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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 supporting water oxidation catalysis and at open circuit.
4 he capacitance of a potentiometric sensor at open circuit.
6 nt positive feedback above a Pt substrate at open circuit as an indication of the reactivity of this
7 bolic effects of UCN were monitored using an open circuit calorimeter which measured oxygen consumpti
9 NPY (19.5-78 pmol) were determined using an open-circuit calorimeter by measuring the volumes of oxy
10 similar pretreatment were monitored using an open-circuit calorimeter measuring the volume of oxygen
14 of complementary electrochemical techniques: open-circuit chronopotentiometry (CP), linear polarizati
17 pithelial potentials (V(t)) were recorded in open circuit conditions while applying constant current
18 at the substrate at a given potential under open circuit conditions, a feature not attainable with c
19 borated between freshly prepared, aged under open circuit conditions, and cycled electrodes of compos
22 axation, in which the membrane relaxes under open-circuit conditions in a diffusion-controlled proces
27 ricidal properties, compared to the control (open-circuit) diffusate, and reduced observable biofilm
28 y is produced by simple solution exchange in open circuit, due to the associated decrease in the capa
32 folding geometry that generates 110 volts at open circuit or 27 milliwatts per square metre per gel c
36 ed in an additional twofold reduction in the open-circuit permeability when the ionic strength was de
39 ot intentionally doped and showed a positive open-circuit photovoltage based on photoelectrochemical
40 2, BQ (2 mM), BQ(*-) (2 mM)/carbon, shows an open-circuit photovoltage of 1.05 V and a short-circuit
41 t-circuit photocurrent J(sc)= 16.1 mA/cm(2), open-circuit photovoltage V(oc) = 0.631 V, and a fill fa
42 ty of the cyclometalated compound, while the open-circuit photovoltage was significantly larger for t
44 Au/TiO2/Ti multilayer structure had typical open-circuit photovoltages of 600-800 mV and short-circu
45 w fundamental energy losses; it can generate open-circuit photovoltages of more than 1.1 volts, despi
46 e to the anode (63.5-78.7%) than that in the open circuit positive controls (37.6-43.4%) during a per
47 electrochemical technique incorporating both open circuit potential (OCP) and amperometric techniques
48 affect significantly the measurement of the open circuit potential (OCP) and cyclic voltammetry (CV)
49 de of 25 mV, a frequency of 81.3 kHz, and an open circuit potential (OCP) as the direct-current (dc)
59 rbed-accumulated on the electrode surface at open circuit potential and then stripped off by applying
60 Approach curves to a conducting substrate at open circuit potential are influenced by the solution ti
61 ted specific ROS activity was lowest for the open circuit potential condition, elevated when cathodic
62 easurements) or the passive tracking (during open circuit potential decay) of the quasi-Fermi level i
65 rrent density of 657 +/- 17 muAcm(-2) and an open circuit potential of 0.57 +/- 0.01 V, which is suff
66 he enzymatic biofuel cell (EFC) generated an open circuit potential of 0.61 (+/-0.02) V with a maximu
67 photocurrent density of 35 mA cm(-2) and an open circuit potential of 450 mV; there was no observabl
69 of two hydroxy groups to AQDS increases the open circuit potential of the cell by 11% and we describ
71 plying AC amplitude of 50 mV at 117.2 Hz and open circuit potential, a minimum of 214 captured cells/
74 s a diazonium activation by reduction at the open circuit potential, with aryl radical secondary prod
75 n film electrode to reductants decreased the open-circuit potential (OCP) and reduced the area of a c
79 electrochemical impedance analysis (EIS) and open-circuit potential decay transients (OCVD), which at
84 ed on the electrochemical measurement of the open-circuit potential of the platinum electrode immerse
