Silver monohydride


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 October, 1974

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 107AgH
StateTeωeωexeωeyeBeαeγeDeβereTrans.ν00
c0 (3Π0)     [5.10] 1   [0.00060]  [1.820] c0 ← X R 46981.1 Z
missing citation
d 3Σ+     [(3.83)] 2     [(2.100)]  (46875) 3
missing citation
c1 3Π1     [(4.95)] 4   [(0.00060)]  [(1.847)] c1 ← X R (46600) 4
missing citation
D 1Π (46720) [844.7] Z (120)  5.23 5 0.58  0.00060  1.797 D ← X R 46360.9 Z
missing citation
StateTeωeωexeωeyeBeαeγeDeβereTrans.ν00
b (3Δ1) 1     [4.805] 6   [0.00035]  [1.8745] b ← X 7 R 44529.2 Z
missing citation
B 1Σ+ (44512) [1089] 8 (65)  (4.87) 8 (0.31)  (0.00038)  (1.862) B ← X R (44234) 8
missing citation
a 3Πr (41700) 9 (1450) (50)  (>6.3) 9     (<1.64)  
missing citation
C 1Π (41261) (1589) 10 (42) 10  [6.54] (0.31) 10  [0.00049]  [1.607] C ← X 41173.6 Z
missing citation
StateTeωeωexeωeyeBeαeγeDeβereTrans.ν00
A 1Σ+ 29959 [1489.6] Z 87.0 11  [6.0905] 0.3485 11  [0.000389]  [1.6650] A ← X R 29897.94 Z
Bengtsson and Olsson, 1931; missing citation; Gero and Schmid, 1943; Learner, 1962; Loginov, 1964
X 1Σ+ 0 1759.9 Z 34.06 12  6.449 13 0.201 12  [0.000344] 14  [1.6181]  

Notes

1Strong perturbations. Constants valid near J=0 only.
2From perturbations in c1(v=0).
3Estimated energy of v'=0,N'=0 relative to X 1Σ (v=0,N=0).
4The only observed level is strongly perturbed by more than one state. Constants refer to unperturbed region around J=l9. Origin of 0-0 band (not observed) at 46692 cm-1.
5Perturbations in v=0,1; bands going to v'=0 of AgD have not been analyzed. Constants refer to unperturbed regions near J=0. Large Λ-type doubling. AgH: Δνef(v=0) = 0.244J(J+1)-... AgD: Δνef(v=1) = +0.0772J(J+1).
6Constants refer to unperturbed region near J=O. Large Ω-type doubling; AgH: Δνef = 0.156J(J+1)-... AgD: Δνef = 0.0337J(J+1)+ ...
7P branch very weak or absent.
8Approximate constants for the deperturbed state. Origins of the 0-0 bands at 44225.0 cm-1 (AgH) and 44277.4 cm-1 (AgD). v=1 is free of perturbations. AgH; B1=4.4l2, D1=3.5E-4, ν0(1-0)=45322.8 cm-1; AgD; B1=2.343, D1=0.95E-4, ν0(1-0)=45097.8 cm-1.
9Constants estimated from perturbations in C 1Π , B 1Σ+, D 1Π of AgH, and b 1 of AgD; vibrational numbering uncertain. +150 ≤ A ≤ +200.
10Approximate constants for the deperturbed state. Perturbations in v=0,1,2 are caused by a 3Π. AgH: ΔG(1/2)= 1519, ΔG(3/2)= 1453; AgD: ΔG(1/2)= 1056, ΔG(3/2)= 987.
11Anomalous potential curve; see Learner, 1962. Constants for higher vibrational levels of AgH in Bengtsson and Olsson, 1931, Bengtsson-Knave, 1932. The constants for AgD are valid for v ≤ 4.
12Higher order terms are needed to represent levels with v ≥ 4; see Bengtsson and Olsson, 1931, Bengtsson-Knave, 1932, Gero and Schmid, 1943.
13RKRV potential curve Singh and Rai, 1965.
14H0= +88E-10(AgH); H0= +6E-10 (AgD).
15Graphical Birge-Sponer extrapolation of X 1Σ+. Thermochemical value 2.49 eV Farkas, 1929.
16From the value for AgH.
17Constants refer to unperturbed regions near J=0. Small Λ-type doubling.
18R,P much weaker than Q branches.
19Approximate constants for the deperturbed state. v=0 strongly perturbed by more than one state. Origin of 0-0 band (not observed) at 46794 cm-1.

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.

Bengtsson and Olsson, 1931
Bengtsson, E.; Olsson, E., Eine neue untersuchung uber die banden des silberhydrids, Z. Phys., 1931, 72, 163. [all data]

Gero and Schmid, 1943
Gero, L.; Schmid, R., Uber das bandenspektrum des silberhydrids, Z. Phys., 1943, 121, 459. [all data]

Learner, 1962
Learner, R.C.M., The influence of vibration-rotation interaction on intensities in the electronic spectra of diatomic molecules. II. The silver hydride molecule, Proc. R. Soc. London A, 1962, 269, 327. [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]

Bengtsson-Knave, 1932
Bengtsson-Knave, E., Uber die bandenspektren einiger metallhydride, Nova Acta Regiae Soc. Sci. Ups., 1932, 8, 4, 1-98. [all data]

Singh and Rai, 1965
Singh, R.B.; Rai, D.K., On the potential energy curves of AgH, AgCl, and AgI, Can. J. Phys., 1965, 43, 1685. [all data]

Farkas, 1929
Farkas, A., Uber die bildung von gasformigen goldhydrid, Z. Phys. Chem. Abt. B, 1929, 5, 467. [all data]


Notes

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