processes

Home
How to use
Contributors
Data center
Online calculations
- BOLSIG+
Docs and links
Discussion board
Newsletter

data type » databases » first species » second species » data groups » processes » output

Step 6: Select processes & click next

« PREV

NEXT »

select all

select none

SELECT ALL & FILTER TOOL

Puech database

PERMLINK: www.lxcat.net/Puech

DESCRIPTION: Cross section sets assembled by V Puech and colleagues in late 1980's and 1990's. Ne : updated and corrected on Dec 11 2012

CONTACT: Vincent Puech, LPGP, Orsay, France

SCATTERING CROSS SECTIONS

Species: e + Ar [42], C2H4 [8], C3H6 [6], Ne [26], Xe [15]

Updates: 2011-07-22 … 2018-02-20

Downloads: 5542 times from 2012-09-05

select all

select none

expand or collapse

Data Group [Ar]: V Puech and L Torchin, "Collision cross sections and electron swarm parameters in argon", J. Phys. D: Appl. Phys. 19 2309 (1986). Elasic momentum transfer cross section corrected on 27 Nov 2012.

select all

select none

e / Ar

Elastic E + Ar → E + Ar (m/M = 0.0000136, complete set) | elastic MOMENTUM-TRANSFER CROSS SECTION. Updated: 27 November 2012.
Excitation E + Ar → E + Ar(1s5: 4s(3/2)2) (E = 11.548 eV, complete set) | Updated: 14 November 2012.
Excitation E + Ar → E + Ar(1s4: 4s(3/2)1) (E = 11.623 eV, complete set) | Updated: 27 November 2012.
Excitation E + Ar → E + Ar(1s3: 4s'(1/2)0) (E = 11.723 eV, complete set) | Updated: 14 November 2012.
Excitation E + Ar → E + Ar(1s2: 4s'(1/2)1) (E = 11.827 eV, complete set) | Updated: 14 November 2012.
Excitation E + Ar → E + Ar(2p10: 4p(1/2)1) (E = 12.906 eV, complete set) | Updated: 14 November 2012.
Excitation E + Ar → E + Ar(2p9: 4p(5/2)3) (E = 13.075 eV, complete set) | Updated: 14 November 2012.
Excitation E + Ar → E + Ar(2p8: 4p(5/2)2) (E = 13.094 eV, complete set) | Updated: 14 November 2012.
Excitation E + Ar → E + Ar(2p7: 4p(3/2)1) (E = 13.152 eV, complete set) | Updated: 14 November 2012.
Excitation E + Ar → E + Ar(2p6: 4p(3/2)2) (E = 13.171 eV, complete set) | Updated: 14 November 2012.
Excitation E + Ar → E + Ar(2p5: 4p(1/2)0) (E = 13.272 eV, complete set) | Updated: 14 November 2012.
Excitation E + Ar → E + Ar(2p4: 4p'(3/2)1) (E = 13.282 eV, complete set) | Updated: 14 November 2012.
Excitation E + Ar → E + Ar(2p3: 4p'(3/2)2) (E = 13.302 eV, complete set) | Notation corrected, 4p'(1/2)1 => 4p'(3/2)2: 20 feb 2018. Updated: 20 February 2018.
Excitation E + Ar → E + Ar(2p2: 4p'(1/2)1) (E = 13.327 eV, complete set) | Updated: 14 November 2012.
Excitation E + Ar → E + Ar(2p1: 4p'(1/2)0) (E = 13.479 eV, complete set) | Updated: 14 November 2012.
Excitation E + Ar → E + Ar(3d6: 3d(1/2)0) (E = 13.844 eV, complete set) | Updated: 14 November 2012.
Excitation E + Ar → E + Ar(3d5: 3d(1/2)1) (E = 13.863 eV, complete set) | Updated: 14 November 2012.
Excitation E + Ar → E + Ar(3d3: 3d(3/2)2) (E = 13.903 eV, complete set) | Updated: 14 November 2012.
Excitation E + Ar → E + Ar(3d4': 3d(7/2)4) (E = 13.979 eV, complete set) | Updated: 14 November 2012.
Excitation E + Ar → E + Ar(3d4: 3d(7/2)3) (E = 14.02 eV, complete set) | Updated: 14 November 2012.
Excitation E + Ar → E + Ar(3d1: 3d(5/2)2 and 5s(3/2)2) (E = 14.065 eV, complete set) | Updated: 14 November 2012.
Excitation E + Ar → E + Ar(2s4: 5s(3/2)1) (E = 14.09 eV, complete set) | Updated: 14 November 2012.
Excitation E + Ar → E + Ar(3d2: 3d(3/2)1) (E = 14.152 eV, complete set) | Updated: 14 November 2012.
Excitation E + Ar → E + Ar(3s1: 3d'(5/2)2) (E = 14.213 eV, complete set) | Updated: 14 November 2012.
Excitation E + Ar → E + Ar(3s1: 3d'(3/2)2 and 3d'(5/2)3 (E = 14.236 eV, complete set) | Updated: 14 November 2012.
Excitation E + Ar → E + Ar(2s2: 5s'(1/2)1) (E = 14.254 eV, complete set) | Updated: 14 November 2012.
Excitation E + Ar → E + Ar(3s1: 3d'(3/2)1) (E = 14.303 eV, complete set) | Updated: 14 November 2012.
Excitation E + Ar → E + Ar(3p10) (E = 14.461 eV, complete set) | Updated: 14 November 2012.
Excitation E + Ar → E + Ar(3p9) (E = 14.496 eV, complete set) | Updated: 14 November 2012.
Excitation E + Ar → E + Ar(1s3:3p8) (E = 14.503 eV, complete set) | Updated: 14 November 2012.
Excitation E + Ar → E + Ar(:3p7) (E = 14.522 eV, complete set) | Updated: 14 November 2012.
Excitation E + Ar → E + Ar(1s3:3p6) (E = 14.526 eV, complete set) | Updated: 14 November 2012.
Excitation E + Ar → E + Ar(:3p5) (E = 14.573 eV, complete set) | Updated: 14 November 2012.
Excitation E + Ar → E + Ar(:3p4) (E = 14.678 eV, complete set) | Updated: 14 November 2012.
Excitation E + Ar → E + Ar(: 3p2) (E = 14.684 eV, complete set) | Updated: 14 November 2012.
Excitation E + Ar → E + Ar(:3p3) (E = 14.686 eV, complete set) | Updated: 14 November 2012.
Excitation E + Ar → E + Ar(:3p1) (E = 14.735 eV, complete set) | Updated: 14 November 2012.
Excitation E + Ar → E + Ar(: 4d(1/2)1 and 6S(3/2)1 and 4 (E = 14.805 eV, complete set) | Updated: 14 November 2012.
Excitation E + Ar → E + Ar(:4d'(3/2)1 and 6s'(1/2)1 and (E = 15.103 eV, complete set) | Updated: 14 November 2012.
Excitation E + Ar → E + Ar(:6d(1/2)1 and 5d'(3/2)1 and 7 (E = 15.346 eV, complete set) | Updated: 14 November 2012.
Excitation E + Ar → E + Ar(:7d(1/2)1 and ...) (E = 15.66 eV, complete set) | Updated: 14 November 2012.
Ionization E + Ar → E + E + +ionized Ar (E = 15.8 eV, complete set) | Updated: 27 November 2012.

Copyright © 2009-2024, the LXCat team. The use without proper referencing to databases and software used is prohibited. All Rights Reserved. You currently use FR | NL | US mirror site.