2008
DOI: 10.1103/physreva.78.033431
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Bound-freee+epair creation with a linearly polarized laser field and a nuclear field

Abstract: The process of bound-free pair production of electrons and positrons in combined laser and Coulomb fields is investigated. It is assumed that an ion collides at relativistic speed with an intense x-ray laser beam of linear polarization. The process proceeds nonlinearly due to simultaneous absorption of a few laser photons. The capture of the electron into the ground state and the L-shell is considered. The scaling of the total rate, the angular distributions of the emitted positrons and a comparison to the com… Show more

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Cited by 17 publications
(6 citation statements)
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“…Theoretical calculations were based on a laser-dressed quantum electrodynamics [17]. Theoretical predictions were also made for the pair creation that involves the nucleus in the laser fields [18][19][20][21][22][23][24]. The creation process triggered solely by a laser has the virtue of being free of any nuclear processes and can be studied more unambiguously on the theoretical level.…”
Section: Introductionmentioning
confidence: 99%
“…Theoretical calculations were based on a laser-dressed quantum electrodynamics [17]. Theoretical predictions were also made for the pair creation that involves the nucleus in the laser fields [18][19][20][21][22][23][24]. The creation process triggered solely by a laser has the virtue of being free of any nuclear processes and can be studied more unambiguously on the theoretical level.…”
Section: Introductionmentioning
confidence: 99%
“…Therefore, only the combination µ f = +1/2 and m s = +1/2 can compensate the helicity λ = +1, see Eq. (15). However as we already mentioned above, m s is the projection of the positron spin on the direction of the incident light which is related to the helicity as m s = m s = +1/2 for θ + = 0 • and m s = − m s = −1/2 for θ + = 180 • .…”
Section: A Differential Cross Sectionsmentioning
confidence: 91%
“…In contrast, for larger angles θ + the degree of polarization decreases and reaches the value P pos (θ + ) = −1 for θ + = 180 • ; the effect which can be expected from Eq. (15). The behaviour of P pos (θ + ) between the two ultimate angles θ + = 0 • and θ + = 180 • strongly depends on the positron energy and charge of the target ion.…”
Section: B Degree Of Polarizationmentioning
confidence: 99%
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“…. , 16. Each of the calculated values was obtained as the average of more than 10 9 sample points in each Monte Carlo run.…”
Section: Carrier-envelope Phase Effectsmentioning
confidence: 99%