ライフサイエンスコーパス: Fourier transform

1 orm becomes a special case of the fractional Fourier transform.

2 ical realizations of the discrete fractional Fourier transform.

3 butions of the particles as for the indirect Fourier transform.

4 cally evaluate a complex-to-complex discrete Fourier transform.

5 ection coefficients having uniform magnitude Fourier transforms.

6 Herein, use of large amplitude Fourier transformed ac voltammetry and comprehensive ana

7 ome the limiting O(nlogn) complexity of fast Fourier transform algorithms.

8 Using large amplitude Fourier transformed alternating current voltammetry (FTa

9 On the basis of Fourier transformed alternating current voltammetry meas

10 nterrogated for their redox properties using Fourier transformed alternating current voltammetry, whi

11 tudy, the impact of surface heterogeneity on Fourier-transformed alternating current voltammetry (FTA

12 es along the cob axis using a sliding-window Fourier transform analysis of image intensity features.

13 However, while conventional Fourier transform analysis of the 2DES data allows oscil

14 omposition can be determined by using a dual Fourier transform approach to obtain the average lipid m

15 ld find applications in various fields where Fourier transforms are essential tools.

16 al focal plane, as well as imaging and 1D/2D Fourier transforms, are observed on the same lens.

17 Here, we present a fast Fourier transform-based algorithm that can be used to de

18 ery property and application of the ordinary Fourier transform becomes a special case of the fraction

19 he periodic nature of the response, temporal Fourier transforms can be used to identify and quantify

20 ) underwent phase/frequency mapping (Hilbert/Fourier transforms; CARTO-Finder) of the left and right

21 esent a wide-field imaging implementation of Fourier transform coherent anti-Stokes Raman scattering

22 We present a Fourier-transform coherent anti-Stokes Raman scattering

23 o linearly increase with harmonic order in a Fourier transform electrostatic linear ion trap (ELIT) m

24 ehalose) structures, when investigated using Fourier transform far infra-red (FT-FIR) with synchrotro

25 ical soliton method for calculating the Fast Fourier Transform (FFT) algorithm is presented.

26 ermi pockets at the Fermi level via the fast Fourier transform (FFT) analysis.

27 We use a Fast Fourier Transform (FFT) based docking method to quickly

28 ein-protein docking server based on the fast Fourier transform (FFT) correlation approach.

29 ple-reference point normalization and a fast-Fourier transform (FFT)-based pre-processing scheme to q

30 Energy evaluation using fast Fourier transforms (FFTs) enables sampling billions of p

31 DynOmics is based on the fast Fourier transform, from which the difference in expressi

32 Fourier transform (FT) near-infrared (NIR) and attenuate

33 Standard three-dimensional Fourier transform (FT) NMR experiments of molecular syst

34 simultaneous acquisition of mass spectra via Fourier transform (FT) techniques (frequency measurement

35 free mass spectra with resolution beyond the Fourier transform (FT) uncertainty limit.

36 ach of 12 points per slab was obtained using Fourier transform (FT)-Raman spectroscopy.

37 e great practical importance of the discrete Fourier transform, implementation of fractional orders o

38 n determined by Attenuated Total Reflectance Fourier Transform Infra Red (ATR-FTIR) spectroscopy.

39 oscopy, X-ray diffraction (XRD) analysis and Fourier transform infra-red (FTIR) spectroscopy.

40 d using transmission electron microscopy and Fourier transform infra-red spectroscopy.

41 ure, corresponding to a peak displacement in Fourier-transform infra-red spectra, which was ascribed

42 Fourier-transform infra-red spectroscopy suggested that

43 we have applied attenuated total reflection Fourier transform infrared (ATR-FT-IR) spectroscopy and

44 ein, we employed attenuated total reflection Fourier transform infrared (ATR-FT-IR) spectroscopy and

45 Attenuated total reflectance Fourier transform infrared (ATR-FTIR) and Raman spectra

46 oducts by using attenuated total reflectance Fourier transform infrared (ATR-FTIR) spectra combined w

47 ased PNPs while attenuated total reflectance-fourier transform infrared (ATR-FTIR) spectra provided i

48 acquired using attenuated total reflectance-Fourier transform infrared (ATR-FTIR) spectrometer.

