ライフサイエンスコーパス: current density

1 -scale electrolyzers operating at industrial current density.

2 lectrical properties and excellent breakdown current density.

3 nd the efficacy depended on insulin dose and current density.

4 ent inactivation of I(Ca,L) without changing current density.

5 vex cross sections are created due to uneven current density.

6 a1 rescued Ca(2+)-mediated regulation of Kv4 current density.

7 due to the locally enhanced surface exchange current density.

8 to the interdependency of photogain and dark current density.

9 hannel inactivation accompanied by increased current density.

10 arizing shift in activation and reduction in current density.

11 ctive materials and poor performance at high current density.

12 with carbon and platinum electrodes at high current density.

13 electivity but at high overpotential and low current density.

14 te the trap states, helping to maintain high current density.

15 less overpotential to drive an 800 mA cm(-2) current density.

16 nuous product extraction and in flow at high current density.

17 to take place at an order-of-magnitude lower current density.

18 es owing to their small size and low driving-current density.

19 m and regulate the reaction rate through the current density.

20 ore compact structure and can achieve higher current densities.

21 ted with this anode under different cathodic current densities.

22 rthermophilic archaea can also generate high current densities.

23 annels and L268F at the pore decreases their current densities.

24 on their surface and to improve the produced current densities.

25 ntial of 219 mV is achieved at the geometric current density 10 mA cm(-2) in an alkaline electrolyte,

26 Capsaicin evoked inward currents (current density ~10% of sensory neurons) and raised intr

27 troactive sites (270 nmol cm(-2)) and a high current density (-16.5 mA cm(-2); overpotential, -0.52 V

28 current of 527 mA mg(-1) and excellent peak current density (29.8 mA cm(-2) ) at low potential (0.6

29 n (OER), with low overpotential at different current densities (316 mV at 10 mA cm(-2)), low Tafel sl

30 performance to attain stable high power and current density (38 muW/cm(2) and 120 muA/cm(2)) that th

31 upling with a high activity (formate partial current densities ~450 mA cm(-2)), selectivity (maximal

32 Tafel slope (37 mV per decade), high maximum current density (710 mA cm(-2) at 2.0 V vs RHE), and gre

33 d (0.1 M Li(2)SO(4)), even at relatively low current densities, a pH difference of three units is mea

34 ring a significantly higher pitch-normalized current density-above 0.9 milliampere per micrometer at

35 ses SUMOylation to continuously adjust ionic current densities according to changes in activity.

36 ver, the energy efficiency and productivity (current density) achieved so far still fall below the va

37 l shift (NICS) and anisotropy of the induced current density (ACID) were utilized in this study to pr

38 Partial current density analysis reveals the dominating associat

39 er LSPR excitation with significantly higher current densities and a shift to more positive potential

40 for 900 cycles and smooth deposition at high current densities and capacities, surpassing most previo

41 esults show how changes in cEC transmembrane current densities and gap junctional resistances can aff

42 to generate much higher CO and H(2) partial current densities and greater CO Faradaic efficiency tha

43 , and the effect of variations in dTL on the current densities and IR spectra were analyzed and discu

44 these surface functional groups even at high current densities and large mass loading/electrode thick

45 ucture, induced both an increase in Na(V)Sp1 current density and a negative shift in the activation c

46 of 27.7 mV to achieve 10 mA cm(-2) geometric current density and a Tafel slope of 30.88 mV dec(-1) ,

47 Cav3-S141R decreased current density and also slowed activation kinetics and

48 The Cav3-F97C mutation reduced current density and altered the kinetics of I(Kv4.2) and

49 h faradic-to-capacitive current ratios, high current density and electron mobility, and faster mass t

50 ile the tortuous 3D-Cu electrode reduces the current density and geometrically frustrates dendrites.

51 s yields enhanced photovoltaic short-circuit current density and good open-circuit voltage, so that I

52 fusion in this scaffold enable reduced local current density and homogeneous ionic flux during platin

53 ived neurons also displayed increased sodium current density and increased excitatory and decreased i

54 e, measurements of the resistivity, critical current density and magnetic-field response of Nd(0.8)Sr

55 ed CaValpha2delta1-mediated increase in peak current density and modulation of the voltage-dependent

56 However, this strategy is limited by high current density and narrow safety-to-efficacy window.

57 ection of the mutation re-establishes sodium current density and SCN5A expression.

