ライフサイエンスコーパス: electron beam

1 two different irradiation sources (gamma and electron beam).

2 iation doses and technologies (cobalt-60 and electron-beam).

3 manipulating the lasing medium, that is, the electron beam.

4 negative resist through interactions with an electron beam.

5 magnesium oxide nanocubes using an atom-wide electron beam.

6 hene by tailoring its exposure to a focussed electron beam.

7 droplet into a toroidal shape induced by the electron beam.

8 ent, exert Lorentz forces on the propagating electron beam.

9 ansverse momentum structure imprinted on the electron beam.

10 of 100 megaelectronvolts for a subset of the electron beam.

11 g can be controlled by proper shaping of the electron beam.

12 science and medical therapy with X-rays and electron beams.

13 standing membranes into tubes by exposure to electron beams.

14 with independent control of both the ion and electron beams.

15 well as time-resolved experiments with free-electron beams.

16 changes of the kinetic state of relativistic electron beams.

17 the laser pulse and can be used for guiding electron beams.

18 scanners (110.0 HU), followed by GE-Imatron electron-beam (116.0 HU) and GE LightSpeed multi-detecto

19 ve of this work was to display the effect of electron beam accelerator doses on properties of plastic

20 n with swift ( approximately 2.5 MeV energy) electron beams allows to compensate these defects, bring

21 the screw displacements are parallel to the electron beam and become invisible when viewed end-on.

22 The production mechanism micro-bunches the electron beam and ensures the pulses are radially polari

23 s evaporated due to the use of a high-energy electron beam and the process was imaged in situ inside

24 atoms give excellent scattering contrast for electron beam and x-ray experiments.

25 tight constraints on the properties of such electron beams and new diagnostics for their presence in

26 alcium scores for the two scans was 15.8 for electron-beam and 16.9 for multi-detector row CT scanner

27 wok was designed to evaluate the effects of electron-beam and gamma irradiation over the phenolic pr

28 uplicate scans was high and similar for both electron-beam and multi-detector row CT (96%, kappa = 0.

29 ied coronary artery plaque was measured with electron-beam and multi-detector row CT and a standardiz

30 Electron-beam and multi-detector row CT scanners have eq

31 Maskless nanolithography, including electron-beam and scanning-probe lithography, offers the

32 Gamma, electron-beam and UV irradiation have been shown to be p

33 the hydrated electrons e(-)aq created by the electron beam are responsible for the reduction of metal

34 gment ions produced by interactions with the electron beam are subsequently analyzed by resonant ejec

35 ticles, such as protons and ion beams.Vortex electron beams are generated using single electrons but

36 Here, we use a scanning electron beam as a point source to probe the LDOS.

37 ck inorganic membrane with a tightly focused electron beam, as a transducer that detects single molec

38 lysin pores have been prepared, primarily by electron-beam-assisted techniques: these are more robust

39 Powerful field-aligned electron beams associated with the Io-Jupiter coupling,

40 t by releasing an additional tailored escort electron beam at a later phase of the acceleration, when

41 elerator of 85 cm length, driven by a 42 GeV electron beam at the Stanford Linear Accelerator Center

42 onization injection generates higher-quality electron beams at lower intensities and densities, and i

43 s with nanometre precision is possible using electron-beam-based techniques.

44 ever, none has attempted to manipulate multi-electron beams, because the repulsion between electrons

45 ability to shape the wavefunction of EBeams (Electron-Beams) become experimentally accessible.

46 direction to the movement of a single sheet electron beam bunch in the experiment.

47 acuum focal spot produces a greatly inferior electron beam, but instead correspond to the particular

48 slocation lying in a plane transverse to the electron beam by optical sectioning using annular dark f

49 as essential to achieve narrow energy-spread electron beams by ionization injection.

50 cheme for the realization of non-diffracting electron beams by shaping wavepackets of multiple electr

51 With this device, a low-energy electron beam can be injected orthogonally into the anal

52 Here, we show that irradiation with an 80 kV electron beam can selectively remove monolayers in few-l

53 Although the emittance of accelerated electron beams can be low, it can grow due to the effect

54 control, through photoionization, attosecond electron beams carrying OAM.

