ライフサイエンスコーパス: current density

1 ging the optical pump intensity or injection current density.

2 mately 99% over hundreds of cycles at a high current density.

3 y, activation of Wnt/beta-catenin reduces BK current density.

4 electrical and physical breakdown under high current density.

5 electivity but at high overpotential and low current density.

6 of wild-type RyR1 partially restored L-type current density.

7 g galvanostatic polarization at a predefined current density.

8 RPV1, despite similar or even reduced sodium current density.

9 ion, cell efficiency, cycling stability, and current density.

10 can be easily regulated by adjusting pulsed current density.

11 and exogenous channel blockers, and on NMDA current density.

12 d thereby greatly enhance the Nb3Sn critical current density.

13 ransfer rate (kS) and a maximum biocatalytic current density.

14 differences in cold-induced TRPM8-dependent current density.

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

16 s associated with significantly lower sodium current density.

17 ristics to the microhole and generate higher current densities.

18 mise electro-luminescence efficiency at high current densities.

19 eased with increasing applied potentials and current densities.

20 s of cycles of charge and discharge at fixed current densities.

21 ance to lithium dendrite growth even at high current densities.

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

23 show tremendous improvement in amorphization current densities (0.13-0.6 MA cm(-2)) compared with the

24 with 150 mM NaCl), higher glucose oxidation current densities, 0.41 mA cm(-2), are obtained from enz

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

26 rated by 10 h of stable operation with C2-C3 current density 10 mA/cm(2) (at -0.75 V), rendering it a

27 fficiency exceeding 80% at considerably high current densities (100 mA cm(-2)).

28 by H(ad) recombination, results in the high current density [200 mA/cm(2) at an overpotential of 0.3

29 ides excellent morphological control at high current densities (3-5 mA cm(-2) ) for Li and even for n

30 [5], p<0.0001) and a significant decrease in current density (42 pA/pF [19] vs 61 [20], p=0.044).

31 To achieve large current densities, a nanostructured TiO2 scaffold, proce

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

33 ctor layer is required to inject the maximum current density across the contact.

34 of metal dissolution with applied potential/current density allows for narrowing down suitable mater

35 wafers, indicating by the lowest passivation current density among silica, citric acid and hydrogen p

36 NMR, diamagnetic susceptibility exaltation, current density analyses (CDA) and nucleus independent c

37 ofilm growth with three times higher maximum current densities and about 6.9 times thicker biofilms c

38 We accurately predict current densities and chart functional redundancy.

39 ting' processes which require lower critical current densities and faster writing and reading speeds.

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

41 ygenates at high Faradaic efficiencies, high current densities and low overpotentials.

42 Higher current densities and non-abrasive brushes produce rough

43 The short-circuit current densities and power conversion efficiencies unde

44 The correlation between current densities and VFA concentrations was first evalu

45 o linear relationships were observed between current densities and VFA levels from 1 to 30 mM (0.04 t

46 the sunlight-driven evolution of CO at large current densities and with high selectivity.

47 , the engraved Co3 O4 exhibits a much higher current density and a lower onset potential.

48 epared Ag-CoSe2 nanobelts exhibited a higher current density and a lower Tafel slope towards OER.

49 ne, while also showing a 10-fold increase in current density and a significant change in Tafel slope.

50 ances of this primary ion source in terms of current density and achievable lateral resolution have b

51 Both current density and brush material have a significant im

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

53 ested associations between resting state EEG current density and endophenotypes of interest.

54 result in a greatly increased short-circuit current density and fill factor, as a result, enhanced p

55 e broad linear relationship between the peak-current density and glucose concentration from 2 to 15mM

56 CaValpha2delta increases the peak current density and improves the voltage-dependent activ

57 ealed a complex phenotype, including loss of current density and inactivation in combination with inc

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

59 ormone-induced up-regulation of BKCa channel current density and NS1619-mediated relaxations, which w

60 exhibited normalized pyramidal neuron sodium current density and reduced hippocampal NaV1.6 protein l

61 promotes KV1 channel endocytosis, reduced KV current density and restored myogenic responses in PAs f

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

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

64 The influence of bath load, current density and the brush material used was investig

65 However, this approach is limited by low current density and the need for rectification (2) .

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

67 aValpha2delta1-mediated increase in the peak current density and voltage-dependent gating of CaV1.2.

