ライフサイエンスコーパス: line width

1 of cross-peaks, but some general increase in line width.

2 lipid-to-water ratios, lipid fractions, and line width.

3 ctra of YZ. and YD. differ in line shape and line width.

4 ed by merging the splittings with the signal line width.

5 residues have amide I bands with >20 cm(-1) line width.

6 articles, which caused unfavorably large NMR line widths.

7 roduces many well-dispersed peaks with sharp line widths.

8 hibits few poorly dispersed peaks with broad line widths.

9 ces more poorly dispersed peaks with sharper line widths.

10 d 15N- and 15N/13C-labeled protein to narrow line widths.

11 r the enzyme as measured by TRNOE or 31P NMR line widths.

12 tions, as well as changes in peak height and line widths.

13 etime, and excited-state chemical shifts and line widths.

14 nL, high-resolution 300-MHz 1H-NMR spectra (line width, 0.6 Hz) are presented of 10 mM alpha-bag cel

15 G, which are equal or close to the narrowest line width (1.5 G) of the common DPPH standard in the fo

16 by independent measurements of the intrinsic line width (1.6 kHz from T2e experiments) and the effect

17 Measurements of pH-dependent 1H line-width also demonstrate that the C.C mispairs are mo

18 Detailed line width analyses slightly favored an equal line width

19 NMR experiments (TRNOE and 31P line width analyses) were carried out to investigate the

20 Line width analysis shows that ligand off rates are slow

21 a) = 79 meV) was derived from the (45)Sc NMR line-width analysis.

22 The changes in line width and center frequency demonstrate that the unf

23 Luminosity-line width and Dn-sigma methods are less accurate for an

24 oublet to a wide singlet of slightly smaller line width and finally to a 25-G narrow singlet.

25 54 microm, 118 microm, and 132 microm for EZ-line width and horizontal and vertical ring diameters, r

26 Measurement of the ellipsoid zone (EZ) line width and hyperautofluorescent ring diameters was p

27 The ellipsoid zone line width and hyperautofluorescent ring horizontal diam

28 Titin filaments may specify Z-line width and internal structure by varying the length

29 uble resonance spectra, it exhibits a larger line width and larger 8alpha-methyl proton splittings, c

30 R signal underwent a continuous reduction in line width and lost intensity as the incubation time inc

31 Because line width and patterning speed in DPN are independent o

32 pid bilayer, the sinusoidal trend of the SFG line width and peak-center frequency suggests that the p

33 resolution by simultaneously reducing proton line width and spectral crowding despite a high local pr

34 d linear growth correlated strongly with the line width and splitting of the C horizontal lineC pheny

35 istically significant progression rate in EZ line width and SW-AF ring diameters over time, verifying

36 unfolded protein increases its inhomogeneous line width and the center frequency shifts as the temper

37 Reductions in (13)C NMR line widths and changes in chemical shifts upon complex

38 dentified by monitoring perturbations in the line widths and chemical shifts of cross peaks in the HS

39 The temperature dependence of the line widths and chemical shifts of the 19F resonances we

40 The EPR line widths and collision accessibilities of 18 spin-lab

41 The calculated spectra predict the line widths and frequencies nearly quantitatively.

42 ne width on lipid composition, with narrower line widths and hence greater structural order observed

43 6-methylation of the TpA adenine on both the line widths and its local structure.

44 l three materials show very similar broad PL line widths and large Stokes shifts.

45 mobility by observing the corresponding (1)H line widths and line shapes in water-saturated spider dr

46 -seven spectra in 25 individuals with narrow line widths and low lipid content were adequate for quan

47 neration was determined from the SEC elution line widths and the spectral homogeneity of the elution

48 the resonances of the active site, resonance line widths and the T1 of a ligand proton are not signif

49 From the SFG spectral peak-center frequency, line width, and polarization dependence of the isotope l

50 n of a capillary spinner to improve spectral line widths, and (3) facile sample changing via the use

51 luminescence quantum yields, narrow emission line widths, and considerable air stability.

