ライフサイエンスコーパス: multiplet

1 ltiplet, and g = 8.8 and 11.6 from the S = 3 multiplet.

2 her-order coplanar base associations, termed multiplets.

3 n the resonance lines constituting the shift multiplets.

4 s required for editing the components of the multiplets.

5 positional isotopic enrichment and spin-spin multiplets.

6 yields subspectra containing "chemical shift multiplets", alternative data processing is required for

7 proton is coupled) "units of intensity" of a multiplet and (b) then apply a clearly delineated sequen

8 of (1)H-(1)H couplings gives rise to complex multiplets and severe overlap in crowded spectra, greatl

9 spin-orbit coupling, the strength of atomic multiplets and the degree of itinerancy.

10 nt, E, that considers the complexity of (1)H multiplets (and in general the width) of the original si

11 -mode EPR signals at g = 8.17 from the S = 2 multiplet, and g = 8.8 and 11.6 from the S = 3 multiplet

12 The high-field 13C multiplets are observed as a function of pH, and the lin

13 on and (ii) RDCs are multiply encoded in the multiplets arising from the joint sampling.

14 n of NMR resonances and molecule-to-spectrum multiplets assignments.

15 an alternating sum of the characters of the multiplet associated to the trivial representation of F.

16 an alternating sum of the characters in the multiplet associated to Vlambda and whose denominator is

17 but also actually enhances the resolution of multiplets, by reducing signal broadening by magnetic fi

18 Charge-transfer multiplet calculations coupled with data acquired on low

19 nt photons can be reproduced by model atomic-multiplet calculations of the RIXS spectra.

20 ray absorption spectroscopy and ligand field multiplet calculations show that Cu(II), Ni(II), and Fe(

21 the experimental results with crystal-field multiplet calculations shows that the spin-orbital dd ex

22 Using atomic multiplet calculations, we have estimated the key energy

23 yU RNAs >5000 nt in length are packaged into multiplet capsids, in which a single RNA molecule is sha

24 Observed 15N multiplets clearly indicated that the spin system for th

25 reases as the temperature is lowered and the multiplets coalesce into broad singlets.

26 uence show significant charge clusters, high multiplet count, and extremes of amino acid usage.

27 he partial self-decoupling effect on 15Nzeta multiplets due to the rapid hydrogen exchange is also di

28 at treats magnetism, Kondo screening, atomic multiplet effects and crystal field splitting on the sam

29 ttings in the Sigma, Xi, D, and Xicc isospin multiplets, exceeding in some cases the precision of exp

30 Spectral simulation and multiplet fitting reveal that the catalyst undergoes che

31 This enables overlapping multiplets from different species, and by extension whol

32 Herein an approach that simulates (13) C multiplets in NMR spectra and utilizes mass increments t

33 orbital occupancy control between t2g and eg multiplets in quasi-two-dimensional transition metal oxi

34 in its morphology to doublets, triplets, and multiplets in the first dorsal interossei and flexor dig

35 ibit narrow signals that are not overlapping multiplets, in contrast to [Mn(12)O(12)(O(2)CMe)(16)(H(2

36 tic procedure to decipher first-order 1H NMR multiplets is described.

37 GvpL exhibited a multiplet ladder on sodium dodecyl sulfate-polyacrylamid

38 The ligand field multiplet model commonly used to simulate L-edge spectra

39 ings can be understood within a ligand field multiplet model, i.e., (3d,3d) and (2p,3d) two-electron

40 ing a valence bond configuration interaction multiplet model, is applied to directly probe the electr

41 ing a valence bond configuration interaction multiplet model, to directly experimentally probe the el

42 ies can be extracted using a charge-transfer multiplet model, without previous information from the L

43 ) or absence (group B, n = 18) of doublet or multiplet myokymic motor unit discharges.

44 yokymia or neuromyotonia, and EMG doublet or multiplet ('myokymic') motor unit discharges, indicated

45 Here, we report a multiplet of AFM dissipation peaks arising a few nanomet

46 ible representation Vlambda of F we assign a multiplet of irreducible representations of B with m ele

47 A multiplet of such bands appears at small cluster sizes.

48 22-nm-diameter capsids, in analogy with the multiplets of 28-nm-diameter particles formed with norma

49 We show that J-HSQC reports isotopomer multiplet patterns identical to those reported by direct

50 tion, (13)C isotope effects lead to spectral multiplet patterns that become dependent on the amount o

51 Comparison to a simple analysis of atomic multiplets provides a quantitative estimate of the Hund'

52 t of (13)C chemical shifts, spin-lattice and multiplet relaxation times, as well as self-diffusion co

53 13C NMR multiplet relaxation was used to characterize the intera

54 of phospho compound, as revealed by a major multiplet signal in the pyrophosphate region.

55 ormed both first-principles calculations and multiplet simulations of the spectra and quantitatively

56 Kerr soliton transition dynamics, in which a multiplet soliton state evolves into a stable singlet so

57 scopy has been utilized to obtain the L-edge multiplet spectra for a series of non-heme ferric and fe

58 -ray magnetic linear dichroism effect at the multiplet-split L edge of Fe.

59 pectra from each of the thermally accessible multiplet states of the coupled complex by multivariate

60 n experiment is demonstrated that suppresses multiplet structure in both domains of a homonuclear two

61 ra is obtained by collapsing 2D signals with multiplet structure into 2D singlets.

62 gy that allows for the interpretation of the multiplet structure of Fe L-edges in terms of differenti

63 solution in (1)H NMR is limited primarily by multiplet structure.

64 ting in peak overlap and partial loss of the multiplet structures.

65 from lig1 yielded site-specific ligand-state multiplets that provide a convenient format for assessin

66 tively unusual example of using VCD carbonyl multiplets, the absolute configuration could be reliably

67 ata, supported by density functional theory, multiplet theory, and multireference calculations, suppo

68 ction diffusion that it is possible for cell multiplets to oscillate independently initially, but to

69 BASHD-TOCSY spectra from collapse of CalphaH multiplets to singlets in the F1 dimension to resolve re

70 olution in the F1 dimension, and collapse of multiplets to singlets in the F1 dimension, cross-peaks

71 el, the fixed amplitude relationship between multiplets typical for (1)H NMR spectra must be abandone

72 representations of B with m elements in each multiplet, where m is the index of the Weyl group of B i

73 procedure for detecting restriction fragment multiplets while simultaneously determining the amplitud

74 (1)H NMR spectra with many overlapping spin multiplets, while achieving 50-100 times sensitivity enh

75 ferromagnetically coupled to yield a ground multiplet with S = 2.

76 As different multiplets within a given molecule accumulate various am