ライフサイエンスコーパス: volt

1 (with a barrier to tunneling of 1.4 electron volts).

2 nergy than rutile (2.32 versus 3.00 electron volts).

3 with a very low charge potential (about 3.2 volts).

4 y at ~0.3 hertz, with a peak voltage of ~1.0 volt.

5 apparent activation energy of 0.16 electron volt.

6 ation with a normalized magnitude of ~7% per volt.

7 on monoxide (CO) at overpotentials below 0.2 volt.

8 pronounced at approximately 1 kilo-electron volt.

9 er the narrow range of a few hundredths of a volt.

10 ficiency of 1% for n-type TiO2 biased at 0.6 volt.

11 t unoccupied orbitals of 0.4 to 0.9 electron volt.

12 inuously and actively tuned by more than 0.6 volt.

13 uch voltages higher than several hundreds of volts.

14 ve this at a low power-supply voltage of 0.1 volts.

15 arcs, and a gap as large as 80 millielectron volts.

16 f Ag, Cu, and Au electrodes to 3.65 electron volts.

17 ging from gigaelectron volts to teraelectron volts.

18 ctron intensity down to ~10 x 10(6) electron volts.

19 ivation energies of 100 to 150 millielectron volts.

20 electrochemical voltage over a range of 2.5 volts.

21 ly narrow absorber band gap of 1.55 electron volts.

22 and voltages, from several volts to tens of volts.

23 minimum (i.e., equilibrium) voltage of 1.33 volts.

24 c rays to energies close to ~10(15) electron volts.

25 10(8) electron volts and 3 x10(11) electron volts.

26 ndem open-circuit voltage of as high as 1.92 volts.

27 rved at energies from 0.2 to 6 kilo-electron volts.

28 tical gap edge of approximately 2.2 electron volts.

29 nection-driven flows are just a few electron volts.

30 ry high energies of several million electron volts.

31 h a band width of approximately 0.5 electron volts.

32 ) and an optical energy gap of 0.34 electron volts.

33 dulators operate with halfwave voltages of 5 volts.

34 rption energies between 0.2 and 3.5 electron volts.

35 within ~10 seconds by the application of ~10 volts.

36 Mean stimulation voltage was 3.0+/-0.1 volts.

37 ctrum, up to photon energies of 280 electron volts.

38 via synchrotron radiation from peta-electron-volt (10(15) electron volts) electrons in a region small

39 ctron microscope, we detected a 5.7-electron volt (2175 angstrom) feature in interstellar grains embe

40 ately 2.5 x 10(8) T. vaginalis cells and 350 volts, 960 microFd for electroporation; however, other c

41 tron-hole excitations below 75 millielectron-volts, a manifestation of a partially coherent state for

42 ll-defined discharge voltage plateaus near 2 volts, a specific capacity of about 70 mA h g(-1) and a

43 overlayer state that is 2.3 +/- 0.2 electron volts above the Fermi level.

44 an unoccupied electronic state 2.4 electron volts above the Fermi level.

45 ally spin-independent already a few electron-Volts above the vacuum level.

46 es produce a sustained voltage of around 0.5 volts across a 7-micrometre-thick film, with a current d

47 The updated Volt'Air model allowed a better description of the volat

48 We used the Volt'Air model: we first extended the van Genuchten curv

49 lization following application on bare soil (Volt'Air) and the local-scale dispersion and deposition

50 e ultraviolet to more than 1.6 kilo-electron volts, allowing, in principle, the generation of pulses

51 Electrochemical volt- ammetry recording revealed the restoration of DA r

52 ic and perfused segments on low-kiloelectron volt and iodine material density images.

53 d at -2 volts, and read at approximately 0.1 volt and may be recycled many times under ambient condit

54 rgy are highly scalable and could be below 1 volt and single femtojoules per bit, respectively.

55 scope at energies between 2 x 10(8) electron volts and 3 x10(11) electron volts.

