ライフサイエンスコーパス: vacuum

1 pitaxial growth and ion erosion in ultrahigh vacuum.

2 However, we do not operate in a social vacuum.

3 y photoelectron spectroscopy under ultrahigh vacuum.

4 levitation from atmospheric pressure to high vacuum.

5 s of high- and low-vapor pressure liquids in vacuum.

6 eft vast areas of health care in an evidence vacuum.

7 thout generating oxygen defects even in high vacuum.

8 ity gases and introduce the analyte into the vacuum.

9 in control of its built-in NV centres in low vacuum.

10 than 60 at the interface of copper metal and vacuum.

11 and reactions at the surfaces of liquids in vacuum.

12 eter decreases chatter, up to 400 mm Hg with vacuum.

13 ignificant amounts of water, even under high vacuum.

14 d layer that is stable within the microscope vacuum.

15 t, they were not subjected to degassing into vacuum.

16 nclassical states of light like the squeezed vacuum.

17 sure is reduced or the sample is annealed in vacuum.

18 dies at temperatures of finite difference in vacuum.

19 bly of two-dimensional building blocks under vacuum.

20 dynamics of a levitated nanoparticle in high vacuum.

21 create atmospheric plasma without an applied vacuum.

22 vironment is changed from atmosphere to high vacuum.

23 lativistic or near-relativistic electrons in vacuum.

24 stepwise SPD process in a UIC KDL 5 system (vacuum 10(-3)mbar, feeding flow 1.0 mL/min) was proceede

25 vaginal delivery with the use of forceps or vacuum (115 of 304 women [38%] and 104 of 314 women [33%

26 Samples were fried under vacuum (6.5 kPa, Twater-boiling-point=38 degrees C) or a

27 gestibility can be reduced when frying under vacuum (9.9kPa), after feeding Sprague-Dawley rats, whil

28 ymmetric double tunnel junctions with both a vacuum and a MgO tunnel barrier.

29 ency on the examples of alanine dipeptide in vacuum and C-terminal beta-hairpin of protein G in expli

30 Sensory characteristics of the vacuum and conventionally fried potato crisps were evalu

31 y-Assisted Vapor Deposition (ESAVD) is a non-vacuum and cost-effective method to deposit metal oxide,

32 ecular probe is not restricted to ultra-high vacuum and cryogenic settings.

33 nano/atomic scale from ambient to ultrahigh-vacuum and electrochemical environments.

34 oviding stabilization to proteins during the vacuum and electron-beam irradiation steps.

35 Chatter correlated with both vacuum and flow such that increasing either parameter de

36 In our work, eco-friendly, non-vacuum and low cost Electrostatic Spray Assisted Vapour

37 Vacuum and low temperature drying without osmotic pretre

38 h 15% of maltodextrin were dried by freeze-, vacuum and spray drying methods.

39 Samples were dried under vacuum, and carbonyl groups were protected with methoxyl

40 ions were successfully electrosprayed into a vacuum, and these three ECX(-) anions were investigated

41 x nanosheet colloidal solutions, followed by vacuum annealing at 200 degrees C.

42 tic adaptation utilizing liquid rubidium and vacuum annealing of the mixed elemental reagents in fuse

43 After a vacuum annealing process, a high gain in exceeding 10(7)

44 A total of 1509 MR imaging-guided vacuum-assisted biopsy procedures were performed in nine

45 ADH and DCIS diagnosed at MR imaging-guided vacuum-assisted biopsy were high, at around 25%, and wer

46 Both patients underwent ultrasound-guided vacuum-assisted biopsy.

47 S) at magnetic resonance (MR) imaging-guided vacuum-assisted breast biopsy and to explore the imaging

48 tato slices were fried in rapeseed oil under vacuum at 125 degrees C and atmospheric pressure at 165

49 sublime this high-spin diradical under high vacuum at 140 degrees C with no significant decompositio

50 ucting state is accomplished by annealing in vacuum at 400 degrees C.

51 recursor followed by thermal treatment under vacuum at 500 degrees C.

52 corated with iridium deposited in ultra-high vacuum at low temperature (7 K) as a function of Ir conc

53 minantly fabricated by complex and expensive vacuum-based integrated circuit (IC) processes.

54 hin films into organic solar cells through a vacuum-based polymer vapor printing technique.

