ライフサイエンスコーパス: soft X-ray

1 ating deuterium-filled plastic capsules with soft x rays.

2 -biased magnetic multilayer with exposure to soft X-rays.

3 targeted low doses of carbon-characteristic soft X-rays.

4 icelle drug delivery platform using resonant soft X-rays.

5 ials at wavelengths ranging from infrared to soft X-rays.

6 maging methods that make use of electrons or soft X-rays.

7 hoton energy from the extreme ultraviolet to soft X-rays.

8 ditions, that is, layered ices irradiated by soft X-rays.

9 econcile with the persistence of M81 ULS-1's soft X-rays.

10 a full coverage of the EUV (2.5 to 50 nm) to soft X-ray (1.25 to 2.5 nm) spectrum; for the second opt

11 olved analysis was carried out by using both soft X-rays (100-800 eV) and hard X-rays (2000-7000 eV)

12 Using soft x-ray absorption (XAS) and resonant inelastic x-ray

13 ed absorption spectroscopy (SEIRAS), in situ soft X-ray absorption spectroscopy (Cu L-edge), and onli

14 e Li-birnessite were investigated by ex situ soft X-ray absorption spectroscopy (sXAS) and X-ray pair

15 electron energy loss spectroscopy (EELS) and soft X-ray absorption spectroscopy (sXAS) results reveal

16 X-ray photoelectron spectroscopy (XPS), and soft X-ray absorption spectroscopy (sXAS), as well as el

17 probed their oxidation kinetics with in situ soft X-ray absorption spectroscopy (sXAS).

18 Electron energy loss spectroscopy (EELS) and soft X-ray absorption spectroscopy (XAS) measurements of

19 In situ soft X-ray absorption spectroscopy (XAS) was employed to

20 matic magnetic property characterization and soft X-ray absorption spectroscopy analysis indicate tha

21 Ab initio calculation and soft X-ray absorption spectroscopy analysis suggest that

22 chniques such as photoelectron spectroscopy, soft X-ray absorption spectroscopy and X-ray emission sp

23 Here we show that operando soft X-ray absorption spectroscopy in total electron yie

24 Here we achieve in situ and operando soft X-ray absorption spectroscopy of lithium-ion batter

25 nd CaCu(3)Cr(4)O(12) as revealed by resonant soft x-ray absorption spectroscopy on the Cu L(3,2)- and

26 Here, we present a magnetic and soft x-ray absorption spectroscopy study of the chemical

27 iments with scanning electron microscopy and soft X-ray absorption spectroscopy to characterize the m

28 bility and unique potential of time-resolved soft X-ray absorption spectroscopy to study ultrafast re

29 Through soft X-ray absorption spectroscopy, hard X-ray Raman sca

30 ux and high spectral and temporal resolution soft X-ray absorption spectroscopy, is a new route to th

31 Combined soft X-ray absorption spectroscopy, resonant inelastic X

32 ied and understood through synchrotron-based soft X-ray absorption spectroscopy, which also reveals t

33 he element and site specificity of near-edge soft X-ray absorption spectroscopy.

34 In-situ hard X-ray absorption and ex-situ soft X-ray absorption study, along with density function

35 exploit the element and site selectivity of soft X-ray absorption to sensitively follow the ultrafas

36 zeolite H-mordenite, using in situ STXM and soft X-ray absorption tomography, complemented with (27)

37 f the energy radiated in radio, optical, and soft X-ray afterglows.

38 ent CO(2) as identified by synchrotron-based soft X-ray analyses.

39 s was elucidated via time-resolved Al K-edge soft X-ray and (27)Al NMR, confirming the tricoordinated

40 a multifaceted investigation combining local soft X-ray and vibrational spectroscopic probes with ab

41 We use soft x-ray angle-resolved photoelectron spectroscopy to

42 Traditional ultraviolet/soft X-ray angle-resolved photoemission spectroscopy (AR

43 We use inelastic neutron scattering, soft x-ray angle-resolved photoemission spectroscopy mea

44 ear the Fermi energy through spin-integrated soft X-ray angular resolved photoemission spectroscopy.

