亚洲免费av电影一区二区三区,日韩爱爱视频,51精品视频一区二区三区,91视频爱爱,日韩欧美在线播放视频,中文字幕少妇AV,亚洲电影中文字幕,久久久久亚洲av成人网址,久久综合视频网站,国产在线不卡免费播放

        ?

        Scheme for Asymmetric and Deterministic Controlled Bidirectional Joint Remote State Preparation?

        2018-11-19 02:22:30JinShi施錦andYouBangZhan詹佑邦
        Communications in Theoretical Physics 2018年11期

        Jin Shi(施錦) and You-Bang Zhan(詹佑邦)

        School of Physics and Electronic Electrical Engineering,Jiangsu Province Key Laboratory of Modern Measurement Technology and Intellige,Huaiyin Normal University,Huaian 223300,China

        AbstractThe scheme for asymmetric and deterministic controlled bidirectional joint remote state preparation by using one ten-qubit entangled state as the quantum channel is proposed.In this scheme,Alice and David want to remotely prepare an arbitrary single-qubit state at Bob’s site,at the same time,Bob and Eve wish to help Alice remotely prepare an arbitrary two-qubit entangled state.Alice and Bob can simultaneously prepare the desired states with the cooperation of David and Eve under the control of Charlie.

        Key words:joint remote state preparation,entangled state,unitary transformation

        1 Introduction

        As the carrier of information,quantum states are easily intercepted or replaced by eavesdroppers when direct transmission.Quantum teleportation(QT)[1]and remote state preparation(RSP)[2?4]are two important techniques for transferring information in quantum communication.Based on quantum entanglement,many QT and RSP schemes can be realized via local operations and classical communication.Different from QT protocols,the prepared state is completely known to the sender in RSP schemes.RSP can consume less resources than QT,especially for reconstructing large quantum states.RSP protocols are widely used in quantum information.Various theoretical and experimental RSP schemes[5?16]have been proposed.

        In order to avoid the combination of information concentrated on one person,joint remote state preparation(JRSP)schemes[17?37]have been put forward.Each of senders knows partly the state to be prepared in JRSP,which is a secure method for transmitting quantum state.Deterministic joint remote state preparation is that the total successful probability reaches 100%.[32?37]Recently,as the new type of quantum communication schemes,bidirectional RSP schemes include symmetric bidirectional RSP[38?41]and asymmetric bidirectional RSP[42?46]have been proposed.The schemes of controlled bidirectional RSP(CBRSP)were presented.[47?48]The distant collaborators can simultaneously prepare the desired states with permission of the controller in CBRSP protocols.

        In this paper,a novel scheme for asymmetric and deterministic controlled bidirectional JRSP(CBJRSP)is proposed by using one ten-qubit entangled state as the quantum channel.In our asymmetric and deterministic CBJRSP scheme,Alice and David wish to remotely prepare an arbitrary single-qubit state at distant Bob’s site,meanwhile,Bob and Eve want to remotely prepare an arbitrary two-qubit state at distant Alice’s site under the control of the supervisor Charlie.It is shown that,only if the controller Charlie agrees to collaborate with four senders,they can remotely prepare the desired states by means of some appropriate basis vectors measurement and unitary operations.

        2 Asymmetric and Deterministic CBJRSP by Using One Ten-Qubit Entangled State

        Since bidirectional QT schemes and bidirectional JRSP schemes by using multi-qubit entangled state have been reported in many papers,we try to propose the scheme for asymmetric and deterministic CBJRSP by using one ten-qubit entangled state as the quantum channel in this section.Suppose Alice and David wish to help Bob remotely prepare an arbitrary one-qubit state|??,at the same time,Bob and Eve wish to help Alice remotely prepare an arbitrary two-qubit stateunder the control of Charlie.

        where modulus coefficients(x,y,a,b,c and d)are real and x2+y2=1,a2+b2+c2+d2=1.Alice knows modulus coefficients(x and y).David knows phase coefficient θ.Bob knows modulus coefficients(a,b,c and d).Eve knows phase coefficients αj,(j=1,2,3).Alice,Bob,Charlie,David,and Eve share one ten-qubit entangled state as the quantum channel.

        where the qubits 1,9,and 10 belong to Alice,the qubits 3,5,and 6 belong to Bob,the qubit 4 belongs to Charlie,the qubit 2 belongs to David,the qubits 7 and 8 belong to Eve.As shown in Fig.1,we have presented the sketch of the protocol for CBJRSP via a ten-qubit entangled state as the quantum channel.

        Fig.1 The sketch of our CBJRSP protocol.

