diff --git a/wk/He_ela_cross_sec.in b/wk/He_ela_cross_sec.in new file mode 100644 index 0000000..20c9d2b --- /dev/null +++ b/wk/He_ela_cross_sec.in @@ -0,0 +1,115 @@ +!LXCat, www.lxcat.net +!Generated on 17 Feb 2022. All rights reserved. +! +!RECOMMENDED REFERENCE FORMAT +!- Biagi database, www.lxcat.net, retrieved on February 17, 2022. +!Be aware that some databases and solvers can additionally have instructions how to reference corresponding data. +!Please check below in the headers of databases. +! +!CROSS SECTION DATA FORMAT +!In downloaded files, each collision process is defined by a block consisting of +!1st line +!Keyword in capitals indicating the type of the collision. Possible collision types are elastic, effective, excitation, +!ionization, or attachment (capital letters required, key words are case sensitive), where "elastic" is used to denote +!the elastic momentum transfer cross section and where "effective" denotes the total momentum transfer cross section (sum +!of elastic momentum transfer and total inelastic cross sections). The latter is useful for solving the Boltzmann +!equation in the 2-term approximation. +!2nd line +!Name of the target particle species. This name is a character string, freely chosen by the user, e.g. "Ar". Optionally +!for excitation processes, the name of the corresponding excited state can be specified on the same line, separated from +!the first name either by arrow "->" (dash + greater than) or by double-head arrow "<->" (less than + dash + +!greater than), e.g. "Ar -> Ar*" and "Ar <-> Ar*", respectively. In the later case BOLSIG+ will automatically +!define the inverse superelastic process, constructing the superelastic cross-section by detailed balancing, and +!considering the indicated excited state as the target. In this case, the ratio of statistical weights must be input in +!the 3rd line (see below). +!3rd line +!For elastic and effective collisions, the ratio of the electron mass to the target particle mass. For excitation or +!ionization collisions, the electron energy loss (nominally the threshold energy) in eV. For attachment, the 3rd line is +!missing. In case of an excitation process where an excited state has been indicated on the 2nd line using double-head +!arrow "<->", the 3rd line must specify also ratio of the statistical weights of the final state to the initial state +!as the second parameter in 3rd line this is needed by BOLSIG+ to calculate the de-excitation cross-section. The +!statistical weight ratio, if given, will also be used by the automatic superelastics option in BOLSIG+. If this ratio is +!not provided then BOLSIG+ will assume it unity. +!from 4th line (optionally) +!User comments and reference information, maximum 100 lines. The only constraint on format is that these comment lines +!must not start with a number. +!Finally +!Table of the cross section as a function of energy. The table starts and ends by a line of dashes "------" (at least 5), +!and has otherwise two numbers per line: the energy in eV and the cross section in m2. +! +!xxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxx +!DATABASE: Biagi (transcription of data from SF Biagi's Fortran code, Magboltz.) +!PERMLINK: www.lxcat.net/Biagi +!DESCRIPTION: These data were transcribed from S.F. Biagi's FORTRAN code, MagBoltz, versions 8.9 and later. The +! exact version number is given for each species. At this time, the Biagi database contains cross +! sections for rare gases, for a few simple molecules, and for SF6. The transcription of cross sections +! for other gases is in progress. These data were compiled for use a Monte Carlo simulation (or +! multi-term Boltzmann code), but their use in