2010
DOI: 10.1103/physrevlett.105.063903
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Determining the Carrier-Envelope Phase of Intense Few-Cycle Laser Pulses

Abstract: The electromagnetic radiation emitted by an ultrarelativistic accelerated electron is extremely sensitive to the precise shape of the field driving the electron. We show that the angular distribution of the photons emitted by an electron via multiphoton Compton scattering off an intense (I>10(20)  W/cm(2)), few-cycle laser pulse provides a direct way of determining the carrier-envelope phase of the driving laser field. Our calculations take into account exactly the laser field, include relativistic and quantum… Show more

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Cited by 133 publications
(176 citation statements)
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“…On this respect, we observe that, based on the relation (34), we have proposed in [36] a method for determining the CEP of laser pulses with…”
Section: A High Intensitiesmentioning
confidence: 99%
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“…On this respect, we observe that, based on the relation (34), we have proposed in [36] a method for determining the CEP of laser pulses with…”
Section: A High Intensitiesmentioning
confidence: 99%
“…Also, in [25], the authors consider effects of the absolute phase [the so-called carrier envelope phase (CEP)] of few-cycle pulses and its impact on the emitted photon energy spectra. Here we also consider the effect of CEP on the angular distribution of the emitted radiation (see also [36]). …”
Section: Introductionmentioning
confidence: 99%
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“…Other aspects of nonlinear Compton scattering in short laser pulses that affect inverse Compton x-ray sources include the prospects for the generation of x-ray frequency combs [51,52], asymmetries in the angular distributions [53,54], spin- [35,36,55,56] and higher-order QED effects [57][58][59][60][61]. Moreover, using vortex beams that carry orbital angular momentum in a Compton backscattering set-up allows to generate high-energy vortex beams [62] or to control the spatial distribution of the generated x-rays [63].…”
Section: Theoretical Backgroundmentioning
confidence: 99%
“…Thus, it is physically justified to describe the driving field as a pulsed plane wave [7]. This approach has been used recently in connection to not only Thomson and Compton scattering [8][9][10][11][12][13][14][15][16][17][18], but also to other strong-field processes such as * E-mail address: Katarzyna.Krajewska@fuw.edu.pl…”
Section: Introductionmentioning
confidence: 99%