@article{winter_coherent_2006,
	title = {Coherent matter waves for ultrafast laser pulse characterization},
	volume = {264},
	issn = {00304018},
	url = {https://linkinghub.elsevier.com/retrieve/pii/S0030401806004895},
	doi = {10.1016/j.optcom.2005.12.079},
	abstract = {A technique for the characterization of ultrashort laser pulses using coherent matter waves is demonstrated. We emphasize the analogy between matter wave packets and electromagnetic wave packets propagating in dispersive media. Due to quadratic dispersion the wave packets are stretched and their temporal structure eventually converges to their spectrum, thus providing a possibility for energy measurements in conjugate space. This is demonstrated theoretically and experimentally and is the basis for our laser pulse characterization technique. We use energy resolved interferometrically recorded photoelectron spectra generated by above-threshold ionization in an autocorrelation setup to characterize ultrashort laser pulses at 800 nm wavelength. This approach is potentially applicable to the XUV wavelength region.},
	language = {en},
	number = {2},
	urldate = {2020-06-16},
	journal = {Optics Communications},
	author = {Winter, M. and Wollenhaupt, M. and Baumert, T.},
	month = aug,
	year = {2006},
	pages = {285--292},
}

A technique for the characterization of ultrashort laser pulses using coherent matter waves is demonstrated. We emphasize the analogy between matter wave packets and electromagnetic wave packets propagating in dispersive media. Due to quadratic dispersion the wave packets are stretched and their temporal structure eventually converges to their spectrum, thus providing a possibility for energy measurements in conjugate space. This is demonstrated theoretically and experimentally and is the basis for our laser pulse characterization technique. We use energy resolved interferometrically recorded photoelectron spectra generated by above-threshold ionization in an autocorrelation setup to characterize ultrashort laser pulses at 800 nm wavelength. This approach is potentially applicable to the XUV wavelength region.

@article{Mairesse2005,
	title = {Frequency-resolved optical gating for complete reconstruction of attosecond bursts},
	volume = {71},
	issn = {1050-2947},
	url = {http://link.aps.org/doi/10.1103/PhysRevA.71.011401},
	doi = {10.1103/PhysRevA.71.011401},
	number = {1},
	urldate = {2014-05-04},
	journal = {Physical Review A},
	author = {Mairesse, Y. and Quéré, F.},
	month = jan,
	year = {2005},
	keywords = {\#nosource, ★},
	pages = {011401},
}

@article{sekikawa_measurement_2002,
	title = {Measurement of the {Intensity}-{Dependent} {Atomic} {Dipole} {Phase} of a {High} {Harmonic} by {Frequency}-{Resolved} {Optical} {Gating}},
	volume = {88},
	issn = {0031-9007, 1079-7114},
	url = {https://link.aps.org/doi/10.1103/PhysRevLett.88.193902},
	doi = {10.1103/PhysRevLett.88.193902},
	abstract = {The temporal profile and phase of the fifth harmonic of a Ti:sapphire laser were fully characterized by
two-photon ionization frequency-resolved optical gating technique for the first time. The fifth harmonic
was found to have negative chirp and the pulse compression was demonstrated. The negative chirp is
well explained by using a zero-range potential model. This technique is scalable to extreme ultraviolet
(XUV) and soft x-ray regions by using currently available light sources, making it possible to measure
the pulse duration and phase of vacuum ultraviolet, XUV, and soft x-ray pulses.},
	language = {en},
	number = {19},
	urldate = {2020-06-16},
	journal = {Physical Review Letters},
	author = {Sekikawa, Taro and Katsura, Tomotaka and Miura, Satoshi and Watanabe, Shuntaro},
	month = apr,
	year = {2002},
	note = {tex.ids: sekikawaMeasurementIntensityDependentAtomic2002a},
	pages = {193902},
}

The temporal profile and phase of the fifth harmonic of a Ti:sapphire laser were fully characterized by two-photon ionization frequency-resolved optical gating technique for the first time. The fifth harmonic was found to have negative chirp and the pulse compression was demonstrated. The negative chirp is well explained by using a zero-range potential model. This technique is scalable to extreme ultraviolet (XUV) and soft x-ray regions by using currently available light sources, making it possible to measure the pulse duration and phase of vacuum ultraviolet, XUV, and soft x-ray pulses.

@article{norin_time-frequency_2002,
	title = {Time-{Frequency} {Characterization} of {Femtosecond} {Extreme} {Ultraviolet} {Pulses}},
	volume = {88},
	issn = {0031-9007, 1079-7114},
	url = {https://link.aps.org/doi/10.1103/PhysRevLett.88.193901},
	doi = {10.1103/PhysRevLett.88.193901},
	abstract = {We present energy-resolved cross-correlation measurements of an extreme ultraviolet (XUV) pulse,
generated as the fifth harmonic (15.5 eV) of an intense 80 fs laser pulse centered at 400 nm. Spectrally
resolving the cross-correlation signal allows us to characterize the time-dependent frequency of the XUV
pulse. We find that the fifth harmonic has a small negative chirp in excess of that predicted by pertur-
bation theory. In addition, by manipulating the chirp of the driving laser we can induce and measure a
positive or a negative chirp on the XUV pulse.},
	language = {en},
	number = {19},
	urldate = {2020-06-16},
	journal = {Physical Review Letters},
	author = {Norin, J. and Mauritsson, J. and Johansson, A. and Raarup, M. K. and Buil, S. and Persson, A. and Dühr, O. and Gaarde, M. B. and Schafer, K. J. and Keller, U. and Wahlström, C.-G. and L'Huillier, A.},
	month = apr,
	year = {2002},
	note = {tex.ids: norin2002TimeFrequencyCharacterizationFemtoseconda
publisher: American Physical Society},
	pages = {193901},
}

We present energy-resolved cross-correlation measurements of an extreme ultraviolet (XUV) pulse, generated as the fifth harmonic (15.5 eV) of an intense 80 fs laser pulse centered at 400 nm. Spectrally resolving the cross-correlation signal allows us to characterize the time-dependent frequency of the XUV pulse. We find that the fifth harmonic has a small negative chirp in excess of that predicted by pertur- bation theory. In addition, by manipulating the chirp of the driving laser we can induce and measure a positive or a negative chirp on the XUV pulse.