3 and the optical pulse ν4" based on the value dependent on the number of photons of the optical pulse ν3 and ν4, and determines failure in sharing of quantum tangle when it is estimated that "there is no difference in the number of photons contained in the optical pulse ν3 and the optical pulse ν4".;COPYRIGHT: (C)2013,JPO&INPIT"/> Quantum entanglement generation system, entanglement generation method
首页> 外国专利> Quantum entanglement generation system, entanglement generation method

Quantum entanglement generation system, entanglement generation method

机译:量子纠缠产生系统,纠缠产生方法

摘要

PROBLEM TO BE SOLVED: To provide a quantum tangle generation system capable of attaining an efficiency close to a theoretical limit in a case where kinds of error is not limited because no limitation is paused on kinds of error.;SOLUTION: A transmission device includes a first quantum tangle generation section in which a quantum tangle state is generated between a quantum bit A and optical pulse μ, and the optical pulse μ is transmitted to a reception device. The reception device includes a second quantum tangle generation section for generating a quantum tangle state, a detection light generation section which receives optical pulses ν1 and ν2 and generates optical pulses ν3 and ν4, a detection section which measures a value dependent on the number of photons of the optical pulses ν3 and ν4, and a determination section which determines success of sharing of quantum tangle when it is estimated that "there is a difference between the number of photons contained in the optical pulse ν3 and the optical pulse ν4" based on the value dependent on the number of photons of the optical pulse ν3 and ν4, and determines failure in sharing of quantum tangle when it is estimated that "there is no difference in the number of photons contained in the optical pulse ν3 and the optical pulse ν4".;COPYRIGHT: (C)2013,JPO&INPIT
机译:解决的问题:提供一种量子纠缠发生系统,该系统在不限制各种错误的情况下能够获得接近于理论极限的效率,因为没有对任何错误进行限制。第一量子缠结产生部分,其中在量子比特A和光脉冲μ之间产生量子缠结状态,并且光脉冲μ被发送到接收装置。该接收装置包括:第二量子缠结产生部分,用于产生量子缠结状态;检测光产生部分,接收光脉冲ν 1 和ν 2 并产生光脉冲ν 3 和ν 4 ,一个检测部分,根据光脉冲ν 3 和ν的光子数测量值4 ,以及确定部,当估计“光脉冲ν 3 中包含的光子数与光的数量之间存在差异时,确定量子纠缠的共享成功与否。根据与光脉冲ν 3 和ν 4 的光子数相关的值,确定ν 4 脉冲,并确定共享失败估计“在光脉冲ν 3 和光脉冲ν 4 中包含的光子数量没有差异”时的量子纠缠度; COPYRIGHT: (C)2013,日本特许厅&INPIT

著录项

  • 公开/公告号JP5526087B2

    专利类型

  • 公开/公告日2014-06-18

    原文格式PDF

  • 申请/专利权人 日本電信電話株式会社;

    申请/专利号JP20110173031

  • 发明设计人 東 浩司;加藤 豪;

    申请日2011-08-08

  • 分类号H04B10/70;

  • 国家 JP

  • 入库时间 2022-08-21 16:16:08

相似文献

  • 专利
  • 外文文献
  • 中文文献
获取专利

客服邮箱:kefu@zhangqiaokeyan.com

京公网安备:11010802029741号 ICP备案号:京ICP备15016152号-6 六维联合信息科技 (北京) 有限公司©版权所有
  • 客服微信

  • 服务号