ライフサイエンスコーパス: spectra

1 constants are obtained from in situ infrared spectra.

2 al particles' environment on the recorded IR spectra.

3 is absorption spectra, and photoluminescence spectra.

4 s metabolites as they have the same emission spectra.

5 negative ion mode to obtain glycolipid mass spectra.

6 antly affects viral mutation frequencies and spectra.

7 ysis of the time-domain Brillouin scattering spectra.

8 gnal generation is inherently encoded in the spectra.

9 significantly improve localization in AI-ETD spectra.

10 o generate a ratiometric signal with varying spectra.

11 the role these isomers might play in the IR spectra.

12 riation across the common- and low-frequency spectra.

13 ctra are lower than those of the original FT spectra.

14 images, quantitative color changes, and mass spectra.

15 the experimental two-dimensional electronic spectra.

16 times, isotopic patterns, full MS, and MS/MS spectra.

17 sotropy, fluorescence lifetime, and emission spectra.

18 tetra- and pentamer, revealed from their IR spectra.

19 e sequences read directly from the resulting spectra.

20 iently been obtained and characterized by CD spectra.

21 been assigned using TD-DFT simulation of ECD spectra.

22 o applicable to first- and higher-order (1)H spectra.

23 tion (MALDI), while producing higher quality spectra.

24 to avoid the congestion inherent to protein spectra.

25 red significant variance in the fluorescence spectra.

26 o quantify proteoforms across multiple MS(1) spectra.

27 process, could be monitored through the NMR spectra.

28 s to the commonly observed smooth generation spectra.

29 diatropic and produced porphyrin-like UV-vis spectra.

30 nce to a nontrivial topology of gapped Dirac spectra.

31 rochemistry, and variable-temperature UV-Vis spectra.

32 lico and compare these to experimental MS/MS spectra.

33 ent light angles, resulting in a Mie scatter spectra.

34 MS(2) acquisition using bordering full-scan spectra.

35 was achieved based on the recorded (1)H NMR spectra.

36 ns showed quenching behavior in the emission spectra.

37 ly measure high-resolution linear absorption spectra.

38 r descriptors of a drug, and terahertz (THz) spectra.

39 ngs, indicated by Mo K-edge X-ray absorption spectra.

40 ), 2D-IR, and vibrational circular dichroism spectra.

41 etabolites could be identified by their HRMS spectra.

42 to directly compare unidentified tandem mass spectra.

43 m, resulting in a closer resemblance to bulk spectra.

44 rise to changes in the luminescence and NMR spectra.

45 y noise dropped close to zero with the first spectra acquired 7 minutes after introduction of the ant

46 iscovered by accurate mass and comparing MS2 spectra (acquired in ddMS2 mode) with spectral libraries

47 Measured spectra agreed well with those predicted.

48 Furthermore, vibrational spectra aid in identifying species and adsorption sites

49 (15)N NMR spectra allow the extraction of four H37 pKas and show t

50 that can be overlapped with reference XANES spectra, allowing this method to be used for fingerprint

51 ID spectra and that of UVnovo on CID or UVPD spectra alone.

52 The mass spectra also indicate the isocitrate dehydrogenase mutat

53 Circular dichroism spectra also supported these evidences indicating that h

54 ences exist in mutation rate and/or mutation spectra among HIV types (i.e., HIV-1 versus HIV-2) and a

55 friction, and the nanoscale current-voltage spectra analysis indicates that the rectifying Schottky

56 intensification of absorbance peaks in FTIR spectra and a systematic change in shape and intensity o

57 hexamer through the analysis of vibrational spectra and appropriate structural order parameters as a

58 We examined the size spectra and biomass of coral reef fish communities at 38

59 By analyzing optical spectra and by DFT computations we show that the HT prop

60 peptide sequencing algorithms annotate MS/MS spectra and deduce peptide/protein information without a

61 sents the first electronically resonant DOVE spectra and demonstrates the capabilities for analytical

62 ul tool for increasing charge states in mass spectra and generating unfolded ion structures, yet key

63 UV spectra and high resolution product ion spectra of the f

64 The nanosecond electronic spectra and kinetics of the radical pairs from various c

65 More precisely, plasmonic extinction spectra and near-field enhancement are described through

66 comparison of the NMR and circular dichroism spectra and of the specific optical rotations.