58 iverse functional defects, including altered current density and shifts in the voltage dependence of

59 ls of Cav1.2 in the brain, as well as Cav1.2 current density and signaling to the nucleus, are reduce

60 nd bulk Ag, Tri-Ag-NPs exhibited an enhanced current density and significantly improved Faradaic effi

61 egulating SCN5A, leading to decreased sodium current density and slower conduction velocity.

62 The correlation between the current density and the probability of void formation in

63 RPC4 activation without altering the maximal current density and this effect was dependent on intrace

64 ived from -0.296 mV (for VB at -10 mA cm(-2) current density) and -0.273 mV (for V(3) B(4) ) we accur

65 cific capacity (~180 mAh g(-1) @200 mA g(-1) current density) and rate capability (~70 mAh g(-1) @100

66 ical shift), ACID (anisotropy of the induced current density), and monohydrogenation free energies an

67 Thus, the capacity, current density, and cycle life of the solid Li anode ar

68 ependent chemical shifts, anisotropy-induced current density, and harmonic oscillation stabilization

69 voltage dependence of activation, a reduced current density, and insensitivity to gating modulation

70 field, linearly proportional to the in-plane current density, and optimized when the current is ortho

71 ly high capacity (up to 40 mAh cm(-2)), high current density, and/or low temperatures (down to -15 de

72 ed during the reaction, especially when high current densities are used.

73 d have no common or prototypical traits, and current densities are usually well below those reported

74 cuit voltage, fill factor, and short circuit current density are also calculated from these transport

75 cs, high background charging current and low current density arising from poor mass transport.

76 siderably reduced EQE roll-off (EQE > 10% to current densities as high as 2000 mA cm(-2) ), and tenfo

77 size and crystal structure even after OER at current densities as high as several kA.m(-2).

78 presence of in-plane fields of 20 mT, charge current densities as low as 5 x 10(5) A cm(-2) are suffi

79 The CPE-K treated BESs had a maximum current density as high as 12.3 +/- 0.5 A/m(2), with tha

80 ), leading to a more than 4-fold increase of current density at -0.236 V (vs.

81 The current density at a fixed potential for the electro-oxi

82 er resistance of ~200 ohm and a 30 mA cm(-2) current density at only 0.53 V versus a reversible hydro

83 e successfully achieved engineering critical current density beyond 2.0 kA/mm(2) at 4.2 K and 16 T, b

84 subunits fails to significantly alter T790A current density but reduces TTX-resistant resurgent curr

85 ted at increased chloride concentrations and current densities, byproduct concentrations remained sim

86 ent chemical shift and anisotropy of induced current density calculations confirmed that benzocarbatr

87 chemical shift and anisotropy of the induced current density calculations, as well as X-ray crystallo

88 nt chemical shifts and anisotropy of induced current density calculations.

89 t at individual catalyst nanoparticles, high current densities can be realized.

90 simulation reveals that the anomalously high current density can be attributed to the non-equilibrium

91 Moreover, the local current density can be minimized due to the 3D C-wood fr

92 h specific capacitance (1734.9 F g(-1)) at a current density (CD) of 2 A g(-1).

93 At this low current density, CO(2) without pre-concentration is dire

94 decrease in Mg(2+) blockade and reduction in current density, confirming that the variant continues t

95 At high current densities, Cr(0.4) Mo(0.6) B(2) outperforms Pt/C

96 od, which defines the window at an arbitrary current density cut-off (J(cut-off)) value.

97 rons vs. non-labelled neurons, and slow K(A) current density decreased in association with hyperexcit

98 ing Re(tBu-bpy)(CO)(3)Cl on MWCNTs increases current densities, decreases overpotential, retains sele

99 otential pulses, leading to a high catalytic current density (Deltaj(cat):193 +/- 4 muA cm(-2)) under

100 ationalizes the experimentally observed weak current-density dependence of CT-EL and poses fundamenta

101 The discrete voids do not change the global current density distribution, but they induce the local

102 olutions and it is possible to have multiple current density distributions corresponding to the same

103 AP-clamp recordings revealed increased I(Kr) current density due to attenuated inactivation, primaril

104 mical reactor can only handle a very limited current density due to the low solubility of gas reactan

105 a large energy conversion efficiency at high current density due to the low solubility of organic rea

106 electrode architectures that both reduce the current density during plating-stripping and serve as ef

107 d be fabricated with high areal capacity and current density (e.g., 6.1 mA h cm(-2) at 0.9 mA cm(-2))

108 tion gradients on electrodes with high local current density (e.g., nanostructured) have important im

109 electrode thickness, influent concentration, current density, electrode flow rate, specific capacitan

110 of void formation indicates that a threshold current density exists for the activation of void format

111 We then identify the global sensitivity of current density, Faraday efficiency, and overpotential a

112 alues in open-circuit voltage, short-circuit current density, fill factor, and thereby much higher po

113 Enhanced current densities for mediated O2 reduction are observed

114 for C(2)H(4) by 3.4-fold and in the partial current density for CO(2) reduction by 2-fold compared w

115 The bioanode shows maximum current density for glucose oxidation up to 6.78 muA cm(

116 rate Li-air battery, and iv) high break-down current density for interconnect applications.

