6533b7d9fe1ef96bd126ce83

RESEARCH PRODUCT

A line-shape analysis for spin-1 NMR signals

J. KyynärämenJ. KyynärämenS. BültmannS. BültmannJ. VogtD. CrabbT. PussieuxF. LeharD. KrämerF. TessarottoYu. KisselevF. Perrot-kunneW. KrögerW. KrögerIskender Atilla ReyhancanT. LindqvistJ. YlöstaloL. NaumannJ. CranshawA. BressanP. SchiavonW. WislickiI. SaboA. KarevC. DulyaC. DulyaMatias RodriguezMatias RodriguezM. LitmaathM. LitmaathG. IgoT. ÇUhadarJ. A. GarzonJ. A. GarzonA. SteinmetzFranco BradamanteD. Y. BardinB. DerroHeinrich B. StuhrmannJ. HarmsenA. WitzmannGünter BaumRicardo PiegaiaRicardo PiegaiaM. GiorgiN. HorikawaPatrick HautlePatrick HautleP. BerglundClemens A. HeuschClemens A. HeuschE. RondioD. L. AdamsS. K. DhawanJ. ZhaoR. BirsaF. FeinsteinA. MagnonN. De BottonD. PoseVictor KukhtinG. UnelJ. H. MoromisatoK. ZarembaH. J. KesslerM. LamannaE. Von GoelerF. SeverRoland WindmoldersD. PeshekhonovK. RurekG. Van MiddelkoopM. PloG. ReicherzV. W. HughesS. Dalla TorreDavid MillerA. ArvidsonL. KlostermannL. KlostermannE. GülmezJ. M. Le GoffAlan D. MartinE. BurtinT. KageyaE. M. KabußA. GallasH. PostmaR. E. SegelM. K. BallintijnM. K. BallintijnA. OgawaG. K. MallotM. BoutemeurM. BoutemeurD. FaschingD. FaschingW. MeyerJ. SaboridoT. HasegawaJ. S. MccarthyA. De LesquenK. M. TeichertA. RijllartAnna ZanettiAnna ZanettiT. MatsudaJ. PretzA. KishiJ. MartinoBernardo AdevaJay RobertsA. RosadoR. GehringD. Von HarrachM. LoweM. LoweT. GaussiranLawrence S. PinskySt. GoertzMichal SzleperM. Grosse PerdekampM. Grosse PerdekampYannis K. SemertzidisJ. PyrlikJ. C. FaivreC. A. WhittenLidia KalinovskayaG. GraciaRegine WillumeitA. SandaczL. BetevA. DyringW. TlaczalaI.a. SavinM. VelascoM. VelascoTakahiro IwataS. EichblattS. EichblattS. RockS. RockP. BjörkholmB. W. MayesC. CavataE. P. SichtermannP. ShanahanP. ShanahanB. FroisK. P. SchülerE. ArikU. StieglerRoy WeinsteinN. De GrootN. De GrootF. SimeoniA. NagaitsevG.i. SmirnovF. MarieAina YañezT. O. NiinikoskiJ. E.j. OberskiJ. NassalskiR. SeitzR. SeitzFaustino GómezKunikazu MoriK. MedvedA. TripetA. TripetJ. LichtenstadtS. PlatchkovS. IshimotoR. Van DantzigB. E. BonnerC. S. ÖZbenRudiger VossUlrich LandgrafV. G. KrivokhijineDrew ParksG. BardinA. StaudeAbhay DeshpandeT. J. KetelB. BadelekC. FernandezC. FernandezN. HayashiI. G. Bird

subject

Coupling constantPhysicsdisNuclear and High Energy PhysicsButanolmedia_common.quotation_subjectsmcpolarized targetQ meterdiPolarization (waves)AsymmetryMolecular physicschemistry.chemical_compoundDipoleNuclear magnetic resonanceDeuteriumchemistrysmc; dis; polarized targetDetectors and Experimental TechniquesInstrumentationShape analysis (digital geometry)media_common

description

An analytic model of the deuteron absorption function has been developed and is compared to experimental NMR signals of deuterated butanol obtained at the SMC experiment in order to determine the deuteron polarization. The absorption function model includes dipolar broadening and a frequency-dependent treatment of the intensity factors. The high-precision TE signal data available are used to adjust the model for Q-meter distortions and dispersion effects. Once the Q-meter adjustment is made, the enhanced polarizations determined by the asymmetry and TE-calibration methods compare well within the accuracy of each method. In analyzing the NMR signals, the quadrupolar coupling constants could be determined for both the CD and the OD bonds of deuterated butanol.

yearjournalcountryeditionlanguage
1997-01-01
10.1016/s0168-9002(97)00317-3http://hdl.handle.net/11368/2557989