793 research outputs found

    Dr. L.H. Whelchel, ITC, June 27, 2014

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    This video is a conversation with Dr. L.H. Whelchel. Dr. Whelchel talks about his book, "Sherman's March and the Emergence of the Independent Black Church Movement". Brad Ost, AUC Woodruff Library, is the interviewer

    Dr. L.H. Whelchel, ITC, June 2011

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    This video is a conversation with Dr. L.H. Whelchel. Dr. Whelchel talks about his book, "The History and Heritage of African American Churches". Brad Ost, AUC Woodruff Library, is the interviewer

    MAGNETIC SPIN-TORSION COUPLING IN METHANOL

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    The hyperfine structure of non-rigid molecules in which hyperfine coupling arises from equivalent nuclei that can be exchanged by large amplitude motions is of great interest and lead to unexpected results. In the non-rigid (C2_2D2_2)2_2 and (D2_2O)2_2 dimers, the hyperfine structure arising for nondegenerate tunneling sublevels can be accounted for using an effective quadrupole coupling Hamiltonian with the same coupling constant for all four deuterium atoms.footnote{Bhattacharjee, Muenter, and Coudert, {em J. Chem. Phys.}~{bf 97} (1992) 8850; and Stahl and Coudert, {em J. Mol. Spectrosc.}~{bf 157} (1993) 161.} In the non-rigid species CD3_3COH and HCOOCH3_3, the large amplitude torsional motion leads to hyperfine patterns which are qualitatively dependent on the torsional symmetry of the levels.footnote{Coudert and Lopez, {em J. Mol. Spectrosc.}~{bf 239} (2006) 135; and Tudorie, Coudert, Huet, Jegouso, and Sedes, {em J. Chem. Phys.}~{bf 134} (2011) 074314.} The interaction between a large amplitude torsional motion and the hyperfine coupling may also lead to a less known hyperfine effect, the so-called magnetic spin-torsion coupling, which was first studied by Heuvel and Dymanusfootnote{Heuvel and Dymanus, {em J. Mol. Spectrosc.}~{bf 45} (1973) 282 and {em ibid} {bf 47} (1973) 363.} and which has not yet been conclusively evidenced. In this talk, the magnetic hyperfine structure of the non-rigid methanol molecule will be investigated experimentally and theoretically. 13 hyperfine patterns were recorded using two molecular beam microwave spectrometers. These patterns, along with previously recorded ones,c^c were analyzed in an attempt to evidence the effects of the magnetic spin-torsion coupling. The theoretical approach setup to analyze the observed data accounts for the spin-torsion coupling, in addition to the familiar magnetic spin-rotation and spin-spin couplings, and relies on symmetry considerations to build a hyperfine coupling Hamiltonian and a spin-rotation-torsion wavefunction compatible with the Pauli exclusion principle. In the talk, the results of the analysis will be presented. The hyperfine coupling parameters retrieved will be discussed and we hope to be able to conclusively evidence the effects of the magnetic spin-torsion.Made available in DSpace on 2016-01-05T20:05:01Z (GMT). No. of bitstreams: 3 880.pdf: 21667 bytes, checksum: cee968d18f0809b6163765eb21bf4bdd (MD5) 322960.pdf: 393825 bytes, checksum: 7113d44bad0558387e93ca12cf3796a4 (MD5) license.txt: 4813 bytes, checksum: 715c4321821a960fa1a1e91d2ac7ebce (MD5) Previous issue date: 2

