Erratum: Relativistic Resonances in Combined Magnetic and Laser Fields [Phys. Rev. Lett. 84, 3282 (2000)]

Wagner, R. E.; Su, Qiang; Grobe, R.

doi:10.1103/physrevlett.84.5682

Cited by 9 publications

(7 citation statements)

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“…For example, Faisal et al [9] studied numerically the spectra of radiation in a sin 2 laser pulse with a uniform magnetic field and showed that the electron trajectories in the laser pulse get distorted by the magnetic field. This is consistent with the perspective of the laser-magnetic resonance acceleration for which the relativistic cyclotron motion will occur in transverse direction [12][13][14][15][16][17][18][19][20][21][22]. In fact the magnetic resonance parameter that has been introduced in our previous (a) E-mail: bsxie@bnu.edu.cn (corresponding author) work [22] would play an important role on the emission spectra.…”

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confidence: 86%

Thomson backscattering in combined fields with a general elliptical polarization

Jiang¹,

Xie²,

Sang³

et al. 2017

EPL

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Thomson backscattering in combined fields with a general elliptical polarization of laser field and an applied constant magnetic field is studied. The monotonous and non-monotonous dependence of emission spectra on the ellipticity and the initial phase of laser field are found. We have also revealed the scaling law of the radiation spectra about the initial axial momentum in the general elliptic polarized case that is similar to the circularly polarized one. However, the scaling law about the laser intensity exists conditionally and the scale invariance about the magnetic resonance parameter exists, too. Another interesting feature is the feasibility to obtain the THz radiation by this scheme.

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confidence: 86%

Thomson backscattering in combined fields with a general elliptical polarization

Jiang¹,

Xie²,

Sang³

et al. 2017

EPL

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“…Moreover, a number of new research areas are being explored. Examples include the investigation of ions in intense laser fields [34] and atoms subjected to both an intense laser pulse and a strong, static magnetic field [35].…”

Section: Discussionmentioning

confidence: 99%

Relativistic Effects in Laser–Atom Interactions

Joachain

Kylstra

2003

Phys. Scr.

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Relativistic effects arise when atoms interact with ultra-strong laser fields. Such effects are expected to become important when the ratio of the ponderomotive energy Up of an electron in the field to the electron rest mass energy mc2 becomes comparable to unity. This ratio is given by q = e2ℰ02/(4m2ω2c2), where e is the magnitude of the electron charge, ℰ0 is the peak strength of the electric field and ω is the angular frequency of the laser light. We discuss recent progress in the theoretical study of relativistic effects in laser–atom interactions. Particular attention is devoted to the modifications of the laser–atom dynamics in the high-intensity, high-frequency regime where non-relativistic theories predict a decrease of the ionization probability of atoms with increasing laser intensity.

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“…Besides controlling the efficiency of HHG by suppression of the wave packet spreading, dynamics of an atomic electron in the presence of a moderate-intensity laser field and a strong static magnetic field has been shown recently to result in a peculiar bound-like system, called the cycloatom by its principal investigators [166,167]. An electronic charge distribution evolves from an initial atomic ground state into a ring, a Fig.…”

Section: Ionized Electrons In Laser Plus Extra Static Fieldsmentioning

confidence: 99%