67 By recording the full fluorescence spectra and super-resolved positions of approximately 10

68 exceeds that of PEAKS and PepNovo on the CID spectra and that of UVnovo on CID or UVPD spectra alone.

69 he overlap of paper and fluorophore emission spectra and the fluorescence intensity on an imaging sys

70 ation between the shape/magnitude of the XRD spectra and the tissue type.

71 ectra correlate with experimental absorption spectra and the vibrational modes of calculated absorpti

72 ional properties such as fast neutron energy spectra and time-dependent neutron count rates were attr

73 Excitation spectra and time-resolved photoluminescence measurements

74 oach that simulates (13) C multiplets in NMR spectra and utilizes mass increments to obtain long-rang

75 The morphology, photoluminescence (PL) spectra and UV-vis spectra of these nanostructures were

76 ce, scanning electron microscopy, UV-Visible spectra and X-ray diffraction pattern.

77 of transport in aperiodic media with fractal spectra, and additionally demonstrate logarithmic sub-di

78 hotoelectron spectroscopy, UV-vis absorption spectra, and photoluminescence spectra.

79 Light intensity, spectra, and timing are important for SCN synchronisatio

80 LipidHunter resembles a workflow of manual spectra annotation.

81 We show that recorded spectra are highly dependent on the cluster morphology a

82 another after membrane binding; all other CD spectra are linear combinations of the two.

83 tions, and the noise levels in the resulting spectra are lower than those of the original FT spectra.

84 els, a total of 262,144 neutron transmission spectra are measured concurrently.

85 hroughput glycan sequencing software, glycan spectra are predominantly sequenced manually.

86 The SERS spectra are recorded simultaneously with the SPR sensorg

87 limited contribution to the resulting MS(2) spectra are removed.

88 a challenge, even if three-dimensional (3D) spectra are used.

89 f Sc is also indicated by the eight-line EPR spectra arising from the I=7/2 (45) Sc nucleus.

90 ns appear in cross-polarized two-dimensional spectra as distinct resonances with respective approxima

91 st-squares (MCR-ALS) was applied to the UVRR spectra, as well as off-line HPLC measurements, to enabl

92 oelectron data, which shows depletion in the spectra assigned to (HCOO(-))(H2SO4), and has also been

93 Having thus obtained accurate mass spectra at high resolution, we found that natural isotop

94 MS/MS spectra available for 828 of these annotations were anal

95 early receptor current amplitude and action spectra between WT and the Opn4-expressing Drosophila fu

96 R programming language, corrects the raw MS spectra both for the naturally occurring isotopes and fo

97 night-time lighting systems differed only in spectra, but not in intensity.

98 ation method was developed to analyze the IR spectra by novel pattern-recognition and statistical too

99 Mie scatter spectra can be detected within a few seconds without ski

100 e observed in real networks, their actuation spectra can be dramatically different.

101 r dissolving the silica matrix, the (1)H NMR spectra can be resolved for every single component of th

102 The resulting EIEIO spectra can be used to discern cis and trans double-bond

103 The consequent isotopic envelopes in mass spectra can reveal the ion stoichiometry but not geometr

104 n accurately reproduce the full Chl emission spectra - capturing the spectral dynamics associated wit

105 stematically compared to the FTIR absorption spectra collected for kerogen samples isolated from Manc

106 z- to terahertz-frequency infrared and Raman spectra contain a wealth of information concerning the s

107 tion and multipeaked fluorescence excitation spectra correlate with experimental absorption spectra a

108 Both in-vitro and ex-vivo spectra correlated well, showing for the first time that

109 ne fluidity can be obtained if time resolved spectra could be measured at each cell location.

