Laser-assisted positronium formation in positron collisions with Rydberg hydrogen

We investigate the formation of positronium (Ps) in the presence of a linearly polarized infrared laser field, via the collision of positrons with Rydberg hydrogen atoms $\mathrm{H}({n}_{\mathrm{H}})$ where ${n}_{\mathrm{H}}$ is the principal quantum number. We are using the classical trajectory Monte Carlo method (CTMC) which is justified for ${n}_{\mathrm{H}}\ensuremath{\ge}3$. The hydrogen in excited states has an effective dipole moment which in the presence of a laser field leads to a dipolar focusing [H. B. Ambalampitiya et al., J. Phys. B: At. Mol. Opt. Phys. 57, 10LT01 (2024)]. Due to this effect, the Ps formation cross section is enhanced substantially as compared to the zero-field case. The degree of this enhancement is controlled by the positron velocity, laser frequency, and laser-field amplitude. The final-state distribution in Ps is much broader than in the zero-field case.

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Publication Details

Journal
Physical review. A/Physical review, A
Published
2025-02-12
DOI
https://doi.org/10.1103/physreva.111.022805
Primary Topic
Atomic and Molecular Physics
Type
article
Field-Weighted Citation Impact
0.00

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article

Laser-assisted positronium formation in positron collisions with Rydberg hydrogen

Harindranath Ambalampitiya, I. I. Fabrikant, M. K. Matfunjwa
Physical review. A/Physical review, A
Atomic and Molecular Physics
article

Laser-assisted positronium formation in positron collisions with Rydberg hydrogen

Harindranath Ambalampitiya, I. I. Fabrikant, M. K. Matfunjwa
article en

Abstract

We investigate the formation of positronium (Ps) in the presence of a linearly polarized infrared laser field, via the collision of positrons with Rydberg hydrogen atoms $\mathrm{H}({n}_{\mathrm{H}})$ where ${n}_{\mathrm{H}}$ is the principal quantum number. We are using the classical trajectory Monte Carlo method (CTMC) which is justified for ${n}_{\mathrm{H}}\ensuremath{\ge}3$. The hydrogen in excited states has an effective dipole moment which in the presence of a laser field leads to a dipolar focusing [H. B. Ambalampitiya et al., J. Phys. B: At. Mol. Opt. Phys. 57, 10LT01 (2024)]. Due to this effect, the Ps formation cross section is enhanced substantially as compared to the zero-field case. The degree of this enhancement is controlled by the positron velocity, laser frequency, and laser-field amplitude. The final-state distribution in Ps is much broader than in the zero-field case.

Physical review. A/Physical review, AVol. 111(2)
University of Nebraska–Lincoln (US)
National Science Foundation, U.S. Department of Energy, Office of Science, Basic Energy Sciences
Climate action
Openalex Percentile: Top 98%
Atomic and Molecular Physics
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