By Y. Hahn, A. Pradhan, H. Tawara, H.L. Zhang
Interactions of photons and electrons with atoms, molecules, and ions are primary straight forward strategies in a large choice of impartial or ionized gases in nature or laboratory. the knowledge at the go sections or comparable amounts for these tactics are eagerly wanted in lots of fields of program similar to astrophysics, atmospheric technological know-how, plasma technology, radiation physics and chemistry, and so forth. also they are vital in realizing actual or chemical houses of atoms, molecules, and their ions. quantity I/17 offers go part information and comparable quantitative info at the collisions of photons with atoms, electrons with atoms, and electrons with atomic ions.
Read Online or Download Collisions of Electrons with Atomic Ions (Landolt-Börnstein: Numerical Data and Functional Relationships in Science and Technology - New Series Elementary Particles, Nuclei and Atoms) PDF
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Collisions of Electrons with Atomic Ions (Landolt-Börnstein: Numerical Data and Functional Relationships in Science and Technology - New Series Elementary Particles, Nuclei and Atoms)
Interactions of photons and electrons with atoms, molecules, and ions are primary undemanding tactics in a large choice of impartial or ionized gases in nature or laboratory. the knowledge at the pass sections or similar amounts for these methods are eagerly wanted in lots of fields of software comparable to astrophysics, atmospheric technological know-how, plasma technology, radiation physics and chemistry, and so on.
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Additional info for Collisions of Electrons with Atomic Ions (Landolt-Börnstein: Numerical Data and Functional Relationships in Science and Technology - New Series Elementary Particles, Nuclei and Atoms)
P. 3–96 Table 1 (continued) Ion Ref. Author Method Transitions Data Rating B iii C iv C iv, O vi 97M1 92B4 Marchalant Burke CCC RM 2s − 2p, 3 , 4 2s − 2p, 3 Q Ω C A 91B1 Fe xxiv 90Z3 Fe xxiv 93F1 Fe xxiv 97B3 Xe lii 93F1 U xc 93F1 Li-like, 6 < Z < 42 95S1 Li-like, 6 < Z < 42 96S1 Badnell Zhang Fontes Berrington Fontes Fontes DW/RM RDW RDW BPRM RDW RDW 2s − 2p mag. levels n=1−2 n = 2,3,4 n=1−2 n=1−2 Q Ω Ω Ω,Υ Ω Ω A,B C C A B A Safronova CB ∆n = 1 Q,q C,D Safronova CB 1s2 2s − 1s2s2p, 1s2s2 , 1s2p2 Q,q C,D Zhang RDW n = 2 − 3, 4, 5 Ω,f C Zhang RDW 2s − 2pj Ω,f C Zhang RDW n = 2 − 3, 4, 5 Ω,f B Zhang RDW 2s − 2pj Ω,f B Zhang RDW n = 2 − 3, 4, 5 Ω,f A Zhang RDW 2s − 2pj Ω,f A Li-like, 8 ≤ Z ≤ 30 90Z1 Li-like, 8 ≤ Z ≤ 40 90Z1 Li-like, 31 ≤ Z ≤ 50 90Z1 Li-like, 41 ≤ Z ≤ 60 90Z1 Li-like, 51 ≤ Z ≤ 92 90Z1 Li-like, 61 ≤ Z ≤ 92 90Z1 N =4 Be-like 94B4 Berrington B ii 92B1 Berrington B ii 96C2 Clark C iii 92K1 Keenan N iv 94R1 Ramsbottam Ov 90K1 Kato O v, Si xi, Fe xxiii, Mo xxxix 90S1 Safronova O v, Si xi, Fe xxiii, Mo xxxix 91K1 Kato O v, Si xi, Fe xxiii, Mo xxxix 92S1 Safronova Ne vii 94R2 Ramsbottam Ne vii 95R1 Ramsbottam Fe xxiii 93K1 Keenan Fe xxiii 98C2 Chen Mo xxxix 94C3 Chen Xe li 93Z1 Zhang U lxxxix 94F3 Fontes (Be-like) review fits DW fits RM RM review many n=1−3 many 2s2 − 2s2p 3 PJ 2s2 , 2s2p, 2s3 , 2p2 n = 2, 3 Ω,Υ Ω,Υ Q Υ Υ q A-C A,B C A A A,B CBR 2s2 , 2s2p, 2p2 Ω C,D CBR 2s2 , 2s2p, 2p2 Ω,q C,D CBR RM RM RM RDW RM RDW RDW 2s2 , 2s2p, 2p2 2s2 , 2s2p, 2s3 , 2p2 n = 2,3 2s2 , 2s2p, 2p2 n = 2, 3 1s2 2s2 − 1s2s2 2p 2s2 , 2s2p, 2p2 n=2−2 Q,q Υ Υ Υ Q Q Ω Ω C,D A A A C B B A Landolt-B¨ ornstein New Series I/17B Ref.
The Iron Project (IP) [93H1] is mostly devoted to calculating reliable collisional data for all iron ions using the most accurate method, the Breit-Pauli R-matrix closecoupling method, with relativistic fine structure effects. The effective, or maxwellian-averaged, collision strengths tabulated in this section are mostly taken from the collective efforts by the IP. Because this is an on-going endeavor, data for some iron ions by the IP are currently not available. For some of these ions data calculated by the RDW method are also tabulated.
The “–” indicate that the data is not available for those transitions. The order of transitions in Table 2 with respect to the upper and lower levels is mixed, and the initial levels under the column ’Transition’ is not usually the lower one. Therefore care must be exercised in using Eq. (7) or (8) to determine the lower and the upper levels Ei or Ej . 26708). Table 2. Effective collision strengths and A-values. 1 Excitation [Ref. p. 3–96 Table 1 (continued) Ion Ref. 2 95S3 Schoning Data Rating (Rb-like) 4s − 5f, 5s − 4f CDW N = 51 Xe iv Transitions Ω B Ω,Υ C (Sb-like) CC 5s2 5p3 ; J-levels Effective collision strengths, wavelengths, and A-values At electron temperatures around 10000 K the elements in a plasma source are in low ionization stages and low levels of excitation.