ライフサイエンスコーパス: mA

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

2 endures a critical current density up to 1.0 mA cm(-2) .

3 r average CE of 99.3% (2.0 mAh cm(-2) at 2.0 mA cm(-2) ) compared to bare electrodes.

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

5 d high short-circuit current density of 22.0 mA cm(-2), resulting in high power conversion efficienci

6 ange, including 130 cycles (2600 min) at 3.0 mA cm(-2) , with 0.178 V overpotential.

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

8 (R(2) = 0.9997), sensitivity = 2.83 +/- 0.01 mA-L mol(-1), and response variability <=4% RSD.

9 onjunction with this high sensitivity (2.014 mA mM(-1).cm(-2)), the material possesses excellent sele

10 he maximum current density was 4.10 +/- 0.02 mA cm(-2), which is 8-fold higher than that of a rGO ele

11 than that of a rGO electrode (0.51 +/- 0.03 mA cm(-2)), and is among the best performance reported f

12 or and stable photocurrents of up to ~ 0.036 mA/cm(2).

13 over 100 cycles at a current density of 0.05 mA cm(-2) .

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

15 sity was lower (9.6+/-0.9 versus 16.9+/-0.09 mA/mm(2); P<0.0001).

16 drogen electrode in 0.1 M KOH to deliver 0.1 mA cm(-2) H(2)O(2) current, and a high H(2)O(2) selectiv

17 We achieve a photocurrent density of 15.1 mA cm(-2) at 1.23 V vs. reversible hydrogen electrode (R

18 p, photoconductivity (responsivity = 4 +/- 1 mA/W), and stability for months in air.

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

20 stripping Coulombic efficiency of 99.55 % (1 mA cm(-2) , 1.0 mAh cm(-2) ) and the electrolyte also en

21 real capacity and current density (e.g., 6.1 mA h cm(-2) at 0.9 mA cm(-2)), providing an intriguing c

22 Stimulation (amplitude 1 mA, frequency 1 Hz for 40 minutes, followed by a 20 minu

23 de is demonstrated by cycling for 500 h at 1 mA cm(-2) , followed by another 500 h at 2 mA cm(-2) wit

24 cm(-2) for 10 000 min (100 cycles), and at 1 mA cm(-2) for 5000 min.

25 high areal capacitance of 3.54 F/cm(2) at 1 mA/cm(2) and an excellent rate capability.

26 day EA treatments (mixture of 2 Hz/100 Hz, 1 mA, 30 minutes once a day) at the acupoints of Yintang (

27 n the linear range (10(-12) - 10(-8) M) is 1 mA dec(-1) (drain current variations).

28 5-10 min post 20 min-1 mA tDCS, D(eff) increased by ~ 10% for a small solute, s

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

30 required to generate a current density of 1 mA/cm(2) shifts anodically by 260 mV to give an onset po

31 1)% with a conversion rate of (4.5 +/- 0.1) mA cm(-2), and a record n-propanol cathodic energy conve

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

33 verpotentials of 61 and 285 mV to achieve 10 mA cm(-2) for HER and OER in alkaline medium, respective

34 small overpotential of 27.7 mV to achieve 10 mA cm(-2) geometric current density and a Tafel slope of

35 small overpotential of 39 mV to achieve -10 mA cm(-2) and a very low Tafel slope of 32 mV dec(-1) .

36 cile and scalable sol-gel method achieves 10 mA cm(-2) at a low overpotential of only 340 mV (and sma

37 OER with a low overpotential of 1.51 V at 10 mA cm(-2) and a small Tafel slope of 45 mV dec(-1) in al

38 s a record low overpotential of 178 mV at 10 mA cm(-2) and maintains the excellent performance throug

39 uiring an overpotential of only 358 mV at 10 mA cm(-2) in Fe-free electrolyte and, above all, exhibit

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

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

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

43 We predict an onset potential (at 10 mA cm(-2)) U(onset) = -0.84 V (vs.

44 at different current densities (316 mV at 10 mA cm(-2)), low Tafel slope (37 mV per decade), high max

45 ves an ultralow overpotential of 27 mV at 10 mA cm(-2), and a low Tafel slope of 36 mV dec(-1), repre

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

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

48 with an overpotential of merely 42 mV at 10 mA cm(geo) (-2) .

