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 up to five times smaller than the (19)F NMR line width.

5 s, we investigate their impact on V2 optical line width.

6 operties, including field-response range and line width.

7 in filament line spacing and +/- 0.022 mm in line width.

8 lications is a narrow photoluminescence (PL) line width.

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

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

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

12 hibits few poorly dispersed peaks with broad line widths.

13 ces more poorly dispersed peaks with sharper line widths.

14 lved from each other within their respective line widths.

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

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

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

18 articles, which caused unfavorably large NMR line widths.

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

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

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

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

23 l Stokes shift (110-120 meV) and a narrow PL line width (112 meV at 728 nm).

24 parameters to achieve a 12 parts per billion line width; (2) sensitivity, with searches and refinemen

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

26 Detailed line width analyses slightly favored an equal line width

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

28 Line width analysis shows that ligand off rates are slow

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

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

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

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

33 54 microm, 118 microm, and 132 microm for EZ-line width and horizontal and vertical ring diameters, r

34 By using EZ line width and horizontal diameter as parameters of dise

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

36 The ellipsoid zone line width and hyperautofluorescent ring horizontal diam

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

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

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

40 e advantage of Nd(3+) emission is its narrow line width and NIR emission, which is enhanced by ~3000

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

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

43 Their EPR spectroscopic properties line width and relaxation times influence their performa

44 EZ line width and ring diameter rates of disease progressio

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

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

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

48 the rather narrow room-temperature emission line width and the absence of significant spectral diffu

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

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

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

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

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

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

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

56 6-methylation of the TpA adenine on both the line widths and its local structure.

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

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

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

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

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

62 ere extracted-Cramer-Rao lower bound (CRLB), line width, and coefficient of variation.

63 ion, increased effective Q-factor, decreased line width, and improved sensitivity.

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

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

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

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

68 et-triplet energy splitting, narrow emission line widths, and high photostability enhance their perfo

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

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

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

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

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

74 Narrow emission line widths are needed to ensure both color and single-p

75 n dynamics is valid, but such "exact" phonon line widths are not essential to obtain accurate magneti

76 tral parameters, such as chemical shifts and line widths, are sensitive to both the nature of the flu

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

78 y, structure, and mechanics, enables printed line widths as fine as 20 mum, surpassing commercially a

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

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

81 in MOF (13)C NMR peak positions and (1)H NMR line widths, as well as dramatic reductions in the MOF (

82 led TPA based on the significantly different line widths associated with entangled and unentangled pr

83 the pressure dependence of the NMR resonance line-widths associated with a maximum in hydrogen mobili

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

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

86 signals (i) vary in intensity, position, and line width between spectra and (ii) interfere with many

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

88 ider spectral dispersion and narrower signal line width but is barely used in metabolomics due to its

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

90 They cover a wide range of EPR line widths but have in common a cysteine-targeting meth

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

92 rspectral deviations of signal positions and line widths can be pronounced; hence, interferences cann

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

94 on in line widths respectively, evident from line width changes in the NMR spectra.

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

96 agonist-bound complexes with sensitivity and line widths closely comparable to those achieved using s

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

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

99 2 without refolding exhibited heterogeneous line widths, consistent with an acid-denatured molten gl

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

101 3/Ca(2+) complexes, indicated by (13)C ssNMR line widths, continues to increase beyond 27 ms.

102 EZ line width declined at a rate of -123 +/- 8 um per year,

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

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

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

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

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

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

109 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

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

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

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

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

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

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

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

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

118 urrent state of the art in terms of emission line width for a variety of colloidal materials includin

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

120 s that for the dendrimers being studied, the line width for ETPA is orders of magnitude narrower than

121 initio determination of phonon lifetimes and line widths for a molecular magnet to prove that the com

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

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

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

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

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

127 , demonstrates the capability to improve NMR line width from 84 to 4 Hz in a 1.05 T preclinical MRI s

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

152 blue perovskite LEDs, the emission spectrum line width is broadened to over 25 nm by the coexistence

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

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

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

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

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

158 Due to spin-spin relaxation and line width limitations, it has been difficult to determi

159 zle geometry, resulting in ultrafine traces (line width < 6 mum, overspray < 0.1 mum).

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

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

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

163 Neonatal line width measured within 3 portions of the tooth crown

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

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

166 1D solid-state NMR line width measurements of singly 13C carbonyl labeled p

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

168 NMR line width measurements provided similar exchange rates

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

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

171 45)Nd, (146)Nd, (148)Nd, and (150)Nd) with a line width narrowed to 0.1 pm, significantly improving u

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

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

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

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

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

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

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

179 ) = 3.347 G, and (4)A((14)N) = 0.765 G and a line width of 0.24 G), and theoretical calculations supp

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

181 skite LEDs, the first to exhibit narrowband (line width of 18 nm) and spectrally stable (no wavelengt

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

197 Moreover, the line width of the (13)C=(18)O peak is highly sensitive t

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

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

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

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

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

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

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

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

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

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

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

209 d to printing without acoustic focusing, the line width of the traces decreases to 60 +/- 5% while th

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

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

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

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

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

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

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

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

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

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

220 pendent exciton radiative rates and emission line widths of CsPbBr(3) quantum dots at the single part

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

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

223 However, line widths of individual Ile residues are directly link

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

225 n in (1)H NMR spectra in which positions and line widths of signals were predicted from a constant me

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

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

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

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

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

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

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

233 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-

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

235 gressive decrease of the ellipsoid zone (EZ) line width on spectral domain optical coherence tomograp

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

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

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

239 J-resolved spectroscopy and line width reduction by picric acid addition aided in re

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

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

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

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

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

245 Subnatural line width resonant inelastic X-ray scattering allowed u

246 ing in approximately 63 and 25% reduction in line widths respectively, evident from line width change

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

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

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

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

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

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

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

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

255 mitting diodes (LEDs) with a narrow emission line width that emit between 620 and 635 nm are needed t

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

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

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

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

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

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

262 at least 10-fold narrower spectral-resonance line widths, thereby significantly increasing our precis

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

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

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

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

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

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

269 In this cohort study, neonatal line width was associated with exposure to maternal peri

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

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

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

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

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

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

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

277 ide estimates of the excited state radiative line width, which we relate to the entangled two-photon

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

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

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

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