Multi-octave spectral comb from a gas-filled hollow fiber

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10.1117/2.1200802.1052
Multi-octave spectral comb from
a gas-filled hollow fiber
Fetah Benabid
A new strategy for designing optical fibers enables coverage of a wide
frequency range with the potential to generate ultrashort pulses.
Attoscience is the production of light pulses lasting on the order of a millionth of a billionth of a second. These pulses make
it possible to measure and control physical and chemical processes extremely rapidly. The pulses are conventionally produced from an initial optical excitation using high-harmonic
generation (HHG) in a gas-phase (gaseous) medium. The result
is an ultrabroad, comblike optical spectrum, with mutually coherent ‘teeth’ spanning spectral regions from the visible to XUV
and soft x-ray. Up to now, HHG has demanded complex, cumbersome, pulsed lasers to drive the gas-phase medium. These
pump lasers emit ultrashort pulses (<10fs) with extraordinarily
high instantaneous power (≥1MW). The stringent requirements
on the driving lasers limited their use to a few specialized laboratories.
Recently, our team from the University of Bath collaborated
with the Technical University of Denmark and the University of
Oregon to demonstrate a much simpler system.1 We generated a
coherent spectral comb, covering more than three octaves of frequency, using a single pump laser that emitted moderately powerful, quasi-continuous infrared pulses. The novel generation
medium was a compact photonic structure consisting of an ∼1m
length of a newly designed, hollow-core photonic-crystal fiber
(HC-PCF), shown in Figure 1. Although prior work had found
unprecedented nonlinearity at low optical powers in HC-PCF,
the spectral width was limited by the modest bandgap achievable in the fibers used.
The results1 represent two advances: a new theory of mode
guiding in these fibers, and harmonic generation with unprecedented low powers and long pulses. The first advance theoretically relates photonic guidance in HC-PCF to the ‘Von
Neumann–Wigner’ bound and quasi-bound states within a continuum. In contrast to common intuition, the HC-PCF concurrently accommodates both discrete core-guided modes and
Figure 1. The hollow-core photonic-crystal fiber (HC-PCF), as seen under an optical microscope.
Figure 2. The intensity distribution, on a color scale, for the core mode
(a) and cladding mode (b) of the HC-PCF. The center panel shows
the transverse intensity oscillations of the two modes along the dotted
cross-sections.
continuum cladding modes, even if they have the same symmetry. This situation arises from the strong transverse phase
mismatch between the fields in the fiber core and cladding, as
shown in Figure 2. The fiber we developed has transmission
bandwidths several times wider than state-of-the-art photonicbandgap HC-PCF, with relatively low loss.
The unique properties of this fiber allowed the second development, in ultrafast optics. A coherent comblike spectrum,
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10.1117/2.1200802.1052 Page 2/2
that synthesizing attosecond pulses could be achieved more
readily than they are now. The wavelengths required are also
more ‘tamed’ than those currently used, which lie in the XUV
and soft x-ray regions. Our techniques would then enable lowcost compact systems for subfemtosecond optical-pulse generation, with a potentially major impact in many research areas,
including laser science, materials science, and biology.
Author Information
Fetah Benabid
Physics Department
University of Bath
Bath, UK
Figure 3. Stimulated Raman scattering from a hydrogen-filled HCPCF generates a multi-octave comblike spectrum
spanning three octaves, was generated using transient stimulated Raman scattering (SRS) in a hydrogen-filled HC-PCF (see
Figure 3). Relative to previous techniques, the comb is generated
with power levels six orders of magnitude lower and with pulses
five orders of magnitude longer in duration. The extension of
transient SRS to much longer pulses than the usual transformlimited, subpicosecond pulses was made possible by the combination of tight transverse confinement and long interaction
length.2 The results were obtained in a new excitation regime
for coherent SRS. Since it is seeded by quantum noise, the preparation is not adiabatic, but it is also not impulsive because the
pulses are longer than the period of the Raman molecular excitation.
Both of these developments are supported by rigorous theory and modeling (see supplemental online material1 ). The implications are wide-ranging. The photonic guidance theory not
only creates a design direction for next-generation broadband
HC-PCF but can also be exploited by the whole photonic-crystal
community. The similarity between this guidance and the Von
Neumann–Wigner states constitutes a novel conceptual bridge
between photonics and quantum mechanics. Furthermore, multiline coherent stimulated Raman scattering is a long-standing
basic problem in nonlinear optical physics, and our new experiments and theory, stimulated by the availability of the new
hollow-core fiber, are a large step forward in this area.
In addition, the generation of ultrabroad, coherent, comblike
spectra using simple and moderately powerful lasers suggests
References
1. F. Couny, F. Benabid, P. J. Roberts, P. S. Light, and M. G. Raymer, Generation and
photonic guidance of multi-octave optical-frequency combs, Science 318, 2007.
2. F. Benabid, G. Antonopoulos, J. C. Knight, and P. S. J. Russell, Stokes amplification regimes in quasi-CW pumped hydrogen-filled hollow-core photonic crystal fiber, Phys.
Rev. Lett. 95, p. 213903, 2005.
c 2008 SPIE
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