ライフサイエンスコーパス: mA

1 y revealed generally good reliability of 1.0 mA anodal tDCS (ICC(2,1) = 0.74 over the first 30 min).

2 ) sensitivity correlated negatively with 1.0 mA anodal tDCS effects on excitability.

3 e variance in the early after-effects of 1.0 mA anodal tDCS, which may be of practical relevance for

4 cal cells up to 150 and 200 h at 2.0 and 1.0 mA cm(-2), respectively.

5 ve to sham while for cathodal tDCS, only 1.0 mA resulted in sustained excitability diminution.

6 sity; effects of lower intensities (0.5, 1.0 mA) showed equal, if not greater effects in motor-cortic

7 ential by 150 mV at a current density of 1.0 mA/cm(2) after coating its surface electrophoretically w

8 photocurrent densities on the order of -1.0 mA/cm(2) at 0.0 V vs RHE and evolve hydrogen with a fara

9 A short circuit current density of 12.0 mA/cm(2) is achieved in 210 nm thick patterned Si films,

10 62% on glass substrates while a Jsc of 13.0 mA/cm(2) and FF of 62% was achieved on plastic substrate

11 ytic activity with a current density of 15.0 mA cm(-2) and a turnover frequency of 4.1 s(-1) at the o

12 nge of current intensity between 0.5 and 2.0 mA on left primary motor cortex (M1) plasticity, as well

13 tigated the full DC intensity range (0.5-2.0 mA) for both anodal and cathodal tDCS in a sham-controll

14 DC intensities (sham, 0.5, 1.0, 1.5 and 2.0 mA) were investigated in separate sessions.

15 cuit current density (Jsc, from 32.5 to 37.0 mA/cm(2)).

16 arge and discharge current density of 12 000 mA g(-1) over approximately 4000 cycles.

17 one minute with a current density of ~4,000 mA g(-1) (equivalent to ~3,000 W kg(-1)), and to withsta

18 0 nm) gave photocurrents up to 0.23 +/- 0.02 mA cm(-2) at 1.23 VRHE under standard simulated solar il

19 the plasma-engraved Co3 O4 nanosheets (0.055 mA cm(-2) BET at 1.6 V) is 10 times higher than that of

20 ort-circuit current density (J sc ) of 17.07 mA cm(-2) .

21 de exhibits excellent rate capability (129.1 mA h/g at 2 C; 110.9 mA h/g at 10 C) and cycling stabili

22 sed on ferroelectric materials, reached 20.1 mA cm(-2) under one sun illumination in OTP devices with

23 h short-circuit current densities up to 42.1 mA cm(-2).

24 aching values up to 12.95 mW cm(-2) and 53.1 mA cm(-2) for maximum power and current density at 323 K

25 Current densities of approximately 1 mA/cm(2) over 30-h electrolysis are achieved at a 2.5-V

26 eved a desalination/salination cycle at +/-1 mA cm(-2) with a net potential input of only 0.20 V.

27 ost from 1.5 mA tDCS on Visual WM and from 1 mA tDCS on Spatial WM.

28 apacity 80- to 100-fold and enables rates >1 mA cmareal(-2) for cathodes with capacities of >4 mAh cm

29 provide phosphorene TFET outstanding ION ~ 1 mA/um, ON/OFF ratio ~ 10(6) for a 15 nm channel and 0.5

30 , were measured before and after 20 min of 1 mA anodal or sham tDCS.

31 tion of MtrC and a high current density of 1 mA cm(-2) at 0.4 V vs SHE could be obtained at pH 6.5 (E

32 electrodes exhibited current densities of 1 mA cm(-2) at 1.07 V vs NHE.

33 table (tens of hours) current densities of 1 mA cm(-2) at overpotentials as low as 540 mV at pH 9.2 a

34 a (0.68 V) for OER at a current density of 1 mA/cm(2).

35 ion from water to proceed at rates of over 1 mA cm(-2) on WO3 photoanodes without the need for any ad

36 Anodal stimulation (1 mA, 20 min) was applied over the DLPFC.

37 same activity for H2 evolution from water (1 mA/cm(2)).

