Deuterium
- Formula: D2
- Molecular weight: 4.0282035556
- IUPAC Standard InChIKey: UFHFLCQGNIYNRP-VVKOMZTBSA-N
- CAS Registry Number: 7782-39-0
- 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. - Isotopologues:
- Other names: D2; UN 1957
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Gas phase thermochemistry data
Go To: Top, Phase change data, 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.
Quantity | Value | Units | Method | Reference | Comment |
---|---|---|---|---|---|
S°gas,1 bar | 144.96 | J/mol*K | Review | Chase, 1998 | Data last reviewed in March, 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) | 298. to 1000. | 1000. to 2500. | 2500. to 6000. |
---|---|---|---|
A | 32.684534 | 20.123015 | 46.787245 |
B | -14.841301 | 15.023850 | -5.552026 |
C | 21.064857 | -4.776967 | 1.451072 |
D | -7.204633 | 0.593203 | -0.106099 |
E | -0.066534 | 0.670912 | -19.521487 |
F | -9.480583 | -4.449853 | -40.496576 |
G | 187.691048 | 168.515874 | 178.087513 |
H | 0.0 | 0.0 | 0.0 |
Reference | Chase, 1998 | Chase, 1998 | Chase, 1998 |
Comment | Data last reviewed in March, 1977; New parameter fit October 2001 | Data last reviewed in March, 1977; New parameter fit October 2001 | Data last reviewed in March, 1977; New parameter fit October 2001 |
Phase change data
Go To: Top, Gas phase thermochemistry data, 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: Thermodynamics Research Center, NIST Boulder Laboratories, Chris Muzny director
Quantity | Value | Units | Method | Reference | Comment |
---|---|---|---|---|---|
Ttriple | 18.73 | K | N/A | McConville and Pavese, 1988 | Uncertainty assigned by TRC = 0.0005 K; for normal D2 Temp. on IPTS-678, reproducible to 0.0002 K |
Ttriple | 18.69 | K | N/A | McConville and Pavese, 1988 | Uncertainty assigned by TRC = 0.0005 K; for equilibrium D2 Temp. on IPTS-678, reproducible to 0.0002 K |
Ttriple | 18.65 | K | N/A | Clusius and Weigand, 1940 | Uncertainty assigned by TRC = 0.2 K; see property X for dP/dT for c-l equil. |
Reaction thermochemistry data
Go To: Top, Gas phase thermochemistry data, Phase change 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
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.
Individual Reactions
Quantity | Value | Units | Method | Reference | Comment |
---|---|---|---|---|---|
ΔrH° | 1683.2 | kJ/mol | N/A | Shiell, Hu, et al., 2000 | gas phase; exact: 402.258±0.003 kcal/mol at 298K. Acid: D2; B |
ΔrH° | 1678.663 ± 0.042 | kJ/mol | D-EA | Lykke, Murray, et al., 1991 | gas phase; Reported: 6086.2±0.6 cm-1. Acid taken as HD -> H+ + D-; B |
ΔrH° | 1683.2 | kJ/mol | D-EA | Lykke, Murray, et al., 1991 | gas phase; Acid: D2 -> D- + D+. BDE: 105.98 Gurvich, Veyts, et al.. ΔSacid 22.9; B |
Quantity | Value | Units | Method | Reference | Comment |
ΔrG° | 1652.5 ± 0.46 | kJ/mol | H-TS | Lykke, Murray, et al., 1991 | gas phase; Reported: 6086.2±0.6 cm-1. Acid taken as HD -> H+ + D-; B |
ΔrG° | 1654.8 ± 0.42 | kJ/mol | H-TS | Lykke, Murray, et al., 1991 | gas phase; Acid: D2 -> D- + D+. BDE: 105.98 Gurvich, Veyts, et al.. ΔSacid 22.9; B |
By formula: (D3+ • 9D2) + D2 = (D3+ • 10D2)
Quantity | Value | Units | Method | Reference | Comment |
---|---|---|---|---|---|
ΔrH° | 3. | kJ/mol | PHPMS | Hiraoka and Mori, 1989 | gas phase; Entropy change calculated or estimated; M |
Quantity | Value | Units | Method | Reference | Comment |
ΔrS° | 84. | J/mol*K | N/A | Hiraoka and Mori, 1989 | gas phase; Entropy change calculated or estimated; M |
By formula: (D3+ • 2D2) + D2 = (D3+ • 3D2)
Quantity | Value | Units | Method | Reference | Comment |
---|---|---|---|---|---|
ΔrH° | 14.0 ± 0.8 | kJ/mol | PHPMS | Hiraoka and Mori, 1989 | gas phase; M |
Quantity | Value | Units | Method | Reference | Comment |
ΔrS° | 83.7 | J/mol*K | PHPMS | Hiraoka and Mori, 1989 | gas phase; M |
By formula: (D3+ • 3D2) + D2 = (D3+ • 4D2)
Quantity | Value | Units | Method | Reference | Comment |
---|---|---|---|---|---|
ΔrH° | 7.7 ± 0.4 | kJ/mol | PHPMS | Hiraoka and Mori, 1989 | gas phase; M |
