Arsenic monohydride


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

(CAS Reg. No. 13937-35-4 • 4294967295Arsenic monohydride) + Arsenic monohydride = CAS Reg. No. 13937-35-4

By formula: (CAS Reg. No. 13937-35-4 • 4294967295HAs) + HAs = CAS Reg. No. 13937-35-4

Quantity Value Units Method Reference Comment
Δr86.8 ± 2.5kcal/molN/AGal, Maria, et al., 1989gas phase

As- + Hydrogen cation = Arsenic monohydride

By formula: As- + H+ = HAs

Quantity Value Units Method Reference Comment
Δr360.44 ± 0.70kcal/molD-EAWalter, Gibson, et al., 2009gas 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 as indicated in comments:
B - John E. Bartmess
LL - Sharon G. Lias and Joel F. Liebman

View reactions leading to HAs+ (ion structure unspecified)

Electron affinity determinations

EA (eV) Method Reference Comment
1.00 ± 0.10PDRackwitz, Feldman, et al., 1977B
<1.09997IMRBEbinghaus, Kraus, et al., 1964From AsH3; B

Ionization energy determinations

IE (eV) Method Reference Comment
9.641 ± 0.008PIBerkowitz, 1988LL

De-protonation reactions

As- + Hydrogen cation = Arsenic monohydride

By formula: As- + H+ = HAs

Quantity Value Units Method Reference Comment
Δr360.44 ± 0.70kcal/molD-EAWalter, Gibson, et al., 2009gas phase; B

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 February, 1976

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 75AsH
StateTeωeωexeωeyeBeαeγeDeβereTrans.ν00
A 3Πi 0 1 [1207.5] 2 Z   [6.5623] 3 4 0.886 2  [0.000703]  [1.6203] 5 A ← X R 30518.34 Z
Dixon and Lamberton, 1968; Veseth, 1972
A 3Πi 1     [6.4726] 6 4   [0.000624]   A ← X R 29821.97 Z
Dixon and Lamberton, 1968; Veseth, 1972
A 3Πi 2     [6.3387] 4   [0.000554]   A ← X R 29282.16 Z
Dixon and Lamberton, 1968; Veseth, 1972
X 3Σ- 0 7 (2130)   [7.1998] 7   [0.000329]  [1.5344]  

Notes

1A0 = -615.4. Small J-dependence Veseth, 1972.
2ΔG(1/2) and α for the 3Π0+ component only.
3Λ-type doubling,Δνef(v=0) = +44.72 + 0.0056J(J+1).
4Lines are sharp for the 3Π0+ state only. Line width increases in the order 3Π0+ < 3Π0- < 3Π1 < 3Π2, and also with increasing vibrational energy. The predissociation is due to interaction with the unstable 5Σ- state arising from As(4S) + H(2S) Dixon and Lamberton, 1968.
5From the "true" B0 values in Veseth, 1972.
6Λ-type doubling,Δνef(v=0) = +0.0214J(J+1).
7Spin splitting constants λ0 = +58.87, γ0 = -0.281.
8From the predissociation in A 3Π.
9From a short extrapolation Dixon and Lamberton, 1968 of the 3Π state to the limit As(2D) + H(2S).
10A0 = -616.9, small J-dependence Veseth, 1972; A1 = -599.8.
11Λ-type doubling, Δνef(v=0) = +43.39 + 0.00472J(J+1).
12Λ-type doubling, Δνef(v=0) = +0.0046J(J+1).
13Spin splitting constants λ0 = +58.811, γ0 = -0.l475.
14H0 = +5E-9.

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.

Gal, Maria, et al., 1989
Gal, J.-F.; Maria, P.-C.; Decouzon, M., The Gas-Phase Acidity and Bond Dissociation Energies of Hydrogen Telluride, Int. J. Mass Spectrom. Ion Proc., 1989, 93, 1, 87, https://doi.org/10.1016/0168-1176(89)83076-9 . [all data]

Walter, Gibson, et al., 2009
Walter, C.W.; Gibson, N.D.; Field, R.L.; Snedden, A.P.; Shapiro, J.Z.; Janczak, C.M.; Hanstorp, D., Electron affinity of arsenic and the fine structure of As- measured using infrared photodetachment threshold spectroscopy, Phys. Rev. A, 2009, 80, 1, 014501, https://doi.org/10.1103/PhysRevA.80.014501 . [all data]

Rackwitz, Feldman, et al., 1977
Rackwitz, R.; Feldman, D.; Kaiser, H.J.; Heincke, E., Photodetachment bei einigen zweiatomigen negativen hydridionen: BeH-, MgH-, CaH-, ZnH-, PH-, AsH-, Z. Naturforsch. A:, 1977, 32, 594. [all data]

Ebinghaus, Kraus, et al., 1964
Ebinghaus, H.; Kraus, K.; Neuert, H.; Muller-Duysing, W., Negative Ionen durch Elecktronenresonanzeinfang in PH3, AsH3, und SiH4, Z. Naturfor., 1964, 19A, 732. [all data]

Berkowitz, 1988
Berkowitz, J., Photoionization mass spectrometric studies of AsHn(n=1-3), J. Chem. Phys., 1988, 89, 7065. [all data]

Dixon and Lamberton, 1968
Dixon, R.N.; Lamberton, H.M., The A, 3Πi-X, 3Σ- band systems of AsH and AsD, J. Mol. Spectrosc., 1968, 25, 12. [all data]

Veseth, 1972
Veseth, I., Fine structure of 3Π and 3Σ- states in diatomic molecules, J. Phys. B:, 1972, 5, 229. [all data]


Notes

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