38 was greater with 0.25 mA compared with 0.10 mA stimulations, suggesting a dose-dependent relationshi

39 Moreover, we achieve 10 mA cm(-2) at a low voltage of 1.44 V for 48 h in basic m

40 We achieve 10 mA cm(-2) water-splitting current at only 1.51 V for ove

41 thout any external bias and approximately 10 mA/cm(2) with a modest bias under one sun illumination.

42 ultralow overpotential of only 232 mV at 10 mA cm(-2) and possesses outstanding kinetics (the Tafel

43 al of 1.43 V and a potential of 1.61 V at 10 mA cm(-2) current density.

44 , a lithium|lithium cell can be cycled at 10 mA cm(-2) for more than 6,000 cycles, and a copper|lithi

45 The intrinsic catalytic activity at 10 mA cm(-2) for oxygen evolution reaction (OER) is current

46 Meanwhile, an overpotential of 540 mV at 10 mA cm(-2) is attained in an acidic electrolyte and stabl

47 term cycling performance of over 480 h at 10 mA cm(-2) with high efficiency.

48 lution and 235 mV for oxygen evolution at 10 mA cm(-2) with long-term stability, which have superior

49 g HER catalysts, several could operate at 10 mA cm(-2) with overpotentials <0.1 V in acidic and/or al

50 oximately 0.1 V in overpotential shift at 10 mA cm(-2)) is observed for the LCO nanoparticles, where

51 em that achieves a 1.99 V cell voltage at 10 mA cm(-2), reducing CO2 into CO and oxidizing H2O to O2

52 extremely low overpotential of -68 mV at 10 mA cm(-2), small Tafel slopes of approximately 34 mV dec

53 n extremely low overpotential of 64 mV at 10 mA cm(-2), which is, to our knowledge, the best among th

54 achieved at the geometric current density 10 mA cm(-2) in an alkaline electrolyte, with the Tafel slo

55 able operation with C2-C3 current density 10 mA/cm(2) (at -0.75 V), rendering it attractive for solar

56 electrocatalytic current density of j = -10 mA cm(-2) , and a Tafel slope of 52 mV dec(-1) .

57 of 400 mV for OER at an anodic current of 10 mA cm(-2) .

58 evolution, achieving current densities of 10 mA cm(-2) and 100 mA cm(-2) at overpotentials of 48 mV a

59 tential of 280 mV at a current density of 10 mA cm(-2) and high durability in an alkaline medium.

60 ut 1.53 V to achieve a current density of 10 mA cm(-2) and maintains its activity for at least 24 h i

61 ution reaction, with a current density of 10 mA cm(-2) at a low potential of -175 mV and a Tafel slop

62 alkaline media, with a current density of 10 mA cm(-2) at overpotentials of -94 mV for HER and 345 mV

63 to achieve a magnitude current density of 10 mA cm(-2) per geometric area, the approximate current de

64 200 mV at a benchmark current density of 10 mA cm(-2).

65 of -eta < 100 mV at a current density of -10 mA cm(-2) in 0.500 M H2SO4(aq).

66 otential of 96 mV at a current density of 10 mA.cm(-2) and a Tafel slope of 78 mV per decade under al

67 the surface, yields current densities of 10 mA/cm(2) at an overpotential of 177 mV, 500 mA/cm(2) at

68 ble cycling, and high-power output (up to 10 mA/cm(2)) even in carbonate electrolytes.

69 The overall-water-splitting with 10 mA cm(-2) at a low voltage of 1.64 V is achieved using t

70 ative to pure water splitting to achieve 100 mA cm(-2), while the oxidation product (FDCA) at the ano

71 ng current densities of 10 mA cm(-2) and 100 mA cm(-2) at overpotentials of 48 mV and 109 mV, respect

72 trodes gives current densities of 10 and 100 mA cm(-2) at potentials of 1.54 and 1.72 V, respectively

73 and 270 mV are required to reach 10 and 100 mA cm(-2), respectively.

74 at considerably high current densities (100 mA cm(-2)).

75 find photoresponsivities that can exceed 100 mA W(-1).

76 mperature, by applying a bias current of 100 mA.

77 as 480 mAh.g(-1) at a current density of 100 mA.g(-1), and retained 84% capacity after 300 cycles.