45 Soft X-ray APPI does not require a dopant to achieve hig

46 st compounds in the negative ion mode, using soft X-ray APPI source emitting 4.9 keV photons.

47 X-ray atmospheric pressure photoionization (soft X-ray APPI) as an ionization method in liquid chrom

48 Our soft-X-ray ARPES data on Ag metal reveals, however, that

49 econd transient absorption spectroscopy with soft x-rays at the carbon K-edge revealed that the disto

50 Soft X-ray atmospheric pressure photoionization (soft X-

51 tally demonstrate the generation of isolated soft X-ray attosecond pulses at photon energies up to 18

52 Most of the soft X-ray background has been resolved into individual

53 olyte were found to experience a predominant soft X-ray beam-induced oxidation to CuO despite only su

54 We used soft x-ray beams generated by high-harmonic upconversion

55 mplement and generates coherent, laser-like, soft X-ray beams, it is currently being developed for ap

56 ser pulses are required to generate isolated soft X-ray bursts efficiently, to mitigate group velocit

57 nuclear and cytoplasmic irradiation using a soft X-ray (carbon K-shell, 278 eV) microbeam in MDA-MB-

58 our method will enable searches for further soft-X-ray clock transitions(8,12) in HCIs, which are re

59 e than 3 x 10(39) ergs per second, unusually soft X-ray components (with a typical temperature of les

60 ere further integrated with fluorescence and soft X-ray cryo microscopy data applied on experimental

61 mbines serial cryoFIB/SEM volume imaging and soft X-ray cryo-tomography with cell lamellae-based cryo

62 use a microchannel plate (MCP) based Timepix soft X-ray detector to conduct a time-resolved RIXS meas

63 We used synchrotron resonant soft x-ray diffraction (RSXRD) at multiple energies near

64 Femtosecond resonant soft X-ray diffraction is used to determine the spatiote

65 are identified by a combination of hard and soft x-ray diffraction measurements, optical studies and

66 A tabletop soft x-ray diffraction microscope should find broad appl

67 Here, we report a versatile soft x-ray diffraction microscope with 70- to 90-nm reso

68 s have a skyrmion number of +1, and resonant soft-X-ray diffraction experiments show circular dichroi

69 It blocks 90% of the soft x-ray emission and causes simultaneous deep, broad

70 ifferent sulfates are studied using S L(2,3) soft X-ray emission spectroscopy (XES).

71 seed coherent extreme-ultraviolet (EUV) and soft X-ray emission with nearly MHz repetition rate.

72 with an overdensity of galaxies and diffuse, soft-X-ray emission, and contributes a mass comparable t

73 photoelectron spectroscopy at bulk-sensitive soft X-ray energies (SX-ARPES) combined with photoelectr

74 20 electronvolts, reminiscent of the typical soft-X-ray excess, an almost universal thermal-like feat

75 s requires that relative enhancements in the soft x-ray fluxes far exceed those in the UV.

76 e achieve all-optical synchronization at the soft X-ray free-electron laser FLASH and demonstrate fac

77 1s level using synchrotron radiation and the soft X-ray free-electron laser LCLS provide direct evide

78 le-shot wide-angle scattering of femtosecond soft X-ray free-electron laser pulses allows three-dimen

79 ccelerators for applications such as driving soft X-ray free-electron lasers and producing gamma-rays

80 a lifetime of about 130 days, the potential soft-X-ray frequency reference at 4.96 x 10(16) hertz (c

81 odic eruptions (QPEs) are luminous bursts of soft X-rays from the nuclei of galaxies, repeating on ti

82 t) is five to ten times greater than that of soft X-rays, from which we conclude that 4U0142+61 is a

83 neration, the conditions for optimal bright, soft X-ray generation naturally coincide with the genera

84 A laboratory setup for soft X-ray GEXRF measurements is presented.

85 rgence properties of extreme ultraviolet and soft x-ray high-harmonic combs.

