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14 13 19 86 65 79 80 58 66 47 48 COMPUTATIONAL DETAILS AND THE ACCURACY OF FULLERENE CALCULATIONS All calculations ... stants o were calculated in the framework of the GIAO method [ 20 , 21 ) at the B3LYP / 6-31G * // B3LYP / 6- Fig .
14 13 19 86 65 79 80 58 66 47 48 COMPUTATIONAL DETAILS AND THE ACCURACY OF FULLERENE CALCULATIONS All calculations ... stants o were calculated in the framework of the GIAO method [ 20 , 21 ) at the B3LYP / 6-31G * // B3LYP / 6- Fig .
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Calculated and experimental frequencies of IR- and Raman - active normal modes of fullerene Coo and the carbon skeleton ( C20 ) in dodecahedrane C20H20 C60 C20H20 Vi 6-31G * ( 22 ) 6-31GA 6-316 exp .
Calculated and experimental frequencies of IR- and Raman - active normal modes of fullerene Coo and the carbon skeleton ( C20 ) in dodecahedrane C20H20 C60 C20H20 Vi 6-31G * ( 22 ) 6-31GA 6-316 exp .
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Unfortunately , calculation of the vibrational frequencies of asymmetric structures is impracticable , and the ... H , were calculated in the framework of the GIAO method ( 13 , 14 ) at the B3LYP / 6-31G * // B3LYP / 6-31G * level .
Unfortunately , calculation of the vibrational frequencies of asymmetric structures is impracticable , and the ... H , were calculated in the framework of the GIAO method ( 13 , 14 ) at the B3LYP / 6-31G * // B3LYP / 6-31G * level .
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Vol 49 No 5 | 662 |
Synthesis and XRay Diffraction Characteristics of MMgDyMn206 M Li Na K | 674 |
Synthesis and Crystal Structure | 685 |
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