A line-shape analysis for spin-1 NMR signals

vonGoeler, E; 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; Yanez, A; Ylostalo, J; Zanetti, AM; Zaremba, K; Zhao, J; 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; Bjorkholm, P; Bonner, BE; deBotton, N; Boutemeur, M; Bradamante, F; Bressan, A; Bultmann, S; Burtin, E; Cavata, C; Crabb, D; Cranshaw, J; Cuhadar, T; DallaTorre, S; vanDantzig, 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; Goertz, S; Gomez, F; Gracia, G; deGroot, N; Perdekamp, MG; Gulmez, E; Harmsen, J; vonHarrach, 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; Kramer, D; Krivokhijine, V; Kroger, W; Kukhtin, V; Kurek, K; Kyynarainen, J; Lamanna, M; Landgraf, U; LeGoff, JM; Lehar, F; deLesquen, 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; vanMiddelkoop, G; Miller, D; Mori, K; Moromisato, J; Nagaitsev, A; Nassalski, J; Naumann, L; Niinikoski, TO; Oberski, JEJ; Ogawa, A; Ozben, C; Parks, DP; PerrotKunne, 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; Schuler, KP

Author

vonGoeler, E

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

Yanez, A

Ylostalo, J

Zanetti, AM

Zaremba, K

Zhao, J

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

Bjorkholm, P

Bonner, BE

deBotton, N

Boutemeur, M

Bradamante, F

Bressan, A

Bultmann, S

Burtin, E

Cavata, C

Crabb, D

Cranshaw, J

Cuhadar, T

DallaTorre, S

vanDantzig, 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

Goertz, S

Gomez, F

Gracia, G

deGroot, N

Perdekamp, MG

Gulmez, E

Harmsen, J

vonHarrach, 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

Kramer, D

Krivokhijine, V

Kroger, W

Kukhtin, V

Kurek, K

Kyynarainen, J

Lamanna, M

Landgraf, U

LeGoff, JM

Lehar, F

deLesquen, 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

vanMiddelkoop, G

Miller, D

Mori, K

Moromisato, J

Nagaitsev, A

Nassalski, J

Naumann, L

Niinikoski, TO

Oberski, JEJ

Ogawa, A

Ozben, C

Parks, DP

PerrotKunne, 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

Schuler, KP

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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.

URI

http://hdl.handle.net/20.500.12627/20299
https://doi.org/10.1016/s0168-9002(97)00317-3

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