A line-shape analysis for spin-1 NMR signals

C. Dulya; D. Adams; B. Adeva; E. Arik; A. Arvidson; B. Badelek; M. K. Ballintijn; D. Bardin; G. Bardin; G. Baum; P. Berglund; L. Betev; I. G. Bird; R. Birsa; P. Björkholm; B. E. Bonner; N. de Botton; M. Boutemeur; F. Bradamante; A. Bressan; S. Bültmann; E. Burtin; C. Cavata; D. Crabb; J. Cranshaw; T. Çuhadar; S. Dalla Torre; R. van Dantzig; B. Derro; A. Deshpande; S. Dhawan; A. Dyring; S. Eichblatt; J. C. Faivre; D. Fasching; F. Feinstein; C. Fernandez; B. Frois; A. Gallas; J. A. Garzon; T. Gaussiran; R. Gehring; M. Giorgi; E. von Goeler; S. Goertz; F. Gomez; G. Gracia; N. de Groot; M. Grosse Perdekamp; E. Gülmez; J. Harmsen; D. von Harrach; T. Hasegawa; P. Hautle; N. Hayashi; C. A. Heusch; N. Horikawa; V. W. Hughes; G. Igo; S. ishimoto; T. Iwata; E. M. Kabuß; T. Kageya; L. Kalinovskaya; A. Karev; H. J. Kessler; T. J. Ketel; A. Kishi; Y. Kisselev; L. Klostermann; D. Krämer; V. Krivokhijine; W. Kroger; V. Kukhtin; K. Rurek; J. Kyynärämen; M. Lamanna; U. Landgraf; J. M. Le Goff; F. Lehar; A. de Lesquen; J. Lichtenstadt; T. Lindqvist; M. Litmaath; M. Lowe; A. Magnon; G. K. Mallot; F. Marie; A. Martin; J. Martino; T. Matsuda; B. Mayes; J. S. McCarthy; K. Medved; W. Meyer; G. van Middelkoop; D. Miller; K. Mori; J. Moromisato; A. Nagaitsev; J. Nassalski; L. Naumann; T. O. Niinikoski; J. E.J. Oberski; A. Ogawa; C. Ozben; D. P. Parks; F. Perrot-Kunne; D. Peshekhonov; R. Piegaia; L. Pinsky; S. Platchkov; M. Plo; D. Pose; H. Postma; J. Pretz; T. Pussieux; J. Pyrlik; G. Reicherz; I. Reyhancan; A. Rijllart; J. B. Roberts; S. Rock; M. Rodriguez; E. Rondio; A. Rosado; I. Sabo; J. Saborido; A. Sandacz; I. Savin; P. Schiavon; K. P. Schüler; R. Segel; R. Seitz; Y. Semertzidis; F. Sever; P. Shanahan; E. P. Sichtermann; F. Simeoni; G. I. Smirnov; A. Staude; A. Steinmetz; U. Stiegler; H. Stuhrmann; M. Szleper; K. M. Teichert; F. Tessarotto; W. Tlaczala; A. Tripet; G. Unel; M. Velasco; J. Vogt; R. Voss; R. Weinstein; C. Whitten; R. Windmolders; R. Willumeit; W. Wislicki; A. Witzmann; A. Yañez; J. Ylöstalo; A. M. Zanetti; K. Zaremba; J. Zhao