56 s at a supra-electroporation threshold of 80 volts and 300 microseconds were applied across the strat

57 of pulsed emission between 100 mega-electron volts and 400 GeV is described by a broken power law tha

58 de of approximately 10 to 100 milli-electron volts and a nanotube radius (r) dependence of approximat

59 f 25 unipolar elements generated more than 2 volts and a peak power of 5 microwatts using body heat.

60 B1g symmetry and energy of 75 millielectron-volts and a pseudogap for electron-hole excitations belo

61 ith a temperature of 1.0 to 1.5 kiloelectron volts and an optical depth around 10.

62 ticles to energies exceeding 10(12) electron volts and are bright sources of very-high-energy (VHE) g

63 tor with a discrete band gap of 1.9 electron volts and can be chemically oxidized to enhance conducti

64 at include peak potential differences of 600 volts and currents of 1 ampere.

65 c cells with an open-circuit voltage of 1.23 volts and efficiency of 10.77%.

66 ls that reached open-circuit voltages of 1.2 volts and power conversion efficiency of over 17% on sma

67 enerate streaming potentials on the order of volts and that this is sufficient to carry out reactions

68 ar the OFF state) at low supply voltages (<1 volt) and ultralow power (<1 nanowatt).

69 ductivity (activation energy, 0.054 electron volts) and an optical energy gap of 0.34 electron volts.

70 ncreases the actuation voltage (to about 100 volts) and can compromise reliability owing to dielectri

71 e voltage plateaus (1.1-0.2 volts or 1.8-0.8 volts) and insufficient cycle life (less than 100 cycles

72 ow energy gaps (between 0.2 and 2.0 electron volts) and low densities, and they may be useful in opto

73 irtual monoenergetic energy (in kiloelectron volts) and phantom size by using a paired t test.

74 emitter of hard x-rays (2 to 10 kiloelectron volts), and the emission forms a narrow continuous ridge

75 iency (93.2%) with a voltage gap of only 0.2 volt, and impressive rechargeability.

76 e switch is opened at +2 volts, closed at -2 volts, and read at approximately 0.1 volt and may be rec

77 trons with energies less than 1 kiloelectron volt are substantially energized in Mercury's magnetosph

78 an oscillators, whereas the pineal gland and VOLT are weak oscillators that require input from the SC

79 100 kilocalories per mole (about 4 electron volts) are reported for polyatomic molecules, including

80 gy separation of approximately 0.25 electron volts, are capped by an epitaxial zinc selenide (ZnSe) s

81 igh zero-field splitting of 58 millielectron volts as well as slow relaxation of the Co atom's magnet

82 sts (700 hours at a fuel cell voltage of 0.4 volts) as well as excellent four-electron selectivity (h

83 f gamma-ray emissions above 200 megaelectron volts at a significance level of 17sigma from the globul

84 he plasma frequency of 32.5 +/- 2.1 electron volts at a temperature of 5.5 kelvin, with a correspondi

85 cking or folding geometry that generates 110 volts at open circuit or 27 milliwatts per square metre

86 EO modulators with halfwave voltages of 0.8 volts (at a telecommunications wavelength of 1318 nanome

87 at 320, 400, 490, 560, 600, and 670 electron volts, attributable to electron capture and radiative de

88 e develop an infrared-absorbing 1.2-electron volt band-gap perovskite, FA0.75Cs0.25Sn0.5Pb0.5I3, that

89 ielectron volts to less than 1 millielectron volt because of gain narrowing and eventually laser acti

90 rgy splitting of more than 10 milli-electron volts between the K and K' valley exciton transitions.

91 ifference of approximately 60 milli-electron volts between zero-point energies of incident protons an

92 article physics is several trillion electron volts, but colliders capable of reaching this regime (su

93 ve voltage-interaction length product of 2.2 volt-centimeters.

