Germanium monofluoride
- Formula: FGe
- Molecular weight: 91.64
- IUPAC Standard InChIKey: HHFCFXJTAZTLAO-UHFFFAOYSA-N
- CAS Registry Number: 14929-46-5
- Chemical structure:
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Constants of diatomic molecules
Go To: Top, References, Notes
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, 1976
Symbol | Meaning |
---|---|
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) |
State | Te | ωe | ωexe | ωeye | Be | αe | γe | De | βe | re | Trans. | ν00 |
---|---|---|---|---|---|---|---|---|---|---|---|---|
G 2Δr(4dδ) | 49412.89 1 | 710.37 Z | 2.82 H | 0.38408 | 0.00261 | [4.43E-7] 2 | 1.70411 | G → X V | 48523.4 HQ | |||
↳Barrow, Butler, et al., 1959; missing citation | ||||||||||||
G → X V | 49415.6 HQ | |||||||||||
↳Barrow, Butler, et al., 1959; missing citation | ||||||||||||
D 2Σ+(6sσ) | 48581.26 | 833.12 Z 3 | 6.52 H | 0.39972 3 | 0.00214 | [3.73E-7] 4 | 1.6704 | D → A V | 25473.30 Z | |||
↳missing citation | ||||||||||||
D → X V | 47726.6 HQ | |||||||||||
↳missing citation | ||||||||||||
D → X V | 48662.6 HQ | |||||||||||
↳missing citation | ||||||||||||
State | Te | ωe | ωexe | ωeye | Be | αe | γe | De | βe | re | Trans. | ν00 |
D' 2p(4dπ) | 47920.73 5 | 803.96 6 Z | 3.38 H | 0.40068 6 7 | 0.00259 | 3.62E-7 6 | 1.6684 | D' → A V | 24798.98 6 Z | |||
↳missing citation | ||||||||||||
D' → X 8 V | 47043.0 H | |||||||||||
↳missing citation | ||||||||||||
D' → X 8 V | 47976.3 H | |||||||||||
↳missing citation | ||||||||||||
E 2Σ+ (5pσ) | 46645.41 | 760.08 Z | 2.967 | 0.39845 9 | 0.00290 | 4.33E-7 | 1.67310 | E → B 10 | 11616.26 Z | |||
↳missing citation | ||||||||||||
State | Te | ωe | ωexe | ωeye | Be | αe | γe | De | βe | re | Trans. | ν00 |
C 2Δ | 43977.49 11 | [684.00] Z | 9.31 | 0.38835 | 0.00421 | [4.97E-7] 12 | 1.69472 | C → X V | 43059.27 13 Z | |||
↳Barrow, Butler, et al., 1959; Uzikov and Kuzyakov, 1969; missing citation | ||||||||||||
C → X V | 43994.43 13 Z | |||||||||||
↳Barrow, Butler, et al., 1959; Uzikov and Kuzyakov, 1969; missing citation | ||||||||||||
C' 2Π (5pπ) | 43369.61 14 | 796.88 Z | 3.415 | 0.39957 15 | 0.00258 | 4.13E-7 | 1.67075 | C' → A 16 R | 20244.31 | |||
↳Martin and Merer, 1974 | ||||||||||||
C' → X 17 V | 42547.8 H | |||||||||||
↳Uzikov and Kuzyakov, 1969; missing citation | ||||||||||||
C' → X 17 V | 43379.9 H | |||||||||||
↳Uzikov and Kuzyakov, 1969; missing citation | ||||||||||||
State | Te | ωe | ωexe | ωeye | Be | αe | γe | De | βe | re | Trans. | ν00 |
a 4Σ- | 35194.68 18 | [628.31] Z | 6.66 19 | 0.36676 18 | 0.00369 | [4.94E-7] 20 | 1.7439 | a → X | 35181.77 Z | |||
↳missing citation | ||||||||||||
B 2Σ+(5sσ) | 35010.85 | 796.99 Z | 3.613 21 | 0.0124 | 0.39440 22 | 0.00255 | 3.88E-7 | 1.68167 | B → A V | 11885.56 Z | ||
↳Barrow, Butler, et al., 1959 | ||||||||||||
B → X 23 V | 34141.23 Z | |||||||||||
↳missing citation; missing citation | ||||||||||||
B → X 23 V | 35076.39 Z | |||||||||||
↳missing citation; missing citation | ||||||||||||
State | Te | ωe | ωexe | ωeye | Be | αe | γe | De | βe | re | Trans. | ν00 |
A 2Σ+ | 23316.65 | 413.03 Z | 1.124 24 | 0.32039 25 | 0.00307 26 | 7.78E-7 27 | 1.86582 | A → X 23 R | 22255.67 Z | |||
413.03 Z | 1.124 24 | 0.32039 25 | 0.00307 26 | 7.78E-7 27 | 1.86582 | 23190.83 Z | ||||||
X 2Π3/2 | 934.33 | 667.33 Z | 3.150 28 | 0.36660 | 0.002675 29 | 4.50 | 1.7452 | |||||
X 2Π1/2 | 0 | 665.67 Z | 3.150 28 | 0.36578 30 | 0.002675 29 | 4.47 | 1.7452 |
Notes
1 | A0 = +22.20, A1 = +21.5: small J dependence. |
2 | D1 = 4.52E-7. |
3 | Rotational analysis of v=2, and tentative results for v=0. |
4 | D2 = 3.33E-7. |
