Iodine
- Formula: I2
- Molecular weight: 253.80894
- IUPAC Standard InChIKey: PNDPGZBMCMUPRI-UHFFFAOYSA-N
- CAS Registry Number: 7553-56-2
- Chemical structure:
This structure is also available as a 2d Mol file or as a computed 3d SD file
The 3d structure may be viewed using Java or Javascript. - Other names: I2; Eranol; Iode; Iodine-127; Iodio; Iosan Superdip; Jod; Jood; Molecular iodine; Tincture iodine; Vistarin; Iodine crystals; Iodine sublimed; Diiodine; Diatomic iodine
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- Information on this page:
- Other data available:
- Condensed phase thermochemistry data
- Phase change data
- Reaction thermochemistry data: reactions 51 to 75
- Henry's Law data
- Data at other public NIST sites:
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Gas phase thermochemistry data
Go To: Top, Reaction thermochemistry data, Gas phase ion energetics data, Ion clustering 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.
Quantity | Value | Units | Method | Reference | Comment |
---|---|---|---|---|---|
ΔfH°gas | 62.42 ± 0.08 | kJ/mol | Review | Cox, Wagman, et al., 1984 | CODATA Review value |
ΔfH°gas | 62.42 | kJ/mol | Review | Chase, 1998 | Data last reviewed in June, 1982 |
Quantity | Value | Units | Method | Reference | Comment |
S°gas,1 bar | 260.687 ± 0.005 | J/mol*K | Review | Cox, Wagman, et al., 1984 | CODATA Review value |
S°gas,1 bar | 260.69 | J/mol*K | Review | Chase, 1998 | Data last reviewed in June, 1982 |
Gas Phase Heat Capacity (Shomate Equation)
Cp° = A + B*t + C*t2 + D*t3 +
E/t2
H° − H°298.15= A*t + B*t2/2 +
C*t3/3 + D*t4/4 − E/t + F − H
S° = A*ln(t) + B*t + C*t2/2 + D*t3/3 −
E/(2*t2) + G
Cp = heat capacity (J/mol*K)
H° = standard enthalpy (kJ/mol)
S° = standard entropy (J/mol*K)
t = temperature (K) / 1000.
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Temperature (K) | 457.666 to 2000. | 2000. to 6000. |
---|---|---|
A | 37.79763 | 76.73414 |
B | 0.225453 | -4.045782 |
C | -0.912556 | -1.848145 |
D | 1.034913 | 0.219044 |
E | -0.083826 | -82.39384 |
F | 50.86865 | -53.87151 |
G | 305.9199 | 281.2267 |
H | 62.42110 | 62.42110 |
Reference | Chase, 1998 | Chase, 1998 |
Comment | Data last reviewed in June, 1982 | Data last reviewed in June, 1982 |
Reaction thermochemistry data
Go To: Top, Gas phase thermochemistry data, Gas phase ion energetics data, Ion clustering 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
MS - José A. Martinho Simões
ALS - Hussein Y. Afeefy, Joel F. Liebman, and Stephen E. Stein
M - Michael M. Meot-Ner (Mautner) and Sharon G. Lias
Note: Please consider using the reaction search for this species. This page allows searching of all reactions involving this species. A general reaction search form is also available. Future versions of this site may rely on reaction search pages in place of the enumerated reaction displays seen below.
Reactions 1 to 50
+ = I3-
Quantity | Value | Units | Method | Reference | Comment |
---|---|---|---|---|---|
ΔrH° | 136. ± 10. | kJ/mol | N/A | Taylor, Asmis, et al., 1999 | gas phase; B |
ΔrH° | 126. ± 5.9 | kJ/mol | CIDT | Do, Klein, et al., 1997 | gas phase; B |
ΔrH° | 356.1 | kJ/mol | Ther | Finch, Gates, et al., 1977 | gas phase; This value is far more bound than expected from other studies; B |
ΔrH° | 136.4 | kJ/mol | N/A | Check, Faust, et al., 2001 | gas phase; FeF3-(t); ; ΔS(EA)=2.8; B |
Quantity | Value | Units | Method | Reference | Comment |
ΔrG° | 94.14 | kJ/mol | N/A | Check, Faust, et al., 2001 | gas phase; FeF3-(t); ; ΔS(EA)=2.8; B |
By formula: C10Mn2O10 (cr) + I2 (cr) = 2C5IMnO5 (cr)
Quantity | Value | Units | Method | Reference | Comment |
---|---|---|---|---|---|
ΔrH° | -185.0 ± 8.7 | kJ/mol | PC | Harel and Adamson, 1986 | The reaction enthalpy was calculated from the enthalpy of the same reaction in cyclohexane, -187.9 ± 8.4 kJ/mol Harel and Adamson, 1986, and from the solution enthalpies of Mn2(CO)10(cr), 36.0 ± 2.1 kJ/mol, I2(cr), 20.5 ± 0.4 kJ/mol, and Mn(CO)5(I)(cr), 26.8 ± 0.5 kJ/mol Harel and Adamson, 1986. The latter value refers to the solution in benzene and is therefore taken as an approximation; MS |
By formula: C10O10Re2 (cr) + I2 (cr) = 2C5IO5Re (cr)
Quantity | Value | Units | Method | Reference | Comment |
---|---|---|---|---|---|
ΔrH° | -172. ± 18. | kJ/mol | PC | Harel and Adamson, 1986 | The reaction enthalpy was calculated from the enthalpy of the same reaction in cyclohexane, -157. ± 16. kJ/mol, and from the solution enthalpies of Re2(CO)10(cr), 34.3 ± 2.1 kJ/mol, I2(cr), 20.5 ± 0.4 kJ/mol, and Re(CO)5(I)(cr), 34.7 ± 4.2 kJ/mol Harel and Adamson, 1986; MS |
By formula: HI + C3H5I = C3H6 + I2
Quantity | Value | Units | Method | Reference | Comment |
---|---|---|---|---|---|
ΔrH° | -33.3 ± 1.4 | kJ/mol | Eqk | Rodgers, Golden, et al., 1966 | gas phase; ALS |
ΔrH° | -39.7 ± 4.2 | kJ/mol | Eqk | Rodgers, Golden, et al., 1966 | gas phase; Reanalyzed by Cox and Pilcher, 1970, Original value = -34.9 ± 0.96 kJ/mol; At 527 K; ALS |
By formula: HI + CH3I = CH4 + I2
Quantity | Value | Units | Method | Reference | Comment |
---|---|---|---|---|---|
ΔrH° | -52.55 ± 0.54 | kJ/mol | Eqk | Golden, Walsh, et al., 1965 | gas phase; ALS |
ΔrH° | -53.0 ± 0.2 | kJ/mol | Eqk | Goy and Pritchard, 1965 | gas phase; ALS |
ΔrH° | -46.2 ± 5.6 | kJ/mol | Cm | Nichol and Ubbelohde, 1952 | gas phase; ALS |
C12H16Nb (cr) + 2 (cr) = C10H10I2Nb (cr) + 2 (l)
By formula: C12H16Nb (cr) + 2I2 (cr) = C10H10I2Nb (cr) + 2CH3I (l)
Quantity | Value | Units | Method | Reference | Comment |
---|---|---|---|---|---|
ΔrH° | -242.3 ± 2.4 | kJ/mol | RSC | Diogo, Simoni, et al., 1993 | The difference between the enthalpies of formation of Nb(Cp)2(I)2 and Nb(Cp)2(Me)2 is calculated as -215.1 ± 2.6 kJ/mol; MS |
C20H26CoN5O4 (solution) + (solution) = C13H19CoIN5O4 (solution) + (solution)
By formula: C20H26CoN5O4 (solution) + I2 (solution) = C13H19CoIN5O4 (solution) + C7H7I (solution)
Quantity | Value | Units | Method | Reference | Comment |
---|---|---|---|---|---|
ΔrH° | -63.2 ± 3.8 | kJ/mol | RSC | Toscano, Seligson, et al., 1989 | solvent: Bromoform; The enthalpy of solution of Co(py)(dmg)2(Bz)(cr) was measured as 11.3 kJ/mol Toscano, Seligson, et al., 1989; MS |
C14H22CoN5O4 (solution) + (solution) = C13H19CoIN5O4 (solution) + (solution)
By formula: C14H22CoN5O4 (solution) + I2 (solution) = C13H19CoIN5O4 (solution) + CH3I (solution)
Quantity | Value | Units | Method | Reference | Comment |
---|---|---|---|---|---|
ΔrH° | -92.9 ± 2.5 | kJ/mol | RSC | Toscano, Seligson, et al., 1989 | solvent: Bromoform; The enthalpy of solution of Co(py)(dmg)2(Me)(cr) was measured as 10.9 kJ/mol Toscano, Seligson, et al., 1989; MS |
By formula: C5HMnO5 (l) + I2 (cr) = HI (g) + C5IMnO5 (cr)
Quantity | Value | Units | Method | Reference | Comment |
---|---|---|---|---|---|
ΔrH° | -108. ± 8. | kJ/mol | RSC | Connor, Zafarani-Moattar, et al., 1982 | The reaction enthalpy relies on -25. ± 5. kJ/mol for the enthalpy of solution of HI(g) in benzene Connor, Zafarani-Moattar, et al., 1982.; MS |
By formula: C2H4 + I2 = C2H4I2
Quantity | Value | Units | Method | Reference | Comment |
---|---|---|---|---|---|
ΔrH° | -48.1 ± 0.8 | kJ/mol | Eqk | Abrams and Davis, 1954 | gas phase; ALS |
ΔrH° | -56. ± 2. | kJ/mol | Eqk | Cutherbertson and Kistiakowsky, 1935 | gas phase; Heat of dissociation; ALS |
