TY - GEN
T1 - Electromagnetically induced waveguiding in double-A systems
AU - Wilson-Gordon, A. D.
AU - Shpaisman, H.
AU - Friedmann, H.
PY - 2005
Y1 - 2005
N2 - Near the threshold for electromagnetically-induced transparency (EIT) or coherent population trapping (CPT), two-photon-resonance-enhanced self-focusing of a A system can be exploited to induce spatial confinement in a second, diffracting A system [1]. The diffracting A system is characterized by parameters below the EIT or CPT threshold, and the two A systems must be coupled to form a closed-loop double-A system (see Fig. 1). The waveguiding effect is shown to be strongly phase dependent, indicating that it derives from the phase-dependent effective third-order susceptibility rather than the phase-independent effective first-order susceptibility, as is the case in previously studied systems. We also show that when the second A system initially involves only a single laser beam, the loop is completed by the efficient generation of radiation at the four-wave mixing frequency, within a propagation distance much shorter than the diffraction length. As shown in Fig. 2, both the applied (V′32, V′32, V′42) and generated (V′41) fields exhibit electromagnetically-induced waveguiding.
AB - Near the threshold for electromagnetically-induced transparency (EIT) or coherent population trapping (CPT), two-photon-resonance-enhanced self-focusing of a A system can be exploited to induce spatial confinement in a second, diffracting A system [1]. The diffracting A system is characterized by parameters below the EIT or CPT threshold, and the two A systems must be coupled to form a closed-loop double-A system (see Fig. 1). The waveguiding effect is shown to be strongly phase dependent, indicating that it derives from the phase-dependent effective third-order susceptibility rather than the phase-independent effective first-order susceptibility, as is the case in previously studied systems. We also show that when the second A system initially involves only a single laser beam, the loop is completed by the efficient generation of radiation at the four-wave mixing frequency, within a propagation distance much shorter than the diffraction length. As shown in Fig. 2, both the applied (V′32, V′32, V′42) and generated (V′41) fields exhibit electromagnetically-induced waveguiding.
UR - http://www.scopus.com/inward/record.url?scp=33847269776&partnerID=8YFLogxK
U2 - 10.1109/eqec.2005.1567260
DO - 10.1109/eqec.2005.1567260
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AN - SCOPUS:33847269776
SN - 0780389735
SN - 9780780389731
T3 - 2005 European Quantum Electronics Conference, EQEC '05
SP - 89
BT - 2005 European Quantum Electronics Conference, EQEC '05
T2 - 2005 European Quantum Electronics Conference, EQEC '05
Y2 - 12 June 2005 through 17 June 2005
ER -