49 f supernatants, attenuated total reflectance-Fourier transform infrared (ATR-FTIR) spectroscopy and m

50 In this study, Attenuated Total Reflection Fourier transform infrared (ATR-FTIR) spectroscopy in co

51 study, we used attenuated total reflectance Fourier transform infrared (ATR-FTIR) spectroscopy to an

52 Attenuated total reflectance Fourier transform infrared (ATR-FTIR) spectroscopy using

53 Attenuated total reflectance Fourier transform infrared (ATR-FTIR) spectroscopy, Sync

54 ablished with subsequent diffuse reflectance-Fourier transform infrared (DRS-FTIR) analysis.

55 r structural changes were investigated using Fourier transform infrared (FT-IR) and Raman spectroscop

56 Table-top Fourier transform infrared (FT-IR) imaging spectrometers

57 Fourier transform infrared (FT-IR) microscopy coupled wi

58 Fourier transform infrared (FT-IR) spectra revealed rand

59 Fourier transform infrared (FT-IR) spectroscopic imaging

60 Fourier transform infrared (FT-IR) spectroscopy can be u

61 Fourier Transform Infrared (FT-IR) spectroscopy has been

62 Fourier transform infrared (FT-IR) spectroscopy of micro

63 ermined using chemical composition analysis, Fourier transform infrared (FT-IR) spectroscopy, scannin

64 MIP-template interaction is verified also by Fourier Transform Infrared (FT-IR) spectroscopy.

65 Thin layer chromatography (TLC), Fourier transform infrared (FTIR) analysis, and measurem

66 erlayer space of BDTA-Mt organoclays as both Fourier transform infrared (FTIR) and X-ray diffraction

67 stoned olive pastes was carried out by using Fourier transform infrared (FTIR) data and partial least

68 cell wall constituent sugar composition and Fourier transform infrared (FTIR) data showed that NaOH

69 The UV-vis, fluorescence and Fourier transform infrared (FTIR) demonstrated that BSA

70 Using DFPT, we calculated Fourier transform infrared (FTIR) spectra for six most w

71 his protocol allowed us to collect the first Fourier transform infrared (FTIR) spectra of intact hydr

72 compared with standardized methods based on Fourier transform infrared (FTIR) spectrometry.

73 The Fourier transform infrared (FTIR) spectroscopic method w

74 'cold' cathodoluminescence (CL)-imaging and Fourier Transform Infrared (FTIR) spectroscopy analyses.

75 ich suggests a good predictive capability of Fourier Transform Infrared (FTIR) spectroscopy and chemo

76 energy-dispersive X-ray spectroscopy (EDAX), Fourier transform infrared (FTIR) spectroscopy and elect

77 TGA-Fourier transform infrared (FTIR) spectroscopy and NOx c

78 Further studies using Fourier transform infrared (FTIR) spectroscopy demonstra

79 udy, we demonstrate the first application of Fourier transform infrared (FTIR) spectroscopy for simul

80 situ, we coupled affinity chromatography and Fourier transform infrared (FTIR) spectroscopy for the f

81 This review highlights the contribution Fourier transform infrared (FTIR) spectroscopy has made

82 Fourier transform infrared (FTIR) spectroscopy is a powe

83 Additionally, time-resolved Fourier transform infrared (FTIR) spectroscopy of TM3 mo

84 Fourier transform infrared (FTIR) spectroscopy suggested

85 s (NOx) and investigating the application of Fourier transform infrared (FTIR) spectroscopy to quanti

86 ed using TEM, atomic force microscopy (AFM), Fourier transform infrared (FTIR) spectroscopy, circular

87 We applied Fourier transform infrared (FTIR) spectroscopy, scanning

88 tering and refractive index detectors and by Fourier Transform Infrared (FTIR) spectroscopy.

89 was confirmed by X-ray diffraction (XRD) and Fourier transform infrared (FTIR) spectroscopy.

