Author Affiliations
1GoLP/Instituto de Plasmas e Fusão Nuclear, Instituto Superior Tecnico, Universidade de Lisboa, 1049-001 Lisboa, Portugal2Central Laser Facility, Science and Technology Facilities Council, Rutherford Appleton Laboratory, Harwell Science and Innovation Campus, Didcot, UK3INFN-LNF, Via Enrico Fermi 54, 00044 Frascati, Italyshow less
Fig. 1. Representation of noncollinear phase-matching condition. o.a. is the crystal optic axis.
Fig. 2. Parametric scan for the BiBO nonlinear crystal. (a) Simulated phase-matched wavelength (λsM) dependence of the amplified spectrum. The crystal thickness is 2.5 mm and the pump intensity is ~50 GW/cm2. (b) Simulated noncollinear angular dependence of the amplified spectrum over a range ~1.6. The crystal thickness is 2.5 mm and the pump intensity is ~50 GW/cm2. The box (translucent white) highlights the region of interest where the bandwidth is maximized but the central region (~0.9 μm) is not heavily depleted.
Fig. 3. Simulated amplification spectrum for a 5 mm YCOB crystal pumped at 515 nm with an intensity of ~50 GW/cm2.
Fig. 4. Simulated noncollinear angular dependence of the BiBO amplified spectrum. Crystal thickness is 2.5 mm and the pump intensity is ~50 GW/cm2.
Fig. 5. Schematic of the OPCPA chain used for crystal comparison. SHG, second harmonic generation; WLG, white light generation.
Fig. 6. Noncollinear OPA stage seed: supercontinuum generation.
Fig. 7. Experimental results for the YCOB NOPA stage compared to theoretical analysis. Amplified spectra for (a) 5 mm, (b) 7.5 mm and (c) 15 mm crystals. The shadowed curve is the numerically calculated amplified spectrum for the following parameters: λp = 515 nm, Ip ~50 GW/cm2, deff = 5, 7.5, 15 mm YCOB crystal thicknesses, and the signal and crystal angles are those reported in Table 2.
Fig. 8. Experimental results for the BiBO NOPA stage: amplified spectrum for a 2.5 mm crystal. Different noncollinear angles are plotted to show the influence of θNC on the spectral dip around 920 nm.
Fig. 9. Theoretical amplified spectrum for LBO and BBO crystals in a noncollinear geometry to maximize the bandwidth.
| A | B | C | D |
---|
YCOB[27] | | | | | nx | 2.7697 | 0.02034 | 0.01779 | 0.00643 | ny | 2.8741 | 0.02213 | 0.01871 | 0.01078 | nz | 2.9107 | 0.02232 | 0.01887 | 0.01256 | BiBO[35] | | | | | nx | 3.0740 | 0.0323 | 0.0316 | 0.01337 | ny | 3.1685 | 0.0373 | 0.0346 | 0.01750 | nz | 3.6545 | 0.0511 | 0.0371 | 0.02260 |
|
Table 1. Sellmeier equation (
) coefficients for YCOB and BiBO
[27,35].
NL crystal | YCOB | BiBO |
---|
Axis plane | xz | yz | Interaction | oo-e | ee-o | Central λs (nm) | @850 | @850 | θC (°) | 55 | 12 | ϕ (°) | 62 | 90 | deff (pm/V) | 1.41 | 3.02 | θNC (°) | 3.75 | 2.9 | LC (mm) | 5 | 2.5 | LC (mm) | 7.5 | / | LC (mm) | 15 | / |
|
Table 2. Parameters for the nonlinear crystals BiBO and YCOB to obtain broadband amplification. θC (°) and ϕ (°) are the crystal angles for perfect phase matching, deff (pm/V) is the nonlinear efficiency, θNC (°) is the noncollinear angle and LC (mm) is the crystal length.