By formula: I2 + CClF3 = CF3I + ClI
Quantity | Value | Units | Method | Reference | Comment |
---|---|---|---|---|---|
ΔrH° | 72.3 ± 1.1 | kJ/mol | Eqk | Lord, Goy, et al., 1967 | gas phase; Reanalyzed by Cox and Pilcher, 1970, Original value = 71.55 ± 0.71 kJ/mol; ALS |
By formula: HI + C6H11I = C6H12 + I2
Quantity | Value | Units | Method | Reference | Comment |
---|---|---|---|---|---|
ΔrH° | -32.6 ± 8.4 | kJ/mol | Cm | Brennan and Ubbelohde, 1956 | gas phase; Reanalyzed by Cox and Pilcher, 1970, Original value = -28. ± 4.2 kJ/mol; ALS |
By formula: C2H3F3 + I2 = HI + C2H2F3I
Quantity | Value | Units | Method | Reference | Comment |
---|---|---|---|---|---|
ΔrH° | -64. ± 2. | kJ/mol | Eqk | Wu and Rodgers, 1974 | gas phase; Heat of formation Unpublished results by B.J. Zwolinski; ALS |
By formula: C2H2BrF3 + I2 = C2H2F3I + BrI
Quantity | Value | Units | Method | Reference | Comment |
---|---|---|---|---|---|
ΔrH° | 28. ± 2. | kJ/mol | Eqk | Buckley, Ford, et al., 1980 | gas phase; GLC;hf298_gas[kcal/mol]=-166.8±1.1; Kolesov and Papina, 1983; ALS |
By formula: C2H6Hg (l) + 2I2 (cr) = 2CH3I (l) + HgI2 (cr)
Quantity | Value | Units | Method | Reference | Comment |
---|---|---|---|---|---|
ΔrH° | -184.5 ± 0.8 | kJ/mol | RSC | Hartley, Pritchard, et al., 1950 | Please also see Pedley and Rylance, 1977 and Cox and Pilcher, 1970, 2.; MS |
(solution) + (solution) = 2 (solution)
By formula: C10O10Re2 (solution) + I2 (solution) = 2C5IO5Re (solution)
Quantity | Value | Units | Method | Reference | Comment |
---|---|---|---|---|---|
ΔrH° | -157. ± 16. | kJ/mol | PC | Harel and Adamson, 1986 | solvent: Cyclohexane; Please also see Adamson, Vogler, et al., 1978.; MS |
(l) + 3 (cr) = GaI3 (cr) + 3 (l)
By formula: C3H9Ga (l) + 3I2 (cr) = GaI3 (cr) + 3CH3I (l)
Quantity | Value | Units | Method | Reference | Comment |
---|---|---|---|---|---|
ΔrH° | -200.0 ± 8.4 | kJ/mol | RSC | Fowell and Mortimer, 1958 | Please also see Pedley and Rylance, 1977 and Cox and Pilcher, 1970, 2.; MS |
(l) + 2 (cr) = CH3GaI2 (cr) + 2 (l)
By formula: C3H9Ga (l) + 2I2 (cr) = CH3GaI2 (cr) + 2CH3I (l)
Quantity | Value | Units | Method | Reference | Comment |
---|---|---|---|---|---|
ΔrH° | -158.6 ± 4.2 | kJ/mol | RSC | Fowell and Mortimer, 1958 | Please also see Pedley and Rylance, 1977 and Cox and Pilcher, 1970, 2.; MS |
(l) + (cr) = 2C3H9ISn (l)
By formula: C6H18Sn2 (l) + I2 (cr) = 2C3H9ISn (l)
Quantity | Value | Units | Method | Reference | Comment |
---|---|---|---|---|---|
ΔrH° | -184.1 ± 2.9 | kJ/mol | RSC | Pedley, Skinner, et al., 1957 | Please also see Pedley and Rylance, 1977 and Cox and Pilcher, 1970, 2.; MS |
By formula: C4H8I2 = C4H8 + I2
Quantity | Value | Units | Method | Reference | Comment |
---|---|---|---|---|---|
ΔrH° | 50.2 ± 6.3 | kJ/mol | Cm | Cline and Kistiakowsky, 1937 | gas phase; Heat of formation derived by Cox and Pilcher, 1970; ALS |
(cr) + (solution) = (solution) + C8H5IO3W (solution)
By formula: C8H6O3W (cr) + I2 (solution) = HI (solution) + C8H5IO3W (solution)
Quantity | Value | Units | Method | Reference | Comment |
---|---|---|---|---|---|
ΔrH° | -67.4 ± 3.8 | kJ/mol | RSC | Landrum and Hoff, 1985 | solvent: Dichloromethane; MS |
C15H12MoO3 (solution) + (solution) = C8H5IMoO3 (solution) + (solution)
By formula: C15H12MoO3 (solution) + I2 (solution) = C8H5IMoO3 (solution) + C7H7I (solution)
Quantity | Value | Units | Method | Reference | Comment |
---|---|---|---|---|---|
ΔrH° | -120.5 ± 4.2 | kJ/mol | RSC | Nolan, de la Vega, et al., 1988 | solvent: Tetrahydrofuran; MS |
C8H6MoO3 (cr) + (solution) = C8H5IMoO3 (solution) + (solution)
By formula: C8H6MoO3 (cr) + I2 (solution) = C8H5IMoO3 (solution) + HI (solution)
Quantity | Value | Units | Method | Reference | Comment |
---|---|---|---|---|---|
ΔrH° | -75.3 ± 2.5 | kJ/mol | RSC | Landrum and Hoff, 1985 | solvent: Dichloromethane; MS |
C10MnO10Re (solution) + (solution) = (solution) + (solution)
By formula: C10MnO10Re (solution) + I2 (solution) = C5IO5Re (solution) + C5IMnO5 (solution)
Quantity | Value | Units | Method | Reference | Comment |
---|---|---|---|---|---|
ΔrH° | -233. ± 13. | kJ/mol | PC | Harel and Adamson, 1986 | solvent: Cyclohexane; MS |
C8H5MoNaO3 (solution) + (cr) = C8H5IMoO3 (solution) + (cr)
By formula: C8H5MoNaO3 (solution) + I2 (cr) = C8H5IMoO3 (solution) + INa (cr)
Quantity | Value | Units | Method | Reference | Comment |
---|---|---|---|---|---|
ΔrH° | -133.1 ± 5.4 | kJ/mol | RSC | Nolan, López de la Vega, et al., 1986 | solvent: Tetrahydrofuran; MS |
By formula: C2F4I2 = C2F4 + I2
Quantity | Value | Units | Method | Reference | Comment |
---|---|---|---|---|---|
ΔrH° | 69. ± 2. | kJ/mol | Eqk | Wu, Pickard, et al., 1975 | gas phase; Spectrophotometery at 298.15°K; ALS |
By formula: 2C3H8S + I2 = 2HI + C6H14S2
Quantity | Value | Units | Method | Reference | Comment |
---|---|---|---|---|---|
ΔrH° | -124.9 | kJ/mol | Cm | Sunner, 1955 | liquid phase; solvent: Ethanol/water(90/10); ALS |
By formula: 2C5H12S + I2 = 2HI + C10H22S2
Quantity | Value | Units | Method | Reference | Comment |
---|---|---|---|---|---|
ΔrH° | -124.9 | kJ/mol | Cm | Sunner, 1955 | liquid phase; solvent: Ethanol/water(90/10); ALS |
By formula: C4H10S2 + I2 = 2HI + C4H8S2
Quantity | Value | Units | Method | Reference | Comment |
---|---|---|---|---|---|
ΔrH° | -123.2 | kJ/mol | Cm | Sunner, 1955 | liquid phase; solvent: Ethanol/water(90/10); ALS |
By formula: C8H16O2S2 + I2 = 2HI + C8H14O2S2
Quantity | Value | Units | Method | Reference | Comment |
---|---|---|---|---|---|
ΔrH° | -109.6 | kJ/mol | Cm | Sunner, 1955 | liquid phase; solvent: Ethanol/water(90/10); ALS |
C22H36Zr (solution) + 2 (solution) = C20H30I2Zr (solution) + 2 (solution)
By formula: C22H36Zr (solution) + 2I2 (solution) = C20H30I2Zr (solution) + 2CH3I (solution)
Quantity | Value | Units | Method | Reference | Comment |
---|---|---|---|---|---|
ΔrH° | -292.9 ± 2.5 | kJ/mol | RSC | Schock and Marks, 1988 | solvent: Toluene; MS |
By formula: C3H8S2 + I2 = 2HI + C3H6S2
Quantity | Value | Units | Method | Reference | Comment |
---|---|---|---|---|---|
ΔrH° | -107.7 | kJ/mol | Cm | Sunner, 1955 | liquid phase; solvent: Ethanol/water(90/10); ALS |
C12H16Zr (solution) + 2 (solution) = C10H10I2Zr (solution) + 2 (solution)
By formula: C12H16Zr (solution) + 2I2 (solution) = C10H10I2Zr (solution) + 2CH3I (solution)
Quantity | Value | Units | Method | Reference | Comment |
---|---|---|---|---|---|
ΔrH° | -291.2 ± 2.5 | kJ/mol | RSC | Schock and Marks, 1988 | solvent: Toluene; MS |
C22H30O2Zr (solution) + (solution) = C20H30I2Zr (solution) + 2 (solution)
By formula: C22H30O2Zr (solution) + I2 (solution) = C20H30I2Zr (solution) + 2CO (solution)
Quantity | Value | Units | Method | Reference | Comment |
---|---|---|---|---|---|
ΔrH° | -191.6 ± 1.7 | kJ/mol | RSC | Schock and Marks, 1988 | solvent: Toluene; MS |
C22H36Hf (solution) + 2 (solution) = C20H30HfI2 (solution) + 2 (solution)
By formula: C22H36Hf (solution) + 2I2 (solution) = C20H30HfI2 (solution) + 2CH3I (solution)
Quantity | Value | Units | Method | Reference | Comment |
---|---|---|---|---|---|
ΔrH° | -265.3 ± 3.3 | kJ/mol | RSC | Schock and Marks, 1988 | solvent: Toluene; MS |
C37H30ClIrO3P2S (solution) + (solution) = C37H30ClI2IrOP2 (solution) + (solution)
