Relativistic electron scattering from freely movable proton/<inline-formula> <tex-math> <?CDATA ${{\rm{\mu }}}^{+}$?> </tex-math><mml:math> <mml:msup> <mml:mrow> <mml:mi mathvariant="normal">μ</mml:mi> </mml:mrow> <mml:mrow> <mml:mo>+</mml:mo> </mml:mrow> </mml:msup> </mml:math> <inline-graphic xmlns:xlink="https://www.w3.org/1999/xlink" xlink:href="cpb_28_9_093402_ieqn1.gif"/> </inline-formula> in the presence of strong laser field

Relativistic electron scattering from freely movable proton/

μ +

in the presence of strong laser field

Wang Ningyue¹, Jiao Liguang², Liu Aihua^{1, 3, †}

The cross section of scattering versus the field intensity at θ = 90 ° and ϕ = 0 ° . The solid line is the laser-free case, and the dashed line is the dependence on different laser intensities. The photon energy ℏ ω = 1.17 eV .