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1 linewidth approaching limits dictated by the spin-spin relaxation.
2 rhauser effect, spin-lattice relaxation, and spin-spin relaxation.
3 ecule (39.3 ppm), and the corresponding 13C1 spin-spin relaxation becomes nonexponential.
4 essure and the T(1) (spin-lattice) and T(2) (spin-spin) relaxation data on each section were collecte
5      Measurements of interspin distances via spin-spin relaxation enhancement have the advantages tha
6 a ligand of interest can be determined via a spin-spin relaxation measurement of a reporter ligand in
7                                              Spin-spin relaxation measurements are in agreement with
8  of 15N spin-lattice relaxation rate (R(1)), spin-spin relaxation rate (R(2)), and heteronuclear nucl
9 ficantly reduced the intermolecular electron spin-spin relaxation rate and increased the DEER signal-
10                         15N spin-lattice and spin-spin relaxation rate constants (R1 and R2, respecti
11                         15N spin-lattice and spin-spin relaxation rate constants (R1 and R2, respecti
12 ice relaxation rate constants (RN(Nz)=1/T1), spin-spin relaxation rate constants (RN(Nx,y)=1/T2) and
13                                              Spin-spin relaxation rate, R2*, was measured, which is d
14 spin-echo measurements of the enhancement of spin-spin relaxation rates at 10-30 K.
15            Exchange contributions, R(ex), to spin-spin relaxation rates for (13)C(alpha) and (13)C(be
16 es and the population indexes indicated that spin-spin relaxation represents the behavior of the boun
17        15N spin-lattice relaxation [Rn(Nz)], spin-spin relaxation [Rn(Nx,y)], cross-relaxation [RN(Hz
18 ggregated states resulting in changes in the spin-spin relaxation time (T(2)) of their surrounding wa
19 ide nanoparticles, specifically by measuring spin-spin relaxation time (T(2)), is reported.
20       Magnetic resonance imaging (MRI)-based spin-spin relaxation time (T2) mapping has been shown to
21 temperatures (50-80 K) to increase the short spin-spin relaxation time (T2) upon which the technique
22 sonances) to creatine (at 3.03 ppm), and the spin-spin relaxation time for these metabolites (resonan
23 dentified from changes in the backbone (15)N spin-spin relaxation time in the presence and absence of
24         The abrupt change of the 13C nuclear spin-spin relaxation time of the confined liquid benzene
25 ce of molecular targets, with changes in the spin-spin relaxation time of water (T2).
26 persed state, resulting in a decrease in the spin-spin relaxation time, T(2).
27 lattice relaxation time, T1) and coherences (spin-spin relaxation time, T2) to the immediate environm
28 ith metabolite concentrations and metabolite spin-spin relaxation time, the metabolic ratios presente
29 ional approach to correlate spin-lattice and spin-spin relaxation times (T1-T2) including acquisition
30 y (approximately 45 kHz), coupled with short spin-spin relaxation times (T2) indicates that the loops
31 anoassemblies resulting in a decrease of the spin-spin relaxation times (T2) of neighboring water pro
32      15N spin-lattice relaxation times (T1), spin-spin relaxation times (T2), and heteronuclear NOEs
33 Proton populations were identified measuring spin-spin relaxation times (T2).
34 se sequences: eCPMG and eDiff, by modulating spin-spin relaxation times and diffusion of MBC molecula
35 n increase in spin-lattice and a decrease in spin-spin relaxation times in mixed-lipid model membrane
36 oom-Gill (CPMG) sequence was used to measure spin-spin relaxation times of proton pools representing
37 lues of backbone and tryptophan indole (15)N spin-spin relaxation times, and from the negative (1)H-(
38   For 13C-enriched organics, the 13C nuclear spin-spin relaxation was demonstrated as a sensitive too

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