55 se oscillation, and the other relying on the electron beam catching up with the rear part of the lase

56 We are able to improve both the electron beam charge and angular distribution by an orde

57 edge of the distribution of laser energy and electron beam charge, which determine the overall effici

58 atio (R) of Fe to Lanthanide (Dy + Tb) using electron beam co-evaporation at room temperature.

59 was to determine the prognostic accuracy of electron beam computed tomographic (CT) scanning of the

60 nd quantity of CAC and AC were measured with electron beam computed tomography and fasting blood test

61 sured genes to CAC progression measured by 2 electron beam computed tomography examinations an averag

62 res in 2000 to 2001, and CAC was measured by electron beam computed tomography in 2000 to 2001 and 20

63 presence of subclinical atherosclerosis, by electron beam computed tomography scanning.

64 those, 98 patients underwent a total of 248 electron beam computed tomography studies at 0.5, 1, 1.5

65 coronary artery calcification determined by electron beam computed tomography was assessed in models

66 dial perfusion were determined in vivo using electron beam computed tomography, and myocardial sample

67 The electron beam computed tomography-derived coronary calci

68 d at baseline and at 3 years follow up using electron beam computed tomography.

69 accurately and noninvasively with the use of electron beam computed tomography.

70 ocardiography, intravascular ultrasound, and electron beam computed tomography.

71 g modalities, including computed tomography (electron-beam computed and multi-detector computed tomog

72 Three study centers used electron-beam computed tomography (CT), and three used m

73 compare the results and prognostic value of electron-beam computed tomography (EBCT) and exercise ec

74 Electron-beam computed tomography (EBCT) detects coronar

75 Electron-beam computed tomography (EBCT) is used to meas

76 m (CAC) score >10 Agatston units measured by electron-beam computed tomography and detectable aortic

77 s and function were quantified in vivo using electron-beam computed tomography at baseline and after

78 Electron-beam computed tomography CACS was predictive of

79 nical coronary heart disease were studied by electron-beam computed tomography for the extent of calc

80 Electron-beam computed tomography was used to measure th

81 ness, coronary artery calcification score on electron-beam computed tomography, homocysteine, and lip

82 coronary artery calcium score as measured by electron-beam computed tomography, lipoprotein(a) level,

83 by coronary artery calcification (CAC) using electron-beam computed tomography.

84 onary artery calcification (CAC) assessed by electron-beam computed tomography.

85 odynamics and function were quantified using electron-beam-computed tomography (CT) in normocholester

86 e liquid cell membrane surface chemistry and electron beam conditions, the dynamics and growth of met

87 unstable and may interact with the incident electron beam, constraining the electron beam density th

88 The electron beam CT coronary calcium score predicts CAD eve

89 tomatic persons age 50 to 70 years underwent electron beam CT scanning of the coronary arteries.

90 ning test for coronary artery disease (CAD), electron beam CT scanning remains controversial.

91 k race, male sex, coronary artery calcium by electron beam CT, a composite marker of congestive heart

92 enal artery stenosis) were studied with both electron-beam CT and 64-section multidetector CT at 1-we

93 Electron-beam CT calcium scores were higher than multi-d

94 -detector row CT appears to be comparable to electron-beam CT for coronary calcification screening, e

95 Electron-beam CT scans were used to measure coronary art

96 Scans were obtained with electron-beam CT without oral or intravenous contrast ma

97 qualitatively similar to those obtained with electron-beam CT, as were the quantitative values of ren

98 ronary calcification have been obtained with electron-beam CT, but recently multislice CT, which is m

99 to those obtained with previously validated electron-beam CT.

100 data for comparison with those obtained from electron-beam CT.

101 2 years) underwent multi-detector row CT and electron-beam CT.