Quantity | Value | Units | Method | Reference | Comment |
ΔrS° | 76.1 | J/mol*K | PHPMS | Hiraoka and Mori, 1989 | gas phase; M |
By formula: (D3+ • 4D2) + D2 = (D3+ • 5D2)
Quantity | Value | Units | Method | Reference | Comment |
---|---|---|---|---|---|
ΔrH° | 7.6 ± 0.4 | kJ/mol | PHPMS | Hiraoka and Mori, 1989 | gas phase; M |
Quantity | Value | Units | Method | Reference | Comment |
ΔrS° | 79.9 | J/mol*K | PHPMS | Hiraoka and Mori, 1989 | gas phase; M |
By formula: (D3+ • 5D2) + D2 = (D3+ • 6D2)
Quantity | Value | Units | Method | Reference | Comment |
---|---|---|---|---|---|
ΔrH° | 7.3 ± 0.4 | kJ/mol | PHPMS | Hiraoka and Mori, 1989 | gas phase; M |
Quantity | Value | Units | Method | Reference | Comment |
ΔrS° | 91.2 | J/mol*K | PHPMS | Hiraoka and Mori, 1989 | gas phase; M |
By formula: (D3+ • 6D2) + D2 = (D3+ • 7D2)
Quantity | Value | Units | Method | Reference | Comment |
---|---|---|---|---|---|
ΔrH° | 3.8 ± 0.4 | kJ/mol | PHPMS | Hiraoka and Mori, 1989 | gas phase; M |
Quantity | Value | Units | Method | Reference | Comment |
ΔrS° | 53.6 | J/mol*K | PHPMS | Hiraoka and Mori, 1989 | gas phase; M |
By formula: (D3+ • 7D2) + D2 = (D3+ • 8D2)
Quantity | Value | Units | Method | Reference | Comment |
---|---|---|---|---|---|
ΔrH° | 3.4 ± 0.4 | kJ/mol | PHPMS | Hiraoka and Mori, 1989 | gas phase; M |
Quantity | Value | Units | Method | Reference | Comment |
ΔrS° | 64.0 | J/mol*K | PHPMS | Hiraoka and Mori, 1989 | gas phase; M |
By formula: (D3+ • 8D2) + D2 = (D3+ • 9D2)
Quantity | Value | Units | Method | Reference | Comment |
---|---|---|---|---|---|
ΔrH° | 3.0 ± 0.4 | kJ/mol | PHPMS | Hiraoka and Mori, 1989 | gas phase; M |
Quantity | Value | Units | Method | Reference | Comment |
ΔrS° | 81.2 | J/mol*K | PHPMS | Hiraoka and Mori, 1989 | gas phase; M |
By formula: (D3+ • D2) + D2 = (D3+ • 2D2)
Quantity | Value | Units | Method | Reference | Comment |
---|---|---|---|---|---|
ΔrH° | 14.6 ± 0.8 | kJ/mol | PHPMS | Hiraoka and Mori, 1989 | gas phase; M |
Quantity | Value | Units | Method | Reference | Comment |
ΔrS° | 74.9 | J/mol*K | PHPMS | Hiraoka and Mori, 1989 | gas phase; M |
By formula: D3+ + D2 = (D3+ • D2)
Quantity | Value | Units | Method | Reference | Comment |
---|---|---|---|---|---|
ΔrH° | 30. ± 1. | kJ/mol | PHPMS | Hiraoka and Mori, 1989 | gas phase; M |
Quantity | Value | Units | Method | Reference | Comment |
ΔrS° | 78.7 | J/mol*K | PHPMS | Hiraoka and Mori, 1989 | gas phase; M |
By formula: Co+ + D2 = (Co+ • D2)
Enthalpy of reaction
ΔrH° (kJ/mol) | T (K) | Method | Reference | Comment |
---|---|---|---|---|
71.5 (+6.7,-0.) | CID | Haynes and Armentrout, 1996 | gas phase; guided ion beam CID; M |
Constants of diatomic molecules
Go To: Top, Gas phase thermochemistry data, Phase change data, Reaction thermochemistry 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 November, 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 |
---|---|---|---|---|---|---|---|---|---|---|---|---|
u 3Πu 6pπ | 122365.6 | 1649.03 | 35.13 1 | 0.627 | 15.036 | 0.587 2 | 0.008 | 0.0053 | 1.0551 | u → a | 26286.75 | |
↳Cunningham and Dieke, 1950 | ||||||||||||
w (3Πg) 5dπ 3 | w → c | |||||||||||
↳Cunningham and Dieke, 1950 | ||||||||||||
q (3Σg+) 5dσ 3 | q → c | |||||||||||
↳Cunningham and Dieke, 1950 | ||||||||||||
n 3Πu 5pπ | 120976.9 | 1652.73 | 34.25 4 | 0.627 | 15.040 5 | 0.560 6 | 0.035 | 0.0053 | 1.0550 | n → a | 24900.14 | |
↳Cunningham and Dieke, 1950 | ||||||||||||
State | Te | ωe | ωexe | ωeye | Be | αe | γe | De | βe | re | Trans. | ν00 |
r 3Πg 4dπ | [(119380)] | 7 8 | r → c R | (22650) 7 | ||||||||
↳Cunningham and Dieke, 1950 | ||||||||||||
p 3Σg+ 4dδ | [119242] | p → c R | 22509.9 7 | |||||||||
↳Cunningham and Dieke, 1950 | ||||||||||||
k 3Πu 4pπ | 118396.7 | 1658.85 | 33.88 9 | 0.508 | 15.075 10 | 0.566 11 | 0.008 | 0.0046 | 1.0538 | k → a | 22323.06 | |
↳Cunningham and Dieke, 1950 | ||||||||||||
f 3Σu+ 4pσ | 116640 | 1618 | 32.8 | 14.66 | 0.62 | 1.069 | f → a R | 20546.0 | ||||
↳Cunningham and Dieke, 1950 | ||||||||||||
State | Te | ωe | ωexe | ωeye | Be | αe | γe | De | βe | re | Trans. | ν00 |