doi:10.1016/S0168-9002(97)00317-3

A line-shape analysis for spin-1 NMR signals

C. Dulya^*, D. Adams, B. Adeva, E. Arik, A. Arvidson, B. Badelek, M. K. Ballintijn, D. Bardin, G. Bardin, G. Baum, P. Berglund, L. Betev, I. G. Bird, R. Birsa, P. Björkholm, B. E. Bonner, N. de Botton, M. Boutemeur, F. Bradamante, A. BressanS. Bültmann, E. Burtin, C. Cavata, D. Crabb, J. Cranshaw, T. Çuhadar, S. Dalla Torre, R. van Dantzig, B. Derro, A. Deshpande, S. Dhawan, A. Dyring, S. Eichblatt, J. C. Faivre, D. Fasching, F. Feinstein, C. Fernandez, B. Frois, A. Gallas, J. A. Garzon, T. Gaussiran, R. Gehring, M. Giorgi, E. von Goeler, S. Goertz, F. Gomez, G. Gracia, N. de Groot, M. Grosse Perdekamp, E. Gülmez, J. Harmsen, D. von Harrach, T. Hasegawa, P. Hautle, N. Hayashi, C. A. Heusch, N. Horikawa, V. W. Hughes, G. Igo, S. ishimoto, T. Iwata, E. M. Kabuß, T. Kageya, L. Kalinovskaya, A. Karev, H. J. Kessler, T. J. Ketel, A. Kishi, Y. Kisselev, L. Klostermann, D. Krämer, V. Krivokhijine, W. Kroger, V. Kukhtin, K. Rurek, J. Kyynärämen, M. Lamanna, U. Landgraf, J. M. Le Goff, F. Lehar, A. de Lesquen, J. Lichtenstadt, T. Lindqvist, M. Litmaath, M. Lowe, A. Magnon, G. K. Mallot, F. Marie, A. Martin, J. Martino, T. Matsuda, B. Mayes, J. S. McCarthy, K. Medved, W. Meyer, G. van Middelkoop, D. Miller, K. Mori, J. Moromisato, A. Nagaitsev, J. Nassalski, L. Naumann, T. O. Niinikoski, J. E.J. Oberski, A. Ogawa, C. Ozben, D. P. Parks, F. Perrot-Kunne, D. Peshekhonov, R. Piegaia, L. Pinsky, S. Platchkov, M. Plo, D. Pose, H. Postma, J. Pretz, T. Pussieux, J. Pyrlik, G. Reicherz, I. Reyhancan, A. Rijllart, J. B. Roberts, S. Rock, M. Rodriguez, E. Rondio, A. Rosado, I. Sabo, J. Saborido, A. Sandacz, I. Savin, P. Schiavon, K. P. Schüler, R. Segel, R. Seitz, Y. Semertzidis, F. Sever, P. Shanahan, E. P. Sichtermann, F. Simeoni, G. I. Smirnov, A. Staude, A. Steinmetz, U. Stiegler, H. Stuhrmann, M. Szleper, K. M. Teichert, F. Tessarotto, W. Tlaczala, A. Tripet, G. Unel, M. Velasco, J. Vogt, R. Voss, R. Weinstein, C. Whitten, R. Windmolders, R. Willumeit, W. Wislicki, A. Witzmann, A. Yañez, J. Ylöstalo, A. M. Zanetti, K. Zaremba, J. Zhao

^*Corresponding author for this work

Physics and Astronomy

Research output: Contribution to journal › Article › peer-review

24 Scopus citations

Abstract

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.

Original language	English (US)
Pages (from-to)	109-125
Number of pages	17
Journal	Nuclear Instruments and Methods in Physics Research, Section A: Accelerators, Spectrometers, Detectors and Associated Equipment
Volume	398
Issue number	2-3
DOIs	https://doi.org/10.1016/S0168-9002(97)00317-3
State	Published - Oct 21 1997

Funding

I9 Now at Ericsson Telecommunication,5 120 AA Rijen, The Netherlands. 2oD eceased. ?’ Permanenta ddress: University of Buenos Aires, Physics Department, I428 Buenos Aires, Argentina. 22P ermanenta ddress: The American University, Washington D.C. 20016, USA. 2’ Now at Uppsala University, 75121 Uppsata, Sweden. 24N ow at DESY. 25N ow at Dresden Technical University, 01062 Dresden, Germany Permanenta ddress: Brookhaven National Laboratory, Upton, 11973 NY, USA. 26P resent address: ESFR, F-38043 Grenoble, France. *’ Now at Institute of Physics, Warsaw University of Technology. 28N ow at Institute of Radioelectronics, Warsaw University of Technology. 29S upportedb y the Bund~sm~nisterjumfu r Bildung, Wissenscha~,F orschung und Technologie. 3oP artially supportedb y TUBITAK and the Centre for Turkish-Balkan Physics Research and Application (BogaziCi University). 3’ Supportedb y the U.S. Departmento f Energy. 3zS upported by the U.S. National Science Foundation. j3 Supportedb y lshida Foundation, Monbusho Grant-in-Aid for Scientific Research (Intemational Scientific Research Program and Specially Promoted Research). 34S upported by the National Science Foundation (NWO) of the Netherlands. 35S upported by the Commissariat B I’Energie Atomique. 36S upported by Comision Interministeriald e Ciencia y Tecnologia. j7 Supported by the Israel Science Foundation. 3xS upported by KBN SPUBIP31209/94.

