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dc.creatorWang, Da-wei
dc.creatorLi, Ai-jun
dc.creatorWang, Li-gang
dc.creatorZhu, Shi-yao
dc.creatorZubairy, M. Suhail
dc.date.accessioned2011-09-08T21:36:39Z
dc.date.available2011-09-08T21:36:39Z
dc.date.issued2009
dc.identifier.citationDa-wei Wang, Ai-jun Li, Li-gang Wang, Shi-yao Zhu and M. Suhail Zubairy. Phys.Rev.A 80 063826 2009. "Copyright (2009) by the American Physical Society."en
dc.identifier.urihttp://dx.doi.org/10.1103/PhysRevA.80.063826
dc.identifier.urihttps://hdl.handle.net/1969.1/126636
dc.descriptionJournals published by the American Physical Society can be found at http://publish.aps.org/en
dc.description.abstractThe effect of the counterrotating terms on the linear polarizability is investigated, which is responsible for the validity of the optical theorem in all frequency regions. A unitary transformation method [H. Zheng, S. -Y. Zhu, and M. S. Zubairy, Rev. Lett. 101, 200404 (2008)] is adopted to overcome the difficulty brought in by the counterrotating terms, which yields a rotating-wave-approximation-like Hamiltonian with modified coupling constant due to the counterrotating terms. A simple expression for the polarizability is obtained, which is a sum of resonant (minus sign) and antiresonant (plus sign) parts, and from which the role of the counterrotating terms and quantum interference between the counterrotating terms and rotating terms at far off-resonance are discussed.en
dc.language.isoen
dc.publisherAmerican Physical Society
dc.subjectOpticsen
dc.subjectPhysicsen
dc.titleEffect of the counterrotating terms on polarizability in atom-field interactionsen
dc.typeArticleen
local.departmentPhysics and Astronomyen


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