110 t they possess different melting points, NMR spectra, crystal structures, and stacking patterns in th

111 (1)H-NMR spectra datasets of serum, urine, cortex, and stomach ti

112 magnetic susceptibility data, and Mossbauer spectra demonstrate that 1 has a low-spin (S = 1/2) ferr

113 nd antioxidants were confirmed by FTIR where spectra displayed a shift of the amide-III peak.

114 Structural changes observed in the Raman spectra during permeabilization indicated acyl chain dis

115 ed on the in situ-obtained UV/Vis absorption spectra during the reaction, we propose two different ex

116 ted (GC x GC/MS), allowing high-quality mass spectra (EI) to be obtained for the individual compounds

117 parallel factor analysis of the fluorescence spectra enabled monitoring of multiple types of organic

118 oth the standard result output and by visual spectra evaluation).

119 sical attributes including narrower emission spectra, excimer -based white emission, and thermally ac

120 For each oligomer, the UV spectra exhibit distinct changes in the electronic envir

121 Spectra extracted from allochthonous DOM were highly sim

122 esults show that extensive sampling of force spectra, facilitated by robot-enhanced AFM, can help rev

123 -based spectral library containing consensus spectra for 1829 compounds.

124 (EThcD) provides exceptional data-rich MS/MS spectra for direct and unambiguous pyrophosphosite assig

125 functional theory calculations of the X-ray spectra for the excited electronic singlet and triplet s

126 e vibrational modes of calculated absorption spectra for the neutral Trp radical.

127 sed approach to the generation of protein CD spectra from atomic coordinates.

128 volatile organic compounds (VOC) spectra from coffee samples of 7 Arabica and 6 Robusta c

129 TREND reads spectra from many spectroscopies in the most common form

130 ate signature in the electron kinetic energy spectra from mixed Xe core - Ar shell clusters ionized b

131 approach to enable researchers to produce CD spectra from protein atomic coordinates.

132 re performed on the secondary ion images and spectra from selected regions of interest.

133 ations used to guide the acquisition of SIMS spectra from the cells.

134 mplete overlapping of random and aligned RBS spectra from the sample with T g = 700 degrees C indicat

135 is capable of obtaining two-dimensional (2D) spectra from three spatial dimensions.

136 Binding gave quantifiable changes in the EPR spectra from which binding profiles could be obtained th

137 However, these spectra generally have a large number of contributions r

138 or acquisition of high-resolution mutational spectra (HRMS) during the process of hepatocarcinogenesi

139 lysis (TG-DSC-FTIR) and High-resolution mass spectra (HRMS).

140 observations of iPTF14hls, an event that has spectra identical to a hydrogen-rich core-collapse super

141 o split in differential ion mobility (FAIMS) spectra in a manner dependent on the ion geometry and bu

142 This enables us to observe high-resolution spectra in a single ion (CaH(+)) and coherent phenomena

143 From the SFG spectra in the C-H and O-H regions, we found that the su

144 measuring of NIR (760nm excitation) emission spectra in the skin.

145 Comparison of mass spectra in the two systems reveals similar features obse

146 bserved by combining emission and excitation spectra in two-dimensional representations.

147 The T2DIR spectra indicate that the macrocycle adopts a boat-like

148 The fluorescence spectra indicate that the singlet excited states of thes

149 X-ray absorption spectra indicated that U(IV) in both hematite and lepido

150 Analysis of the NIR and IR spectra indicates that the polaron is delocalized over 2

151 The analysis of numerically modeled Dol mass spectra is a novel method to follow modulation of the co

152 content of nuclear magnetic resonance (NMR) spectra is routinely used to identify and characterize m

153 e 3D concentration maps based on vibrational spectra, label-free; however, when using any optical ima

154 tomated tool we designed for exhaustive mass spectra matching, the promiscuity of binding of cisplati

155 These changes in the hail size spectra may imply a weakened intensity of hailstorms in

156 ton absorption bands in transient absorption spectra measured by our group for oligomers (1, 2, and 3

157 evaluate the capabilities of PROSPECT-MP for spectra modelling and pigment retrieval.

158 encing based on matched pairs of tandem mass spectra (MS/MS) obtained by collision induced dissociati

159 nformation) is provided to overcome the PTIR spectra nonlinearity.