94 measurements of energetic (>40 kiloelectron volts) charged particles on Voyager 1 from the interface

95 At an applied potential of 0.3 volt, chemically modified n-type TiO2 performs water spl

96 h a passivated graphite anode, we create a 4-volt-class aqueous Li-ion full cell with an energy densi

97 The switch is opened at +2 volts, closed at -2 volts, and read at approximately 0.1

98 hot electrons with energies of mega-electron volts, cold ions in the inner wall surface implode towar

99 4.1 milliamps per square centimeter at -0.22 volts, compared with -85 millivolts and 1.1 milliamps pe

100 ) from 0.5 to approximately 3.5 megaelectron volts, consistent with a weak termination shock having a

101 ction at a collision energy of 1.97 electron volts contradict this behavior.

102 ntration rises, a narrow peak at ~2 electron volts, corresponding to vertical photodetachment of loca

103 veal a confinement gap of up to 0.5 electron volt, demonstrating the possibility of molecular-scale e

104 open-circuit photovoltages of more than 1.1 volts, despite the relatively narrow absorber band gap o

105 arp peaks (widths of 12 to 25 milli-electron volts) devoid of the characteristic background absorptio

106 ) as a function of maximum work (in electron volts) done by electron (laser photon) E(alpha) - E(beta

107 s of energetic radiation (>> 10 kiloelectron volts) during the dart leader phase of rocket-triggered

108 ic field of antibody immobilization and a 60-volt electric field of antibody immobilization showed th

109 devices made of this material can detect sub-volt electric potentials in salt water.

110 , bidirectional, energetic (>15 kiloelectron volts) electron beams were discovered by the Galileo ene

111 on interactions rather than low-energy (<0.1 volts) electron-boson interactions are responsible for s

112 intensities of approximately 10-megaelectron volt electrons, ACRs, and galactic cosmic rays have stea

113 ion from peta-electron-volt (10(15) electron volts) electrons in a region smaller than 1.4 x 10(-2) p

114 resolved the 67.87- and 78.32-kilo-electron volt emission lines from decay of (44)Ti produced in the

115 ated leptons, but the measured tera-electron volt emission profile constrains the diffusion of partic

116 coherently interconvert over an ~1-electron volt energy barrier with a 140-milli-electron volt shift

117 near optical spectroscopy with nano-electron volt energy resolution and low-temperature near-field mi

118 by ions in the several tens of kiloelectron volts energy range.

119 (-1)) at pH 7 with an overpotential of -0.55 volts, equivalent to a 26-fold improvement in activity c

120 ed attraction of approximately 0.12 electron volt (eV).

121 kite cell optical band gap of ~1.75 electron volts (eV) can be achieved by varying halide composition

122 verage temperature dependence (0.96 electron volts (eV)), which corresponds to a 57-fold increase bet

123 analyte surface activity in the gentler zero volt experiment than in the other methods due to the sig

124 photon energy greater than 100 mega-electron volts) flares from this source detected by the Large Are

125 ity of greater than 5 x 10(4) picometres per volt for second harmonic generation at a wavelength of a

126 through electrochemical poling of a SOC at 2 volts for a few seconds.

127 1.1 milliamps per square centimeter at -0.20 volts for a platinum-carbon electrode.

128 energies of approximately 400 millielectron volts for semiconducting single-walled nanotubes with 0.

129 deling yields an energy of 4.3 millielectron volts for the lowest quantized phonon subband and a tube

130 VPT scores (mean +/- SEM volts) for OA subjects and controls were as follows: fir

131 VPT scores (mean+/-SEM volts) for OA subjects and normal subjects were as follo

132 mma-ray emission (0.1 to 10 billion electron volts) from the recently detected optical nova of the sy

133 bservatory (HAWC), of extended tera-electron volt gamma-ray emission coincident with the locations of

134 gnetic order through application of a +/-0.5-volt gate voltage, a value compatible with present micro

135 c actuators, low operating voltages of a few volts generate large actuator strains.