55 MR-guided vacuum biopsy and MR-guided lesion bracketing were perfo

56 o acknowledge that they operate not within a vacuum but within a society in which diverse perspective

57 1 muC.cm(-2), and is preserved in ultrahigh vacuum, but disappears upon heating to 100 degrees C.

58 ty factors, such as cantilevers vibrating in vacuum, can show characteristic Fano asymmetric curves w

59 This material is prepared by the vacuum carbonization of a zinc-based metal-organic frame

60 idual gas analyzer (RGA) coupled with a high-vacuum chamber has been explored to measure atmospheric

61 a capillary pressure reduction system into a vacuum chamber, where they are analyzed using a quadrupo

62 ctor approach, i.e. minimizing the number of vacuum chambers and sample transferences.

63 tional microelectronic devices with a gas or vacuum channel may scale their speed, wavelength and pow

64 m pipette-dispensed PDMS microdroplets using vacuum-chucked microspheres.

65 and POP levels in dust from their household vacuum cleaners.

66 re more predictive of serum PBDE levels than vacuum-collected dust.

67 erties of three resulting products (an under-vacuum concentrate, a dilute-to-taste syrup and a ready-

68 why they overwhelmingly preferred the under-vacuum concentrate, regardless of their age, gender or f

69 components in the last stage of processing (vacuum concentration).

70 to 5 nm gap sizes, performed under ultrahigh vacuum conditions between a Au-coated probe featuring em

71 es at well-defined surfaces under ultra-high vacuum conditions represents an unconventional synthesis

72 cally-heated chemical vapor deposition under vacuum conditions were relatively thick and short.

73 on the known surface dynamic behavior under vacuum conditions, indicating that the same dynamics als

74 at room temperature so as to preserve ideal vacuum conditions, represent concrete alternatives, inde

75 r high oxygen conditions for 15 or 22days in vacuum conditions.

76 a turbomolecular pump-by 2% compared to high-vacuum conditions.

77 within water's "no man's land" in ultrahigh-vacuum conditions.

78 f molecular building blocks under ultra-high-vacuum conditions.

79 by calculations under crystal, solution, and vacuum conditions.

80 orophene) on silver surfaces under ultrahigh-vacuum conditions.

81 em appreciated potato-like fresh flavour of 'vacuum crisps' and classified this product as 'tasty'.

82 We present a high-vacuum cryo-transfer system that streamlines the entire

83 mbrane contactor (MC) and distillation under vacuum (D).

84 the functions of the Na treatment in our non-vacuum deposited CIGS are mainly used for defect passiva

85 igh-resolution e-beam lithography, thin film vacuum deposition and reactive-ion etching processes eli

86 ng a domestic microwave oven equipped with a vacuum desiccator inside.

87 For volatile DBPs, cryogenic vacuum distillation performed unsatisfactorily.

88 in the field, we found that a single PYP in vacuum does not provide an accurate description of the c

89 erence in the proximate composition; however vacuum dried CPI (VDCPI) had the highest bulk density an

90 For this purpose, beads were vacuum-dried and stored under controlled conditions.

91 acquired blood viscosity was compared with a vacuum-driven capillary viscometer at high shear rates (

92 ying (VD), convective drying (CD), microwave-vacuum drying (MVD) and combination of convective pre-dr

93 hot air convective drying (HACD), microwave vacuum drying (MWVD) and their combination (HACD+MWVD) o

94 The effect of freeze-drying (FD), vacuum drying (VD), convective drying (CD), microwave-va

95 An industrially applicable 2-step vacuum drying and heating process was explored, which fi

96 study drying of pequi slices (convective or vacuum drying at 40 degrees C and 60 degrees C) preceded

97 converted to powders using spray, freeze and vacuum drying methods, to investigate the effect of dryi

98 ion with a PG aqueous solution followed with vacuum drying of the supernatant.

99 se in temperature up to 100 degrees C during vacuum drying of XAD extracts resulted in degradation of

100 investigate the effect of temperature in the vacuum drying process of Mentha piperita L.

101 investigate the effect of temperature in the vacuum drying process of Mentha piperita L. (50 to 90 de

102 Fresh red currants were dried by vacuum drying process under different drying conditions.

103 It could be concluded that vacuum drying provides samples with good physico-chemica

104 ng with super critical CO2 drying, or simple vacuum drying up to 95 degrees C.

105 Mango slices were dried by microwave-vacuum drying using a domestic microwave oven equipped w

106 sses affect the quality of product, however, vacuum drying works under sub-atmospheric pressures.