    The Microwave Spectrum Of Monodeuterated Acetamide Ch2dc(=o)nh2

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    Acetamide is an oblate asymmetric top displaying almost free internal rotation of its methyl group. The microwave spectrum of the normal species (\chem{CH_3C(=O)NH_2}) has already been studied and a value\footnote{Ilyushin, Alekseev, Dyubko, Kleiner, and Hougen, {\em J.\ Molec.\ Spectrosc.}~{\bf 227} (2004) 115} of only 25~\wn\ was retrieved for the height of the potential barrier hindering the internal rotation. No spectroscopic results are available about the monodeutared species with a partially deuterated \chem{CH_2D} methyl group which will be the subject of the present talk. The effects of deuteration on the hindering potential\footnote{Lauvergnat, Coudert, Klee, and Smirnov, {\em J.\ Molec.\ Spectrosc.}~{\bf 256} (2009) 204} will be investigated first. They lead to qualitative changes of the hindering potential no longer resembling that of the normal species and displaying several inequivalent minima.\footnote{Margul\`es, Coudert, M\o llendal, Guillemin, Huet and Jane\v{c}kov\`a, {\em J.\ Molec.\ Spectrosc.}~{\bf 254} (2009) 55} A determination of the torsional potential will be attempted through an analysis of the microwave spectrum of the monodeuterated species in which torsion-rotation energies are calculated with the approach developed for monodeuterated methanol,\footnote{Coudert, Zemouli, Motiyenko, Margul\`es, and Klee, {\em J.\ Chem.\ Phys.}~{\bf 140} (2014) 064307} accounting for the torsion-rotation Coriolis coupling and for the dependence of the inertia tensor on the torsional angle. A low temperature spectrum, recorded with the MB-FTMW spectrometer in Lille, has already been analyzed and 14 transitions could be assigned up to J=6J=6. Room temperature spectra have also been recorded in the 7--91 and 150--165~GHz frequency ranges and more than 100 transitions have been assigned up to J=16J=16 for the ground torsional state. In the paper, deuteration effects will be discussed and we hope to assign a sufficient number of microwave transitions in order to obtain the first quantitative information about the hindering potential of monodeuterated acetamide.Made available in DSpace on 2014-09-17T16:56:32Z (GMT). No. of bitstreams: 3 license.txt: 4922 bytes, checksum: 910b249b4beec47e7ab768910c8f966f (MD5) 77.pdf: 25428 bytes, checksum: c0f63c160e717e6dc3367a8a84e8acbb (MD5) abstract.txt: 2390 bytes, checksum: 3881b0bdd0fc9325b7bd4f99e0b55abf (MD5) Previous issue date: 2014-06-20Made available in DSpace on 2015-04-14T18:39:02Z (GMT). No. of bitstreams: 4 license.txt: 4922 bytes, checksum: 910b249b4beec47e7ab768910c8f966f (MD5) FA07_Presentation.pptx: 530997 bytes, checksum: b01e074dee48335dc838abf13db788c9 (MD5) FA07_Abstract.pdf: 25428 bytes, checksum: c0f63c160e717e6dc3367a8a84e8acbb (MD5) FA07_Abstract.txt: 2390 bytes, checksum: 3881b0bdd0fc9325b7bd4f99e0b55abf (MD5) Previous issue date: 2014-06-2