136 b pulsar at energies above 100 giga-electron volts (GeV) with the Very Energetic Radiation Imaging Te

137 and vascular organ of the lamina terminalis (VOLT) harvested from SCNX rats but had little effect on

138 l generation mix at night; (2) the Chevrolet Volt has higher expected life cycle emissions than the T

139 distinct nonthermal (0.2 to 6 kilo-electron volts) heliosheath proton populations with spectral sign

140 al energy barriers that are several electron-volts high and several nanometers wide.

141 iconducting behavior (bandgap ~1.94 electron volts), high strength (~66 gigapascals), and excellent a

142 arged ions are observed, but at or near zero volts, highly charged ions are observed for peptides and

143 "lattice") Debye energy of 1.1 millielectron volts, implying a small intertube coupling in bundles.

144 nt of 2.75 amps per square centimetre at 1.3 volts in 50% water/nitrogen gas).

145 opic red shift of 4.8 +/- 0.4 milli-electron volts in C-O asymmetric stretching modes was observed fo

146 on and potential cycling between 0.6 and 1.1 volts in over 30,000 cycles.

147 , it is found that changes of milli-electron volts in the energy range of up to 50 electron volts rev

148 giant electrocaloric effect (0.48 kelvin per volt) in 350-nanometer PbZr(0.95)Ti(0.05)O3 films near t

149 1.62 per angstrom (the barrier, 2.6 electron volts) in a frozen 2-methyl-tetrahydrofuran glass.

150 oad resonance centered at +20 milli-electron volts) in spectroscopic measurements, indicating that it

151 An applied bias of a fraction of a volt increases the measured pressure-driven ionic transp

152 The transistors operate in air with a few volts input.

153 onds and deposited many tens of megaelectron volts into the detector.

154 etic and ferromagnetic order with only a few volts, just above room temperature.

155 first observed at an applied voltage of 1.5 volts, just slightly above the minimum (i.e., equilibriu

156 ormation at energies of tens of kiloelectron volts (keV) at altitudes of ~0.8-1.5 Earth radii on time

157 with energies greater than 30 kilo-electron volts (keV) shortly after its insertion into orbit about

158 ing intensities of ions from 40 kiloelectron volts (keV) to >/=50 megaelectron volts per nucleon and

159 x-ray emission line around 3.5 kilo-electron volts (keV).

160 f electron volts to hundreds of kiloelectron volts (keV).

161 ved iodine attenuation at lower kiloelectron volt levels and reduced beam-hardening artifacts at high

162 uation with VM imaging at lower kiloelectron volt levels enables better delineation and diagnostic ac

163 m-hardening artifacts at higher kiloelectron volt levels have been demonstrated from all major manufa

164 nodes, together with good cyclability of a 4-volt lithium cobalt oxide cathode and operation as low a

165 hase ionization energy (onset, 3.51 electron volts) lower than that of the cesium atom (which has the

166 junction with its wide bandgap (6.2 electron volts) makes cBN a promising material for microelectroni

167 w of aqueous lithium-ion batteries to 3 to 4 volts, making it possible to couple high-voltage cathode

168 e in bulk electroporation, where hundreds of volts may be applied between electrodes, a rather small

169 ne is composed predominantly of megaelectron volt (MeV) electrons that wax and wane in intensity on t

170 The optical and >100-megaelectron volt (MeV) gamma-ray flux show a close correlation durin

171 A preliminary design of a mega-electron-volt (MeV) monochromator with 10(-5) energy spread for u

172 typically extend up to 10 to 20 megaelectron volts (MeV); a simple bremsstrahlung model suggests that

173 ng millivolts, as compared with the thousand volts needed to achieve giant-stroke electrostatic actua

174 al emissions, and (conceivably) megaelectron-volt neutrino emissions.

175 ors: size, the production of 14-megaelectron volt neutrons, and maintenance.

