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Beam Parameters

  The BEAM command makes it possible to define a beam in terms of the conventional Twiss parameters. A beam is defined by many parameters described in Sec.3.3. Here, we will give formulas how to generate a beam using these parameters. An important point is that the beam is defined on a plane s=constant rather than t=constant. Thus, the longitudinal structure of the beam appears as the time structure. Note that t is larger at the bunch tail.

The parameters are

tex2html_wrap_inline9544
Reference point of the Twiss parameters. (m)
tex2html_wrap_inline7362
Reference energy. (eV)
tex2html_wrap_inline9548
Twiss parameters.
tex2html_wrap_inline9550
Geometric emittance. (radtex2html_wrap_inline7234m)  
tex2html_wrap_inline7394
R.m.s. bunch length. (m)
tex2html_wrap_inline7398
R.m.s. relative energy spread.
tex2html_wrap_inline9558
Gaussian tail cut off.
tex2html_wrap_inline9560
Orbit slope. (rad)
tex2html_wrap_inline9562
Crab angle. (rad) 
tex2html_wrap_inline7454
Beam roll in the x-y plane. (rad)
tex2html_wrap_inline7450
Coherent energy slope (1/m).

First, generate particle variables in usual accelerator coordinate:




eqnarray3222


where tex2html_wrap_inline9572 (tex2html_wrap_inline9574) is a Gaussian random number of zero mean and unit standard deviation cut at tex2html_wrap_inline7408 (tex2html_wrap_inline7412), tex2html_wrap_inline9580 (j=1,2) is a random number of exponential distribution (tex2html_wrap_inline9584) cut at tex2html_wrap_inline9586 and tex2html_wrap_inline9588 a uniform random number in tex2html_wrap_inline9590.

These variables are then transformed to




eqnarray3230


Finally, the energy-momentum is given by




eqnarray3238


where tex2html_wrap_inline9528 is + for right-going beam and - for left-going (note that right/left appears only here) and m is the relevant particle mass in units of eV/ctex2html_wrap_inline7792.



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