117 ciency higher than 40 per cent and a partial current density greater than 10 milliamperes per square

118 2.1-KCNE5 channels, increasing their maximum current density >2-fold, whereas BrS-associated KCNE5 mu

119 ton-polaritons at room temperature with high current densities (>10 kA cm(-2)) and tunability in the

120 olatile or gaseous species at high operating current densities (>100 mA cm(-2) ).

121 rom low selectivity at commercially relevant current densities (>100 mA cm(-2)).

122 loading amount of lithium and endure a large current density has not been achieved.

123 Specifically, the impacts of current density, hydraulic retention time, and feed comp

124 cluster in terms of the potential at a given current density, implying the single molecular catalyst

125 nanotubes to afford substantially increased current density, improved selectivity for carbon monoxid

126 d intracellular [Ca(2+)] rises and the TRPM8 current density in CCSNs were larger than in sham animal

127 .7), which displayed significantly increased current density in HEK293 cells while largely retaining

128 nnels, vincristine failed to alter TTX-S Na+ current density in medium dorsal root ganglion neurons a

129 lity and autism-but not epilepsy-reduced Na+ current density in neuroblastoma cells and expectedly de

130 tion increased mean ventricular myocyte K(V) current density in the apex and also in the subpopulatio

131 ogy, measured an ~1.5-fold increase in Kv4.2 current density in the presence of elevated intracellula

132 P2 component localization indicated a higher current density in the right middle frontal gyrus, a reg

133 cs and as much as five-times higher exchange current densities, in comparison to their spontaneously

134 vices, and the IQE had a larger droop as the current density increased for the LEDs grown on c-plane

135 We found that the CO(2) R to CO partial current density increased with increased Ni content befo

136 antum well confirms efficiency droop at high current densities is caused by a combination of strong n

137 The increase in TTX-S Na+ current density is likely mediated by Nav1.6, because in

138 Operation at such a current density is possible only because the magnet is w

139 and control the high sensitivity of critical current density J(c) to strain epsilon.

140 ave so far been the low engineering critical current density J(E), especially in high-current cables,

141 rchitecture, which allows us to produce high current densities (j) up to approximately 18 A cm(-2) wi

142 these factors contribute to a short-circuit current density (J sc ) of 17.07 mA cm(-2) .

143 een 450 and 800 nm, and a high short-circuit current density (J SC ) of 17.92 mA cm(-2) .

144 Further, the critical current density (J(c)) as a function of applied magnetic

145 The higher short-circuit current density (J(sc)) results from the smaller polymer

146 lead to both higher overall T c and critical-current-density, J c .

147 d synergically improves device short-circuit current density (Jsc ) to 17.99 mA cm(-2) and fill facto

148 efficiency (PCE) of 6.72% with short-circuit current density (Jsc) of 18.53 mA/cm(2), open circuit vo

149 in spite of having comparable short-circuit current density (Jsc).

150 triggered improvements in the short circuit current density (Jsc, from 32.5 to 37.0 mA/cm(2)).

151 odulation; i.e. we observed less increase in current density, less slowing of macroscopic current dec

152 t for hydrogen evolution, demonstrating high current densities, low overpotential, and remarkable sta

153 feature devices operated at relatively small current densities (<500 mA cm(-2) ) with moderate radian

154 ction on copper electrodes at relatively low current densities, <10 mA/cm(2).

155 The values of the magnitude of current density (MCD) obtained from the configuration we

156 s ion transport, particularly under the high current density necessary for devices requiring high pow

157 ical calculations (anisotropy of the induced current density, nucleus independent chemical shift, and

158 -Si/TiO2/C/CNT/[1+1(O)] electrodes exhibited current densities of 1 mA cm(-2) at 1.07 V vs NHE.