176 oped silicon wafers in air, with only +/-2.5 volts of driving voltage, a few microamperes of current

177 te fish, humans, and horses with hundreds of volts of electricity.

178 n the charges, we measure ~200 millielectron volts of electrostatic energy arising from electron-hole

179 ormation, where H atoms lose 1 to 2 electron volts of energy within a 10-femtosecond interaction time

180 don exposure averaging 130,000 mega-electron volts of potential alpha energy per liter of air, per wo

181 resistance (TER) was measured (by epithelial volt ohmmeter), and cytotoxicity was determined by trypa

182 TEER was measured in 3D models using a volt/ohmmeter and cellZscope.

183 ydronium ions were soft-landed at 1 electron volt on cold films of 3-methylpentane ("oil") on a metal

184 oscopy near the carbon K-edge ( 284 electron volts) on a tabletop apparatus to directly reveal the va

185 inal tandem efficiencies of 17.0% with >1.65-volt open-circuit voltage.

186 without discharge voltage plateaus (1.1-0.2 volts or 1.8-0.8 volts) and insufficient cycle life (les

187 ayer, with a temperature of 100 kiloelectron volts or higher and an optical depth around unity.

188 be driven by electric signals of only a few volts or optical signals with power of only a few milliw

189 extend up to an energy of about 0.3 electron volt, or 40kTc (where k is the Boltzmann constant).

190 a maximum energy gain of 0.915 kilo-electron volts over 30 micrometers, corresponding to an accelerat

191 rformance and a suggested mechanism for zero volt paper spray using chromatography paper are presente

192 ic system of silica to strong (more than one volt per angstrom) few-cycle optical (about 750 nanometr

193 the Fermi level of 15.5 states per electron volt per mole.

194 lly low counting rates of >0.5 mega-electron volt per nuclear particle.

195 bility as high as 1.3 square centimetres per volt per second and a high on/off current ratio exceedin

196 ility of more than 0.3 square centimeter per volt per second and current modulation of 10(5), with th

197 ained as high as 1.12 square centimetres per volt per second at 100 per cent strain along the directi

198 re up to 1200 and 320 square centimeters per volt per second at low temperatures for hole and electro

199 ease from 2.7 and 1.7 square centimeters per volt per second at room temperature up to 1200 and 320 s

200 ities as high as 4050 square centimeters per volt per second at room temperature.

201 ility values of >1000 square centimeters per volt per second in field-effect transistors with microwa

202 rformance (more than 1 square centimetre per volt per second) even after a hundred cycles at 100 per

203 ities exceeding 10(4) square centimeters per volt per second.

204 obility of 167 +/- 20 square centimetres per volt per second.

205 a peak electric field strength exceeding 2.5 volts per angstrom) in turn indicates the viability of p

206 recipitation of energetic (>300 kiloelectron volts per atomic mass unit) sulfur and oxygen ions out o

207 Several hundred million volts per centimetre of electric-field strength are requ

208 rally directed electric field of order 10(9) volts per meter, seen in proximity to the capsule surfac

209 mic characteristics down to approximately 20 volts per meter.

210 acceleration gradient of 30.5 mega-electron volts per meter.

211 ter was observed at applied fields of 3 to 5 volts per micrometer.

212 ure of 290 kelvin by electric fields of 29.0 volts per micrometre.

213 large electric field in the order of several volts per nanometre is required to effectively tune its

214 peaks from 10 x 10(6) to 40 x 10(6) electron volts per nucleon and an increasing galactic cosmic-ray

215 loelectron volts (keV) to >/=50 megaelectron volts per nucleon and of electrons from >26 keV to >/=35

216 t energetic (> approximately 10 kiloelectron volts per nucleon) ion at closest approach.