By formula: C37H30ClIrO3P2S (solution) + I2 (solution) = C37H30ClI2IrOP2 (solution) + O2S (solution)
Quantity | Value | Units | Method | Reference | Comment |
---|---|---|---|---|---|
ΔrH° | -102.9 ± 0.4 | kJ/mol | RSC | Drago, Nozari, et al., 1979 | solvent: Benzene; MS |
By formula: HI + C7H7I = C7H8 + I2
Quantity | Value | Units | Method | Reference | Comment |
---|---|---|---|---|---|
ΔrH° | -33. ± 4.6 | kJ/mol | Cm | Graham, Nichol, et al., 1955 | liquid phase; solvent: p-Xylene; ALS |
By formula: H2 + 2CH3I = 2CH4 + I2
Quantity | Value | Units | Method | Reference | Comment |
---|---|---|---|---|---|
ΔrH° | -126. ± 3. | kJ/mol | Chyd | Carson, Carter, et al., 1961 | liquid phase; solvent: Ether; ALS |
C20H32Zr (solution) + (solution) = C20H30I2Zr (solution) + (g)
By formula: C20H32Zr (solution) + I2 (solution) = C20H30I2Zr (solution) + H2 (g)
Quantity | Value | Units | Method | Reference | Comment |
---|---|---|---|---|---|
ΔrH° | -309.2 ± 3.3 | kJ/mol | RSC | Schock and Marks, 1988 | solvent: Toluene; MS |
C20H32Hf (solution) + (solution) = C20H30HfI2 (solution) + (g)
By formula: C20H32Hf (solution) + I2 (solution) = C20H30HfI2 (solution) + H2 (g)
Quantity | Value | Units | Method | Reference | Comment |
---|---|---|---|---|---|
ΔrH° | -296.6 ± 2.9 | kJ/mol | RSC | Schock and Marks, 1988 | solvent: Toluene; MS |
C16H10O6W2 (cr) + (solution) = 2C8H5IO3W (solution)
By formula: C16H10O6W2 (cr) + I2 (solution) = 2C8H5IO3W (solution)
Quantity | Value | Units | Method | Reference | Comment |
---|---|---|---|---|---|
ΔrH° | -146.4 ± 3.8 | kJ/mol | RSC | Landrum and Hoff, 1985 | solvent: Dichloromethane; MS |
C16H10Mo2O6 (cr) + (solution) = 2C8H5IMoO3 (solution)
By formula: C16H10Mo2O6 (cr) + I2 (solution) = 2C8H5IMoO3 (solution)
Quantity | Value | Units | Method | Reference | Comment |
---|---|---|---|---|---|
ΔrH° | -133.1 ± 4.2 | kJ/mol | RSC | Landrum and Hoff, 1985 | solvent: Dichloromethane; MS |
(solution) + (solution) = 2 (solution)
By formula: C10Mn2O10 (solution) + I2 (solution) = 2C5IMnO5 (solution)
Quantity | Value | Units | Method | Reference | Comment |
---|---|---|---|---|---|
ΔrH° | -187.9 ± 8.4 | kJ/mol | PC | Harel and Adamson, 1986 | solvent: Cyclohexane; MS |
By formula: I- + I2 = (I- • I2)
Quantity | Value | Units | Method | Reference | Comment |
---|---|---|---|---|---|
ΔrH° | 100. | kJ/mol | N/A | Downs and Adams, 1973 | gas phase; from ΔrH(f); M |
By formula: H2 + 2C2H5I = 2C2H6 + I2
Quantity | Value | Units | Method | Reference | Comment |
---|---|---|---|---|---|
ΔrH° | -88.7 ± 3.3 | kJ/mol | Chyd | Ashcroft, Carson, et al., 1965 | liquid phase; ALS |
2 + = C6H14Hg + 2
By formula: 2C3H7I + HgI2 = C6H14Hg + 2I2
Quantity | Value | Units | Method | Reference | Comment |
---|---|---|---|---|---|
ΔrH° | 242.3 ± 1.9 | kJ/mol | Cm | Mortimer, Pritchard, et al., 1952 | liquid phase; ALS |
2 + = C6H14Hg + 2
By formula: 2C3H7I + HgI2 = C6H14Hg + 2I2
Quantity | Value | Units | Method | Reference | Comment |
---|---|---|---|---|---|
ΔrH° | 215.7 ± 2.4 | kJ/mol | Cm | Mortimer, Pritchard, et al., 1952 | liquid phase; ALS |
By formula: HI + CH3IS = CH4S + I2
Quantity | Value | Units | Method | Reference | Comment |
---|---|---|---|---|---|
ΔrH° | -12.0 ± 2.3 | kJ/mol | Eqk | Shum and Benson, 1983 | gas phase; ALS |
By formula: C3H6O + I2 = HI + C3H5IO
Quantity | Value | Units | Method | Reference | Comment |
---|---|---|---|---|---|
ΔrH° | 50.6 ± 5.0 | kJ/mol | Eqk | Solly, Golden, et al., 1970 | gas phase; ALS |
By formula: I2 + CBrF3 = CF3I + BrI
Quantity | Value | Units | Method | Reference | Comment |
---|---|---|---|---|---|
ΔrH° | 40.0 ± 0.1 | kJ/mol | Eqk | Lord, Goy, et al., 1967 | gas phase; ALS |
Gas phase ion energetics data
Go To: Top, Gas phase thermochemistry data, Reaction thermochemistry data, Ion clustering 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 evaluated as indicated in comments:
L - Sharon G. Lias
Data compiled as indicated in comments:
LL - Sharon G. Lias and Joel F. Liebman
LBLHLM - Sharon G. Lias, John E. Bartmess, Joel F. Liebman, John L. Holmes, Rhoda D. Levin, and W. Gary Mallard
LLK - Sharon G. Lias, Rhoda D. Levin, and Sherif A. Kafafi
RDSH - Henry M. Rosenstock, Keith Draxl, Bruce W. Steiner, and John T. Herron
B - John E. Bartmess
View reactions leading to I2+ (ion structure unspecified)
Quantity | Value | Units | Method | Reference | Comment |
---|---|---|---|---|---|
IE (evaluated) | 9.3074 ± 0.0002 | eV | N/A | N/A | L |
Electron affinity determinations
EA (eV) | Method | Reference | Comment |
---|---|---|---|
2.5240 ± 0.0050 | LPES | Zanni, Taylor, et al., 1997 | B |
2.52 ± 0.10 | NBIE | Auerbach, Baeda, et al., 1973 | B |
2.42 ± 0.20 | Endo | Hughes, Lifschitz, et al., 1973 | B |
2.58 ± 0.10 | Endo | Chupka, Berkowitz, et al., 1971 | B |
2.60 ± 0.10 | EIAE | DeCorpo and Franklin, 1971 | From CHI3; B |
2.40 ± 0.10 | NBIE | Moutinho, Aten, et al., 1971 | B |
2.33004 | ECD | Ayala, Wentworth, et al., 1981 | Vertical Detachment Energy: 1.7 eV; B |
1.722 ± 0.050 | NBIE | Hubers, Kleyn, et al., 1976 | Stated electron affinity is the Vertical Detachment Energy; B |
Ionization energy determinations
IE (eV) | Method | Reference | Comment |
---|---|---|---|
9.3074 ± 0.0002 | TE | Cockett, Donovan, et al., 1996 | LL |
9.3074 ± 0.0002 | TE | Cockett, Goode, et al., 1995 | LL |
9.33 | PE | Carlson, Gerard, et al., 1988 | LL |
9.29 ± 0.05 | PI | Grade and Rosinger, 1985 | LBLHLM |
9.3 ± 0.2 | EI | Grade and Rosinger, 1985 | LBLHLM |
9.3 ± 0.2 | EI | Grade and Rosinger, 1984 | LBLHLM |
9.3 ± 0.2 | EI | Grade, Rosinger, et al., 1984 | LBLHLM |
9.3 ± 0.05 | EI | Hoareau, Cabaud, et al., 1981 | LLK |
9.5 | EI | Pittermann and Weil, 1980 | LLK |
9.311 ± 0.002 | PE | Higginson, Lloyd, et al., 1973 | LLK |
9.22 ± 0.01 | PE | Potts and Price, 1971 | LLK |
~9.37 | PI | Dibeler, Walker, et al., 1971 | LLK |
9.3995 ± 0.0012 | S | Venkateswarlu, 1970 | RDSH |
9.331 | PI | Myer and Samson, 1970 | RDSH |
9.356 | PE | Kimura, Katsumata, et al., 1981 | Vertical value; LLK |
9.34 | PE | Cornford, Frost, et al., 1971 | Vertical value; LLK |
Appearance energy determinations
Ion | AE (eV) | Other Products | Method | Reference | Comment |
---|---|---|---|---|---|
I+ | 8.8 ± 0.2 | I- | EI | Grade and Rosinger, 1985 | LBLHLM |
I+ | 11.94 ± 0.15 | I | PI | Grade and Rosinger, 1985 | LBLHLM |
I+ | 8.83 ± 0.07 | I- | PI | Grade and Rosinger, 1985 | LBLHLM |
I+ | 8.9 ± 0.2 | I- | EI | Grade and Rosinger, 1984 | LBLHLM |
I+ | 8.8 ± 0.2 | I- | EI | Grade, Rosinger, et al., 1984 | LBLHLM |
I+ | 13.0 | I | EI | Pittermann and Weil, 1980 | LLK |
I+ | 8.922 ± 0.013 | I- | PI | Myer and Samson, 1970 | RDSH |
I+ | 8.95 ± 0.02 | I- | PI | Morrison, Hurzeler, et al., 1960 | RDSH |
I+ | 8.83 ± 0.02 | I- | PI | Watanabe, 1957 | RDSH |
Ion clustering data
Go To: Top, Gas phase thermochemistry data, Reaction thermochemistry data, Gas phase ion energetics 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:
M - Michael M. Meot-Ner (Mautner) and Sharon G. Lias
B - John E. Bartmess
Note: Please consider using the reaction search for this species. This page allows searching of all reactions involving this species. Searches may be limited to ion clustering reactions. A general reaction search form is also available.
