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 Results for DC.creator="B." AND DC.creator="Boulanger" in section 1.7.3 of volume D   page 1 of 4 pages.
Propagation phenomena
Boulanger, B. and Zyss, J.  International Tables for Crystallography (2013). Vol. D, Section 1.7.3, pp. 186-215 [ doi:10.1107/97809553602060000906 ]
... relative to the refractive indices in the phase-matching direction (Boulanger & Marnier, 1991). Phase-matching relationsConfigurations of polarizationTypes of interaction ... and the types according to SFG (), DFG (), DFG () and DFG () (Boulanger et al., 1993) Phase-matching relationsConfigurations of polarizationTypes of interaction ... two directions in the principal planes; the possible loci a, b, c, d are shown on the stereographic projection given ...

DFG () with undepletion at
Boulanger, B. and Zyss, J.  International Tables for Crystallography (2013). Vol. D, Section 1.7.3.3.5.2, p. 211 [ doi:10.1107/97809553602060000906 ]
DFG () with undepletion at 1.7.3.3.5.2. DFG () with undepletion at or . The resolution of system (1.7.3.22) with , , and , followed by the integration over (), leads to the same solutions as for SFG with undepletion at [omega]1 or [omega]2: formulae (1.7.3.84), (1.7.3.85) and (1.7.3.86). References International Tables for Crystallography (2013 ...

DFG () with undepletion at and
Boulanger, B. and Zyss, J.  International Tables for Crystallography (2013). Vol. D, Section 1.7.3.3.5.1, p. 211 [ doi:10.1107/97809553602060000906 ]
DFG () with undepletion at and 1.7.3.3.5.1. DFG () with undepletion at and or . The resolution of system (1.7.3.22) with , , and , followed by integration over (), leads to the same solutions as for SFG with undepletion at [omega]1 and [omega]2, i.e. formulae (1.7.3.81), (1.7.3.82) and (1.7.3.83), by replacing [omega]1 by ...

Difference-frequency generation (DFG)
Boulanger, B. and Zyss, J.  International Tables for Crystallography (2013). Vol. D, Section 1.7.3.3.5, pp. 211-215 [ doi:10.1107/97809553602060000906 ]
... length allows a reduction in the linewidth. For type II, b is never nil, even at degeneracy. A parametric amplifier placed ... power. (a) can be a SROPO, DROPO or TROPO and (b) can be a SROPO or DROPO, according to the reflectivity ... alpha]) for (a) BBO pumped at [lambda]p = 355nm and (b) KTP pumped at [lambda]p = 1064nm, where or is ...

SFG () with undepletion at
Boulanger, B. and Zyss, J.  International Tables for Crystallography (2013). Vol. D, Section 1.7.3.3.4.2, p. 211 [ doi:10.1107/97809553602060000906 ]
SFG () with undepletion at 1.7.3.3.4.2. SFG () with undepletion at or . The undepleted wave at [omega]p, the pump, is mixed in the nonlinear crystal with the depleted wave at [omega]s, the signal, in order to generate the idler wave at . The integrations of the coupled amplitude equations over ...

SFG () with undepletion at and
Boulanger, B. and Zyss, J.  International Tables for Crystallography (2013). Vol. D, Section 1.7.3.3.4.1, p. 211 [ doi:10.1107/97809553602060000906 ]
SFG () with undepletion at and 1.7.3.3.4.1. SFG () with undepletion at and The resolution of system (1.7.3.22) with , , and , followed by integration over , leads towithin the same units as equation (1.7.3.70). References International Tables for Crystallography (2013). Vol. D, ch. 1.7, p. 211 International Union of Crystallography 2013 | home | resources ...

Sum-frequency generation (SFG)
Boulanger, B. and Zyss, J.  International Tables for Crystallography (2013). Vol. D, Section 1.7.3.3.4, pp. 210-211 [ doi:10.1107/97809553602060000906 ]
Sum-frequency generation (SFG) 1.7.3.3.4. Sum-frequency generation (SFG) SHG () and SFG () are particular cases of three-wave SFG. We consider here the general situation where the two incident beams at [omega]1 and [omega]2, with , interact with the generated beam at [omega]3, with , as shown in Fig. 1.7.3.17. ...

Direct THG ()
Boulanger, B. and Zyss, J.  International Tables for Crystallography (2013). Vol. D, Section 1.7.3.3.3.3, p. 210 [ doi:10.1107/97809553602060000906 ]
Direct THG () 1.7.3.3.3.3. Direct THG () As for the cascading process, we consider a flat plane wave which propagates in a direction without walk-off. The integration of equations (1.7.3.24) over the crystal length L, with and in the undepleted pump approximation, leads to According to (1.7.3.36) and (1.7.3.38), the integration of ...

SHG () and SFG () in the same crystal
Boulanger, B. and Zyss, J.  International Tables for Crystallography (2013). Vol. D, Section 1.7.3.3.3.2, p. 210 [ doi:10.1107/97809553602060000906 ]
... equations relative to SHG and those relative to SFG separately (Boulanger, Fejer et al., 1994). In order to compare this ... amplitude of the third harmonic field inside the crystal is (Boulanger, 1994)with[Gamma] is as in (1.7.3.59). (1.7.3.73) can ... at [omega] and 2[omega] between the two crystals. References Boulanger, B. (1994). CNRS-NSF Report, Stanford University. Boulanger, ...

SHG () and SFG () in different crystals
Boulanger, B. and Zyss, J.  International Tables for Crystallography (2013). Vol. D, Section 1.7.3.3.3.1, pp. 209-210 [ doi:10.1107/97809553602060000906 ]
... Picosecond third-harmonic light generation in [beta]-BaB2O4. Appl. Phys. B, 45, 225-236. International Tables for Crystallography (2013). Vol. ...

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