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

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

70 displays decreased membrane localization and current density, and reduces neuronal excitability.

71 nal hyperexcitability, suppressed the sodium current density, and right-shifted the V1/2 of the inact

72 implications for pinning phenomena and high current density applications.

73 These current densities are leading to an exceptional acetate

74 Notch-induced changes in K(+) current density are regulated at least in part via trans

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

76 The current densities as functions of time for both diodes s

77 Taking the potential at a certain current density as a measure of the relative rate of the

78 y with full recovery even after cycled under current density as high as 10 A g(-1).

79 des can generate a DC voltage with an output current density as high as 218.6 muA cm(-2) upon mechani

80 , or coating) to obtain long cycle life with current density as high as 9 A g(-1) for hundreds of cha

81 ents that demonstrated increased L-type VGCC current density as well as increased mRNA expression of

82 ith pure water splitting to achieve the same current density, as well as exhibiting robust stability

83 Notch activation decreases peak outward K(+) current density, as well as the outward K(+) current com

84 ificant enhancements in the electrocatalytic current densities at the electrode.

85 -2) and 53.1 mA cm(-2) for maximum power and current density at 323 K, respectively.

86 It was found that an electrolyte current density at an edge tip structure near the workin

87 ate an ultrahigh activity with 200 mA cm(-2) current density at only 206 mV overpotential using a car

88 llumination occurs at 0.95 V vs RHE, and the current density at the reversible potential for water ox

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

90 environment, we found that reducing hCaV3.3 current densities by 22% or more eliminates rebound burs

91 t is shown that these effects may modify the current density by orders of magnitude from the widely u

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

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

94 that a remarkable reduction in the critical current density can be achieved for in-plane magnetised

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

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

97 ne wastewater over variable treatment times, current densities, chloride concentrations, and anode ma

98 he relationship between the increases in the current density collected by the bioanode to the decreas

99 f 1.1 x 10(13) cm(-2) show ~382 times higher current densities compared to the control sample embedde

100 d a net improvement in terms of primary beam current density compared to the commonly used duoplasmat

101 Scn2b null atria had normal levels of sodium current density compared with wild type.

102 +/- 0.42 mS/cm, indicating that the maximum current density could be as high as 270 A/m(2) if only O

103 mic vortex states of superconductors at high current densities, crucial for many applications.Ultrafa

104 hypoxia significantly inhibited BKCa channel current density, decreased NS1619-induced relaxations an

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

106 To deduce the current density distribution, finite-element models were

107 se that is ascribed to the redistribution of current densities due to spin accumulation inducing coup

108 n the probability of void formation when the current density exceeds half of the maximum value.

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

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

111 s from septic mice the presence of defective current densities for Ik1, l-type calcium channel, and N

112 Enhanced current densities for mediated O2 reduction are observed

113 at 350 degrees C, the surface-area corrected current density for CO reduction is 44-fold lower and th

114 We estimated intracranial current density for standard EEG frequency bands in 82 u

115 ction with relatively stable selectivity and current density for up to 16 h, which is one of the best

116 Here we show that the short-circuit current density from SS-OPV devices can be enhanced sign

117 considerably greater than that obtained from current density-functional theory approximations and fro

118 pe (SEM) field emission gun, our tip shows a current density gain that is about 1,000 times greater t

119 tunable syngas production while maintaining current densities greater than 20 mA/cm(2).

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

121 The resulting VFETs possess high on-state current densities (>3000 A cm(-2) ) and on/off current r

122 molecular oxygen saturated electrolyte with current densities higher than 1.0 mAcm(-2) at 0.0 V.

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

124 This paper explores tunneling current densities in self-assembled monolayer (SAM)-base

125 We observed reduced sodium and potassium current densities in ventricular myocytes, as well as co

126 n potential and an increase in the corrosion current density in the presence of the P. aeruginosa bio

127 ed with increased resting gamma (36.5-44 Hz) current density in the ventral (subgenual) anterior cing

128 g Mg deposition/dissolution with high CE and current density in these PEGylated IL media.

