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1 xperimental relationship, between the methyl quadrupolar, (13)C-(13)C and (13)C-(1)H dipolar coupling
2 1) in nonpolar solvents, it is symmetric and quadrupolar; (2) in weakly polar media, the quadrupolar
4 rimental restraint on the values of the (2)H quadrupolar and (13)C-(1)H dipolar interactions and grea
7 17.6-35.2 T/750-1500 MHz for (1)H) the (17)O quadrupolar and chemical shift parameters were determine
10 ometry of the methyl group, the sizes of the quadrupolar and dipolar couplings, and the effects of bo
11 We discuss the implications of cooperative quadrupolar and multipolar states for the design of rela
14 , the other reference frame is the principal quadrupolar axes calculated with respect to the molecula
16 (SORI) collision-induced dissociation (CID), quadrupolar axialization, multiple stages of isolation a
17 at 40 T is nearly free from the second-order quadrupolar broadening and can be interpreted quantitati
19 culations that demonstrate how this leads to quadrupolar capillary interactions between the particles
20 onate (with DFS (double field sweep), QCPMG (quadrupolar Carr-Purcell-Meiboom-Gill), and WURST (wideb
22 kHz from T2e experiments) and the effective quadrupolar coupling constant (38.8-39.8 kHz from analys
24 eltaCS) and quadrupolar coupling parameters (quadrupolar coupling constant, QCC, and asymmetry parame
25 R measurements yield an average value of the quadrupolar coupling constant, QCC, for D(alpha) sites i
27 scopy is applied to characterize the nuclear quadrupolar coupling constants (C(Q)) and asymmetry para
29 er that the 3.8-5.0 A range obtained without quadrupolar coupling included in the simulation represen
30 e 17O isotropic chemical shift (deltaCS) and quadrupolar coupling parameters (quadrupolar coupling co
31 otropic chemical shifts and nuclear electric quadrupolar coupling parameters turn out to be extremely
32 ance from the Co(II) ion, and resolved (11)B quadrupolar coupling showed approximately 30% electronic
33 onents of the hyperfine coupling and nuclear quadrupolar coupling tensors of the hydrogen-bonded prot
34 leads at a mean-field level to the expected quadrupolar coupling, but also for certain structures to
38 H NMR enables direct measurement of residual quadrupolar couplings (RQCs) due to individual C-(2)H-la
39 ation is manifested as near rigid-limit (2)H quadrupolar couplings and (13)C-(1)H, (15)N-(1)H, and (1
42 erical simulations show that moderate (87)Sr quadrupolar couplings decrease the envelope modulation r
43 /POPG membrane, the peptides caused distinct quadrupolar couplings for the two lipids, indicating dom
44 xed POPE/POPG membranes should give the same quadrupolar couplings for the two lipids, whereas the pr
47 of the two lipids should cause distinct (2)H quadrupolar couplings that reflect different chain disor
49 btained, allowing isotropic chemical shifts, quadrupolar couplings, and asymmetric parameters to be e
50 the membrane normal is characterized via 2H quadrupolar couplings, C-H and N-H dipolar couplings, 13
55 nematic LC 4-cyano-4'-pentylbiphenyl create quadrupolar distortions in the director field causing pa
56 r line width in most of the studied cases is quadrupolar dominated and field-strength independent.
57 solvate was obtained by variable-temperature quadrupolar echo (2)H NMR data acquired with samples pre
61 ed by variable-temperature 13C CPMAS NMR and quadrupolar echo 2H NMR line-shape analysis: 12.8 kcal/m
62 he main techniques employed are deuteron NMR quadrupolar echo line shape analysis, and T(1Z) (Zeeman)
63 ction, variable-temperature (13)C CPMAS NMR, quadrupolar echo solid-state (2)H NMR, and thermal analy
67 ass of strained nanostructures where nuclear quadrupolar effects have a significant but largely unkno
68 While this structure hosts both dipolar and quadrupolar electric and magnetic delocalized modes, onl
69 re continually removed by the application of quadrupolar excitation in the form of band-limited or "c
70 ver the head (often with striking dipolar or quadrupolar forms), while crude source modeling yielded
71 ange in the electric field gradient (nuclear quadrupolar frequency) or in the distribution of it, thu
72 aromatic rings cannot be treated as a simple quadrupolar functional group at van der Waals' distance.
73 pecific high-resolution spectra to yield the quadrupolar interaction parameters but also the CSA or H
74 only anisotropic interaction; the deuterium quadrupolar interaction was apparently averaged due to a
75 lar magnitude (chemical shift anisotropy and quadrupolar interaction), and the full interpretation of
76 spective, we provide a brief overview of the quadrupolar interaction, describe some of the basic expe
80 s of solid-state NMR by unifying dipolar and quadrupolar interactions and highlights the unique featu
82 ar spin of 83Kr atoms (I = 9/2) is driven by quadrupolar interactions during brief adsorption periods
83 e values, we demonstrate that strain-induced quadrupolar interactions make nuclear spin fluctuations
85 t first, this appears surprising because the quadrupolar interactions present in nuclei with spin > 1
86 ation of (131)Xe (S = (3)/(2)) is subject to quadrupolar interactions which may lead to higher rank s
87 is based on 15N and 13C chemical shifts, 2H quadrupolar interactions, and 15N-2H dipolar interaction
89 ines that directly coordinate F(-) through a quadrupolar-ion interaction cannot be functionally subst
90 e-particle spacing enabled either dipolar or quadrupolar lattice modes to be selectively accessed and
92 delocalized modes, only dipolar electric and quadrupolar magnetic modes remain at normal incidence.
