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1 rized by a fast (tau(1)) and a slow (tau(2)) decay time.
2 and prevents the shortening in NMDAR current decay time.
3 ishes the developmental change in NMDAR-EPSC decay time.
4 diction of brightness, stability, Phi(f), or decay time.
5 ctivity did not significantly alter the EPSC decay time.
6 cholinesterase inhibitor, prolonged the EPSC decay time.
7 cumulation but had no effect on the rise and decay time.
8 velength emission associated with the longer decay time.
9 using a long lifetime standard with a known decay time.
10 the deactivation kinetics by prolonging the decay time.
11 (cis) isomer in DOPC (DPPC) presents a fast decay time.
12 ag-1 and a sharp rise in the autocorrelation decay time.
13 2+ transient amplitude and prolonged the 50% decay time.
14 smission to Bergmann glia and decreased EPSC decay time.
15 ise times, amplitudes, charge transfers, and decay times.
16 to CaN to maintain NMDAR currents with long decay times.
17 of the eIPSC could be distinguished by their decay times.
18 imilar to WT bumps, but with slightly slower decay times.
19 current amplitudes with significantly faster decay times.
20 complexes led to variations in fluorescence decay times.
21 elations with relatively long characteristic decay times.
22 s of more than PhiPL = 90% at short emission decay times.
23 mations that fit the experimentally measured decay times.
24 tes of LOV390 formation but exhibited adduct decay times 1 order of magnitude faster than wild type.
25 netically fast (rise time, 0.32 +/- 0.02 ms; decay time, 1.66 +/- 0.18 ms; mean +/- SD; n = 6 cells),
26 (31%), and prolongation of the Ca(2+) signal decay time (165%) than overexpression (2-fold) of wild t
27 imes greater), and decayed more slowly (half-decay time 189 ms for strontium and 32 ms for calcium).
29 tivity exhibit significantly longer AHP half-decay times (24.67 vs. 11.02 ms) and greater AHP amplitu
30 d trimer system, the fluorescence anisotropy decay time (35 fs) is found to be much shorter than that
32 pressure is typically much shorter than the decay time after cessation or decline in the volume of d
34 e different membrane phases via fluorescence decay time analysis, making this new probe versatile for
35 an account for frequency-dependent change of decay time and force potentiation at intermediate stimul
36 d in gas phase by measuring the fluorescence decay time and ion-neutral collision cross sections (CCS
37 Elevating quantal content lengthened EPSC decay time and prolonged both the fast (alpha7-nAChR-med
38 osolic Ca(2+) followed by an increase in the decay time and the spread of the spontaneous Ca(2+) spik
39 wo adjustable parameters instead of the many decay times and amplitudes required in standard analysis
42 ic modeling of temperature-dependent singlet decay times and quantum yields of fluorescence, isomeriz
44 peak parameters including shorter rise time, decay time, and half-width as compared to a bare carbon
46 peak amplitudes, prolonged current rise and decay times, and altered responses to benzodiazepine ago
49 (A) receptor, the peak amplitudes, 90-to-10% decay times, and total charge transfer of spontaneous mi
50 than 10-fold slower in nucleo-olivary cells (decay time, approximately 25 ms) than in large cells ( a
51 s (reductions of approximately 48% in 10-90% decay time, approximately 40% in tau, and approximately
53 ant glycine receptors, we show that response decay times are accelerated by addition of GABA, a weak
54 efficient scintillation crystals with short decay times are indispensable for improving the performa
55 echnique in which fluorescence excited state decay times are measured as fluorescently labeled cells
57 We also rule out small increases in IPSC decay times (as caused by W170S and R414H) as a possible
58 L-type calcium channel window current, slow decay time at various voltages, and increased late calci
59 es as photodetectors, for both intensity and decay-time based monitoring of the sensing element's PL.