90 ipids and probed at the molecular level with Fourier transform infrared (FTIR) spectroscopy.

91 steps of pectin extraction were followed by Fourier transform infrared (FTIR) spectroscopy.

92 ansmission electron microscopy (TEM), UV and Fourier transform infrared (FTIR) spectroscopy.

93 roton nuclear magnetic resonance ((1)H NMR), Fourier transform infrared (FTIR), and X-ray photoelectr

94 e microscopy (AFM), X-ray diffraction (XRD), Fourier transform infrared (FTIR), cyclic voltammetry (C

95 Micro-Fourier transform infrared (micro-FTIR) spectroscopy and

96 molecular interactions were characterized by Fourier transform infrared and fluorescence spectroscopi

97 A combination of Fourier transform infrared and phase transition measurem

98 Fourier transform infrared and solid-state NMR spectrosc

99 Through a combination of Fourier transform infrared and two-dimensional infrared

100 y such a nutrient flow, a new application of Fourier transform infrared imaging (FTIRI) was developed

101 d functional magnetic resonance imaging with Fourier transform infrared microscopy, fluorescence-base

102 Applying Fourier transform infrared microspectroscopy, the cutin

103 ctrophotometer, Attenuated total reflectance Fourier transform infrared spectrometer (ATR-FTIR), and

104 sized imprinted polymer was characterized by Fourier transform infrared spectrometry (FTIR) and scann

105 Fourier transform infrared spectroscopic measurements sh

106 ined by means of attenuated total reflection Fourier transform infrared spectroscopy (ATR-FTIR) and c

107 determined from attenuated total reflection Fourier transform infrared spectroscopy (ATR-FTIR) nicel

108 We used attenuated total reflection - Fourier transform infrared spectroscopy (ATR-FTIR) to de

109 angle (CA) and attenuated total reflectance-Fourier transform infrared spectroscopy (ATR-FTIR).

110 as observed with in situ diffuse-reflectance Fourier transform infrared spectroscopy (DRIFTS).

111 opy (TEM), atomic force microscopy (AFM) and Fourier transform infrared spectroscopy (FT-IR) studies.

112 rization of the complexes was carried out by Fourier Transform Infrared Spectroscopy (FT-IR), Differe

113 s (DSC and TGA), X-ray diffractometry (XRD), Fourier transform infrared spectroscopy (FT-IR), sorptio

114 icroscopy (SEM), X-ray diffraction (XRD) and Fourier transform infrared spectroscopy (FT-IR).

115 trochemical impedance spectroscopy (EIS) and Fourier transform infrared spectroscopy (FT-IR).

116 Fourier Transform infrared spectroscopy (FTIR) and densi

117 ated the bacteria disinfection process using Fourier transform infrared spectroscopy (FTIR) and matri

118 Fourier transform infrared spectroscopy (FTIR) and scann

119 d by the scanning electron microscopy (SEM), Fourier transform infrared spectroscopy (FTIR) and X - r

120 ng electron microscopy (SEM), Raman spectra, Fourier Transform infrared spectroscopy (FTIR) and X-ray

121 The first example is the Fourier transform infrared spectroscopy (FTIR) follow-up

122 Fourier transform infrared spectroscopy (FTIR) proposed

123 Dynamic Light Scattering (DLS) and Fourier Transform Infrared spectroscopy (FTIR) suggest e

124 tigated by atomic force microscopy (AFM) and Fourier transform infrared spectroscopy (FTIR) technique

125 PL), x-ray photoelectron spectroscopy (XPS), Fourier transform infrared spectroscopy (FTIR), atomic f

126 synthesized composite is characterized using Fourier transform infrared spectroscopy (FTIR), Raman sp

127 eveloped immunosensor was performed by using Fourier transform infrared spectroscopy (FTIR), scanning

128 is confirmed by X-ray diffraction (XRD) and Fourier transform infrared spectroscopy (FTIR).

129 oscopy, subtractively normalized interfacial Fourier transform infrared spectroscopy (SNIFTIRS), and

130 Rutherford backscattering spectrometry and Fourier transform infrared spectroscopy analyses confirm

131 Fourier transform infrared spectroscopy analyses of the

132 Attenuated total reflectance-Fourier transform infrared spectroscopy analysis further

133 discussed, which was described previously by Fourier transform infrared spectroscopy analysis.