Clustering reactions
By formula: I- + I2 = (I- • I2)
Quantity | Value | Units | Method | Reference | Comment |
---|---|---|---|---|---|
ΔrH° | 100. | kJ/mol | N/A | Downs and Adams, 1973 | gas phase; from ΔrH(f); M |
+ = I3-
Quantity | Value | Units | Method | Reference | Comment |
---|---|---|---|---|---|
ΔrH° | 136. ± 10. | kJ/mol | N/A | Taylor, Asmis, et al., 1999 | gas phase; B |
ΔrH° | 126. ± 5.9 | kJ/mol | CIDT | Do, Klein, et al., 1997 | gas phase; B |
ΔrH° | 356.1 | kJ/mol | Ther | Finch, Gates, et al., 1977 | gas phase; This value is far more bound than expected from other studies; B |
ΔrH° | 136.4 | kJ/mol | N/A | Check, Faust, et al., 2001 | gas phase; FeF3-(t); ; ΔS(EA)=2.8; B |
Quantity | Value | Units | Method | Reference | Comment |
ΔrG° | 94.14 | kJ/mol | N/A | Check, Faust, et al., 2001 | gas phase; FeF3-(t); ; ΔS(EA)=2.8; B |
By formula: I3- + I2 = (I3- • I2)
Quantity | Value | Units | Method | Reference | Comment |
---|---|---|---|---|---|
ΔrH° | 49.0 ± 5.9 | kJ/mol | CIDT | Do, Klein, et al., 1997 | gas phase; B |
Constants of diatomic molecules
Go To: Top, Gas phase thermochemistry data, Reaction thermochemistry data, Gas phase ion energetics data, Ion clustering 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 January, 1977
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 |
---|---|---|---|---|---|---|---|---|---|---|---|---|
The absorption spectrum from 450000 to 870000 cm-1 (55.8 to 107.9 eV) at low resolution has been described by Myer and Samson, 1970. It corresponds to excitation from 4d shell to various unfilled orbitals. | ||||||||||||
↳Comes, Nielsen, et al., 1973 | ||||||||||||
The absorption spectrum in the VUV region at high resolution has most recently been photographed by Venkateswarlu, 1970 who gives an extensive table of observed features in the region 56500 - 75800 cm-1. Most of the bands are assigned to extended Rydberg series converging to a common limit at 75814 cm-1 (9.400 eV), a smaller number to fragments of series converging to 80895 cm-1 (10.03 eV). The limits are assumed to correspond to v=0 of X 2 Πg, 3/2 and 1/2, respectively, of I2+; see, however, 1. Several of the progressions observed in absorption Venkateswarlu, 1970 appear to correspond to emission bands recorded by Haranath and Rao, 1958 under medium resolution in the region 56000 - 68000 cm-1 and classified by them as belonging to twelve systems. See also Cordes, 1935 Myer and Samson, 1970*. | ||||||||||||
↳Haranath and Rao, 1958; missing citation | ||||||||||||
I | (51973) 2 | 112.4 H | 0.705 | 0.004 | I → (B) 2 R | 36197 H | ||||||
↳Venkateswarlu, 1951; Verma, 1959; Mulliken, 1971 | ||||||||||||
(H) | (46063) | 103.7 H | 0.095 | (H → B) 3 R | 30283 H | |||||||
↳Verma, 1959; Mulliken, 1971 | ||||||||||||
State | Te | ωe | ωexe | ωeye | Be | αe | γe | De | βe | re | Trans. | ν00 |
F (1Σu+) 6 | 47217.8 | 95.955 H | 0.3623 | (3.6) 4 | F ↔ X 5 R | 47158.6 H | ||||||
↳Verma, 1959; Mulliken, 1971; missing citation | ||||||||||||
F' | 45230 | 93.4 H | 0.6 | F' → X 7 R | 45169 H | |||||||
↳Haranath and Rao, 1958 | ||||||||||||
G' (3Π1g) 9 | (42300) 8 | G' ← A | ||||||||||
↳Skorko, 1933; Mulliken, 1971 | ||||||||||||
E 3Πo+g 9 | 41411.4 | 101.59 H | 0.2380 | (3.65) | E → B 10 R | 25630.5 H | ||||||
↳Haranath and Rao Prasada, 1960; Mulliken, 1971; Wieland, Tellinghuisen, et al., 1972 | ||||||||||||
State | Te | ωe | ωexe | ωeye | Be | αe | γe | De | βe | re | Trans. | ν00 |
D 1Σu+ 13 | (40679) | 104.41 H | 0.2343 11 | 0.00045 | D ↔ X 12 R | (40624) | ||||||
↳missing citation; Mulliken, 1971; Mulliken, 1971 | ||||||||||||
G 3Π2g 9 | (40300) 14 | G ← A' 15 | ||||||||||
↳Skorko, 1933; Mulliken, 1971 | ||||||||||||
C 3Σ1u+ 13 | 16 | C ← X | ||||||||||
↳Kortum and Friedheim, 1947; Mathieson and Rees, 1956; Mulliken, 1971 | ||||||||||||
B" 1Π1u 19 | 17 | B" ↔ X 18 | ||||||||||
↳Oldman, Sander, et al., 1971; Tellinghuisen, 1973; Brown and Burns, 1974 | ||||||||||||
State | Te | ωe | ωexe | ωeye | Be | αe | γe | De | βe | re | Trans. | ν00 |
B' 3Π0-u 19 | 20 | |||||||||||
B 3Π0+u 19 | 15769.01 | 125.697 Z | 0.7642 21 22 | 0.029039 23 24 | 0.0001582 25 22 | 5.43E-9 26 | 0.30E-9 | 3.0247 | B ↔ X 18 27 28 R | 15724.57 29 Z | ||
↳Barrow and Yee, 1973; missing citation; Wei and Tellinghuisen, 1974 | ||||||||||||
A 3Π1u 19 | (11888) | (44.0) 30 H | (1.0) | 30 | A ← X 31 R | (11803) 30 | ||||||
↳Brown, 1931; Tellinghuisen, 1973 | ||||||||||||
A' 3Π2u 19 | (10100) 32 | |||||||||||
X 1Σg+ | 0 | 214.502 33 Z | 0.6147 33 | 0.037372 33 34 | 0.0001138 33 | 4.25E-9 35 | 3.2E-10 | 2.6663 36 | ||||
↳Kiefer and Bernstein, 1972; Williams, Rousseau, et al., 1974 |
Notes
1 | From the photoelectron spectrum Potts and Price, 1971, Higginson, Lloyd, et al., 1973; adiabatic potential established by temperature variation. The same method yields 9.953 eV for the ionization potential to 2Π1/2g(v=0). Neither result agrees with the values obtained by Venkateswarlu, 1970 from Rydberg series, i.e. 9.400 and 10.03 eV. The discrepancy could be understood if the Rydberg series were to correspond to v'=3, but the absence of series with v' = 0, 1, 2 would still be puzzling. |
2 | Weak emission bands in the presence of foreign gases, 2785-2731 . Te is based on the assumption that the lower state is the B state, but Mulliken, 1971, has suggested that instead it may be the D state leading to Te ~ 76872 cm-1 Mulliken, 1971. |
3 | Strong emission bands in the presence of foreign gases, 3460 - 3015 Angstroms. It is by no means certain that the lower state has been correctly identified as the B state. Mulliken, 1971, suggests that the bands arise from the transition G → A'. |
4 | From the intensity distribution and Franck-Condon principle Mulliken, 1971, Wieland, Tellinghuisen, et al., 1972. |
5 | In emission in electric discharges in the presence of foreign gases, 2740 - 2490 . Also observed for 129 I2, confirming the vibrational numbering. Emission bands in the region 2240 - 1950 Angstroms are assigned by Haranath and Rao, 1958, to a separate system (called H → X), with v00 = 48072 and w ~ 79. It seems, however, possible that these bands belong to F → X. |
6 | Configuration...σg2πu3πg3σu2. |
7 | The analysis of this fairly extensive system [2400 - 2240 , called E → X by Haranath and Rao, 1958] is not yet supported by isotope studies, nor is it seen in absorption. |
8 | Suggested upper state of high temperature absorption "continuum" shortward of 3263 (30640 cm-1) |
9 | Configuration...σgπu4πg3σu2. |
10 | Emission bands in the presence of foreign gases, 4400 - 4000 . Also observed for 129I2, confirming the vibrational numbering. The E → B fluorescence spectrum following two-photon absorption Rousseau and Williams, 1974, consists of transitions both to the discrete and to the continuous part of B, the latter giving rise to diffuse bands ("structured" continuum) Tellinghuisen, 1975. From a comparison of the calculated with the observed intensity distribution Tellinghuisen, 1975, obtains the potential function of E as well as the variation of the transition moment with r. The lifetime of E → B is 27 ns Rousseau, 1975 confirming that this is an allowed transition and that the E state is 3Π0+g. |
11 | The v' numbering is uncertain and, therefore, the vibrational constants are subject to change. |
12 | The system includes the absorption bands of Pringsheim and Rosen, 1928, Kimura and Miyanishi, 1929, Cordes, 1935, remeasured by Nobs and Wieland, 1966. It also includes the resonance series of Verma, 1960 in the region 1830 - 2370 which arise from very high vibrational levels (v' ~ 195), of the D state excited by the 1830 atomic line of iodine. The system further includes the diffuse emission bands in the region 2500 - 5000 with a characteristic group near 3250 [McLennan bands McLennan, 1913]. The diffuse bands have been recognized by Mulliken, 1971, to correspond to transitions from D to the continuum of X [Condon diffraction bands, see also Tellinghuisen, 1974]. Earlier summaries Mathieson and Rees, 1956, Haranath and Rao, 1958, Venkateswarlu, 1970 gave an electronic state at Te = 51427.9 with ωe = 169.41, ωexe = 0.941, ωeye = +0.0022 which was to represent the Cordes absorption bands from 1950 to 1795 Cordes, 1935. Following Mulliken, 1971, Mulliken, 1971, we consider these bands as part of D ← X. |
13 | Configuration . . . σgπu4πg4σu. |
14 | Suggested upper state of high temperature absorption "continuum" shortward of 3427 (29170 cm-1) |
15 | The G →A' transition has been observed to lase strongly when mixtures of HI or CF3I or CH3I with argon (1000 - 4000 torr), are excited by a pulsed high current electron beam Hays, Hoffman, et al., 1976. See also H → B footnote 3. |
16 | Repulsive state from 2P3/2 + 2P1/2 responsible for a weak but broad absorption continuum with maximum at 2700 (37000 cm-1). 38 |
17 | Repulsive state from 2P3/2 + 2P3/2, responsible for absorption continuum with maximum at 20050 cm-1 and for the predissociation of B 3Π0+u. |
