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1\section{Introduction}
2
3Additional electromagnetic physics processes for photons, electrons, hadrons
4and ions have been implemented in Geant4 in order to extend the validity
5range of particle interactions to lower energies than those available in the
6standard Geant4 electromagnetic processes~\cite{ov-leg4,ov-had,ov-ion}.
7Because atomic shell structure is more important in most cases at low energies
8than it is at higher energies, the low energy processes make direct use of
9shell cross section data.  The standard processes, which are optimized for
10high energy physics applications, rely on parameterizations of these data.
11 
12The low energy processes include the photo-electric effect, Compton scattering,
13Rayleigh scattering, gamma conversion, bremsstrahlung and ionization. 
14Fluorescence of excited atoms is also considered. 
15
16Some features common to all low energy processes currently implemented in
17Geant4 are summarized in this section.  Subsequent sections provide more
18detailed information for each process.
19
20\subsection{Physics}
21
22The low energy processes of Geant4 represent electromagnetic interactions
23at lower energies than those covered by the equivalent Geant4 standard
24electromagnetic processes.
25
26The current implementation of low energy processes is valid for energies
27down to 250 eV (and can be used up to approximately 100 GeV), unless
28differently specified.  It covers elements with atomic number between 1 and
2999.
30
31All processes involve two distinct phases:
32\begin{itemize}
33\item the calculation and use of total cross sections, and
34\item the generation of the final state.
35\end{itemize}
36Both phases are based on the theoretical models and on
37exploitation of evaluated data.
38
39\subsection{Data Sources}
40
41The data used for the determination of cross-sections and
42for sampling of the final state are extracted
43from a set of publicly distributed evaluated data
44libraries:
45\begin{itemize}
46\item
47EPDL97 (Evaluated Photons Data Library)~\cite{ov-EPDL97};
48\item
49EEDL (Evaluated Electrons Data Library)~\cite{ov-EEDL};
50\item
51EADL (Evaluated Atomic Data Library)~\cite{ov-EADL};
52\item
53stopping power data~\cite{ov-Ziegler771,ov-Ziegler774,ov-Ziegler85,ov-ICRU49};
54\item
55binding energy values based on data of Scofield~\cite{ov-bindingEnergies}.
56\end{itemize}
57
58Evaluated data sets are produced through the process of critical comparison,
59selection, renormalization and averaging of the available experimental data,
60normally complemented by model calculations.
61%Evaluated Libraries are computer files of evaluated data which, appropriately
62%processed, form the input data to computations for a wide variety of nuclear
63%science and technology applications. Each of these evaluated libraries
64%may consist of individual evaluated data sets for several hundred isotopes
65%or elements (commonly referred to as 'materials')~\cite{ov-NEA}.
66These libraries provide the following data relevant for the simulation of
67Geant4 low energy processes:
68
69\begin{itemize}
70
71\item 
72total cross-sections for photoelectric effect, Compton scattering,
73Rayleigh scattering, pair production and bremsstrahlung,
74\item 
75subshell integrated cross sections for photo-electric effect and ionization,
76\item 
77energy spectra of the secondaries for electron processes,
78\item 
79scattering functions for the Compton effect,
80\item 
81form factors for Rayleigh scattering,
82\item 
83binding energies for electrons for all subshells,
84\item 
85transition probabilities between subshells for fluorescence and the Auger
86effect, and
87\item
88stopping power tables.
89\end{itemize}
90
91The energy range covered by the data libraries extends from 100 GeV
92down to 1 eV for Rayleigh and Compton effects, down to the lowest binding
93energy for each element for photo-electric effect and ionization, and
94down to 10 eV for bremsstrahlung.
95
96%\subsubsection{Data validity and accuracy}
97%For a rough estimate of the accuracy of EPDL97 data libraries in different
98%energy regimes, see \cite{ov-data-est}.
99%The data are only applicable to cold, neutral,
100%ground-state and isolated atoms,
101%i.e. solid-state effects, plasmas,
102%external electric or magnetic fields are not taken into
103%account although they could have significant
104%effects on the cross-sections near photoeffect
105%thresholds of inner-shell electrons,
106%and completely alter the cross-sections near the
107%thresholds of outer-shells~\cite{ov-EPDL97}.
108
109%The precision of the binding energies is estimated
110%to be better than 1\%~\cite{ov-EPDL97}
111%which is small compared to the differences expected due
112%to elements combining into radicals or
113%compounds.
114%For example, the K shell binding energy of
115%H is 13.6 eV, and that of H2 is 16.4 eV,
116%about 21\% higher. This will effect accuracy
117%over narrow energy ranges near photoionisation
118%edges.
119
120%Precision estimates on the data can be
121%found in~\cite{ov-EPDL97},~\cite{ov-EEDL} and~\cite{ov-EADL}.