85 OS was adjusted by polarization to the known open-circuit potential of the solid contact in 0.1 M KCl
86 H2O2 was estimated by measuring the H(+)/H2 open-circuit potential under the reaction conditions.
87 SAED, EDX, XPS, UV-visible spectroscopy, and open-circuit potential versus time experiments to unders
91 Through electrochemical testing including open circuit potentials, potentiodynamic scans, anodic p
93 hat the methodology compares well to that of open circuit potentiometry, despite giving complementary
94 volves a short (1 s) galvanostatic pulse, an open-circuit pulse (0.5 s) during which the EMF of the c
97 approximately 1.7microWcm(-2)) with similar open circuit voltage (0.27V) compared to native GOX when
100 rated for 450 h and results indicated a high open circuit voltage (about 810 mV) compared with previo
101 node following exposure to butane, and under open circuit voltage (OCV) conditions the graphite persi
102 r density of 2.3microWcm(-2) at 0.21V and an open circuit voltage (OCV) of 0.49V were registered as a
107 at PIPCP:PC61BM blends yield devices with an open circuit voltage (V(oc)) of 0.86 V, while maintainin
108 the [Co(bpy)(3)](2+/3+) redox couple, and an open circuit voltage (V(oc)) of almost 1.0 V at 100% sun
109 rstand the impact of these fluorine atoms on open circuit voltage (V(oc)), short circuit current (J(s
110 ueisser limit, but they suffer from a larger open circuit voltage (VOC ) deficit than narrower bandga
111 uit current density (Jsc) of 18.53 mA/cm(2), open circuit voltage (Voc) of 0.538 V, and fill factor (
113 he charge transfer process and increases the open circuit voltage (Voc) to 260 mV above reference dev
118 ncentration (5mM), the biofuel cell exhibits open circuit voltage and power density of 302.1 mV and 1
119 45 mM glucose, the biofuel cell exhibited an open circuit voltage and power density of 681.8 mV and 6
120 o higher short-circuit current, fill factor, open circuit voltage and significantly reduced device-to
122 groups on the anion significantly alters the open circuit voltage and yields a clear dependence on el
123 ultant FeS-based enzyme electrode reached an open circuit voltage closer to its standard potential un
124 current density versus applied potential and open circuit voltage decay measurements were employed to
125 While the electrical power output and the open circuit voltage decreased with increasing temperatu
130 exhibited the following characteristics: an open circuit voltage of 0.54 V, a maximal power density
131 all known all-carbon-based materials with an open circuit voltage of 0.59 V and a power conversion ef
133 of-concept of a membrane-free battery has an open circuit voltage of 1.4 V with a high theoretical en
134 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
143 The enzymatic fuel cell reaches 0.5 V at open circuit voltage with both, ethanol and methanol, wh
144 perovskite have the benefit of retaining an open circuit voltage ~0.14 V closer to its radiative lim
146 taic device is fabricated to produce a large open circuit voltage, 0.85-0.95 V, which is higher than
147 d as the offset between optical band gap and open circuit voltage, and compare the results to those o
149 accessible in polymer solar cells with high open circuit voltage, and we therefore suggest this loss
151 results from synergistic effects of enlarged open circuit voltage, suppressed trap-assisted recombina
152 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 atio of the three components was varied, the open-circuit voltage (V(oc)) increased as the amount of
165 hose of the individual "subcells", while the open-circuit voltage (V(oc)) is between those of the "su
166 form is more basic than the Sp form, and the open-circuit voltage (V(oc)) is related to the proton co
167 3HT to SWNTs is proposed to explain the high open-circuit voltage (V(OC)) obtained from the photovolt
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 conversion efficiency of 4.02%, featuring an open-circuit voltage (V(oc)) of 929 mV and a short-circu
171 ) (>0.57) at all fullerene ratios, while the open-circuit voltage (V(oc)) was found to vary from 0.61
172 ties for the two dyes, a consistently higher open-circuit voltage (V(oc)) was measured for Dye-S rela
173 molecules that are shown to tune the output open-circuit voltage (VOC) across three types of pristin
174 rformed better than RSQ1 owing to its higher open-circuit voltage (Voc) and fill factor (ff) in spite
175 ad to enhanced efficiencies due to increased open-circuit voltage (VOC) and improved absorption of so
176 high photocurrent generation, the achievable open-circuit voltage (Voc) is fundamentally limited due
177 ectric conversion efficiency (eta) of 2%, an open-circuit voltage (Voc) of 0.39 mV, and a short-circu
178 , which induce a simultaneous enhancement in open-circuit voltage (Voc), short-circuit current (Jsc),
179 isible and infrared light, we measure a d.c. open-circuit voltage and a short-circuit current that ap
180 of sterics and molecular orientation on the open-circuit voltage and absorbance properties of charge
