Robust creation and phase-sensitive probing of superposition states via stimulated Raman adiabatic passage (STIRAP) with degenerate dark states
We describe a method for creating an arbitrary coherent superposition of two atomic states in a controlled and robust way by using a sequence of three pulses in a four-state system. The proposed technique is based on the existence of two degenerate dark states (i.e. states having no component of the...
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| Published in: | Optics communications Vol. 155; no. 1; pp. 144 - 154 |
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| Main Authors: | , , , |
| Format: | Journal Article |
| Language: | English |
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Elsevier B.V
01-10-1998
Elsevier Science |
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| Abstract | We describe a method for creating an arbitrary coherent superposition of two atomic states in a controlled and robust way by using a sequence of three pulses in a four-state system. The proposed technique is based on the existence of two degenerate dark states (i.e. states having no component of the excited state) and their interaction. The mixing of the dark states can be controlled by changing the relative delay of the pulses, and thus an arbitrary superposition state can be generated. It is shown that the method is robust against small variations of parameters (e.g. the area of the pulses) and is insensitive to radiative decay from the intermediate excited state. A time reversed version of the technique makes possible the determination of phase occurring in a superposition of two atomic states. |
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| AbstractList | We describe a method for creating an arbitrary coherent superposition of two atomic states in a controlled and robust way by using a sequence of three pulses in a four-state system. The proposed technique is based on the existence of two degenerate dark states (i.e. states having no component of the excited state) and their interaction. The mixing of the dark states can be controlled by changing the relative delay of the pulses, and thus an arbitrary superposition state can be generated. It is shown that the method is robust against small variations of parameters (e.g. the area of the pulses) and is insensitive to radiative decay from the intermediate excited state. A time reversed version of the technique makes possible the determination of phase occurring in a superposition of two atomic states. |
| Author | Fleischhauer, M. Bergmann, K. Shore, B.W. Unanyan, R. |
| Author_xml | – sequence: 1 givenname: R. surname: Unanyan fullname: Unanyan, R. organization: Fachbereich Physik, Universität Kaiserslautern, 67653 Kaiserslautern, Germany – sequence: 2 givenname: M. surname: Fleischhauer fullname: Fleischhauer, M. organization: Sektion Physik, Ludwig-Maximilians Universität München, 80333 Munich, Germany – sequence: 3 givenname: B.W. surname: Shore fullname: Shore, B.W. organization: Fachbereich Physik, Universität Kaiserslautern, 67653 Kaiserslautern, Germany – sequence: 4 givenname: K. surname: Bergmann fullname: Bergmann, K. organization: Fachbereich Physik, Universität Kaiserslautern, 67653 Kaiserslautern, Germany |
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| Cites_doi | 10.1016/0009-2614(88)80364-6 10.1063/1.882030 10.1103/PhysRevB.39.3435 10.1103/PhysRevLett.71.3095 10.1103/PhysRevA.29.690 10.1103/PhysRevLett.73.2563 10.1088/0954-8998/6/4/016 10.1103/RevModPhys.68.733 10.1103/PhysRevA.54.1556 10.1103/PhysRevA.44.R4118 |
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| Snippet | We describe a method for creating an arbitrary coherent superposition of two atomic states in a controlled and robust way by using a sequence of three pulses... |
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| SubjectTerms | Exact sciences and technology Fundamental areas of phenomenology (including applications) Nonclassical field states; squeezed, antibunched and sub-poissonian states; operational definitions of the phase of the field; phase measurements Optics Physics Quantum optics |
| Title | Robust creation and phase-sensitive probing of superposition states via stimulated Raman adiabatic passage (STIRAP) with degenerate dark states |
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