    The rotation-torsion spectrum of doubly deuterated methanol cd2hoh

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    Made available in DSpace on 2020-06-26T03:04:23Z (GMT). No. of bitstreams: 2 4265.pdf: 25945 bytes, checksum: c818a1ac9a41d8b37e92c20f39b706b7 (MD5) license.txt: 4802 bytes, checksum: 58353f9dd6876860dd5221f3d7872a95 (MD5) Previous issue date: 22Doubly deuterated methanol CD2_2HOH is a non-rigid molecule displaying internal rotation of its asymmetrical CD2_2H methyl group. Like the isotopic species of methanol with a symmetrical CH3_3 or CD3_3 group, it displays a strong rotation-torsion Coriolis coupling. Unlike these species, it also displays a dependence of its generalized inertia tensor on the angle of internal rotation. Its complicated rotation-torsion spectrum was investigated in the microwave,\footnote{Liu \& Quade, {\em J.\ Mol.\ Spectrosc.}~{\bf 146} (1991) 252; Su, Liu, \& Quade, {\em J.\ Mol.\ Spectrosc.}~{\bf 149} (1991) 557; Quade, Liu, Mukhopadhyay, \& Su, {\em J.\ Mol.\ Spectrosc.}~{\bf 192} (1998) 378; Su \& Quade, {\em J.\ Chem.\ Phys.}~{\bf 90} (1989) 1396} submillimeter-wave,\footnotetext[2]{Ndao, Tchana, Coudert, Motiyenko, Margul\`es, Barros, Manceron, \& Roy, {\em J.\ Mol.\ Spectrosc.}~{\bf 326} (2015) 136}\footnotetext[3]{Mukhopadhyay, {\em Inf.\ Phys.\ Tech.}~{\bf 75} (2016) 139; {\em ibid.}~{\bf 76} (2016) 116}b,c^{b,c} terahertz,b^b and FIRb,c^{b,c} domains. Although more than 3000 transitions have been assigned so far, no global analysis, like the one performed for the similar species CH2_2DOH,\footnotetext[4]{Coudert, Zemouli, Motiyenko, Margul\`es, \& Klee, {\em J.\ Chem.\ Phys.}~{\bf 140} (2014) 064307}d^d has been carried out. In this talk, new assignments in the terahertz and FIR spectra of CD2_2HOH will be reported. Parallel and perpendicular transitions, characterized by a higher KK-value than in our previous investigation,b^b could be identified up to J=35J=35 for the three lowest lying torsional states. Using the theoretical approach developed for CH2_2DOH,d^d a global analysis of the available high-resolution data has been attempted in order to check the new assignments and to retrieve spectroscopic parameters such as those describing the hindering potential and the generalized inertia tensor.\footnotetext[5]{Liu \& Quade, {\em J.\ Mol.\ Spectrosc.}~{\bf 146} (1991) 238; El Hilali, Coudert, Konov, \& Klee, {\em J.\ Chem.\ Phys.}~{\bf 135} (2011) 194309}e^e So far, this global analysis has been restricted to transitions with K4K\geq4 as rotation-torsion levels with K<4K<4 are affected by strong rotation-torsion couplings and cannot be properly modeled. Hopefully this issue will be dealt with by the time of the Symposium

    The bending-rotation approach applied to the methylene radical ch2

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    Made available in DSpace on 2020-06-26T03:04:31Z (GMT). No. of bitstreams: 2 4273.pdf: 21690 bytes, checksum: 1284a731f1e6e20f283c63b1c043bb80 (MD5) license.txt: 4802 bytes, checksum: 58353f9dd6876860dd5221f3d7872a95 (MD5) Previous issue date: 22Quasi-linear molecules display a large amplitude bending mode allowing them to sample their linear configuration. This leads to a strong coupling between the overall rotation and the bending mode and to a singularity in their Hamiltonian. Quasi-linearity has been extensively studied in bent light triatomic molecules like water molecule and the amidogen (NH2_2) and methylene (CH2_2) radicals as they display a low barrier to linearity ranging from 12\,000~cm1^{-1} for NH2_2 to less than 2000~cm1^{-1} for CH2_2.\footnotetext[1]{Jungen, Hallin, \& Merer, {\em Molec.\ Phys.}~{\bf 40} (1980) 25; Bunker, Jensen, Kraemer, \& Beardsworth, {\em J.\ Chem.\ Phys.}~{\bf 85} (1986) 3724; Partridge \& Schwenke, {\em J.\ Chem.\ Phys.}~{\bf 106} (1997) 4618}a^a Their rovibrational energy levels can be computed with almost spectroscopic accuracy using variational approaches or, if a higher accuracy is needed, with reduced dimensionality models such as the effective Bending-Rotation approach,\footnotetext[2]{Coudert, {\em Mol.\ Phys.}~{\bf 96} (1999) 941}b^b already applied to treat the anomalous centrifugal distortion of the water molecule\footnotetext[3]{Yu, Pearson, Drouin, Martin-Drumel, Pirali, Vervloet, Coudert, M\"uller, \& Br\"unken, {\em J.\ Mol.\ Spectrosc.}~{\bf 279} (2012) 16}c^c and the amidogen radical.\footnotetext[4]{TD03, Martin-Drumel, Pirali, \& Coudert, 72nd ISMS, Urbana-Champaign, June 19--23, 2017}d^d In this talk, the Bending-Rotation approachb^b will be tentatively applied to the fitting of high-resolution data pertaining to the vibronic ground state of the methylene radical. The data from previous experimental investigations will be considered in the analysis. Due to the very low barrier to linearitya^a of CH2_2, its rovibrational energy levels are somewhere in between those of a bent molecule and those of a linear molecule leading to anomalous centrifugal distortion.\footnotetext[5]{Br\"unken, M\"uller, Lewen, \& Giesen, {\em J.\ Chem.\ Phys.}~{\bf 123} (2005) 164315}e^e Its rotational energy cannot be computed using the standard approaches developed for semi-rigid molecules. The present analysis will, therefore, provide us with a test for the Bending-Rotation approach.b^b In the talk, we will try to see how well the anomalous centrifugal distortion is taken into account and we will try to retrieve the dependence of the spin-rotation coupling on the bending angle

