DC Field | Value | Language |
---|---|---|
dc.contributor.author | Oh, Sangchul | - |
dc.contributor.author | Lee, Soonchil | - |
dc.contributor.author | Lee, Hai-woong | - |
dc.date.accessioned | 2007-08-17T01:46:52Z | - |
dc.date.available | 2007-08-17T01:46:52Z | - |
dc.date.issued | 2002-08-27 | - |
dc.identifier.citation | Phys. Rev. A 66, 022316-1 - 022316-5 | en |
dc.identifier.issn | 1050-2947 | - |
dc.identifier.uri | http://prola.aps.org/abstract/PRA/v66/i2/e022316 | - |
dc.identifier.uri | http://hdl.handle.net/10203/1029 | - |
dc.description | ©2002 The American Physical Society URL: http://link.aps.org/abstract/PRA/v66/e022316 DOI: 10.1103/PhysRevA.66.022316 PACS: 03.67.Hk, 03.65.Yz, 03.67.Lx, 05.40.Ca | en |
dc.description.abstract | We investigate quantum teleportation through noisy quantum channels by solving analytically and numerically a master equation in the Lindblad form. We calculate the fidelity as a function of decoherence rates and angles of a state to be teleported. It is found that the average fidelity and the range of states to be accurately teleported depend on types of noises acting on quantum channels. If the quantum channels are subject to isotropic noise, the average fidelity decays to 1/2, which is smaller than the best possible value of 2/3 obtained only by the classical communication. On the other hand, if the noisy quantum channel is modeled by a single Lindblad operator, the average fidelity is always greater than 2/3. | en |
dc.description.sponsorship | We thank Dr. Jaewan Kim for helpful discussions. This work was supported by the Brain Korea 21 Project of the Korea Ministry of Education, the NRL program of the Korean Ministry of Science and Technology, and KOSEF via eSSC at POSTECH. | en |
dc.language.iso | en_US | en |
dc.publisher | American Physical Society | en |
dc.subject | quantum physics | en |
dc.subject | quantum information | en |
dc.title | Fidelity of quantum teleportation through noisy channels | en |
dc.type | Article | en |
dc.identifier.doi | 10.1103/PhysRevA.66.022316 | - |
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