18 | f values based on magnetic circular dichroism spectra have been estimated as 0.0018 (B"←X) and 0.009 (B ←X) and have been compared with earlier results Brith, Rowe, et al., 1975. For a comparison of theoretical and observed intensities in the B → X resonance series see Zare, 1964. |
19 | Configuration . . . σg2πu4πg3σu. |
20 | Repulsive state from 2P3/2 + 2P3/2. The previous assignment of B' as the state responsible for the magnetic field induced predissociation of B is now in doubt; See 23. |
21 | -0.00178(v +1/2)3 - 0.0000738(v+1/2)4 + 0.00000103(v+1/2)5, from levels with 4≤v≤50 Barrow and Yee, 1973. |
22 | Somewhat different constants, valid for 4≤v≤77, are given by Wei and Tellinghuisen, 1974, Te = 15768.32, ωe = 126.165, ωexe = 0.8673, ..., Be = 0.028939, αe = 0.0001204, ... (using calculated Dv values); see also Brown, Burns, et al., 1973, Tellinghuisen, 1976. RKR potential curve Barrow and Yee, 1973. For a discussion of the long-range potential and ΔG, Bv values near the dissociation limit see LeRoy and Bernstein, 1971, LeRoy, 1972, Barrow and Yee, 1973, Le Roy, 1973, Yee, 1973, LeRoy, 1974. |
23 | Collision induced predissociation of the B state missing citation; magnetic field induced predissociation Degenkolb, Steinfeld, et al., 1969, Capelle and Broida, 1972, Chapman and Bunker, 1972; spontaneous predissociation Tellinghuisen, 1972; hyperfine predissociation Broyer, Vigue, et al., 1976. The purely radiative lifetime Brewer and Tellinghuisen, 1972, Tellinghuisen, 1972, Broyer, Vigue, et al., 1976, increases smoothly from τ= 0.91 μs at v=7 to approximately τ= 10 μs at the highest observed levels. The measured lifetimes Brewer and Tellinghuisen, 1972, missing citation, Capelle and Broida, 1973, Keller, Broyer, et al., 1973, Paisner and Wallenstein, 1974, Broyer, Vigue, et al., 1975 are considerably reduced by spontaneous predissociation due to rotational and hyperfine mixing with B" 1Π1u, the latter leading to differences in lifetime between ortho and para levels Broyer, Vigue, et al., 1976. Only near v=12 and above v~50 are the actual lifetimes close to the purely radiative ones. The magnetic field-induced predissociation of B 3Π0+u was previously assumed to be caused by B' 3Π0-u, and a potential function for this latter state was derived from magnetic quenching data Chapman and Bunker, 1972, Child, 1973. The recent observation, however, of a quantum interference effect between magnetic and spontaneous predissociations Broyer, Vigue, et al., 1973, Vigue, Broyer, et al., 1974, Vigue, Broyer, et al., 1975 has established that the magnetic predissociation, too, is produced by the B" 1Π1u state. |
24 | gJ varies from -0.059 at low v to -5.45 μN near the dissociation limit; from Hanle effect observations Broyer and Lehmann, 1972, Broyer, Lehmann, et al., 1975, Gouedard, Broyer, et al., 1976, Gouedard, Broyer, et al., 1976, 2. See also Wallenstein, Paisner, et al., 1974. |
25 | -3.36E-7(v+1/2)2 - 4.78E-8(v+1/2)3 + 3.26E-10(v+1/2)4, from levels with 4≤v≤77 Barrow and Yee, 1973. |
26 | For v ≤ 10 Barrow and Yee, 1973. Dv increases rapidly above v=20; for more details see Brown, Burns, et al., 1973, Wei and Tellinghuisen, 1974. |
27 | The continuum joining onto the discrete bands is overlapped by the B"← X continuum. A resolution of these two continua and the A ←X continuum was given by Tellinghuisen, 1973,. See also Tellinghuisen, 1973, 2. |
28 | The hyperfine structure of several lines has been observed by various high resolution laser techiques; electric quadrupole, magnetic octupole, and other magnetic hfs constants have been evaluated Hanes and Dahlstrom, 1969, Kroll, 1969, Hansch, Levenson, et al., 1971, Hanes, Lapierre, et al., 1971, Sorem, Levenson, et al., 1971, Levenson and Schawlow, 1972, Sorem, Hansch, et al., 1972, Youmans, Hackel, et al., 1973, Ruben, Kukolich, et al., 1973, Bunker and Hanes, 1974, missing citation; similar analyses for 129I2 and 127,129I2 Tesic and Pao, 1975. |
29 | Extrapolated from data with v' ≥ 4. The vibrational numbering, changed Steinfeld, Zare, et al., 1965, by 1 from the previous table in MOLSPEC 1, has been confirmed by isotope studies Brown and James, 1965. |
30 | Tellinghuisen, 1973, suggests that the v'=4 numbering of Brown, 1931, may have to be raised substantially. Preliminary results of a rotational analysis Ashby, 1975, of nine bands in the A ←X, v"=5 progression and of three bands in the v"=4 progression indicate that w' ~ 57.5 Ashby, 1975, w'x' ~ 1.85 Ashby, 1975, B'(for the lowest analyzed level) = 0.02375 Ashby, 1975, α' ~ 0.0005 Ashby, 1975. |
31 | The continuum joining onto the discrete bands has been studied by many investigators, most recently by Tellinghuisen, 1973, who derives an f value of f= 0.00062 Tellinghuisen, 1973; see also Brith, Rowe, et al., 1975. |
32 | Suggested as lower state of high temperature absorption bands near 3427 Mulliken, 1971 Mulliken, 1971. |
33 | These constants Barrow and Yee, 1973, represent the levels v=0-5; Wei and Tellinghuisen, 1974, for v=0-6, give ωe = 214.582, ωexe = 0.6243, Be = 0.037363, αe = 0.0001145 using calculated Dv values. On the basis of the resonance series of Rank and Baldwin, 1951, Rank and Rao, 1964 and Verma, 1960, LeRoy, 1970 has given polynomial formulae for G(v), Bv, and Dv valid up to v = 82; ωe = 214.548, ωexe = 0.6163 , ...Be = 0.037395, αe = 0.0001244, ... ,De = 4.54E-9, βe = 0.017E-9;... The most accurate constants for v = 0 were derived Gerstenkorn, Luc, et al., 1977 from the analysis by means of Fourier transform spectroscopy of the B←X, 30-0 bands: B0 = 0.0373115, D0 = 4.55E-9, H0 = -0.76E-15. The vibrational levels of the ground state have been observed up to v = 84 [D → X resonance series Verma, 1960], i.e. to within 400 cm-1 of the dissociation limit. The levels v" = 98...115 originally reported by Verma, 1960, were found to be due to an NO impurity Verma and LeRoy, 1974. As a consequence the RKR potential function of Verma, 1960, must be corrected at high v. The RKR curves of Zare, 1964 and LeRoy, 1970 extend only to v = 82 and are unaffected by this correction. 35 see 33. |
34 | gJ(v=0, J=12,14)=9.l3E-4 μN Solarz and Levy, 1972 from non-linear level crossing. |
35 | missing note |
36 | Raman sp. 39 |
37 | From the convergence of the vibrational levels in the B 3Π0+u state Barrow, Broyd, et al., 1973, Barrow and Yee, 1973. |
38 | Nature of the upper state (1u) and of the dissociation products confirmed by photofragment spectroscopy Clear and Wilson, 1973. |
39 | High resolution resonance Raman spectra of I2 vapor up to the eleventh overtone (12-0). Raman spectra in rare gas matrices Howard and Andrews, 1974. |
References
Go To: Top, Gas phase thermochemistry data, Reaction thermochemistry data, Gas phase ion energetics data, Ion clustering 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.
Cox, Wagman, et al., 1984
Cox, J.D.; Wagman, D.D.; Medvedev, V.A.,
CODATA Key Values for Thermodynamics, Hemisphere Publishing Corp., New York, 1984, 1. [all data]
Chase, 1998
Chase, M.W., Jr.,
NIST-JANAF Themochemical Tables, Fourth Edition,
J. Phys. Chem. Ref. Data, Monograph 9, 1998, 1-1951. [all data]
Taylor, Asmis, et al., 1999
Taylor, T.R.; Asmis, K.R.; Zanni, M.T.; Neumark, D.M.,
Characterization of the I-3 radical by anion photoelectron spectroscopy,
J. Chem. Phys., 1999, 110, 16, 7607-7609, https://doi.org/10.1063/1.478672
. [all data]
Do, Klein, et al., 1997
Do, K.; Klein, T.P.; Pommerening, C.A.; Sunderlin, L.S.,
A New Flowing Afterglow-Guided Ion Beam Tandem Mass Spectrometer. Applications to the Thermochemistry of Polyiodide Ions,
J. Am. Soc. Mass Spectrom., 1997, 8, 7, 688, https://doi.org/10.1016/S1044-0305(97)00116-5
. [all data]
Finch, Gates, et al., 1977
Finch, A.; Gates, P.N.; Peake, S.J.,
Thermochemistry of polyhalides. III. Cesium and rubidium tetrachloroiodates,
J. Inorg. Nucl. Chem., 1977, 39, 2135. [all data]
Check, Faust, et al., 2001
Check, C.E.; Faust, T.O.; Bailey, J.M.; Wright, B.J.; Gilbert, T.M.; Sunderlin, L.S.,
Addition of Polarization and Diffuse Functions to the LANL2DZ Basis Set for P-Block Elements,
J. Phys. Chem. A,, 2001, 105, 34, 8111, https://doi.org/10.1021/jp011945l
. [all data]
Harel and Adamson, 1986
Harel, Y.; Adamson, A.W.,
J. Phys. Chem., 1986, 90, 6693. [all data]
Rodgers, Golden, et al., 1966
Rodgers, A.S.; Golden, D.M.; Benson, S.W.,
The thermochemistry of the gas phase equilibrium I2 + C3H6 = C3H5I + HI,
J. Am. Chem. Soc., 1966, 88, 3194-3196. [all data]
Cox and Pilcher, 1970
Cox, J.D.; Pilcher, G.,
Thermochemistry of Organic and Organometallic Compounds, Academic Press, New York, 1970, 1-636. [all data]
Golden, Walsh, et al., 1965
Golden, D.M.; Walsh, R.; Benson, S.W.,
The thermochemistry of the gas phase equilibrium I2 + CH4 «=» CH3I + HI and the heat of formation of the methyl radical,
