2002
DOI: 10.1016/s0030-4018(02)01642-5
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Controlled light storage in a double lambda system

Abstract: It is shown theoretically that after light storing in a medium of four-level atoms it is possible to release a new pulse of a different frequency, the process being steered by another driving beam. It is also possible to store one pulse and to release two different ones, with their time separation and heights being controlled.Comment: 7 pages,3 figure

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Cited by 36 publications
(31 citation statements)
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“…The energy of the atomic state |ν is given byhω ν ,h being the Planck's constant, μ 12 is the electric dipole moment of the |1 − |2 transition, and a † ω p andâ ω p are the creation and annihilation field operators, respectively, for a frequency mode ω p . The Rabi frequencies of the classical beams are denoted by 0 cj = cj e −iω 0 23 is the dipole moment of the |3 − |2 transition and E cj the corresponding electric field amplitude. The amplitudes of the quantum field operators read…”
Section: The Modelmentioning
confidence: 99%
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“…The energy of the atomic state |ν is given byhω ν ,h being the Planck's constant, μ 12 is the electric dipole moment of the |1 − |2 transition, and a † ω p andâ ω p are the creation and annihilation field operators, respectively, for a frequency mode ω p . The Rabi frequencies of the classical beams are denoted by 0 cj = cj e −iω 0 23 is the dipole moment of the |3 − |2 transition and E cj the corresponding electric field amplitude. The amplitudes of the quantum field operators read…”
Section: The Modelmentioning
confidence: 99%
“…For the storage of a general photonic qubit, i.e., a single photon in an arbitrary superposition of two different components, more sophisticated schemes are needed [16][17][18][19][20][21][22][23][24][25][26][27]. In quantum communication with photons, the logical qubits can be encoded in several ways, for example, via polarization, time bin, path, phase, photon number or even frequency encodings.…”
Section: Introductionmentioning
confidence: 99%
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“…In particular it is possible to simultaneously propagate two optical pulses of different frequencies through a medium in the conditions of EIT. In our earlier paper [9] we have pointed out that one can stop one pulse and release a pulse of a different frequency or two different pulses. We have also mentioned that making the medium transparent simultaneously for two pulses is possible provided that the fields are in some special relation, which allows for an adiabatic evolution of the system.…”
Section: Introductionmentioning
confidence: 99%