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Physics Letters A

A probabilistic cloning machine for replicating two non-orthogonal states

L.-M. Duan, Guang‐Can Guo

Published Jul 1, 1998• 114 citations
Publisher
DOI
10.1016/s0375-9601(98)00287-4

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Is It Possible To Clone Using An Arbitrary Blank State?

Roy, A, Ujjwal Sen, Sen, U

We show that using a fixed cloning machine, whether deterministic inexact or probabilistic exact, one can take an arbitrary blank state. Quantum information cannot be cloned. There cannot exist a machine which can produce two (or more) exact copies of an arbitrary state in a deterministic manner [1]. Replication is not allowed even when the input state is taken at random from a given set of two non-orthogonal states [2]. It has been further shown that probabilistic cloning is not possible if the input state is from a given linearly dependent set [3]. Henceforth we deal explicitly with qubits although all the results can be extended to higher dimensions. Although exact cloning is not possible, one can approximately clone an arbitrary input state [4, 5, 6]. In this scheme a fixed state is taken as the blank state, depending on which and the initial machine state, the cloning operation is constructed. We extend this operation such that any arbitrary (pure or mixed) state taken as the blank copy can do the job. The optimal universal 1 → 2 inexact qubit cloner of Brußet al.[5] takes an arbitrary qubit |ψ 〉 〈ψ | = 1 2 (I + − → s. − → σ) along with a fixed blank qubit |b 〉 and a machine state |M 〉 as input. An entangled state of the three qubits is produced as the output such that the reduced density matrices of the first two qubits are two similar approximate copies ρ = 1 2 (I + η− → s. − → σ) of |ψ 〉 〈ψ | with η = 2 3. The unitary operator realizing this process is defined on the combined Hilbert space of the input qubit, the blank qubit and machine by U ′ √ √

•Jan 1, 2001•1 citation

Probabilistic Cloning of Three Real States with Optimal Success Probabilities

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International Journal of Theoretical Physics•Mar 14, 2017•1 citation

No-Cloning Theorem and Quantum Cloning Machines

S. Rajasekar, R. Velusamy

This chapter begins by providing proofs of no-cloning and no-broadcasting theorems. No-cloning theorem makes it possible to detect any eavesdropper on a quantum communication channel. The chapter presents the features of some of the quantum cloning machines. In spite of the no-cloning theorem, it is quite possible to construct a quantum cloning machine which copies an unknown state approximately. A probabilistic cloning machine has been proposed which can succeed only with a probability. When it succeeds it will give a perfect copy. This probabilistic quantum cloning is much useful in studying the B92 quantum key distribution protocol which involves only two non-orthogonal states and we can try to clone it with the largest probability. A telecloning scheme combines cloning with teleportation. A quantum telecloning system for two-level system in which one input is sent to M-receivers has been proposed. The no-hiding theorem is found to have applications in black hole evaporation, quantum teleportation and private quantum channels.

CRC Press eBooks•Oct 5, 2022•0 citations
We show that using a fixed cloning machine, whether deterministic inexact or probabilistic exact, one can take an arbitrary blank state. Quantum information cannot be cloned. There cannot exist a machine which can produce two (or more) exact copies of an arbitrary state in a deterministic manner [1]. Replication is not allowed even when the input state is taken at random from a given set of two non-orthogonal states [2]. It has been further shown that probabilistic cloning is not possible if the input state is from a given linearly dependent set [3]. Henceforth we deal explicitly with qubits although all the results can be extended to higher dimensions. Although exact cloning is not possible, one can approximately clone an arbitrary input state [4, 5, 6]. In this scheme a fixed state is taken as the blank state, depending on which and the initial machine state, the cloning operation is constructed. We extend this operation such that any arbitrary (pure or mixed) state taken as the blank copy can do the job. The optimal universal 1 → 2 inexact qubit cloner of Brußet al.[5] takes an arbitrary qubit |ψ 〉 〈ψ | = 1 2 (I + − → s. − → σ) along with a fixed blank qubit |b 〉 and a machine state |M 〉 as input. An entangled state of the three qubits is produced as the output such that the reduced density matrices of the first two qubits are two similar approximate copies ρ = 1 2 (I + η− → s. − → σ) of |ψ 〉 〈ψ | with η = 2 3. The unitary operator realizing this process is defined on the combined Hilbert space of the input qubit, the blank qubit and machine by U ′ √ √
This chapter begins by providing proofs of no-cloning and no-broadcasting theorems. No-cloning theorem makes it possible to detect any eavesdropper on a quantum communication channel. The chapter presents the features of some of the quantum cloning machines. In spite of the no-cloning theorem, it is quite possible to construct a quantum cloning machine which copies an unknown state approximately. A probabilistic cloning machine has been proposed which can succeed only with a probability. When it succeeds it will give a perfect copy. This probabilistic quantum cloning is much useful in studying the B92 quantum key distribution protocol which involves only two non-orthogonal states and we can try to clone it with the largest probability. A telecloning scheme combines cloning with teleportation. A quantum telecloning system for two-level system in which one input is sent to M-receivers has been proposed. The no-hiding theorem is found to have applications in black hole evaporation, quantum teleportation and private quantum channels.