J. Am. Chem. Soc., 1965, 87, 4053-4057. [all data]
Goy and Pritchard, 1965
Goy, C.A.; Pritchard, H.O.,
Kinetics and thermodynamics of the reaction between iodine and methane and the heat of formation of methyl iodide,
J. Phys. Chem., 1965, 69, 3040-3041. [all data]
Nichol and Ubbelohde, 1952
Nichol, R.J.; Ubbelohde, A.R.,
A thermochemical evaluation of bond strengths in some carbon compounds. part II. Bond strengths based on the reaction CH3I + HI = CH4 + I2,
J. Am. Chem. Soc., 1952, 415-421. [all data]
Diogo, Simoni, et al., 1993
Diogo, H.P.; Simoni, J.A.; Minas da Piedade, M.E.; Dias, A.R.; Martinho Simões, J.A.,
J. Am. Chem. Soc., 1993, 115, 2764. [all data]
Toscano, Seligson, et al., 1989
Toscano, P.J.; Seligson, A.L.; Curran, M.T.; Skrobutt, A.T.; Sonnenberger, D.C.,
Inorg. Chem., 1989, 28, 166; ibid. 1989. [all data]
Connor, Zafarani-Moattar, et al., 1982
Connor, J.A.; Zafarani-Moattar, M.T.; Bickerton, J.; El-Saied, N.I.; Suradi, S.; Carson, R.; Al Takkhin, G.; Skinner, H.A.,
Organomet., 1982, 1, 1166. [all data]
Abrams and Davis, 1954
Abrams, A.; Davis, T.W.,
Use of radioactive iodine to determine equilibrium constants in ethylene-iodine-1,2-diiodoethane systems,
J. Am. Chem. Soc., 1954, 76, 5993-59. [all data]
Cutherbertson and Kistiakowsky, 1935
Cutherbertson, G.R.; Kistiakowsky, G.B.,
The thermal equilibrium between ethylene iodide, ethylene and iodine,
J. Chem. Phys., 1935, 3, 631-634. [all data]
Lord, Goy, et al., 1967
Lord, A.; Goy, C.A.; Pritchard, H.O.,
The heats of formation of trifluoromethyl chloride and bromide,
J. Phys. Chem., 1967, 71, 2705-2707. [all data]
Brennan and Ubbelohde, 1956
Brennan, D.; Ubbelohde, A.R.,
A thermochemical evaluation of bond strengths in some carbon compounds. Part IV. Bond-strength differences based on the reaction: RI + HI = RH + I2, where R = p-methoxyphenyl and cyclohexyl,
J. Chem. Soc., 1956, 3011-3016. [all data]
Wu and Rodgers, 1974
Wu, E.; Rodgers, A.S.,
Thermochemistry of gas-phase equilibrium CF3CH3 + I2 = CF3CH2I + HI. The carbon-hydrogen bond dissociation energy in 1,1,1-trifluoroethane and the heat of formation of the 2,2,2-trifluoroethyl radical,
J. Phys. Chem., 1974, 78, 2315-2317. [all data]
Buckley, Ford, et al., 1980
Buckley, G.S.; Ford, W.G.F.; Rodgers, A.S.,
The thermochemistry of the gas phase reaction: CF3CH2Br + I2 = CF3CH2I + IBr. Polarity effects in thermochemistry,
Thermochim. Acta, 1980, 42, 349-355. [all data]
Kolesov and Papina, 1983
Kolesov, V.P.; Papina, T.S.,
Thermochemistry of Haloethanes,
Russ. Chem. Rev., 1983, 52, 425. [all data]
Hartley, Pritchard, et al., 1950
Hartley, K.; Pritchard, H.O.; Skinner, H.A.,
Thermochemistry of metallic alkyls. III.?mercury dimethyl and mercury methyl halides,
Trans. Faraday Soc., 1950, 46, 1019, https://doi.org/10.1039/tf9504601019
. [all data]
Pedley and Rylance, 1977
Pedley, J.B.; Rylance, J.,
Computer Analysed Thermochemical Data: Organic and Organometallic Compounds, University of Sussex, Brigton, 1977. [all data]
Cox and Pilcher, 1970, 2
Cox, J.D.; Pilcher, G.,
Thermochemistry of Organic and Organometallic Compounds
in Academic Press, New York, 1970. [all data]
Adamson, Vogler, et al., 1978
Adamson, A.W.; Vogler, A.; Kunkely, H.; Wachter, R.,
J. Am. Chem. Soc., 1978, 100, 1298. [all data]
Fowell and Mortimer, 1958
Fowell, P.A.; Mortimer, C.T.,
J. Chem. Soc., 1958, 3734.. [all data]
Pedley, Skinner, et al., 1957
Pedley, J.B.; Skinner, H.A.; Chernick, C.L.,
Thermochemistry of metallic alkyls. Part 8.?Tin tetramethyl, and hexamethyl distannane,
Trans. Faraday Soc., 1957, 53, 1612, https://doi.org/10.1039/tf9575301612
. [all data]
Cline and Kistiakowsky, 1937
Cline, J.E.; Kistiakowsky, G.B.,
The gaseous equilibrium of 1,2-diiodobutane, butene-1 and iodine,
J. Chem. Phys., 1937, 5, 990. [all data]
Landrum and Hoff, 1985
Landrum, J.T.; Hoff, C.D.,
J. Organometal. Chem., 1985, 282, 215. [all data]
Nolan, de la Vega, et al., 1988
Nolan, S.P.; de la Vega, R.L.; Mukerjee, S.L.; Gonzalez, A.A.; Zhang, K.; Hoff, C.,
Polyhedron, 1988, 7, 1491. [all data]
Nolan, López de la Vega, et al., 1986
Nolan, S.P.; López de la Vega, R.; Hoff, C.D.,
J. Organometal. Chem., 1986, 315, 187. [all data]
Wu, Pickard, et al., 1975
Wu, E.C.; Pickard, J.M.; Rodgers, A.S.,
Thermochemistry of the gas-phase reaction tetrafluoroethylene + iodine = 1,2-diiodoperfluoroethane. Heat of formation of 1,2-diiodoperfluoroethane and of iodoperfluoroethane,
J. Phys. Chem., 1975, 79, 1078-1081. [all data]
Sunner, 1955
Sunner, S.,
Strain in 6,8-thioctic acid,
Nature (London), 1955, 176, 217. [all data]
Schock and Marks, 1988
Schock, L.E.; Marks, T.J.,
J. Am. Chem. Soc., 1988, 110, 7701. [all data]
Drago, Nozari, et al., 1979
Drago, R.S.; Nozari, M.S.; Klinger, R.J.; Chamberlain, C.S.,
Inorg. Chem., 1979, 18, 1254. [all data]
Graham, Nichol, et al., 1955
Graham, W.S.; Nichol, R.J.; Ubbelohde, A.R.,
A thermochemical evaluation of bond strengths in some carbon compounds. Part III. Bond strengths based on the reactions: (a) Ph·CH2I + HI=Ph·CH3 + I2 and (b) PhI + HI=PhH + I2,
J. Chem. Soc., 1955, 115-121. [all data]
Carson, Carter, et al., 1961
Carson, A.S.; Carter, W.; Pedley, J.B.,
The thermochemistry of reductions caused by lithium aluminium hydride I. The C-I bond dissociation energy in CH3I,
Proc. Roy. Soc. London A, 1961, 260, 550-557. [all data]
Downs and Adams, 1973
Downs, A.J.; Adams, G.J.,
Comprehensive Inorganic Chemistry, J. C. Bailar, H. J. Emeleus, R. Nyholm and A. F. Trotman - Dickerson, ed(s)., Pergamon Press, New York, 1973, 1543. [all data]
Ashcroft, Carson, et al., 1965
Ashcroft, S.J.; Carson, A.S.; Carter, W.; Laye, P.G.,
Thermochemistry of reductions caused by lithium aluminium hydride. Part 3.- The C-halogen bond dissociation energies in ethyl iodine and ethyl bromide,
Trans. Faraday Soc., 1965, 61, 225-229. [all data]
Mortimer, Pritchard, et al., 1952
Mortimer, C.T.; Pritchard, H.O.; Skinner, H.A.,
Thermochemistry of metallic alkyls. Part V - Mercury di-propyl and mercury di-isopropyl,
Trans. Faraday Soc., 1952, 48, 220-229. [all data]
Shum and Benson, 1983
Shum, L.G.S.; Benson, S.W.,
Thermochemnistry and kinetics of the reaction of methyl mercaptan with iodine,
Int. J. Chem. Kinet., 1983, 15, 433-453. [all data]
Solly, Golden, et al., 1970
Solly, R.K.; Golden, D.M.; Benson, S.W.,
Thermochemical properties of iodoacetone. Intramolecular electrostatic interactions in polar molecules,
J. Am. Chem. Soc., 1970, 92, 4653-4656. [all data]
Zanni, Taylor, et al., 1997
Zanni, M.T.; Taylor, T.R.; Greenblatt, J.; Soep, B.; Neumark, D.M.,
Characterization of the I2- Anion Ground State Using Conventional and Femtosecond Photoelectron Spectroscopy,
J. Chem. Phys., 1997, 107, 19, 7613, https://doi.org/10.1063/1.475110
. [all data]
Auerbach, Baeda, et al., 1973
Auerbach, J.; Baeda, A.P.M.; Los, D.J.,
Fragmentation of Negative Ions Formed in Collisions of Alkali Atoms and Halogen Molecules,
Physica, 1973, 64, 1, 134, https://doi.org/10.1016/0031-8914(73)90119-5
. [all data]
Hughes, Lifschitz, et al., 1973
Hughes, B.M.; Lifschitz, C.; Tiernan, T.O.,
Electron affinities from endothermic negative-ion charge-transfer reactions. III. NO, NO2, S2, CS2, Cl2, Br2, I2, and C2H,
J. Chem. Phys., 1973, 59, 3162. [all data]
Chupka, Berkowitz, et al., 1971
Chupka, W.A.; Berkowitz, J.; Gutman, D.,
Electron Affinities of Halogen Diatomic Molecules as Determined by Endoergic Charge Exchange,
J. Chem. Phys., 1971, 55, 6, 2724, https://doi.org/10.1063/1.1676487
. [all data]
DeCorpo and Franklin, 1971
DeCorpo, J.J.; Franklin, J.L.,
Electron affinities of the halogen molecules by dissociative electron attachment,
J. Chem. Phys., 1971, 54, 1885. [all data]
Moutinho, Aten, et al., 1971
Moutinho, A.M.C.; Aten, J.A.; Los, J.,
Temperature dependence of the total cross section for chemi-ionization in ackali halide-galogen collisions,
Physica, 1971, 53, 471. [all data]
Ayala, Wentworth, et al., 1981
Ayala, J.A.; Wentworth, W.E.; Chen, E.C.M.,
Electron attachment to halogens,
J. Phys. Chem., 1981, 85, 768. [all data]
Hubers, Kleyn, et al., 1976
Hubers, M.M.; Kleyn, A.W.; Los, J.,
Ion pair formation in alkali-halogen collisions at high velocities,
Chem. Phys., 1976, 17, 303. [all data]
Cockett, Donovan, et al., 1996
Cockett, M.C.R.; Donovan, R.J.; Lawley, K.P.,
Zero kinetic energy pulsed field ionization (ZEKE-PFI) spectroscopy of electronically and vibrationally excited states of I2+: The A 2Π3/2,u state and a new electronic state, the a 4σ-u state,
J. Chem. Phys., 1996, 105, 3347. [all data]
Cockett, Goode, et al., 1995
Cockett, M.C.R.; Goode, J.G.; Lawley, K.P.; Donovan, R.J.,
Zero kinetic energy photoelectron spectroscopy of Rydberg excited molecular iodine,
J. Chem. Phys., 1995, 102, 5226. [all data]
Carlson, Gerard, et al., 1988
Carlson, T.A.; Gerard, P.; Pullen, B.P.; Grimm, F.A.,
Autoionization from the ione-pair orbitals of molecules containing iodine,
J. Chem. Phys., 1988, 89, 1464. [all data]