107 r collected by passive sampler and in sieved vacuum dust (<150 mum).

108 Among all PFAAs, only PFNA in air and vacuum dust predicted serum PFNA.

109 illustrate the potential of engineering the vacuum electromagnetic environment to modify and to impr

110 riers into states that are hybridized to the vacuum electromagnetic field.

111 es benefit from the advantages of gas-plasma/vacuum electronic devices while preserving the integrabi

112 as many possible applications, such as novel vacuum electronic devices, particle detectors, accelerat

113 ibility of the liquid samples with ultrahigh vacuum environment of the electron optics and detector.

114 morphology, allows analysis in the ultrahigh vacuum environment, and reduces topographic artifacts, t

115 t oxygen stoichiometry, especially in a high vacuum environment, has been viewed as a challenge.

116 temperatures higher than 300 degrees C in a vacuum environment.

117 eutral, or low charged molecules into a high vacuum environment.

118 ives (2H-TPCN) with Co atoms in an ultrahigh vacuum environment.

119 lf-assembly on solid surface in an ultrahigh vacuum environment.

120 ize-selected supported clusters in ultrahigh-vacuum environments and under realistic reaction conditi

121 To prevent in-vacuum evaporation of the liquid content of the small gl

122 rown on kenaf/lignin agar followed by either vacuum evaporation or acid precipitation.

123 n nanotube electrodes (ICE) were prepared by vacuum filtering a well-dispersed carbon nanotube-Nafion

124 carbon nanotubes can be prepared using slow vacuum filtration.

125 s and are prepared into transparent paper by vacuum filtration.

126 tion intermediate that was generated by high-vacuum flash pyrolysis (HVFP) of the corresponding p-tos

127 Fortunately, vacuum fluctuations are not immutable and can be 'squeez

128 Vacuum fluctuations are one of the most distinctive aspe

129 at enable the inhibition and manipulation of vacuum fluctuations have been key to our ability to cont

130 Here, we theoretically demonstrate that vacuum fluctuations may be naturally inhibited within bo

131 per cent below the fundamental limit set by vacuum fluctuations, while the photon statistics remain

132 ht into oxygen stoichiometry control in high vacuum for understanding the fundamental properties of S

133 Vacuum fried samples showed less starch gelatinization (

134 Results showed that vacuum-fried dough has a lower degree of gelatinization

135 and higher unavailable glucose fractions in vacuum-fried dough.

136 f 1, Der p 1, Mus m 1, and Rat n 1) in dust vacuumed from nearly 7000 bedrooms were measured by usin

137 arch was focused on a critical assessment of vacuum frying as a technology enabling minimization of a

138 In vitro studies have shown that vacuum frying may be an effective process to reduce star

139 This study assessed the effect of vacuum frying on starch gelatinization and its in vitro

140 Vacuum frying reduced the formation of acrylamide by 98%

141 nal asymmetry between the polar Cu2N and the vacuum gap breaks inversion symmetry in the alkali halid

142 requency acoustic phonons tunnel through the vacuum gap by coupling to evanescent electric fields, pr

143 We also find that the vacuum gap resulting from the widely used 300 nm-oxide s

144 nsfer between planar surfaces separated by a vacuum gap smaller than the thermal wavelength exceeds t

145 r, dominated by frustrated modes, only for a vacuum gap thickness of 10 nm and if both electrical and

146 upon 2D material type and number of layers, vacuum gap, oxide thickness, and detecting wavelength, t

147 cale planar surfaces separated by a nanosize vacuum gap.

148 ity 2 W/cm(2) with ~47% efficiency at 300 nm vacuum gap; at 2100 degrees K, 24 W/cm(2) with ~57% effi

149 e-based extraction method does not require a vacuum-gap, which is a significant reduction in the requ

150 d or even new models of heat transfer across vacuum gaps at nanometre distances.

151 Our measurements were performed in vacuum gaps between prototypical materials (SiO2-SiO2, A

152 Using planar capacitors with vacuum gaps of 60 nm and spiral inductor coils of micron

153 y high efficiency and output power, at large vacuum gaps.

154 lied for the analysis of a basic fraction of vacuum gas oil.

155 ckaging materials (i.e. natural casing under vacuum, glass jar, aluminum tube and OVTENE(R)) during 1

156 ed with time (glass jar>natural casing under vacuum>aluminum tube>OVTENE(R)).

