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Thermodynamic properties of dimethylene urethane
Emel'yanenko V., Turovtsev V., Orlov Y.
of 323-353 K. Thermodynamic functions in the ideal gas state are calculated using the rigid rotator-anharmonic
Thermodynamic functions of lactams in the ideal gas state
Emel'Yanenko V., Turovtsev V., Orlov Y.
physics, using an anharmonic approximation in the range of 298-1500 K with allowance for all known
Thermodynamic properties of dimethylene urethane
Emel'yanenko V., Turovtsev V., Orlov Y.
of 323-353 K. Thermodynamic functions in the ideal gas state are calculated using the rigid rotator-anharmonic
Thermodynamic functions of lactams in the ideal gas state
Emel'Yanenko V., Turovtsev V., Orlov Y.
physics, using an anharmonic approximation in the range of 298-1500 K with allowance for all known
Thermodynamic functions of lactones in the gaseous state
Turovtsev V., Emel’yanenko V., Orlov Y.
rigid rotor—anharmonic oscillator
Thermodynamic functions of lactones in the gaseous state
Turovtsev V., Emel’yanenko V., Orlov Y.
rigid rotor—anharmonic oscillator
МАЛАЯ НУТАЦИЯ СИММЕТРИЧНОГО ГИРОСКОПА: ДВЕ ТОЧКИ ЗРЕНИЯ
Voytik, V.V., Migranov, N.G., Войтик, В. В., Мигранов, Н. Г.
is obtained. In this case, the frequencies of third order Raman oscillations are both the tripled frequency
Thermodynamic properties of 2-methyl lactic acid
Emel'yanenko V., Turovtsev V., Fedina Y., Sikorski P.
of the internal rotation in “rigid rotator – anharmonic oscillator” approximation within temperature interval (298
A study of the electronic structure and properties of the propargyl radical
Turovtsev V., Chernova E., Sitnikov V., Emel’yanenko V., Orlov Y.
≡CH and CH2=C=CH2 are compared. With the use of the rigid rotator-anharmonic oscillator model
A study of the electronic structure and properties of the propargyl radical
Turovtsev V., Chernova E., Sitnikov V., Emel’yanenko V., Orlov Y.
≡CH and CH2=C=CH2 are compared. With the use of the rigid rotator-anharmonic oscillator model

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