ASJC Scopus subject areas

Nuclear and High Energy Physics
Instrumentation

Access to Document

10.1016/S0168-9002(97)00317-3

Cite this

Dulya, C., Adams, D., Adeva, B., Arik, E., Arvidson, A., Badelek, B., Ballintijn, M. K., Bardin, D., Bardin, G., Baum, G., Berglund, P., Betev, L., Bird, I. G., Birsa, R., Björkholm, P., Bonner, B. E., de Botton, N., Boutemeur, M., Bradamante, F., ... Zhao, J. (1997). A line-shape analysis for spin-1 NMR signals. Nuclear Instruments and Methods in Physics Research, Section A: Accelerators, Spectrometers, Detectors and Associated Equipment, 398(2-3), 109-125. https://doi.org/10.1016/S0168-9002(97)00317-3

@article{da8a6c6f361940a4aa383ed814f8554e,

title = "A line-shape analysis for spin-1 NMR signals",

abstract = "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.",

author = "C. Dulya and D. Adams and B. Adeva and E. Arik and A. Arvidson and B. Badelek and Ballintijn, {M. K.} and D. Bardin and G. Bardin and G. Baum and P. Berglund and L. Betev and Bird, {I. G.} and R. Birsa and P. Bj{\"o}rkholm and Bonner, {B. E.} and {de Botton}, N. and M. Boutemeur and F. Bradamante and A. Bressan and S. B{\"u}ltmann and E. Burtin and C. Cavata and D. Crabb and J. Cranshaw and T. {\c C}uhadar and {Dalla Torre}, S. and {van Dantzig}, R. and B. Derro and A. Deshpande and S. Dhawan and A. Dyring and S. Eichblatt and Faivre, {J. C.} and D. Fasching and F. Feinstein and C. Fernandez and B. Frois and A. Gallas and Garzon, {J. A.} and T. Gaussiran and R. Gehring and M. Giorgi and {von Goeler}, E. and S. Goertz and F. Gomez and G. Gracia and {de Groot}, N. and {Grosse Perdekamp}, M. and E. G{\"u}lmez and J. Harmsen and {von Harrach}, D. and T. Hasegawa and P. Hautle and N. Hayashi and Heusch, {C. A.} and N. Horikawa and Hughes, {V. W.} and G. Igo and S. ishimoto and T. Iwata and Kabu{\ss}, {E. M.} and T. Kageya and L. Kalinovskaya and A. Karev and Kessler, {H. J.} and Ketel, {T. J.} and A. Kishi and Y. Kisselev and L. Klostermann and D. Kr{\"a}mer and V. Krivokhijine and W. Kroger and V. Kukhtin and K. Rurek and J. Kyyn{\"a}r{\"a}men and M. Lamanna and U. Landgraf and {Le Goff}, {J. M.} and F. Lehar and {de Lesquen}, A. and J. Lichtenstadt and T. Lindqvist and M. Litmaath and M. Lowe and A. Magnon and Mallot, {G. K.} and F. Marie and A. Martin and J. Martino and T. Matsuda and B. Mayes and McCarthy, {J. S.} and K. Medved and W. Meyer and {van Middelkoop}, G. and D. Miller and K. Mori and J. Moromisato and A. Nagaitsev and J. Nassalski and L. Naumann and Niinikoski, {T. O.} and Oberski, {J. E.J.} and A. Ogawa and C. Ozben and Parks, {D. P.} and F. Perrot-Kunne and D. Peshekhonov and R. Piegaia and L. Pinsky and S. Platchkov and M. Plo and D. Pose and H. Postma and J. Pretz and T. Pussieux and J. Pyrlik and G. Reicherz and I. Reyhancan and A. Rijllart and Roberts, {J. B.} and S. Rock and M. Rodriguez and E. Rondio and A. Rosado and I. Sabo and J. Saborido and A. Sandacz and I. Savin and P. Schiavon and Sch{\"u}ler, {K. P.} and R. Segel and R. Seitz and Y. Semertzidis and F. Sever and P. Shanahan and Sichtermann, {E. P.} and F. Simeoni and Smirnov, {G. I.} and A. Staude and A. Steinmetz and U. Stiegler and H. Stuhrmann and M. Szleper and Teichert, {K. M.} and F. Tessarotto and W. Tlaczala and A. Tripet and G. Unel and M. Velasco and J. Vogt and R. Voss and R. Weinstein and C. Whitten and R. Windmolders and R. Willumeit and W. Wislicki and A. Witzmann and A. Ya{\~n}ez and J. Yl{\"o}stalo and Zanetti, {A. M.} and K. Zaremba and J. Zhao",