134 icroscopy, transmission electron microscopy, fourier transform infrared spectroscopy and electrochemi

135 field emission scanning electron microscopy, Fourier transform infrared spectroscopy and energy-dispe

136 ectroscopy, X-ray fluorescence spectroscopy, Fourier transform infrared spectroscopy and scanning ele

137 Fourier transform infrared spectroscopy confirmed the bo

138 Fourier transform infrared spectroscopy confirmed the su

139 The Fourier transform infrared spectroscopy confirms the com

140 nary complex formation were characterized by Fourier transform infrared spectroscopy in the absence o

141 re X-ray photoelectron spectroscopy (APXPS), Fourier transform infrared spectroscopy in the Kretschma

142 XPS and in situ attenuated total reflectance Fourier transform infrared spectroscopy in the Kretschma

143 Attenuated total reflection Fourier transform infrared spectroscopy revealed that cu

144 Scanning electron microscopy and Fourier transform infrared spectroscopy showed the chang

145 Fourier transform infrared spectroscopy suggests the inv

146 Fourier Transform Infrared spectroscopy was evaluated as

147 ied by Raman and attenuated total reflection-Fourier transform infrared spectroscopy, and powder X-ra

148 electron microscopy, Brunauer-emmett-teller, Fourier transform infrared spectroscopy, and selectivity

149 man scattering, attenuated total reflectance Fourier transform infrared spectroscopy, and X-ray photo

150 ed by (11)B NMR, attenuated total reflection Fourier transform infrared spectroscopy, circular dichro

151 scopy, Energy-dispersive X-ray spectroscopy, Fourier transform infrared spectroscopy, electrochemical

152 ction, X-ray photoelectron spectroscopy, and Fourier transform infrared spectroscopy, revealing that

153 tion yield, particle size, thermogravimetry, Fourier transform infrared spectroscopy, stability under

154 Here we show, using Fourier transform infrared spectroscopy, that COR15A sta

155 In addition, characterizations with in-situ Fourier transform infrared spectroscopy, thermal gravity

156 TGA/CdTe QDs nanosensor was characterized by Fourier transform infrared spectroscopy, transmission el

157 erized by X-ray diffraction, UV-vis spectra, Fourier transform infrared spectroscopy, vibrating sampl

158 ed with confocal fluorescence microscopy and Fourier transform infrared spectroscopy, we studied the

159 ApoMb were studied using circular dichroism, Fourier transform infrared spectroscopy, x-ray diffracti

160 Fourier transform infrared spectroscopy, X-ray photoelec

161 unique possibility offered by high-pressure Fourier transform infrared spectroscopy.

162 s were investigated by X-ray diffraction and Fourier transform infrared spectroscopy.

163 pedance spectroscopy, cyclic voltammetry and Fourier transform infrared spectroscopy.

164 duplexed with a target which was revealed by Fourier Transform Infrared Spectroscopy.

165 canning calorimetry, circular dichroism, and Fourier transform infrared spectroscopy.

166 l) using in situ attenuated total reflection Fourier transform infrared spectroscopy.

167 photoelectron spectroscopy, and transmission Fourier transform infrared spectroscopy.

168 titial defects is predicted and confirmed by Fourier transform infrared spectroscopy.

169 ionization mass spectrometry, as well as by Fourier transform infrared spectroscopy.

170 , X-ray diffraction, UV-visible (UV-vis) and Fourier transform infrared spectroscopy.

171 The operando transmission FTIR/SSITKA (Fourier transform infrared spectroscopy/steady-state iso

172 ifferent spectroscopic techniques (Raman and Fourier transform infrared, FT-IR).

173 nsmission electron microscopy (SEM and TEM), Fourier transformed infrared (FT-IR) spectroscopy and fl

174 ffraction (XRD), and in situ electrochemical Fourier transformed infrared (FTIR) experiments.