    Terahertz spectroscopy of deuterated acetaldehyde: CH2DCHO

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    This study follows our recent investigations about deuterated methyl-top species of complex organic molecules: methanol,\footnote{Coudert, L. H.; {\em et al.} {\em J. Chem. Phys.}~{\bf140}, (2014) 64307} methyl formate,\footnote{Coudert, L. H.; {\em et al.} {\em ApJ}~{\bf779}, (2013) 119} and dimethyl ether.\footnote{Richard, C.; {\em et al.} {\em A\&A}~{\bf552}, (2013) A117} In particular these works led the first ISM detection of \chem{HCOOCH_2D} and \chem{CH_2DOCH_3}. Acetaldehyde is not very abundant in the ISM, but this is a very interesting case from the spectroscopic point of view as it is an intermediate case between methyl formate and methanol. In the normal species of acetaldehyde, the barrier to internal rotation\footnote{Smirnov, I. A.; {\em et al.} {\em J. Mol. Spectrosc.} ~{\bf295} (2014) 44} V3_3 is 408cm1^{-1} which is close to the value in methyl formate\footnote{Ilyushin, V.; {\em et al.} {\em J. Mol. Spectrosc.} ~{\bf255} (2009) 32}: 373 cm1^{-1}. However, the value of the Coriolis coupling constant ρ\rho is 0.33 in acetaldehyde which is a much larger value than in methyl formate, 0.08, meaning that the coupling between the torsion and the overall rotation is more important. \\ The sample was not a commercial one and half of its amount is the normal species which leads to a more difficult line assignment. The spectra were recorded in Lille between 75 and 950~GHz with a solid-state submillimeter-wave spectrometer. The starting point of the analysis was the centimeter-wave measurements carried out for the sym and asym- conformers.\footnote{Turner, P. H.; and Cox, A. P. {\em Chem. Phys. Lett.}~{\bf42}, (1976) 84 - Turner, P. H.; Cox, A. P.; and Hardy, J. A. {\em J.C.S. Farady Trans.}~{\bf2}, (1981) 1217} A comparison between the approach developed for deuterated methyl formate (\chem{HCOOCH_2D}), based on the water dimer formalism, and that designed recently for deuterated methanola^{a} (\chem{CH_2DOH}) will be presented.\\ \em{This work is supported by the CNES and the Action sur Projets de l'INSU, PCMI.}Made available in DSpace on 2014-09-17T16:55:39Z (GMT). No. of bitstreams: 3 license.txt: 4922 bytes, checksum: 910b249b4beec47e7ab768910c8f966f (MD5) 369.pdf: 24874 bytes, checksum: 5f4d8e391f106190fea68f48c1df9d9c (MD5) abstract.txt: 2306 bytes, checksum: e68f7bb233099e023337c79d1f3c9cdf (MD5) Previous issue date: 2014-06-20Made available in DSpace on 2015-04-14T18:39:41Z (GMT). No. of bitstreams: 4 license.txt: 4922 bytes, checksum: 910b249b4beec47e7ab768910c8f966f (MD5) FA08_Presentation.pdf: 4401297 bytes, checksum: f2fa12a52646014e11ca51ddb7417994 (MD5) FA08_Abstract.pdf: 24874 bytes, checksum: 5f4d8e391f106190fea68f48c1df9d9c (MD5) FA08_Abstract.txt: 2306 bytes, checksum: e68f7bb233099e023337c79d1f3c9cdf (MD5) Previous issue date: 2014-06-2