52 al shifts, no significant differences in NMR line widths, and few differences in the number of detect

53 MR signal intensities, site-specific MAS NMR line widths, and NMR-detected hydrogen-deuterium exchang

54 vere relaxation (to T(1) approximately 3 ms, line width approximately 1.5 kHz) of two of the protons.

55 conductivities measured with different metal line widths are analyzed using suppression functions cal

56 (sigma = 0.5-2%) are obtained whose spectral line widths are dominated (73-83%) by the intrinsic sing

57 of the protein on a timescale such that the line widths are more characteristic of the molecular wei

58 cal in the menG mutant has a similar overall line width as that for the wild type, but consistent wit

59 salt delivers reduced feature sizes down to line widths as small as 78 nm, a level of structural int

60 --exceeding 10 microm/s--writing speeds with line-widths as small as 50 nm.

61 long (>10 ms) to be manifested in increased line widths, at least up to 41 degrees C.

62 ectrum of this label exhibits an increase in line width because of a decrease in label dynamics, and

63 onsequence, provided high sensitivity of the line-width broadening to pO(2) (DeltaH/DeltapO(2) approx

64 We pattern 1D metallic grating of various line widths but fixed gap size on sample surfaces.

65 assy matrix, electron decoupling reduces the line widths by 11% (47 Hz) and increases the intensity b

66 No significant EPR line width change is detected after exchange into D(2)O

67 aggregates, as indicated by 13C and 15N NMR line widths, chemical shifts, and electron microscopy.

68 tures over large areas, leading to resonance line-widths comparable to that of the ideally uniform st

69 state rCcP(H52L) the comparatively large NMR line widths compromise resolution, but two specific enzy

70 2 without refolding exhibited heterogeneous line widths, consistent with an acid-denatured molten gl

71 Here we show that the observed 2D line width contains valuable information on strain varia

72 ed enzyme moved from 5.4 to 2.2 ppm, and the line width decreased from 73 to 16 Hz, providing the fir

73 The theoretical line width decreased monotonically with the degree of pr

74 We observed on average, EZ-line widths decreased by 140 microm (5.2%, p < 0.001) pe

75 The EPR spectral values of the inverse line width (Delta H (-1)) and of the width between the l

76 : amplitude (A), integral intensity (I), and line-width (DeltaBpp); g-Factor was obtained from resona

77 C60*+ salt gives a signal with much greater line width (DeltaH(pp) = 6-8 G).

78 10(18) spins/g of soil, with a g-factor and line width (DeltaHp-p) of 2.00311-2.00323 and 4.190-5.47

79 of amines while obtaining between 1 and 2 Hz line width, demonstrating the ability to avoid electroph

80 functional B-cluster) and because the 13CO2 line width does not broaden.

81 chitectures in two and three dimensions with line widths down to 1 mum are formed.

82 nd topographic labeling, were patterned with line widths down to 15 nm or approximately 20 molecules.

83 on features in two and three dimensions with line widths down to one micrometer are formed.

84 Line width effects from isotopic labeling (13C and 2H) i

85 Furthermore, the obtained reduction in line widths enabled the use of multidimensional NMR meth

86 l shift dispersion and temperature-dependent line widths exhibited by folded and misfolded s-DAGK sup

87 Large increases in line width for all alpha(1)PI resonances in the covalent

88 demonstrated improved photoluminescence (PL) line widths for cadmium chalcogenide-based nanocrystals.

89 the (13)C dimension due to the narrow (13)C line widths for the identification of spin systems and c

90 Line widths for the metallic (93.42 meV) and two semicon

91 e spectral purity (in terms of narrow E(S)ii line widths) for the resulting ground-state complex sign

92 Improvement of spectral line width from 4.8 Hz to 3.5 Hz was observed at high sp

93 vertical diameter along with ellipsoid zone line width from spectral-domain optical coherence tomogr

94 P dynamics, T(1) relaxation times, and (13)C line widths have been compared.

95 ordinary stability in living tissues, narrow line width, high analytical resolution at micromolar con

96 trate and allow for top-down single-molecule line-width imaging.