j 3Δg 3dδ | [114194.1] | 7 | j → c V | 17462.3 7 | ||||||||
↳Cunningham and Dieke, 1950 | ||||||||||||
i 3Πg 3dπ | (113093) | [1541.9] | 7 12 | i → e R | 5320.0 13 | |||||||
↳missing citation | ||||||||||||
i → c R | 17131.9 13 | |||||||||||
↳Cunningham and Dieke, 1950 | ||||||||||||
g 3Σg+ 3dσ | (112856) | [1511.3] | 7 | g → e R | 5067.8 | |||||||
↳missing citation | ||||||||||||
g → c R | 16879.8 | |||||||||||
↳Cunningham and Dieke, 1950 | ||||||||||||
State | Te | ωe | ωexe | ωeye | Be | αe | γe | De | βe | re | Trans. | ν00 |
d 3Πu 3pπ | 112729.8 14 | 1678.22 15 | 32.94 16 | 0.24 | 15.200 15 | 0.5520 | [0.0049] | 1.0494 | d → a R | 16666.0 | ||
↳Dieke, 1935 | ||||||||||||
e 3Σu+ 3pσ | 107774.0 | 1556.64 | 34.51 17 | 0.287 | 13.856 | 0.451 | [0.004] | 1.0991 | e → a R | 11649.1 | ||
↳Dieke, 1935, 2 | ||||||||||||
a 3Σg+ 2sσ | 95958.08 18 | 1885.84 | 35.96 18 | 0.34 | 17.109 | 0.606 | [0.0055] | 0.9891 | a → b 19 | |||
(a-X) | 95348.18 20 | |||||||||||
↳Dieke, 1935 | ||||||||||||
State | Te | ωe | ωexe | ωeye | Be | αe | γe | De | βe | re | Trans. | ν00 |
c 3Πu 2pπ | [96731.8] | [15.305] 21 | [0.00514] 21 | [1.0458] | c-X 22 | 95185.3 23 | ||||||
↳Cunningham and Dieke, 1950 | ||||||||||||
b 3Σu+ 2pσ | Lower state of continuous spectrum of D2 (a → b). | |||||||||||
Rydberg | Ionization continua joining on to Rydberg series. 24 | |||||||||||
v'=0 Rydberg series of rotational levels observed in low temperature absorption from X 1Σg+ (v=0) and converging to: | ||||||||||||
Rydberg 25 | R(0) lines (ortho-D2) | |||||||||||
↳Takezawa and Tanaka, 1975 | ||||||||||||
State | Te | ωe | ωexe | ωeye | Be | αe | γe | De | βe | re | Trans. | ν00 |
Rydberg 26 | Q(1) lines (para-D2) | |||||||||||
↳Takezawa and Tanaka, 1975 | ||||||||||||
Rydberg 27 | R(0) lines (ortho-D2) | |||||||||||
↳Takezawa and Tanaka, 1975 | ||||||||||||
B bar 1Σu+ | see 1H2 | |||||||||||
↳Dabrowski and Herzberg, 1974; Chupka, Dehmer, et al., 1975; Kolos, 1976 | ||||||||||||
D" 1Πu 5pπ | 121227.5 28 | 1648.68 28 | 33.638 28 29 | 0.3034 | 15.133 30 31 | 0.6521 30 | 0.01329 | [0.00704] 30 | 0.01329 | 1.0517 | D" ← X R | 120497.0 28 |
↳Monfils, 1965; Monfils, 1968; Takezawa and Tanaka, 1975 | ||||||||||||
State | Te | ωe | ωexe | ωeye | Be | αe | γe | De | βe | re | Trans. | ν00 |
D' 1Πu 4pπ | 118887.9 28 | 1653.15 28 | 33.35 28 32 | 0.226 | 15.041 33 31 | 0.5508 33 | 0.00503 | [0.00323] 33 | 1.0550 | D' ← X R | 118159.7 28 | |
↳Monfils, 1965; Monfils, 1968; Takezawa and Tanaka, 1975 | ||||||||||||
B" 1Σu+ 4pσ | 117970.7 | 1563.02 | 35.416 34 | 0.0843 | 13.685 31 | 0.3842 35 | 0.00024 | 1.1060 | B" ← X R | 117196.9 | ||
↳Monfils, 1965; Monfils, 1968; Takezawa and Tanaka, 1975 | ||||||||||||
M 1Σg+ | [114504.5] 36 | [4.0] | [2.06] | M → B R | 22324.2 | |||||||
↳Dieke and Lewis, 1937 | ||||||||||||
D 1Πu 3pπ | 113914.0 | 1667.60 | 33.343 37 | 15.11 38 31 | 0.54 39 | 0.005 39 | -0.002 | 1.053 | D ← X R | 113193.0 40 | ||
↳Monfils, 1965; Monfils, 1968 | ||||||||||||
State | Te | ωe | ωexe | ωeye | Be | αe | γe | De | βe | re | Trans. | ν00 |
I 1Πg 3dπ | 113081.5 | 1600.14 | 39.42 | 14.739 41 42 | 0.526 41 | [0.0025] 41 | 1.0657 | I → B V | 21691.4 43 | |||
↳Dieke and Lewis, 1937 | ||||||||||||
G 1Σg+ 3dσ | (112893) | [1440.8] | 44 45 | G → B R | 21433.2 | |||||||
↳Dieke and Lewis, 1937 | ||||||||||||
K (1Σg+) | (112610) | [1660] | [6.6] | [1.59] | K → B | (21260) 46 | ||||||
↳Dieke and Lewis, 1937 | ||||||||||||
B' 1Σu+ 3pσ | 111642.2 47 | 1451.98 | 45.679 48 | 2.096 | 13.605 31 | 0.920 49 | [0.00415] 50 | 1.1092 | B' ← X R | 110815.65 | ||
↳Monfils, 1965; Monfils, 1968; missing citation | ||||||||||||
State | Te | ωe | ωexe | ωeye | Be | αe | γe | De | βe | re | Trans. | ν00 |
F 1Σg+ 2pσ2 | (100931.2) 51 | [859.1] 52 | 53 | 53 | F → B R | |||||||
↳Dieke and Cunningham, 1965 | ||||||||||||
E 1Σg+ 2sσ | 100128.1 | 1784.42 | 48.105 | 16.3696 | 0.6764 | [0.0054] | 1.01124 | E → N V | 8827.99 | |||
↳Dieke and Cunningham, 1965 | ||||||||||||
