DFG () with undepletion at  and

Boulanger, B.; Zyss, J.

doi:10.1107/97809553602060000634

International
Tables for
Crystallography
Volume D
Physical properties of crystals
Edited by A. Authier

pdf | chapter contents | chapter index | related articles

International Tables for Crystallography (2006). Vol. D. ch. 1.7, p. 208

Section 1.7.3.3.5.1. DFG ( $[\omega_p-\omega_s=\omega_i]$ ) with undepletion at $[\omega_p]$ and $[\omega_s]$

B. Boulanger^a ^* and J. Zyss^b

^a Laboratoire de Spectrométrie Physique, Université Joseph Fourier, 140 avenue de la Physique, BP 87, 38 402 Saint-Martin-d'Hères, France, and ^bLaboratoire de Photonique Quantique et Moléculaire, Ecole Normale Supérieure de Cachan, 61 Avenue du Président Wilson, 94235 Cachan, France
Correspondence e-mail: benoitb@satie-bourgogne.fr

1.7.3.3.5.1. DFG ( $[\omega_p-\omega_s=\omega_i]$ ) with undepletion at $[\omega_p]$ and $[\omega_s]$

| top | pdf |

$[(\omega_s,\omega_i,\omega_p) = (\omega_1,\omega_2,\omega_3)]$ or $[(\omega_2,\omega_1,\omega_3)]$ .

The resolution of system (1.7.3.22) with $[E_s(X,Y,0)\ne 0]$ , $[E_p(X,Y,0)\ne 0]$ , $[\partial E_p(X,Y,Z)/\partial Z=\partial E_s(X,Y,Z)/\partial Z = 0]$ and [E_i(X,Y,0)=0] , followed by integration over ( [X,Y] ), leads to the same solutions as for SFG with undepletion at ω₁ and ω₂, i.e. formulae (1.7.3.81), (1.7.3.82) and (1.7.3.83), by replacing ω₁ by ω_s, ω₂ by ω_p and ω₃ by ω_i. A schematic device is given in Fig. 1.7.3.17 by replacing (ω₁, ω₂, ω₃) by (ω₁, ω₃, ω₂) or (ω₂, ω₃, ω₁).

References

International Tables for Crystallography (2006). Vol. D. ch. 1.7, p. 208

Section 1.7.3.3.5.1. DFG () with undepletion at and

1.7.3.3.5.1. DFG () with undepletion at and

References

Section 1.7.3.3.5.1. DFG ( $[\omega_p-\omega_s=\omega_i]$ ) with undepletion at $[\omega_p]$ and $[\omega_s]$

1.7.3.3.5.1. DFG ( $[\omega_p-\omega_s=\omega_i]$ ) with undepletion at $[\omega_p]$ and $[\omega_s]$