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Doc devel. #1055

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Jul 12, 2024
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Doc devel. #1055

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cf2d8b4
Fixed Tao `set particle_start` for photon energy
DavidSagan Jul 10, 2024
4c5ecc1
Merge branch 'main' of https://github.com/bmad-sim/bmad-ecosystem
DavidSagan Jul 12, 2024
1930200
Doc devel.
DavidSagan Jul 12, 2024
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2 changes: 1 addition & 1 deletion bmad/doc/cover-page.tex
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Expand Up @@ -3,7 +3,7 @@

\begin{flushright}
\large
Revision: July 7, 2024 \\
Revision: July 10, 2024 \\
\end{flushright}

\pdfbookmark[0]{Preamble}{Preamble}
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2 changes: 1 addition & 1 deletion bmad/doc/elements.tex
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Expand Up @@ -1266,7 +1266,7 @@ \section{Crystal}
\index{follow_diffracted_beam}\index{thickness}
Attributes specific to a \vn{crystal} element are:
\begin{example}
b_param = <Real> ! b parameter
b_param = <Real> ! b parameter for photons with the reference energy.
crystal_type = <String> ! Crystal material (\sref{s:cryst.list}) and reflection plane.
psi_angle = <Real> ! Rotation of H-vector about the surface normal.
thickness = <Real> ! Thickness of crystal for Laue diffraction.
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4 changes: 2 additions & 2 deletions bmad/doc/synchrotron-radiation.tex
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Expand Up @@ -247,9 +247,9 @@ \section{Synchrotron Radiation Integrals}
\label{s:synch.ints}
\index{synchrotron radiation!integrals}

the synchrotron radiation integrals can be used to compute emittances, the energy spread,
The synchrotron radiation integrals can be used to compute emittances, the energy spread,
etc. However, using the 6D damped and stochastic transport matrices (\sref{s:map.rad}) has
a number of advantages
a number of advantages:
\begin{itemize}
%
\item
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1 change: 1 addition & 0 deletions regression_tests/nonlin_test/small_ring.bmad
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@@ -1,6 +1,7 @@
parameter[p0c] = 1e9
bmad_com[radiation_damping_on] = f
bmad_com[radiation_fluctuations_on] = f
bmad_com[spin_tracking_on] = T

q1: quad, l = 0.5, k1 = 0.6, tilt = 0.05
q2: quad, l = 0.5, k1 = -0.5
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