Total probability arbitrary multiparty JRSP method
A joint preparation, quantum state technology, applied in the field of communication, can solve the problem of difficult to find a step-by-step preparation strategy for a universal measurement base
Patent Information
- Authority / Receiving Office
- CN · China
- Patent Type
- Applications(China)
- Current Assignee / Owner
- Publication Date
- 2014-03-05
- Estimated Expiration
- Not applicable · inactive patent
Smart Images
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Abstract
Description
technical field
[0001] The invention belongs to the technical field of communication, and specifically refers to a method for remote joint preparation of any multi-party quantum states with full probability. Background technique
[0002] As we all know, current communication channels transmit digital or analog signals. Due to the non-ideal frequency response characteristics of the channel, noise interference and other interference mixed in when the signal is transmitted through the channel, the transmitted signal is damaged and the received signal waveform is distorted or the received digital signal symbol is wrong. For this kind of interference, there are currently two ways to ensure the correct transmission of the channel: one is to improve the performance and quality of lines and transmission equipment, such as using optical fibers; the other is to use error control strategies, such as cyclic redundancy check method Wait. However, improving lines and equipment requires ...
Examples
Embodiment Construction
[0034] A full-probability arbitrary multi-party quantum state remote joint preparation method proposed by the present invention will be described in detail below in conjunction with the accompanying drawings:
[0035] The overall network topology of the present invention is as follows figure 1 As shown, the specific description is as follows:
[0036] Suppose the quantum state to be prepared is There are N+1 participants in total, including N senders and one receiver; among the N senders, one sender is the core sender, and the other N-1 senders are auxiliary senders; N is a natural number. A quantum channel consists of N EPR pairs, namely | Q ⟩ A 1 B 1 A 2 B 2 . . ...