122
123\subsection{Distribution of the Data Sets}
124
125The author of EPDL97~\cite{ov-EPDL97}, who is also responsible for the
126EEDL~\cite{ov-EEDL} and EADL~\cite{ov-EADL} data libraries, Dr. Red Cullen,
127has kindly permitted the libraries and their related documentation to be
128distributed with the Geant4 toolkit.  The data are reformatted for Geant4
129input.  They can be downloaded from the source code section of the Geant4
130page:  http://cern.ch/geant4/geant4.html.
131
132The EADL, EEDL and EPDL97 data-sets are also available from several
133public distribution centres in a format different
134from the one used by Geant4~\cite{ov-NEA}.
135
136Stopping power data are taken from
137publications~\cite{ov-Ziegler771,ov-Ziegler774,ov-Ziegler85,ov-ICRU49}.
138
139\subsection{Calculation of Total Cross Sections}\label{subsubsigmatot}
140
141The energy dependence of the total cross section is derived for each
142process from the evaluated data libraries.  Since the libraries provide
143cross sections for a set of discrete incident energies, the total cross
144section at a given energy, $E$, is obtained by interpolation according to
145the formula~\cite{ov-stepanek}:
146\begin{equation}
147  \label{eqloglog}
148  \log(\sigma(E)) = {log(\sigma_1)log(E_2/E) + log(\sigma_2)log(E/E_1)
149                      \over log(E_2/E_1)}
150\end{equation}
151where $E_1$ and $E_2$ are respectively the closest lower and higher energy 
152for which data ($\sigma_1$ and $\sigma_2$) are available.
153
154For each process a production threshold energy is defined;  by default it
155is set to the low end of the energy validity range of the process (250~eV
156in the current implementation), but a higher or lower value can be set by
157the user. 
158
159For a particle of energy $E$, the mean free path for interacting via a
160given process is calculated as:
161\begin{equation}
162  \lambda = {1\over{\Sigma_i\\ \sigma_{i}(E)\cdot n_i}}
163\end{equation}
164where $\sigma_{i}(E)$ is the microscopic
165integrated cross-section of the process considered at energy $E$, and $n_i$ 
166is the atomic density of the $i-th$ element contributing to the material
167composition.  The sum runs over all the elements of which the material is
168composed.  The cross sections are determined as described in this section. 
169An exception to this method is the implementation of the chemical effect on
170hadron/ion stopping powers for a set of materials.
171
172
173\subsection{Sampling of Relevant Physics Quantities}
174
175The final state products of the processes are generated by sampling
176relevant physical quantities, such as energies and angular distributions
177of secondaries, from distributions derived from theoretical models and
178evaluated data.  The energy dependence of the parameters which characterize
179the distributions is taken into account either by direct interpolation of
180the data available in the libraries, or by interpolation of values obtained
181from fits to the data.
182
183When generating the final state, an atom of the material in which the
184interaction occurs is randomly selected and atomic de-excitation is
185simulated.
186
187Secondaries which would be produced with energies below their user defined
188production threshold are not created and their energy is deposited locally.
189
190
191\subsection{Status of the document}
192
193\noindent
19430.09.1999 created by Alessandra Forti\\
19507.02.2000 modified by V\'eronique Lef\'ebure\\
19608.03.2000 reviewed by Petteri Nieminen and Maria Grazia Pia\\
19704.12.2001 reviewed by Vladimir Ivanchenko\\
19826.01.2003 minor re-write by D.H. Wright .
199
200
201\begin{latexonly}
202
203\begin{thebibliography}{99}
204\bibitem{ov-leg4}
205 ``Geant4 Low Energy Electromagnetic Models for Electrons and Photons",
206   J.Apostolakis et al., CERN-OPEN-99-034(1999), INFN/AE-99/18(1999)
207\bibitem{ov-had}
208V.N.~Ivanchenko et al., GEANT4 Simulation of
209Energy Losses of Slow Hadrons, CERN-99-121, INFN/AE-99/20, (September 1999).
210\bibitem{ov-ion}
211S.~Giani et al., GEANT4 Simulation of
212Energy Losses of Ions, CERN-99-300, INFN/AE-99/21, (November 1999).
213\bibitem{ov-EPDL97} 
214  %http://reddog1.llnl.gov/homepage.red/photon.htm
215 ``EPDL97: the Evaluated Photon Data Library, '97 version",
216  D.Cullen, J.H.Hubbell, L.Kissel,
217  UCRL--50400, Vol.6, Rev.5
218\bibitem{ov-EEDL} 
219  %http://reddog1.llnl.gov/homepage.red/Electron.htm
220  ``Tables and Graphs of Electron-Interaction Cross-Sections from 10~eV to 100~GeV Derived from
221  the LLNL Evaluated Electron Data Library (EEDL), Z=1-100"
222  S.T.Perkins, D.E.Cullen, S.M.Seltzer,
223  UCRL-50400 Vol.31
224\bibitem{ov-EADL} 
225  %http://reddog1.llnl.gov/homepage.red/ATOMIC.htm
226  ``Tables and Graphs of Atomic Subshell and Relaxation Data Derived from
227  the LLNL Evaluated Atomic Data Library (EADL), Z=1-100"
228  S.T.Perkins, D.E.Cullen, M.H.Chen, J.H.Hubbell, J.Rathkopf, J.Scofield,
229  UCRL-50400 Vol.30
230\bibitem{ov-Ziegler771}
231H.H.~Andersen and J.F.~Ziegler,
232The Stopping
233and Ranges of Ions in Matter. Vol.3, Pergamon Press, 1977.