97 -dependent changes, but none show changes in line width, implying that the flexibility of the oxidize

98 proton frequency and 40 kHz MAS rate, proton line widths improve further in an absolute sense (360 +/

99 Furthermore, the IR line width in anions can report a structural change acco

100 The (83)Kr line width in most of the studied cases is quadrupolar d

101 Changes in the hyperfine splitting and/or line width in spectra for l-3,3-[2H2]tyrosine-labeled, b

102 dependence of both the phonon frequency and line width in the low-temperature orthorhombic phase.

103 onclusion reached on the basis of (27)Al NMR line widths in field-swept NMR spectra acquired from 13

104 Membrane-bound RTD-1 exhibits narrow line widths in magic-angle spinning spectra, but the sid

105 Similar line widths in the spectra of apo and bound M2 indicate

106 NMR resonances is nearly constant while, (3) line widths increase exponentially with decreasing tempe

107 Narrower line widths indicate that the amide I backbone is solven

108 d zeolites where the field dependence of the line width indicates a distribution of isotropic chemica

109 nalysis of the homogeneous and inhomogeneous line widths indicates that the apo-M2TMP undergoes signi

110 fts, chemical shift anisotropies (CSAs), NMR line-width information, (13)C rotating frame relaxation

111 ations between the 2D 1 and 2D 2 split vs 2D line widths, intensities, and peak positions.

112 ing dynamic interactions; whilst the reduced line widths/intensities observed were mostly caused by w

113 nd (10,0) zigzag nanotubes, along with (n,m) line widths inversely proportional to their extinction c

114 The luminescence line width is 1.5 times larger in pristine graphane comp

115 Consequently, the 2D line width is a good and easily accessible quantity for

116 rimental evidence suggests that the spectral line width is a result of multiple, discrete electronic

117 While a similar reduction in line width is observed for the corresponding band arisin

118 A significant decrease in the EPR line width is observed when the radical is generated in

119 The magnitude of the excess line width is temperature dependent and reaches a maximu

120 the (31)P chemical shift anisotropy and the line width is used to determine headgroup mobility and m

121 ometer based on a 30 Hz/s stability, sub-kHz line width laser source coupled to a high-stability cavi

122 vative, p1TAM-D (DeltaHpp </= 50 mG, Lorentz line width, </=20 mG) results in high sensitivity to pO2

123 upled with their microscopic size and narrow line widths, may enable new applications in areas such a

124 Spectral simulation techniques and a simple line width measure were used to extract dynamical parame

125 The 13C line widths measured from 13C-13C 2D chemical shift corr

126 Line width measurements in 2D [(1)H,(1)H]-NOESY showed t

127 1D solid-state NMR line width measurements of singly 13C carbonyl labeled p

128 As an ancillary benefit, line width measurements of the ubiquitous tert-butyl alc

129 NMR line width measurements provided similar exchange rates

130 ed by X-ray photoelectron spectroscopy (XPS) line width measurements, for radii of the QDs, R > 2.4 n

131 t the setup can be used for inelastic phonon line-width measurements.

132 The line width narrowing is interpreted to be due to averagi

133 Above 20 K, the line width narrows dramatically as the broad low-tempera

134 N-Bmim(+), SeCN(-) samples its inhomogeneous line width nearly an order of magnitude faster than the

135 he TpA adenine is N6-methylated and that the line width no longer experiences a maximum as the temper

136 Line widths observed for R*-generated GTPgammaS/Mg(2+)-b

137 e absence of deuterium decoupling, the (13)C line widths observed for the deuterated samples are iden

138 he quadrupole couplings in the solid and the line widths observed in the corresponding solution 59Co

139 ) = 3.347 G, and (4)A((14)N) = 0.765 G and a line width of 0.24 G), and theoretical calculations supp

140 s at 370 and 406 nm, and an ESR peak-to-peak line width of 13.9 G.