note = "Funding Information: I9 Now at Ericsson Telecommunication,5 120 AA Rijen, The Netherlands. 2oD eceased. ?{\textquoteright} Permanenta ddress: University of Buenos Aires, Physics Department, I428 Buenos Aires, Argentina. 22P ermanenta ddress: The American University, Washington D.C. 20016, USA. 2{\textquoteright} Now at Uppsala University, 75121 Uppsata, Sweden. 24N ow at DESY. 25N ow at Dresden Technical University, 01062 Dresden, Germany Permanenta ddress: Brookhaven National Laboratory, Upton, 11973 NY, USA. 26P resent address: ESFR, F-38043 Grenoble, France. *{\textquoteright} Now at Institute of Physics, Warsaw University of Technology. 28N ow at Institute of Radioelectronics, Warsaw University of Technology. 29S upportedb y the Bund~sm~nisterjumfu r Bildung, Wissenscha~,F orschung und Technologie. 3oP artially supportedb y TUBITAK and the Centre for Turkish-Balkan Physics Research and Application (BogaziCi University). 3{\textquoteright} Supportedb y the U.S. Departmento f Energy. 3zS upported by the U.S. National Science Foundation. j3 Supportedb y lshida Foundation, Monbusho Grant-in-Aid for Scientific Research (Intemational Scientific Research Program and Specially Promoted Research). 34S upported by the National Science Foundation (NWO) of the Netherlands. 35S upported by the Commissariat B I{\textquoteright}Energie Atomique. 36S upported by Comision Interministeriald e Ciencia y Tecnologia. j7 Supported by the Israel Science Foundation. 3xS upported by KBN SPUBIP31209/94.",

year = "1997",

month = oct,

day = "21",

doi = "10.1016/S0168-9002(97)00317-3",

language = "English (US)",

volume = "398",

pages = "109--125",

journal = "Nuclear Instruments and Methods in Physics Research, Section A: Accelerators, Spectrometers, Detectors and Associated Equipment",

issn = "0168-9002",

publisher = "Elsevier B.V.",

number = "2-3",

}

Dulya, C, Adams, D, Adeva, B, Arik, E, Arvidson, A, Badelek, B, Ballintijn, MK, Bardin, D, Bardin, G, Baum, G, Berglund, P, Betev, L, Bird, IG, Birsa, R, Björkholm, P, Bonner, BE, de Botton, N, Boutemeur, M, Bradamante, F, Bressan, A, Bültmann, S, Burtin, E, Cavata, C, Crabb, D, Cranshaw, J, Çuhadar, T, Dalla Torre, S, van Dantzig, R, Derro, B, Deshpande, A, Dhawan, S, Dyring, A, Eichblatt, S, Faivre, JC, Fasching, D, Feinstein, F, Fernandez, C, Frois, B, Gallas, A, Garzon, JA, Gaussiran, T, Gehring, R, Giorgi, M, von Goeler, E, Goertz, S, Gomez, F, Gracia, G, de Groot, N, Grosse Perdekamp, M, Gülmez, E, Harmsen, J, von Harrach, D, Hasegawa, T, Hautle, P, Hayashi, N, Heusch, CA, Horikawa, N, Hughes, VW, Igo, G, ishimoto, S, Iwata, T, Kabuß, EM, Kageya, T, Kalinovskaya, L, Karev, A, Kessler, HJ, Ketel, TJ, Kishi, A, Kisselev, Y, Klostermann, L, Krämer, D, Krivokhijine, V, Kroger, W, Kukhtin, V, Rurek, K, Kyynärämen, J, Lamanna, M, Landgraf, U, Le Goff, JM, Lehar, F, de Lesquen, A, Lichtenstadt, J, Lindqvist, T, Litmaath, M, Lowe, M, Magnon, A, Mallot, GK, Marie, F, Martin, A, Martino, J, Matsuda, T, Mayes, B, McCarthy, JS, Medved, K, Meyer, W, van Middelkoop, G, Miller, D, Mori, K, Moromisato, J, Nagaitsev, A, Nassalski, J, Naumann, L, Niinikoski, TO, Oberski, JEJ, Ogawa, A, Ozben, C, Parks, DP, Perrot-Kunne, F, Peshekhonov, D, Piegaia, R, Pinsky, L, Platchkov, S, Plo, M, Pose, D, Postma, H, Pretz, J, Pussieux, T, Pyrlik, J, Reicherz, G, Reyhancan, I, Rijllart, A, Roberts, JB, Rock, S, Rodriguez, M, Rondio, E, Rosado, A, Sabo, I, Saborido, J, Sandacz, A, Savin, I, Schiavon, P, Schüler, KP, Segel, R, Seitz, R, Semertzidis, Y, Sever, F, Shanahan, P, Sichtermann, EP, Simeoni, F, Smirnov, GI, Staude, A, Steinmetz, A, Stiegler, U, Stuhrmann, H, Szleper, M, Teichert, KM, Tessarotto, F, Tlaczala, W, Tripet, A, Unel, G, Velasco, M, Vogt, J, Voss, R, Weinstein, R, Whitten, C, Windmolders, R, Willumeit, R, Wislicki, W, Witzmann, A, Yañez, A, Ylöstalo, J, Zanetti, AM, Zaremba, K & Zhao, J 1997, 'A line-shape analysis for spin-1 NMR signals', Nuclear Instruments and Methods in Physics Research, Section A: Accelerators, Spectrometers, Detectors and Associated Equipment, vol. 398, no. 2-3, pp. 109-125. https://doi.org/10.1016/S0168-9002(97)00317-3

