Iodosilylidyne


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 September, 1977

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 28Si127I
StateTeωeωexeωeyeBeαeγeDeβereTrans.ν00
Unassigned bands in the region 41500 - 43600 cm-1.
Olddershaw and Robinson, 1972
F           F ← X1 V 44995 H
missing citation
(E) 1           (E ← X) (44104)
missing citation
D           D ← X1 V 42859 H
missing citation
StateTeωeωexeωeyeBeαeγeDeβereTrans.ν00
C 42711 486 H 3.5        C ← X1 V 42772 H
missing citation
B 2Σ 32380.3 471.7 H 0.9        B ← X1 V 32434.3 H
Oldershaw and Robinson, 1968; missing citation
A 2Σ 21204.9 208.6 H 1.66 2 0.079 3      A ← X1 R 21127.2 H
missing citation
a (4Σ1/2-) x + 20289.7 275.7 H 5.6  [(0.118)] 4     [(2.50)] a ↔ X2 5 R 20246.9 H
missing citation; missing citation
StateTeωeωexeωeyeBeαeγeDeβereTrans.ν00
X2 2Π3/2 x 6 359.0 H 1.1         
X1 2Π1/2 0 363.8 H [(1.25)] 7       [(2.45)]  

Notes

1Diffuse bands, assignment uncertain.
2ωeze = -0.0055.
3Only the 7-0 and 8-0 bands of A ← X1 have been analyzed Billingsley, 1972, B' ~ 0.085 Billingsley, 1972. Of the six expected branches only four have been observed; R11 and Q P 21 (i.e. Ree and Pff) lines are absent. Extensive perturbations by levels of a 4Σ1/2- state; see 4.
4As a full rotational analysis of the emission bands [called A' → X by Billingsley, 1972 and A → X by Lakshminarayana and Haranath, 1970] was not possible, the nature of the a state is not known. Billingsley, 1972 suggests that this is the same 4Σ1/2- state whose higher vibrational levels (ΔG ~ 176, B ~ 0.097) have been identified in perturbations of A 2Σ(v=7,8).
5A much weaker system reported by Lakshminarayana and Haranath, 1970 at 650 cm-1 to the red of the main system was not confirmed by Billingsley, 1972. Transitions to or from X1 2Π1/2 have not been observed.
6 Billingsley, 1972 assumes x ~ 700 cm-1 Billingsley, 1972. Tentative assignments of weak absorption bands would give x=649 cm-1 Billingsley, 1972 or x=757 cm-1 Oldershaw and Robinson, 1968.
7Estimated by assuming the same percentage decrease in bond length from HSiI to SiI as from HSiCl to SiCl Billingsley, 1972. The rotational analysis of the A ← X1 7-0 and 8-0 bands gives B"- |p"|/2 = 0.10987 and D"= 2.1E-7.
8Extrapolation of the vibrational levels in A2Σ Billingsley, 1972. An upper limit of 4.02 eV follows from the predissociation in B 2Σ.
9The bands become progressively more diffuse with increasing v' Billingsley, 1972.

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.

Olddershaw and Robinson, 1972
Olddershaw, G.A.; Robinson, K., Ultraviolet spectra of GeI and SiI: lower wavelength bands, J. Mol. Spectrosc., 1972, 44, 602. [all data]

Oldershaw and Robinson, 1968
Oldershaw, G.A.; Robinson, K., Ultra-violet absorption spectra of GeI and SiI, Trans. Faraday Soc., 1968, 64, 2256. [all data]

Billingsley, 1972
Billingsley, J., The absorption and emission spectrum of silicon monoiodide, J. Mol. Spectrosc., 1972, 43, 3, 128-147. [all data]

Lakshminarayana and Haranath, 1970
Lakshminarayana, A.; Haranath, P.B.V., The emission band spectrum of silicon monoiodide, J. Phys. B:, 1970, 3, 4, 576-579. [all data]


Notes

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