    The Bending-rotation Approach Applied To The Methylene Radical Ch<sub>2</sub>

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    "Quasi-linear molecules display a large amplitude bending mode allowing them to sample their linear configuration. This leads to a strong coupling between the overall rotation and the bending mode and to a singularity in their Hamiltonian. Quasi-linearity has been extensively studied in many species including the closed shell water molecule and the open shell amidogen (NH2_2) and methylene (CH2_2) radicals. For these three species, the barrier to linearity ranges from 12\,000~cm1^{-1} for NH2_2 to less than 2000~cm1^{-1} for CH2_2.\footnote{Jungen, Hallin, and Merer, {\em Molec.\ Phys.}~{\bf 40} (1980) 25; Bunker, Jensen, Kraemer, and Beardsworth, {\em J.\ Chem.\ Phys.}~{\bf 85} (1986) 3724; Partridge and Schwenke, {\em J.\ Chem.\ Phys.}~{\bf 106} (1997) 4618} Their rovibrational energy levels can be computed with almost spectroscopic accuracy using variational approaches or, if a higher accuracy is required, with reduced dimensionality models such as the effective Bending-Rotation approach,\footnote{Coudert, Marin-Drumel, and Pirali, {\em J.\ Mol.\ Spectrosc.}~{\bf 303} (2014) 36} already applied to treat the anomalous centrifugal distortion of the water moleculeb^b and of the amidogen radical.\footnote{TD03, Martin-Drumel, Pirali, and Coudert, 72nd ISMS, Urbana-Champaign, June 19--23, 2017} In this talk, the Bending-Rotation approachb^b is extended, adding the spin-rotation and spin-spin fine couplings, so as to be used in the case of the methylene radical. The new approach is applied to the fitting of high-resolution data pertaining to this species. In addition to the ground state data previously analyzed,\footnote{Br\""unken, M\""uller, Lewen, and Giesen, {\em J.\ Chem.\ Phys.}~{\bf 123} (2005) 164315} the data set includes FIR transitions belonging to the ν2\nu_2 band.\footnote{Sears, Bunker, and McKellar, {J.\ Chem.\ Phys.}~{\bf 77} (1982) 5363; McKellar, Yamada, and Hirota, {\em J.\ Chem.\ Phys.}~{\bf 79} (1983) 1220; and Marshall and McKellar, {\em J.\ Chem.\ Phys.}~{\bf 85} (1986) 3716} 336 transitions were reproduced with a standard deviation of 1.3 using 42 spectroscopic parameters.\footnote{Coudert, {\em J.\ Chem.\ Phys.}~{\bf 153} (2020) 144115} In the talk, the results of this analysis will be reported and the dependence on the bending angle retrieved for the spin-rotation and spin-spin fine couplings will be discussed. We will also try to see if the analysis resultsf^f can be further improved."Made available in DSpace on 2021-09-24T21:09:33Z (GMT). No. of bitstreams: 2 4776.pdf: 22569 bytes, checksum: d58651467ec7d945051809a05e6ce340 (MD5) license.txt: 4802 bytes, checksum: 58353f9dd6876860dd5221f3d7872a95 (MD5) Previous issue date: 2021-06-24Made available in DSpace on 2022-01-21T16:09:15Z (GMT). No. of bitstreams: 4 4776.pdf.txt: 2431 bytes, checksum: aa31805a5167001ca98715d66caf1f21 (MD5) license.txt: 4802 bytes, checksum: 58353f9dd6876860dd5221f3d7872a95 (MD5) 4776.pdf: 22569 bytes, checksum: d58651467ec7d945051809a05e6ce340 (MD5) RH04_4776.pdf: 82726 bytes, checksum: 9c08ebfe2c6bb2f5ef9eefa9f3ada24a (MD5) Previous issue date: 2021-06-2