102 on of the rate of Pd deposition at different electron beam currents and as a function of distance fro

103 ally, the present study provides examples of electron beam damage on lithium-ion battery materials an

104 owever, battery materials are susceptible to electron beam damage, complicating the data interpretati

105 pristine chemical environments by minimizing electron beam damage, for example, using fast electron i

106 o the generation of narrow energy-spread GeV electron beams, demonstrating its robustness and scalabi

107 the incident electron beam, constraining the electron beam density that can be used and the duration

108 then deposited on the fibAu_NR arrays using electron beam deposition to improve the surface-enhanced

109 We measured coronary calcification using electron-beam dual-source computed tomography and Agatst

110 volving reduction by e(-)aq generated by the electron beam during in situ liquid TEM/STEM.

111 anus asymmetry of the nanomotors is given by electron beam (e-beam) deposition of a very thin platinu

112 Electron beam (e-beam) efficiently and non-thermally ina

113 sion electron microscopy studies is that the electron beam (e-beam) exposure does not fundamentally a

114 Electron-beam (e-beam) deposition of carbon on a gold su

115 a silicon-on-insulator (SOI) substrate using electron-beam (e-beam) lithography and reactive-ion-etch

116 In this report we used an electron-beam (e-beam) lithography technique to fabricat

117 sment of glomerular filtration rate (GFR) on electron-beam (EB) computed tomographic (CT) images, wit

118 number of lithographic methods such as AFM, electron-beam, elastomeric microprinting, and photolitho

119 , the coherence of which depends directly on electron beam emittance.

120 particular, the outstanding transparency to electron beam endows graphene membranes great potential

121 By controlling the electron-beam energy, we demonstrate the contrast imagin

122 layers with native defects are deposited by electron beam evaporation in an oxygen-deficient environ

123 The top contact was obtained by direct electron-beam evaporation on the molecular layers throug

124 trates: one used as-deposited (AS-DEP) by an electron-beam evaporator, and one prepared using the met

125 t a new resist that protects proteins during electron-beam exposure and its application in direct-wri

126 Total skin electron beam followed by allogeneic stem-cell transplan

127 radical protein footprinting using a pulsed electron beam from a 2 MeV Van de Graaff electron accele

128 ally symmetric magnetic field compresses the electron beam from the electron source into a long narro

129 Stable electron beams from a first LPA were focused to a twenty

130 high-gradient acceleration of monoenergetic electron beams from a helical IFEL.

131 rs on surfaces, but the damage caused by the electron beam has made it difficult to image zeolites.

132 The OAM states of electron beams have been shown to be similarly useful, f

133 Electron beam illumination greatly increases the local c

134 cedented, reaching 0.63 eV under the 200-keV electron beam illumination, and separated peaks of the P

135 llium-ion beam mills the particle, while the electron beam images the slice faces and energy-dispersi

136 Electron beam imaging and analysis show that olivine and

137 t of PINEM using a focused, nanometer-scale, electron beam in diffraction space for measurements of i

138 unction shaping facilitates the use of multi-electron beams in electron microscopy with higher curren

139 esent a method of creating highly collimated electron beams in graphene based on collinear pairs of s

140 ervations at Earth and the barely understood electron beams in Jupiter's magnetosphere, demonstrate t

141 re we report anti-planetward acceleration of electron beams in Saturn's magnetosphere along field lin

142 r rACP but not when PMN were challenged with electron beam-inactivated C. burnetii.

143 ve post-processing methods such as localised electron beam induced chemical etching.

144 We have applied this to the study of electron beam induced defect coalescence and to long ran

145 was designed specifically for use in focused electron beam induced deposition (FEBID) of Pt nanostruc

146 This is briefly illustrated by the case of electron beam induced deposition where additional strate

147 croscopes can now provide atomic resolution, electron beam induced specimen damage precludes high res

148 In addition, cryo-EM can be used to observe electron-beam induced dissipation of nanobubble encapsul

149 graphy, transmission electron microscopy and electron beam-induced current are used to clarify the de

150 To this end, we demonstrate electron beam-induced current measurements as a powerful

151 By clarifying the contrast mechanisms in electron beam-induced current microscopy, it is possible

152 By comparing beam energy-dependent electron beam-induced currents with Monte Carlo simulati

153 e report the experimental description of the electron beam-induced dynamics of nanoscale water drople