C 1Πu 2pπ | 100097.2 54 | 1729.92 | 34.917 55 | 0.2612 | 15.6731 56 | 0.5679 57 | 0.00532 58 | 1.03346 | CX ↔ 59 R | 99409.18 60 | ||
↳missing citation; missing citation | ||||||||||||
B 1Σu+ 2pσ | 91697.2 54 | 963.08 | 11.038 61 | 10.0680 56 | 0.4198 62 | 0.00403 63 | 1.28944 | B ↔ X 64 65 R | 90633.79 | |||
↳missing citation; missing citation; missing citation | ||||||||||||
State | Te | ωe | ωexe | ωeye | Be | αe | γe | De | βe | re | Trans. | ν00 |
X 1Σg+ 1sσ2 | 0 | 3115.50 | 61.82 66 | 0.562 | 30.4436 67 | 1.0786 68 | 0.01141 69 | 0.74152 | ||||
↳Brannon, Church, et al., 1968 | ||||||||||||
Field- and pressure-induced sp. 70 | ||||||||||||
↳Watanabe and Welsh, 1965; Reddy and Kuo, 1971; Russell, Reddy, et al., 1974 | ||||||||||||
Raman sp. | ||||||||||||
↳Stoicheff, 1957 | ||||||||||||
Rf magn. Reson. sp. 71 | ||||||||||||
↳Kolsky, Phipps, et al., 1952; Ramsey, 1956; English and MacAdam, 1970; Code and Ramsey, 1971 |
Notes
1 | Uncertain. |
2 | Uncertain. |
3 | Fragment |
4 | Uncertain. |
5 | Λ-type doubling constant q(v=0) = 0.25 cm-1 Cunningham and Dieke, 1950. |
6 | missing note |
7 | Strongly affected by l-uncoupling, no constants given by Cunningham and Dieke, 1950; ν00 roughly evaluated from their wave number data. See also H2 4 and H2 10. |
8 | Anti-crossings of r 3Πg(v=0,N=2) with G 1Σg+(v=4,N=2) yielding orbital g factors and hyperfine structure Miller, Freund, et al., 1976). |
9 | ωeze = +0.0345. |
10 | Λ-type doubling constant q(v=0) = 0.29 cm-1 Cunningham and Dieke, 1950. |
11 | Uncertain. |
12 | Anti-crossings between i 3Πg(v=1,N=1) and I 1Πg(v=1,N=1) observed by Jost, Lombardi, et al., 1976. |
13 | Refers to Π-(v=0,N=1); Π+(v=0, N=1) is at 5348.9 cm-1 above e 3Σu+(v=0,N=0). The rotational levels are very irregular. |
14 | Microwave optical magnetic resonance induced by electrons Freund and Miller, 1973 gives the following triplet splittings for v=0, N=1 of para-D2: Δ ν10 = 0.04301, Δ ν02 = 0.00656, and of ortho-D2: Δ ν02 = 0.08286, Δ ν21 = 0.00402 cm-1; similar splittings for v=1...5. Freund and Miller, 1973, 2 derive Ae = -0.02809 cm-1. |
15 | Refers to the 3Π- component; 3Π+ is strongly perturbed. The Λ-type doubling is large and irregular missing citation; for v=0, N=1 it is 0.13 cm-1 Freund and Miller, 1973, 2. Breaking-off of P and R branches for v'> 4 on account of predissociation Dieke, 1935; see also Freund and Miller, 1973. |
16 | missing note |
17 | ωeze = -0.04. |
18 | Te takes account of Y00 in both upper (Y'00 = 2.67) and lower state. |
19 | Lifetime τ(v=0,1) = 12.5 ns Smith and Chevalier, 1972. |
20 | From singlet-triplet anti-crossings Jost, Lombardi, et al., 1976, Miller, Freund, et al., 1976. |
21 | From the assignments of Cunningham and Dieke, 1950 in the g-c, i-c, j-c,...bands by evaluating combination differences. |
22 | Lifetime τ(v=0) = 1.02 ms Johnson, 1972, refers to the non-predissociating component c 3Πu- and corresponds to radiative (magnetic dipole) transitions to b 3Σu+; See H2 49. |
23 | From T0 of a 3Σg+ and the ν00 values for the transitions e-a, g-e, and g-c. |
24 | Cross sections for photoionization into the various vibrational levels of D2+ and the adjoining continuum (dissociative photoionization) observed by Villarejo, 1968, Berkowitz and Spohr, 1973 and calculated by Dunn, 1966, Villarejo, 1968, 2, Itikawa, 1973, Ford, Docken, et al., 1975. |
25 | N=2 of D2+: J=1 levels of npπ 1Πu+ (n=6...9, joining on to C, D, D', D")74; ν = 124833 - RD2/(n+0.082)2. |
26 | N=1 of D2+: J=1 levels of npπ 1Πu- (n=6...24, joining on to C, D, D', D")75; ν = 124775.0 - RD2/(n+0.082)2. Similar series with v'=1,2. |
27 | N=0 of D2+: J=1 levels of npσ 1Σu+ (n=5...25,36..45, joining on to B, B', B")74; ν = 124745.55 - RD2/(n-0.203)2. Similar series with v'=1,2. |
28 | Average of Π+ and Π-. |
29 | v=0-5. |
30 | Constants refer to Π-. For Π+ Takezawa and Tanaka, 1975 give Be= 16.198 , αe= 0.6188 ; D0= 0.00785. |
31 | RKR potential functions Monfils, 1968, 2. |
32 | A very small quartic term differs in sign for Π+ and Π- Takezawa and Tanaka, 1975; v=0-7. |
