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1 nd low-Na(+) solutions were determined under open circuit.
2 tons exceeding the semiconductor band gap at open circuit.
3 amounts released when the EBFCs were held at open circuit.
4 and leg blood flow ( QL ) were measured via open-circuit acetylene wash-in technique and constant in
7 of complementary electrochemical techniques: open-circuit chronopotentiometry (CP), linear polarizati
10 pithelial potentials (V(t)) were recorded in open circuit conditions while applying constant current
11 borated between freshly prepared, aged under open circuit conditions, and cycled electrodes of compos
14 (98.6% reduction), which was similar to the open circuit control and degraded regardless of the reco
18 ricidal properties, compared to the control (open-circuit) diffusate, and reduced observable biofilm
19 y is produced by simple solution exchange in open circuit, due to the associated decrease in the capa
22 ing substantially enhance the voltage of the open-circuit, i.e., from 140 mV (1-cylinder thermocell)
24 folding geometry that generates 110 volts at open circuit or 27 milliwatts per square metre per gel c
27 rmed g-C(3)N(4), in particular generating an open circuit photovoltage as high as 1.3 V, while C(3)N(
31 ot intentionally doped and showed a positive open-circuit photovoltage based on photoelectrochemical
32 2, BQ (2 mM), BQ(*-) (2 mM)/carbon, shows an open-circuit photovoltage of 1.05 V and a short-circuit
33 t-circuit photocurrent J(sc)= 16.1 mA/cm(2), open-circuit photovoltage V(oc) = 0.631 V, and a fill fa
34 ty of the cyclometalated compound, while the open-circuit photovoltage was significantly larger for t
36 w fundamental energy losses; it can generate open-circuit photovoltages of more than 1.1 volts, despi
37 e to the anode (63.5-78.7%) than that in the open circuit positive controls (37.6-43.4%) during a per
38 electrochemical technique incorporating both open circuit potential (OCP) and amperometric techniques
39 affect significantly the measurement of the open circuit potential (OCP) and cyclic voltammetry (CV)
40 de of 25 mV, a frequency of 81.3 kHz, and an open circuit potential (OCP) as the direct-current (dc)
45 the development of the third-generation type open circuit potential (OCP) principle-based glucose sen
48 e absence of external electrical power), the open circuit potential (OCP), the formation of struvite
52 rbed-accumulated on the electrode surface at open circuit potential and then stripped off by applying
53 ted specific ROS activity was lowest for the open circuit potential condition, elevated when cathodic
54 easurements) or the passive tracking (during open circuit potential decay) of the quasi-Fermi level i
57 rrent density of 657 +/- 17 muAcm(-2) and an open circuit potential of 0.57 +/- 0.01 V, which is suff
58 he enzymatic biofuel cell (EFC) generated an open circuit potential of 0.61 (+/-0.02) V with a maximu
59 photocurrent density of 35 mA cm(-2) and an open circuit potential of 450 mV; there was no observabl
61 of two hydroxy groups to AQDS increases the open circuit potential of the cell by 11% and we describ
63 ntials of the EABs with the solution pH: (i) open circuit potential, (ii) half-wave potential, and (i
64 plying AC amplitude of 50 mV at 117.2 Hz and open circuit potential, a minimum of 214 captured cells/
71 e containing 0.01 M KTFAB, had a very stable open-circuit potential and an outstanding potential repr
72 electrochemical impedance analysis (EIS) and open-circuit potential decay transients (OCVD), which at
75 ed on the electrochemical measurement of the open-circuit potential of the platinum electrode immerse
