2009
DOI: 10.1364/ol.34.002918
|View full text |Cite
|
Sign up to set email alerts
|

Optical amplification in the near-infrared in gas-filled hollow-core fibers

Abstract: We demonstrate efficient optical parametric amplification and generation in a gas-filled hollow-core fiber of near-infrared pulses, peaked at 1.4 microm wavelength, with 5 microJ energy and 45 fs duration at the fiber output. Numerical simulations confirm that the OPA is phase matched through excitation of higher-order fiber modes.

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
1
1
1
1

Citation Types

0
35
0

Year Published

2012
2012
2024
2024

Publication Types

Select...
7
1

Relationship

0
8

Authors

Journals

citations
Cited by 27 publications
(35 citation statements)
references
References 11 publications
(10 reference statements)
0
35
0
Order By: Relevance
“…For the gas-filled hollow fiber, it should be necessary to take into account the contributions from high-order propagation modes. For several combinations of high-order propagation modes, the gas pressure at which phase matching is satisfied becomes higher than the phase-matching gas pressure for the lowest-order propagation modes [29][30][31][32].…”
Section: Phase Mismatch In the Generation Of High-order Anti-stokes Ementioning
confidence: 95%
“…For the gas-filled hollow fiber, it should be necessary to take into account the contributions from high-order propagation modes. For several combinations of high-order propagation modes, the gas pressure at which phase matching is satisfied becomes higher than the phase-matching gas pressure for the lowest-order propagation modes [29][30][31][32].…”
Section: Phase Mismatch In the Generation Of High-order Anti-stokes Ementioning
confidence: 95%
“…This effect is also well known in the normal GVD regime in both bulk and large diameter hollow core fibers used for high energy (mJ or higher) pulse compression (see e.g. [10][11][12]). Conversely, spectral red-shifting is typically not observed in positive GVD: in solid core fibers the pulse will usually temporally broaden and thus reduce the peak intensity before efficient red-shifting can take place.…”
Section: Introductionmentioning
confidence: 62%
“…Contrary to the amplification by stimulated Raman scattering, the amplification of light in the present research relies on the nonresonant FWM [10,11] that originates from the instantaneous response of the bound electrons rather than the nuclear response. The FWOPA poses no limitation on the frequency separation between the two input pulses, pump and signal pulses, except that the signal frequency must be lower than twice the pump frequency.…”
Section: Excitation Of Rotational Wavepackets By the Pump Pulse And Tmentioning
confidence: 98%
“…The parametric amplification based on third-order nonlinearity, nonresonant four-wave optical parametric amplification (FWOPA), also amplifies light in a broad spectral range [8][9][10][11]. An amplification gain as high as 100 has been reached in bulk media such as water and glasses [8,9].…”
Section: Open Accessmentioning
confidence: 99%
See 1 more Smart Citation