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1 l differences of 600 volts and currents of 1 ampere.
2 -peak performance on modern GPU generations (Ampere, Ada, Hopper) with throughput rates of up to 1.94
3 ), current efficiency (about 5.3 candela per ampere) and stretchability (about 100 per cent strain).
4 rnational System of Units (SI): the ohm, the ampere, and the kilogram (Kibble Balance).
5 ing Io, driving currents of around 1 million amperes down through Jupiter's ionosphere.
6 nt-carrying bar to provide a locally induced Ampere field.
7 lopment as a realization of the SI base unit ampere, following a redefinition of the ampere in terms
8 n which electromagnetic Coulomb, Lorentz and Ampere forces, as well as thermal stimulation and optica
9 urrent densities of [Formula: see text] peta-ampere/[Formula: see text] are produced with a few tens
10         The cumulative capacity reached ~581 ampere hour per gram, surpassing the benchmarks of lithi
11 h cells with lean electrolyte (2.5 grams per ampere hour) achieve stable cycling with an average Coul
12                     Extreme fast charging of Ampere-hour (Ah)-scale electrochemical energy storage de
13 ly by RFBs with increased volumetric (Q ~ 11 ampere-hours per liter) and areal (108 milliampere-hours
14 atholyte capacity utilization up to over 120 ampere-hours per litre at 80 per cent SoC with homogeneo
15 o 90 per cent SoC at 2 moles per litre (47.7 ampere-hours per litre) for bromide, revealing previousl
16 unit ampere, following a redefinition of the ampere in terms of a fixed value of the elementary charg
17 etween the quantized Hall states, using nano-ampere level currents with opposite polarities.
18 his anode catalyst further attains a hundred-ampere level water electrolysis, with kilowatt scale whi
19 duces recent advances in the CO(2)RR/CORR at ampere-level current densities, especially the catalytic
20 ty and energy efficiency (EE), especially at ampere-level current densities.
21 +) products with high faradaic efficiency at ampere-level current densities.
22 er a wide potential range above 1.0 V and at ampere-level current densities.
23  190% with pure hydrogen generation under an ampere-level current density and a low cell voltage of 2
24 ivers a 100 +/- 1% Faradaic efficiency at an ampere-level current density of 1035 mA cm(-2) at -0.2 V
25 hange membrane water electrolyzer (AEMWE) at ampere-level current density.
26 aining stability for at least 120 h under an Ampere-level of 800 mA cm(-2).
27 ing the CO(2)RR/CORR at current densities at ampere levels (>500 mA cm(-2)).
28 ts, as well as the longitudinal component of Ampere-Maxwell in Fourier space, assuming the continuity
29 nt magnetic moments as large as 1.3 x 10(17) ampere-meter2 in the Terra Sirenum region contribute to
30 liampere (mA) per centimeter squared and 4.3 ampere per milligram of platinum at 0.9 volts versus the
31 trial current densities: >=2000 hours at 1.0 ampere per square centimeter and 1000 hours at 1.5 amper
32 and a dark current J(d) of just 2.3 x 10(-6) ampere per square centimeter at -2 volts. We demonstrate
33 ter at 2 volts, and stable operation up to 1 ampere per square centimeter in a PEMWE system at indust
34 ate a switching current density of ~0.1 mega-ampere per square centimeter in flexible superlattice PC
35 ement in activity; and stable operation at 1 ampere per square centimeter over the course of 600 hour
36 electrolysis mode, a current density of >0.6 ampere per square centimeter with a Faradaic efficiency
37                    At current densities of 1 ampere per square centimeter, it had an overpotential 33
38 plied current with magnitudes of order 10(6) ampere per square centimeter.
39 aic devices with photoresponsivity above 0.1 ampere per watt (corresponding to an external quantum ef
40 e hours per gram at an ultrahigh rate of 200 amperes per gram and a 90% capacity retention over 15,00
41 er 15,000 cycles at a current density of 5.0 amperes per gram.
42 ric coefficient, reaching a value of about 5 amperes per kelvin per metre with a logarithmic temperat
43  to 0.001 and magnetizations from 1800 to 15 amperes per meter.
44  in a mass activity towards the ORR of 16.37 amperes per milligram of palladium at 0.9 volts versus t
45 electrode), yielding a mass activity of 13.6 amperes per milligram of Pt, nearly double previously re
46 radation rate <0.5 millivolt per hour at 2.0 amperes per square centimeter and 70 degrees C-a >20-fol
47 wer overpotentials, a current density of 1.8 amperes per square centimeter at 2 volts, and stable ope
48 h an ethylene partial current density of 1.3 amperes per square centimeter at 45% cathodic energy eff
49 ducting critical currents of more than 10(6) amperes per square centimeter at low temperature in micr
50 ng catalyst reaches a current density of 3.0 amperes per square centimeter at only 1.77 volts and a l
51 current densities of about 10(-9) to 10(-10) amperes per square centimeter at zero bias.
52 tage of 1.72 volts at a current density of 3 amperes per square centimeter with an Ir loading of just
53 , the PEET achieves a current density of 2.5 amperes per square centimeter, an average power output o
54 ely high stable current densities, J > 10(7) amperes per square centimeter, have been attained.
55 d with current density approaching 3 x 10(4) amperes per square centimeter.
56  per square centimeter and 1000 hours at 1.5 amperes per square centimeter.
57 reakdown current density of more than 10(11) amperes per square meter for the wire bonds.
58 netic dipole moment of 12.5 +/- 1.4 x 10(22) amperes per square meter, three times greater than mean
59 e very high winding current density of 1,260 amperes per square millimetre.
60                   This technique is based on Ampere's law and exploits the linear relationship betwee
61 ing a set of partial differential equations (Ampere's law and Gauss' law for magnetism) numerically w
62 simple bilayer structure to 42.9 candela per ampere, similar to the CE of phosphorescent organic ligh
63 specific magnetic moment being <3.1 x 10(-5) ampere-square meters per kilogram for meter-size homogen
64  maximum dipole moment of 67P is 1.6 x 10(8) ampere-square meters.
65 tionize electrical metrology by enabling the ampere to be redefined in terms of the elementary charge
66 ic fields of some 10 kV.cm(-1) amplitude and ampere-transient currents.
67             The effects of PFA (biphasic, 24 amperes) were investigated in 25 swine using a lattice-t
68 amplification efficiency is 38.2 siemens per ampere, which is near the theoretical thermionic limit,