49 rement derived from -0.296 mV (for VB at -10 mA cm(-2) current density) and -0.273 mV (for V(3) B(4)

50 ayed merely an overpotential of 12 mV at -10 mA cm(-2), which is substantially lower than that of Pt

51 vs RHE and an overpotential of 400 mV at 10 mA.cm(-2) as well as the electrochemical long-term stabi

52 ydrogen production efficiencies (>90%) at 10 mA.cm(-2) were mainly attributed to the use of NF in thr

53 with an overpotential of 270 +/- 3 mV at 10 mA/cm(2) and a Tafel slope of 39 mV/dec, both of which a

54 a competitive overpotential of 380 mV at 10 mA/cm(2).

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

56 des at relatively low current densities, <10 mA/cm(2).

57 n outperforms the Pt/C benchmark (32.7 mV@10 mA cm(-2) and 30.90 mV dec(-1) ).

58 mV, respectively, at a current density of 10 mA cm(-2) .

59 over 2500 h at a high current density of 10 mA cm(-2) .

60 as 14 and 13.3 mV at a current density of 10 mA cm(-2) .

61 otential 198 mV at the current density of 10 mA cm(-2) and a small Tafel slope of 39 mV dec(-1) for o

62 tential of 240 mV at a current density of 10 mA cm(-2) and a Tafel slope of 58 mV dec(-1) .

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

64 ight, achieving a photocurrent density of 10 mA cm(-2) at +0.13 V vs RHE.

65 (2) Mo(3) N exhibits a current density of 10 mA cm(-2) at a nominal overpotential of 270 mV in 0.1 m

66 activity, achieving a current density of 10 mA cm(-2) at an overpotential of 218 mV, which is smalle

67 R activity, yielding a current density of 10 mA cm(-2) at an overpotential of 66 mV, which is slightl

68 required to maintain a current density of 10 mA cm(-2) decreases from 320 mV to just 178 mV.

69 tentiometry test at a constant current of 10 mA cm(-2) in 0.5 M H(2)SO(4) solution.

70 otential of 49 mV at a current density of 10 mA cm(-2) in 1 m phosphate buffer solution (PBS, pH 7.0)

71 produce hydrogen at a current density of 10 mA cm(-2) under overpotentials of only 20, 50, and 36 mV

72 ficiency of 84.5% at a current density of 10 mA cm(-2), a power density of 86.2 mW cm(-2) and a stabl

73 e of 1.52 V to reach a current density of 10 mA cm(-2).

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

75 tential of 139 mV at a current density of 10 mA/cm(2), with a Tafel slope of only 32 mV/dec, showing

76 overpotential of only 226 mV for reaching 10 mA cm(-2) (geo) at a loading of Ir as low as 12.5 mug(Ir

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

78 in operational lifetime (when driven at 100 mA cm(-2) ).

79 xhibit a low potential gap of ~1.17 V at 100 mA g(-1) and can be repeatedly charged and discharged fo

80 flux into the draw solution (5.56 LMH at 100 mA), compared to the control (1.10 LMH with no current).

81 led with these two catalysts can deliver 100 mA cm(-2) at 1.39 V.

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

83 when the current rate is increased from 100 mA g(-1) to 2000 mA g(-1).

84 es at high operating current densities (>100 mA cm(-2) ).

85 ommercially relevant current densities (>100 mA cm(-2)).

86 An applied fixed current of 100 mA (1.7 mA cm(-2)) was sustained by the proton flux thro

87 5 mF cm(-2) at a high current density of 100 mA cm(-2) but also an ultrahigh intrinsic capacitance of

88 ility tests at a high current density of 100 mA cm(geo) (-2) show its super-stable performance with o

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

90 the driving current increases from 10 to 100 mA, indicating that the quantum confined Stark effect is

91 capacity after 450 and 550 cycles under 100 mA g(-1) in 4.57 V pouch full-cells matched with a graph

92 ing AEMFCs where the kinetic current was 100 mA cm(-2) at 0.85 V.