129 nel beta1 subunit abundance and BKCa channel current density in uterine arteries from pregnant sheep

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

131 h the zero-order dependence of Pi on the OER current density; in contrast, Bi exchange is sufficientl

132 it coupling (SOC) materials convert a charge current density into a spin current density which can be

133 ovide an optimal surface coverage, a uniform current density into and/or from a substrate, and a mini

134 with high selectivity, efficiency, and large current densities is a critical step on the path to prod

135 Alteration in the L-type current density is one aspect of the electrical remodeli

136 oltage (Voc) of 0.39 mV, and a short-circuit current density (Isc) of 12.2 mA/cm(2) were obtained.

137 applications is the low engineering critical current density J e because of the low superconductor fi

138 l ester chain, we observe an increase in the current density J of a factor of 35 at 1 V when the clos

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

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

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

142 oltage (V(oc)) of 929 mV and a short-circuit current density (J(sc)) of 9.42 mA/cm(2) from the n = 3

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

144 We demonstrate that for H//c critical current density Jc at high temperatures is dominated by

145 The critical temperature Tc and the critical current density Jc determine the limits to large-scale s

146 The anisotropy of the critical current density Jc is both influenced by the Hc2 anisotr

147 In general, the critical current density, Jc, of type II superconductors and its

148 transepithelial potential (TEP) and electric current densities (JI) during regeneration.

149 ial areas, affording increased short-circuit current densities (Jsc).

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

151 light harvesting and enhancing short-circuit current density (JSC ).

152 nowire top contacts attained a short-circuit current density (Jsc) of 13.9 mA/cm(2) and a fill factor

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

154 ding to significantly improved short circuit current density (Jsc) value.

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

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

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

158 method at the CHF/6-31G** level to calculate current-density maps.

159 icient devices has been hampered by the high current densities needed to initiate domain wall motion.

160 ined over a pH range of 5.4-8.3, with higher current densities observed at higher pH values.

161 ible for the observed odd-even effect in the current densities obtained by J(V) measurements).

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

163 xhibits a high capacitance of 1360 Fg(-1) at current densities of 10 Ag(-1) after 3000 cycles and an

164 an electrocatalyst at both electrodes gives current densities of 10 and 100 mA cm(-2) at potentials

165 ward hydrogen evolution in alkali, achieving current densities of 10 and 20 mA cm(-2) at overpotentia

166 r activity for hydrogen evolution, achieving current densities of 10 mA cm(-2) and 100 mA cm(-2) at o

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

168 able emission wavelength, very low threshold current densities of 29-33 A/cm(2) are achieved.

169 Current densities of approximately 1 mA/cm(2) over 30-h

170 ust platforms for CO evolution, with partial current densities of jCO = 5-8 mA/cm(2) at applied overp

171 At -5 V reverse bias, the dark current densities of the diodes were measured to be (347

172 ry high aspect ratios of more than 200 using current densities of the order of 10(8) A/m(2).

173 e macroporous electrodes, the device reached current densities of up to 0.68 mA cm(-2) at 0.5 V vs RH

174 moval of evolved oxygen bubbles even at high current densities of up to 250 mA/cm(2).

175 DEMS) cell geometry that enables the partial current densities of volatile electrochemical reaction p

176 ly high temperature, which for a typical arc current density of 100 A/cm(2), is above the boron melt

177 The highest bioelectrocatalytic current density of (597+/-25)muAcm(-2) and the highest G

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

179 ated using the mass of phosphorus only) at a current density of 0.05 A g(-1) and an 83% capacity rete

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

181 tripping/plating at room temperature, with a current density of 0.2 mA/cm(2) for around 500 h and a c

182 e/discharge cycles and ca. 7h at a discharge current density of 0.2mAcm(-2).

183 tric capacitance of ca. 773.6 F g(-1) ) at a current density of 0.5 A g(-1) while maintaining excelle

184 uch higher capacitance of 527.9 F g(-1) at a current density of 0.5 A g(-1), compared with ~247 F g(-

185 nsity of 0.2 mA/cm(2) for around 500 h and a current density of 0.5 mA/cm(2) for over 300 h.

186 ed optimal immobilization of MtrC and a high current density of 1 mA cm(-2) at 0.4 V vs SHE could be

187 hibits the highest eta (0.68 V) for OER at a current density of 1 mA/cm(2).

