HSr


Reaction thermochemistry data

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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: John E. Bartmess

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Individual Reactions

Sr- + Hydrogen cation = HSr

By formula: Sr- + H+ = HSr

Quantity Value Units Method Reference Comment
Δr350.46 ± 0.88kcal/molD-EAAndersen, Petrunin, et al., 1997gas phase

Gas phase ion energetics data

Go To: Top, Reaction thermochemistry data, Constants of diatomic molecules, 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: John E. Bartmess

De-protonation reactions

Sr- + Hydrogen cation = HSr

By formula: Sr- + H+ = HSr

Quantity Value Units Method Reference Comment
Δr350.46 ± 0.88kcal/molD-EAAndersen, Petrunin, et al., 1997gas phase

Constants of diatomic molecules

Go To: Top, Reaction thermochemistry data, Gas phase ion energetics data, 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, 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 (88)SrH
StateTeωeωexeωeyeBeαeγeDeβereTrans.ν00
Fragments of several additional absorption systems above 30000 cm-1; tentative rotational analyses.
missing citation; Khan and Butt, 1968; missing citation; missing citation
F 2Σ+ 34096 [1337.0] Z (33) 1  [4.0020] 2 0.092  [13.84E-5]  [2.0561] F ← X V 34189.97 Z
missing citation; Khan, 1963; Khan, 1966; Khan and Butt, 1968
C 2Σ+ 26230 1347 H 23.5  4.008 3 0.132  14E-5  2.055 C ↔ X V 26298.7 Z
Frederickson, Hogan, et al., 1935; Humphreys and Fredrickson, 1936; More and Cornell, 1938; missing citation
D 2Σ+ 20847.6 1014.1 Z 15.4  1.925 4 0.024  3E-5  2.965 D ↔ X 5 R 20752.0 Z
Watson, Fredrickson, et al., 1936; More and Cornell, 1938
StateTeωeωexeωeyeBeαeγeDeβereTrans.ν00
E 2Π     [3.869] 6   [20E-5]  [2.091] E → X V 18960 Z
Frederickson, Hogan, et al., 1935
     [3.639] 6   [10E-5]  [2.156] E → X V 18860 Z
Frederickson, Hogan, et al., 1935
B 2Σ+ 14340 [1193.0] Z (19) 1  3.8788 7 0.0930  17.3E-5  2.0885 B → X V 14352.1 Z
missing citation; Watson, Fredrickson, et al., 1936
A 2Πr 8    [3.679] 9   [11.3E-5]  [2.144] A → X V 13653 Z
missing citation
8    [3.668] 9   [13.3E-5]  [2.148] A → X V 13360 Z
missing citation
StateTeωeωexeωeyeBeαeγeDeβereTrans.ν00
X 2Σ+ 0 1206.2 Z 17.0  3.6751 10 0.0814  [13.5E-5] 11  2.1456 12  
Knight and Weltner, 1971

Notes

1From isotope relations.
2Spin doubling constant γ0 = +0.076. All lines are diffuse owing to predissociation.
3Breaking-off in emission at low pressure above N'=19 and 4 in v'=0 and 1, respectively Khan, 1963, 2. Perturbations.
4Strong perturbations.
5Franck-Condon factors Singh and Srivastava, 1968.
6Perturbations.
7Spin doubling constant γ0 = -3.81 N < 10 Watson, Fredrickson, et al., 1936. For a more elaborate evaluation of the spin splitting including higher-order correction terms see Veseth, 1971.
8A0 ~ +300. See also 9.
9Very large Λ-type doubling, see Watson and Fredrickson, 1932, Veseth, 1971, 2. The constants given here are effective values; see, however, Veseth, 1971, 3 who has evaluated the true constants by taking into account several usually neglected corrections to the rotational energy formulae for a 2Π state.
10From Watson, Fredrickson, et al., 1936; spin doubling constant γ0 = 0.122 Watson, Fredrickson, et al., 1936. Edvinsson, Kopp, et al., 1963 give B0 = 3.6336, D0 = 13.39E-5.
11D1 = 12.9E-5.
12ESR sp. 14
13From the predissociation in C 2Σ+ assuming dissociation into 3P0 + 2S.
14In argon matrix at 4 K.
15Spin doubling constant γ0 = +0.0357.
16From the value for SrH.
17Breaking-off above N'=29 and 19 in v'=0 and 1, respectively Khan, 1963, 2. Strong perturbations.
18Spin doubling constant γ0 = -2.01 N < 10 Watson, Fredrickson, et al., 1936. See 7.
19D1 = 3.81E-5.
20Spin doubling constant γ0 = +0.0613.
21D1 = 3.64E-5.