175 nsor assembly were followed and confirmed by Fourier Transformed Infrared s pectrometry (FTIR) and Ra

176 functional groups present were determined by Fourier transformed infrared spectroscopy (FTIR) and the

177 study was to investigate the feasibility of Fourier Transformed Infrared Spectroscopy (FTIR) on Atte

178 Fourier transformed infrared spectroscopy was used with

179 pies, X-ray diffraction, diffuse reflectance Fourier transformed infrared spectroscopy, and measureme

180 By Fourier transformed infrared spectroscopy, we have demon

181 study presents, attenuated total reflection Fourier transforms infrared spectroscopy of dried serum

182 chnique, in situ attenuated total reflection Fourier-transform infrared (ATR FT-IR) spectroscopy, tim

183 etermine whether attenuated total reflection Fourier-transform infrared (ATR-FTIR) or Raman spectrosc

184 iques, including attenuated total reflection Fourier-transform infrared (ATR-FTIR) spectroscopy and s

185 Attenuated total reflection Fourier-transform infrared (ATR-FTIR) spectroscopy can d

186 emporaria, using attenuated total reflection-Fourier-transform infrared (ATR-FTIR) spectroscopy with

187 alyses following attenuated total reflection Fourier-transform infrared (ATR-FTIR) spectroscopy; alth

188 cryo-sections of hamster brain tissue using Fourier-transform infrared (FT-IR) microspectroscopy, co

189 (U937) upon IAV infection using synchrotron Fourier-transform infrared (FTIR) and deep UV (DUV) micr

190 We developed an automatic, reproducible Fourier-transform infrared (FTIR) imaging-based techniqu

191 nned, primarily, to determine the ability of Fourier-transform infrared (FTIR) spectroscopy to distin

192 anning electron microscopy (SEM) analysis, a Fourier-transform infrared microspectroscopy (FTIRM) met

193 firin as evaluated by circular dichroism and Fourier-transform infrared red spectroscopy.

194 acterization of the MIPs were carried out by Fourier-transform infrared spectrometry.

195 , X-ray photoelectron spectroscopy (XPS) and Fourier-transform infrared spectroscopy (FTIR) were used

196 ssion-scanning electron microscopy (FE-SEM), Fourier-transform infrared spectroscopy (FTIR), high res

197 graphene nanoplatelets as observed from the Fourier-transform infrared spectroscopy (FTIR).

198 ctron Microscopy (SEM), X-ray-tomography and Fourier-Transform Infrared spectroscopy (FTIR); releases

199 c interaction by attenuated total reflection Fourier-transform infrared spectroscopy and measuring th

200 The results of Fourier-transform infrared spectroscopy indicated physic

201 Fourier-transform infrared spectroscopy provides evidenc

202 he Hox-->HredH(+) reduction step measured by Fourier-transform infrared spectroscopy showed an enthal

203 py, energy dispersive X-ray spectroscopy and fourier-transform infrared spectroscopy showed that the

204 Employing Fourier-transform infrared spectroscopy we probe changes

205 red by real-time attenuated total reflection Fourier-transform infrared spectroscopy.

206 g, monosaccharide composition determination, Fourier-transformed infrared microspectroscopy, quantita

207 on step by transmission electron microscopy, Fourier-transformed infrared spectroscopy, thermogravime

208 es regression (PLS) analysis on the basis of Fourier transform-infrared (FT-IR) spectra of fruit cell

209 des from PPW (PPPW) was examined by means of Fourier transform-infrared spectroscopy (FT-IR) analysis

210 differential scanning calorimetry (DSC) and Fourier transform-infrared spectroscopy (FT-IR).

211 y UV-vis and photoluminescence spectroscopy, Fourier transform-infrared spectroscopy, transmission el

212 ned using attenuated total reflectance (ATR)-Fourier transformed-infrared (FT-IR) spectroscopy (4000-

213 Fourier transforms, integer and fractional, are ubiquito

214 for the first time the use of a 15 T solariX Fourier transform ion cyclotron mass spectrometer to cha

215 ultrahigh resolution electrospray ionization Fourier transform ion cyclotron mass spectrometry.

