2021
DOI: 10.1126/sciadv.abe2265
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Table-top extreme ultraviolet second harmonic generation

Abstract: The lack of available table-top extreme ultraviolet (XUV) sources with high enough fluxes and coherence properties has limited the availability of nonlinear XUV and x-ray spectroscopies to free-electron lasers (FELs). Here, we demonstrate second harmonic generation (SHG) on a table-top XUV source by observing SHG near the Ti M2,3 edge with a high-harmonic seeded soft x-ray laser. Furthermore, this experiment represents the first SHG experiment in the XUV. First-principles electronic structure calculations sugg… Show more

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Cited by 30 publications
(14 citation statements)
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References 48 publications
(52 reference statements)
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“…The χ eff (2) spectrum was then extracted using eq after binning and averaging spectra based on the photon energy and intensity of the driving fundamental pulse. The inherent jitter of the XFEL, both in frequency and intensity, allowed for a high-fidelity extraction of χ eff (2) ( 2ω) with significantly more data points, compared to refs . For the T = 62 K set of measurements, a quadratic function was fit to a plot of I (ω) vs I (2ω), at each energy where the second-order fit coefficient is modulo |χ eff (2) (2ω)| 2 , with χ eff (2) (2ω) a rank-three tensor of four independent components (χ zzz (2) ,χ xxz (2) , χ zxx (2) , and χ xxy (2) ), because of point group symmetry (Figure e).…”
Section: Resultsmentioning
confidence: 99%
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“…The χ eff (2) spectrum was then extracted using eq after binning and averaging spectra based on the photon energy and intensity of the driving fundamental pulse. The inherent jitter of the XFEL, both in frequency and intensity, allowed for a high-fidelity extraction of χ eff (2) ( 2ω) with significantly more data points, compared to refs . For the T = 62 K set of measurements, a quadratic function was fit to a plot of I (ω) vs I (2ω), at each energy where the second-order fit coefficient is modulo |χ eff (2) (2ω)| 2 , with χ eff (2) (2ω) a rank-three tensor of four independent components (χ zzz (2) ,χ xxz (2) , χ zxx (2) , and χ xxy (2) ), because of point group symmetry (Figure e).…”
Section: Resultsmentioning
confidence: 99%
“…Such effects were not visible in XUV-SHG at 160 K, but may have been below the detection limit of this experiment. Through complementary theory calculations, Helk et al 23 noted that resonant and nonresonant contributions to SHG can be of the same order of magnitude in the XUV regime, because of allowed transitions from the valence band to high-energy continuum states. Further development of SHG methodology in the XUV and SXR regimes will be essential to deconvolute these contributions and to fully characterize element-specific responses.…”
Section: Discussionmentioning
confidence: 99%
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“…In addition to linear X-ray absorption spectroscopy, novel nonlinear X-ray methods are emerging as a promising field for both fundamental light-matter interaction and material characterization. 57 Recent developments of intense X-ray sources at larger facilities are now making nonlinear X-ray measurements possible. X-ray transient grating spectroscopy 58 can directly give element-specific measurements of vibrational, magnetic, or electronic transport.…”
Section: Discussionmentioning
confidence: 99%
“…Ultrashort, intense extreme-ultraviolet (XUV) pulses are used in a growing number of applications, which include nonlinear multiphoton ionization of atoms [1][2][3][4][5][6], molecules [7,8] and clusters [9][10][11], second-harmonic generation in thin films [12] and the study of XUV strong-field physics [13,14]. Intense XUV pulses are also a prerequisite for performing XUV-pump XUV-probe experiments where XUV pulse durations down to the attosecond regime have already been used [15][16][17].…”
mentioning
confidence: 99%