159 , the dual-doped Ni, Zn CoO nanorods achieve current densities of 10 and 20 mA cm(-2) at overpotentia

160 lar-panel-powered electrolyzer, resulting in current densities of 10 and 50 mA cm(-2) at overpotentia

161 xyhydroxide catalysts at the surface, yields current densities of 10 mA/cm(2) at an overpotential of

162 ion by direct electron transfer with maximum current densities of 3 mA cm(-2).

163 , we have achieved the industrially required current densities of 500 and 1000 mA cm(-2) at record lo

164 les with an exceptional activity-ORR and OER current densities of 7.21 and 6.85 mA cm(-2) at 2.0 and

165 rticles around the central axis, strong spin current densities of [Formula: see text] peta-ampere/[Fo

166 potentials of several tens of millivolt and current densities of several microA cm(-2) at aqueous fl

167 Current densities of ~4 mA/cm(2) and selectivities (FE(C

168 fficiency (FE) of (48 +/- 2)% with a partial current density of (108 +/- 5) mA cm(-2) and a methane c

169 The switching current density of (BiSb)(2) Te(3) (1.20 x 10(5) A cm(-2

170 le-nickel-atom electrode exhibits a specific current density of -32.87 mA cm(-2) and turnover frequen

171 , the designed CuFe catalyst exhibits a high current density of -38.3 mA.cm(-2) using industry-ready

172 an electrode material was able to achieve a current density of -9.5 mA cm(-2) with a FE(CO) of 79%.

173 triping and plating for over 100 cycles at a current density of 0.05 mA cm(-2) .

174 of approximately 0.13 W cm(-2) at a constant current density of 0.15 A cm(-2) with a carbon utilizati

175 Using a current density of 0.2 mA cm(-2) , the Li/LNZTO/Li symme

176 Li(+) from under porcine skin by applying a current density of 0.4 mA cm(-2) via two electrodes.

177 igh specific capacitance of 440 F g(-1) at a current density of 0.5 A g(-1), and excellent cycling st

178 de shows high capacity of 545 mAh g(-1) at a current density of 0.5 C.

179 ow capacity decay rate of 0.0126 % at a high current density of 0.5 C.

180 cut-off capacity of 1000 mAh g(-1) at a high current density of 1 A g(-1) .

181 At high current density of 1 A/g, alpha-NiS showed the highest c

182 the HER overpotential required to generate a current density of 1 mA/cm(2) shifts anodically by 260 m

183 apable of operating at the very high winding current density of 1,260 amperes per square millimetre.

184 cycling stability over 200 cycles at a high current density of 1.0 A g(-1) .

185 ectrolyte (pH ~ 15) with an ethylene partial current density of 1.3 amperes per square centimeter at

186 At 150K, the photodetectors exhibit a dark current density of 1.8 x 10(-10) A/cm(2) and a quantum e

187 tentials of 27 and 34 mV, respectively, at a current density of 10 mA cm(-2) .

188 e Li plating/stripping over 2500 h at a high current density of 10 mA cm(-2) .

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

190 ng activity with overpotential 198 mV at the current density of 10 mA cm(-2) and a small Tafel slope

191 he OER, with an overpotential of 240 mV at a current density of 10 mA cm(-2) and a Tafel slope of 58

192 vity with a low overpotential of 280 mV at a current density of 10 mA cm(-2) and high durability in a

193 Ni(2) Mo(3) N exhibits a current density of 10 mA cm(-2) at a nominal overpotenti

194 sesses outstanding OER activity, achieving a current density of 10 mA cm(-2) at an overpotential of 2

195 iCu exhibits better HER activity, yielding a current density of 10 mA cm(-2) at an overpotential of 6

196 lt, the overpotential required to maintain a current density of 10 mA cm(-2) decreases from 320 mV to

197 formance with an overpotential of 49 mV at a current density of 10 mA cm(-2) in 1 m phosphate buffer

198 orption, the catalysts produce hydrogen at a current density of 10 mA cm(-2) under overpotentials of

199 liver a high energy efficiency of 84.5% at a current density of 10 mA cm(-2), a power density of 86.2

200 require a cell voltage of 1.52 V to reach a current density of 10 mA cm(-2).

201 a-NiS showed an overpotential of 139 mV at a current density of 10 mA/cm(2), with a Tafel slope of on

202 an overpotential of only -12 mV to reach the current density of 10 mV cm(-2) in 1 M KOH and -47 mV in

203 ith an equivalent 100% spin polarised charge current density of 10(7) A cm(-2).