78 -1) when the current density returned to 100 mA.g(-1) after continuous cycling at 2400 mA.g(-1) (192

79 excellent cycling performance from 40 to 100 mA/cm(2).

80 uracy with IC-IR was noninferior at 50% (100 mAs [effective]) and 25% (300 mAs [effective]) exposure

81 nds by 13 scans, one every 2 seconds, at 100 mAs, and then five scans, one every 5 seconds, at 75 mAs

82 charge/discharge rate is increased to 10000 mA g(-1) during cycling between 2.25 and 5.0 V.

83 total reference milliampere seconds (ie, 110 mAs) split up in a way that 40% was applied to tube A an

84 (-1), exhibit charge capacities of about 120 mA h g(-1).

85 ctrode delivers a reversible capacity of 125 mA h g(-1), which may include a minor contribution of hy

86 red with the commercial Pt/C catalyst (0.127 mA/cm(2) and 0.096 A/mg(Pt)).

87 nstant Km and Imax equal to 0.24 mM and 0.13 mA cm(-1), respectively.

88 drates show a specific capacity of about 130 mA h g(-1) at 35 C (fully charged within 100 s) and su

89 t the short-circuit current still reaches 14 mA cm(-2).

90 ity of 250 mA h g(-1) at 50 mA g(-1) and 140 mA h g(-1) at 10 A g(-1).

91 ter 300 cycles at 30 mA g(-1) and 84% at 150 mA g(-1) over 1300 cycles.

92 (based on the mass of anode) at 15 and 1500 mA g(-1), respectively.

93 hotocurrent yet generated from TTA-UC (0.158 mA cm(-2)) under 1 sun.

94 5 days and maintain a high capacity of 1600 mA h g(-1) in humid air ( approximately 10% relative hum

95 3)) as well as a gravimetric capacity of 161 mA h g(-1) and volumetric capacity of 281 mA h cm(-3) at

96 opic (0.6 mm) diagnostic CT scan (80 kV, 165 mAs) and a subsequent PET scan (2 min per bed position).

97 the high theoretical specific capacity (1675 mA h g(-1) ) and low cost, lithium-sulfur (Li-S) batteri

98 d the first time to combine high Jsc over 17 mA cm(-2) and high FF over 77% into one SM-OPV.

99 than conventional pulse amplitudes (112-174 mA for ECT and 37.4% of maximum device amplitude for MST

100 ith the extraordinarily high Jsc values (>18 mA/cm(2)), comparable with those of the corresponding PC

101 ty of 65 and 116 mAh g(-1) at a rate of 1800 mA g(-1) when charged to 5.0 and 5.25 V vs. Li/Li(+) , r

102 cathodic photocurrents of up to 5.96+/-0.19 mA cm(-2), which are close to the highest record in conv

103 The Pt/TiO2/n-Si electrode produced 19 mA cm(-2) of photocurrent density under 100 mW cm(-2) ir

104 0.3 mA, CCh 2.4 +/- 0.4 mA, wash 1.1 +/- 0.2 mA) and flattened the restitution curve (n = 6) derived

105 m temperature, with a current density of 0.2 mA/cm(2) for around 500 h and a current density of 0.5 m

106 h a large dynamic current range (5 nA to 1.2 mA) and short conversion time (10 ms) were fabricated in

107 otocathodes reach current densities of -11.2 mA cm(-2) at the reversible hydrogen potential in 0.1 M

108 short-circuit current density (Isc) of 12.2 mA/cm(2) were obtained.

109 insic photo-responsivity of 518, 30, and 2.2 mA W(-1) at 3.4, 5, and 7.7 mum, respectively, at 77 K.

110 mV, a short-circuit current density of 33.2 mA/cm(2), and a fill factor of 71.3% by virtue of the en

111 ctures can deliver a current density of 37.2 mA cm(-2) at an overpotential of 70 mV, which is 9.7 tim

112 M training paired with tDCS (sham, 1, 1.5, 2 mA).

113 s could be cycled stably for 180 cycles at 2 mA cm(-2).

114 When stimulating at 2 mA, cortical electric fields reach 0.8 V/m, the lower li

115 (CE) of 90% and high current density (ca. 2 mA/cm(2) for the stripping peak).