141 f 1.2 G compared to a nondeuterated analogue line width of 2.1 G allowing for an increase of Overhaus

142 singlet tyrosyl radical with an overall EPR line width of 29-31 gauss (G) was generated by reaction

143 8), with a signal-to-noise ratio of 16 and a line width of 31 Hz after 3 h of total measurement time.

144 de-generated radical in MnPGHS-1 exhibited a line width of 36-38G, but was also able to convert AA to

145 sought to understand the unexpectedly narrow line width of 4-oxo-2,2,6,6-tetramethyl-1-piperidinyloxy

146 integrated circuit patterns, with a feature line width of 800 nm and a low sheet resistance of 205 o

147 The nonspinning line width of a decoupled [3-13C]-L-alanine (99%) peak a

148 ibits a g = 2.005 signal with a peak-to-peak line width of approximately 1.1 milliteslas at 150 K, ha

149 (2)O(2) revealed a single-line signal with a line width of approximately 10 G.

150 The line width of bulk H2(17)O is measured in the presence a

151 The PL line width of HgTe NPLs (40 nm full width at half-maximu

152 es in binding of G-6-P (monitored by the 31P line width of inorganic phosphate when G-6-P is added in

153 Increased disorder was observed as excess line width of proton resonances near the lesion site.

154 erons significantly decreased the individual line width of pTAM down to 40 mG and, as consequence, pr

155 The nonradiative decay and luminescence line width of pure graphane are governed by electron cou

156 in one-dimensional 1H NMR spectra as excess line width of the aromatic proton resonances.

157 The frequency and line width of the C-D bonds were easily observable and s

158 esis of the D2-H117 residue also altered the line width of the Chl(Z)(+) EPR signal, but the line sha

159 that is based on measuring the peak-to-peak line width of the EPR spectrum in the presence of the pa

160 The line width of the EPR spectrum is approximately 0.9 mT,

161 The electron paramagnetic resonance (EPR) line width of the flavin radical is indicative of a neut

162 The line width of the g = 2 signal becomes narrower, while i

163 The line width of the imino proton of the ClU residue is sub

164 mine the nonradiative lifetime and radiative line width of the lowest energy singlet excitations in p

165 An extraordinary low line width of the synthesized deuterated derivative, p1T

166 [d(CGAGGTTTAAACCTCG)]2 show that the excess line width of the TpA adenine-H2 is diminished when the

167 uniformly labeled samples exhibit (13)C NMR line widths of <2 ppm, demonstrating that the peptide, i

168 Chemical shifts and line widths of (83)Kr are moderately dependent on small

169 L149C/H93G double mutants depict peaks with line widths of 100 and 23 Hz, respectively.

170 pal g values of 2.089, 2.076, and 2.028, and line widths of 13.76, 16.65, and 5.41 G, respectively.

171 ave been created routinely, and on occasions line widths of 25 nm (lambda/10) have been achieved.

172 Biotin patterns with line widths of 5-20 microns were produced by varying the

173 The EPR spectra show broad signals with line widths of about 1000 G.

174 The temperature dependence of the line widths of carbon atoms of Zn-bleomycin strongly res

175 This value is similar to the fluorescence line widths of CNTs suspended in air.

176 relation was also found between the spectral line widths of coated SWCNTs and the efficiency of their

177 The NMR line widths of FGF-2 in the presence of the decasacchari

178 ally, the approach fully exploits the narrow line widths of glycans (nu1/2 < 3 Hz) in the (13)C spect

179 The line widths of Phe68 and Phe93 are broader than those of

180 The strongly phase-dependent static NMR line widths of the (1)H, (19)F, and (31)P nuclei in this

181 red-shifts up to 45 nm, exceptionally small line widths of the absorption and emission event (up to

182 Analysis of the line widths of the Bragg reflections in the neutron diff

183 used to rationalize the observation that the line widths of the C1 and C3 resonances are narrower whe

184 n both the FAD and 2Fe-2S center mutants the line widths of the neutral and anionic flavo-semiquinone

185 ally those obtained from measurements of the line widths of these proton resonances.

