Download Laser Optics of Condensed Matter by V. M. Tuchkevich, Joseph L. Birman (auth.), Joseph L. PDF
By V. M. Tuchkevich, Joseph L. Birman (auth.), Joseph L. Birman, Herman Z. Cummins, A. A. Kaplyanskii (eds.)
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7) for orthogonal and para~le1 polarizations of the pump waves. ). In some experiments additional illumination by Nd: YAG laser second harmonic pulses with peak intensity 10 was used (Fig. 7). In the BP method the SD efficiency ~ was measured as a function of the frequency detuning ~ = w - w (Fig. 8). 5 (exciton line); 614; 609 nm (interband transitions) - was varied. The orthogonal pump wave ~ytarizations were chosen to eliminate scattering from acoustic gratings • 33 Fig. 3. SS, PP method. ), ~2 &T ....
The comparison of steady state and dynamic cooling rates. Dashed lines - JF' solid curves Jst (Eq. (14»: 1 - n = 10 16 cm- 3 , 2 n = 2x10 17 cm-", n = 4x10 17 cm- 3 • Crosses are calculated from Eq. (9) for n = 4x10 17 cm- 3 • Dotted line Jdm (Eq. (10», n = 4x10 17 em 3. 1 "'. 02 References 1. 2. 3. 4. 5. 6. 7. 8. 9. S. A. Lyon, Journal of Luminescence 35:121 (1986). E. J. Yoffa, Phys. Rev. B 23:1909 (1981)~ M. Pugnet, J. Collet, A. Cornet, Solid St. Commun. 38:531 (1981); A. R. Vasconsellos, R.
1) dNq/dt = Nc (hwlT c 2) dTc/dt. For Na = 0, using the same approximations that led to Eq. (9), we obtain dT c C dt = n·Jdyn 2 A = Ci? (flw) Tc 3/2 Jst Jdyn = 1 +A nh w (1'1 -) 3/2 Ron ( C Tc 2 A nTa hW l+A (11) Ta 1'lw ) eXP(-T) Tqhmin c where C is the plasma heat capacity. One can see that for A » 1 (if, however, the concentration is sufficiently large for the condition Tqcmin < Ta to be satisfied) the dynamical cooling rate in much less than the static one. The value Jdyn (for A » 1) is practically concentration independent, just as for small n, but rrruch lower.