116 For met/met homozygotes, 2 mA resulted in significantly poorer performance compared

117 reviously showed that brief application of 2 mA (peak-to-peak) transcranial currents alternating at 1

118 9% over 400 cycles at a current density of 2 mA cm(-2)).

119 ed high photocurrent densities, surpassing 2 mA cm(-2) with an incident photon-to-current efficiency

120 First, we observed that 2 mA currents generated substantial intracranial fields, w

121 atory functional signatures (p < 0.001) to 2 mA electrical forepaw stimulation, found to be innocuous

122 347.2 +/- 0.4) mA cm(-2) and (189.0 +/- 0.2) mA cm(-2), respectively.

123 , and exchange current density of 3.9x10(-2) mA cm(-2) .

124 The tDCS was administered in 30-minute, 2-mA prefrontal stimulation sessions for 15 consecutive we

125 cts (OCBPs) during galvanostatic (10, 15, 20 mA . cm(-2)) electro-oxidation of urine on boron-doped d

126 region with excellent photocurrents above 20 mA cm(-2) was achieved for all polymers, making these hi

127 li, achieving current densities of 10 and 20 mA cm(-2) at overpotentials of 150 and 180 mV, respectiv

128 le short-circuit current of approximately 20 mA cm(-2) and a highest power conversion efficiency of 9

129 e within 20 min at 200 mA ( approximately 20 mA/cm(2)), using Fe as the anode and cathode.

130 les an alkaline electrolyzer operating at 20 mA cm(-2) at a voltage lower than 1.5 V, lasting longer

131 discharge-charge voltage gap of 0.77 V at 20 mA cm(-2) under ambient conditions.

132 overpotential of approximately 0.12 V at 20 mA/cm(2), small Tafel slope of approximately 46 mV/decad

133 Successful CI was defined by exit block (20 mA at 2 ms) within the isolated region.

134 imately 230 mAh/g at a testing current of 20 mA/g) with nearly 100% Columbic efficiency in sodium sto

135 ckel-zinc batteries with good power rate (20 mA cm(-2), 20 C rate for our anodes).

136 aintaining current densities greater than 20 mA/cm(2).

137 g cancer screening (120-kVp tube voltage, 20-mAs reference tube current-time product for both detecto

138 of the parent molecule within 20 min at 200 mA ( approximately 20 mA/cm(2)), using Fe as the anode a

139 on, results in the high current density [200 mA/cm(2) at an overpotential of 0.3 V comparable to plat

140 hase shows high intercalation capacity (>200 mA.h.g(-1)) but only at moderate rates.

141 s demonstrate an ultrahigh activity with 200 mA cm(-2) current density at only 206 mV overpotential u

142 tion of a contrast agent, with a scan at 200 mAs, followed after 4 seconds by 13 scans, one every 2 s

143 , the nanowire solar cells yielded Jsc of 21 mA/cm(2) and efficiency of 8.67%.

144 with an unprecedented photocurrent up to 21 mA cm(-2).

145 s show a high prelithiation capacity of 2100 mA h g(-1) with negligible capacity decay in dry air aft

146 able and enhanced output performance of 1.22 mA and 46.8 mW cm(-2) under low frequency of 3 Hz is pro

147 ix to achieve high sensitivity (2.4 +/- 0.24 mA cm(-2) mM(-1)) for H2O2 oxidation.

148 00 mA.g(-1) after continuous cycling at 2400 mA.g(-1) (192 mAh.g(-1)).

149 s were stimulated in vivo for 30 min at 0.25 mA and then allowed to return to their home cage for 24

150 tude of the LTP effect was greater with 0.25 mA compared with 0.10 mA stimulations, suggesting a dose

151 have been subjected to tDCS of 0.10 or 0.25 mA for 30 min followed by 30 min of recovery time displa

152 PPF, continued 24 h after completion of 0.25 mA of tDCS.

153 l for water oxidation (1.23 V vs RHE) is >25 mA cm(-2).

154 -ion batteries, delivering a capacity of 250 mA h g(-1) at 50 mA g(-1) and 140 mA h g(-1) at 10 A g(-

155 even at high current densities of up to 250 mA/cm(2).

