ライフサイエンスコーパス: kA

1 ineering critical current density beyond 2.0 kA/mm(2) at 4.2 K and 16 T, by growing thick REBa2Cu3Ox

2 (C)) value for Hf(2)MnIr(5)B(2) (H(C) = 62.1 kA/m) reported to date for Ti(3)Co(5)B(2)-type compounds

3 sity of 2.5 kA cm(-2) and an EQE of ~1% at 1 kA cm(-2) are shown using electrical pulses, which repre

4 Footprint current densities exceeding 1 kA cm(-2) at less than +/-0.7 V, transconductances of 0.

5 temperature with high current densities (>10 kA cm(-2)) and tunability in the near-infrared (1,060 nm

6 oride and Rare-Earth-Barium-Copper-Oxide 100 kA class superconducting system.

7 ciency can be up to 70% and currents of 100s kA are achievable.

8 t amplitudes of 1,410 (113 kA/m), 1,300 (104 kA/m), and 700 (56 kA/m) oersteds (Oe) at 30%, 60%, and

9 espectively, for x = 0, to 552 kA/m and 7.11 kA/m respectively for x = 0.2.

10 oprobe injection at amplitudes of 1,410 (113 kA/m), 1,300 (104 kA/m), and 700 (56 kA/m) oersteds (Oe)

11 ably higher NLDN-reported peak currents: 113 kA vs. 33 kA (GM values).

12 d to transfer a total current of up to |117| kA with magnesium diboride and Rare-Earth-Barium-Copper-

13 tudy the effects of ELF MF (30-160 Hz, 8-120 kA/m) on the activity and release of a model enzyme, sup

14 t of field strength (between 30 kA/m and 120 kA/m at f = 50 Hz) are reported and explained.

15 has plasma current [Formula: see text] ~ 130 kA, duration ~ 150 ms, chord-averaged electron density ~

16 eading to a 14% increase in coercivity (1438 kA m(-1)) and matched remanence (1.16 T) giving a BHmax

17 to produces a train of high peak current (17 kA) electron bunches with a modulation wavelength of 10'

18 mately 1500 cm(-1) at a current density of 2 kA cm(-2).

19 25-mum Al wires on a compact L-C (40 kV, 200 kA and 200 ns) generator, and the time integrated spectr

20 dB for a magnetic field of ~2.80 kOe ( = 223 kA m(-1)) applied perpendicular to the film.

21 urrent in the plasma undulator can reach 0.3 kA level, making such an undulator a potential candidate

22 uration effect of field strength (between 30 kA/m and 120 kA/m at f = 50 Hz) are reported and explain

23 reported peak currents for isolated CIDs (33 kA) were similar to those initiating normal lightning ev

24 r NLDN-reported peak currents: 113 kA vs. 33 kA (GM values).

25 those initiating normal lightning events (34 kA).

26 end attached to the ground and produced a 36-kA return stroke.

27 me of 0.7 cm(3) are capable of producing 2.4 kA current, not achievable in electrochemical capacitors

28 civity (H C ) increase from 426 kA/m and 4.4 kA/m respectively, for x = 0, to 552 kA/m and 7.11 kA/m

29 erties are: intrinsic coercivity Hci = 688.4 kA/m, remanence Br = 0.51 T, and energy product (BH)max

30 s needed at the typical current density of 4 kA m(-2) , leading to a low energy consumption of 483 kW

31 S ) and coercivity (H C ) increase from 426 kA/m and 4.4 kA/m respectively, for x = 0, to 552 kA/m a

32 cies (150-375 kHz) and magnetic fields (4-44 kA/m).

33 management, a maximum current density of 2.5 kA cm(-2) and an EQE of ~1% at 1 kA cm(-2) are shown usi

34 e and infrared ranges (5 to 25 and 1.5 to 5% kA(-1)), and the broad absorption feature in the 2.9-to-

35 and 4.4 kA/m respectively, for x = 0, to 552 kA/m and 7.11 kA/m respectively for x = 0.2.

36 10 (113 kA/m), 1,300 (104 kA/m), and 700 (56 kA/m) oersteds (Oe) at 30%, 60%, and 90% "on" time (duty

37 a TGF and a cloud-to-ground discharge of -56 kA occurred when a downward negative leader was collidin

38 These coils carried up to 8.6 kA while generating 3.5 T at 4.2 K at a J(E) of 1020 A/m

39 triggered gas switches, could generate ~ 600-kA and ~ 700-kV across a ~ 0.9-Omega matched load when f

40 me (duty), respectively, and at 1,050 Oe (84 kA/m) at 50% and 70% duty over the 20-min treatment.

41 = 45) and highest peak current density (~90 kA/cm(2)) ever reported in a solid-state tunneling devic

42 T shell structure was estimated to be - 1.92 kA/Vm (- 24 Oe/V).

43 An electron coupling matrix element of H(kA) = (4.7 +/- 1.1) x 10(-4) eV ( approximately 46 J/mol

44 vingly depressed selectivity (1 < kappaobs < kA/kB), caused by inefficient microscopic mixing of a re

45 d, 2 mm.mrad normalized emittance, and multi-kA peak current.

46 OER at current densities as high as several kA.m(-2).