2002
DOI: 10.1021/jp020003t
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Rayleigh Depolarization Ratios, Kerr Effects, Polarizabilities, and Hyperpolarizabilities of CH3Br, CH2Br2, CHBr3, and CBr4. Comparison of Experimental and ab Initio Calculated Polarizabilities

Abstract: Improved equipment has been used to record the vapor-phase Rayleigh depolarization ratios and electrooptical Kerr effects of CH 3 Br, CH 2 Br 2 , CHBr 3 , and CBr 4 at elevated temperatures. The measurements yield experimental values of the anisotropic polarizabilities and the Kerr hyperpolarizabilities of these molecules. As well, Dougherty and Spackman's HUZ-SV(+sd+sp) basis set has been used to compute SCF and MP2level polarizabilities, and these are compared with the experimental results.

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Cited by 6 publications
(2 citation statements)
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“…Equipment for investigation of the temperature and pressure dependence of the electrooptical Kerr effect in gases and vapors has also been described . Measurements of the electric field-induced birefringences of CH 3 CH 2 CN and (CH 3 ) 2 CHCN at 632.8 nm were made at 10 temperatures (≈340−500 K) within the available span and, at each temperature, over a range of pressures (≈10−30 kPa).…”
Section: Methodsmentioning
confidence: 99%
“…Equipment for investigation of the temperature and pressure dependence of the electrooptical Kerr effect in gases and vapors has also been described . Measurements of the electric field-induced birefringences of CH 3 CH 2 CN and (CH 3 ) 2 CHCN at 632.8 nm were made at 10 temperatures (≈340−500 K) within the available span and, at each temperature, over a range of pressures (≈10−30 kPa).…”
Section: Methodsmentioning
confidence: 99%
“…Improved equipment for measurements of the temperature and pressure dependence of the electrooptical Kerr effect in gases has been described. , Observations of the field-induced birefringences of NH 3 , CH 3 NH 2 , (CH 3 ) 2 NH, and (CH 3 ) 3 N at 632.8 nm typically were made at 12 temperatures (∼295−495 K) within the available span and, at each temperature, over a range of pressures (∼40−400 kPa). The definition of the molar Kerr constant, m K , is , where n and ε r are the refractive index and relative permittivity of the gas in the absence of the field; n X − n Y is the birefringence for XZ - and YZ -polarized light that is induced by the uniform electric field, F X ; and V m is the molar volume.…”
Section: Methodsmentioning
confidence: 99%