76 OS was adjusted by polarization to the known open-circuit potential of the solid contact in 0.1 M KCl
77 H2O2 was estimated by measuring the H(+)/H2 open-circuit potential under the reaction conditions.
78 SAED, EDX, XPS, UV-visible spectroscopy, and open-circuit potential versus time experiments to unders
80 low established fade rates that also exhibit open circuit potentials of 1.0 V or higher and transferr
83 Through electrochemical testing including open circuit potentials, potentiodynamic scans, anodic p
84 nadium, or nickel, 10 to 30 nm thin, produce open-circuit potentials of several tens of millivolt and
87 hat the methodology compares well to that of open circuit potentiometry, despite giving complementary
89 volves a short (1 s) galvanostatic pulse, an open-circuit pulse (0.5 s) during which the EMF of the c
92 approximately 1.7microWcm(-2)) with similar open circuit voltage (0.27V) compared to native GOX when
95 rated for 450 h and results indicated a high open circuit voltage (about 810 mV) compared with previo
96 arn generated a 2.8-fold higher peak-to-peak open circuit voltage (OCV) and a 1.5-fold higher peak po
97 r density of 2.3microWcm(-2) at 0.21V and an open circuit voltage (OCV) of 0.49V were registered as a
100 ,1-diylidene))dimalononitrile) decreases the open circuit voltage (V(OC)) but increases the short cir
103 at PIPCP:PC61BM blends yield devices with an open circuit voltage (V(oc)) of 0.86 V, while maintainin
104 a good average PCE of 8.26% with an average open circuit voltage (V(oc)) of 1.79 V for 2-terminal ta
105 In contrast to previous reports where the open circuit voltage (V(OC)) of a conventional, blended
106 the [Co(bpy)(3)](2+/3+) redox couple, and an open circuit voltage (V(oc)) of almost 1.0 V at 100% sun
107 rstand the impact of these fluorine atoms on open circuit voltage (V(oc)), short circuit current (J(s
108 ueisser limit, but they suffer from a larger open circuit voltage (VOC ) deficit than narrower bandga
109 uit current density (Jsc) of 18.53 mA/cm(2), open circuit voltage (Voc) of 0.538 V, and fill factor (
115 ncentration (5mM), the biofuel cell exhibits open circuit voltage and power density of 302.1 mV and 1
116 45 mM glucose, the biofuel cell exhibited an open circuit voltage and power density of 681.8 mV and 6
117 o higher short-circuit current, fill factor, open circuit voltage and significantly reduced device-to
119 groups on the anion significantly alters the open circuit voltage and yields a clear dependence on el
120 designs must be developed that maximize the open circuit voltage by minimizing both non-radiative an
121 ultant FeS-based enzyme electrode reached an open circuit voltage closer to its standard potential un
122 current density versus applied potential and open circuit voltage decay measurements were employed to
123 While the electrical power output and the open circuit voltage decreased with increasing temperatu
128 exhibited the following characteristics: an open circuit voltage of 0.54 V, a maximal power density
129 all known all-carbon-based materials with an open circuit voltage of 0.59 V and a power conversion ef
132 of-concept of a membrane-free battery has an open circuit voltage of 1.4 V with a high theoretical en
133 achieved a high efficiency of 6.63% with an open circuit voltage of 428.67 mV, a short-circuit curre
135 y levels, which can potentially maximize the open circuit voltage of bilayer organic solar cells.
138 nce efficiency measurements indicate that an open circuit voltage of up to 930 mV can be achieved, on
140 We show the FEC condenses on the surface at open circuit voltage then is reduced to C-O containing p
144 The enzymatic fuel cell reaches 0.5 V at open circuit voltage with both, ethanol and methanol, wh
145 perovskite have the benefit of retaining an open circuit voltage ~0.14 V closer to its radiative lim
147 taic device is fabricated to produce a large open circuit voltage, 0.85-0.95 V, which is higher than
148 d as the offset between optical band gap and open circuit voltage, and compare the results to those o
150 rs including photovoltaic device efficiency, open circuit voltage, fill factor, and short circuit cur
151 he device performance by mainly limiting the open circuit voltage, interfacial layers are also crucia
153 results from synergistic effects of enlarged open circuit voltage, suppressed trap-assisted recombina
154 ere analysed in response to temperature: the open circuit voltage, the maximum output power and the i
158 erials, we derive an empirical limit for the open circuit voltage: V(OC) less, similar E(opt,min)/e -
161 ted backbone led to a 19% enhancement in the open-circuit voltage (0.735 V) vs poly(3-hexylthiophene)
162 circuit current (10.14 mA/cm(2)) with a high open-circuit voltage (0.86 V) to give a power conversion