5 | A2 = (+)4.23, A3 = (+)4.35. |
6 | Extrapolation from the rotationally analyzed levels v'=2 and 3; βe = +0.21E-7. |
7 | Large Λ-type doubling, also spin-rotation interaction; see Martin and Merer, 1974. |
8 | The 0-1 and 0-2 bands were previously considered by Barrow, Butler, et al., 1959 as 0-0 bands of their transitions F-X and E-X, respectively. |
9 | Spin-doubling constant γ(v=0) = -0.0358. |
10 | Δv=0 sequence of slightly V shaded bands, provisionally assigned in Barrow, Butler, et al., 1959 to a E(2Π)- B(2Σ) transition. |
11 | A0 = 13.88, A1 = 14.25. |
12 | D1 = 5.15E-7 |
13 | Referring in the upper state to the zero point of the Hill-Van Vleck expression. |
14 | A0 = 105.63, A1 = 105.88, A2 = 105.96; small J dependence. |
15 | Λ-type doubling in 2Π1/2, Δvfe(v=0)=-0.0373(J+1/2). |
16 | Extremely weak system consisting of a long 0-v" progression; not analyzed. |
17 | The 3-1 and 1-0 bands of C' 2Π1/2 - X 2Π1/2 correspond to the 0-0 subbands of a system D-X proposed earlier by Barrow, Butler, et al., 1959. The 2-1 band of the 3/2- 3/2 system was assigned by Barrow, Butler, et al., 1959 as 0-0 band of C'-X2Π1/2. |
18 | Spin-splitting constants for v=0: λ = +8.086, v=0 [4λ = T0(4Σ3/2) - T0(4Σ1/2), v=0]; γ1 ~ γ2 = 0.0119, v=0. See also 22. |
19 | Based on the interpretation of a perturbation in B 2Σ+, v=4. |
20 | D1 = 4.90E-7. |
21 | missing note |
22 | Spin=doubling constant γ(v=0) = +0.00100. Extensive perturbations between B 2Σ+, v=0, and, a 4Σ-, v=0. |
23 | Franck-Condon factors Singh, 1975. |
24 | missing note |
25 | Spin-doubling constant γ(v) = -[0.03662 + 0.000l4(v+1/2)]. |
26 | missing note |
27 | Dv= -0.22E-7(v+1/2) +... |
28 | missing note |
29 | missing note |
30 | Λ-type doubling, Δvfe = -[0.02184 + 0.000195 (v+1/2)](J+1/2). |
31 | Thermochemical value (mass-spectrom.) Ehlert and Margrave, 1964; see also Harland, Cradock, et al., 1973. |
32 | Approximate limit of the ns (n = 5, 6, ...) Rydberg series Martin and Merer, 1974. Harland, Cradock, et al., 1973 give 7.2 eV from electron impact mass spectrometry. |
References
Go To: Top, Constants of diatomic molecules, Notes
Data compilation copyright by the U.S. Secretary of Commerce on behalf of the U.S.A. All rights reserved.
Barrow, Butler, et al., 1959
Barrow, R.F.; Butler, D.; Johns, J.W.C.; Powell, J.L.,
Some observations on the spectra of the diatomic fluorides of silicon, germanium, tin, and lead,
Proc. Phys. Soc. London, 1959, 73, 317. [all data]
Uzikov and Kuzyakov, 1969
Uzikov, A.N.; Kuzyakov, Yu.Ya.,
Analysis of the vibrational structure of C-X2P and C'X2P-band systems and the energy of dissociation of GeF,
Moscow Univ. Chem. Bull. Engl. Transl., 1969, 24, 22, In original 30. [all data]
Martin and Merer, 1974
Martin, R.W.; Merer, A.J.,
Rotational structure in some higher excited states of the GeF molecule,
Can. J. Phys., 1974, 52, 1458. [all data]
Singh, 1975
Singh, J.,
Vibrational transition probabilities & r-centroids for diatomic fluorides of Si & Ge,
Indian J. Pure Appl. Phys., 1975, 13, 204. [all data]
Ehlert and Margrave, 1964
Ehlert, T.C.; Margrave, J.L.,
Mass-spectrometric studies at high temperatures. II. The dissociation energies of the monofluorides and difluorides of silicon and germanium,
J. Chem. Phys., 1964, 41, 1066. [all data]
Harland, Cradock, et al., 1973
Harland, P.W.; Cradock, S.; Thynne, J.C.J.,
Bond dissociation energies, ionisation potentials and electron affinities of some germanium fluoride species,
Inorg. Nucl. Chem. Lett., 1973, 9, 53. [all data]
Notes
Go To: Top, Constants of diatomic molecules, References
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