hlike_wjdh92#h.dat
Resolved Specific Ion Data Collections
- Ion
- H0+
- Temperature Range
- 8.617 eV → 1723 eV
ADF04
- Filename
- hlike_wjdh92#h.dat
- Full Path
- adf04/hlike/hlike_wjdh92#h.dat
Download data
- Spontaneous Emission: H+0(i) → H+0(j) + hv
- Electron Impact Excitation: H+0(i) + e → H+0(j) + e
- Free Electron Recombination: H+1(i) + e → H+0(j)
| 1s 2S0.5 | 0.0 cm-1 |
| 2s 2S0.5 | 82259.0 cm-1 |
| 2p 2P2.5 | 82259.0 cm-1 |
| 3s 2S0.5 | 97492.0 cm-1 |
| 3p 2P2.5 | 97492.0 cm-1 |
| 3d 2D4.5 | 97492.0 cm-1 |
| 4s 2S0.5 | 102824.0 cm-1 |
| 4p 2P2.5 | 102824.0 cm-1 |
| 4d 2D4.5 | 102824.0 cm-1 |
| 4f 2F6.5 | 102824.0 cm-1 |
| 5s 2S0.5 | 105292.0 cm-1 |
| 5p 2P2.5 | 105292.0 cm-1 |
| 5d 2D4.5 | 105292.0 cm-1 |
| 5f 2F6.5 | 105292.0 cm-1 |
| 5g 2G8.5 | 105292.0 cm-1 |
----------------------------------------------------------------------- This is a composite data set for high temperature use formed from Kingston et al. (1989) HLIKE.DATA(AEK89H) and Callaway et al. (1987) HLIKE.DATA(CALL87H) using a three parameter fit with the first two Bethe coefficients fixed - obtained from Golden, Sampson & Goett S#HDATA.TEXT (nb *2) Preferred data is taken from large scale comparative figures for the transitions from the 1s state. The decisions on the preferred data is rather arbitrary, but makes use of the 1/n**3 scaling rule in circumstances where the original data is dubious. The compilation prepared by Giovanardi et al. (1987) is also shown in these diagrams but does not appear to be of much assistance. For transitions from n = 2 - 3, the extrapolated fits to Callaway are used. For transitions from n = 3,4 - 4,5 the extrapolated fits to Kingston are used. Data for the degenerate transitions due to electrons are taken from Kingston et al. extrapolated as ln(Te) H.P. Summers, Jan. 1991 ----------------------------------------------------------------------- ------------------------------------------------------------------------------- RADIATIVE RECOMBINATION DATA ADDED PROCESSED BY ADASRRC ON :/JETXLE.RADREC.#LIKE(H1LS) 8/2/93 ------------------------------------------------------------------------------- --------------------------------------------------------------------------------- ---------------------------------------------------------------------------------