65 2AP does not exhibit the long fluorescence decay time characteristic of the free nucleoside, sugges
68 The absorption spectrum and fluorescence decay time components of the complex at room temperature
70 postsynaptic currents (mIPSCs) (predominant decay time constant (tau(decay)), 1.0 ms) in addition to
71 ntly with distance from the soma whereas the decay time constant (taudecay) of Delta[Ca2+] decreases
73 +/- 0.59 to -4.15 +/- 0.73 nA with the fast decay time constant accelerating from 0.75 +/- 0.09 ms a
75 is derived as the inverse of the exponential decay time constant based on a heterogeneous Michaelis-M
78 tential was approximately 6 min, whereas the decay time constant for STP of the NMDA receptor-mediate
79 e recovery from desensitization is slow (the decay time constant is roughly 500 milliseconds), little
80 ronal firings are asynchronous, the synaptic decay time constant needs to be comparable to that of th
82 five cells, with a time to peak of 1.0 ms, a decay time constant of 2.3 ms, and a reversal potential
85 0 and 15 ms after an action potential, had a decay time constant of about 30 ms, and showed no accumu
86 Also, halothane considerably prolonged the decay time constant of evoked IPSCs in pyramidal cells a
87 howed that R(A) resulted in a slowing of the decay time constant of excitatory postsynaptic currents
88 he amplitude but increased its effect on the decay time constant of field EPSPs recorded under condit
89 at 38 h after ischemia; the rising slope and decay time constant of I(A) were accordingly increased a
91 opregnanolone caused an increase in the slow decay time constant of spontaneous GABA-mediated IPSCs i
94 enzodiazepine agonist zolpidem increased the decay time constant of the IPSCs of immature granule cel
95 velocity, the quick-phase frequency, and the decay time constant of the negative OKAN were dependent
96 ation had no effect on the peak amplitude or decay time constant of the NMDA component, or the I-V re
98 nnection, amplitude, latency, rise time, and decay time constant of the unitary EPSC were not differe
100 e induced absorption shows quadratic and the decay time constant shows linear dependence on the laser
101 ure/volume measurements (-dP/dtmin, pressure decay time constant tau-Glantz, and passive filling stif
102 a significantly higher frequency and faster decay time constant than those recorded from the medulla
103 9 +/- 0.0299 pA pF(-1) (n = 7 cells) and the decay time constant was tau = 790 +/- 76 ms (n = 5).
104 709 +/- 0.0299 pA pF-1 (n = 7 cells) and the decay time constant was tau = 790 +/- 76 ms (n = 5).
105 and the benzodiazepine potentiation of this decay time constant were both significantly increased in
106 ns (10-100 pA, 10 ms rise time constant, 5 s decay time constant) in the presence of various synaptic
107 cay time, weighted decay time constant, slow decay time constant, and, consequently, the total charge
109 ak amplitude, 90-to-10% decay time, weighted decay time constant, slow decay time constant, and, cons
116 r is marked by a significant increase in the decay-time constant for evoked and spontaneous IPSCs and
117 e Pb2+ changed neither the amplitude nor the decay-time constant of the MPSCs, Pb2+-induced changes i
118 but not young, rats exhibit a twofold longer decay time-constant and temporally summate a train of st
119 erculoventral cells had significantly faster decay time constants (0.35-0.40 msec) than did those fro
120 bicuculline methiodide (BMI), and had longer decay time constants (4.5-6.0 ms) that were modulated by
122 ell recordings at 22 degrees C, the weighted decay time constants (tau(w)) of spontaneous IPSCs (sIPS
123 tants were increased by 195% and evoked IPSC decay time constants by 220% compared with age-matched c
128 wer IPSCs, with a 2.6-fold difference in the decay time constants of spontaneous IPSCs and a 5.3-fold
129 an inactivating potassium (IA) current with decay time constants of up to 225 ms, and small-amplitud
130 ated quantum states of multiple nuclei, have decay time constants that may exceed T1 by large factors
131 s methods for assessing ventricular pressure decay time constants to test whether sensitivity to slig
134 ication of L-glutamate to nucleated patches, decay time constants were similar at +/-60 mV in the pre
135 current amplitudes, altered desensitization decay time constants, and reduced GlyR clustering and sy
142 ak) of fAMPAsEPSCs was 1.5+/-1.05 ms and the decay time could be fitted with a single exponential wit