188 tained is as high as 530 m/s at a reasonable current density of 1 x 10(12) A/m(2) for device applicat

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

190 decreasing its overpotential by 150 mV at a current density of 1.0 mA/cm(2) after coating its surfac

191 iocatalyst to generate the maximum power and current density of 1.0microW/cm(2) and 6.3microA/cm(2),

192 c activity in alkaline solution, providing a current density of 1.33 mA/cm(2) at an overpotential of

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

194 ll voltage of only about 1.53 V to achieve a current density of 10 mA cm(-2) and maintains its activi

195 for the hydrogen evolution reaction, with a current density of 10 mA cm(-2) at a low potential of -1

196 r both HER and OER in alkaline media, with a current density of 10 mA cm(-2) at overpotentials of -94

197 ieved with a low overpotential of 96 mV at a current density of 10 mA.cm(-2) and a Tafel slope of 78

198 re, we show in nanowires that under the high current density of 10(8)-10(9) A m(-2), the THE decrease

199 nanotubes per micro-meter is achieved with a current density of 10.08 muA mum(-1) at VDS = -1 V.

200 r lithium ion battery was 480 mAh.g(-1) at a current density of 100 mA.g(-1), and retained 84% capaci

201 croW/cm(2) at 166.3 mV, respectively, with a current density of 100 microA/cm(2).

202 mA h g(-1) under a high charge and discharge current density of 12 000 mA g(-1) over approximately 40

203 A short circuit current density of 12.0 mA/cm(2) is achieved in 210 nm t

204 ental MFC has been observed at corresponding current density of 1444.44 mA/m(2) and 1777.77 mA/m(2).

205 and extraordinary catalytic activity with a current density of 15.0 mA cm(-2) and a turnover frequen

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

207 be modulated into a good Ohmic contact with current density of 18.7 +/- 0.6 A/cm(2) and 10.4 +/- 0.4

208 d that tungsten diselenide nanoflakes show a current density of 18.95 milliamperes per square centime

209 e dinucleotide (NAD(+)) generating a maximum current density of 1muAcm(-2) with 10mM NAD(+) leads to

210 erial gain of approximately 1500 cm(-1) at a current density of 2 kA cm(-2).

211 ulombic efficiency (99% over 400 cycles at a current density of 2 mA cm(-2)).

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

213 microW/cm(2) at 335 mV, respectively, with a current density of 202.2 microA/cm(2).

214 ircuit voltage of 428.67 mV, a short-circuit current density of 24.28 mA cm(-2), and a fill factor of

215 e can be discharged as a supercapacitor at a current density of 2mAcm(-2) providing a maximum power d

216 g/stripping overpotential (<90 mV) at a high current density of 3 mA/cm(2) over 80 cycles.

217 afel slope of 98 mV per decade, and exchange current density of 3.9x10(-2) mA cm(-2) .

218 When fed with 4 M NaCl, the MDC achieve a current density of 300 A m(-3) (anode volume), which was

219 1000 cycles without obvious decay at a high current density of 3000 mA g(-1) .

220 circuit voltage of 547.7 mV, a short-circuit current density of 33.2 mA/cm(2), and a fill factor of 7

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

222 tage of only 0.64 V is needed at the typical current density of 4 kA m(-2) , leading to a low energy

223 city of 1068 mAh g(-1) after 100 cycles at a current density of 400 mAg(-1).

224 e than 100 cycles is achieved even at a high current density of 5 mA cm(-2) in both carbonate and eth

225 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

226 the capacity increases to 567 mAh g(-1) at a current density of 50 mA g(-1) , which is the highest ca

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

228 oxygen evolution reaction, which requires a current density of 500 mA/cm(2) at an overpotential belo

229 The bioanode generated the current density of 510microAcm(-2) at pH 7.0 and 0V vs.

230 le electron barrier design results in a dark current density of 6.3 x 10(-6) A/cm(2) at 77 K.

231 power density of 122 +/- 5 muWcm(-2) with a current density of 657 +/- 17 muAcm(-2) and an open circ

232 fel slope of 45 mV dec(-1) , higher exchange current density of 8.6x10(-4) A cm(-2) , and long-term s

233 Tafel slope of 49 mV per decade and exchange current density of 9.62 x 10(-3) mA cm(-2), performing a

234 Coulombic efficiency approximately 98%, at a current density of 99 mA g(-1) (0.9 C) with clear discha

235 ell was 4nW at a voltage of 260mV and with a current density of 9muAcm(-2).