154 lectron-counting detector, we confirmed that electron beam-induced motion substantially degrades reso

155 improves on signal quality, while minimizing electron beam-induced structure modifications even for s

156 ields using off-axis electron holography and electron-beam-induced current with in situ electrical bi

157 namic high-angle annular dark-field imaging, electron-beam-induced damage was followed, revealing the

158 We prepare the metallic bead strings by electron-beam-induced interparticle fusion of nanopartic

159 Furthermore, though electron-beam-induced irreversible atomic displacements

160 We also report electron-beam-induced rapid displacement of monolayers,

161 ers in few-layer graphene sheets by means of electron-beam-induced sputtering.

162 ct-ratios of ~100 can be grown using focused electron-beam-induced-deposition.

163 we report that graphene edges fabricated by electron beam-initiated mechanical rupture or tearing in

164 ions are steady in liquid cell regardless of electron beam intensity.

165 ion trapping period at the region of ion and electron beam intersection.

166 Is (specifically (40)Ar(13+)) produced in an electron beam ion trap and retrapped in a cryogenic line

167 study aims to evaluate the effectiveness of electron beam irradiation (EBI) exposure on CSP for micr

168 ar. candida alba Buch.-Ham were submitted to electron beam irradiation at the doses of 0.5, 0.8 and 1

169 The effects of different electron beam irradiation doses in Amanita genus, were a

170 Among the emerging irradiation technologies, electron beam irradiation has wide applications, allowin

171 n(0.4)Co(0.18)Ti(0.02)O2 particles, repeated electron beam irradiation induced a phase transition fro

172 h nanometer-scale spatial density by focused electron beam irradiation induced local 2H to 1T phase c

173 ective formation of radicals was achieved by electron beam irradiation of aqueous solutions of H2O2 o

174 of vacuum packaging followed by high-energy electron beam irradiation on the shelf-life of fillets o

175 During Joule heating and electron beam irradiation, carbon atoms are vaporized, a

176 e behavior within the liquid cell, and under electron beam irradiation, is of paramount importance fo

177 In this study, we demonstrate that, under electron beam irradiation, the surface and bulk of batte

178 due to the extreme instability of MOFs upon electron beam irradiation.

179 , and rapid optical signal degradation under electron beam irradiation.

180 bilization to proteins during the vacuum and electron-beam irradiation steps.

181 ene is ferromagnetic and may be patterned by electron-beam irradiation.

182 e interaction between water and oxides under electron-beam irradiation.

183 An electron beam is a physical tool that is capable of prep

184 We also demonstrate that the micro-bunched electron beam is itself an effective wakefield driver th

185 ugh numerical simulations that a high-energy electron beam is produced simultaneously with two stable

186 f ultra-intense lasers and laser-accelerated electron beams is enabling the development of a new gene

187 rogressively varied relative to the incident electron beam it is also possible to extend electron mic

188 ts of the catalytic properties of Pt and the electron beam itself.

189 osed by the physics of 'standard' photon and electron beams limit further dose escalation.

190 Our method combines electron beam lithography and a low temperature hydrothe

191 We use electron beam lithography and wafer scale processes to c

192 the Au/ZnO-nanowire/Au nanomemory device by electron beam lithography and, subsequently, utilized in

193 2 nanowire arrays across 6-inch wafer, using electron beam lithography at 100 kV and polymethyl metha

194 A new resist material for electron beam lithography has been created that is based

195 Electron beam lithography is a powerful technique for th

196 r three-dimensional multilayer formats using electron beam lithography is described.

197 Electron beam lithography is used to pattern MoSe2 monol

198 all spacer technique instead of an expensive electron beam lithography method.

