This is just a sample file to test loading the data from the LXCat, www.lxcat.net database. The format mimics
the e- + Ar scattering data from the Phelps database.

xxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxx

************************************************************************************************************************

COMMENT:

********************************************************** He **********************************************************

EFFECTIVE
He
 1.360000e-4
SPECIES: e / He
PROCESS: E + He -> E + He, Effective
PARAM.:  m/M = 0.000136, complete set
COMMENT: momentum TRANSFER - FROM CROMPTON ET AL AT LOW ENERGY, HAYASHI AT HIGH ENERGIES(IN SIGLO).
UPDATED: 2011-06-06 11:19:56
COLUMNS: Energy (eV) | Cross section (m2)
-----------------------------
 0.000000e+0	4.960000e-20
 1.000000e-3	4.980000e-20
 1.000000e-2	5.210000e-20
 1.000000e-1	5.860000e-20
 1.000000e+0	6.850000e-20
 1.000000e+1	4.720000e-20
 1.000000e+2	7.500000e-21
 1.000000e+3	1.700000e-21
-----------------------------

EXCITATION
He -> He*(19.8eV)
 1.980000e+1
SPECIES: e / He
PROCESS: E + He -> E + He*(19.8eV), Excitation
PARAM.:  E = 19.8 eV, complete set
COMMENT: FROM 1960'S ANALYSIS OF MEIR-LEIBNITZ AND OTHERS BY PHELPS.
UPDATED: 2010-06-24 08:11:57
COLUMNS: Energy (eV) | Cross section (m2)
-----------------------------
 1.980000e+1	0.000000e+0
 2.002000e+1	4.100000e-22
 1.000000e+2	1.150000e-21
 1.000000e+3	2.500000e-22
-----------------------------

IONIZATION
He -> He^+
 2.460000e+1
SPECIES: e / He
PROCESS: E + He -> E + E + He+, Ionization
PARAM.:  E = 24.6 eV, complete set
COMMENT: RAPP AND ENGLANDER-GOLDEN, 1965.
UPDATED: 2010-03-13 05:04:39
COLUMNS: Energy (eV) | Cross section (m2)
-----------------------------
 2.460000e+1	0.000000e+0
 3.000000e+1	7.100000e-22
 1.000000e+2	3.510000e-21
 1.000000e+3	1.400000e-21
-----------------------------
xxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxx
