next up previous contents index
Next: Usage Up: Breit-Wheeler Process Previous: Breit-Wheeler Process

Formulas

    k,tex2html_wrap_inline10922,p,p'
    4-momenta of the initial photon, laser photon, final electron and positron.
    tex2html_wrap_inline10028,tex2html_wrap_inline10240,tex2html_wrap_inline9312,tex2html_wrap_inline11322
    Energies of the initial photon, laser photon, final electron and positron.
    tex2html_wrap_inline7924
    Laser intensity parameter
    tex2html_wrap_inline7944
    Laser energy parameter: tex2html_wrap_inline11328.
    n
    Number of absorbed laser photons
    x
    =tex2html_wrap_inline11334. (0<x<1)
    u
    u=1/[4x(1-x)], tex2html_wrap_inline11342, (tex2html_wrap_inline11344).
    tex2html_wrap_inline11346
    Maximum u for given n: tex2html_wrap_inline11352.
    tex2html_wrap_inline10978
    tex2html_wrap_inline11356
    tex2html_wrap_inline10254
    Initial photon helicity
    tex2html_wrap_inline10222
    Laser helicity
    tex2html_wrap_inline10220
    Final electron helicity
    tex2html_wrap_inline10256
    `Detector' helicity of the final electron.
    tex2html_wrap_inline11366
    Final electron angle
    tex2html_wrap_inline11368
    tex2html_wrap_inline11012
    The argument of the Bessel functions in the following expressions:
    tex2html_wrap_inline11372

Total number of pair electrons per unit time summed over the positron polarization is
equation6156
Sum over final electron polarization gives
equation6158





eqnarray6164


These formulas can be obtained from those of tex2html_wrap_inline10242 by the replacement
equation6168
This implies
equation6170
For convenience, we have changed the sign as
equation6172

For given x and n, the final momenta are given by
equation6174

equation6176
Here, tex2html_wrap_inline8612 is the azimuthal scattering angle in a head-on frame and
equation6178
These vectors satisfy
equation6219


Toshiaki Tauchi
Thu Dec 3 17:27:26 JST 1998