93 ty) and rate capability (~70 mAh g(-1) @1000 mA g(-1)), while achieving capacity retention close to 1

94 y required current densities of 500 and 1000 mA cm(-2) at record low voltages of 1.608 and 1.709 V, r

95 ap up to 1.96 V at a current density of 1000 mA g(-1) , stability over 360 cycles, and good flexibili

96 M (R(2) = 0.996) and high sensitivity of 106 mA M(-1) cm(-2).

97 arbon nanotubes shows a high capacity of 116 mA h g(-1) , with high utilization of its redox-active s

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

99 able rate capability of 96 mAh g(-1) at 1200 mA g(-1) .

100 performance, including a high capacity (1253 mA h g(-1) ) and ultralong lifespan (1000 cycles) with a

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

102 y, outstanding rate performance (e.g., 1,138 mA h g(-1) at 0.2 C or 440 mA h g(-1) at 60 C with a mas

103 At 15 mA.cm(-2), and in the absence of chloride (0.6 mol.L(-1)

104 The system draws 15 mA under continuous operation when powered by a 3.7 V 15

105 78.8% even at a high current density of 150 mA cm(-2).

106 CO(2) reduction current densities up to 150 mA/cm(2).

107 sible range, in which a responsivity of 0.16 mA/W was achieved at 532 nm.

108 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

109 e cathode with 99.0% capacity remaining (194 mA h g(-1)) after 100 cycles at 1 C.

110 s(-1) and currents per channel width of 0.2 mA cm(-1) at operation voltages as low as 1 V, owing to

111 Using a current density of 0.2 mA cm(-2) , the Li/LNZTO/Li symmetric cell can cycle for

112 @3D-Cu cells exhibit stable cycling at 0.1-2 mA cm(-2) , while baseline Cu prematurely fails when the

113 s, yet a low overpotential of 322 mV at 10.2 mA cm(-2) and a high current density of more than 300 mA

114 ieves a high critical current density of 2.2 mA cm(-2) under ambient conditions due to the enhanced i

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

116 CO at -0.11 V vs. RHE (j(-0.11, CO)) of -3.2 mA cm(-2).

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

118 ed solar illumination, with currents above 2 mA cm(-2) at 1.23 V(RHE).

119 300 h in a symmetrical cell is obtained at 2 mA cm(-2) , implying great potential to stabilize lithiu

120 tting the SAW leads to short circuiting at 2 mA cm(-2) .

121 h with a small overpotential of ~80 mV at 2 mA cm(-2) .

122 1 mA cm(-2) , followed by another 500 h at 2 mA cm(-2) without short-circuiting, realizing a record h

123 20 min of active prefrontal stimulation at 2 mA or sham stimulation.

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

125 ower overpotential at a current density of 2 mA cm(-2)) is observed at the edge plane compared to the

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

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

128 orods achieve current densities of 10 and 20 mA cm(-2) at overpotentials of, respectively, 53 and 79

129 loss over 900 charge-discharge cycles at 20 mA cm(-2) .

130 ed settings (0.25 mm electrode spacing at 20 mA) compared to traditional ESI.

131 iving WD with overpotentials of <10 mV at 20 mA.cm(-2) and pure water BPM electrolyzers that operate

132 ulation at 20 Hz, 4 ms pulse width, and <=20 mA.

133 ility at an ultra-high current density of 20 mA cm(-2) .

134 of 648 mAh g(-1) at a current density of 20 mA cm(-2) with a good long-term durability, outperformin

135 high specific capacity (~180 mAh g(-1) @200 mA g(-1) current density) and rate capability (~70 mAh g

136 retention of 88.4% within 200 cycles at 200 mA g(-1) .

137 .8 F cm(-2) even at a current density of 200 mA cm(-2) .

138 E > 10% to current densities as high as 2000 mA cm(-2) ), and tenfold increase in operational lifetim

139 nt density per catalyst mass loading of 2000 mA g(cat.) (-1) , as well as good stability and durable

140 rate is increased from 100 mA g(-1) to 2000 mA g(-1).