156 by the mutant were 0.135 mW cm(-2) and 0.255 mA cm(-2), ~25% higher than those obtained from the wide

157 the theoretical value (260 mA h g(-1); >257 mA h g(-1) for AQ), a very small voltage gap between the

158 y almost equal to the theoretical value (260 mA h g(-1); >257 mA h g(-1) for AQ), a very small voltag

159 2 full cell is 81% after 1,500 cycles at 268 mA gSeS2(-1).

160 ic sensitivity and limit of detection of 270 mA M(-1) cm(-2) and 10 muM at -0.25 V (V vs Hg/Hg2SO4).

161 outstandingly at very high charge rates (270 mA g(-1), 80 cycles) and, at a charge rate of 30 mA g(-1

162 a high theoretical capacity for lithium (279 mA h g(-1) or 1,005 C g(-1)).

163 mV, a short-circuit current density of 24.28 mA cm(-2), and a fill factor of 63.72%.

164 61 mA h g(-1) and volumetric capacity of 281 mA h cm(-3) at 0.05 C-rate.

165 ificant increase in VFT (control 1.5 +/- 0.3 mA, CCh 2.4 +/- 0.4 mA, wash 1.1 +/- 0.2 mA) and flatten

166 ate current density was kept at 11.0 +/- 1.3 mA/m(2) in a microbial electrochemical cell, and isotopi

167 erformance, with a specific activity of 10.3 mA/cm(2) and mass activity of 6.98 A/mg(Pt), which are 8

168 An areal capacity of as high as 11.3 mA h cm(-2) is achieved with a six-sulfur-layer cathode.

169 eaches a short-circuit current (jsc) of 13.3 mA cm(-2) and a power conversion efficiency (PCE) of 6.1

170 cy (80, 140 and 250 Hz), current (1, 2 and 3 mA) and duration (500 and 1000 ms) parameters.

171 low overpotential ( approximately 80 mV at 3 mA cm(-2)) and a flat voltage profile in a carbonate ele

172 tial (<90 mV) at a high current density of 3 mA/cm(2) over 80 cycles.

173 nd exchange current density of 9.62 x 10(-3) mA cm(-2), performing among the best of current molybden

174 tor operating conditions require short 20-30 mA pulses of electrical current.

175 and eta of the optimized solar cell of 29.30 mA cm(-2), 0.564 V, 65.59% and 10.83%, respectively.

176 city retention of 90% after 300 cycles at 30 mA g(-1) and 84% at 150 mA g(-1) over 1300 cycles.

177 (-1), 80 cycles) and, at a charge rate of 30 mA g(-1), exhibit charge capacities of about 120 mA h g(

178 or at 50% (100 mAs [effective]) and 25% (300 mAs [effective]) exposure reduction for the 30- and 40-c

179 ious decay at a high current density of 3000 mA g(-1) .

180 hock (MES) test and the psychomotor 6 Hz (32 mA) seizure models.

181 olution, providing a current density of 1.33 mA/cm(2) at an overpotential of 0.42 V.

182 ter 1100 cycles and 74.6 mA h g(-1) (at 3350 mA g(-1) ) after 4000 cycles are delivered outstandingly

183 etric capacities of, respectively, 43 and 35 mA h cm(-2) , 648 and 536 mA h g(-1) , and 1067 and 881

184 xhibits a maximum photocurrent density of 35 mA cm(-2) and an open circuit potential of 450 mV; there

185 y due to its highest specific capacity (3860 mA h g(-1)) and lowest potential, but low Coulombic effi

186 n reach 3.4 V, with specific capacity of 395 mA h g(-1) and stable capacity retention about 99.7% per

187 40.5 m(2) g(-1)), a high mass activity (398 mA mg(-1)) and specific activity (0.98 mA cm(-2)), and a

188 EA (0.1 - 0.4 mA, 2 Hz) was applied at ST36-37 acupoints overlying the

189 VFT (control 1.5 +/- 0.3 mA, CCh 2.4 +/- 0.4 mA, wash 1.1 +/- 0.2 mA) and flattened the restitution c

190 MPES system produced a stable current of 0.4 mA/cm(2) for 24 h without any external bias and approxim

191 High capacities of 144.4 mA h g(-1) (at 837.5 mA g(-1) ) after 1100 cycles and 74

192 battery demonstrates a high capacity of 5.4 mA h cm(-2) at a discharge current density of 2.75 mA cm

193 and a copper|lithium cell can be cycled at 4 mA cm(-2) for more than 1,000 cycles with an average Cou

194 e diodes were measured to be (347.2 +/- 0.4) mA cm(-2) and (189.0 +/- 0.2) mA cm(-2), respectively.