86 pplication, using a time-resolved pump-probe soft X-ray imaging technique.

87 optics have played a major role in nanoscale soft X-ray imaging, high-resolution and high-efficiency

88 h more rarely implemented because the use of soft X-rays implies ultrahigh vacuum conditions.

89 However, the short penetration depth of soft X-rays imposes stringent constraints on sample type

90 nown in the Milky Way, and the absorption of soft X-rays in the interstellar medium hinders the deter

91 Soft X-ray, indirect immunofluorescence, and green fluor

92 ocesses on the optical properties of XUV and soft X-ray irradiated Si[Formula: see text]N[Formula: se

93 te the generation of intense, low-divergence soft X-ray isolated attosecond pulses in a gas-filled ho

94 Using soft x-ray laminography, we reconstruct with about 20-na

95 erent tabletop coherent soft x-ray sources-a soft x-ray laser and a high-harmonic source.

96 e Ti M(2,3) edge with a high-harmonic seeded soft x-ray laser.

97 In contrast, table-top soft X-ray lasers (SXRL) feature excellent temporal cohe

98 gest that the population of objects emitting soft X-rays (less than 10 kiloelectronvolts) within the

99 nt between the laser light and the generated soft x-ray light can be partially compensated.

100 A contemporaneous 7-day soft x-ray light curve obtained using the Extreme Ultrav

101 ive central galaxies(3-6) and the absence of soft X-ray lines from the cooling gas(7-9) suggest that

102 tudies exhibit the powerful contributions of soft X-ray liquid spectroscopies in the last few years.

103 al magnetic state of the double helices with soft-X-ray magnetic laminography(12,13), we identify the

104 served in scanning tunnelling microscopy and soft X-ray measurements.

105 ms by applying subcellular targeting using a soft X-ray microbeam in combination with GNPs.

106 nction and it is the first report applying a soft X-ray microbeam to study the radiobiological effect

107 Using the Gray Cancer Institute soft X-ray microprobe, it has been possible to follow th

108 The specimen is then cryo-transferred to a soft x-ray microscope (SXM) for SXT data acquisition.

109 ement of sub-15-nm spatial resolution with a soft X-ray microscope--and a clear path to below 10 nm--

110 urces have led to the development of compact soft X-ray microscopes.

111 Cryo-electron and synchrotron-based soft X-ray microscopies revealed that amorphous guanine

112 ms with tubular shape by means of full-field soft X-ray microscopies.

113 Soft x-ray microscopy is a novel approach for investigat

114 Here we review and exemplify the ability of soft X-ray microscopy to provide information that is oth

115 Using cryo-soft X-ray microscopy we imaged intracellular calcium-co

116 Using operando scanning transmission soft X-ray microscopy with high spatial resolution and c

117 -resolution full-field magnetic transmission soft X-ray microscopy.

118 need that is often uniquely addressed using soft X-ray microscopy.

119 etal ferromagnets with magnetic transmission soft X-ray microscopy.

120 We applied scanning transmission (soft) X-ray microscopy (STXM) spectrotomography for deta

121 sealed electrochemical microcell for in situ soft X-ray microspectroscopy in transmission, dedicated

122 Using soft x-ray observations of the bright new comet C/1999 S

123 ow that the resonant scattering of polarized soft X-rays (P-SoXS) by molecular orbitals is not limite

124 We overcame this limitation by applying soft x-ray photoelectron spectroscopy to characterize ex

125 We used synchrotron radiation-based soft x-ray photoemission to show that monolayer films of

126 We found that autoionization after soft x-ray photoionization of molecular oxygen follows a

127 lectron is simultaneously excited during the soft x-ray photoionization process.