236 photoelectrode mediates H2 production with a current density of approximately 9 mA cm(-2) at a potent

237 lectron recovery in the form of acetate at a current density of around -200 A m(-2).

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

239 The maximum power density and current density of the biobattery catalyzed by the mutan

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

241 The anodic current density of the metal film increased, while the e

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

243 hich produces peak output voltage of ~370 V, current density of ~12 muA . cm(-2), and average power d

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

245 higher potential than on AuNPs/gr; (ii) the current density on AuNPs/gr was 2.4 times higher than on

246 con, the tunneling transistors can deliver a current density over 20 A cm(-2) .

247 deterministic magnetization reversal at low current densities, paving the road towards ultralow-diss

248 d the formation was attributed to decreasing current density radially inward on the silicon surface e

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

250 ith strongly contracted positive column with current densities reaching 10(3) A/cm(2).

251 Current densities recorded in the kinetic region of cath

252 that are completely fixed by the macroscopic current density relation and compressibility matrix of t

253 factor of 33 (mass activity) or 21 (exchange current density) relative to unsupported nickel nanopart

254 ability testing, the negligible variation of current density remains exsisting after 1000 electrochem

255 Although current densities reported here need further improvement

256 However, the current density required for the spin-transfer torque is

257 ents; and this translates to large switching current densities, responsible for chemical segregation

258 nium oxide species, and correlate these with current densities resulting from proton reduction.

259 city of approximately 530 mAh.g(-1) when the current density returned to 100 mA.g(-1) after continuou

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

261 The anisotropy of the critical current density shows a complex behavior whereby additio

262 This relatively high current density significantly affects the devices' struc

263 Metallic nanosheets exhibited a much higher current density, smaller onset potential and stronger du

264 significantly larger menthol-induced inward current densities than medium-large cells, most of which

265 But such components have a much higher current density than 2- or 3-dimensional films, and high

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

267 AnEMBR (TSS = 17 mg/L), likely due to higher current densities that minimized the accumulation of cel

268 yanide (CN) or the known opener P1075 with a current density that was ~8-fold smaller than adult; The

269 Such high engineering critical current density, the highest value ever observed so far,

270 The porous electrode reduces the effective current density; thus, flat voltage profiles and stable

271 The measured critical current density to set these walls in motion, detected u

272 pseudo-myasthenia caused by a marginal Na(+) current density to support sustained high-frequency acti

273 nce, shunt resistance and catalytic exchange current density-to account for imperfect light absorptio

274 esence of a photonic band gap, low threshold current density, unconventional angular emission and opt

275 The device could be discharged at current densities up to 2mAcm(-2) supplying a maximum in

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

277 free and stable cycling over 300 cycles with current densities up to 5 mA/cm(2).

278 for the high silicon utilization under high current densities (up to 4C).

279 ciency of 20.15% is achieved with negligible current density-voltage hysteresis.

280 ould be measured by constructing a plot of 1/current density vs 1/mass transfer rate from the series

281 Subsequently, a linear plot of (1/current density) vs 1/m at different potentials can be c

282 The steady-state current density was 0.82 +/- 0.03 A/m(2) in a miniature

283 Similarly, Kv current density was 25% greater in ventricular myocytes

284 siological temperature indicated that the Na current density was 62% lower in BCs, and the voltage de

285 l temperature, the maximal sustained outward current density was almost three times the mean value ob

286 Sodium current density was half that of wild-type muscle and no

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

288 Current density was lowest for the TFE and SPE surfaces

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

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

291 1) were also downregulated (P<0.05), but the current densities were much lower than for Ito.

292 th infrared photodetectors with reduced dark current density were demonstrated.

293 with Cav1.4 had no significant influence on current density when examined with BaCl2 as the charge c

294 wed fast turn-on transients and increases in current density when illuminated with X-ray photons of e

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

296 convert a charge current density into a spin current density which can be used to switch a magnet eff

297 ) A m(-2), the THE decreases with increasing current densities, which demonstrates the current-driven

298 ectrodes with a geometry which offer greater current density while keeping the overall footprint of t

299 lecular design, we are able to suppress dark current density while retaining high responsivity in an

300 uces defects, resulting in a remarkably high current density with a high rectification ratio, as well