    Global Analysis Of The Cd<sub>2</sub>hoh Molecule Rotation-torsion Spectrum

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    Doubly deuterated methanol CD2_2HOH is a non-rigid molecule displaying internal rotation of its asymmetrical CD2_2H methyl group. Like the isotopic species of methanol with a symmetrical CH3_3 or CD3_3 group, it displays a strong rotation-torsion Coriolis coupling. Unlike these species, it also displays a dependence of its generalized inertia tensor on the angle of internal rotation. Its complicated rotation-torsion spectrum was investigated in the microwave,\footnote{Liu and Quade, {\em J.\ Mol.\ Spectrosc.}~{\bf 146} (1991) 252; Su, Liu, and Quade, {\em J.\ Mol.\ Spectrosc.}~{\bf 149} (1991) 557; Quade, Liu, Mukhopadhyay, and Su, {\em J.\ Mol.\ Spectrosc.}~{\bf 192} (1998) 378; Su and Quade, {\em J.\ Chem.\ Phys.}~{\bf 90} (1989) 1396} submillimeter-wave,\footnotetext[2]{Ndao, Tchana, Coudert, Motiyenko, Margul\`es, Barros, Manceron, and Roy, {\em J.\ Mol.\ Spectrosc.}~{\bf 326} (2015) 136}\footnotetext[3]{Mukhopadhyay, {\em Inf.\ Phys.\ Tech.}~{\bf 75} (2016) 139; {\em ibid.}~{\bf 76} (2016) 116}\footnotetext[4]{Mukhopadhyay and Billinghurst, {\em Inf.\ Phys.\ Tech.}~{\bf 113} (2021) 103563}b,c^{b,c} terahertz,b^b and FIRb,c,d^{b,c,d} domains. Although more than 3000 transitions have been assigned so far, no global analysis, like the one performed for the analogous species CH2_2DOH,\footnotetext[5]{Coudert, Zemouli, Motiyenko, Margul\`es, and Klee, {\em J.\ Chem.\ Phys.}~{\bf 140} (2014) 064307}e^e has been carried out. In this talk, new assignments in the terahertz and FIR spectra of CD2_2HOH will be reported. Parallel and perpendicular transitions, characterized by a higher KK-value than in our previous investigation,b^b could be identified up to J=35J=35 for the three lowest lying torsional states. Using the theoretical approach developed for CH2_2DOH,e^e a global analysis of the available high-resolution data could also be carried out and parameters describing the hindering potential and the generalized inertia tensor\footnotetext[6]{Liu and Quade, {\em J.\ Mol.\ Spectrosc.}~{\bf 146} (1991) 238; El Hilali, Coudert, Konov, and Klee, {\em J.\ Chem.\ Phys.}~{\bf 135} (2011) 194309}f^f were determined. So far, this global analysis has been restricted to transitions with K9K\leq 9 as rotation-torsion levels with K>9K>9 are affected by a yet non-identified rotation-torsion couplings and cannot be properly modeled.Made available in DSpace on 2021-09-24T21:08:52Z (GMT). No. of bitstreams: 2 4770.pdf: 25913 bytes, checksum: e2ba91e78f6b8e9a10aa373008ad501d (MD5) license.txt: 4802 bytes, checksum: 58353f9dd6876860dd5221f3d7872a95 (MD5) Previous issue date: 2021-06-22Made available in DSpace on 2022-01-21T16:10:33Z (GMT). No. of bitstreams: 4 4770.pdf.txt: 2499 bytes, checksum: 1c1992539a0eab8ee71fcfd55d738c1c (MD5) license.txt: 4802 bytes, checksum: 58353f9dd6876860dd5221f3d7872a95 (MD5) 4770.pdf: 25913 bytes, checksum: e2ba91e78f6b8e9a10aa373008ad501d (MD5) TH05_4770.pdf: 116926 bytes, checksum: d491e6f82b39ce44aaba822622f1a111 (MD5) Previous issue date: 2021-06-2