163 combinatorial studies and demonstrate record open-circuit voltage (V OC) of 970 mV and efficiency of
164 d (PLQY) measurements show that nonradiative open-circuit voltage (V(OC) ) losses outweigh radiative
165 atio of the three components was varied, the open-circuit voltage (V(oc)) increased as the amount of
166 hose of the individual "subcells", while the open-circuit voltage (V(oc)) is between those of the "su
167 form is more basic than the Sp form, and the open-circuit voltage (V(oc)) is related to the proton co
168 t-circuit photocurrent of 19.0 mA cm(-2), an open-circuit voltage (V(OC)) of 0.71 V, and a fill facto
169 .2% (the highest PCE of 6.8%), along with an open-circuit voltage (V(oc)) of 0.93 +/- 0.02 V, a short
170 significantly suppressed to result in a high open-circuit voltage (V(OC)) of 1.17 V and a reduced V(O
171 conversion efficiency of 4.02%, featuring an open-circuit voltage (V(oc)) of 929 mV and a short-circu
172 ) (>0.57) at all fullerene ratios, while the open-circuit voltage (V(oc)) was found to vary from 0.61
173 ties for the two dyes, a consistently higher open-circuit voltage (V(oc)) was measured for Dye-S rela
174 molecules that are shown to tune the output open-circuit voltage (VOC) across three types of pristin
175 rformed better than RSQ1 owing to its higher open-circuit voltage (Voc) and fill factor (ff) in spite
176 ad to enhanced efficiencies due to increased open-circuit voltage (VOC) and improved absorption of so
177 high photocurrent generation, the achievable open-circuit voltage (Voc) is fundamentally limited due
178 ectric conversion efficiency (eta) of 2%, an open-circuit voltage (Voc) of 0.39 mV, and a short-circu
179 , which induce a simultaneous enhancement in open-circuit voltage (Voc), short-circuit current (Jsc),
180 isible and infrared light, we measure a d.c. open-circuit voltage and a short-circuit current that ap
181 of sterics and molecular orientation on the open-circuit voltage and absorbance properties of charge
185 bricate core-shell nanowire solar cells with open-circuit voltage and fill factor values superior to
186 10.3 to 11.7 mA cm(-2) (while retaining the open-circuit voltage and fill factor) to result in an en
190 ing the intensity dependence of the external open-circuit voltage and the internal quasi-Fermi level
191 :InI(3) and carbon electrode exhibit PCE and open-circuit voltage as high as 12.04% and 1.20 V, respe
192 provide both high short-circuit current and open-circuit voltage at room temperature, and be driven
193 maximum, our focus is on efforts to increase open-circuit voltage by means of improving charge-select
195 ethylene)malononitrile leads to an increased open-circuit voltage compared with its isomer 2-((7-(N-(
201 Pb-exposed surface, resulting in an improved open-circuit voltage from 1.10 V to 1.16 V after passiva
204 as been speculated to contribute to the high open-circuit voltage in several types of high efficiency
212 short-circuit current of 1.3 muA and a large open-circuit voltage of 0.61 V under visible light illum
213 ell voltage of 0.52 V and in human blood; an open-circuit voltage of 0.65 V, a maximum power density
214 e BFC were obtained: in phosphate buffer; an open-circuit voltage of 0.68 V, a maximum power density
215 ort-circuit current values of 14.2 mA/cm(2), open-circuit voltage of 0.7 V, and a broad external quan
216 arbon nanotube yarn biofuel cells provide an open-circuit voltage of 0.70 V, and a maximum areal powe
217 f up to 9.58% with a fill factor of 0.63, an open-circuit voltage of 0.73 V, and a very high short-ci
218 , a short-circuit current of 14 mA/cm(2), an open-circuit voltage of 0.74 V, and a fill factor of 58%
219 conversion efficiency of 20.09% with a high open-circuit voltage of 0.88 V, a fill factor of 79.74%,
220 Corresponding solar cells featured a high open-circuit voltage of 0.9 V, a fill factor around 0.6,
221 conversion efficiency of 7.03% with a large open-circuit voltage of 0.95 V without using any additiv
224 wer conversion efficiency of over 14% and an open-circuit voltage of 1.06 V measured under reverse vo
225 onversion efficiency approaching 13% with an open-circuit voltage of 1.10 V, short-circuit current de
227 PEA=C6H5(CH2)2NH3(+), MA=CH3NH3(+)) show an open-circuit voltage of 1.18 V and a power conversion ef
228 or blade-coated PSCs is demonstrated with an open-circuit voltage of 1.18 V, corresponding to a very
229 ng interface defects, the device exhibits an open-circuit voltage of 1.20 V and an efficiency of 3.97
230 iency of 21.9% for blade-coated PSCs with an open-circuit voltage of 1.20 V, corresponding to a recor
231 dal perovskite QD photovoltaic cells with an open-circuit voltage of 1.23 volts and efficiency of 10.
