@article {1873,
	title = {Quantization axes in coherent two-field spectroscopy},
	journal = {Journal of the Optical Society of America B-Optical Physics},
	volume = {19},
	number = {8},
	year = {2002},
	note = {<p>ISI Document Delivery No.: 583VBTimes Cited: 0Cited Reference Count: 22Cited References:      Chen YC, 2001, PHYS REV A, V64, DOI 10.1103/PhysRevA.64.053806     Chen YC, 2001, PHYS REV A, V63     Phillips DF, 2001, PHYS REV LETT, V86, P783, DOI 10.1103/PhysRevLett.86.783     Liu C, 2001, NATURE, V409, P490, DOI 10.1038/35054017     McGloin D, 2000, PHYS REV A, V62, part. no., DOI 10.1103/PhysRevA.62.053802     Chen YC, 2000, PHYS REV A, V61, DOI 10.1103/PhysRevA.61.053805     Wang S, 2000, PHYS REV A, V61     Akulshin AM, 1999, PHYS REV LETT, V83, P4277, DOI 10.1103/PhysRevLett.83.4277     Lukin MD, 1999, PHYS REV A, V60, P3225, DOI 10.1103/PhysRevA.60.3225     Taichenachev AV, 1999, JETP LETT+, V69, P819, DOI 10.1134/1.568096     Durrant AV, 1998, OPT COMMUN, V151, P136, DOI 10.1016/S0030-4018(98)00052-2     Marangos JP, 1998, J MOD OPTIC, V45, P471, DOI 10.1080/09500349808231909     Padmabandu GG, 1996, PHYS REV LETT, V76, P2053, DOI 10.1103/PhysRevLett.76.2053     Arimondo E, 1996, PROG OPTICS, V35, P257, DOI 10.1016/S0079-6638(08)70531-6     LI YQ, 1995, PHYS REV A, V51, pR2703     COURTOIS JY, 1994, PHYS REV LETT, V72, P3017, DOI 10.1103/PhysRevLett.72.3017     BOLLER KJ, 1991, PHYS REV LETT, V66, P2593, DOI 10.1103/PhysRevLett.66.2593     GRISON D, 1991, EUROPHYS LETT, V15, P149, DOI 10.1209/0295-5075/15/2/007     IMAMOGLU A, 1989, OPT LETT, V14, P1344, DOI 10.1364/OL.14.001344     KOCHAROVSKAYA OA, 1988, JETP LETT+, V48, P630     ASPECT A, 1988, PHYS REV LETT, V61, P826, DOI 10.1103/PhysRevLett.61.826     GRAY HR, 1978, OPT LETT, V3, P218, DOI 10.1364/OL.3.000218Chen, YW Lin, CW Chen, YC Yu, IAOPTICAL SOC AMERWASHINGTON</p>
},
	month = {Aug},
	pages = {1917-1921},
	type = {Article},
	abstract = {<p>Coherent two-field spectroscopy calculations with different choices of the quantization (z) axis are compared. In a system driven by a strong coupling field and a weak probe field, alignment of the z axis along either the polarization direction of a linearly polarized coupling field or the propagation direction of a circularly polarized coupling field is shown to simplify the calculations and facilitate interpretation of the results. The advantages of a suitable choice of the z axis are highlighted with an example of a degenerate three-level system of electromagnetically induced transparency. (C) 2002 Optical Society of America.</p>
},
	keywords = {ATOMS, CESIUM, electromagnetically induced transparency, INTERACTING DARK RESONANCES, INTERFERENCE, LASER, POPULATION-INVERSION, STATES, STORAGE, vapor},
	isbn = {0740-3224},
	url = {<Go to ISI>://WOS:000177430100024},
	author = {Y.W. Chen and Lin, C. W. and Y. C. Chen and Yu, I. A.}
}