160 Reference spectra normally are collected under specific conditions

161 In addition, the Raman spectra not only indicated the morphological changes tha

162 extends the scope of the library to include spectra of "nearest-neighbor" compounds that differ from

163 eap method based on the acquisition of FT-IR spectra of 3g/L hydroalcoholic tannin solutions, overcom

164 termolecular interactions on the vibrational spectra of a N-N'-bis(2,6-diisopropylphenyl)-perylene-3,

165 NOE-derived distance restraints, and the NMR spectra of a series of designed eta-helices were altoget

166 r poor physicochemical properties and narrow spectra of activity have limited their utility.

167 rs (10 Si atoms/molecule) dominated the mass spectra of aerosols at higher mass loadings, while ring-

168 nor 10 Si atoms/molecule) dominated the mass spectra of aerosols at lower mass loadings.

169 Detailed NMR spectra of all complexes as well as IR and single crysta

170 exploration, increased thigmotaxis, abnormal spectra of basic behavioral activities, impaired muscle

171 ectra of the S2 state and flash-induced FTIR spectra of both D1-N87A and D1-N87D PSII core complexes

172 products display classical UV-vis electronic spectra of carbo-benzenes in solution (lambdamax = 445.5

173 lculation for the two-dimensional electronic spectra of Cholorobaculum tepidum which correctly descri

174 Vibrational progressions in the NIPE spectra of ECX(-) were assigned to the symmetric and the

175 report the direct measurement of the energy spectra of electrons emitted from single layer graphene

176 his theory to study near-infrared absorption spectra of excitons in oligomers of the ubiquitous conju

177 The obtained mass spectra of five pure polycyclic aromatic hydrocarbons as

178 However, the mutation spectra of genes involved in OGID and cancer differ, sug

179 hich have been used to interpret vibrational spectra of ionic liquids, helping the reader to distingu

180 NMR spectra of isolated MOS indicated minimal amounts of bra

181 In this study, mass specific absorption spectra of laboratory-generated smoldering wood particle

182 This is particularly well-suited for spectra of mAbs, where some of the individual peaks migh

183 ples were correctly classified using the NIR spectra of milk dried on paper.

184 tes factors controlling single particle mass spectra of nascent supermicron SSA.

185 rier transform infrared (ATR-FTIR) and Raman spectra of non-extracted seed material have been recorde

186 recently been reported in understanding the spectra of particles with well-defined geometries, we re

187 rs by comparison with a library of DESI mass spectra of pathologically determined tissue types.

188 tanding the origin of beating signals in the spectra of photosynthetic complexes has been given consi

189 redshift both in the absorption and emission spectra of QDs occured.

190 erved from chemical shift changes in the NMR spectra of residues in the helices and on the surface of

191 pal component analysis applied to the UV-vis spectra of saffron aqueous extracts revealed a clear dif

192 volving soft ionization high-resolution mass spectra of SCCP mixtures.

193 light sensitivity of plants under the broad spectra of solar radiation in nature.

194 However, these organisms exhibit rates and spectra of spontaneous mutations similar to MMR-bearing

195 e technique of single electron spectroscopy, spectra of states in CS2 and SF6 with a double hole in t

196 um absorption, which is commonly seen in the spectra of subluminous ones.

197 We were able to produce high-quality NMR spectra of substrate bound to microcrystalline LeuT samp

198 Additionally, the infrared excitation spectra of the 1800 nm luminescence, as well as the visi

199 uired 4D (H)COCANH, (H)CACONH, and (H)CBCANH spectra of the 20 kDa bacteriophage tail-tube protein gp

200 inescence, as well as the visible excitation spectra of the 522 nm and 652 nm luminescence, of (A) Er

201 rption band intensity in diffuse reflectance spectra of the adsorbent, which was used for their direc

202 lity to specific antibiotics based on the IR spectra of the bacteria.