33 | Constants refer to Π-. Π+ is perturbed by B" 1Σu+, particularly for v=3 and 7. After deperturbation, and excluding v = 2,4,8, Takezawa and Tanaka, 1975 obtain Bv(Π+,v=0-10) = 15.336 - 0.4966(v+1/2) - 0.00489(v+1/2)2 Takezawa and Tanaka, 1975; D0(Π+) = 0.00756 Takezawa and Tanaka, 1975. |
34 | ωeye= +0.0843. ωeze = -0.01364; Monfils, 1968 gives slightly different constants. There are strong perturbations which make vibrational constants somewhat ambiguous. |
35 | Strong rotational perturbations in v=4, weaker ones in v=3, 5, and 9 caused by D' 1Πu+ Takezawa and Tanaka, 1975. |
36 | v=0(?) only, fragmentary. |
37 | ωexe= +0.1698(v+1/2)3 + 0.00296(v+1/2)4 - 0.000307(v+1/2)5: the vibrational constants refer to the average of Π+ and Π- Monfils, 1968. |
38 | Strong predissociation for v≥4, not yet studied in detail but Comes and Schumpe, 1971 observe line widths of 3.5 cm-1 for J-2, v=4...7 of Π+. Comes and Wenning, 1970 observe Lyα of D in fluorescence as a consequence of predissociation and find a noticeable increase of predissociation when an electric field is applied (field-induced predissociation). Theoretical discussion Fiquet-Fayard and Gallais, 1972. |
39 | Dv irregular; the rotational constants refer to Π-. |
40 | Average of Π+ and Π- extrapolated to J=0. The Λ-type doubling is ΛD= 2.14 cm-1; v=0, J=1 with Π+ above Π-. |
41 | Effective constants for Π-, strongly affected by l-uncoupling. See also I 1Πg of H2. |
42 | Anti-crossings between i 3Πg(v=1,N=1) and I 1Πg(v=1,N=1) observed by Jost, Lombardi, et al., 1976. |
43 | Refers to the J=1 level of 1Π-; the J=1 level of 1Π+ lies 18.7 cm-1 higher. |
44 | Zeeman effect in 0-0 band Dieke, 1954. |
45 | Anti-crossings of r 3Πg(v=0,N=2) with G 1Σg+(v=4,N=2) yielding orbital g factors and hyperfine structure Miller, Freund, et al., 1976. |
46 | Refers to J'=1. |
47 | Takes account of Y00 in both upper and lower state. The Y'00 values for B, C, B' are Y'00(B)= 4.2 cm-1,Y'00(C)= 2.2 cm-1,(Y'00(B')= 5.1 cm-1), respectively, but Y00(B') is uncertain; see comments regarding H2. |
48 | ωeze = -0.294 Dabrowski and Herzberg, 1974, seven-level fit Dabrowski and Herzberg, 1974. Monfils, 1968 gives rather different constants based on a nine-level fit; his ninth level (v=8) disagrees strongly with that of Dabrowski and Herzberg, 1974. |
49 | +0.102(v+1/2)2 - 0.0134(v+1/2)3, seven-level fit Dabrowski and Herzberg, 1974. |
50 | D1 = 0.00371, higher Dv values are irregular. |
51 | From the observed ν60 and the energy of v=6 above the (outer) minimum as calculated by Kolos and Wolniewicz, 1969; see H2. |
52 | Calculated ΔG(1/2) value of the outer minimum of the double-minimum state Kolos and Wolniewicz, 1969; see H2. According to Kolos and Wolniewicz, 1969 the lowest level of the outer minimum is 9190.1 cm-1 above B 1Σu+(v=0), but the v=0...5 levels have not yet been observed. The v=6 level lies just below the potential maximum. |
53 | B6 = 3.5. r6 =2.2. Vibrational numbering of Kolos and Wolniewicz, 1969. The D6 value is large and negative. Higher vibrational levels lie above the potential maximum and have larger Bv values (e.g. B12 = 5.688) corresponding to the fact that for these levels the vibrational motion covers both minima of the E,F state. A few rotational levels of v=4 have been observed. |
54 | Takes account of Y00 in both upper and lower state.The Y'00 values for B, C, B' are Y'00(B)= 4.2 cm-1,Y'00(C)= 2.2 cm-1,(Y'00(B')= 5.1 cm- 1), but Y00(B') is uncertain; see comments regarding H2. Te of C 1Πu and ν00(C-X) both exclude -BΛ2. |
55 | ωeze = -0.00946; the zero-point energy (Y00 = 2.2 included) is 858.46 cm-1. The eight-level fit refers to Π Dabrowski and Herzberg, 1974. All vibrational levels up to v=19 have been observed. The last level lies 50 cm-1 above the dissociation limit confirming the theoretical prediction Kolos and Wolniewicz, 1965 of a maximum in the potential function. |
56 | RKR potential functions Monfils, 1968, 2. |
57 | αv= +0.00419(v+1/2)2 - 0.000101(v+1/2)3 Dabrowski and Herzberg, 1974, eight-level fit referring to 1Πu- Dabrowski and Herzberg, 1974. Several of the 1Πu+ levels are strongly perturbed by B 1Σu+. |