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

142 daic efficiency of 41% toward ethanol at 250 mA/cm(2) and -0.67 V vs RHE, leading to a cathodic-side

143 muM to 15 mM, and a high sensitivity of 250 mA/cm(2)/M at a potential of -0.3 V.

144 2 full cell is 81% after 1,500 cycles at 268 mA gSeS2(-1).

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

146 ity (R) and detectivity (D*) reach up to 270 mA W(-1) and 5.4 x 10(14) Jones, respectively.

147 nificantly, its current density reaches ~288 mA cm(-2) at -0.61 V versus reversible hydrogen electrod

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

149 85%) with high current densities up to -17.3 mA cm(-2) as a composite with carbon black at 1:1 mass r

150 yst exhibits a high current density of -38.3 mA.cm(-2) using industry-ready silicon photoelectrodes w

151 and a power density of 0.64 mW cm(-2) at 4.3 mA cm(-2) .

152 (1/2) =0.83 V vs. RHE, n=3.93, and j(L) =5.3 mA cm(-2) ) in alkaline media, which is the record value

153 A h g(-1) , superior rate capability of 79.3 mA h g(-1) at 20 C, and 85.4 % capacity retention after

154 3.1 A/mg(Pt) and a specific activity of 9.3 mA/cm(2) at room temperature with only 15.9% loss of mas

155 onger than bare Li at a current density of 3 mA cm(-2) ).

156 Geobacter and attains a current density of 3 mA cm(-2) stemming from bacterial respiration.

157 transfer with maximum current densities of 3 mA cm(-2).

158 rge transfer resistance of ~200 ohm and a 30 mA cm(-2) current density at only 0.53 V versus a revers

159 its a high photocurrent density of almost 30 mA cm(-2) at 0 V against the reversible hydrogen electro

160 ets array exhibits a voltage of 1.58 V at 30 mA cm(-2) as bifunctional electrode for water splitting,

161 reduced to ~205 mV at current density of 30 mA cm(-2) , which represents the best performance achiev

162 (-1), 80 cycles) and, at a charge rate of 30 mA g(-1), exhibit charge capacities of about 120 mA h g(

163 ns stable lithium stripping/plating under 30 mA cm(-2) and 5 mAh cm(-2) with a very low overpotential

164 ycles (1500 h) with a cutoff capacity of 300 mA h g(-1) .

165 and a high current density of more than 300 mA cm(-2) at 1.7 V(NHE) were obtained in 1 m KOH.

166 ty, and its working current can go up to 300 mA.

167 ws a remarkable photocurrent density of 7.32 mA cm(-2) at a potential of 1.23 V versus a reversible h

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

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

170 cathode with a high reversible capacity (387 mA h g(-1) ), large specific energy density (775 Wh kg(-

171 d with the highest photocurrent of up to 0.4 mA cm(-2) and near-quantitative faradaic efficiency for

172 ne skin by applying a current density of 0.4 mA cm(-2) via two electrodes.

173 hibits a higher reversible capacity of 123.4 mA h g(-1) , superior rate capability of 79.3 mA h g(-1)

174 .10 V, short-circuit current density of 15.4 mA cm(-2) , and fill factor of 74.8%, demonstrating the

175 anode generated photocurrents of 1.8 and 5.4 mA cm(-2) at 0.6 and 1.2 V(RHE) , respectively, with a p

176 ic efficiency of ~99.2% over 150 cycles at 4 mA cm(-2) .

177 y demanding current-capacity conditions of 4 mA cm(-2) -8 mAh cm(-2) .

178 Current densities of ~4 mA/cm(2) and selectivities (FE(CO)) of 99% were achieved

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

180 At a high current density of 4000 mA g(-1) (~18 C), 75.0% of the initial capacity is maint

181 s found to be 8.8 ng/L with sensitivity 0.41 mA/ng/L/cm(2) for chlorpyrifos (CPF); and 10.2 ng/L with

182 d cathodic photocurrent densities of + 38.41 mA cm(-2) (+ 0.76 V(RHE)) and- 2.48 mA cm(-2) (0 V(RHE))

183 mM (R(2) = 0.971) and high sensitivity of 41 mA M(-1) cm(-2).