216 atmospheric pressure photoionization (APPI) Fourier transform ion cyclotron resonance (FTICR) mass a

217 hot electron capture dissociation (HECD) and Fourier transform ion cyclotron resonance (FTICR) mass s

218 tion and compatibility with high-performance Fourier transform ion cyclotron resonance (FTICR) mass s

219 ropose to use ultrahigh resolution 15T MALDI-Fourier transform ion cyclotron resonance (FTICR) MS to

220 n development of an instrument with a set of Fourier transform ion cyclotron resonance (ICR) cells as

221 matrix-assisted laser/desorption ionisation Fourier transform ion cyclotron resonance (MALDI-FTICR)

222 isted laser desorption ionization and either Fourier transform ion cyclotron resonance detection (at

223 d ultrahigh resolution and mass accuracy 21T Fourier transform ion cyclotron resonance mass spectrome

224 rshall for frequency-multiple detection in a Fourier transform ion cyclotron resonance mass spectrome

225 tion of DOC in a drinking water reservoir by Fourier transform ion cyclotron resonance mass spectrome

226 resence of dissolved organic matter (DOM) by Fourier transform ion cyclotron resonance mass spectrome

227 rahigh resolution mass spectrometry, such as Fourier transform ion cyclotron resonance mass spectrome

228 more established state-of-the-art technique, Fourier transform ion cyclotron resonance mass spectrome

229 Two-dimensional Fourier transform ion cyclotron resonance mass spectrome

230 etry which is solved by two-dimensional (2D) Fourier transform ion cyclotron resonance mass spectrome

231 ty subfraction using electrospray ionization Fourier transform ion cyclotron resonance mass spectrome

232 uadrupole time-of-flight and high resolution Fourier transform ion cyclotron resonance mass spectrome

233 found in low-concentrations were analyzed by Fourier transform ion cyclotron resonance mass spectrome

234 Electrospray ionization (ESI) Fourier transform ion cyclotron resonance mass spectrome

235 High-field Fourier transform ion cyclotron resonance mass spectrome

236 A bioassay method was coupled with Fourier transform ion cyclotron resonance mass spectrome

237 Two-dimensional Fourier transform ion cyclotron resonance mass spectrome

238 ng negative-ion mode electrospray ionisation Fourier transform ion cyclotron resonance mass spectrome

239 obility spectrometry (SA-TIMS) is coupled to Fourier transform ion cyclotron resonance mass spectrome

240 was investigated as an ionization method for Fourier transform ion cyclotron resonance mass spectrome

241 mobility spectrometry (TIMS) in tandem with Fourier transform ion cyclotron resonance mass spectrome

242 ltra-high-resolution electrospray ionization Fourier transform ion cyclotron resonance mass spectrome

243 ion mode ESI in a linear quadrupole ion trap/Fourier transform ion cyclotron resonance mass spectrome

244 Fourier transform ion cyclotron resonance mass spectrome

245 Fourier transform ion cyclotron resonance mass spectrome

246 astewater samples using ultrahigh resolution Fourier transform ion cyclotron resonance mass spectrome

247 ing hydrogen/deuterium exchange monitored by Fourier transform ion cyclotron resonance MS, we have pr

248 ct infusion electrospray ionization (DI-ESI) Fourier transform ion cyclotron resonance/mass spectrome

249 In this regard, Fourier-transform ion cyclotron resonance (FTICR) has th

250 ve comparison between a high mass resolution Fourier-transform ion cyclotron resonance (FTICR) mass s

251 ions are shown to be structurally similar by Fourier-transform ion cyclotron resonance mass spectrome

252 the ion cyclotron resonance (ICR) cell of a Fourier transform-ion cyclotron resonance (FT-ICR) mass

253 rganic matter (DOM) within these lakes using Fourier transform-ion cyclotron resonance mass spectrome

254 matrix assisted laser desorption ionization-fourier transform-ion cyclotron resonance mass spectrome

255 Sample extracts were analysed by Fourier Transform-Ion Cyclotron Resonance-Mass Spectrome

256 Fourier transform-IR (FT-IR) spectra of clusters of elec

257 The Fourier transform is a ubiquitous mathematical operation

258 acting the phase from the well-known optical Fourier transform is challenging.