References

Go To: Top, Reaction thermochemistry data, Gas phase ion energetics data, 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.

Andersen, Petrunin, et al., 1997
Andersen, H.H.; Petrunin, V.V.; Kristensen, P.; Andersen, T., Structural properties of the negative strontium ion: Binding energy and fine-structure splitting, Phys. Rev. A, 1997, 55, 4, 3247-3249, https://doi.org/10.1103/PhysRevA.55.3247 . [all data]

Khan and Butt, 1968
Khan, M.A.; Butt, M.R., A study of some new absorption bands of SrH and SrD in the ultra-violet region, J. Phys. B:, 1968, 1, 745. [all data]

Khan, 1963
Khan, M.A., SrH and SrD bands at 2927 Å and 2928 Å, Proc. Phys. Soc. London, 1963, 81, 1047. [all data]

Khan, 1966
Khan, M.A., Rotational analysis of some new absorption bands of SrH and SrD in the ultra-violet region, Proc. Phys. Soc. London, 1966, 89, 165. [all data]

Frederickson, Hogan, et al., 1935
Frederickson, W.R.; Hogan, M.E., Jr.; Watson, W.W., The spectra of strontium hydride, Phys. Rev., 1935, 48, 602. [all data]

Humphreys and Fredrickson, 1936
Humphreys, R.F.; Fredrickson, W.R., The pressure effect on the C band of strontium hydride, Phys. Rev., 1936, 50, 542. [all data]

More and Cornell, 1938
More, K.R.; Cornell, S.D., The band spectra of SrCl and SrH, Phys. Rev., 1938, 53, 806. [all data]

Watson, Fredrickson, et al., 1936
Watson, W.W.; Fredrickson, W.R.; Hogan, M.E., Jr., Strontium deuteride and hydride spectra, Phys. Rev., 1936, 49, 150. [all data]

Knight and Weltner, 1971
Knight, L.B., Jr.; Weltner, W., Jr., Hyperfine interaction and chemical bonding in MgH, CaH, SrH, and BaH molecules, J. Chem. Phys., 1971, 54, 3875. [all data]

Khan, 1963, 2
Khan, M.A., Extension of the C2Σ → X2Σ system of SrD, Proc. Phys. Soc. London, 1963, 82, 564. [all data]

Singh and Srivastava, 1968
Singh, P.D.; Srivastava, Y.P., Franck-Condon factors and r-centroids for some bands of the SrH, J. Quant. Spectrosc. Radiat. Transfer, 1968, 8, 1443. [all data]

Veseth, 1971
Veseth, L., An investigation of the interaction between close-lying 2Σ and 2Π states of diatomic molecules. I. Spin-splitting of the 2Σ levels, Mol. Phys., 1971, 20, 1057. [all data]

Watson and Fredrickson, 1932
Watson, W.W.; Fredrickson, W.R., The spectrum of strontium hydride, Phys. Rev., 1932, 39, 765. [all data]

Veseth, 1971, 2
Veseth, L., An investigation of the interaction between close-lying 2Σ and 2Π states of diatomic molecules. II. Λ-doubling of the 2Π levels, Mol. Phys., 1971, 21, 287. [all data]

Veseth, 1971, 3
Veseth, L., Corrections to the spin-orbit splitting in 2Π states of diatomic molecules, J. Mol. Spectrosc., 1971, 38, 228. [all data]

Edvinsson, Kopp, et al., 1963
Edvinsson, G.; Kopp, I.; Lindgren, B.; Aslund, N., Rotational analysis of an ultraviolet system of the hydrides and deuterides of Ca, Sr and Ba, Ark. Fys., 1963, 25, 95. [all data]


Notes

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