217 gy helium ions (approximately62 megaelectron volts per nucleon) that peaked at approximately1.5RJ ins

218 ei, with energies ~195 to ~500 mega-electron volts per nucleon, of which we identify 15 (60)Fe nuclei

219 ctic cosmic rays down to ~3 x 10(6) electron volts per nucleon, revealing H and He energy spectra wit

220 voltabsorptometry, up to a scan rate of few volts per second with a satisfactory single-scan signal-

221 techniques capable of exceeding gigaelectron-volt-per-metre (GeV m(-1)) gradients in order to enable

222 of Sn-Pb mixed, low-band gap (~1.25 electron volt) perovskite films.

223 rgetic neutral atoms (ENAs) >6 kilo-electron volts produced by energetic protons occupying the region

224 on comprises accelerated ions (<800 electron volts), produced upstream of Rosetta, and lower energy l

225 teepening above approximately 10(9) electron volts provides a probe with which to study how particle

226 The signal intensity of zero volt PS is also lower than in the other methods.

227 While the range of analytes to which zero volt PS is applicable is very similar to kV PS and nESI,

228 eposition overpotential being in excess of 1 volt, Pt deposition was quenched at potentials just nega

229 excitation photon energy over a ~1-electron volt range, and dependent on the excitation polarization

230 tion, low cell discharge voltage (about 0.55 volts; ref.

231 te absorber, with a bandgap of 1.68 electron volts, remained phase-stable under illumination through

232 nanometers, femtoseconds, and millielectron volts, respectively.

233 lts in the energy range of up to 50 electron volts reveal the compression and expansion of layers on

234 lses to positive potentials and back to zero volts revealed that electrons are injected from the Ti t

235 ly alter the line shape on the millielectron volt scale that is now observable through improved resol

236 ty for a completely integrated mega-electron volt-scale DLA.

237 lities of 0.05 to 0.1 square centimeters per volt second and ON-OFF current ratios of >10(6).

238 gh mobilities of 0.02 square centimeters per volt second and on-off current switching ratios of 10(5)

239 ect mobilities up to 1 square centimeter per volt second.

240 ect mobilities of 0.6 square centimeters per volt-second and current modulation greater than 10(4).

241 hibit mobilities >100 square centimeters per volt-second and on-off ratios of 100,000.

242 approximately 10,000 square centimeters per volt-second can be induced by applying gate voltage.

243 e mobility (9000 to 10,000 centimeter(2) per volt-second) that is substantially higher than in the bu

244 ies (greater than 10(6) square centimers per volt-second).

245 lities of 0.9 and 0.2 square centimeters per volt-second, respectively; with current modulations of a

246 h mobilities exceeding 2.5 square meters per volt-second.

247 on mobilities of 21.7 square centimeters per volt-second.

248 ilities exceeding 300 square centimeters per volt-second.

249 LC-MS, Raman spectroscopy, and mega-electron volt-secondary ionization mass spectrometry.

250 olt energy barrier with a 140-milli-electron volt shift in their excitonic energy gaps.

251 An integrated design for a compact, sub-volt, sub-fJ/bit, hyperuniform-clad, electrically contro

252 lar modulation of high-energy (tera-electron volts, TeV) cosmic rays and diffusive propagation from s

253 e solar cell with a bandgap of ~1.7 electron volts that retained more than 80% of its initial PCE of

254 ges (less than approximately 5 millielectron volts), the transfer rate between sites was independent

255 the desorption yield peaks at 0.26 electron volt: the energy of the Si-H vibrational stretch mode.

256 ith a temperature of 0.2 to 0.5 kiloelectron volts, there is a warm layer with a temperature of 1.0 t

257 icles were observed up to 200 kilo--electron volts; these particles are capable of penetrating down t

258 distribution width of less than 0.5 electron volts, this source of monochromatic electrons may find a

259 (ENAs) at energies between tens of electron volts to hundreds of kiloelectron volts (keV).