204 real capacitance of 2195 mF cm(-2) at a high current density of 100 mA cm(-2) but also an ultrahigh i

205 Stability tests at a high current density of 100 mA cm(geo) (-2) show its super-st

206 y with a low potential gap up to 1.96 V at a current density of 1000 mA g(-1) , stability over 360 cy

207 pen-circuit voltage of 1.10 V, short-circuit current density of 15.4 mA cm(-2) , and fill factor of 7

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

209 ith V(OC) = 0.94 +/- 0.01 V, a short circuit current density of 16.0 +/- 0.5 mA cm(-2), and a fill fa

210 l slope of 46 mV dec(-1) and a high exchange current density of 17 muA cm(-2) , which is far better t

211 capacitance reaching up to 254 F g(-1) at a current density of 2 A g(-1).

212 tic activity (i.e., lower overpotential at a current density of 2 mA cm(-2)) is observed at the edge

213 ~1 Omega cm(2) and achieves a high critical current density of 2.2 mA cm(-2) under ambient condition

214 e, with proper thermal management, a maximum current density of 2.5 kA cm(-2) and an EQE of ~1% at 1

215 ytic CO(2) reduction performance, yielding a current density of 2.84 mA cm(-2) with Faradaic efficien

216 t high rate capability of 197.1 mAh g(-1) at current density of 20 A g(-1) with capacity retention of

217 At a current density of 20 A m(-2), TAN removal rate from the

218 s excellent cycle stability at an ultra-high current density of 20 mA cm(-2) .

219 able specific capacity of 648 mAh g(-1) at a current density of 20 mA cm(-2) with a good long-term du

220 acitance remaining at 1.8 F cm(-2) even at a current density of 200 mA cm(-2) .

221 oltage loss of 0.57 V and high short-circuit current density of 22.0 mA cm(-2), resulting in high pow

222 adaic efficiency of 72 per cent at a partial current density of 230 milliamperes per square centimetr

223 a fill factor of 79.74%, and a short-circuit current density of 28.63 mA cm(-2).

224 longed (three times longer than bare Li at a current density of 3 mA cm(-2) ).

225 of current-producing Geobacter and attains a current density of 3 mA cm(-2) stemming from bacterial r

226 ravimetric capacity of 457 C g(-1) at a high current density of 30 A g(-1) , which is nearly two and

227 e OER overpotential is reduced to ~205 mV at current density of 30 mA cm(-2) , which represents the b

228 Emission current density of 300 uA/cm(2) has been achieved at an

229 , we report on a selector with a large drive current density of 34 MA cm(-2) and a ~10(6) high nonlin

230 ickel sulfide heterostructures can deliver a current density of 37.2 mA cm(-2) at an overpotential of

231 ut 66 per cent for pure Cu) is achieved at a current density of 400 milliamperes per square centimetr

232 At a high current density of 4000 mA g(-1) (~18 C), 75.0% of the i

233 power density of 81 mW cm(-2) and a maximum current density of 456 mA cm(-2) , which exceeds all pre

234 With a dark current density of 5.3 x 10(-4) A/cm(2) under -20 mV app

235 rate of 335 gN m(-2) d(-1) was achieved at a current density of 50 A m(-2) and an energy demand of 56

236 an 4 mol peroxide g(catalyst)(-1) h(-1) at a current density of 50 mA cm(-2).

237 a reversible capacity of 466 mAh g(-1) at a current density of 50 mA g(-1) .

238 formate with nearly 100 % selectivity and a current density of 56.7 mA cm(-2) in the presence of 5 %

239 A current density of 65.8 mA.cm(-2) at -1.8 V vs. Ag/Ag(+)

240 w in neutral media (60 per cent at a partial current density of 7 milliamperes per square centimetre

241 ode (RHE), with a FE for formate of 96 % and current density of 8.87 mA cm(-2) at low potential of -0

242 y selective GOD-based SECM tip showed a high current density of 94.44 (+/-18.55) muA.mM(-1).cm(-2) fr

243 lts across a 7-micrometre-thick film, with a current density of around 17 microamperes per square cen

244 ugh a general kinase inhibitor increased the current density of BdALMT12, a calmodulin (CaM) inhibito

245 C1 in HEK293 cells significantly reduced the current density of heterologously expressed Kv4.3, Kv1.5

246 gen electrode (RHE) for the electrocatalytic current density of j = -10 mA cm(-2) , and a Tafel slope

247 ve ion accessibility and decreases the local current density of Li anode.