143 ch as high solubility and short fluorescence decay time, could be obtained from fluorophors composed
146 prolonged (63 +/- 14 %; mean +/- s.e.m.) the decay time course of miniature IPSCs (mIPSCs) without si
147 rong correlation between prolongation of the decay time course of sIPSCs and potentiation of single-c
148 e whether the magnitude of modulation of the decay time course of sIPSCs correlates with the extent o
152 The averaged macroscopic current exhibited a decay time course which was well described by a single e
155 receptor-mediated sEPSC with slower rise and decay time courses and larger peak amplitudes (sAMPAsEPS
157 bly phased bends, the relative birefringence decay times depend on the flexibility of each bend, not
159 Although pure GABAergic and glycinergic decay times did not differ depending on HM location, the
161 e temperature dependence of the luminescence decay time enables intrinsic temperature compensation of
162 ied out, as a function of expected diffusion decay time for a particular solute, and show that use of
163 seconds) was markedly greater than the half decay time for cytosolic Ca2+ sparks (31.2+/-0.56 ms) ob
164 thdrawal is due to a sixfold decrease in the decay time for GABA currents and consequent decreased in
171 d on Floquet modes, which increases the Rabi decay time ([Formula: see text]) in a number of material
172 g by electron transfer predict heterogeneous decay times from 50-500 ps that agree with our experimen
174 m2 mass transporting area), 90 s 10-90% rise/decay time glucose electrode, and an on-the-skin electro
177 er miniature inhibitory postsynaptic current decay time in null mice, with no change in miniature inh
178 ons displayed a larger amplitude and shorter decay time in spontaneously hypertensive rats (SHRs) tha
179 addition, the normal downregulation of NMDAR decay time in sSC neurons at P11 was absent after NMDA t
184 ontains at least seven transient states with decay times in the range from 10 micros to 200 ms, but t
186 Under control conditions, GABA(A slow) IPSC decay times increased linearly with membrane depolarizat
187 tic trauma (AT, loud sounds) slow AMPAR-EPSC decay times, increasing GluA1 and decreasing GluA4 mRNA.
188 es, such as (Pro-Pro-Gly)(10), show multiple decay times, indicating multiple scission locations and
190 The observed temperature dependence of the decay time is discussed in terms of two possible mechani
194 he level of screening achieved at nanosecond decay times is shown to change with the coverage of elec
196 mplicated in developmental plasticity, shows decay time kinetics that shorten postnatally as NR2A sub
197 ncreased, while GABA-ACh pairing affects the decay time leading to elevated calcium levels during the
198 l populations, noise can render the measured decay times meaningless for small amplitude Ca2+ sparks.
199 elationship between Ca2+ spark amplitude and decay time might be used to distinguish Ca2+ sparks from
200 curate diffusion constants for both species, decay times must be bounded by adequate minimum and maxi
202 ltrafast (tens of femtoseconds) hot electron decay times observed experimentally arise from electron-
204 somer dissociates through thermolysis with a decay time of 14 min at 296 K to form the [6,6]-closed e
205 rong fluorescence at 1544 nm with a measured decay time of 3 ms and an estimated quantum efficiency o
207 ations of OHBI give an estimated first-order decay time of 476 fs for the S(1) state, which is larger
208 itated neural excitability by shortening the decay time of 5-HT(3)R currents, lowering the stimulus t
210 cated by increased rectification and reduced decay time of AMPAR-mediated excitatory postsynaptic cur
211 d triplet pair states, but the rapid singlet decay time of approximately 200 ps in solution-grown sin
214 a(2+) exchange activity (indexed by the half decay time of caffeine-elicited Ca(2+) transient) by 27%
216 ampal slices from CIE rats revealed that the decay time of GABAR-mediated miniature inhibitory postsy
219 re, bounding the scrambling time by a finite decay time of local quantum correlations at late times.
220 ion as shown by increasing the frequency and decay time of mEPSCs, and simultaneously inhibiting GABA
225 i) in cultured neurons SGE-301 prolonged the decay time of NMDAR-dependent spontaneous excitatory pos
226 ith these changes, the current amplitude and decay time of NMDARs in PFC was significantly reduced.