259 Certainly, since the ordinary Fourier transform is merely a particular case of a conti

260 ve dual-frequency designer waveform into the Fourier-transformed large-amplitude alternating current

261 ent and metabolomics (linear trap quadrupole-Fourier transform mass spectrometer) analysis.

262 deconvolution method (PhiSDM), designed for Fourier transform mass spectrometry (FT MS).

263 such as C3 vs SH4: (a) ultrahigh resolution Fourier transform mass spectrometry (FT-MS); (b) high-re

264 reversed-phase liquid chromatography (SPLC), Fourier transform mass spectrometry (FTMS), data-indepen

265 pe juice by liquid chromatography coupled to Fourier transform mass spectrometry experiments.

266 adjacent tissues (AT) using high-resolution Fourier-transform mass spectrometry and a novel algorith

267 A spectroscopic method based on Fourier Transform micro-Raman spectroscopy coupled with

268 dy investigated the potential application of Fourier transform mid-infrared spectroscopy (FT-MIR) for

269 rac masses on a locally finite set, (ii) the Fourier transform mu f mu is also a sum of weighted Dira

270 nal processing techniques such as short time fourier transform, multitaper method, wavelet transform,

271 Vinho Verde wine samples were analyzed using Fourier transform near infrared (FT-NIR) transmission sp

272 ture was ultimately disclosed by an indirect Fourier transform of static light scattering, small angl

273 A short-time Fourier transform of the time-domain data indicates that

274 cal optics, we implement discrete fractional Fourier transforms of exemplary wave functions and exper

275 noise (SNR) analysis of diffraction peaks in Fourier transforms of specimens imaged by negative-stain

276 We also perform a coherent quantum Fourier transform on five trapped-ion qubits for phase e

277 By implementing the Fourier transform optically we can overcome the limiting

278 ity spectrometry (AP-DTIMS) was coupled with Fourier transform Orbitrap mass spectrometry.

279 In this paper, a Fourier Transform Raman spectroscopy method, to authenti

280 Fourier transform Raman spectroscopy was applied to dete

281 Performing larger optical Fourier transforms requires higher resolution spatial li

282 m each channel were demodulated using a fast Fourier transform, resolving the contributions from each

283 The time-domain ion current, once Fourier transformed, reveals a standard ion mobility dri

284 apply this approach in the quantum realm to Fourier transform separable and path-entangled biphoton

285 e as the target function the fidelity of the Fourier Transform spectra of nanostructures that are des

286 ing conventional attenuated total reflection Fourier transform spectroscopy (ATR-FTIR) without the ne

287 ucture (EXAFS), diffuse reflectance infrared Fourier transform spectroscopy (DRIFT), and mass spectro

288 Using in situ diffuse reflectance infrared Fourier transform spectroscopy (DRIFTS), structural chan

289 tor and in situ Diffuse Reflectance Infrared Fourier Transform Spectroscopy (DRIFTS).

290 Here we use optical two-dimensional Fourier transform spectroscopy to measure the exciton ho

291 ined in DRIFTS (diffuse reflectance infrared Fourier transform spectroscopy) mode and of slightly wor

292 lculation through reflective interferometric Fourier transform spectroscopy.

293 ures not reliably resolved using traditional Fourier transform spectroscopy.

294 Diffuse reflectance mid-infrared Fourier-transform spectroscopy (DRIFTS) is capable of de

295 bility of the master model and the nonlinear Fourier transform, the lower bound on the capacity per s

296 stic neutron scattering and frequency-domain Fourier-transform THz electron paramagnetic resonance sp

297 od could unlock the potential of the optical Fourier transform to permit 2D complex-to-complex discre

298 g the input and exploiting symmetries of the Fourier transform we are able to determine the phase dir

299 intensity measurements, creating an optical Fourier transform with O(n) apparent complexity.

300 orm to permit 2D complex-to-complex discrete Fourier transforms with a performance that is currently