157 zinc-oxide-based ultraviolet sensors in air/vacuum has long been an obstacle to developing such dete

158 ing Ru(bpy)3, emission is bipolar, occurs in vacuum, has rapid rise time (<5 ms), and persists for >1

159 ) centre in a nanodiamond, levitated in high vacuum, has recently been proposed as a probe for demons

160 s with nitrogen-vacancy (NV) centres in high vacuum have been proposed as a unique system for experim

161 By vacuum heating the hybrid materials at an intermediate t

162 u growth of graphene on flaky Cu powders and vacuum hot-press sintering.

163 e glycol (PEG) and RMS were prepared through vacuum impregnating method.

164 Vacuum improved efficiency up to 500 mm Hg independent o

165 However, liberating electrons into gas/vacuum in a practical microelectronic device is quite ch

166 s and layers and a post-annealing process in vacuum in order to remove the organic template.

167 Increasing vacuum increased efficiency regardless of aspiration rat

168 roduces the same high-quality images without vacuum-induced artifacts; it is also less invasive, whic

169 Put at 0, 1 and 2mM were applied to fruit by vacuum infiltration at 26.665kPa for 8min and then store

170 "interfacial" hydrated electron at the water/vacuum interface, performed using liquid microjet photoe

171 Au plasmon resonance is localized at the Au/vacuum interface, rather than presenting an isotropic di

172 tion microchannel", before entering the high-vacuum ion source.

173 effect on efficiency through 50 mL/min, when vacuum is at 400 mm Hg or higher, and only up to 35 mL/m

174 yer, a molecule whose HOMO energy level in a vacuum is close to the Fermi level of the gold bottom el

175 eak field gravitational waves propagating in vacuum is derived directly from the linearized general r

176 icate that oxygen vacancy generation in high vacuum is strongly influenced by the energetics of the l

177 thermal-activation (400-500 degrees C) under vacuum, is demonstrated.

178 /- 0.8)c, where c is the speed of light in a vacuum, is in the incipient stages of a collision with a

179 mm Hg or higher, and only up to 35 mL/min at vacuums less than 400 mm Hg.

180 (-)(aq) in bulk water lies too far below the vacuum level to induce such reactions.

181 A recent measurement of the energy (below vacuum level) of the putative "interfacial" hydrated ele

182 ndent already a few electron-Volts above the vacuum level.

183 pothetical Zn-based ZIFs with respect to the vacuum level.

184 from the Fermi level of the electrode to the vacuum level.

185 of MoTe2 flakes annealed via RTA at various vacuum levels are tuned between predominantly pristine n

186 Vacuum levels were tested at 200, 300, 400, and 500 mm H

187 onradioactive electron emitters require high vacuum (<10(-6) hPa) to prevent electrical sparkovers.

188 ext to the ion trap mass analyzer inside the vacuum manifold.

189 ve optical heating of the nanodiamonds under vacuum may make the method impractical with currently av

190 ior development with cyanoacrylate fuming or Vacuum Metal Deposition, was also examined.

191 , for example, surface plasmon-polaritons at vacuum-metal interfaces.

192 lood from the micro-channel (4.17cP) and the vacuum method (4.22cP) at 500 s(-1) were closely correla

193 by a combined method (convective pre-drying+vacuum microwave finish drying).

194 onvective drying (CD: 50, 60, 70 degrees C), vacuum-microwave drying (VMD: 120, 480, 480-120 W), a co

195 , a combination of convective pre-drying and vacuum-microwave finish drying [(CPD (60 degrees C)-VMFD

196 machine was used in peristaltic and Venturi vacuum modes with transversal and micropulsed ultrasound

197 ed DPH is stable for at least 24 h under the vacuum of our MALDI mass spectrometer.

198 nto the substrate, and then deposit them (in vacuum-off mode) in the desired location.

199 which provides values of ca. -4.0 eV versus vacuum on both ITO and TiO2 electrodes.

200 ronic circuitry by using an empty nozzle (in vacuum-on mode) to pick up individual components, place

201 b:TiO2 conductors on glass (without breaking vacuum) only occurs within a narrow processing range and

202 scale using simple metal precursors without vacuum or heat.

203 ging conditions (MAP), in our case, aerobic, vacuum or high O2, to extend the shelf life of beef.

204 instability and the need to work under high-vacuum or high-temperature conditions have imposed strin

205 nly becoming relevant for structures held in vacuum or under extreme thermal isolation.

