共查询到20条相似文献,搜索用时 604 毫秒
1.
Arun Kumar Pati 《Pramana》2002,59(2):221-228
Entangling an unknown qubit with one type of reference state is generally impossible. However, entangling an unknown qubit
with two types of reference states is possible. To achieve this, we introduce a new class of states called zero sum amplitude (ZSA) multipartite, pure entangled states for qubits and study their salient features. Using shared-ZSA states, local operations
and classical communication, we give a protocol for creating multipartite entangled states of an unknown quantum state with
two types of reference states at remote places. This provides a way of encoding an unknown pure qubit state into a multiqubit
entangled state. 相似文献
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Based on the newly constructed two mutually conjugate 3-mode entangled states of continuum variablesin three-mode Fock space we introduce entangled fractional Fourier transform (EFFT) for the tripartite entangled staterepresentations, which are not a direct product of three 1-dimensional FFTs. The eigenmodes of EFFT are obtained,which is different from the usual Hermite polynomials. The EFFT of the three-mode squeezed state is derived. 相似文献
4.
We deduce entangled fractional Fourier transformation (EFFT) for
the multipartite entangled state representation, which was newly
constructed with two mutually conjugate n-mode entangled states of
continuum variables in n-mode Fock space. We establish a formalism
of EFFT for quantum mechanical wave functions, which provides
us a convenient way to derive some wave functions. We find that
the eigenmode of EFFT is different from the usual Hermite Polynomials.
We also derive the EFFT of the n-mode squeezed state. 相似文献
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FANHong-Yi JIANGNian-Quan 《理论物理通讯》2003,40(1):39-44
Based on the newly constructed two mutually conjugate 3-mode entangled states of continuum variables in three-mode Fock space we introduce entangled fractional Fourier transform (EFFT) for the tripartite entangled state representations, which are not a direct product of three 1-dimensional FFTs. The eigenmodes of EFFT are obtained,which is different from the usual Hermite polynomials. The EFFT of the three-mode squeezed state is derived. 相似文献
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Application of three-mode Einstein-Podolsky-Rosen entangled state with continuous variables to teleportation 下载免费PDF全文
We consider how to teleport two- and three-mode
Einstein--Podolsky--Rosen entangled states (|\eta> and |
pt,\chi2,\chi3>) via a |
pt,\chi2,\chi3> quantum channel for continuous
variables. Using the complete and orthogonal representation of the
entangled states, we can not only find the a complete basis set for
the joint measurement but also propose the specific scheme of
teleportation. Our calculation can be greatly simplified by using
their Schmidt decompositions. 相似文献
9.
Based on the quantum information theory, this paper has investigated
the entanglement properties of a system which is composed of the two
entangled two-level atoms interacting with the two-mode entangled
coherent fields. The influences of the strength of light field and
the two parameters of entanglement between the two-mode fields on
the field entropy and on the negative eigenvalues of partial
transposition of density matrix are discussed by using numerical
calculations. The result shows that the entanglement properties in a
system of a pairwise entangled states can be controlled by
appropriately choosing the two parameters of entanglement between
the two-mode entangled coherent fields and the strength of two light
fields respectively. 相似文献
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We push the limits of the direct use of partially pure entangled states to perform quantum teleportation by presenting several protocols in many different scenarios that achieve the optimal efficiency possible. We review and put in a single formalism the three major strategies known to date that allow one to use partially entangled states for direct quantum teleportation (no distillation strategies permitted) and compare their efficiencies in real world implementations. We show how one can improve the efficiency of many direct teleportation protocols by combining these techniques. We then develop new teleportation protocols employing multipartite partially entangled states. The three techniques are also used here in order to achieve the highest efficiency possible. Finally, we prove the upper bound for the optimal success rate for protocols based on partially entangled Bell states and show that some of the protocols here developed achieve such a bound. 相似文献
12.
A scheme for teleporting a two-particle entangled state via a three-particle entangled state is proposed. It is shown that the probability of successful teleportation is twice the modulus square of the smaller Schmidt coefficient of the entangled three-particle state. 相似文献
13.
By analogy with the bosonic bipartite entangled state we construct fermionic entangled state with the Grassmann numbers. The Wigner operator in the fermionic entangled state representation is introduced, whose marginal distributions are understood in an entangled way. The technique of integration within an ordered product (IWOP) of Fermi operators is used in our discussion. 相似文献
14.
We present an explicit protocol for probabilistic teleport an arbitrary and unknown two-qubit entangled state via a one-dimensional
four-particle non-maximally entangled cluster state. By construction, our four-partite state is not reducible to a pair of
Bell states. We show that teleportation can be successfully realized with a certain probability. This protocol indicate that
the four-qubit state is a likely candidate for the genuine four-particle analogue to a Bell state. 相似文献
15.
介绍了路径纠缠微波及其生成原理,将生成信号以量子力学算符的形式表示,并在光子数态表象下展开,定性地给出了生成信号与压缩参量之间的关系.提出了一种路径纠缠微波信号质量评价方法,即通过信号中纠缠微波光子总数的期望值表征信号的纠缠度,间接实现对信号质量的评价.基于这种信号质量评价方法,提出了一种生成质量最优路径纠缠微波信号的压缩参量选取方法:在近似确定有效纠缠微波光子数的前提下,找出生成不同微波光子数纠缠概率最大时的一组压缩参量值,进而得出各个压缩参量值所对应的一组纠缠微波光子总数的期望值,其中的最大值对应的压缩参量值即为生成质量最优信号所要选择的压缩参量值.通过理论分析,发现路径纠缠微波信号质量由压缩参量决定,且只与压缩幅有关,而与压缩角无关.仿真实验结果表明,在纠缠微波光子数的最大有效值取为"26"时,纠缠微波光子总数期望值的最大值对应的压缩幅值为1.77,即压缩幅取此值时所得到的路径纠缠微波信号质量最佳,仿真结果表明该方法是有效的.本文的研究为路径纠缠微波在实验研究和实际应用中如何生成高质量信号的问题提供了思路. 相似文献
16.
FAN Hong-Yi WANG Ji-Suo 《理论物理通讯》2007,48(2):245-248
By analogy with the bosonic bipartite entangled state we construct fermionic entangled state with the Grassmann numbers. The Wigner operator in the fermionic entangled state representation is introduced, whose marginal distributions are understood in an entangled way. The technique of integration within an ordered product (IWOP) of Fermi operators is used in our discussion. 相似文献
17.
KUANG Mai-Hua MA Shan-Jun LIU Dong-Mei 《理论物理通讯》2008,50(10):867-872
Based on the technique of integral within an ordered product of nonlinear bosonic operators, we construct a new kind of tripartite nonlinear entangled state |α,γ)λ in 3-mode Fock space, which can make up a complete set. We also simply discuss its properties and application. 相似文献
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Paolo Facchi, et al. [Phys. Rev. A77 (2008) 060304(R)] presented a maximally multipartite entangled state (MMES). Here, we give a criterion for the identification of maximally entangled four-qubit states. Using this criterion, we not only identify some existing maximally entangled four-qubit states in the literature, but also find several new maximally entangled four-qubit states as well. 相似文献