Macroscopic effects in electromagnetically-induced transparency in a Doppler-broadened system<xref ref-type="fn" rid="cpb141337fn1">*</xref>

Macroscopic effects in electromagnetically-induced transparency in a Doppler-broadened system*

Pei Li-Ya^a), Niu Jin-Yan^b), Wang Ru-Quan^c), Qu Yi-Zhi^a), Wu Ling-An^c), Fu Pan-Ming^c)†, Zuo Zhan-Chun^c)‡

Fig.#cod#x00A0;6. Velocity dependence of a #cod#x025B; #cod#x00B1; and b the imaginary part of #cod#x03C7; nl for #cod#x03B6; 2 #cod#x003D; 1, G 2 #cod#x0393; 10 #cod#x003D; 5, #cod#x0394; 2 #cod#x0393; 10 #cod#x003D; 0, and #cod#x0394; 1 #cod#x0393; 10 #cod#x003D; 0 solid curve, 1 dashed curve, 2 dotted curve, and 4 dash-dotted curve. The resonant velocity v 2 correspond to the cross point of the curve #cod#x025B; #cod#x2212; v with a line y #cod#x003D; 0 thin solid line shown in panel a. In panel b the maximum of Im[ #cod#x03C7; nl ] with #cod#x0394; 1 #cod#x0393; 10 #cod#x003D; 4 is normalized to 1.