By Y. Hahn, A. Pradhan, H. Tawara, H.L. Zhang
Interactions of photons and electrons with atoms, molecules, and ions are primary common tactics in a wide selection of impartial or ionized gases in nature or laboratory. the information at the move sections or comparable amounts for these techniques are eagerly wanted in lots of fields of program akin to astrophysics, atmospheric technology, plasma technological know-how, radiation physics and chemistry, and so forth. also they are very important in figuring out actual or chemical homes of atoms, molecules, and their ions. quantity I/17 offers move part information and similar 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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Additional resources 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. 1 Excitation [Ref. p. 64 − 1 Landolt-B¨ ornstein New Series I/17B Ref. p. 92 + 0 Excitation data for iron ions Electron-impact excitation data for iron ions are very important for astrophysical and other plasam modeling applications. 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.
2b gives the effective collision strengths Υ as a function of temperatures T [K]. Table 3. List of the data tables for the iron ions included. 16b Ion Method Ref. 1a. Fe i. Lowest 10 fine-structure energy levels of the states included in the calculation [97P1] and their observed energies E [Ry] in rydbergs [75R1]. 1b for transition keys; J is the total angular momentum for specifying the fine-structure level. 0895 Landolt-B¨ ornstein New Series I/17B Ref. p. 1b. Fe i. 1a [97P1]. 1 Excitation [Ref.
1 Excitation [Ref. p. 34 + 0 ⇓ 3 − − − − − − − λ [˚ A] S0 S0 1 S0 1 S0 3 o P0 3 o P0 3 o P1 1 1 Do5/2 Do3/2 2 o P3/2 2 o P1/2 2 o D5/2 2 o P3/2 2 o P3/2 2 o P3/2 2 o P1/2 2 o P1/2 2 − − − − − − − − − − 4 o S3/2 4 o S3/2 4 o S3/2 4 o S3/2 2 o D3/2 2 o P1/2 2 o D5/2 2 o D3/2 2 o D5/2 2 o D3/2 D2 − 3 P0 D2 − 3 P1 1 D2 − 3 P2 1 S0 − 3 P1 1 S0 − 3 P2 1 S0 − 1 D2 3 P1 − 3 P0 3 P2 − 3 P0 3 P2 − 3 P1 5 o S2 − 3 P1 5 o S2 − 3 P2 1 Landolt-B¨ ornstein New Series I/17B Ref. p. 1 Excitation [Ref. p. 88 − 1 Po1/2 − 2 Po3/2 1 1 Po2 Po1 3 o P0 1 o P1 3 o P1 3 o P2 3 o P2 3 − − − − − − − Po3/2 P1/2 4 P1/2 4 P3/2 4 P3/2 4 P3/2 4 P5/2 4 1 S0 S0 1 S0 1 S0 3 o P0 3 o P0 3 o P1 1 − − − − − − − 2 Po1/2 Po1/2 2 o P3/2 2 o P1/2 2 o P3/2 4 P1/2 2 o P1/2 2 Landolt-B¨ ornstein New Series I/17B Ref.