199 Using electron beam lithography the targeted structure has bee

200 We demonstrate that by using electron beam lithography to manipulate the nanoscale ge

201 nlike the common approaches, which depend on electron beam lithography to sequentially fabricate each

202 The photomasks were produced by electron beam lithography, and apertures in the photomas

203 in technologies such as electron microscopy, electron beam lithography, and field-emission flat-panel

204 , such as incompatibility with spin coating, electron beam lithography, optical lithography, or wet c

205 Besides electron beam lithography, stencil lithography, nano-imp

206 ch can be readily fabricated by conventional Electron Beam Lithography, sustain highly complex struct

207 ome high-end applications require the use of electron-beam lithography (EBL) to generate such nanostr

208 (SOI) layers achieved by combination of the electron-beam lithography (EBL), plasma dry etching and

209 ple of the viability of all-water-based silk electron-beam lithography (EBL), we fabricate nanoscale

210 Here we describe the use of electron-beam lithography and dry oxidative etching to c

211 lymer films, focused ion-beam sculpting, and electron-beam lithography and tuning of silicon nitride

212 ted that focused ion beam and layer-by-layer electron-beam lithography can be used to pattern the nec

213 Direct-write techniques such as electron-beam lithography can create complex nanostructu

214 f-the-art nanofabrication techniques such as electron-beam lithography have a resolution of a few nm

215 ensions of the DBTs enabled high-sensitivity electron-beam lithography of patterns with widths of onl

216 ransitions combined with nanometre-precision electron-beam lithography offers us the capability to fi

217 Previous routes use electron-beam lithography or direct laser writing but wi

218 Electron-beam lithography was used to fabricate micromet

219 of reach of lithographic approaches (such as electron-beam lithography) that are otherwise required t

220 iation (photo- and interference lithography, electron-beam lithography), mechanical contact (scanning

221 res with top-down patterning methods such as electron-beam lithography, an initial nanometer-scale la

222 ed either as 'top down', involving photo- or electron-beam lithography, or 'bottom up', involving the

223 g the high-precision alignment capability of electron-beam lithography, surfaces with complex pattern

224 tion of PhC cavities has typically relied on electron-beam lithography, which precludes integration w

225 isting fabrication methods typically involve electron-beam lithography--a technique that enables high

226 lk as a natural and biofunctional resist for electron-beam lithography.

227 t is currently achievable using conventional electron-beam lithography.

228 he molecular layers through masks defined by electron-beam lithography.

229 d nanoaperture arrays that were generated by electron-beam lithography.

230 be limited by laser diffraction, dephasing, electron-beam loading and laser-energy depletion.

231 post-manufacture HIPing the fatigue life of electron beam melting (EBM) additively manufactured part

232 The Electron Beam Melting (EBM) process alleviates this to s

233 ad industrial applicability, including where electron-beam melting or directed-energy-deposition tech

234 Electron beam nanolithography was used to fabricate 20 x

235 roscope (SEM), optical tweezers, and focused electron-beam nanomanipulation.

236 etermined by optimizing the intensity of the electron beam not to melt or deform the quartz nanotip w

237 The pores are created using the electron beam of a conventional transmission electron mi

238 The continuous electron beam of conventional scanning electron microsco

239 ield regime would translate to monoenergetic electron beams of ~100 keV.

240 detection of magnetic-field-aligned ion and electron beams (offset several moon radii downstream fro

241 , 49, 25, and 20%, respectively, measured by electron-beam or multi-detector row computed tomography.

242 nary artery calcification was assessed using electron-beam or multidetector computed tomography.

243 andwidth can be made with moderate laser and electron beam parameters.

244 grated chemiresistor (CR) vapor sensors with electron-beam patterned interface layers of thiolate-mon

245 refully spaced and shaped posts, prepared by electron-beam patterning of an inorganic resist, can be

246 Hollow cylindrical specimens, with electron beam physical vapour deposited coatings, were t

247 ajor difficulty is overcome using an 'aloof' electron beam, positioned tens of nanometres away from t

248 With an electron beam probe, we visualized the distribution of s

249 t high-resolution energy measurements of the electron beams produced from intense laser-plasma intera

250 However, the electron beams produced from previous laser-plasma exper

251 ngly charged lipid ions are irradiated by an electron beam, producing diagnostic product ions.