184 ance (e.g., 1,138 mA h g(-1) at 0.2 C or 440 mA h g(-1) at 60 C with a mass loading of 1 mg cm(-2)),

185 vity (formate partial current densities ~450 mA cm(-2)), selectivity (maximal Faradaic efficiency ~97

186 cm(-2) and a maximum current density of 456 mA cm(-2) , which exceeds all previously reported COF ma

187 reduction reaction (ORR) mass activity of 47 mA mg(cat.) (-1) represents 1.3- and 6.4-fold enhancemen

188 + 38.41 mA cm(-2) (+ 0.76 V(RHE)) and- 2.48 mA cm(-2) (0 V(RHE)), respectively.

189 tionally high short-circuit current of 27.48 mA/cm(2) and a power conversion efficiency of 17.08%.

190 A photocurrent density of 4.48 mA.cm(-2) at 1.23 V vs reversible hydrogen electrode (RH

191 1.72 A mg(-1) and specific activity of 2.49 mA cm(-2) for MOR, which are 3.17 and 2.79 times higher

192 ell is stable at 1000 cycles (1950 h) at 0.5 mA cm(-2) , with 98.9% cycling Coulombic efficiency and

193 ematurely fails when the current reaches 0.5 mA cm(-2) .

194 rGO@3D-Cu (no K reservoir) are stable at 0.5 mA cm(-2) for 10 000 min (100 cycles), and at 1 mA cm(-2

195 hort circuit current density of 16.0 +/- 0.5 mA cm(-2), and a fill factor of 0.70 +/- 0.01.

196 timulations at each DCN from T6 to L1 at 0.5 mA to activate A-fiber alone or 5 mA to activate both A-

197 adjacent DCNs concurrently, but only at 0.5 mA, affected HR but not BP.

198 ol cm(-2)) and a high current density (-16.5 mA cm(-2); overpotential, -0.52 V) for the CO(2) to CO r

199 The obtained mass activity of ~2.5 mA.mug(-1) at the defined overpotential of 300 mV is 1 o

200 as able to achieve a current density of -9.5 mA cm(-2) with a FE(CO) of 79%.

201 high areal capacitance of 3.1 F cm(-2) at 5 mA cm(-2) , with areal capacitance remaining at 1.8 F cm

202 and an energy density of 517 Wh kg(-1) at 5 mA cm(-2) together with good cycling stability.

203 ed-oriented Au thin films by DC plating at 5 mA/cm(2).

204 ize, <0.5 mm; feed rate, 0.4 L/d; current, 5 mA), in a continuous flow system, the CaCO(3) packed ele

205 4 months of stimulation parameters (14 Hz, 5 mA, pulses of 330 mus) or no stimulation (control); 149

206 formance over 5000 h, a rate capability of 5 mA cm(-2) , and a remarkably high Coulombic efficiency (

207 L1 at 0.5 mA to activate A-fiber alone or 5 mA to activate both A- and C-fibers at different frequen

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

209 ith a partial current density of (108 +/- 5) mA cm(-2) and a methane cathodic energy efficiency of 20

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

211 resulting in current densities of 10 and 50 mA cm(-2) at overpotentials of 293 and 506 mV, respectiv

212 a reversible capacity of 220 mAh g(-1) at 50 mA g(-1) , corresponding to the energy density of 440 Wh

213 h reversible capacity of 228 mAh g(-1) at 50 mA g(-1).

214 ewater at near-neutral pH after 60 min at 50 mA with 0.4 g L(-1) catalyst as optimum dose.

215 talyst)(-1) h(-1) at a current density of 50 mA cm(-2).

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

217 talytic reaction rates, ranged from 15 to 50 mA cm(-2) mM(-1) comparable to those reported for state-

218 an alkaline anode and acidic cathode at 500 mA.cm(-2) with a total electrolysis voltage of ~2.2 V.

219 at relatively small current densities (<500 mA cm(-2) ) with moderate radiance (<400 W sr(-1) m(-2)

220 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

221 operation condition (27-40 g L(-1) NaCl, 500 mA).

