Table 1. Laser parameters for the different Raman Amplification regimes to generate and amplify OAM lasers.
Amplification of existing modes |
Generation and amplification of new OAM modes |
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Pump | Seed |
OAM seed |
TEM seed |
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Pump | Seed | Pump | Seed | |||
TEM | — | — | — | — | TEM00ex+TEM00ey | TEM01ex+iTEM10ey |
OAM | L00ex | L01ex | L00ex+L02ey | L01ex | — | — |
a0 (peak) | 0.02 | 0.06 | 0.02 | 0.03 | 0.02 | 0.08 |
Spot (μm) | 718 | 435 | 718 | 435 | 718 | 435 |
Duration (fs) | 25 × 103 | 25 | 25 × 103 | 25 | 25 × 103 | 25 |
w0/wp | 20 | 19 | 20 | 19 | 20 | 19 |
Simulation parameters are close to ideal Raman amplification regimes determined in ref. 21. In all simulations, the probe has a central wavelength of 1 μm. The background plasma density is n0=4.3 × 1018 cm−3 for all simulations presented. When the pump/probe initially has components in both the transverse directions, the initial peak a0, spot size and durations present in the table are identical for every component. refers to a Laguerre–Gaussian mode, where the OAM corresponds to the index . TEMmn correspond to Hermite–Gaussian lasers with order (m, n). The table only describes the initial simulation conditions.