HPt


Constants of diatomic molecules

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Data compilation copyright by the U.S. Secretary of Commerce on behalf of the U.S.A. All rights reserved.

Data compiled by: Klaus P. Huber and Gerhard H. Herzberg

Data collected through May, 1975

Symbols used in the table of constants
SymbolMeaning
State electronic state and / or symmetry symbol
Te minimum electronic energy (cm-1)
ωe vibrational constant – first term (cm-1)
ωexe vibrational constant – second term (cm-1)
ωeye vibrational constant – third term (cm-1)
Be rotational constant in equilibrium position (cm-1)
αe rotational constant – first term (cm-1)
γe rotation-vibration interaction constant (cm-1)
De centrifugal distortion constant (cm-1)
βe rotational constant – first term, centrifugal force (cm-1)
re internuclear distance (Å)
Trans. observed transition(s) corresponding to electronic state
ν00 position of 0-0 band (units noted in table)
Diatomic constants for (195)PtH
StateTeωeωexeωeyeBeαeγeDeβereTrans.ν00
IV (2Σ) 2  [2051] H   8.03 0.40  [4.4E-4] 1  1.447 IV ← III R 36504 H
Scullman, 1971
III (2Σ) 2     [9.51]   [3.7E-4]  [1.330]  
II (2Σ) 2     [5.22]   [4.1E-4]  [1.795] II ← I R 30311 H
Scullman, 1971
I (2Σ) 2     [7.13]   [2.8E-4]  [1.536]  
B (2Δ)5/2 (26962) [1548.18] 3 Z (80) 4  6.003 5 6 0.301  [3.15E-4] 7  1.6736 B ↔ X1 R 26613.91 3 Z
Loginov, 1964; missing citation; Loginov, 1966; Kaving and Scullman, 1971
StateTeωeωexeωeyeBeαeγeDeβereTrans.ν00
B' (2Φ)7/2 (24218) [1428.7] 3 Z (74)  5.758 0.326 8  [3.6E-4] 9  1.7088 B' → X1 R 23806.48 3 Z
missing citation
A (2Δ)5/2 (22311) 1690.6 3 Z 55.3 10 -3.88 [5.534] 11 12  [3.55E-4] 13  [1.7430] A ↔ X1 R 21960.59 3 Z
Loginov, 1964; Neuhaus and Scullman, 1964; missing citation; Kaving and Scullman, 1971
A' (2Δ)3/2 (x2 + 19938) [1500.08] 3 Z (58)  6.1103 14 0.2869  [4.717E-4] 15  1.65879 A' ↔ X2 R 19610.82 3 Z
missing citation
X2 (2Δ)3/2 x2 16 [2177.31] 3 Z (43)  7.2784 14 0.2029  [2.834E-4] 17  1.51987  
StateTeωeωexeωeyeBeαeγeDeβereTrans.ν00
X1 (2Δ)5/2 0 18 [2294.68] 3 Z (46)  7.1963 0.1996  [2.613E-4] 19  1.52852  

Notes

1D1 = 4.9E-4.
2Preliminary data only.
3Band origins in the tables for PtH and PtD correspond to the energy of J'=0 relative to J"=0. Vibrational constants recalculated accordingly.
4From the corresponding value for PtD.
5Perturbations in both v=0 and v=1.
6Predissociation above v=0, J=12.5, see Kaving and Scullman, 1971.
7D1 = 3.94E-4.
8Perturbation in v=1 at J~6.5, see Scullman, 1971.
9D1 = 3.5E-4.
10(v=0, ..., 3).
11Ω-type doubling; for details see Scullman, 1965, Kaving and Scullman, 1971, Kaving and Scullman, 1974.
12B1= 5.244, B2= 4.924, B3= 4.517 (v=3 perturbed for J ≥ 10.5).
13D1(E-4 cm-1)= 3.68, D2(E-4 cm-1)= 4.42, D3(E-4 cm-1)= 8.8.
14Ω-type doubling; see Kaving and Scullman, 1971.
15D1 = 6.08E-4.
16x2 ~1320; see Kaving and Scullman, 1971.
17D1 = 2.84E-4
18Not certain that this is the ground state.
19D1 = 2.607E-4.
20From the predissociation in v=0 of B (2Δ)5/2, assuming that X1 is the ground state.

References

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Data compilation copyright by the U.S. Secretary of Commerce on behalf of the U.S.A. All rights reserved.

Scullman, 1971
Scullman, Dissertation, see USIP Report 71-02, Stockholm, 1971, 1. [all data]

Loginov, 1964
Loginov, V.A., The production of electronic band spectra by the exploding wire method, Opt. Spectrosc. Engl. Transl., 1964, 16, 220, In original 402. [all data]

Loginov, 1966
Loginov, V.A., Absorption spectra of PtH and PtD, Opt. Spectrosc. Engl. Transl., 1966, 20, 88, In original 167. [all data]

Kaving and Scullman, 1971
Kaving, B.; Scullman, R., Two new subsystems of PtH in the region 3500-5800 Å, Can. J. Phys., 1971, 49, 2264. [all data]

Neuhaus and Scullman, 1964
Neuhaus, H.; Scullman, R., Das Bandenspektrum des PtH und PtD, Z. Naturforsch. A, 1964, 19, 659. [all data]

Scullman, 1965
Scullman, R., Rotational analysis of violet and green bands of PtH, Ark. Fys., 1965, 28, 255. [all data]

Kaving and Scullman, 1974
Kaving, B.; Scullman, R., Rotational analysis of the A2Δ5/2-X2Δ5/2 and B2Δ5/2 - X2Δ5/2 band sub-system of PtD, Phys. Scr., 1974, 9, 33. [all data]


Notes

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