222 at 4-degree incident angle, 41.29 and 41.52 mA/cm(2) for the Inverted Pyramid and Teepee PhC, respec

223 ith a high mass specific peak current of 527 mA mg(-1) and excellent peak current density (29.8 mA cm

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

225 s (CPF); and 10.2 ng/L with sensitivity 0.58 mA/ng/L/cm(2) for methyl parathion (MP).

226 6 mA-Finder outperforms its peer tools in general and spec

227 lability at a high current density up to 0.6 mA cm(-2) A solid electrolyte interphase layer formed in

228 pping/plating at current densities up to 0.6 mA.cm(-2).

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

230 Cycled under 6 C (6.6 mA cm(-2)), a 1.0 mAh cm(-2) LiNi(0.6)Co(0.2)Mn(0.2)O(2)

231 e 90% above accuracy for detecting 5mC and 6 mA using only 2x coverage of reads.

232 F substrates stably operate over 1500 h at 6 mA cm(-2) for 6 mA h cm(-2) .

233 h read level and genome level on detecting 6 mA and 5mC methylation states comparing to previous hidd

234 The abnormal status of DNA 6 mA modification has been reported in cancer and other di

235 further experimental investigation of DNA 6 mA modification.

236 We present a novel online DNA 6 mA site tool, 6 mA-Finder, by incorporating seven sequen

237 bly operate over 1500 h at 6 mA cm(-2) for 6 mA h cm(-2) .

238 chieves a record-high critical current of >6 mA cm(-2) even at a high capacity of 6.0 mAh cm(-2) .

239 DNA N6-methyladenine (6 mA) has recently been found as an essential epigenetic m

240 The annotation of 6 mA marks in genome is the first crucial step to explore

241 peer tools in general and species-specific 6 mA site prediction, suggesting it can provide a useful r

242 SAW-integrated Li cells can operate up to 6 mA cm(-2) in a commercial carbonate-based electrolyte; o

243 present a novel online DNA 6 mA site tool, 6 mA-Finder, by incorporating seven sequence-derived infor

244 Deposition of N(6)-mA also antagonizes SATB1 function in vivo by preventing

245 However, the biological role of N(6)-mA and the molecular pathways that exert its function re

246 e an unexpected molecular mechanism for N(6)-mA function via SATB1, and reveal connections between DN

247 Concordantly, N(6)-mA functions at the boundaries between euchromatin and h

248 Here we show that N(6)-mA has a key role in changing the epigenetic landscape d

249 of SIDD-SATB1 interactions mediated by N(6)-mA is essential for gene regulation during trophoblast d

250 We found that N(6)-mA is upregulated during the development of mouse tropho

251 We show that the presence of N(6)-mA reduces the in vitro interactions by more than 500-fo

252 recent discovery of N(6)-methyladenine (N(6)-mA) in mammalian genomes suggests that it may serve as a

253 impressive energy efficiency of 70.6 % at 60 mA cm(-2) and a high power density of 91.5 mW cm(-2) at

254 ion with a voltage decay of only 15 % at 600 mA cm(-2) under H(2) /air (CO(2) -free) reacting gas fee

255 operated continuously for over 1000 h at 600 mA cm(-2) with voltage decay rate of only 32-muV h(-1) -

256 and a short-circuit current density of 28.63 mA cm(-2).

257 oth of these values exceed the MAPD (= 39.63 mA/cm(2)) corresponding to the Lambertian limit for a 10

258 igh areal capacitance of 2.1 F cm(-2) at 1.7 mA cm(-2) and a gravimetric capacitance of 242.5 F g(-1)

259 oanodes with photocurrents that reach to 1.7 mA cm(-2) with an optimized, applied bias photon-to-curr

260 An applied fixed current of 100 mA (1.7 mA cm(-2)) was sustained by the proton flux through the

261 is significantly enhanced from 10.3 to 11.7 mA cm(-2) (while retaining the open-circuit voltage and

262 es stable operation of high-rate (10 C, 16.7 mA cm(-2) ) and electrolyte-starved (4.7 muL mg(S) (-1)

263 athode shows a photocurrent density of -16.7 mA cm(-2) at 0 V versus reversible hydrogen electrode (R

264 % selectivity and a current density of 56.7 mA cm(-2) in the presence of 5 % O(2) .

