von Neumann测量信息,便可实现量子隐形传态网络。
3) entangled W state
纠缠W态
1.
Preparation of entangled W state via resonant interaction of V-type three-level atoms and two-mode cavity-field;
利用V-型三能级原子与双模腔场的共振相互作用制备纠缠W态(英文)
2.
Teleportation of a three-particle entangled W state through two-particle entangled quantum channels;
三粒子纠缠W态的隐形传态
3.
A new protocol of quantum secret sharing for single qubit through an entangled W state is proposed.
提出用纠缠W态来完成单个量子位的量子秘密分享方案。
4) W class state
W类态
1.
Quantum properties of three entangled atoms in W class state interacting with radiation field in coherent state;
W类态三纠缠原子与相干态光场相互作用过程中光场的量子特性
5) general W state
一般W态
1.
Scheme for deterministic quantum teleportation of four-atom entanglement general W state;
四原子一般W态的确定隐形传态方案
2.
In Chapter 4, it discusses the N-qubit general W state.
在第4章中,较为详细地阐述了对于N量子比特体系中一般W态的各方面的研究。
6) W entangled state
W纠缠态
1.
The results show that if the two atoms are prepared in maximun entangled(EPR)state initially,the maximum of three-body entanglement measure is equated with the perfect three-body W entangled state.
研究结果表明:当双原子初始处在EPR态时,三体纠缠量最大值与理想W纠缠态纠缠量相同。
2.
When the field is vacuum and the two atoms stay in Einstein-Podolsky-Rosem entangled state or disentangled state initially, we obtain that the system will evolve to a three-body approximate W entangled state.
在场和两原子初始分别为真空场和纠缠或非纠缠状态下 ,得出体系状态将演化为三体近似W纠缠态 。
补充资料：Frobenius自同态
Frobenius自同态
Froberius endomorphism
I加饭对璐自同态〔Fm加对旧曰吐阅翔解白n;。，o6e，。yea翎八oMo帅.3M] q个元素的有限域乓上概形(scheme)X的自同态咖domo印城m)杯X一X，使得价限制在X(气)上是恒等映射，并且结构层的映射扩:今~今是自乘到q次幂的映射(即把t映到t“).Fro坎对留自同态是纯不可分态射·且具有零微分·对于定义在巩上的仿射簇XC才，F拍b目五出自同态毋把点(x，，…，凡)映到(川，，’‘，对). 定义在巩上的X的几何点的个数等于价的不动点的个数，因此，能够利用1刀台如血公式(此反址忱fo卜m血恤)来确定这些点的个数、义在只上的万履答，.se‘浏’夕翩集合，即“定
说明：补充资料仅用于学习参考，请勿用于其它任何用途。
参考词条