252 capability of analyzing and controlling the electron beam properties with few-femtosecond time resol

253 raphic slice parameters instead of projected electron beam properties.

254 n technology, which uses X-rays, gamma rays, electron beams, protons, or high-intensity focused ultra

255 method, combined with the precession of the electron beam, provides high quality data enabling the d

256 obulin A demonstrate that one submicrosecond electron beam pulse produces extensive protein surface m

257 on wakefields, where an intense relativistic electron beam radiates the demanded fields directly into

258 cts of a treatment program of intraoperative electron beam radiation therapy (IOERT) and external bea

259 realistic liquid conditions achievable under electron-beam radiation.

260 plemented using a deformable mirror with the electron beam signal as feedback, which allows a heurist

261 n rates are much higher, indicating that the electron beam strongly affects the galvanic-type process

262 t of femtosecond sources of X-ray pulses and electron beams suggests that they might soon be capable

263 ifferent techniques including intraoperative electron beam techniques and high-dose rate brachytherap

264 In electron cryo-microscopy (cryo-EM), the electron beam that is used for imaging also causes the s

265 By selecting the appropriate energy of the electron beam, the metal-nanotube interactions can be co

266 otene, and radiotherapy including total skin electron beam therapy.

267 omogeneous superficial dosing of traditional electron beam therapy.

268 photon energy is achieved by passing a 3 GeV electron beam through a two-stage plasma insertion devic

269 ffraction data obtained by using a very weak electron beam to collect large numbers of diffraction pa

270 results reveal how energy transfer from the electron beam to few-layer graphene sheets leads to uniq

271 nstrate the ability to employ a high density electron beam to perturb electric fields within the ICR

272 report a new strategy that uses the focused electron beam to probe the effect of differences in hydr

273 ores by using a tightly focused, high-energy electron beam to sputter atoms in 10-nm-thick silicon ni

274 ere then cross-linked onto Si surfaces using electron beams to form micron-sized patterns of the func

275 38 consecutive patients who underwent CTA by electron beam tomography (age 59 +/- 14 years, 70% males

276 Electron beam tomography (EBT) provides information on t

277 : 53 +/- 10 years) who presented to a single electron beam tomography facility for coronary artery ca

278 cohort of symptomatic patients who underwent electron beam tomography to allow for longer follow-up (

279 ultrasound to assess flow-mediated dilation, electron beam tomography to assess coronary artery and a

280 CAC by electron beam tomography was performed in 8549 asymptoma

281 variables and coronary calcium detected with electron beam tomography.

282 We used sequential electron-beam tomography (EBT) scanning to quantify chan

283 f known CHD, and had their CAC quantified by electron-beam tomography at baseline as part of a preven

284 ry artery calcium (CAC) scores measured with electron-beam tomography in asymptomatic patients for th

285 After the electron-beam treatment some additives decomposed and th

286 The safety of microwave and electron-beam treatments has been demonstrated, in regar

287 However, electron beams typically create high-energy excitations

288 er that can potentially accelerate a witness electron beam up to 6 GeV.

289 investigate sample heating from the incident electron beam using a transmission electron microscope.

290 Activated by an 80 keV electron beam, W reacts only weakly with the SWNT, Re cr

291 In this work, by steering a focused electron beam, we directly fabricate MX nanowires that a

292 -rays are usually produced via self-injected electron beams, which are not controllable and are not o

293 ontinuously under momentum transfer from the electron beam, while maintaining their structural integr

294 tudied the safety and efficacy of total skin electron beam with allogeneic hematopoietic stem-cell tr

295 Changing the arrival time of the electron beam with respect to the second-stage laser pul

296 emonstrate a laser accelerator that produces electron beams with an energy spread of a few per cent,

297 However, usually it generates electron beams with continuous energy spectra.

298 Electron beams with helical wavefronts carrying orbital

299 m the precursor compound SrBi2Ta2O9 under an electron beam within a high-resolution transmission elec

300 as cross-linked onto silicon wafers using an electron beam writer forming micro- and nanopatterns.