TY - JOUR

T1 - A line-shape analysis for spin-1 NMR signals

AU - Dulya, C.

AU - Adams, D.

AU - Adeva, B.

AU - Arik, E.

AU - Arvidson, A.

AU - Badelek, B.

AU - Ballintijn, M. K.

AU - Bardin, D.

AU - Bardin, G.

AU - Baum, G.

AU - Berglund, P.

AU - Betev, L.

AU - Bird, I. G.

AU - Birsa, R.

AU - Björkholm, P.

AU - Bonner, B. E.

AU - de Botton, N.

AU - Boutemeur, M.

AU - Bradamante, F.

AU - Bressan, A.

AU - Bültmann, S.

AU - Burtin, E.

AU - Cavata, C.

AU - Crabb, D.

AU - Cranshaw, J.

AU - Çuhadar, T.

AU - Dalla Torre, S.

AU - van Dantzig, R.

AU - Derro, B.

AU - Deshpande, A.

AU - Dhawan, S.

AU - Dyring, A.

AU - Eichblatt, S.

AU - Faivre, J. C.

AU - Fasching, D.

AU - Feinstein, F.

AU - Fernandez, C.

AU - Frois, B.

AU - Gallas, A.

AU - Garzon, J. A.

AU - Gaussiran, T.

AU - Gehring, R.

AU - Giorgi, M.

AU - von Goeler, E.

AU - Goertz, S.

AU - Gomez, F.

AU - Gracia, G.

AU - de Groot, N.

AU - Grosse Perdekamp, M.

AU - Gülmez, E.

AU - Harmsen, J.

AU - von Harrach, D.

AU - Hasegawa, T.

AU - Hautle, P.

AU - Hayashi, N.

AU - Heusch, C. A.

AU - Horikawa, N.

AU - Hughes, V. W.

AU - Igo, G.

AU - ishimoto, S.

AU - Iwata, T.

AU - Kabuß, E. M.

AU - Kageya, T.

AU - Kalinovskaya, L.

AU - Karev, A.

AU - Kessler, H. J.

AU - Ketel, T. J.

AU - Kishi, A.

AU - Kisselev, Y.

AU - Klostermann, L.

AU - Krämer, D.

AU - Krivokhijine, V.

AU - Kroger, W.

AU - Kukhtin, V.

AU - Rurek, K.

AU - Kyynärämen, J.

AU - Lamanna, M.

AU - Landgraf, U.

AU - Le Goff, J. M.

AU - Lehar, F.

AU - de Lesquen, A.

AU - Lichtenstadt, J.

AU - Lindqvist, T.

AU - Litmaath, M.

AU - Lowe, M.

AU - Magnon, A.

AU - Mallot, G. K.

AU - Marie, F.

AU - Martin, A.

AU - Martino, J.

AU - Matsuda, T.

AU - Mayes, B.

AU - McCarthy, J. S.

AU - Medved, K.

AU - Meyer, W.

AU - van Middelkoop, G.

AU - Miller, D.

