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1 l differences of 600 volts and currents of 1 ampere.
2 ing Io, driving currents of around 1 million amperes down through Jupiter's ionosphere.
3 nt-carrying bar to provide a locally induced Ampere field.
4 lopment as a realization of the SI base unit ampere, following a redefinition of the ampere in terms
5 n which electromagnetic Coulomb, Lorentz and Ampere forces, as well as thermal stimulation and optica
6 unit ampere, following a redefinition of the ampere in terms of a fixed value of the elementary charg
7 nt magnetic moments as large as 1.3 x 10(17) ampere-meter2 in the Terra Sirenum region contribute to
8 liampere (mA) per centimeter squared and 4.3 ampere per milligram of platinum at 0.9 volts versus the
9 plied current with magnitudes of order 10(6) ampere per square centimeter.
10 aic devices with photoresponsivity above 0.1 ampere per watt (corresponding to an external quantum ef
11  to 0.001 and magnetizations from 1800 to 15 amperes per meter.
12 electrode), yielding a mass activity of 13.6 amperes per milligram of Pt, nearly double previously re
13 current densities of about 10(-9) to 10(-10) amperes per square centimeter at zero bias.
14 ely high stable current densities, J > 10(7) amperes per square centimeter, have been attained.
15 d with current density approaching 3 x 10(4) amperes per square centimeter.
16 reakdown current density of more than 10(11) amperes per square meter for the wire bonds.
17 netic dipole moment of 12.5 +/- 1.4 x 10(22) amperes per square meter, three times greater than mean
18                   This technique is based on Ampere's law and exploits the linear relationship betwee
19 simple bilayer structure to 42.9 candela per ampere, similar to the CE of phosphorescent organic ligh
20 specific magnetic moment being <3.1 x 10(-5) ampere-square meters per kilogram for meter-size homogen
21  maximum dipole moment of 67P is 1.6 x 10(8) ampere-square meters.
22 tionize electrical metrology by enabling the ampere to be redefined in terms of the elementary charge

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