195 a very tiny shuttle current of 2.60 x 10(-4) mA cm(-2) , a rapid redox reaction of polysulfide, and t

196 er glucose oxidation current densities, 0.41 mA cm(-2), are obtained from enzyme electrodes containin

197 hort-circuit current density (J(sc)) of 9.42 mA/cm(2) from the n = 3 compound.

198 ated biosensor showed high sensitivity of 42 mA M(-1) cm(-2), a linear range of glucose detection of

199 exceptionally high reversible capacity (420 mA h g(-1)), excellent rate capability, and good cyclic

200 ds the highest Jph and etaseparation of 1.43 mA cm(-2) and 87.7% at 1.23 V versus reversible hydrogen

201 at corresponding current density of 1444.44 mA/m(2) and 1777.77 mA/m(2).

202 ne layers shows a specific capacity of 2,440 mA h g(-1) (calculated using the mass of phosphorus only

203 ted unpredictably either in punishment (0.45 mA foot-shock) or the opportunity to make a taking respo

204 or around 500 h and a current density of 0.5 mA/cm(2) for over 300 h.

205 1 years) both before and after 20 min of 1.5 mA anodal (n = 18) or sham (n = 14) tDCS applied to the

206 illumination, sustained photocurrents of 1.5 mA cm(-2) were measured under an applied bias.

207 type male mice 2 and 4 weeks after a 2 s 1.5 mA footshock.

208 ificantly poorer performance compared to 1.5 mA on Spatial WM.

209 val/val homozygotes benefited most from 1.5 mA tDCS on Visual WM and from 1 mA tDCS on Spatial WM.

210 sing tRNS intensities (ranging from 0 to 1.5 mA), the detection accuracy of a visual stimuli changed

211 y as high as ~225 F/cm(3) (measured at 103.5 mA cm(-3) in a three-electrode cell), as well as a long

212 PCE) of 10.1% with Voc = 0.833 V, Jsc = 16.5 mA/cm(2), and FF = 70.0% is achieved, among the highest

213 hotocurrent densities for CuBi2O4 up to -2.5 mA/cm(2) at 0.6 V vs RHE with H2O2 as an electron scaven

214 gical control at high current densities (3-5 mA cm(-2) ) for Li and even for notoriously unstable Na

215 pulse frequency (2-20 Hz), intensity (0-3.5 mA) and pulse widths (130-750 mus) over 14 months.

216 ells deliver a short-circuit current of 34.5 mA cm(-2) and power conversion efficiency of 15.7%.

217 e highest diffusion-limited ORR current (5.5 mA cm(-2) ) among a series of lambda-MnO2-z electrocatal

218 igh capacities of 144.4 mA h g(-1) (at 837.5 mA g(-1) ) after 1100 cycles and 74.6 mA h g(-1) (at 335

219 /Si photocathode with high photocurrents (>5 mA cm(-2) ).

220 With low current intensity (<5 mA and 100 micros pulse width) stimulation, our results

221 achieved even at a high current density of 5 mA cm(-2) in both carbonate and ether electrolyte.

222 urrent density in PEC water splitting over 5 mA cm(-2) before the dark current onset, which originate

223 er 300 cycles with current densities up to 5 mA/cm(2).

224 rical currents in the target peaked at 40-50 mA, greatly exceeding thresholds for nociceptor activati

225 acity of 3.72 mAh cm(-2) is achieved at 5.50 mA cm(-2) on the quinonoid imine-doped graphene based el

226 and VFA levels from 1 to 30 mM (0.04 to 8.50 mA/m(2), R(2) = 0.97) and then from 30 to 200 mM (8.50 t

227 elivering a capacity of 250 mA h g(-1) at 50 mA g(-1) and 140 mA h g(-1) at 10 A g(-1).

