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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

39 1s level using synchrotron radiation and the soft X-ray free-electron laser LCLS provide direct evide

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

81 1 fs root mean square has been achieved for soft X-ray pulses.

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

111 Soft X-ray spectroscopies are powerful tools for probing

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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