58 | -0.000216(v+1/2) + 0.000011(v+1/2)2. |
59 | Franck-Condon factors from electron energy loss spectra Geiger and Schmoranzer, 1969. Theoretical band oscillator strengths, transition probabilities and photodissociation cross sections Allison and Dalgarno, 1969. |
60 | missing note |
61 | ωexe= +0.4109(v+1/2)3 - 0.0370(v+1/2)4 + 0.00154(v+1/2)5, the zero- point energy (Y00 = 4.2 included) is 483.03 cm-1; eight-level fit Dabrowski and Herzberg, 1974. All vibrational levels up to v=51 have been observed. |
62 | +0.0296(v+1/2)2 - 0.0015(v+1/2)3 Dabrowski and Herzberg, 1974; eight-level fit Dabrowski and Herzberg, 1974. |
63 | -0.000320(v+1/2) + 0.000013(v+1/2)2. |
64 | Selective enhancements of v' = 7 and 9 in Ar-D2 mixtures studied by Takezawa, Innes, et al., 1967. Experimental Franck-Condon factors Geiger and Schmoranzer, 1969, calculated Halmann and Laulicht, 1966. Theoretical band oscillator strengths, transition probabilities, and photodissociation cross sections Allison and Dalgarno, 1969. |
65 | Continuous component of B-X (corresponding to the continuum of X 1Σg+) observed by Dalgarno, Herzberg, et al., 1970. |
66 | ωeze = -0.02286; the zero-point energy (Y00 = 4.13 included) is 1546.49 cm-1. Data from the Raman measurements of Stoicheff, 1957 and the field-induced spectrum of Brannon, Church, et al., 1968 have been combined with the somewhat less accurate VUV results in the least-squares solution (10-level fit) for the vibrational and rotational constants Bredohl and Herzberg, 1973. All vibrational levels have been observed, the last one, v=21, being only 2.1 cm-1 below the dissociation limit Bredohl and Herzberg, 1973. Theoretical values for all bound and quasi-bound levels are given by LeRoy, 1971; see also Kolos and Wolniewicz, 1975. For a discussion of the small differences observed-calculated, see Bunker, 1972, Bredohl and Herzberg, 1973, Dabrowski and Herzberg, 1976. |
67 | According to Ramsey, 1952 the hyperfine levels F=1 and 2 for v=0,J=1 (para-D2) are 0.6609E-5 and 0.4669E-5 cm-1 below the F=0 component. |
68 | +0.01265(v+1/2)2 - 0.00069(v+1/2)3; see 66. As for H2 the Bv curve has a slightly negative curvature at low v. |
69 | -0.000224(v+1/2) - +..., from the data of Stoicheff, 1957, Brannon, Church, et al., 1968, Bredohl and Herzberg, 1973. |
70 | 1-0 and 2-0 bands. |
71 | Nuclear spectrum Kolsky, Phipps, et al., 1952; the rotational spectrum gives the rotational magnetic moment for J=1: 0.44288 μN Ramsey, 1956. Code and Ramsey, 1971 determine spin-rotation and quadrupole interaction constants for J=1,2 and derive the quadrupole moment of D. Polarizability anisotropy α parallel - α perp = 0.2897 Å3 English and MacAdam, 1970. |
72 | 36748.9 cm-1, from the dissociation limit (beginning of continuum) in the B'-X system Herzberg, 1970. The same value has been derived by LeRoy and Barwell, 1975 from the last observed levels in the ground state by relations involving the long-range behavior of the potential function. 36748.2 cm-1 from ab initio calculations Kolos and Wolniewicz, 1975. |
73 | From the Rydberg limits of Takezawa and Tanaka, 1975 after correction for pressure shift Herzberg, 1972. |
74 | See the remarks in H2 52 concerning the corresponding series of H2. Note, however, that an accurate representation using Fano's quantum defect theory has not yet been attempted for D2. |
75 | This series of levels is obtained Takezawa and Tanaka, 1975 from a Rydberg series of Q(1) lines whose limit is at 124715.2 cm-1. A similar series of Q(2) lines with a limit at 124654 cm-1 converges to the N=2 level of D2+; also observed for v=1 and 2. These series, unlike J=1 of npσ, 1Σu+ and npπ, 1Πu+, are essentially unperturbed. |
76 | Franck-Condon factors from electron energy loss spectra Geiger and Schmoranzer, 1969. |
77 | Excludes -BΛ2. |
References
Go To: Top, Gas phase thermochemistry data, Phase change data, Reaction thermochemistry 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.
