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1 acellular impedance is low and approximately resistive.
2  varies in relation to the charging time and resistive and capacitive noise.
3 ia-derived ZnS nanoparticles, exhibit unique resistive and capacitive responses to changes in O2 and
4                                 The in-plane resistive and impedance properties of ZnO films, fabrica
5                             The operation of resistive and phase-change memory (RRAM and PCM) is cont
6 effective arterial elastance (Ea) represents resistive and pulsatile afterload of the heart derived f
7 tion rather than enhanced pulmonary vascular resistive and pulsatile loading.
8 nce in cerebral cortex could be high and non-resistive, and we propose further experiments to settle
9            METHODS AND Total, pulsatile, and resistive arterial load were measured in 2141 patients w
10 liquid-like, rho proportional, variant T(2)) resistive behavior in the pseudogap regime.
11 n Indium Phosphide (InP) semiconductor-based resistive biosensor using the change of its electronic p
12 oach may pave the way for the development of resistive biosensors at very low-cost with high performa
13                                      Magneto-resistive biosensors have been found to be useful becaus
14 eriments in patterned strands, mimicking the resistive boundaries that occur naturally in the heart,
15                        Curium is also highly resistive, but its susceptibility is Curie-like at high
16                                 They possess resistive, capacitive and inductive components that can
17 sting mechanical sensing technologies (i.e., resistive, capacitive, or piezoelectric) have yet offere
18 he flagellum (f(N) and f(T)) were related by resistive coefficients (C(N) and C(T)) to the correspond
19                  The estimated values of the resistive coefficients are consistent among all three ge
20                                          The resistive component is bell-shaped for both voltage and
21                                          The resistive component of the impedance was relatively smal
22                           The capacitive and resistive components are similar to experimental measure
23 sent an equivalent circuit model to describe resistive components in a CDI cell.
24 lectric field that determines capacitive and resistive components of the transferred charge.
25  components, a capacitive current (Ic) and a resistive current (Iion), corresponding to the cardiac a
26 RNA-DNA duplex in the nanopore recorded as a resistive current pulse.
27                      The results suggest the resistive detection of spin resonance, and provide a mea
28 nductors (CMOSs) and adjustable two-terminal resistive devices (memristors) have been developed.
29 traction, whereas microtubules contribute as resistive/dissipative elements.
30 ipation allows us to estimate the torque and resistive drag that act on the flagella of these major s
31                   The dynamic load is highly resistive during on-switching allowing access to the hig
32 tive touch screens and pixels of microscopic resistive electrodes are demonstrated.
33 rresponds to the appearance of an additional resistive element on one side of the OmpU protein and co
34                               Memristors are resistive elements retaining information of their past d
35 of blebs in rounded cells moving in a highly resistive environment.
36 es in intrathoracic pressure that occur with resistive exercise and can lead to unpredictable effects
37 coronary artery disease, potentially through resistive exercise training or nutrition interventions.
38 at incorporate higher intensity, progressive resistive exercises that target all major muscle groups
39 s the problem of cellular proteins acting as resistive factors preventing efficient drug penetration,
40  friction-dominated and noninertial granular resistive force environment, and the simplicity of the m
41                       Here, we show that all resistive force hypotheses in grains arise from local fr
42  to obey surprisingly simple, yet empirical 'resistive force hypotheses'.
43 erion to determine which rheologies can obey resistive force hypotheses.
44 hing of kinetochore motility through loss of resistive force is further evidence for the emerging mod
45                        Here we show that the resistive force predicted previously for dynamic adhesio
46  helps to focus MT minus ends and provides a resistive force that acts antagonistically to plus-end-d
47 umerical simulations are conducted using the resistive force theories, the slender body theories of L
48 the slender body, regularized Stokeslet, and resistive force theories; thus readers can readily compu
49  the predictions to our previously developed resistive force theory (RFT) which models sand-swimming
50                      The commonly used local resistive force theory assumes a stationary background f
51 cal flagellum is often interpreted using the resistive force theory developed by Gray and Hancock and
52                                      We test resistive force theory in experiments on macroscopic swi
53                 We show that an extension of resistive force theory is able to use the dynamics of a
54           Although pedagogically attractive, resistive force theory is not generally applicable to ex
55                                      Using a resistive force theory model we demonstrate that hyperac
56                                              Resistive force theory modeling incorporating variation
57 tal results and kinematic simulations from a resistive force theory propulsion model, we demonstrate
58    However, quantitative comparisons suggest resistive force theory underestimates the influence of c
59                                        Using resistive force theory, we show how the helical motion o
60 efficients that are not captured by original resistive force theory.
61 y and quantitatively from the predictions of resistive force theory.
62 nanoprobe structure, which were converted to resistive force.
63 mately 70 degrees to translate actin against resistive force.
64 mately 70 degrees to translate actin against resistive force.
65  than grains, and to predict a new family of resistive-force-obeying materials: cohesive media such a
66 ity spectrometer constructed with monolithic resistive glass desolvation and drift regions.
67                                      Using a resistive glass tube, mobility spectra were obtained by
68 rols assay temperature through an integrated resistive heater and monitors real-time fluorescence sig
69           Furthermore, by integrating a thin resistive heater as the thermal trigger of Joule heating
70                    The device has integrated resistive heaters and temperature sensors as well as a 7
71 eight parallel PCR reactions, and integrated resistive heaters for rapid thermocycling (>5 degrees C/
72 tly complement and close the gap between the resistive heating and the shock compression experiment.