234\bibitem{ov-Ziegler774}
235J.F.~Ziegler, The Stopping
236and Ranges of Ions in Matter. Vol.4, Pergamon Press, 1977.
237\bibitem{ov-Ziegler85}
238J.F.~Ziegler, J.P.~Biersack,
239U.~Littmark, The Stopping
240and Ranges of Ions in Solids. Vol.1, Pergamon Press, 1985.
241\bibitem{ov-ICRU49}
242ICRU (A.~Allisy et al),
243Stopping Powers and Ranges for Protons and Alpha
244Particles,
245ICRU Report 49, 1993.
246\bibitem{ov-bindingEnergies}
247  J.H. Scofield, ``Radiative Transitions", in ``Atomic Inner-Shell Processes",
248  B.Crasemann ed. (Academic Press, New York, 1975),pp.265-292.
249%\bibitem{ov-data-est}
250%  http://reddog1.llnl.gov/homepage.red/DOCUMENT/EPDL97/epdl97.htm
251\bibitem{ov-NEA}
252  http://www.nea.fr/html/dbdata/nds\_evaluated.htm
253\bibitem{ov-stepanek}
254   ``New Photon, Positron and Electron Interaction Data
255for Geant in Energy Range
256   from 1 eV to 10 TeV",
257   J. Stepanek, Draft to be submitted for publication
258
259\end{thebibliography}
260
261\end{latexonly}
262
263\begin{htmlonly}
264
265\subsection{Bibliography}
266
267\begin{enumerate}
268\item
269 ``Geant4 Low Energy Electromagnetic Models for Electrons and Photons",
270   J.Apostolakis et al., CERN-OPEN-99-034(1999), INFN/AE-99/18(1999)
271\item
272V.N.~Ivanchenko et al., GEANT4 Simulation of
273Energy Losses of Slow Hadrons, CERN-99-121, INFN/AE-99/20, (September 1999).
274\item
275S.~Giani et al., GEANT4 Simulation of
276Energy Losses of Ions, CERN-99-300, INFN/AE-99/21, (November 1999).
277\item
278  %http://reddog1.llnl.gov/homepage.red/photon.htm
279 ``EPDL97: the Evaluated Photon Data Library, '97 version",
280  D.Cullen, J.H.Hubbell, L.Kissel,
281  UCRL--50400, Vol.6, Rev.5
282\item 
283  %http://reddog1.llnl.gov/homepage.red/Electron.htm
284  ``Tables and Graphs of Electron-Interaction Cross-Sections from 10~eV to 100~GeV Derived from
285  the LLNL Evaluated Electron Data Library (EEDL), Z=1-100"
286  S.T.Perkins, D.E.Cullen, S.M.Seltzer,
287  UCRL-50400 Vol.31
288\item 
289  %http://reddog1.llnl.gov/homepage.red/ATOMIC.htm
290  ``Tables and Graphs of Atomic Subshell and Relaxation Data Derived from
291  the LLNL Evaluated Atomic Data Library (EADL), Z=1-100"
292  S.T.Perkins, D.E.Cullen, M.H.Chen, J.H.Hubbell, J.Rathkopf, J.Scofield,
293  UCRL-50400 Vol.30
294\item
295H.H.~Andersen and J.F.~Ziegler,
296The Stopping
297and Ranges of Ions in Matter. Vol.3, Pergamon Press, 1977.
298\item
299J.F.~Ziegler, The Stopping
300and Ranges of Ions in Matter. Vol.4, Pergamon Press, 1977.
301\item
302J.F.~Ziegler, J.P.~Biersack,
303U.~Littmark, The Stopping
304and Ranges of Ions in Solids. Vol.1, Pergamon Press, 1985.
305\item
306ICRU (A.~Allisy et al),
307Stopping Powers and Ranges for Protons and Alpha
308Particles,
309ICRU Report 49, 1993.
310\item
311  J.H. Scofield, ``Radiative Transitions", in ``Atomic Inner-Shell Processes",
312  B.Crasemann ed. (Academic Press, New York, 1975),pp.265-292.
313%\bibitem{ov-data-est}
314%  http://reddog1.llnl.gov/homepage.red/DOCUMENT/EPDL97/epdl97.htm
315\item
316  http://www.nea.fr/html/dbdata/nds\_evaluated.htm
317\item
318   ``New Photon, Positron and Electron Interaction Data
319for Geant in Energy Range
320   from 1 eV to 10 TeV",
321   J. Stepanek, Draft to be submitted for publication
322\end{enumerate}
323
324\end{htmlonly}
325
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