Chase, 1998
Chase, M.W., Jr.,
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Clusius and Weigand, 1940
Clusius, K.; Weigand, K.,
Melting Curves of the Gases A, Kr, Xe, CH4, CH3D, CD4, C2H4, C2H6, COS, and PH3 to 200 Atmospheres Pressure. The Chane of Volume on Melting,
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Shiell, Hu, et al., 2000
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Cunningham and Dieke, 1950
Cunningham; Dieke,
Johns Hopkins University, Department of Physics, Rpt. NYO-692, 1950, 1. [all data]
Dieke, 1935
Dieke, G.H.,
The triplet 3p complex of the hydrogen molecule,
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Dieke, 1935, 2
Dieke, G.H.,
The 3p3Σ→2s3Σ bands of HD and D2,
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Takezawa and Tanaka, 1975
Takezawa, S.; Tanaka, Y.,
The absorption spectrum of D2 in the vacuum-uv region, Rydberg bands, noσ1Σu+←X1Σg+ and npπ1π←X1Σg+ with n=4-6, and the ionization energy,
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Dabrowski and Herzberg, 1974
Dabrowski, I.; Herzberg, G.,
The absorption spectrum of D2 from 1100 to 840 Å,
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Chupka, Dehmer, et al., 1975
Chupka, W.A.; Dehmer, P.M.; Jivery, W.T.,
High resolution photoionization study of ion-pair formation in H2, HD, and D2,
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Kolos, 1976
Kolos, W.,
Ab initio potential energy curves and vibrational levels for the B", B«macron», and B'1Σu+ states of the hydrogen molecule,
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Monfils, 1965
Monfils, A.,
The absorption spectra of the molecules H2, HD, and D2. Part VI. Rotational analysis of the B', B", D, D', and D" states,
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Monfils, 1968
Monfils, A.,
Absorption spectra of molecules H2, HD, and D2. VII. Vibrational constants of the B, B', B", C, D, D', and D" states,
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Dieke and Lewis, 1937
Dieke, G.H.; Lewis, M.N.,
Bands of HD and D2 ending on the 2p1Σ state,
Phys. Rev., 1937, 52, 100. [all data]
Dieke and Cunningham, 1965
Dieke, G.H.; Cunningham, S.P.,
Bands of D2 and T2 originating from the lowest excited 1Σg states (1sσ)(2sσ)1Σg and (2pσ)21Σg,
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Brannon, Church, et al., 1968
Brannon, P.J.; Church, C.H.; Peters, C.W.,
Electric field induced spectra of molecular hydrogen, deuterium and deuterium hydride,
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Watanabe and Welsh, 1965
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Pressure-induced infrared absorption of gaseous hydrogen and deuterium at low temperatures,
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Reddy and Kuo, 1971
Reddy, S.P.; Kuo, C.Z.,
Collision-induced 1st overtone infrared absorption band of deuterium,
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Russell, Reddy, et al., 1974
Russell, W.E.; Reddy, S.P.; Cho, C.W.,
Collision-induced fundamental band of D2 in D2-He and D2-Ne mixtures at different temperatures,
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Stoicheff, 1957
Stoicheff, B.P.,
High resolution Raman spectroscopy of gases. IX. Spectra of H2, HD, and D2,
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Kolsky, Phipps, et al., 1952
Kolsky, H.G.; Phipps, T.E., Jr.; Ramsey, N.F.; Silsbee, H.B.,
Nuclear radiofrequency spectra of H2 and D2 in high and low magnetic fields,
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Ramsey, 1956
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English and MacAdam, 1970
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Molecular-beam resonance measurement of deuterium polarizability anisotropy,
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Code and Ramsey, 1971
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Molecular-beam magnetic resonance studies of HD and D2,
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Miller, Freund, et al., 1976
Miller, T.A.; Freund, R.S.; Zegarski, B.R.,
A forbidden singlet-triplet anticrossing in D2,
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Jost, Lombardi, et al., 1976
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Freund and Miller, 1973
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Fine structure of ortho- and para-D2 d(3p) 3Πu via microwave optical magnetic resonance induced by electrons,
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Freund and Miller, 1973, 2
Freund, R.S.; Miller, T.A.,
Fine structure of para-H2 d(3p) 3Πu (ν=0-3) via microwave optical magnetic resonance induced by electrons,
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Smith and Chevalier, 1972
Smith, W.H.; Chevalier, R.,
Radiative-lifetime studies of the emission continua of the hydrogen and deuterium molecules,
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Johnson, 1972
Johnson, C.E.,
Lifetime of the c3Πu metastable state of H2, D2, and HD,
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Villarejo, 1968
Villarejo, D.,
Measurement of threshold electrons in the photoionization of H2 and D2,
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Berkowitz and Spohr, 1973