206 teviol glycosides (SGs) by spray, freeze and vacuum oven drying in order to minimise the bitter after

207 tracts, then spray drying, freeze drying, or vacuum oven drying to prepare dry, flour-like matrices.

208 polarization from ferroelectric material in vacuum (P 10(-6) torr).

209 rgent data were compared to those subject to vacuum packaging as well as conventional preservative me

210 concentration was higher under air than in a vacuum packaging atmosphere.

211 ical, microbiological and sensory quality in vacuum-packed fresh shibuta (Barbus grypus) fillets duri

212 egarding the total metabolites content, were vacuum packing and freezing for intermediary storage tim

213 t of freezing, freeze-drying, air drying and vacuum packing, was evaluated on these potential aroma m

214 TiO2 multishell nanotubes by a combined full vacuum-plasma approach at mild temperatures.

215 A three-step vacuum procedure for the fabrication of vertical TiO2 an

216 zed as near-infrared absorbing materials for vacuum processable organic solar cells.

217 any external chemical, high-temperature, or vacuum processes.

218 These results show how vacuum processing may be used to control the degree of s

219 Quantum fluctuations of the electromagnetic vacuum produce measurable physical effects such as Casim

220 by e-beam to the eC surface without breaking vacuum protects the surface from the environment after f

221 When a 12 W vacuum pump was used for carrying the generated CO2 out

222 rbenes were generated by falling solid flash vacuum pyrolysis (FS-FVP).

223 y 2080 cm(-1) by a combination of mild flash vacuum pyrolysis (FVP) at 200-600 degrees C with low tem

224 Flash vacuum pyrolysis (FVP) of 1-(5-(13)C-5-tetrazolyl)isoqui

225 Flash vacuum pyrolysis (FVP) of azides is an extremely valuabl

226 iazolo[1,5-a]quinoline by conventional flash vacuum pyrolysis (FVP) were observed by IR spectroscopy.

227 Flash vacuum pyrolysis of 1,3-bis-iodomethyl-benzene (m-C8H8I2

228 Through flash vacuum pyrolysis of CF3 S(O)NCO at ca. 1200 K, sulfinyl

229 e cascade (RDA/ICE) reaction under the flash-vacuum pyrolysis of maleic anhydride adducts is develope

230 Upon flash vacuum pyrolysis of sulfinyl azide CF3S(O)N3 at 350 degr

231 apors rapidly through a very hot oven (flash vacuum pyrolysis) promotes high-temperature thermal reac

232 Via flash vacuum pyrolysis, even metaparacyclophanes as small and

233 enzyne, 1,2-azaborine, is generated by flash vacuum pyrolysis, trapped under cryogenic conditions, an

234 kcal/mol and thus to be accessible via flash vacuum pyrolysis.

235 ew route harnessing a ring-contracting flash vacuum pyrolytic extrusion of sulfur dioxide from the re

236 For example, a direct modulation of the vacuum Rabi frequency is obtained by deforming the EMNZ

237 We selectively stimulate vacuum Rabi oscillations between the transmon and indivi

238 We also observe quantum beats, so-called vacuum Rabi oscillations, between the upper and lower vi

239 asmons, polarons, and a phonon analog of the vacuum Rabi splitting in atomic systems.

240 owave cavity, as shown by the observation of vacuum Rabi splitting.

241 inner pressures of the device in the medium vacuum range (>10(-3) hPa).

242 nt coming from a nanoLC column into the high-vacuum region of an electron ionization source.

243 Cleaving a single crystal under ultra-high vacuum results in multiple terminations: an ordered Pt4A

244 Annealing in ultrahigh vacuum revealed a thermal stability limit of approximate

245 erminated scanning probe is performed at the vacuum-solid interface often at a few Kelvin, but is not

246 dimensional bimolecular organizations at the vacuum-solid interface.

247 s become possible through the utilization of vacuum-stabilized imaging windows.

248 Compared to vacuum-stabilized windows, this window produces the same

249 linking atmospheric pressure and the initial vacuum stage of the mass spectrometer.

250 the operation time, each cavity remains in a vacuum state, thus decoherence caused by the cavity deca

251 Only the charged crystal structure in vacuum supports a LBHB if Arg52 is neutral in PYP at the

252 ion by infrared laser pumping, and ultrahigh vacuum surface analysis techniques make it possible to s

253 While ultrahigh vacuum surface science techniques have provided useful i

254 ce of low-frequency nonlocal plasmons at the vacuum-surface interface of a superlattice of N graphene

255 ty used for frequency stabilisation with its vacuum system takes 30 x 30 x 30 cm(3).

