A noise-seeded transient comb of Raman sidebands spanning three octaves from 180 to 2400 nm, is generated by pumping a hydrogen-filled hollow-core photonic crystal fiber with 26-mu J, 300-fs pulses at 800 nm. The pump pulses are spectrally broadened by both Kerr and Raman-related self-phase modulation (SPM), and the broadening is then transferred to the Raman lines. In spite of the high intensity, and in contrast to bulk gas-cell based experiments, neither SPM broadening nor ionization are detrimental to comb formation. (C) 2015 Optical Society of Americ
A strong anti-Stokes Raman signal, from the vibrational Q(1) transition of hydrogen, is generated in...
In a relatively simple setup consisting of a microchip laser as pump source and two hydrogen-filled ...
International audienceFrequency combs are of constant significant interest for their use in diverse ...
A noise-seeded transient comb of Raman sidebands spanning three octaves from 180 to 2400 nm, is gene...
A noise-seeded transient Raman frequency comb spanning three octaves from 180 to 2400 nm is generate...
A noise-seeded transient Raman frequency comb spanning three octaves from 180 to 2400 nm is generate...
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...
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...
International audienceWe report on experimental and theoretical demonstrations of an optical comb sp...
International audienceWe report on experimental and theoretical demonstrations of an optical comb sp...
International audienceWe report on experimental and theoretical demonstrations of an optical comb sp...
A strong anti-Stokes Raman signal, from the vibrational Q(1) transition of hydrogen, is generated in...
A strong anti-Stokes Raman signal, from the vibrational Q(1) transition of hydrogen, is generated in...
In a relatively simple setup consisting of a microchip laser as pump source and two hydrogen-filled ...
International audienceFrequency combs are of constant significant interest for their use in diverse ...
A noise-seeded transient comb of Raman sidebands spanning three octaves from 180 to 2400 nm, is gene...
A noise-seeded transient Raman frequency comb spanning three octaves from 180 to 2400 nm is generate...
A noise-seeded transient Raman frequency comb spanning three octaves from 180 to 2400 nm is generate...
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...
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...
International audienceWe report on experimental and theoretical demonstrations of an optical comb sp...
International audienceWe report on experimental and theoretical demonstrations of an optical comb sp...
International audienceWe report on experimental and theoretical demonstrations of an optical comb sp...
A strong anti-Stokes Raman signal, from the vibrational Q(1) transition of hydrogen, is generated in...
A strong anti-Stokes Raman signal, from the vibrational Q(1) transition of hydrogen, is generated in...
In a relatively simple setup consisting of a microchip laser as pump source and two hydrogen-filled ...
International audienceFrequency combs are of constant significant interest for their use in diverse ...