Grade and Rosinger, 1985
Grade, M.; Rosinger, W.,
Correlation of electronic structures and stabilities of gaseous FeI2, Fe2I2 and Fe2I4 molecules, solid [FeI2], and iodine adsorbed on [Fe],
Surf. Sci., 1985, 156, 920. [all data]
Grade and Rosinger, 1984
Grade, M.; Rosinger, W.,
A mass spectrometric investigation of iron(II)-iodide,
Ber. Bunsen-Ges. Phys. Chem., 1984, 88, 767. [all data]
Grade, Rosinger, et al., 1984
Grade, M.; Rosinger, W.; Dowben, P.A.,
Core and valence electron binding energies of FeI2 and stabilities of gas phase species,
Ber. Bunsen-Ges. Phys. Chem., 1984, 88, 65. [all data]
Hoareau, Cabaud, et al., 1981
Hoareau, A.; Cabaud, B.; Melinon, P.,
Time-of-flight mass spectroscopy of supersonic beam of metallic vapours: Intensities and appearance potentials of Mx aggregates,
Surf. Sci., 1981, 106, 195. [all data]
Pittermann and Weil, 1980
Pittermann, U.; Weil, K.G.,
Massenspektrometrische Untersuchungen an Silberhalogeniden V: Verdampfung von Silberiodid,
Ber. Bunsen-Ges. Phys. Chem., 1980, 84, 542. [all data]
Higginson, Lloyd, et al., 1973
Higginson, B.R.; Lloyd, D.R.; Roberts, P.J.,
Variable temperature photoelectron spectroscopy. The adiabatic ionization potential of the iodine molecule,
Chem. Phys. Lett., 1973, 19, 480. [all data]
Potts and Price, 1971
Potts, A.W.; Price, W.C.,
Photoelectron spectra of the halogens and mixed halides ICI and lBr,
J. Chem. Soc. Faraday Trans., 1971, 67, 1242. [all data]
Dibeler, Walker, et al., 1971
Dibeler, V.H.; Walker, J.A.; McCulloh, K.E.; Rosenstock, H.M.,
Effect of hot bands on the ionization threshold of some diatomic halogen molecules,
Intern. J. Mass Spectrom. Ion Phys., 1971, 7, 209. [all data]
Venkateswarlu, 1970
Venkateswarlu, P.,
Vacuum ultraviolet spectrum of the iodine molecule,
Can. J. Phys., 1970, 48, 1055. [all data]
Myer and Samson, 1970
Myer, J.A.; Samson, J.A.R.,
Absorption cross section and photoionization yield of I2 between 1050 and 2200 A,
J. Chem. Phys., 1970, 52, 716. [all data]
Kimura, Katsumata, et al., 1981
Kimura, K.; Katsumata, S.; Achiba, Y.; Yamazaki, T.; Iwata, S.,
Ionization energies, Ab initio assignments, and valence electronic structure for 200 molecules
in Handbook of HeI Photoelectron Spectra of Fundamental Organic Compounds, Japan Scientific Soc. Press, Tokyo, 1981. [all data]
Cornford, Frost, et al., 1971
Cornford, A.B.; Frost, D.C.; McDowell, C.A.; Ragle, J.L.; Stenhouse, I.A.,
Photoelectron spectra of the halogens,
J. Chem. Phys., 1971, 54, 2651. [all data]
Morrison, Hurzeler, et al., 1960
Morrison, J.D.; Hurzeler, H.; Inghram, M.G.; Stanton, H.E.,
Threshold law for the probability of excitation of molecules by photon impact. A study of the photoionization efficiencies of Br2, I2, HI, and CH3I,
J. Chem. Phys., 1960, 33, 821. [all data]
Watanabe, 1957
Watanabe, K.,
Ionization potentials of some molecules,
J. Chem. Phys., 1957, 26, 542. [all data]
Comes, Nielsen, et al., 1973
Comes, F.J.; Nielsen, U.; Schwarz, W.H.E.,
Inner electron excitation of iodine in the gaseous and solid phase,
J. Chem. Phys., 1973, 58, 2230. [all data]
Haranath and Rao, 1958
Haranath, P.B.V.; Rao, P.T.,
Band spectra of iodine, chlorine, and bromine in the spectral region 2400-1400 A,
J. Mol. Spectrosc., 1958, 2, 428. [all data]
Cordes, 1935
Cordes, H.,
Das absorptionsspektrum des jodmolekuls im vakuumultraviolett,
Z. Phys., 1935, 97, 603. [all data]
Venkateswarlu, 1951
Venkateswarlu, P.,
The spectrum of iodine excited in the presence of argon,
Phys. Rev., 1951, 81, 821. [all data]
Verma, 1959
Verma, R.D.,
The spectrum of iodine excited in the presence of argon,
Proc. Indian Acad. Sci. Sect. A, 1959, 48, 197. [all data]
Mulliken, 1971
Mulliken, R.S.,
Iodine revisited,
J. Chem. Phys., 1971, 55, 288. [all data]
Skorko, 1933
Skorko, E.,
Absorption bands of iodine vapour at high temperatures,
Nature (London), 1933, 131, 366. [all data]
Haranath and Rao Prasada, 1960
Haranath, P.B.V.; Rao Prasada, T.A.,
The emission band system of iodine in the blue violet,
Indian J. Phys., 1960, 34, 123. [all data]
Wieland, Tellinghuisen, et al., 1972
Wieland, K.; Tellinghuisen, J.B.; Nobs, A.,
The band systems E → B(4000-4360 Å) and F → X(2530-2740 Å) of 127I2 and 129I2, and the corresponding system E = B of Br2 and Cl2,
J. Mol. Spectrosc., 1972, 41, 69. [all data]
Kortum and Friedheim, 1947
Kortum, G.; Friedheim, G.,
Lichtabsorption und molekularzustand des jods in dampf und losung,
Z. Naturforsch. A, 1947, 2, 20. [all data]
Mathieson and Rees, 1956
Mathieson, L.; Rees, A.L.G.,
Electronic states and potential energy diagram of the iodine molecule,
J. Chem. Phys., 1956, 25, 753. [all data]
Oldman, Sander, et al., 1971
Oldman, R.J.; Sander, R.K.; Wilson, K.R.,
Reinterpretation of I2 main visible continuum,
J. Chem. Phys., 1971, 54, 4127. [all data]
Tellinghuisen, 1973
Tellinghuisen, J.,
Resolution of the visible-infrared absorption spectrum of I2 into three contributing transitions,
J. Chem. Phys., 1973, 58, 2821. [all data]
Brown and Burns, 1974
Brown, J.D.; Burns, G.,
The thermal emission of iodine,
Can. J. Phys., 1974, 52, 1862. [all data]
Barrow and Yee, 1973
Barrow, R.F.; Yee, K.K.,
B3Π0u+ - X1Σg+ system of 127I2: rotational analysis and long-range potential in the B3Π0u+| state,
J. Chem. Soc. Faraday Trans. 2, 1973, 69, 684. [all data]
Wei and Tellinghuisen, 1974
Wei, J.; Tellinghuisen, J.,
Parameterizing diatomic spectra: "best" spectroscopic constants for the I2 B = X transition,
J. Mol. Spectrosc., 1974, 50, 317. [all data]
Brown, 1931
Brown, W.G.,
An infrared absorption band system of iodine,
Phys. Rev., 1931, 38, 1187. [all data]
Kiefer and Bernstein, 1972
Kiefer, W.; Bernstein, H.J.,
Vibrational-rotational structure in the resonance Raman effect of iodine vapor,
J. Mol. Spectrosc., 1972, 43, 366. [all data]
Williams, Rousseau, et al., 1974
Williams, P.F.; Rousseau, D.L.; Dworetsky, S.H.,
Resonance fluorescence and resonance Raman scattering: lifetimes in molecular iodine,
Phys. Rev. Lett., 1974, 32, 196. [all data]
Rousseau and Williams, 1974
Rousseau, D.L.; Williams, P.F.,
Discrete and diffuse emission following two-photon excitation of the E state in molecular iodine,
Phys. Rev. Lett., 1974, 33, 1368. [all data]
Tellinghuisen, 1975
Tellinghuisen, J.,
E → B structured continuum in I2,
Phys. Rev. Lett., 1975, 34, 1137. [all data]
Rousseau, 1975
Rousseau, D.L.,
Lifetime of E → B transition in molecular iodine,
J. Mol. Spectrosc., 1975, 58, 481. [all data]
Pringsheim and Rosen, 1928
Pringsheim, P.; Rosen, B.,
Uber die bandesysteme im spektrum des J2-dampfes,
Z. Phys., 1928, 50, 1. [all data]
Kimura and Miyanishi, 1929
Kimura, M.; Miyanishi, M.,
A band absorption spectrum of iodine in an extreme ultra-violet region,
Sci. Pap. Inst. Phys. Chem. Res. Jpn., 1929, 10, 33. [all data]
Nobs and Wieland, 1966
Nobs, A.; Wieland, K.,
The ultraviolet absorption spectrum of iodine (I2) vapour - a forgotten problem of old time spectroscopy,
Helv. Phys. Acta, 1966, 39, 564. [all data]
Verma, 1960
Verma, R.D.,
Ultraviolet resonance spectrum of the iodine molecule,
J. Chem. Phys., 1960, 32, 738. [all data]
McLennan, 1913
McLennan, J.C.,
On a fluorescence spectrum of iodine vapour,
Proc. R. Soc. London A, 1913, 88, 289. [all data]
Tellinghuisen, 1974
Tellinghuisen, J.,
The McLennan bands of I2: a highly structured continuum,
Chem. Phys. Lett., 1974, 29, 359. [all data]
Hays, Hoffman, et al., 1976
Hays, A.K.; Hoffman, J.M.; Tisone, G.C.,
Molecular-iodine laser,
Chem. Phys. Lett., 1976, 39, 353. [all data]
Brith, Rowe, et al., 1975
Brith, M.; Rowe, M.D.; Schnepp, O.; Stephens, P.J.,
The magnetic circular dichroism spectrum of the halogen molecules I2, Br2, Cl2. Resolution of overlapping continua,
Chem. Phys., 1975, 9, 57. [all data]
Zare, 1964
Zare, R.N.,
Calculation of intensity distribution in the vibrational structure of electronic transitions: the B3Π0+u-X1Σ0g+ resonance series of molecular iodine,
J. Chem. Phys., 1964, 40, 1934. [all data]
Brown, Burns, et al., 1973
Brown, J.D.; Burns, G.; Le Roy, R.J.,
Improved spectroscopic data synthesis for I2(B3Π0u+) and predictions of J dependence for B(3Π0u+)-X(1Σg+) transition intensities,
Can. J. Phys., 1973, 51, 1664. [all data]
Tellinghuisen, 1976
Tellinghuisen, J.,
Reassignment of I2 B-X transitions near 5145 Å,
J. Mol. Spectrosc., 1976, 62, 294. [all data]
LeRoy and Bernstein, 1971
LeRoy, R.J.; Bernstein, R.B.,
Dissociation energies and long-range potentials of diatomic molecules from vibrational spacings: the halogens,
J. Mol. Spectrosc., 1971, 37, 109. [all data]
LeRoy, 1972
LeRoy, R.J.,
Dependence of the diatomic rotational constant Bv on the long-range internuclear potential,
Can. J. Phys., 1972, 50, 953. [all data]
Le Roy, 1973
Le Roy, R.J.,
Chapt. 3. Energy levels of a diatomic near dissociation
in Molecular Spectroscopy. Volume 1, Barrow,R.F.; Long,D.A.; Millen,D.J., ed(s)., The Chemical Society, Burlington House, London, W1V 0BN, 1973, 113-175. [all data]