128 ts and more challenging applications such as soft X-ray photonics.

129 In addition, we show that when soft x-ray photons irradiate the system-mimicking radiat

130 The energy of the soft X-ray photons is in the keV range, which is high en

131 Centre than is the surface brightness of the soft-X-ray population.

132 We demonstrate visible pump soft X-ray probe near-edge X-ray absorption fine structu

133 The simulated UV-pump/soft-X-ray-probe spectra exhibit detailed dynamical info

134 Ultrafast UV-pump/soft-X-ray-probe spectroscopy is a subject of great inte

135 sing 1.8-millimeter-diameter capsules by the soft x-rays produced by the hohlraum.

136 and the dynamics are probed by an attosecond soft X-ray pulse at the carbon K-edge.

137 Here we demonstrate a soft X-ray pulse duration of 53 as and single pulse stre

138 k power with fully coherent ultrafast EUV to soft X-ray pulses based on the NSLS-II parameters.

139 These measurements exploit attosecond soft X-ray pulses from a free-electron laser to scan acr

140 We used tunable femtosecond soft x-ray pulses from an x-ray free electron laser to r

141 ture trends in generating and characterizing soft X-ray pulses from gas-phase HHG and extreme ultravi

142 heet microjets and terawatt-scale attosecond soft X-ray pulses from the LCLS X-ray free electron lase

143 time-resolved measurements using attosecond soft x-ray pulses produced by a free-electron laser, to

144 lement- and site-specificity using broadband soft X-ray pulses produced by high harmonic generation,

145 1 fs root mean square has been achieved for soft X-ray pulses.

146 is review presents recent developments using soft X-ray radiation for probing the electronic structur

147 er resolved elemental depth profiling in the soft X-ray range with a laboratory source, opening, for

148 differential solvents are shown by resonant soft X-ray reflectivity (RSoXR) to be very smooth and sh

149 ubmolecular resolution from energy-dependent soft X-ray reflectivity data.

150 X-ray absorption spectroscopy and resonant soft X-ray reflectivity revealed a depth-decaying near-s

151 absorption edges of matter, which lie in the soft X-ray regime above 200 eV, permit the probing of el

152 design of harmonic combs-particularly in the soft x-ray regime, where very limited options are availa

153 pulses often suffer from low photon flux in soft X-ray regime.

154 and temporal shape of high harmonics in the soft X-ray region by manipulating the driving laser wave

155 t extending into the extreme ultraviolet and soft x-ray region of electromagnetic spectrum.

156 cularly polarized high-harmonic beams in the soft X-ray region of the electromagnetic spectrum, and u

157 tally by demonstrating phase matching in the soft X-ray region of the spectrum around 330 eV, using u

158 guides that can generate bright beams in the soft x-ray region of the spectrum, up to photon energies

159 of electromagnetic radiation throughout the soft X-ray region of the spectrum.

160 ear optics can be applied effectively in the soft x-ray region of the spectrum.

161 r studies in the extreme-ultraviolet or even soft-X-ray region with comb sources of low photon yield.

162 Soft X-ray reveals directly the valence states of Fe 3d

163 An image of comet Hale-Bopp (C/1995 O1) in soft x-rays reveals a central emission offset from the n

164 Synchrotron-based soft-X-ray scanning transmission X-ray microscopy (STXM)

165 developed operando electrochemical resonant soft X-ray scattering (EC-RSoXS) to probe the chemical i

166 gold nanoparticles using polarized resonant soft X-ray scattering (P-RSoXS).

167 es as evidenced by PL quenching and resonant soft X-ray scattering (R-SoXS) analyses.

