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BrNCO |
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Bromine and Nitrogen |
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Nuclear
Quadrupole Coupling Constants |
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in Bromine Isocyanate
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Calculation of the
chlorine nqcc's in bromine isocyanate was made on the ro and rz
structures of Hensel et al. [1]. These are compared with the experimental nqcc's [1,2] in Tables 1 - 5. Structure
parameters are given in Table 6.
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In Tables 1 - 5, subscripts a,b,c refer to the
principal axes of the inertia tensor; 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 molecular plane.
Ø (degrees) is the angle between its subscripted
parameters. ETA = (Xxx - Xyy)/Xzz. |
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RMS is the root mean square
difference between calculated and experimental diagonal nqcc's.
RSD is the standard deviation of the residuals of the calibration
of the models for calculation of the nqcc's, which may
be taken as an estimate of the uncertainty in the calculated nqcc's. |
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Table 1. 79Br
nqcc's in BrNCO (MHz). Calculation was made on the molecular ro and rz structures. |
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Calc. / ro
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Calc. / rz |
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Expt. [2] |
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Xaa |
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619.17 |
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619.54 |
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608.41(52) |
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Xbb |
- |
170.26 |
- |
172.03 |
- |
164.16 |
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Xcc |
- |
448.91 |
- |
447.51 |
- |
444.25(26) |
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|Xab| |
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556.49 |
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554.02 |
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549.67(12) |
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RMS |
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7.63 (1.88 %) |
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8.09 (1.99 %) |
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RSD |
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1.58 (0.39 %) |
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1.58 (0.39 %) |
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Xxx |
- |
457.81 |
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457.12 |
- |
449.70(36) |
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Xyy |
- |
448.91 |
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447.51 |
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444.25(26) |
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Xzz |
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906.72 |
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904.63 |
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893.95(46) |
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ETA |
- |
0.0098 |
- |
0.0106 |
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Øz,a |
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27.33 |
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27.23 |
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27.45(1) |
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Øa,BrN |
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28.76 |
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28.72 |
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Øz,BrN |
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1.43 |
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1.49 |
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Table 2. 81Br
nqcc's in BrNCO (MHz). Calculation was made on the molecular ro and rz structures. |
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Calc. / ro
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Calc. / rz |
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Expt. [2] |
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Xaa |
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517.96 |
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518.26 |
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508.49(52) |
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Xbb |
- |
142.92 |
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144.38 |
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132.98 |
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Xcc |
- |
375.05 |
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373.88 |
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375.51(31) |
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|Xab| |
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464.46 |
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462.40 |
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458.60(12) |
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RMS |
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7.93 (2.34 %) |
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8.72 (2.57 %) |
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RSD |
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1.38 (0.40 %) |
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1.38 (0.40 %) |
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Table 3. Bromine
nqcc's in BrNC18O (MHz). Calculation was made on the molecular ro and rz structures. |
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Calc. / ro
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Calc. / rz |
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Expt. [1] |
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Xaa (79Br) |
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609.22 |
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609.66 |
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598.3(14) |
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Xbb |
- |
160.31 |
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162.15 |
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154.15 |
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Xcc |
- |
448.91 |
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447.51 |
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444.14(35) |
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|Xab| |
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563.42 |
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560.95 |
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556.06(25) |
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RMS |
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7.75 (1.94 %) |
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8.26 (2.07 %) |
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RSD |
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1.58 (0.39 %) |
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1.58 (0.39 %) |
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Xaa (81Br) |
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509.67 |
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510.03 |
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500.2(17) |
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Xbb |
- |
134.62 |
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136.15 |
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128.96 |
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Xcc |
- |
375.05 |
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373.88 |
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371.24(43) |
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|Xab| |
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470.25 |
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468.19 |
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464.28(38) |
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RMS |
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6.74 (2.02 %) |
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7.19 (2.16 %) |
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RSD |
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1.38 (0.40 %) |
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1.38 (0.40 %) |
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Table 4. 14N
nqcc's in 79BrNCO (MHz). Calculation was made on the molecular ro and rz structures. |
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Calc. / ro
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Calc. / rz |
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Expt. [2] |
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Xaa |
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3.706 |
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3.755 |
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5.09(78) |
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Xbb |
- |
0.893 |
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0.916 |
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1.64 |
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Xcc |
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2.813 |
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2.840 |
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3.45 |
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|Xab| |
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1.729 |
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1.680 |
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RMS |
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0.98 (29 %) |
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0.94 (28 %) |
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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 |
- |
1.471 |
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1.457 |
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Xyy |
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2.813 |
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2.840 |
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Xzz |
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4.284 |
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4.297 |
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ETA |
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0.313 |
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0.322 |
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Øz,a |
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18.47 |
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17.87 |
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Øa,BrN |
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28.76 |
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28.72 |
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Øz,BrN |
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10.28 |
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10.85 |
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Table 5. 14N
nqcc's in 81BrNCO (MHz). Calculation was made on the molecular ro and rz structures. |
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Calc. / ro
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Calc. / rz |
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Expt. [2] |
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Xaa |
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3.709 |
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3.758 |
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4.75(51) |
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Xbb |
- |
0.896 |
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0.918 |
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1.42 |
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Xcc |
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2.813 |
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2.840 |
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3.33 |
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|Xab| |
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1.726 |
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1.677 |
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RMS |
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0.74 (23 %) |
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0.70 (22 %) |
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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 6. BrNCO. Molecular structure parameters (Å and degrees). |
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ro [1] |
rz [1] |
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BrN |
1.8617(23) |
1.85565(73) |
NC |
1.2166(40) |
1.2224(15) |
CO |
1.1692(13) |
1.16496(53) |
BrNC |
117.38(42) |
117.99(14) |
NCO |
172.33(44) |
173.13(15) |
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ClNCO |
BrNO |
ClNO |
CH3CH2NCO |
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[1] K.D.Hensel, M.E.Lam, and M.C.L.Gerry, J.Mol.Spectrosc. 151,184(1992).
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[2] H.M.Jemson, W.Lewis-Bevan, N.P.C.Westwood, and M.C.L.Gerry, J.Mol.Spectrosc. 118,481(1986). |
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Table of Contents |
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Molecules/Bromine |
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Molecules/Nitrogen |
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BrNCO.html |
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Last
Modified 2 Feb 2008 |
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