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SYNCRAD


     Activates synchrotron radiation emission for selected charged particles

     See also ASSIGNMAT


     For 
SDUM
= BMAX-REG (see note 1) below), compulsory when the magnetic field is not constant and uniform, and or anyway is provided by a magfld.f routine:
WHAT(1)
= Maximum magnetic field intensity (T) in the regions defined by WHAT(4-6), no default
WHAT(2)
= not used
WHAT(3)
= not used
WHAT(4)
= lower bound (or name corresponding to it) of the region indices with maximum magnetic field intensity corresponding to
WHAT(1)
. ("From region
WHAT(4)
...")
Default
= 2.0
WHAT(5)
= upper bound (or name corresponding to it) of the region indices with maximum magnetic field intensity corresponding to
WHAT(1)
. ("...to region
WHAT(5)
...")
Default
=
WHAT(4)
WHAT(6)
= step length in assigning indices ("...in steps of
WHAT(6)
")
Default
= 1.0
SDUM
= BMAX-REG For
SDUM
= SYPRONLY, SYNCRALL, or null:
WHAT(1)
> 0 : Synchrotron radiation emission activated for the particles defined by
WHAT(4)
, (5), and (6), down to the photon energy threshold given by
WHAT(1)
(GeV) < 0 : Synchrotron radiation emission de-activated for the particles defined by
WHAT(4)
, (5), and (6) = 0 : ignored
WHAT(2)
> 0 : Upper threshold (GeV) for considering synchrotron radiation photons as optical photons and transport them as such. If defined, synchrotron radiation photons with energy between
WHAT(1)
and
WHAT(2)
will be loaded on the optical photon stack and then transported as such. Viceversa, those with energy above
WHAT(2)
will be transported and interact using EMF < 0 : reset to default
Default
= 0.0
WHAT(3)
> 0 : relativistic gamma factor (E/m) threshold for generating synchrotron radiation photons. Only charged particles with gamma larger than the threshold will emit sychrotron radiation photons. It cannot be set lower than 3 < 0 : reset to default
Default
= 100.0
WHAT(4)
= lower bound of the particle numbers (or corresponding name) for which synchrotron radiation is activated ("From particle
WHAT(4)
...").
Default
= 1.0
WHAT(5)
= upper bound of the particle numbers (or corresponding name) for which synchrotron radiation is activated ("...to particle
WHAT(5)
...").
Default
=
WHAT(4)
if
WHAT(4)
> 0, 1.0 otherwise.
WHAT(6)
= step length in assigning numbers. ("...in steps of
WHAT(6)
").
Default
= 1.0
SDUM
= SYPRONLY: synchrotron radiation emission restricted to primary particles only SYNCRALL: synchrotron radiation emission activated for all generations
Default
(
SDUM
null) synchrotron radiation emission activated for all generations
Default
(option SYNCRAD not given): synchrotron radiation activated for all generations of electrons, positrons, and muons inside the regions flagged for synchrotron radiation emission (see ASSIGNMAT), with minimum photon energy set at 1 eV, no optical photons, and minimum gamma set at 100, for all particle generations
Notes:
1) Setting of the maximum magnetic field intensity is compulsory for all regions where synchrotron radiation emission is activated (see the ASSIGNMAt option) if the magnetic field is not constant and uniform, or anyway provided by a magfld routine (see the MGNFIELD option). The maximum magnetic field does not need to be "exact" to the last digit, an approximate upper boundary is sufficient. 2) Synchrotron radiation emission activation is automatically ignored for neutral particles included in those defined by
WHAT(4)
, (5), and (6),
SDUM
= SYPRONLY, SYNCRALL, or null. 3) The maximum magnetic field intensity is automatically ignored for regions not flagged for synchrotron radiation production with the ASSIGNMAt card, even if defined by
WHAT(4)
, (5), and (6),
SDUM
= BMAX-REG. 4) The emission threshold can be set as low as 1 eV (indeed by default it is set to 1 eV) even if FLUKA cannot deal with photons below 100 eV and no optical photon properties are set by the user. In this way most of the emitted power is anyway generated, transported through vacuum and then dumped in the first material region encountered. Therefore the emitting particle energy loss and the power loading on eg a vacuum chamber can still be accurately described.

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