168 absorption fine structure (EXAFS); resonant soft X-ray scattering (R-SoXS); ultraviolet photoelectro

169 Here, we report a combined resonant soft X-ray scattering (RSXS) and neutron scattering stud

170 BCO) and YBa2Cu3O6.67 (YBCO), using resonant soft X-ray scattering and a model mapped to the CDW orbi

171 pic and nanoscopic properties using resonant soft X-ray scattering and a number of other experimental

172 ted with the magnetic helices using resonant soft x-ray scattering and find two distinct nematic phas

173 A combination of resonant soft X-ray scattering and grazing incidence X-ray scatte

174 Here, we employ resonant soft x-ray scattering and polarimetry on thin films of b

175 ring anisotropy was observed in the resonant soft X-ray scattering of the blends that provided insigh

176 Here we use time-resolved resonant soft x-ray scattering spectroscopy to probe the dynamics

177 Here we use resonant soft x-ray scattering spectroscopy to reveal a novel c-a

178 acing (about 1 nm) in BiFeO3, using resonant soft X-ray scattering techniques and soft X-ray spectros

179 We use ultrafast resonant soft x-ray scattering to track the transient evolution o

180 nsity wave (CDW) with time-resolved resonant soft x-ray scattering, as well as a high magnetic field

181 ed, which is fully characterized by resonant soft X-ray scattering, high-angle annular dark film imag

182 Here, using resonant soft X-ray scattering, we study the archetypal cuprate L

183 ed with variable temperature liquid resonant soft X-ray scattering.

184 LCLS X-ray free electron laser, we employed soft X-ray second harmonic generation (SXSHG) spectrosco

185 ons when only a single cell is targeted with soft X-rays, significant bystander-mediated cell killing

186 (NEXAFS) spectroscopy system consisting of a soft X-ray source and an integrated spectrometer with a

187 The soft X-ray source is based on a long-term stable and nea

188 s advance the prospects for compact coherent soft x-ray sources for applications in biomicroscopy and

189 rtant for the development of high-brightness soft x-ray sources for applications in spectroscopy and

190 ion by using two different tabletop coherent soft x-ray sources-a soft x-ray laser and a high-harmoni

191 g magnetic stripe and skyrmion phase using a soft X-ray speckle metrology technique.

192 The soft X-ray spectra of Li(x)FePO(4) nanoparticles evolve

193 th emphasis on the transient response in the soft-X-ray spectral region as described by the ab initio

194 monstrates the advantages of this method for soft X-ray spectromicroscopy, which can readily provide

195 ull-field transmission X-ray microscopy with soft X-ray spectroscopic analysis that is performed on l

196 Soft X-ray spectroscopies are powerful tools for probing

197 boratory- and synchrotron-based electron and soft X-ray spectroscopies to characterize the chemical a

198 Soft X-ray spectroscopy (SXS) techniques such as photoel

199 l supercapacitor is monitored in operando by soft X-ray spectroscopy and interpreted through ab initi

200 demonstrate feasibility and power of in situ soft X-ray spectroscopy for studying integrated and dyna

201 esonant soft X-ray scattering techniques and soft X-ray spectroscopy measurements.

202 Here, we used femtosecond (fs) soft x-ray spectroscopy near the carbon K-edge ( 284 ele

203 surface artifacts that frequently occur with soft X-ray spectroscopy of light elements.

204 However, soft X-ray spectroscopy, one of the most sensitive probe

205 )O labeled Li[Li0.2Ni0.2Mn0.6]O2 with XANES, soft X-ray spectroscopy, resonant inelastic X-ray spectr

206 d active sites were investigated by hard and soft X-ray spectroscopy, which revealed that pyrrolic ni

207 ethyl)amine) has been studied via picosecond soft X-ray spectroscopy.

208 nt light in the "water window" region of the soft x-ray spectrum at 4.4 nanometers, using quasi-phase

209 ssion model that successfully reproduces the soft x-ray spectrum of comet Linear C/1999 S4, observed

210 Recently, a very soft X-ray spectrum was observed in a rare and transient

211 We present a table-top beamline providing a soft X-ray supercontinuum extending up to 370 eV from hi

212 While modern spectroscopic tools using soft X-ray synchrotron photons perspicuously reveal the

213 core-level band photoelectron spectra using soft X-ray synchrotron radiation.

