Synchrotron Radiation power density

Synchrotron Radiation power density#

Basic example of computation of the power density of the radiation emitted by an electron beam deflected by the Simple dipole magnet magnet.

Import modules required for simulations and for comparison with the theoretical distribution of dipole radiation.

import pysrw as srw

We take as example the parameters of a typical bending magnet of a third-generation light source (ALBA-Spain)

energy = 3.0    # GeV
rho = 7.047     # m
length = 1.384  # m
gap = 36e-3     # m

The magnet is created with the default SRW model for dipoles and embedded in a magnet container

dipole = srw.magnets.Dipole(energy=energy, bendingR=rho,
                            coreL=length, edgeL=gap)

mag_container = srw.magnets.MagnetsContainer([dipole])

The last input for the simulation is the emitter, instance of ParticleBeam(). Note that we leave the default beam intensity of 1 A

beam = srw.emitters.ParticleBeam(energy, xPos=0, yPos=0, zPos=0)

Create a 5 mm x 5 mm observation mesh, with a resolution that matches the horizontal symmetry of dipole radiation

observer = srw.wavefronts.Observer(centerCoord=[0, 0, 5],
                                   obsXextension=5e-3,
                                   obsYextension=5e-3,
                                   obsXres=200e-6,
                                   obsYres=20e-6)

We can finally simulate and plot the power density radiated by the beam

pwrDensity = srw.computeSrPowerDensity(particleBeam=beam,
                                       magnetsContainer=mag_container,
                                       observer=observer, relPrec=10.)
srw.plotPwrDensity(pwrDensity)
power density
Warning: Electron Beam Emittance was not taken into account.

Total running time of the script: (0 minutes 19.151 seconds)

Estimated memory usage: 28 MB

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