AU - Mori, K.

AU - Moromisato, J.

AU - Nagaitsev, A.

AU - Nassalski, J.

AU - Naumann, L.

AU - Niinikoski, T. O.

AU - Oberski, J. E.J.

AU - Ogawa, A.

AU - Ozben, C.

AU - Parks, D. P.

AU - Perrot-Kunne, F.

AU - Peshekhonov, D.

AU - Piegaia, R.

AU - Pinsky, L.

AU - Platchkov, S.

AU - Plo, M.

AU - Pose, D.

AU - Postma, H.

AU - Pretz, J.

AU - Pussieux, T.

AU - Pyrlik, J.

AU - Reicherz, G.

AU - Reyhancan, I.

AU - Rijllart, A.

AU - Roberts, J. B.

AU - Rock, S.

AU - Rodriguez, M.

AU - Rondio, E.

AU - Rosado, A.

AU - Sabo, I.

AU - Saborido, J.

AU - Sandacz, A.

AU - Savin, I.

AU - Schiavon, P.

AU - Schüler, K. P.

AU - Segel, R.

AU - Seitz, R.

AU - Semertzidis, Y.

AU - Sever, F.

AU - Shanahan, P.

AU - Sichtermann, E. P.

AU - Simeoni, F.

AU - Smirnov, G. I.

AU - Staude, A.

AU - Steinmetz, A.

AU - Stiegler, U.

AU - Stuhrmann, H.

AU - Szleper, M.

AU - Teichert, K. M.

AU - Tessarotto, F.

AU - Tlaczala, W.

AU - Tripet, A.

AU - Unel, G.

AU - Velasco, M.

AU - Vogt, J.

AU - Voss, R.

AU - Weinstein, R.

AU - Whitten, C.

AU - Windmolders, R.

AU - Willumeit, R.

AU - Wislicki, W.

AU - Witzmann, A.

AU - Yañez, A.

AU - Ylöstalo, J.

AU - Zanetti, A. M.

AU - Zaremba, K.

AU - Zhao, J.

N1 - Funding Information: I9 Now at Ericsson Telecommunication,5 120 AA Rijen, The Netherlands. 2oD eceased. ?’ Permanenta ddress: University of Buenos Aires, Physics Department, I428 Buenos Aires, Argentina. 22P ermanenta ddress: The American University, Washington D.C. 20016, USA. 2’ Now at Uppsala University, 75121 Uppsata, Sweden. 24N ow at DESY. 25N ow at Dresden Technical University, 01062 Dresden, Germany Permanenta ddress: Brookhaven National Laboratory, Upton, 11973 NY, USA. 26P resent address: ESFR, F-38043 Grenoble, France. *’ Now at Institute of Physics, Warsaw University of Technology. 28N ow at Institute of Radioelectronics, Warsaw University of Technology. 29S upportedb y the Bund~sm~nisterjumfu r Bildung, Wissenscha~,F orschung und Technologie. 3oP artially supportedb y TUBITAK and the Centre for Turkish-Balkan Physics Research and Application (BogaziCi University). 3’ Supportedb y the U.S. Departmento f Energy. 3zS upported by the U.S. National Science Foundation. j3 Supportedb y lshida Foundation, Monbusho Grant-in-Aid for Scientific Research (Intemational Scientific Research Program and Specially Promoted Research). 34S upported by the National Science Foundation (NWO) of the Netherlands. 35S upported by the Commissariat B I’Energie Atomique. 36S upported by Comision Interministeriald e Ciencia y Tecnologia. j7 Supported by the Israel Science Foundation. 3xS upported by KBN SPUBIP31209/94.

PY - 1997/10/21

Y1 - 1997/10/21

N2 - 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.

AB - 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.

UR - http://www.scopus.com/inward/record.url?scp=0041163081&partnerID=8YFLogxK

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U2 - 10.1016/S0168-9002(97)00317-3

DO - 10.1016/S0168-9002(97)00317-3

M3 - Article

AN - SCOPUS:0041163081

SN - 0168-9002

VL - 398

SP - 109

EP - 125

JO - Nuclear Instruments and Methods in Physics Research, Section A: Accelerators, Spectrometers, Detectors and Associated Equipment

JF - Nuclear Instruments and Methods in Physics Research, Section A: Accelerators, Spectrometers, Detectors and Associated Equipment

IS - 2-3

ER -

A line-shape analysis for spin-1 NMR signals

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