A noise-seeded transient Raman frequency comb spanning three octaves from 180 to 2400 nm is generated by pumping a hydrogen-filled hollow-core photonic crystal with 300 fs pulses of energy 26 mu J and wavelength 800 nm
Ultrabroad coherent comb-like optical spectra spanning several octaves are a chief ingredient in the...
In a relatively simple setup consisting of a microchip laser as pump source and two hydrogen-filled ...
A strong anti-Stokes Raman signal, from the vibrational Q(1) transition of hydrogen, is generated in...
A noise-seeded transient Raman frequency comb spanning three octaves from 180 to 2400 nm is generate...
A noise-seeded transient comb of Raman sidebands spanning three octaves from 180 to 2400 nm, is gene...
A noise-seeded transient comb of Raman sidebands spanning three octaves from 180 to 2400 nm, is gene...
Starting from a microchip laser and a Stokes seed generated from noise in a hydrogen-filled hollow-c...
Starting from a microchip laser and a Stokes seed generated from noise in a hydrogen-filled hollow-c...
We use Raman amplification in hydrogen-filled hollow-core kagome photonic crystal fiber to generate ...
We use Raman amplification in hydrogen-filled hollow-core kagome photonic crystal fiber to generate ...
Hollow-core photonic crystal fibre (HC-PCF) is unique host for gas-based nonlinear optical experimen...
This thesis explores the generation and the coherence properties of Raman frequency combs that are i...
Forward stimulated Raman scattering is used to generate a strong anti-Stokes signal in a hydrogen-fi...
Forward stimulated Raman scattering is used to generate a strong anti-Stokes signal in a hydrogen-fi...
A strong anti-Stokes Raman signal, from the vibrational Q(1) transition of hydrogen, is generated in...
Ultrabroad coherent comb-like optical spectra spanning several octaves are a chief ingredient in the...
In a relatively simple setup consisting of a microchip laser as pump source and two hydrogen-filled ...
A strong anti-Stokes Raman signal, from the vibrational Q(1) transition of hydrogen, is generated in...
A noise-seeded transient Raman frequency comb spanning three octaves from 180 to 2400 nm is generate...
A noise-seeded transient comb of Raman sidebands spanning three octaves from 180 to 2400 nm, is gene...
A noise-seeded transient comb of Raman sidebands spanning three octaves from 180 to 2400 nm, is gene...
Starting from a microchip laser and a Stokes seed generated from noise in a hydrogen-filled hollow-c...
Starting from a microchip laser and a Stokes seed generated from noise in a hydrogen-filled hollow-c...
We use Raman amplification in hydrogen-filled hollow-core kagome photonic crystal fiber to generate ...
We use Raman amplification in hydrogen-filled hollow-core kagome photonic crystal fiber to generate ...
Hollow-core photonic crystal fibre (HC-PCF) is unique host for gas-based nonlinear optical experimen...
This thesis explores the generation and the coherence properties of Raman frequency combs that are i...
Forward stimulated Raman scattering is used to generate a strong anti-Stokes signal in a hydrogen-fi...
Forward stimulated Raman scattering is used to generate a strong anti-Stokes signal in a hydrogen-fi...
A strong anti-Stokes Raman signal, from the vibrational Q(1) transition of hydrogen, is generated in...
Ultrabroad coherent comb-like optical spectra spanning several octaves are a chief ingredient in the...
In a relatively simple setup consisting of a microchip laser as pump source and two hydrogen-filled ...
A strong anti-Stokes Raman signal, from the vibrational Q(1) transition of hydrogen, is generated in...
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