        Asymmetric and deterministic CBJRSP can be realized under control of Charlie.The controller Charlie performs a one-qubit measurement on the qubit 4 under the measuring basis{|+?,|??}.If the measuring result is|+?4,then the statecan be transformed into

        Alice operates CNOT on her qubits 1 and 9.The qubit 1 as controlled qubit and the qubit 9 as target qubit(C1NOT9).Bob also operates CNOT on his qubits 3 and 5.The qubit 3 as controlled qubit and the qubit 5 as target qubit(C3NOT5).Then the statecan be transformed into

        The state can be rewritten as

        Alice operates C1NOT9on her qubits 1 and 9.Bob also operates C3NOT5on his qubits 3 and 5.Then the statecan be transformed into

        The state can be rewritten as

        In order to complete the asymmetric and deterministic CBJRSP,Alice chooses a set of mutually orthogonal basis vectorsas the measuring basis of the qubit 1,which are given by

        where γ is given

        David chooses a set of mutually orthogonal basis vectorsas the measuring basis of the qubit 2,which are given by

        where

        Bob chooses a set of mutually orthogonal basis vectorsas the measuring basis of the qubits 5 and 6,which are given by

        where B is given

        Eve chooses a set of mutually orthogonal basis vectorsas the measuring basis of the qubits 7 and 8,which are given by

        where

        Suppose the measuring results areandthe state can be expressed as

        Bob makes unitary transformation(I)3.Alice operates controlled σzgate.The qubit 9 as controlled qubit and qubit 10 as target qubitThen Alice and David help Bob remotely prepare the one-qubit stateBob and Eve help Alice remotely prepare the two-qubit state

        simultaneously. If Charlie’s measuring result isBob makes unitary transformation(σz)3.Alice operates.Then Alice and David help Bob remotely prepareAt the same time,Bob and Eve help Alice remotely prepare the two-qubit stateAll measuring results and operations of Alice and Bob,the measuring results of David and Eve are listed in Table 1.As we can see from Table 1,the measuring results are,then Bob makes unitary transformation(I)3.Bob can obtain one-qubit stateAlice makes unitary transformation,and(σx)9.Alice can obtain two-qubit state

        Table 1 The measuring results and operations of Alice and Bob,the measuring results of David and Eve.

        Table 1(continued)

        Table 1(continued)

        3 Conclusion

        In summary,by using basis vectors measurement,controlled not gate operation,controlled σzgate operation,and appropriate unitary transformations,the new scheme for asymmetric and deterministic CBJRSP is proposed.In this scheme,Alice and David remotely prepare an arbitrary single-qubit state at distant Bob’s site.Meanwhile,Bob and Eve remotely prepare an arbitrary twoqubit state at distant Alice’s site under the control of Charlie.Our CBJRSP process can be divided into two JRSP processes with only one controller.Different from former controlled JRSP schemes,the asymmetric and deterministic CBJRSP scheme proposed in this paper has higher efficiency and lower resource costs.The asymmetric and deterministic CBJRSP scheme herein has many potential applications in the field of quantum information.For example,in our asymmetric and deterministic CBJRSP scheme,Alice and Bob can exchange their quantum states simultaneously with the cooperators under the controller Charlie,which can realize long-distance safe transmission of information.Similarly,the asymmetric and deterministic CBJRSP scheme can be extended to CBJRSP of N(N>2)different M-qubit(M>2)quantum states.Multi-party exchange their quantum states at the same time with the cooperators under the controller,which can be applied in the quantum internet.Compared with other bidirectional JRSP protocols,our scheme is more secret.We have provided a new way to construct safer quantum channel for quantum secure communication.

        日韩国产成人精品视频| 女人高潮被爽到呻吟在线观看| 与漂亮的女邻居少妇好爽 | 精品人妻码一区二区三区剧情| 天天躁夜夜躁狠狠是什么心态| 亚洲av日韩av天堂久久| 国产性生大片免费观看性| 玩两个丰满老熟女| 日韩免费小视频| 亚洲精品综合色区二区| 亚洲在线视频一区二区| 日韩一区三区av在线| 成人偷拍自拍视频在线观看 | 亚洲一区二区视频蜜桃| 精品人妻在线一区二区三区在线 | 午夜精品一区二区久久做老熟女| 国产精品亚洲在线播放| 丰满人妻中文字幕一区三区| 国产极品粉嫩福利姬萌白酱| 99久久免费国产精品| 亚洲国产高清在线一区二区三区 | 精品av熟女一区二区偷窥海滩| 99久久久国产精品免费蜜臀| 亚洲人成人77777网站| 久久er这里都是精品23| 内射爆草少妇精品视频| 国产大屁股视频免费区| 亚洲熟妇无码一区二区三区导航 | 国产精品成人无码a 无码| 成人性生交大片免费看激情玛丽莎| 成人性生交大片免费5| 大尺度免费观看av网站| 777米奇色8888狠狠俺去啦| 日日鲁鲁鲁夜夜爽爽狠狠视频97| 亚洲aⅴ无码国精品中文字慕| 人妻少妇精品一区二区三区| 亚洲av一区二区在线| 在线人成视频播放午夜| 7777奇米四色成人眼影| 91网站在线看| 久久精品国产亚洲av热九|