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HNCO |
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Deuterium,
Nitrogen, and Oxygen
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Nuclear
Quadrupole Coupling Constants |
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in
Isocyanic Acid |
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2H, 14N, and 17O
nqcc's have been measured in isocyanic acid [1-4]. |
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Calculations of the nqcc's were made
here on the "modified substitution" molecular structure of Yamada [5],
and on the ab initio
equilibrium structure of Demaison et al. [6]. These calculated
nqcc's are compared with the experimental values in Tables 1-6.
Structure parameters are given in Table 7. |
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In Tables 1-6, RMS is the root mean
square difference between calculated and experimental diagonal nqcc's
(percentage of the average of the magnitudes of the experimental
nqcc's). RSD is the calibration residual standard deviation of
the model for calculation of the nqcc's: B3LYP/6-31G(df,3p) for
deuterium, B3PW91/6-311+G(df,pd) for nitrogen, and
B1LYP/6-311++G(3df,3p) and MP4(SDQ)/6-311++G(3df,3pd) for oxygen. |
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Subscripts a,b,c refer to the
principal axes of the inertia tensor, subscripts x,y,z to the principal
axes of the nqcc tensor. The nqcc y-axis is chosen coincident
with the inertia c-axis, these are perpendicular to the plane of the
molecule. Ø (degrees) is the angle between its subscripted
parameters. ETA = (Xxx - Xyy)/Xzz. |
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Table 1. Deuterium nqcc's
in DNCO (kHz). Calculation was made on the
substitution [5] and equilibrium [6] structures. PDF |
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Calc. [5]
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Calc. [6] |
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Expt. [1] |
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Xaa |
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53.2 |
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48.7 |
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57.6(54) |
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Xbb |
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92.6 |
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88.9 |
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84.9(38) |
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Xcc |
- |
145.8 |
- |
137.7 |
- |
142.5(38) |
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|Xab| |
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207.0 |
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194.7 |
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RMS |
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5.5 (5.7 %) |
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6.3 (6.6 %) |
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RSD |
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1.1 (0.9 %) |
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1.1 (0.9 %) |
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Xxx |
- |
135.0 |
- |
126.9 |
- |
136.2 * |
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Xyy |
- |
145.8 |
- |
137.7 |
- |
142.5 |
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Xzz |
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280.8 |
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264.5 |
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278.7 |
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ETA |
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0.038 |
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0.041 |
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0.023 |
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Øz,a |
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47.7 |
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47.95 |
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46.9 |
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Øa,ND |
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49.2 |
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49.46 |
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49.2 |
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Øz,ND |
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1.5 |
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1.51 |
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2.3 |
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* Calculated here from the
experimental diagonal nqcc's and the calculated off-diagonal nqcc of
207.0 kHz. |
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Table 2. 14N nqcc's in DNCO (MHz).
Calculation was made on the substitution [5] and equilibrium
[6] structures. PDF |
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Calc. [5]
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Calc. [6] |
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Expt. [1] |
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Xaa |
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2.138 |
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2.136 |
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2.1237(15) |
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Xbb |
- |
0.569 |
- |
0.530 |
- |
0.5528(18) |
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Xcc |
- |
1.569 |
- |
1.606 |
- |
1.5709(18) |
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|Xab| |
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1.008 |
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1.031 |
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RMS |
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0.012 (0.9 %) |
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0.025 (1.8 %) |
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RSD |
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0.030 (1.3 %) |
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0.030 (1.3 %) |
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Xxx |
- |
0.903 |
- |
0.882 |
- |
0.890 * |
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Xyy |
- |
1.569 |
- |
1.606 |
- |
1.5709 |
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Xzz |
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2.472 |
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2.488 |
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2.461 |
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ETA |
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0.269 |
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0.291 |
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0.277 |
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Øz,a |
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18.3 |
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18.86 |
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18.5 |
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Øa,ND |
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49.2 |
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49.46 |
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49.2 |
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Øz,ND |
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30.8 |
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30.60 |
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30.7 |
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* Calculated here from the
experimental diagonal nqcc's and the calculated off-diagonal nqcc
of 1.008 kHz. |
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Table 3. 14N nqcc's in HNCO (MHz).
Calculation was made on the substitution [5] and
equilibrium [6] structures. |
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Calc. [5]
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Calc. [6] |
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Expt. [2] |
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Xaa |
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2.083 |
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2.080 |
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2.056(11) |
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Xbb |
- |
0.514 |
- |
0.473 |
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0.473 |
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Xcc |
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1.569 |
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1.606 |
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1.583 |
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|Xab| |
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1.078 |
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1.100 |
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RMS |
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0.030 (2.2 %) |
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0.019 (1.4 %) |
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RSD |
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0.030 (1.3 %) |
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0.030 (1.3 %) |
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Table 4. 14N nqcc's in HNC17O
(MHz). Calculation was made on the substitution [5] and
equilibrium [6] structures. |
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Calc. [5]
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Calc. [6] |
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Expt. [3] |
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Xaa |
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2.084 |
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2.080 |
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2.051(13) |
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Xbb |
- |
0.515 |
- |
0.474 |
- |
0.4725(68) |
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Xcc |
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1.569 |
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1.606 |
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1.578 |
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|Xab| |
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1.077 |
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1.100 |
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RMS |
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0.031 (2.3 %) |
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0.023 (1.7 %) |
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RSD |
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0.030 (1.3 %) |
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0.030 (1.3 %) |
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Table 5. 17O nqcc's in HNCO (MHz).