228 eversible capacity of 384.8 mA h g(-1) at 50 mA g(-1) and a good rate capability of 221.9 mA h g(-1),

229 to 567 mAh g(-1) at a current density of 50 mA g(-1) , which is the highest capacity value reported

230 of 466 mAh g(-1) at a current density of 50 mA g(-1) .

231 s display catalytic currents greater than 50 mA cm(-2) with 96 +/- 3% Faradaic efficiency for CO prod

232 with a coulombic efficiency over 99% at 500 mA . g(-1) after 500 cycles.

233 capability by retaining 75 mA h g(-1) at 500 mA g(-1) (or 3.7 C), and a stable cycle life.

234 08 F/g at 1 mV/s using CV and 185 F/g at 500 mA/g using charge-discharge measurements with excellent

235 mA/cm(2) at an overpotential of 177 mV, 500 mA/cm(2) at only 265 mV, and 1,705 mA/cm(2) at 300 mV, w

236 ion, which requires a current density of 500 mA/cm(2) at an overpotential below 300 mV with long-term

237 short-circuit current density (Jsc) of 18.53 mA/cm(2), open circuit voltage (Voc) of 0.538 V, and fil

238 ctively, 43 and 35 mA h cm(-2) , 648 and 536 mA h g(-1) , and 1067 and 881 mA h cm(-3) with a stable

239 current at 50 mV s(-1) is 825, 615, and 550 mA cm(-1), respectively, which is significant dominated

240 314 mAh g(-1) (4.7 mAh cm(-2)) at 0.1 C (0.6 mA cm(-2)) accompanied with good cycling stability.

241 ith the highest performance observed at 17.6 mA/cm(2) of photocurrent and 7.5% PCE for a cosensitized

242 837.5 mA g(-1) ) after 1100 cycles and 74.6 mA h g(-1) (at 3350 mA g(-1) ) after 4000 cycles are del

243 a high initial reversible capacity of 852.6 mA h g(-1) at 1 C between 0.02 and 3 V with a long-term

244 ischarges the upper positive layer by >/=9.6 mA, strong enough to be an important charging mechanism

245 We examined if 6 mA is present and regulated by early life stress associa

246 e stress and biological sex, and increased 6 mA is associated with gene repression.

247 Recent evidence described 6-methyladenine (6 mA) as a novel epigenetic regulator in a variety of mult

248 Our results provide evidence that 6 mA is present in the mammalian brain, is altered within

249 ith a discharge capacity of approximately 60 mA h g(-1) under a high charge and discharge current den

250 d long cycling performance, 700 cycles at 60 mA/cm(2) with 99.99% capacity retention per cycle, and d

251 vice reached current densities of up to 0.68 mA cm(-2) at 0.5 V vs RHE under AM 1.5 with an incident

252 operation ( approximately 600 mAh/g at 6.69 mA/cm(2)).

253 t of 4,942 W/kg (8,649 Wh/kg) at 2 A/ge (1.7 mA/cm(2)).

254 obtained a measured photoresponsivity of 2.7 mA W(-1) cm(-2) at -0.1 V.

255 lectrodes (Voc = 207 +/- 5.2 mV; Jsc = -21.7 mA/cm(2); ff = 0.22; etaH2 = 0.99%).

256 rains, five trains per second, 100 micros, 7 mA) and was compared with sham stimulation.

257 ear 2 volts, a specific capacity of about 70 mA h g(-1) and a Coulombic efficiency of approximately 9

258 7 mV, 500 mA/cm(2) at only 265 mV, and 1,705 mA/cm(2) at 300 mV, with high durability in alkaline ele

259 ith capacity 680 mAh g(-1) at 0.5C (1C = 718 mA g(-1)) is achieved after 1000 cycles.

260 s a high reversible specific capacity of 719 mA g(-1) and good cycling stability with 81% capacity re

261 m(-2) at a discharge current density of 2.75 mA cm(-2) (C/2 rate) while delivering good mechanical fl

262 d a very high short-circuit current of 20.75 mA cm(-2) .