    The Torsional Spectrum Of Doubly Deuterated Methanol Chd2oh

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    Although the torsional spectrum of several isotopic species of methanol with a symmetrical \chem{CH_3} or \chem{CD_3} was analyzed some time ago, it is recently,\footnote{El Hilali, Coudert, Konov, and Klee, {\em J.\ Chem.\ Phys.}~{\bf 135} (2011) 194309} and only for the monodeuterated species \chem{CH_2DOH}, that such an analysis was extended to the case of an asymmetrical methyl group. In this talk, based on a Fourier transform high-resolution spectrum recorded in the 20 to 670~\wn\ region, the first analysis of the torsional spectrum of doubly deuterated methanol \chem{CHD_2OH} will be presented. The QQ branch of many torsional subbands could be observed and their assignment was initiated using a theoretical torsion-rotation spectrum computed with an approach accounting for the torsion-rotation Coriolis coupling and for the dependence of the generalized inertia tensor on the angle of internal rotation.\footnote{Lauvergnat, Coudert, Klee, and Smirnov, {\em J.\ Mol.\ Spectrosc.}~{\bf 256} (2009) 204} 46 torsional subbands were thus assigned. For 28 of them, their rotational structure could be assigned and fitted using an effective Hamiltonian expressed as a J(J+1)J(J+1) expansion; and for 2 of them microwave transitions within the lower torsional level could also be included in the analysis.\footnote{Quade, Liu, Mukhopadhyay, and Su, {\em J.\ Mol.\ Spectrosc.}~{\bf 192} (1998) 378} In several cases these analysis revealed that the torsional levels are strongly perturbed.\footnote{Pearson, Yu, and Drouin, {\em J.\ Mol.\ Spectrosc.}~{\bf 280} (2012) 119} In the talk, the torsional parameters retrieved in the analysis of the torsional subband centers will be discussed. The results of the analysis of the rotational structure of the torsional subbands will be presented and we will also try to understand the nature of the perturbations. At last, preliminary results about the analysis of the microwave spectrum will be presented.Made available in DSpace on 2014-09-17T16:54:51Z (GMT). No. of bitstreams: 3 license.txt: 4922 bytes, checksum: 910b249b4beec47e7ab768910c8f966f (MD5) 120.pdf: 25004 bytes, checksum: a0607c92c70cbc59f97e962e4bd047d1 (MD5) abstract.txt: 2216 bytes, checksum: 3b61f76b4ddca92a67e5240396f4ee89 (MD5) Previous issue date: 2014-06-20Made available in DSpace on 2015-04-14T18:37:33Z (GMT). No. of bitstreams: 4 license.txt: 4922 bytes, checksum: 910b249b4beec47e7ab768910c8f966f (MD5) FA06_Presentation.pptx: 496631 bytes, checksum: e0eee671c870bd3ac41debbfebe2bde2 (MD5) FA06_Abstract.pdf: 25004 bytes, checksum: a0607c92c70cbc59f97e962e4bd047d1 (MD5) FA06_Abstract.txt: 2216 bytes, checksum: 3b61f76b4ddca92a67e5240396f4ee89 (MD5) Previous issue date: 2014-06-2
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