227 s the inhibitory signaling by prolonging the decay time of postsynaptic GABAergic currents upon photo
228 te the relatively slow transfer, the overall decay time of PSI-LHCI-LHCII remains fast enough to assu
232 stimulation or uncaging of IP3 increased the decay time of spontaneous Ca(2+) events without changing
234 cerebellar synapses selectively prolongs the decay time of synaptic currents, whereas a switch from G
235 d calcium kinetics associated with prolonged decay time of the calcium transient and increased diasto
237 simple strategy to control and modulate the decay time of the functionalized Yb(3+)-doped nanopartic
239 ns is however limited by the relatively fast decay time of the hyperpolarized spin state together wit
240 n of the gamma oscillation, in which the the decay time of the inhibitory cells is critical to the fr
241 longer times we find an ambient temperature decay time of the Omega Fe-C5' bond of tau ~ 5-6 s, like
244 hematite, this recombination exhibits a 50% decay time of ~6 ps, ~10(3) times faster than that of Ti
245 cay displays multiexponential character with decay times of 1.2 and 16 ps, and 0.6, 2.2, and 4.2 ns.
247 lipid hydrogen bonds are long lived, showing decay times of 50 ns, and forming strings of lipids, and
248 this issue, we have measured the rotational decay times of a 'gapped-duplex' DNA molecule possessing
249 is described by two kinetic components with decay times of approximately 20 and approximately 200 ns
250 tracellular space, is reflected by increased decay times of neuronal NR2A-mediated NMDA currents.
251 Increasing quantal content also prolonged decay times of pharmacologically isolated alpha7-nAChR-
252 The rise times, areas, half-widths, and decay times of sEPSCs and emEPSCs and interevent interva
253 lay very high luminescence quantum yields at decay times of several tens of mus even in solution unde
254 etectably, in that the amplitudes, areas and decay times of spontaneous miniature EJCs were unchanged
256 second carbamate is evident from bimodal T2 decay times of the approximately 163 ppm peak, indicatin
258 showed that an alteration of amplitudes and decay times of the GABAergic currents to the dentate nuc
259 llows a bi-exponential time dependence, with decay times of the order of picoseconds, indicating that
260 ground state bacteriorhodopsin and the mean decay times of the photocycle M-state intermediates.
261 the similarities between the characteristic decay times of the time correlation function, as obtaine
264 d at P12-13; (3) the kinetics (rise time and decay time) of both mEPSCs and mIPSCs accelerated with a
265 t pure graphane has a very long nonradiative decay time, on the order of 100 ns, while epoxy- and hyd
268 s with multiple peaks and increased rise and decay times, reflecting "desynchronized" SV fusion.
269 ependent long-term depression decreased EPSC decay time, revealing a 'late' current that is present w
271 ectra (TRES) indicate that this fluorescence decay time should be ascribed to a highly quenched confo
273 EPSCs in low quantal-content conditions had decay times similar to the time course of receptor deact
275 c membrane input resistance or EPSC rise and decay time suggested that the effects of PPs on EPSCs we
276 large drop in NMDA receptor (NMDAR) current decay time synchronized across all neurons and occurring
277 with a 2-fold faster rise and 7-fold faster decay time (t1/2 of 40 ms) than GCaMP6f, indicating that
279 th GCaMP6fu displaying fluorescence rise and decay times (t1/2) of 1 and 3 ms (37 degrees C) in vitro
280 ce (TEB) measurement in which the rotational decay times (taugap) of DNA molecules possessing central
284 2O8+x characterized by an excited population decay time that maps directly to a discrete component of
285 s that the mutant subunit increases synaptic decay times, thereby prolonging postsynaptic activity.
288 s accompanied by a nearly 2-fold increase in decay time, to values that are indistinguishable from th
289 anostructures exhibit extremely long carrier decay times up to 20 micros that are combined with high
291 with membrane depolarization, and this IPSC decay time voltage dependence was not significantly alte
293 The spike amplitude as well as rise and decay time were comparable with those measured by carbon
298 by the histograms of the rise times and half-decay times, which revealed modes at 38 and 65 ms, respe
300 e scaling of the characteristic fluorescence decay time with the vesicle diameter and the buildup of