2014
DOI: 10.1364/oe.22.006194
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High flux coherent super-continuum soft X-ray source driven by a single-stage, 10mJ, Ti:sapphire amplifier-pumped OPA

Abstract: Abstract:We demonstrate the highest flux tabletop source of coherent soft X-rays to date, driven by a single-stage 10 mJ Ti:sapphire regenerative amplifier at 1 kHz. We first down-convert the laser to 1.3 µm using a parametric amplifier, before up-converting it to soft X-rays using high harmonic generation in a high-pressure, phase matched, hollow waveguide geometry. The resulting optimally phase matched broadband spectrum extends to 200 eV, with a soft X-ray photon flux of > 10 6 photons/pulse/1% bandwidth at… Show more

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Cited by 57 publications
(30 citation statements)
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“…By using counterrotating driving lasers at 0.79 μm (1.57 eV) and 1.3 μm (0.95 eV), we generate bright circularly polarized soft X-ray HHG beams with photon energies greater than 160 eV (14) and with flux comparable to the HHG flux obtained using linearly polarized 800-nm driving lasers (15). Moreover we implement, to our knowledge, the first advanced simulations of the coherent buildup of circularly polarized high harmonics to show how the macroscopic phase-matching physics and ellipticity of the driving lasers influence the HHG spectra, number of bright attosecond bursts, and the degree of circular polarization.…”
mentioning
confidence: 98%
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“…By using counterrotating driving lasers at 0.79 μm (1.57 eV) and 1.3 μm (0.95 eV), we generate bright circularly polarized soft X-ray HHG beams with photon energies greater than 160 eV (14) and with flux comparable to the HHG flux obtained using linearly polarized 800-nm driving lasers (15). Moreover we implement, to our knowledge, the first advanced simulations of the coherent buildup of circularly polarized high harmonics to show how the macroscopic phase-matching physics and ellipticity of the driving lasers influence the HHG spectra, number of bright attosecond bursts, and the degree of circular polarization.…”
mentioning
confidence: 98%
“…First, circularly polarized HHG provides a unique route for generating bright narrowband (λ/Δλ > 400) harmonic peaks in the soft X-ray region, to complement the soft X-ray supercontinua that are produced with linearly polarized mid-IR lasers (2,15,16). This capability is significant because it provides an elegant and efficient route for shaping soft X-ray light by manipulating the driving laser light, and is very useful for applications in high-resolution coherent imaging (17)(18)(19)(20)(21) and photoelectron spectroscopies.…”
mentioning
confidence: 99%
“…High-order harmonics in the "water window" with photon energy ranging from 280 to 530 eV have been reported in a number of laboratories in recent years [7][8][9][10][11][12][13][14][15]. Such soft X-ray harmonics are needed to excite core-level transitions in materials.…”
Section: B Broadband Xuv Pulses Where Frog-crab Failsmentioning
confidence: 99%
“…Various techniques have been developed to generate broadband extreme ultraviolet (XUV) light that has available continuum bandwidth capable of supporting pulse duration of a few tens to hundreds of attoseconds, such as amplitude gating [2], ionization gating [3], polarization gating [5], double optical gating [4], and wavefront rotation method [6]. Similarly, using few-cycle phase-stabilized mid-infrared wavelength lasers, ultrabroadband super-continuum harmonics up to the waterwindow and beyond have been reported [7][8][9][10][11][12][13][14][15]. If these pulses are transform-limited, the resulting durations of the attosecond pulses are expected to range from 30 attoseconds down to even a few attoseconds.…”
Section: Introductionmentioning
confidence: 99%
“…One can expect that this type spectroscopy will now be implemented in the SXR range with the tremendous advantage of element sensitivity on carbon, nitrogen, and oxygen. Documented photon numbers of harmonic sources are on the order of 10 7 photons/s in 1% bandwidth at 300 eV with 1 kHz repetition rate [28,35]. Typical spectral resolution needed for NEXAFS on isolated molecules is 0.25 eV, such that about 10 5 -10 6 photons/s are available per spectral bin (given that the spectrometer and detector have low loss).…”
Section: Figure 2: (A) Difference Auger Spectrum (Excited Minus Non-ementioning
confidence: 99%