260 EFT) reduces the required voltage to several volts to induce sufficient electric field strength for e

261 s arising from the application of only a few volts to its nanoscale building blocks-the plasmonic met

262 width of the emission from 120 millielectron volts to less than 1 millielectron volt because of gain

263 range of currents and voltages, from several volts to tens of volts.

264 ission at energies ranging from gigaelectron volts to teraelectron volts.

265 ng jitter information into the mega-electron-volt ultrafast electron diffraction pattern.

266 A full lithium-ion battery of 2.3 volts using such an aqueous electrolyte was demonstrated

267 0.5 NaOH/0.5 KOH, ammonia is produced at 1.2 volts (V) under 2 milliamperes per centimeter squared (m

268 ectron-hole separation yield of 0.90 at 1.23 volts (V) versus the reversible hydrogen electrode (RHE)

269 Potentials as low as 1.8 volts (V) versus the saturated calomel electrode were ap

270 hium ions at an average voltage of about 0.6 volts versus a Li/Li(+) reference electrode.

271 0 milliamperes per square centimetre (at 1.5 volts versus a reversible hydrogen electrode) and a cath

272 m excited-state oxidation potential of -3.36 volts versus a saturated calomel electrode, which is sim

273 he electrode) at an average potential of 4.2 volts versus Li/Li(+).

274 C activity with a low onset potential (~1.07 volts versus reversible hydrogen electrode), high photoc

275 mperes per square centimeter for ORR (at 0.9 volts versus reversible hydrogen electrode), yielding a

276 4.3 ampere per milligram of platinum at 0.9 volts versus the reversible hydrogen electrode (RHE), re

277 37 amperes per milligram of palladium at 0.9 volts versus the reversible hydrogen electrode in alkali

278 e of 1.2 M of water, at a potential of -1.13 volt (versus the ferrocenium/ferrocene couple).

279 ter-scale topography, voltages of 0.0 to 0.3 volts (versus a counter electrode in a two-electrode cel

280 Low-kiloelectron-volt VM imaging may be useful for salvaging CT studies w

281 r neutron emission near 2.5 million electron volts was also observed, as would be expected for deuter

282 citation (at a photon energy of 1.5 electron volts) was used to introduce a spatially periodic densit

283 he carbon-atom framework, above 3.5 electron volts we found atomlike orbitals bound to the core of th

284 ll applied voltages (up to approximately 0.3 volt), weak interaction between transporting electrons a

285 ith electrons with an energy of 300 electron volts were analyzed by scanning tunneling microscopy.

286 on changes on application of a fraction of a volt when the structure is placed in a fraction-of-tesla

287 gies reach hundreds of thousands of electron volts, whereas the typical electron energies associated

288 gamma(33) (approximately 220 picometres per volt), which is far beyond the performance of the common

289 tending to high energies (>10 kilo--electron volts), which is ascribed to an accretion disk corona of

290 arrow electrochemical stability window (1.23 volts), which sets an intrinsic limit on the practical v

291 ined at operating voltage ranges as low as 5 volts, which are much smaller than previously reported r

292 itting with an accuracy of 300 kilo-electron volts, which is greater than 0 by 5 standard deviations.

293 ition state is 1.099 ± 0.010 electron volts, which is lower by 12.1 ± 0.3 kilocalories

294 We report efficient 1.67-electron volt wide-band gap perovskite top cells using triple-hal

295 [Formula: see text] of ~1098 picometers per volt with a high Curie temperature of ~450 degrees C.

296 er micrometer at a low supply voltage of 0.5 volts with a subthreshold swing of 85 millivolts per dec

297 2 can be driven by a gate voltage of several volts with appropriate choice of dielectric.

298 milliamperes per square centimetre at -0.94 volts with respect to the reversible hydrogen electrode

299 lectrolyte whose window was expanded to ~3.0 volts with the formation of an electrode-electrolyte int

300 ional spin resonance (here ~10 nano-electron volts) with scanning tunneling microscopy to measure ele