Yee, 1973
Yee, K.K.,
Analysis of RKR long-range potential of the B3Π0u+ state of I2,
Chem. Phys. Lett., 1973, 21, 334. [all data]
LeRoy, 1974
LeRoy, R.J.,
Long-range potential coefficients from RKR turning points: C6 and C8 for B(3Π0u+)-state Cl2, Br2, and I2,
Can. J. Phys., 1974, 52, 246. [all data]
Degenkolb, Steinfeld, et al., 1969
Degenkolb, E.O.; Steinfeld, J.I.; Wasserman, E.; Klemperer, W.,
Vibrational dependence of the magnetic quenching in iodine,
J. Chem. Phys., 1969, 51, 615. [all data]
Capelle and Broida, 1972
Capelle, G.A.; Broida, H.P.,
Magnetic field dependence of I2 B-state lifetimes,
J. Chem. Phys., 1972, 57, 5027. [all data]
Chapman and Bunker, 1972
Chapman, G.D.; Bunker, P.R.,
Magnetic quenching of iodine fluorescence excited by a 6328 Å He/Ne laser,
J. Chem. Phys., 1972, 57, 2951. [all data]
Tellinghuisen, 1972
Tellinghuisen, J.,
Spontaneous predissociation in I2,
J. Chem. Phys., 1972, 57, 2397. [all data]
Broyer, Vigue, et al., 1976
Broyer, M.; Vigue, J.; Lehmann, J.-C.,
Hyperfine predissociation of molecular iodine,
J. Chem. Phys., 1976, 64, 4793. [all data]
Brewer and Tellinghuisen, 1972
Brewer, L.; Tellinghuisen, J.,
Quantum yield for unimolecular dissociation of I2 in visible absorption,
J. Chem. Phys., 1972, 56, 3929. [all data]
Capelle and Broida, 1973
Capelle, G.A.; Broida, H.P.,
Lifetimes and quenching cross sections of I2(B3Π0+u),
J. Chem. Phys., 1973, 58, 4212. [all data]
Keller, Broyer, et al., 1973
Keller, C.; Broyer, M.; Lehmann, J.-C.,
Mesure directe de la duree de vie des facteurs de lande du niveau 3Π0u+, v'=62, J'=27 de la molecule I2,
C.R. Acad. Sci. Paris, Ser. B, 1973, 277, 369. [all data]
Paisner and Wallenstein, 1974
Paisner, J.A.; Wallenstein, R.,
Rotational lifetimes and self-quenching cross sections in the B3Π0u+ state of 127I2,
J. Chem. Phys., 1974, 61, 4317. [all data]
Broyer, Vigue, et al., 1975
Broyer, M.; Vigue, J.; Lehmann, J.C.,
Direct evidence of the natural predissociation of the I2B state through systematic measurements of lifetimes,
J. Chem. Phys., 1975, 63, 5428. [all data]
Child, 1973
Child, M.S.,
Direct inversion of magnetic fluorescence quenching data for the B3Π(0u+) state of iodine,
J. Mol. Spectrosc., 1973, 45, 293. [all data]
Broyer, Vigue, et al., 1973
Broyer, M.; Vigue, J.; Lehmann, J.-C.,
Two unexpected effects concerning perturbations of the B3Π0+u state of molecular iodine,
Chem. Phys. Lett., 1973, 22, 313. [all data]
Vigue, Broyer, et al., 1974
Vigue, J.; Broyer, M.; Lehmann, J.C.,
Quantum interference effect between the magnetic and natural predissociations in the B3Π0+u state of I2. A new experimental proof,
J. Phys. B:, 1974, 7, 158. [all data]
Vigue, Broyer, et al., 1975
Vigue, J.; Broyer, M.; Lehmann, J.-C.,
Predissociation effects in the B3Π0u+ state of iodine,
J. Chem. Phys., 1975, 62, 4941. [all data]
Broyer and Lehmann, 1972
Broyer, M.; Lehmann, J.C.,
Rotational Lande factors in the B3Π0u+ state of iodine,
Phys. Lett. A, 1972, 40, 43. [all data]
Broyer, Lehmann, et al., 1975
Broyer, M.; Lehmann, J.-C.; Vigue, J.,
g Factors and lifetimes in the B state of molecular iodine,
J. Phys. (Paris), 1975, 36, 235. [all data]
Gouedard, Broyer, et al., 1976
Gouedard, G.; Broyer, M.; Vigue, J.; Lehmann, J.C.,
Comment on Lande factors and chemical shifts in molecular iodine,
Phys. Rev. Lett., 1976, 36, 906. [all data]
Gouedard, Broyer, et al., 1976, 2
Gouedard, G.; Broyer, M.; Vigue, J.; Lehmann, J.C.,
Anomalous behaviour of the Lande factors and the chemical shift close to the dissociation limit of the B state of molecular iodine,
Chem. Phys. Lett., 1976, 43, 118. [all data]
Wallenstein, Paisner, et al., 1974
Wallenstein, R.; Paisner, J.A.; Schawlow, A.L.,
Observation of Zeeman quantum beats in molecular iodine,
Phys. Rev. Lett., 1974, 32, 1333. [all data]
Tellinghuisen, 1973, 2
Tellinghuisen, J.,
Continuous absorption below the band convergence limit in the I2 B ← X transition,
J. Chem. Phys., 1973, 59, 849. [all data]
Hanes and Dahlstrom, 1969
Hanes, G.R.; Dahlstrom, C.E.,
Iodine hyperfine structure observed in saturated absorbtion at 633 nm,
Appl. Phys. Lett., 1969, 14, 362. [all data]
Kroll, 1969
Kroll, M.,
Hyperfine structure in the visible molecular-iodine absorption spectrum,
Phys. Rev. Lett., 1969, 23, 631. [all data]
Hansch, Levenson, et al., 1971
Hansch, T.W.; Levenson, M.D.; Schawlow, A.L.,
Complete hyperfine structure of a molecular iodine line,
Phys. Rev. Lett., 1971, 26, 946. [all data]
Hanes, Lapierre, et al., 1971
Hanes, G.R.; Lapierre, J.; Bunker, P.R.; Shotton, K.C.,
Nuclear hyperfine structure in the electronic spectrum of 127I2 by saturated absorption spectroscopy, and comparison with theory,
J. Mol. Spectrosc., 1971, 39, 506. [all data]
Sorem, Levenson, et al., 1971
Sorem, M.S.; Levenson, M.D.; Schawlow, A.L.,
Saturation spectroscopy of molecular iodine using the 5017 Å argon laser line,
Phys. Lett. A, 1971, 37, 33. [all data]
Levenson and Schawlow, 1972
Levenson, M.D.; Schawlow, A.L.,
Hyperfine interactions in molecular iodine,
Phys. Rev. A: Gen. Phys., 1972, 6, 10. [all data]
Sorem, Hansch, et al., 1972
Sorem, M.S.; Hansch, T.W.; Schawlow, A.L.,
Nuclear quadrupole coupling in the 1Σg+ and 3Π0u+ states of molecular iodine,
Chem. Phys. Lett., 1972, 17, 300. [all data]
Youmans, Hackel, et al., 1973
Youmans, D.G.; Hackel, L.A.; Ezekiel, S.,
High-resolution spectroscopy of I2 using laser-molecular-beam techniques,
J. Appl. Phys., 1973, 44, 2319. [all data]
Ruben, Kukolich, et al., 1973
Ruben, D.J.; Kukolich, S.G.; Hackel, L.A.; Youmans, D.G.; Ezekiel, S.,
Laser-molecular beam measurement of hyperfine structure in the I2 spectrum,
Chem. Phys. Lett., 1973, 22, 326. [all data]
Bunker and Hanes, 1974
Bunker, P.R.; Hanes, G.R.,
Nuclear spin-spin coupling in the spectrum of I2 at 6328 Å,
Chem. Phys. Lett., 1974, 28, 377. [all data]
Tesic and Pao, 1975
Tesic, M.; Pao, Y.-H.,
Theoretical assignment of the observed hyperfine structure in the saturated absorption spectra of I2129 and I127I129 vapors in the 633 nm wavelength region,
J. Mol. Spectrosc., 1975, 57, 75. [all data]
Steinfeld, Zare, et al., 1965
Steinfeld, J.I.; Zare, R.N.; Jones, L.; Lesk, M.; Klemperer, W.,
Spectroscopic constants and vibrational assignment for the B3Π0u+ state of iodine,
J. Chem. Phys., 1965, 42, 25. [all data]
Brown and James, 1965
Brown, R.L.; James, T.C.,
Isotopic determination of the vibrational numbering for the B3Π0u+ state of iodine,
J. Chem. Phys., 1965, 42, 33. [all data]
Ashby, 1975
Ashby,
Private communication cited in Huber and Herzberg, 1979, 1975, 337. [all data]
Rank and Baldwin, 1951
Rank, D.H.; Baldwin, W.M.,
Molecular constants of the ground state of the I2 molecule,
J. Chem. Phys., 1951, 19, 1210. [all data]
Rank and Rao, 1964
Rank, D.H.; Rao, B.S.,
Molecular constants of the ground state of I2,
J. Mol. Spectrosc., 1964, 13, 34. [all data]
LeRoy, 1970
LeRoy, R.J.,
Molecular constants and internuclear potential of ground-state molecular iodine,
J. Chem. Phys., 1970, 52, 2683. [all data]
Gerstenkorn, Luc, et al., 1977
Gerstenkorn, S.; Luc, P.; Perrin, A.,
Rotational analysis of the 5350 Å band of iodine by means of Fourier transform spectroscopy,
J. Mol. Spectrosc., 1977, 64, 56. [all data]
Verma and LeRoy, 1974
Verma, R.D.; LeRoy, R.J.,
Comment on the uv resonance spectrum and ground-state dissociation energy of I2,
J. Chem. Phys., 1974, 61, 438. [all data]
Solarz and Levy, 1972
Solarz, R.; Levy, D.H.,
Non-linear level crossing in the X1Σg+ state of iodine,
Chem. Phys. Lett., 1972, 17, 35. [all data]
Barrow, Broyd, et al., 1973
Barrow, R.F.; Broyd, D.F.; Pederson, L.B.; Yee, K.K.,
The dissociation energies of gaseous Br2 and I2,
Chem. Phys. Lett., 1973, 18, 357. [all data]
Clear and Wilson, 1973
Clear, R.D.; Wilson, K.R.,
Assignment of continuous spectra by photofragment spectroscopy: C state of I2,
J. Mol. Spectrosc., 1973, 47, 39. [all data]
Howard and Andrews, 1974
Howard, W.F., Jr.; Andrews, L.,
Matrix Raman spectra of the molecular halogens: resonance Raman spectra of isolated and aggregated I2,
J. Raman Spectrosc., 1974, 2, 447. [all data]
Huber and Herzberg, 1979
Huber, K.P.; Herzberg, G.,
Molecular Spectra and Molecular Structure. IV. Constants of Diatomic Molecules, Van Nostrand Reinhold Company, New York, 1979, 716. [all data]
Notes
Go To: Top, Gas phase thermochemistry data, Reaction thermochemistry data, Gas phase ion energetics data, Ion clustering data, Constants of diatomic molecules, References
- Symbols used in this document:
AE Appearance energy EA Electron affinity IE (evaluated) Recommended ionization energy S°gas,1 bar Entropy of gas at standard conditions (1 bar) ΔfH°gas Enthalpy of formation of gas at standard conditions ΔrG° Free energy of reaction at standard conditions ΔrH° Enthalpy of reaction at standard conditions - Data from NIST Standard Reference Database 69: NIST Chemistry WebBook
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