256 d within a single superconducting magnet and vacuum system.

257 with O2, the nitrene was generated by flash vacuum thermolysis (FVT) of phenylazide and subsequently

258 uctive membrane to protect animal cells from vacuum, thus enabling high-resolution electron microscop

259 Ultrahigh vacuum tip-enhanced Raman spectroscopy (UHV-TERS) combin

260 e of Cot molecules and Eu vapor in ultrahigh vacuum to an inert substrate, such as graphene.

261 olarization from a ferroelectric material in vacuum to dramatically enhance the TENG output power.

262 ing and spectroscopy, from operation at high vacuum to in live cells.

263 spot for global biodiversity, we used a seed vacuum to increase dispersal at spatial scales varying f

264 These are collected by applying a vacuum to the top of the bottle and cryo-trapping the ex

265 ealistic model for parameter dispersion, and vacuum, to confirm the existence of one-way scatter-immu

266 of technological advances which took us from vacuum tubes to cell phones.

267 ht sources, such as free-electron lasers and vacuum tubes, rely on bunching of relativistic or near-r

268 decomposition of adsorbed 1 under ultrahigh vacuum (UHV) conditions proceeds through initial CO loss

269 (111) upon thermal annealing under ultrahigh vacuum (UHV) conditions.

270 d on a rutile TiO2(110) surface in ultrahigh vacuum (UHV) is studied with spin-polarized density func

271 In ultrahigh vacuum (UHV), TERS can be performed in pristine environm

272 as devised to integrate a gas chromatography-vacuum ultraviolet (GC-VUV) data set in order to provide

273 A GC-vacuum ultraviolet (UV) method to perform group-type sep

274 A new vacuum ultraviolet (VUV) detector for gas chromatography

275 are ionized by 10 eV photons generated by a vacuum ultraviolet (VUV) krypton discharge lamp.

276 aneous-detection spectrometer working in the vacuum ultraviolet (VUV) region of 125-240 nm overcomes

277 Here we report vacuum ultraviolet absorption spectra for the lowest-lyi

278 Vacuum ultraviolet spectra emanating from krypton atoms,

279 via dispersive wave emission in the deep and vacuum ultraviolet, with a multitude of applications.

280 that uniquely reaches simultaneously to the vacuum ultraviolet, with up to 1.7 W of total average po

281 eration of high harmonics extending into the vacuum-ultraviolet and extreme-ultraviolet regions of th

282 on provides a potential approach to generate vacuum-ultraviolet frequency comb.

283 cs as a potential source of intense coherent vacuum-ultraviolet radiation has received considerable a

284 nization (by tunable low energy electrons or vacuum-ultraviolet synchrotron radiation) for product de

285 Chatter improved with increasing vacuum, up to 400 mm Hg (P = .003 for 200 vs 300 mm Hg a

286 chromatography, with selective detection via vacuum UV absorption spectroscopy.

287 Vacuum UV detection was necessary to solve a coelution b

288 e via various spectroscopic tools, including vacuum UV photoionization mass spectrometry, absorption

289 The gas chromatography (GC)-vacuum UV results for the Synfuel samples were similar (

290 ancies were noted between SFC results and GC-vacuum UV results; however, these samples are known to b

291 namics (AIMD) simulations and molecular beam vacuum-UV (VUV) photoionization mass spectrometry experi

292 Here, we implement ultrafast vacuum-UV (VUV)-driven electron-ion coincidence imaging

293 We used vacuum-UV photoionization aerosol mass spectrometry and

294 rowth substrates (Ni(C)/(B, N)-source/Ni) in vacuum, wafer-scale graphene/h-BN films can be directly

295 aspiration further increased efficiency when vacuum was at 400 and 500 mm Hg (P = .004 for 20 vs 35 m

296 -lived, metastable species does exist at the vacuum/water interface, it would be extremely difficult

297 cal-density-of-states which tunnels into the vacuum, when compared with the ferromagnetic background,

298 icant buckling and numerous polymorphs as in vacuum, whereas on more reactive Ag, Cu, and Ni, the pol

299 s the complete CO2 desorption at 328 K under vacuum with an associated moderate energy input of 54 kJ

300 ion factor values exceeding 10(8) A C(-1) in vacuum with undiminished responses in open air, and clea