265 te gave 1 Sun photocurrent density up to 8.7 mA cm(-2) at 0 V vs RHE (pH 1).

266 ghest current is for Ni-N(4), leading to 700 mA cm(-2) at U = -1.12 V.

267 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

268 r decade), high maximum current density (710 mA cm(-2) at 2.0 V vs RHE), and great durability (15 h).

269 w a high syngas evolution (total current >74 mA cm(-2) ) with CO/H(2) ratios (0.23-2.26) that are sui

270 inty of 1 mV, and current from 2 muA to 0.75 mA with a resolution of 1.1 muA.

271 eased photocurrent density from 0.68 to 4.75 mA cm(-2) and provides a promising design strategy for e

272 ing a record high cumulative capacity of 750 mA h cm(-2) for garnet-type all-solid-state Li batteries

273 L(-1) (S/N = 3), sensitivity = 35.6 +/- 0.8 mA-L mol(-1) and response variability <=4% RSD.

274 is applied and the photocurrent reaches 1.8 mA cm(-2) with faradaic efficiency up to 95 % for H(2) O

275 n limit of 22 nM DA, and sensitivity of 13.8 mA/mM((DA)), in a wider range of 0.3-750 muM DA, was obt

276 -1) and excellent peak current density (29.8 mA cm(-2) ) at low potential (0.6 V).

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

278 A current density of 65.8 mA.cm(-2) at -1.8 V vs. Ag/Ag(+) is observed with a Fara

279 uO(2) where initial photocurrent density (>8 mA cm(-2)) deceased only 15% or 33% during continuous op

280 PO(4) cathode exhibits a high capacity of 80 mA h g(-1) at a charge/discharge rate of 10 C with capac

281 ds 180 mV less overpotential to drive an 800 mA cm(-2) current density.

282 formance, yielding a current density of 2.84 mA cm(-2) with Faradaic efficiency of 95.2% for CO gener

283 ts an operating photocurrent density of 6.84 mA cm(-2) and stable gas production with an average sola

284 R and OER current densities of 7.21 and 6.85 mA cm(-2) at 2.0 and 4.2 V versus Li/Li(+) , respectivel

285 xhibits a specific current density of -32.87 mA cm(-2) and turnover frequency of 1962 h(-1) at a mild

286 formate of 96 % and current density of 8.87 mA cm(-2) at low potential of -0.65 V versus RHE.

287 urrent density (e.g., 6.1 mA h cm(-2) at 0.9 mA cm(-2)), providing an intriguing class of materials f

288 limit of 0.22 muM DA, and sensitivity of 4.9 mA/mM((DA)), in the EC.

289 re subjected to x-ray irradiation (90 keV, 9 mA) to doses up to 15 Gy.

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

291 ass (1.99 A mg(-1) (Ir) ) and specific (3.93 mA cm(-2) (Ir) ) activities, but also greatly enhanced d

292 liver an ultrahigh discharge capacity of 947 mA h g(-1) , corresponding to a low electrolyte-to-capac

293 r dynamics simulation with newly constructed mA(3)AR and hA(3)AR homology models.

294 weak in inducing mouse hypothermia, despite mA(1)AR full agonism and variable mA(3)AR efficacy, but

295 (2-phenylethyl) moiety particularly enhanced mA(3)AR affinity by polar interactions with the extracel

296 vitro (hA(3)AR, cAMP inhibition, 31% E(max); mA(3)AR, [(35)S]GTP-gamma-S binding, 16% E(max)) and in

297 at dose levels down to 10 quality reference mAs (size-specific dose estimate, 0.9 mGy) had noninferi

298 in 83 patients (120 kV, 70 quality reference mAs [QRM]) were collected between November 2013 and Apri

299 ectrolyte-to-capacity ratio of about 4.8 uL (mA h)(-1) , and remain stable over 55 cycles under pract

300 a, despite mA(1)AR full agonism and variable mA(3)AR efficacy, but strong hypothermia by 9 depended o