93 strate-mediated hybridization of dipolar and quadrupolar modes predicted by theory, simulations, and
94 Here, excited-state symmetry breaking in a quadrupolar molecule with a D-pi-A-pi-D motif, where D a
96 d its pi electronic structure and associated quadrupolar moment (aromaticity) that favor residing in
97 d it is shown that descriptors involving the quadrupolar moments and related quantities are required
98 the first time that molecular electrostatic quadrupolar moments have been utilized in a 3D-QSAR anal
99 e to its extremely low natural abundance and quadrupolar nature, the (17)O nuclide is very rarely use
102 a new avenue for the application of SSNMR to quadrupolar nuclei and notably the atomic-scale structur
104 lly informative J couplings between pairs of quadrupolar nuclei in dimetallic and dimetalloid coordin
105 allenging new applications of NMR spectra of quadrupolar nuclei in the fields of energy materials, mi
107 ross-polarization and dipolar recoupling for quadrupolar nuclei is completely negated using this tech
108 he acquisition of solid-state NMR spectra of quadrupolar nuclei obtained at very high magnetic fields
109 (and additional parameters, CQ and eta, for quadrupolar nuclei, I > (1)/2) to 2D correlations, to an
112 electron charge distribution surrounding the quadrupolar nucleus enables the unique characterization
113 asis of hyperfine (Fermi contact) shifts and quadrupolar nutation behavior, aided by results from per
115 hape analysis, and T(1Z) (Zeeman) and T(1Q) (quadrupolar order) relaxation experiments performed at 1
117 ecular orientation (multipolar) and orbital (quadrupolar) order in the perovskite-like metal-organic
118 2)H NMR relaxation (spin-lattice, T(1Z), and quadrupolar-order, T(1Q)) experiments in the dark, Meta
119 between the halogen bond environment and the quadrupolar parameters is elucidated through a natural l
123 s analyzer, the planar Paul trap, in which a quadrupolar potential distribution is made between two e
126 nd the induced electric dipolar and magnetic quadrupolar radiation from the two dielectric antenna el
128 region, transferred from the toroidal to the quadrupolar region, and mass-selectively ejected from th
129 te conditions, the measurement of changes in quadrupolar relaxation times is a reliable means of dete
131 c symmetry of the GaAs lattice, resulting in quadrupolar satellites for nuclear [Formula: see text] i
132 s are a critical factor in the adsorption of quadrupolar species such as CO(2) and N(2) in metal-orga
134 how an almost baseline-resolved quintet from quadrupolar splitting ((55)Mn, I = 5/2, 100%), allowing
139 accompanied by a discontinuous change in the quadrupolar splitting of Fe(2+), as determined by Mossba
140 ar to those of temperature variations of the quadrupolar splitting of interbilayer D2O in PC and PE b
141 d PMMA gels were evaluated by monitoring the quadrupolar splitting of the (2)H NMR signal of CDCl(3),
142 2H order parameters were calculated from the quadrupolar splitting of the de-Paked 2H NMR spectra.
143 large changes in the methyl and C(beta)-(2)H quadrupolar splittings (Deltanu(q)) when Ala(5) in nativ
145 ermine the topology of phylloseptin-1, where quadrupolar splittings close to the maximum impose the m
147 ning our data with the previously determined quadrupolar splittings for deuterium labels on the palmi
148 In the C12:0 and C14:0 lipids, the (2)H-NMR quadrupolar splittings for the set of six core alanines
149 o reveal that two orientation-dependent (2)H quadrupolar splittings from methyl-deuterated alanines a
150 istinguished by the difference of their (2)H quadrupolar splittings in a chiral liquid crystal contai
151 ed an approach to directly convert the (14)N quadrupolar splittings into an average orientation of th
152 56 samples revealed broad Pake patterns with quadrupolar splittings of 16.9 kHz and 13.3 kHz, respect
153 Val-50 and Leu-62 showed Pake patterns, with quadrupolar splittings of 3.5 kHz and 3.7 kHz, respectiv
154 manifested by the significantly reduced (2)H quadrupolar splittings of perdeuterated palmitoyloleoylp
155 of the sample made with DPPC-d62 and of the quadrupolar splittings of the chain-methyl-labeled DPPC-
157 present a combined analysis of (2)H-alanine quadrupolar splittings together with (1)(5)N/(1)H dipola
161 quadrupolar; (2) in weakly polar media, the quadrupolar state observed directly after excitation tra
163 olygonal platelets exhibit either dipolar or quadrupolar symmetries, depending on whether their numbe
164 , A(iso) = -6.25 MHz, T = -0.94 MHz) and the quadrupolar tensor (e(2)Qq/h = -2.47 MHz, eta = 0.38) of
165 govern the magnitude and orientation of the quadrupolar tensor as the geometry about the anion is sy
169 coaxial ion trap, in which both toroidal and quadrupolar trapping regions are created simultaneously.
170 iation of NMR parameters (both shielding and quadrupolar) with local structure, including changes in
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