Berkowitz, J.; Spohr, R.,
Comparison of photoelectron intensities and Franck-Condon factors in the photoionization of H2, HD and D2,
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Dunn, 1966
Dunn, G.H.,
Franck-Condon factors for the ionization of H2 and D2,
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Villarejo, 1968, 2
Villarejo, D.,
Vibration-rotation interaction effects in calculated Franck-Condon factors. I. The ionization of H2 and D2,
J. Chem. Phys., 1968, 49, 2523. [all data]
Itikawa, 1973
Itikawa, Y.,
Calculation of the cross sections for the photoionization of H2 and D2 into different vibrational states of the ion,
J. Electron Spectrosc. Relat. Phenom., 1973, 2, 125. [all data]
Ford, Docken, et al., 1975
Ford, A.L.; Docken, K.K.; Dalgarno, A.,
Cross sections for photoionization of vibrationally excited molecular hydrogen,
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Monfils, 1968, 2
Monfils, A.,
Calcul des fonctions potentielles de divers etats signulets excites des molecules H2, HD et D2,
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Comes and Schumpe, 1971
Comes, F.J.; Schumpe, G.,
Einfluss der Rotation auf die Lebensdauer pradissoziierender Molekule,
Z. Naturforsch. A, 1971, 26, 538. [all data]
Comes and Wenning, 1970
Comes, F.J.; Wenning, U.,
Pradissoziation im elektrischen Feld - ein neues Phanomen in der Molekulspektroskopie,
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Fiquet-Fayard and Gallais, 1972
Fiquet-Fayard, F.; Gallais, O.,
Predissociation of H2 and D2 (D1Πu): comparison of calculated and experimental line-widths,
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Dieke, 1954
Dieke, G.H.,
Nouveaux resultats pour le spectre des molecules de l'hydrogene et de ses isotopes,
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Kolos and Wolniewicz, 1969
Kolos, W.; Wolniewicz, L.,
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Kolos and Wolniewicz, 1965
Kolos, W.; Wolniewicz, L.,
Potential-energy curves for the X1Σg+, b3Σu+, and C1Πu states of the hydrogen molecule,
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Geiger and Schmoranzer, 1969
Geiger, J.; Schmoranzer, H.,
Electronic and vibrational transition probabilities of isotopic hydrogen molecules H2, HD, and D2 based on electron energy loss spectra,
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Allison and Dalgarno, 1969
Allison, A.C.; Dalgarno, A.,
Photodissociation of vibrationally excited H2, HD, and D2 by absorption into the continua of the Lyman and Werner systems,
At. Data, 1969, 1, 91. [all data]
Takezawa, Innes, et al., 1967
Takezawa, S.; Innes, F.R.; Tanaka, Y.,
Selective enhancement in hydrogenlike molecules with the rare gases. II. HD and D2 with Ar and Kr,
J. Chem. Phys., 1967, 46, 4555. [all data]
Halmann and Laulicht, 1966
Halmann, M.; Laulicht, I.,
Isotope effects on Franck-Condon factors. V. Electronic transitions of isotopic O2, N2, C2, and H2 molecules,
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Dalgarno, Herzberg, et al., 1970
Dalgarno, A.; Herzberg, G.; Stephens, T.L.,
A new continuous emission spectrum of the hydrogen molecule,
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Bredohl and Herzberg, 1973
Bredohl, H.; Herzberg, G.,
The Lyman and Werner bands of deuterium,
Can. J. Phys., 1973, 51, 867. [all data]
LeRoy, 1971
LeRoy, R.J.,
Eigenvalues and certain expectation values for all bound and quasibound levels of ground-state (X1Σg+)H2, HD, and D2,
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Kolos and Wolniewicz, 1975
Kolos, W.; Wolniewicz, L.,
Improved potential energy curve and vibrational energies for the electronic ground state of the hydrogen molecule,
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Bunker, 1972
Bunker, P.R.,
On the breakdown of the Born-Oppenheimer approximation for a diatomic molecule,
J. Mol. Spectrosc., 1972, 5, 478. [all data]
Dabrowski and Herzberg, 1976
Dabrowski, I.; Herzberg, G.,
The absorption and emission spectra of HD in the vacuum ultraviolet,
Can. J. Phys., 1976, 54, 525. [all data]
Ramsey, 1952
Ramsey, N.F.,
Theory of molecular hydrogen and deuterium in magnetic fields,
Phys. Rev., 1952, 85, 60. [all data]
Herzberg, 1970
Herzberg, G.,
The dissociation energy of the hydrogen molecule,
J.Mol. Spectry., 1970, 33, 147. [all data]
LeRoy and Barwell, 1975
LeRoy, R.J.; Barwell, M.G.,
Ground state D2 dissociation energy from the near-dissociation behavior of rotational level spacings,
Can. J. Phys., 1975, 53, 1983. [all data]
Herzberg, 1972
Herzberg, G.,
Spectroscopic studies of molecular structure,
Science, 1972, 177, 123. [all data]
Notes
Go To: Top, Gas phase thermochemistry data, Phase change data, Reaction thermochemistry data, Constants of diatomic molecules, References
- Symbols used in this document:
S°gas,1 bar Entropy of gas at standard conditions (1 bar) T Temperature Ttriple Triple point temperature ΔrG° Free energy of reaction at standard conditions ΔrH° Enthalpy of reaction at standard conditions ΔrS° Entropy of reaction at standard conditions - Data from NIST Standard Reference Database 69: NIST Chemistry WebBook
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