214 the generation of high-flux, low-divergence soft X-ray tabletop isolated attosecond pulses for appli

215 Traditionally, these surface sensitive soft X-ray techniques that detect electrons or photons r

216 nd unoccupied states at the interface, using soft X-ray techniques, combined with electronic structur

217 biologically relevant information from cryo-soft X-ray tomograms.

218 within human B cells are reconstructed from soft X-ray tomographic images, and modeled as reflecting

219 resolution correlative method involving cryo-soft X-ray tomography (cryo-SXT) and stochastic optical

220 Cryo-soft X-ray tomography (cryo-SXT) is a powerful method to

221 This review introduces Soft X-ray Tomography (SXT) as a powerful imaging techni

222 Here, we utilized soft X-ray tomography (SXT) coupled with fluorescence mi

223 Soft X-ray tomography (SXT) enables native-contrast thre

224 Soft x-ray tomography (SXT) is increasingly being recogn

225 Cryo-soft x-ray tomography analysis revealed that SMAPs had a

226 ly, we exploited synchrotron radiation-based soft X-ray tomography and hard X-ray fluorescence for el

227 We have applied cryogenic soft X-ray tomography and three-dimensional electron mic

228 isition principles, and applications of both soft X-ray tomography and X-ray microscopy and how the u

229 Cryogenic soft X-ray tomography in the "water window" is particula

230 aphy, electron energy loss spectroscopy, and soft X-ray tomography of mature intracellular Plasmodium

231 rus 1-sized particles in a three-dimensional soft x-ray tomography reconstruction of an infected cell

232 Soft X-ray tomography reveals the ultrastructure of mito

233 e permeabilization, electron microscopy, and soft X-ray tomography that both AMPs and ampetoids trigg

234 lectron density information provided by cryo-soft X-ray tomography to characterize mitochondria crist

235 and processing framework in full field cryo soft X-ray tomography to computationally extend the dept

236 In this work we used soft X-ray tomography to image the subcellular changes t

237 We used three-dimensional soft X-ray tomography, combined with cryogenic fluoresce

238 We used three-dimensional soft x-ray tomography, confocal and electron microscopy,

239 g of near-native, unlabeled E. coli cells by soft X-ray tomography, we show that HU remodels nucleoid

240 -structured illumination microscopy and cryo-soft X-ray tomography.

241 r harsh imaging regimes such as electron and soft X-ray tomography.

242 illumination microscopy in conjunction with soft X-ray tomography.

243 ured from the same infected cells using cryo-soft-X-ray tomography (cryoSXT).

244 ere, we report the remarkable sensitivity of soft X-ray transient absorption spectroscopy for followi

245 a vector tomographic reconstruction based on soft X-ray transmission microscopy and magnetic dichrois

246 ssion electron microscopy and bulk-sensitive soft X-ray transmission microscopy using element-specifi

247 ulses by imaging the process with full-field soft X-ray transmission microscopy.

248 Specifically, we applied soft X-ray transmission tomography and hard X-ray fluore

249 ptimizing the conversion of laser light into soft x-rays typically demands a trade-off between two co

250 flare onsets show rapid increase of hard and soft X-rays, ultra-violet emission with large Doppler bl

251 gy recording) and the high brilliance of the soft X-rays used.

252 XRCC4-GFP, key proteins in NHEJ) using ultra-soft X-rays (USX) or multi-photon near infrared (NIR) la

253 Furthermore, we expect that soft X-ray vector ptycho-tomography can be broadly appli

254 We further develop soft X-ray vector ptycho-tomography to determine the mag

255 monic conversion of visible laser light into soft x-rays was demonstrated.

256 ental, chemical and surface sensitivities of soft X-rays, we discover distinct lithium-ion and electr

257 response of atoms and small molecules using soft X-rays with much lower intensities.