263 rage, a good rate capability by retaining 75 mA h g(-1) at 500 mA g(-1) (or 3.7 C), and a stable cycl

264 then five scans, one every 5 seconds, at 75 mAs.

265 hodes deliver peak capacities of 926 and 765 mA h g(-1) , respectively, at C/10 and C/5 rates, which

266 rrent density of 1444.44 mA/m(2) and 1777.77 mA/m(2).

267 Na(+) /Na with a specific capacity of 127.8 mA h g(-1) .

268 pacity loadings in the range from 1.5 to 3.8 mA h cm(-2) are produced by using infiltration of active

269 Photocurrents up to 3.8 mA/cm(2) at 0 V vs RHE were achieved under simulated 1 S

270 ode delivered a reversible capacity of 384.8 mA h g(-1) at 50 mA g(-1) and a good rate capability of

271 with partial current densities of jCO = 5-8 mA/cm(2) at applied overpotentials of eta < 250 mV.

272 A photocurrent of over 6.8 mA cm(-2) and an accordingly high incident photon-to-cur

273 V and a short-circuit current density of 7.8 mA/cm(2) under 100 mW/cm(2) irradiation.

274 A record photocurrent density of -9.8 mA cm(-2) at 0 V versus RHE with an onset potential as p

275 7) and then from 30 to 200 mM (8.50 to 10.80 mA/m(2), R(2) = 0.95).

276 on support reach high mass activities (50-80 mA HCO2(-) synthesis per mg Pd) when driven by less than

277 h as high field emission current density (80 mA/cm(2)), low turn-on field (1.0 V/mum) and field enhan

278 vity and limit of detection to glucose of 80 mA M(-1) cm(-2) and 7 muM after only 30 s of adsorption

279 TCDA, where a reversible capacity of over 80 mA h g(-1) is delivered.

280 ic sensitivity and limit of detection of 830 mA M(-1) cm(-2) and 0.5 muM at 0.05 V, and a cathodic se

281 y of 788 mAh/g at a high current rate of 835 mA/g.

282 ge - 120 kVp, current tube time product - 86 mAs, slice thickness 1 mm.

283 f lithium's highest specific capacity (3,860 mA/g) and lowest negative electrochemical potential ( ap

284 , 648 and 536 mA h g(-1) , and 1067 and 881 mA h cm(-3) with a stable cyclability.

285 rate capability (129.1 mA h/g at 2 C; 110.9 mA h/g at 10 C) and cycling stability (87.2% capacity re

286 short-circuit current density (Jsc) of 13.9 mA/cm(2) and a fill factor (FF) of 62% on glass substrat

287 mA g(-1) and a good rate capability of 221.9 mA h g(-1), even at 1 A g(-1).

288 on with a current density of approximately 9 mA cm(-2) at a potential of 0 V versus RHE under 1-sun i

289 ility, delivering a discharge capacity of 90 mA h g(-1) at 60 C-rate.

290 were conducted: (I) mixed batch with 150-900 mA applied for 1 min to 1 L, (II) stagnant batch with 60

291 min to 1 L, (II) stagnant batch with 600-900 mA applied for 1 min to 1 L, and (III and IV) continuous

292 at conventional current amplitudes (800-900 mA) is highly effective but carries the risk of cognitiv

293 n hydraulic retention times and constant 900 mA.

294 ort-circuit current density (J SC ) of 17.92 mA cm(-2) .

295 ad to photocurrent densities as high as 1.97 mA/cm(2) with 445-nm, approximately 90-mW/cm(2) illumina

296 (398 mA mg(-1)) and specific activity (0.98 mA cm(-2)), and a good If/Ib ratio (1.15), better than t

297 hort-circuit current density (Jsc ) to 17.99 mA cm(-2) and fill factor (FF) to 77.19%, yielding a mil

298 pproximately 98%, at a current density of 99 mA g(-1) (0.9 C) with clear discharge voltage plateaus (

299 asive neuromodulation technique that applies mA currents at the scalp to modulate cortical excitabili

300 mass activities that reach 7.8 milliampere (mA) per centimeter squared and 4.3 ampere per milligram