183 bricate core-shell nanowire solar cells with open-circuit voltage and fill factor values superior to
187 provide both high short-circuit current and open-circuit voltage at room temperature, and be driven
188 maximum, our focus is on efforts to increase open-circuit voltage by means of improving charge-select
190 ethylene)malononitrile leads to an increased open-circuit voltage compared with its isomer 2-((7-(N-(
198 as been speculated to contribute to the high open-circuit voltage in several types of high efficiency
203 ell voltage of 0.52 V and in human blood; an open-circuit voltage of 0.65 V, a maximum power density
204 e BFC were obtained: in phosphate buffer; an open-circuit voltage of 0.68 V, a maximum power density
205 ort-circuit current values of 14.2 mA/cm(2), open-circuit voltage of 0.7 V, and a broad external quan
206 arbon nanotube yarn biofuel cells provide an open-circuit voltage of 0.70 V, and a maximum areal powe
207 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
208 , a short-circuit current of 14 mA/cm(2), an open-circuit voltage of 0.74 V, and a fill factor of 58%
209 Corresponding solar cells featured a high open-circuit voltage of 0.9 V, a fill factor around 0.6,
210 conversion efficiency of 7.03% with a large open-circuit voltage of 0.95 V without using any additiv
212 nversion efficiency (PCE) of 3.7% and a high open-circuit voltage of 1.06 V are obtained under simula
213 wer conversion efficiency of over 14% and an open-circuit voltage of 1.06 V measured under reverse vo
214 PEA=C6H5(CH2)2NH3(+), MA=CH3NH3(+)) show an open-circuit voltage of 1.18 V and a power conversion ef
215 ng interface defects, the device exhibits an open-circuit voltage of 1.20 V and an efficiency of 3.97
216 dal perovskite QD photovoltaic cells with an open-circuit voltage of 1.23 volts and efficiency of 10.
217 ptide-based power generator that produces an open-circuit voltage of 1.4 V and a power density of 3.3
219 The prototype device provides a peak-to-peak open-circuit voltage of 157 V and instantaneous short-ci
220 drop of 400 muL alone could generate a peak open-circuit voltage of 42 V under a 0.25 Hz vibration.
222 ort-circuit current of 32.6 pA mm(-2) and an open-circuit voltage of 78 mV, providing for a maximum p
224 r-conversion-efficiency of 7.26% with a high open-circuit voltage of approximately 1 V and a striking
225 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
226 esence reduces the short-circuit current and open-circuit voltage of solar cells based on blends of P
228 lecular orbitals to be tuned to maximize the open-circuit voltage of the devices but also controls th
229 synthesis is another key for realizing high open-circuit voltage perovskite solar cells without hole
230 ocenium, explaining the large discrepancy in open-circuit voltage potentials between these two redox
231 electronic alloy states that can adjust the open-circuit voltage provides the underlying basis of te
233 f the photocurrent spectral response and the open-circuit voltage show that the HOMO and LUMO levels
234 esent an alternative approach to improve the open-circuit voltage through the use of a zinc chlorodip
235 ate an energy-harvesting application with an open-circuit voltage up to 7 V and a power density up to
236 eveals a molecular design avenue to increase open-circuit voltage while retaining the short-circuit c
237 ating in human tears were registered: 0.57 V open-circuit voltage, about 1 muW cm(-2) maximum power d
239 t is achieved by synergistic improvements in open-circuit voltage, charge generation, and charge tran
241 s and results in substantial improvements in open-circuit voltage, fill factor, and an increased powe
242 mum electrical power, short-circuit current, open-circuit voltage, recombination rates, and variation
243 Thus, IOIC2-based OSCs show higher values in open-circuit voltage, short-circuit current density, fil
244 obtaining polymer solar cells with a higher open-circuit voltage, while 4,7-dithien-2-yl-2,1,3-benzo
250 onversion efficiencies, those displaying low open circuit voltages are better matched to catalysts wi
253 bits promising electrochemical performances: open circuit voltages of 1.11 V and current densities of
256 leakage currents of approximately 1 fA, and open-circuit voltages and fill-factors up to 0.5 V and 7
257 radiative recombination, resulting in larger open-circuit voltages and higher radiative efficiencies.
258 ber of NWs, as well as retention of the high open-circuit voltages and short-circuit current densitie
259 ular orbital (LUMO) levels, and hence higher open-circuit voltages can be observed in the correspondi
260 backbones have been shown to achieve larger open-circuit voltages in solar cells, though with decrea
261 nder light, the photovoltaic devices exhibit open-circuit voltages of 0.44 V, short-circuit current d
262 ch power conversion efficiencies of 8.5% and open-circuit voltages of 0.97 V in BHJ devices with PC71
263 we fabricated perovskite cells that reached open-circuit voltages of 1.2 volts and power conversion
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