232 ptimum CsBr/KBr treatment demonstrate a high open-circuit voltage of 1.3 V, responsivity of 10.1 A W(
233 in the inorganic perovskite, yielding a high open-circuit voltage of 1.33 V and an external quantum e
234 ptide-based power generator that produces an open-circuit voltage of 1.4 V and a power density of 3.3
237 The prototype device provides a peak-to-peak open-circuit voltage of 157 V and instantaneous short-ci
238 drop of 400 muL alone could generate a peak open-circuit voltage of 42 V under a 0.25 Hz vibration.
240 ort-circuit current of 32.6 pA mm(-2) and an open-circuit voltage of 78 mV, providing for a maximum p
242 r-conversion-efficiency of 7.26% with a high open-circuit voltage of approximately 1 V and a striking
244 e from 3.56 to 3.37 A and an increase in the open-circuit voltage of cells from 60 mV to 2.10 V after
246 esence reduces the short-circuit current and open-circuit voltage of solar cells based on blends of P
249 lecular orbitals to be tuned to maximize the open-circuit voltage of the devices but also controls th
251 synthesis is another key for realizing high open-circuit voltage perovskite solar cells without hole
252 ocenium, explaining the large discrepancy in open-circuit voltage potentials between these two redox
253 electronic alloy states that can adjust the open-circuit voltage provides the underlying basis of te
255 f the photocurrent spectral response and the open-circuit voltage show that the HOMO and LUMO levels
256 esent an alternative approach to improve the open-circuit voltage through the use of a zinc chlorodip
257 ate an energy-harvesting application with an open-circuit voltage up to 7 V and a power density up to
258 eveals a molecular design avenue to increase open-circuit voltage while retaining the short-circuit c
259 ating in human tears were registered: 0.57 V open-circuit voltage, about 1 muW cm(-2) maximum power d
261 t is achieved by synergistic improvements in open-circuit voltage, charge generation, and charge tran
264 s and results in substantial improvements in open-circuit voltage, fill factor, and an increased powe
265 mum electrical power, short-circuit current, open-circuit voltage, recombination rates, and variation
266 Thus, IOIC2-based OSCs show higher values in open-circuit voltage, short-circuit current density, fil
267 ltaic short-circuit current density and good open-circuit voltage, so that ITIC-6F achieves the highe
268 obtaining polymer solar cells with a higher open-circuit voltage, while 4,7-dithien-2-yl-2,1,3-benzo
279 onversion efficiencies, those displaying low open circuit voltages are better matched to catalysts wi
283 unction (BHJ) PM6:Y6 system can achieve high open-circuit voltages (V(OC) ) while maintaining excepti
285 leakage currents of approximately 1 fA, and open-circuit voltages and fill-factors up to 0.5 V and 7
286 radiative recombination, resulting in larger open-circuit voltages and higher radiative efficiencies.
287 ber of NWs, as well as retention of the high open-circuit voltages and short-circuit current densitie
288 ular orbital (LUMO) levels, and hence higher open-circuit voltages can be observed in the correspondi
289 ltaic power conversion efficiencies and high-open-circuit voltages for solution-processed CIS and CZG
290 backbones have been shown to achieve larger open-circuit voltages in solar cells, though with decrea
292 nder light, the photovoltaic devices exhibit open-circuit voltages of 0.44 V, short-circuit current d
293 ch power conversion efficiencies of 8.5% and open-circuit voltages of 0.97 V in BHJ devices with PC71
294 we fabricated perovskite cells that reached open-circuit voltages of 1.2 volts and power conversion
298 ces reduce device hysteresis and improve the open-circuit voltages to values up to 1.20 V, resulting