a 2-term Boltzmann solver gives reasonably accurate +! results in most cases. The the LXCat data tables do not always have the same energy resolution as the +! original data in the MagBoltz code. This limited energy resolution can introduce small (1%) +! differences in the calculated drift velocity at low E/N. +! For history and detailed notes, see http://consult.cern.ch/writeup/magboltz/ +! +! Oct 2011 : update of Ar and Kr data taken from MagBoltz version 8.97 Nov 2011 : small changes in Xe +! ionization cross sections, taken from MagBoltz v8.97 +! March 2015: cross sections for SF6 were transcribed from Magboltz version 10.6 from February 2014. +!CONTACT: email Stephen.biagi@@hotmail.co.uk +!HOW TO REFERENCE: Fortran program, MAGBOLTZ, S.F. Biagi. The version number of MAGBOLTZ from which the cross sections +! were transcribed is provided in the comment for each species. This version number must be included in +! the reference. +!xxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxx +! +!************************************************************************************************************************ +! +!COMMENT: Transcribed from S.F. Biagi's FORTRAN code Magboltz, version 8.97, Sept 2011. +! Based in part on K Bartschat 1998 and Ralchenko et al 2008 (after 30 eV). +! +!********************************************************** He ********************************************************** +! +!ELASTIC +!He +! 1.360000e-4 +!SPECIES: e / He +!PROCESS: E + He -> E + He, Elastic +!PARAM.: m/M = 0.000136, complete set +!COMMENT: From Biagi's elastic momentum transfer. +!UPDATED: 2015-03-12 13:44:44 +!COLUMNS: Energy (eV) | Cross section (m2) +!----------------------------- + 0.000000e+0 4.903500e-20 + 1.000000e-4 4.903500e-20 + 3.514000e-2 5.501140e-20 + 7.152000e-2 5.747600e-20 + 1.091700e-1 5.896700e-20 + 1.371370e+0 6.938560e-20 + 5.918310e+0 6.025320e-20 + 8.440610e+0 5.209010e-20 + 1.102264e+1 4.444340e-20 + 1.379108e+1 3.734320e-20 + 1.657924e+1 3.184430e-20 + 1.918366e+1 2.766530e-20 + 2.217395e+1 2.383470e-20 + 2.560725e+1 1.998990e-20 + 2.954921e+1 1.667870e-20 + 3.407519e+1 1.385490e-20 + 3.790451e+1 1.190580e-20 + 4.215191e+1 1.024370e-20 + 4.686301e+1 8.806780e-21 + 5.588529e+1 6.702370e-21 + 6.660830e+1 5.073960e-21 + 7.935261e+1 3.808260e-21 + 9.449926e+1 2.878530e-21 + 1.125011e+2 2.204960e-21 + 1.338963e+2 1.622750e-21 + 1.593245e+2 1.224330e-21 + 1.895461e+2 9.142570e-22 + 2.254644e+2 6.756040e-22 + 2.681535e+2 4.949030e-22 + 3.188895e+2 3.701550e-22 + 3.791894e+2 2.748810e-22 + 4.508559e+2 2.023320e-22 + 5.360318e+2 1.477860e-22 + 6.372635e+2 1.101690e-22 + 7.575776e+2 8.165410e-23 + 9.005711e+2 5.983320e-23 +!----------------------------- diff --git a/wk/He_io_cross_sec.in b/wk/He_io_cross_sec.in new file mode 100644 index 0000000..2914796 --- /dev/null +++ b/wk/He_io_cross_sec.in @@ -0,0 +1,186 @@ +!LXCat, www.lxcat.net +!Generated on 17 Feb 2022. All rights reserved. +! +!RECOMMENDED REFERENCE FORMAT +!- Biagi database, www.lxcat.net, retrieved on February 17, 2022. +!Be aware that some databases and solvers can additionally have instructions how to reference corresponding data. +!Please check below in the headers of databases. +! +!CROSS SECTION DATA FORMAT +!In downloaded files, each collision process is defined by a block consisting of +!1st line +!Keyword in capitals indicating the type of the collision. Possible collision types are elastic, effective, excitation, +!ionization, or attachment (capital letters required, key words are case sensitive), where "elastic" is used to denote +!the elastic momentum transfer cross section and where "effective" denotes the total momentum transfer cross section (sum +!of elastic momentum transfer and total inelastic cross sections). The latter is useful for solving the Boltzmann +!equation in the 2-term approximation. +!2nd line +!Name of the target particle species. This name is a character string, freely chosen by the user, e.g. "Ar". Optionally +!for excitation processes, the name of the corresponding excited state can be specified on the same line, separated from +!the first name either by arrow "->" (dash + greater than) or by double-head arrow "<->" (less than + dash + +!greater than), e.g. "Ar -> Ar*" and "Ar <-> Ar*", respectively. In the later case BOLSIG+ will automatically +!define the inverse superelastic process, constructing the superelastic cross-section by detailed balancing, and +!considering the indicated excited state as the target. In this case, the ratio of statistical weights must be input in +!the 3rd line (see below). +!3rd line +!For elastic and effective collisions, the ratio of the electron mass to the target particle mass. For excitation or +!ionization collisions, the electron energy loss (nominally the threshold energy) in eV. For attachment, the 3rd line is +!missing. In case of an excitation process where an excited state has been indicated on the 2nd line using double-head +!arrow "<->", the 3rd line must specify also ratio of the statistical weights of the final state to the initial state +!as the second parameter in 3rd line this is needed by BOLSIG+ to calculate the de-excitation cross-section. The +!statistical weight ratio, if given, will also be used by the automatic superelastics option in BOLSIG+. If this ratio is +!not provided then BOLSIG+ will assume it unity. +!from 4th line (optionally) +!User comments and reference information, maximum 100 lines. The only constraint on format is that these comment lines +!must not start with a number. +!Finally +!Table of the cross section as a function of energy. The table starts and ends by a line of dashes "------" (at least 5), +!and has otherwise two numbers per line: the energy in eV and the cross section in m2. +! +!xxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxx +!DATABASE: Biagi (transcription of data from SF Biagi's Fortran code, Magboltz.) +!PERMLINK: www.lxcat.net/Biagi +!DESCRIPTION: These data were transcribed from S.F. Biagi's FORTRAN code, MagBoltz, versions 8.9 and later. The +! exact version number is given for each species. At this time, the Biagi database contains cross +! sections for rare gases, for a few simple molecules, and for SF6. The transcription of cross sections +! for other gases is in progress. These data were compiled for use a Monte Carlo simulation (or +! multi-term Boltzmann code), but their use in a 2-term Boltzmann solver gives reasonably accurate +! results in most cases. The the LXCat data tables do not always have the same energy resolution as the +! original data in the MagBoltz code. This limited energy resolution can introduce small (1%) +! differences in the calculated drift velocity at low E/N. +! For history and detailed notes, see http://consult.cern.ch/writeup/magboltz/ +! +! Oct 2011 : update of Ar and Kr data taken from MagBoltz version 8.97 Nov 2011 : small changes in Xe +! ionization cross sections, taken from MagBoltz v8.97 +! March 2015: cross sections for SF6 were transcribed from Magboltz version 10.6 from February 2014. +!CONTACT: email Stephen.biagi@@hotmail.co.uk +!HOW TO REFERENCE: Fortran program, MAGBOLTZ, S.F. Biagi. The version number of MAGBOLTZ from which the cross sections +! were transcribed is provided in the comment for each species. This version number must be included in +! the reference. +!xxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxx +! +!