203 The TXRF spectra of the compounds were measured using variable X-

204 Moreover, the vibrational spectra of the excimer state show that it assumes a geom

205 UV spectra and high resolution product ion spectra of the five compounds also supported their ident

206 Captured images and resulting absorbance spectra of the gold nanoparticle, glutathione, and amino

207 rimposable but differ significantly from the spectra of the monomer and trimer.

208 The direct (13)C NMR and EPR spectra of the nitroxide free radicals and the oxoammoni

209 The MS/MS spectra of the peroxy acids showed fragmentation pattern

210 We showed that the solid-state spectra of the radical pairs are very similar to those d

211 EPR spectra of the S2 state and flash-induced FTIR spectra o

212 The UV spectra of the tetra- and pentamer are superimposable bu

213 f binding to two sites directly from the NMR spectra of the titrations.

214 iver networks, we investigate the eigenvalue spectra of their adjacency matrix.

215 nded X-ray absorption fine structure (EXAFS) spectra of these As-bearing pyrites are explained by loc

216 y, photoluminescence (PL) spectra and UV-vis spectra of these nanostructures were studied.

217 Shifting the action spectra of these proton pumps beyond 700 nm would genera

218 d which allows normalisation of the emission spectra of these PTMs to the fluorescence intensity of T

219 ere, we show that the optical 2D photon echo spectra of this complex at ambient temperature in aqueou

220 Variations in the enhanced Raman spectra of three peptide ligands (i.e., cyclic-RGDFC, cy

221 ement between computational and experimental spectra of Ti K-edge, we identified key spectral feature

222 X-ray absorption spectra of Tl adsorbed onto Na-exchanged IdP indicated a

223 ence-UV spectra were obtained by subtracting spectra of unheated and denatured protein solutions at d

224 To this end, the mass spectra of unlabeled metabolites measured in two media a

225 By comparing the FTIR spectra of wild-type enzyme and two mutagenesis variants

226 we collect two-dimensional infrared (2D IR) spectra on tissue slices of porcine eye lenses.

227 All automatically annotated spectra output by the workflow are provided in the Suppo

228 Glycoforest annotated an additional 50 MS/MS spectra overlooked during manual annotation.

229 Spectral acquisition rates of more than two spectra per second were demonstrated.

230 gmentation rules are combined with in silico spectra prediction programs CFM-ID and MS-FINDER to deri

231 These mass spectra provide direct information on tumor infiltration

232 cally learn from and interpret fragmentation spectra, provided a representative set of training data.

233 The device provided high-quality spectra, regardless of the sample height at the measured

234 the goal of providing red-shifted absorption spectra relative to previously synthesized COE analogs.

235 s demonstrate that bacterial glycolipid mass spectra represent chemical barcodes that identify pathog

236 nounced features in their circular dichroism spectra resulting solely from topological chirality.

237 ed on the stiffest matrices, and fluctuation spectra reveal a high nuclear tension that matches trend

238 istical analysis of their observed DART-HRMS spectra revealed intraspecies similarities and interspec

239 xtracting the dynamic Stokes shift from 2DES spectra revealing an ultrafast solvent relaxation.

240 (15)N heteronuclear single quantum coherence spectra reveals disruption of the tertiary contacts amon

241 experimentally measured N K-edge absorption spectra, reveals the different nature of the electronic

242 e to the scan duty cycle but generates MS/MS spectra rich in b/y-type and c/z(*)-type product ions.

243 Furthermore, (31)P and (2)H solid-state NMR spectra show that liquid crystalline 1,2-dimyristoyl-sn-

244 Both the experimental and calculated far-IR spectra showed a red shift of the low-frequency peaks up

245 her BRCA1 or BRCA2, and the arising mutation spectra showed strong and specific correlation with a mu

246 son of electrospray ionization (ESI) and LDI spectra showed that different types of compounds are ion

247 than iron.) We identify line features in the spectra that are consistent with light r-process element

248 Both samples provide XANES spectra that can be overlapped with reference XANES spec

249 tres) and featureless nature of fluorescence spectra that limits the number of resolvable colours to

250 ture and excitation power dependent emission spectra, thermal quenching ratios, fluorescence intensit

251 al from the purified proteins provides basis spectra to analyze the signals in cells.