Calculation was made on the substitution [5] and equilibrium
[6] structures. PDF |
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Calc = B1LYP/6-311++G(3df,3p) |
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Calc. [5]
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Calc. [6] |
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Expt. [3] |
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Xaa |
- |
3.284 |
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3.191 |
- |
3.276(24) |
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Xbb |
- |
0.131 |
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0.197 |
- |
0.176(13) |
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Xcc |
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3.415 |
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3.388 |
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3.452 |
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|Xab| |
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0.378 |
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0.399 |
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RMS |
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0.034 (1.5 %) |
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0.063 (2.7 %) |
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RSD |
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0.041 (1.4 %) |
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0.041 (1.4 %) |
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Xxx |
- |
0.086 |
- |
0.145 |
- |
0.133 * |
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Xyy |
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3.415 |
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3.388 |
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3.452 |
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Xzz |
- |
3.328 |
- |
3.243 |
- |
3.319 |
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ETA |
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1.052 |
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1.089 |
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Øz,a |
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6.7 |
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7.47 |
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6.8 |
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Øa,CO |
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1.9 |
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2.02 |
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1.9 |
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Øz,CO |
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4.8 |
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5.44 |
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4.9 |
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* Calculated here from the
experimental diagonal nqcc's and the calculated off-diagonal nqcc
of 0.378 MHz. |
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Table 6. 17O nqcc's in HNCO (MHz).
Calculation was made on the substitution [5] and equilibrium
[6] structures. PDF |
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Calc =
MP4(SDQ)/6-311++G(3df,3pd) |
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Calc. [5]
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Calc. [6] |
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Expt. [3] |
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Xaa |
- |
3.318 |
- |
3.228 |
- |
3.276(24) |
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Xbb |
- |
0.175 |
- |
0.243 |
- |
0.176(13) |
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Xcc |
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3.493 |
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3.471 |
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3.452 |
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|Xab| |
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0.316 |
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0.340 |
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RMS |
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0.034 (1.5 %) |
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0.049 (2.1 %) |
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RSD |
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0.027 (0.93 %) |
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0.027 (0.93 %) |
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Xxx |
- |
0.144 |
- |
0.205 |
- |
0.144 * |
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Xyy |
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3.493 |
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3.471 |
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3.452 |
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Xzz |
- |
3.349 |
- |
3.266 |
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3.309 |
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Øz,a |
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5.7 |
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6.43 |
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5.8 |
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Øa,CO |
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1.9 |
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2.02 |
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1.9 |
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Øz,CO |
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3.8 |
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4.41 |
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3.9 |
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* Calculated here from the
experimental diagonal nqcc's and the calculated off-diagonal nqcc
of 0.316 MHz. |
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Table 7. Molecular
structure parameters, (Å and degrees). |
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rs [5] |
re [6] |
re [7] |
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HN |
0.9946 |
1.0037 |
1.0030(20) |
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NC |
1.2140 |
1.2148 |
1.2145(6) |
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CO |
1.1664 |
1.1641 |
1.1634(4) |
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HNC |
123.9 |
123.444 |
123.34(20) |
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NCO |
172.6 |
172.393 |
172.22(20) |
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[1] N.Heineking, M.C.L.Gerry,
and H.Dreizler, Z.Naturforsch. 44a,577(1989); H.Dreizler,
Z.Naturforsch. 47a,342(1992). |
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[2] W.H.Hocking, M.C.L.Gerry,
and G.Winnewisser, Can.J.Phys. 53,1869(1975). |
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[3] M.C.L.Gerry, S.J.Howard,
N.Heineking, and H.Dreizler, Z.Naturforsch. 44a,1187(1989). |
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[4] S.G.Kukolich, A.C.Nelson,
and B.S.Yamanashi, J.Amer.Chem.Soc. 93,6769(1985). |
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[5] K.Yamada, J.Mol. Spectrosc.
79,323(1980). |
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[6] J.Demaison, L.Margulès,
and J.E.Boggs, Chem.Phys. 260,65(2000). |
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[7] A.L.L.East, C.S.Johnson, and
W.D.Allen, J.Chem.Phys. 98,1299(1993). |
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"Electric and magnetic properties ...
from ab initio CCSD(T)
studies" M.Mladenović, M.Elhiyani, and M.Lewerenz, J.Chem.Phys.
131,034302(2009). |
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L.Fusina and I.M.Mills,
J.Mol.Spectrosc. 86,488(1981): rz structure. |
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ClNCO |
HNCS |
HNCSe |
HNSO |
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Table of Contents |
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Molecules/Deuterium |
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Molecules/Nitrogen |
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Molecules/Oxygen |
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DNCO.html |
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Last
Modified 26 Sept 2009 |
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