************************************************************************************************************************ +! +!COMMENT: Transcribed from S.F. Biagi's FORTRAN code Magboltz, version 8.97, Sept 2011. +! Based in part on K Bartschat 1998 and Ralchenko et al 2008 (after 30 eV). +! +!********************************************************** He ********************************************************** +! +! IONIZATION +! He -> He^+ +! 2.458740e+1 +! SPECIES: e / He +! PROCESS: E + He -> E + E + He+, Ionization +! PARAM.: E = 24.5874 eV, complete set +! UPDATED: 2011-10-21 15:05:18 +! COLUMNS: Energy (eV) | Cross section (m2) +! ----------------------------- + 2.458739e+1 0.000000e+0 + 2.458800e+1 9.936770e-27 + 2.462253e+1 3.491990e-24 + 2.465891e+1 7.106710e-24 + 2.469657e+1 1.084840e-23 + 2.473554e+1 1.472170e-23 + 2.477589e+1 1.873100e-23 + 2.481766e+1 2.288130e-23 + 2.486089e+1 2.717740e-23 + 2.490565e+1 3.162440e-23 + 2.495197e+1 3.622780e-23 + 2.499993e+1 4.099290e-23 + 2.504957e+1 4.694820e-23 + 2.510095e+1 5.311430e-23 + 2.515414e+1 5.949700e-23 + 2.520920e+1 6.610410e-23 + 2.526619e+1 7.294340e-23 + 2.532519e+1 8.002300e-23 + 2.538626e+1 8.735140e-23 + 2.544948e+1 9.493740e-23 + 2.551492e+1 1.029390e-22 + 2.558265e+1 1.117450e-22 + 2.565277e+1 1.208600e-22 + 2.572535e+1 1.302960e-22 + 2.580049e+1 1.400630e-22 + 2.587826e+1 1.501740e-22 + 2.595876e+1 1.606390e-22 + 2.604210e+1 1.716410e-22 + 2.612836e+1 1.832010e-22 + 2.621766e+1 1.951660e-22 + 2.631009e+1 2.075520e-22 + 2.640577e+1 2.203740e-22 + 2.650482e+1 2.336360e-22 + 2.660734e+1 2.471690e-22 + 2.671347e+1 2.611780e-22 + 2.682333e+1 2.756790e-22 + 2.693705e+1 2.906900e-22 + 2.705476e+1 3.056810e-22 + 2.717661e+1 3.205460e-22 + 2.730274e+1 3.359350e-22 + 2.743331e+1 3.518640e-22 + 2.756846e+1 3.680790e-22 + 2.770837e+1 3.845870e-22 + 2.785319e+1 4.016760e-22 + 2.800310e+1 4.193590e-22 + 2.815827e+1 4.373600e-22 + 2.831890e+1 4.559930e-22 + 2.848518e+1 4.752810e-22 + 2.865730e+1 4.965050e-22 + 2.883547e+1 5.185980e-22 + 2.901989e+1 5.414270e-22 + 2.921080e+1 5.647180e-22 + 2.940842e+1 5.888280e-22 + 2.961299e+1 6.124290e-22 + 2.982474e+1 6.357210e-22 + 3.004393e+1 6.601840e-22 + 3.027083e+1 6.869580e-22 + 3.050570e+1 7.146730e-22 + 3.074883e+1 7.433610e-22 + 3.100049e+1 7.730530e-22 + 3.126101e+1 8.011890e-22 + 3.153067e+1 8.304970e-22 + 3.180982e+1 8.623190e-22 + 3.209877e+1 8.950620e-22 + 3.239788e+1 9.285620e-22 + 3.270750e+1 9.624100e-22 + 3.302800e+1 9.971360e-22 + 3.335976e+1 1.034290e-21 + 3.370319e+1 1.070320e-21 + 3.405868e+1 1.105870e-21 + 3.442666e+1 1.142670e-21 + 3.480758e+1 1.180760e-21 + 3.520188e+1 1.220190e-21 + 3.561004e+1 1.261000e-21 + 3.603254e+1 1.302930e-21 + 3.646989e+1 1.342290e-21 + 3.692261e+1 1.383030e-21 + 3.739123e+1 1.425210e-21 + 3.787633e+1 1.468870e-21 + 3.837847e+1 1.512170e-21 + 3.889827e+1 1.556350e-21 + 3.943632e+1 1.602090e-21 + 3.999329e+1 1.649430e-21 + 4.056983e+1 1.691030e-21 + 4.116663e+1 1.734000e-21 + 4.178440e+1 1.778480e-21 + 4.242388e+1 1.824520e-21 + 4.308584e+1 1.872180e-21 + 4.377105e+1 1.921520e-21 + 4.448035e+1 1.972590e-21 + 4.521458e+1 2.024160e-21 + 4.597460e+1 2.074320e-21 + 4.676134e+1 2.126250e-21 + 4.757572e+1 2.180000e-21 + 4.841872e+1 2.235640e-21 + 5.632146e+1 2.645500e-21 + 7.000000e+1 3.130000e-21 + 8.000000e+1 3.320000e-21 + 9.000000e+1 3.440000e-21 + 1.000000e+2 3.510000e-21 + 1.500000e+2 3.460000e-21 + 2.000000e+2 3.240000e-21 + 3.000000e+2 2.900000e-21 + 4.309677e+2 2.362320e-21 + 5.000000e+2 2.200000e-21 + 6.401824e+2 1.811600e-21 + 9.568417e+2 1.357680e-21 +----------------------------- +xxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxx \ No newline at end of file