252 rement by relating the fit residual of noisy spectra to the standard deviation of the measured FRET e

253 with infrared absorption and resonance Raman spectra using a Styryl 9 M dye as a model system.

254 etermination of HIV mutation frequencies and spectra using the Illumina sequencing platform.

255 among systematic sets of 2D NMR fingerprint spectra using the NISTmAb and illustrate how spectral va

256 utational simulation of the experimental EPR spectra, using a developed algorithm for J modulation in

257 low for the simultaneous acquisition of mass spectra via Fourier transform (FT) techniques (frequency

258 Here we calculate PTIR spectra via thin-film optics, to identify subtle changes

259 re and collecting data-dependent tandem mass spectra was also demonstrated.

260 A portion containing 521 spectra was manually checked confirming that Glycoforest

261 From neutron scattering spectra, we confirmed that the B. subtilis cell membrane

262 Using these resulting high-quality spectra, we identified a xxxxxxKSxxxxx modification moti

263 To interpret these paired spectra, we modified the UVnovo de novo sequencing softw

264 Raman spectra were acquired in mapping mode from multiple spot

265 tions in dTL on the current densities and IR spectra were analyzed and discussed.

266 on mucosa O-linked glycomes) for which MS/MS spectra were annotated manually.

267 ied all isolates after appropriate reference spectra were created and added to commercial databases.

268 99.0% of the variation between the spectra were described by the first two principal compon

269 The absorption and emission spectra were found to be widely tunable on the basis of

270 The cage structures and UV/Vis spectra were independently confirmed by state-of-the-art

271 The resulting spectra were modeled by (time-dependent) density functio

272 Five different parameters of difference-UV spectra were obtained by subtracting spectra of unheated

273 The oxyresveratrol emission and excitation spectra were obtained for first time.

274 EPR spectra were obtained for the spin-labeled ligands both

275 High-quality spectra were obtained from PPG particles down to 13 nm i

276 High-quality and reproducible SERS spectra were obtained using reporter-modified gold nanop

277 In the proposed method all spectra were obtained with no sample preparation.

278 The resulting XRD spectra were subjected to principal component analysis (

279 These spectra were sufficient to obtain complete resonance ass

280 The computed spectra were then systematically compared to the FTIR ab

281 aromatic hydrocarbons, nicotine) in the mass spectra were used to assign PMF factors to biomass burni

282 MS, and their fragmentation patterns (MS/MS spectra) were identified.

283 laser pulses containing very broad frequency spectra where their amplitudes and phases are mutually c

284 The simulated NIPE spectra, which are based on the calculated Franck-Condon

285 d for generating 1.8-4.2 mum super broadband spectra, which can be used to seed both the signal of th

286 as an initial step, the calculation of their spectra, which has been inaccessible to most users due t

287 cies were used to create reference MALDI-TOF spectra, which were then used for the identification of

288 xchange leads to a blue-shift of the optical spectra, while maintaining the high photoluminescence qu

289 -based sensor device records single-spin NMR spectra with 13 Hz resolution at room temperature.Dissip

290 preparation (30min) and provided clear SERS spectra with characteristic Raman bands of histamine.

291 Comparison of the time-resolved IR spectra with DFT computations allowed to unambiguously i

292 paring electronically resonant TRSF and DOVE spectra with each other and with infrared absorption and

293 within single cells and compare the temporal spectra with existing theoretical models to gain insight

294 imation, to the direct comparability of PTIR spectra with far-field infrared databases.

295 solution multidimensional nonlinear coherent spectra with frequency combs.

296 rned sensor can be converted to fluorescence spectra with high signal-to-noise ratio and calibrated i

297 by monitoring the variation of the harmonic spectra with the carrier density.

298 on the comparison of the observed transient spectra with the one obtained from an independently gene

299 ry methods reveals that single-particle mass spectra with weak sodium ion signals can be produced by

300 , all the zein preparations had similar FTIR spectra, with greater alpha-helical conformation, than t