186 excellent alpha spectral resolution, having line widths of ~33 keV.

187 mation of a sharp singlet at g = 2.0048 with line-width of 5.3 G that is identified as the 8-oxo-7,8-

188 There was some dependence of line width on lipid composition, with narrower line widt

189 that sampled a portion of the inhomogeneous line width on the time scale of approximately 30 ps, whi

190 The values of the inverse line width parameter (deltaH0(-1)) from a family of Sp a

191 measurable influence on the absorption or PL line widths, produce small (+/-0.05), nonmonotonic chang

192 This coupling results in a sharpened NMR line width relative to a GaCu analogue, indicative of a

193 lent resolution, with narrow (13)C and (15)N line widths, representing a high degree of structural or

194 delocalized in these solvents, although the line width required to simulate the vibrational structur

195 ns with widths of only a few DBTs (sub-30 nm line-width resolution).

196 The observed line-width resonance shifts (Deltalambda > 1.7 mum) sugg

197 ation measurements are in agreement with the line width results, reflecting mobility differences and

198 mposed of sharp lines with twice the natural line width, shifted from the center by a random walk of

199 elix, but the low-temperature EPR spin probe line width showed that the probe lies more distant (> 15

200 Central narrow line width signals ("spikes") are ascribed to C120On- (n

201 ne shapes of the G-band features with narrow line widths similar to semiconducting tubes are converte

202 ations (second moment-based solid static NMR line width simulations) for the OIPC diethyl(methyl)(iso

203 ance exhibits a large downfield shift, large line width, steep temperature dependence, and a larger t

204 Holo-IFABP exhibits broader line width than the apo-form, suggesting more flexibilit

205 reveals an oscillation in the inhomogeneous line width that has a period equal to that of an alpha-h

206 the TpA step were also found to have excess line width that is diminished upon N6-methylation.

207 erpolarized (129)Xe NMR resonances of narrow line width that were shifted by 3.0-7.5 ppm downfield, s

208 MR spectrum of the native silk exhibits (1)H line widths that are approximately 40 kHz for all carbon

209 o prominent excitonic resonances with narrow line widths that are tunable from the mid-infrared to th

210 ach spatial position, and, from the observed line width, the localized tissue oxygenation can be mapp

211 Given the relative insensitivity of line width to PEG size, we anticipate that the biodistri

212 , were used to narrow the most of the carbon line widths to 0.5-0.8 ppm.

213 ine width analyses slightly favored an equal line width-unequal population ratio for the two diastere

214 aracterized their absorption frequencies and line widths using IR spectroscopy.

215 and a collagen-like peptide down to 30-50-nm line widths, using the atomic force microscopy technique

216 Signal intensities and line widths vary as a function of amino acid position an

217 The line width was ~12 G, indicating its neutral semiquinone

218 However, of seven mutants examined, the C-D line widths were independent of the redox-state of the p

219 The exchangeable proton resonance line widths were less affected by deuteration, indicatin

220 Line widths were minimized with fast breath-hold B0 fiel

221 At 500 MHz proton frequency, 1-ppm proton line widths were observed (500 +/- 150 Hz), and the sens

222 flurbiprofen nor diclofenac changed the EPR line width when added after peroxide.

223 The homogeneous phosphorescence line width, which can be measured in single-molecule exp

224 y equivalent protons exhibiting a narrow NMR line width while resonating at a (1)H NMR frequency dist

225 er transform ion cyclotron resonance (FTICR) line width with background damping gas pressure, under c

226 nescence intensity and narrowing of spectral line widths with electrolyte addition, indicating a chan

227 onance energy transfer efficiency values and line widths with increasing [Na(+)] are observed for the