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Spontaneous Emission of a Two-Level Static Atom Coupling with Electromagnetic Vacuum Fluctuations Outside a High-Dimensional Einstein Gauss-Bonnet Black Hole |
| ZHANG Ming1, YANG Zhan-Ying1, YUE Rui-Hong2** |
1School of Physics, Northwest University, Xi'an 710069
2Faculty of Science, Ningbo University, Ningbo 315211
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| Cite this article: |
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ZHANG Ming, YANG Zhan-Ying, YUE Rui-Hong 2014 Chin. Phys. Lett. 31 100401 |
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Abstract Using the generalized formalism of Dalibard, Dupont-Roc and Cohen-Tannoudji we investigate the spontaneous excitation of a static atom interacting with electromagnetic vacuum fluctuations outside an Einstein Gauss-Bonnet black hole in d-dimensions. It shows that spontaneous excitation does not occur in a Boulware vacuum, while exists in an Unruh vacuum and Hartle–Hawking vacuum. As to the total rate of change of the atomic energy, it does not receive the contribution from the coupling constant of the Gauss–Bonnet term at spatial infinity, only the dimensional parameter has the contribution to it. Near the event horizon, both the coupling constant and the dimension p contribute to the total rate of change of the atomic energy in all three kinds of vacuum. We discuss the contribution of the coupling constant and dimensional factor to the results in three different kinds of spacetime lastly.
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Published: 31 October 2014
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| PACS: |
04.62.+v
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(Quantum fields in curved spacetime)
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04.50.Gh
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(Higher-dimensional black holes, black strings, and related objects)
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03.70.+k
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(Theory of quantized fields)
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