248 ntial of 322 mV at 10.2 mA cm(-2) and a high current density of more than 300 mA cm(-2) at 1.7 V(NHE)

249 Measurements of current density of SAMs of linear length-matched hydroca

250 port of majority carriers to reduce the dark current density of the device.

251 stray fields directly influence the critical current density of the superconducting film.

252 Finally, the short-circuit current density of the two-terminal tandem organic photo

253 performance and yield, delivering a high ON-current density of up to 900 microamperes per micrometre

254 cycled at room temperature with a practical current density of ~0.2 C.

255 lso describe the dependence of the H2 and CO current densities on cathode voltage that are in strikin

256 erface, the composite electrode displays HOR current densities over 8-fold larger than the diffusion-

257 an regulate SUMOylation to reconfigure ionic current densities over minutes, and this regulation was

258 ronic menthol treatment failed to change the current density (peak current amplitude/cell capacitance

259 i-O(2) battery operations with a record-high current density per catalyst mass loading of 2000 mA g(c

260 centrations of lithium carbonate, and higher current density promotes CNS growth while suppressing CN

261 e potential at + 0.27 V and variable plateau current densities ranging from - 1 to - 22 uA cm(-2) (n

262 operties such as activation energy, exchange current density, rate capabilities, cycle life, etc. hav

263 Most significantly, its current density reaches ~288 mA cm(-2) at -0.61 V versus

264 Current densities recorded in the kinetic region of cath

265 Moreover, current densities, related to catalytic reaction rates,

266 This finding highlights that current densities required for spin-orbit torque switchi

267 om large energy dissipation due to the large current densities required.

268 n properties of the resulting Na(+) membrane current densities revealed reduced maximum currents and

269 D and TRPM8, showing that a reduction in IKD current density shifts the thermal threshold to higher t

270 ng why these biofilms fail to produce higher current densities suggest inhibition by formation of pH,

271 ribution has a more than 30% higher critical current density than a homogeneously disorder supercondu

272 MoS2 flakes exhibit much higher mobility and current density than mechanically exfoliated ML flakes d

273 devices exhibited the maximum IQE at a lower current density than the smaller devices, and the IQE ha

274 hode that can deliver greater power, at high current densities, than a Pt cathode.

275 eparation, which boosts carrier mobility and current density, thus improving the device performance.

276 gn capable of delivering high power at a low current density to increase the therapeutic range of rad

277 age-clamp analysis revealed increased Ca(2+)-current density under specific experimental conditions.

278 formance, the smaller LEDs provided a larger current density under the same voltage and presented a s

279 (Faradaic efficiency FE(CO) = 85%) with high current densities up to -17.3 mA cm(-2) as a composite w

280 ining over 1000 h of Li stripping/plating at current densities up to 0.6 mA.cm(-2).

281 beit to a reduced extent, at CO(2) reduction current densities up to 150 mA/cm(2).

282 hieved >90% selectivity for pure H(2)O(2) at current densities up to 200 milliamperes per square cent

283 of approximately 75% and high short-circuit current densities up to 42.1 mA cm(-2).

284 ell shows an excellent cyclability at a high current density up to 0.6 mA cm(-2) A solid electrolyte

285 ll voltage hysteresis and endures a critical current density up to 1.0 mA cm(-2) .

286 10(5) S m(-1) and an extraordinary breakdown current density up to 3.9 x 10(7) A cm(-2) , while the s

287 a stable amperometric curve and an excellent current density value over a duration of 10 h.

288 The dark current density versus bias (JV) response of nitroazoben

289 furreducens inoculated BESs, and the maximum current density was 4.10 +/- 0.02 mA cm(-2), which is 8-

290 The steady-state current density was kept at 11.0 +/- 1.3 mA/m(2) in a mi

291 0.04 versus 0.2+/-0.002 A(2); P<0.0001), the current density was lower (9.6+/-0.9 versus 16.9+/-0.09

292 The current density was maintained for >200 min at a constan

293 KATP current density was significantly reduced by H(2)O(2) in

294 tive neuronal GABA(A)R expression since GABA current density was unaffected in hippocampal neurons, a

295 Computer simulation of an electrolyte current density was used to investigate several potentia

296 t extends upward from the jump onset, with a current density well below that of lightning leaders.

297 h as high Ca(2+) selectivity, an increase in current density when switching from a Ca(2+)-containing

298 ing in the BZ was modeled by reducing sodium current density, whereas structural conduction slowing w

299 jection, and excellent scaling of the output current density with device dimensions.

300 Modeled stimulation threshold current density with honeycombs does not increase substa