73  desorbed with little power consumption upon resistive heating of the wire.
74 bers do not necessarily constitute undesired resistive heating problem for photovoltaics.
75 sistor (ISFET) sensors, temperature sensors, resistive heating, signal processing and control circuit
76            During electrophoresis, Joule (or resistive) heating degrades separation performance.
77 ral intracellular coupling and accounted for resistive heterogeneity in the extracellular space showe
78 designed six functional inks, based on piezo-resistive, high-conductance, and biocompatible soft mate
79 ties, leakage conduction mechanisms, and the resistive hysteresis of the materials.
80 ting condensate and render the wire slightly resistive (i.e., not fully superconducting), even at tem
81  daily activities that are either aerobic or resistive in nature is compromised and contributes to th
82 ectrodes have shown that it is approximately resistive in the range of biological interest, <10 kHz,
83 biopsy results, was associated with a higher resistive index (0.87 +/- 0.12 vs. 0.78 +/- 0.14 [P=0.05
84 tration rate (P < 0.001), and improved renal resistive index (P < 0.001) and kidney microcirculation.
85 ge was the strongest determinant of a higher resistive index (P<0.001).
86 e-corrected peak systolic velocity (PSV) and resistive index (RI) values were compared between patien
87 ity, portal vein flow volume, hepatic artery resistive index (RI), hepatic artery pulsatility index (
88 city (EDV), peak systolic velocity (PSV) and resistive index (RI).
89  OLT recipients developed DAA (defined by HA resistive index [HARI] <0.5) and received oral SVDs.
90 rmance of the standard IHA and MHA criteria (resistive index [RI] < 0.5 and classic parvus tardus wav
91            Renal Doppler was used to measure resistive index and esophageal Doppler to monitor aortic
92 ng-II, TLR4 deficient mice had reduced renal resistive index and increased renal cortical blood flow
93 aorta ultrasound revealed a reduction in the resistive index and wall-to-lumen ratio.
94  renal-allograft recipients, we measured the resistive index at baseline, at the time of protocol-spe
95    Stroke volume showed no correlations with resistive index changes after fluid challenge in the ove
96         Stroke volume did not correlate with resistive index changes after fluid challenge in the sub
97                        Although the arterial resistive index did not differentiate between rejection
98                                            A resistive index greater than 0.8 was associated with a h
99 entage of nocturnal fall in SBP and elevated resistive index independently correlated with GFR.
100 ction, high chronic vascular score, and high resistive index irrespective of allograft fibrosis.
101                               The intrarenal resistive index is routinely measured in many renal-tran
102                                              Resistive index measurement before and after fluid chall
103 differ significantly between patients with a resistive index of at least 0.80 and those with a resist
104                  Allograft recipients with a resistive index of at least 0.80 had higher mortality th
105             Several new imaging indices like resistive index of capsular artery, presumed circle area
106                       An intrarenal arterial resistive index of less than 0.6 was associated with hig
107 tive index of at least 0.80 and those with a resistive index of less than 0.80 at 3, 12, and 24 month
108  0.80 had higher mortality than those with a resistive index of less than 0.80 at 3, 12, and 24 month
109 -allograft status, although the value of the resistive index remains unclear.
110 ced by fluid challenge do not translate into resistive index variations in patients without acute kid
111 t protocol-specified biopsy time points, the resistive index was not associated with renal-allograft
112                                        Renal resistive index was unchanged after fluid challenge in b
113 intranodular vascularity, pulsatility index, resistive index, or peak-systolic velocity, was associat
114                                          The resistive index, routinely measured at predefined time p
115 iabetes, low chronic vascular score, and low resistive index.
116              A total of 1124 renal-allograft resistive-index measurements were included in the analys
117      Portal blood flow and renal and splenic resistive indexes were calculated through echographic me
118 kinetochores to release one or both from the resistive influence of its sister's K-fiber.
119 g on-switching allowing access to the highly resistive intermediate states; during off-switching the
120 icrom-wide metal rings, overlaid with a thin resistive layer.
121 ) Here, using a carbon nanotube connected to resistive leads, we create a system that emulates tunnel
122 vely on an actin filament bundle against the resistive load of the laser trap.
123 tor wins, its stepping rate slows due to the resistive load of the losing motor (myoV, 2.1 pN; myoVI,
124 h increased mortality (P<0.001 for all), but resistive load was not.
125 s reflected in blood pressure, pulsatile and resistive load-is associated with adverse clinical outco
126 t (i.e., flexor) acted against an additional resistive load.
127 irming a significant increase in inspiratory resistive load.
128 fterload by elevating pulsatile, relative to resistive, load and may contribute to right ventricular
129 th activity in the lateral PAG (lPAG) during resistive loading, revealing spatially and temporally di
130 rolateral PAG (vlPAG) during anticipation of resistive loading, with activity in the lateral PAG (lPA
131 its mistake and step processively forward at resistive loads <0.7 piconewton or stall or detach at hi
132 that the dominant limiting factor is not the resistive loss of the metal, but rather the intrinsic no
133 or semiconductor based optical devices where resistive losses and power consumption are important per
134  photovoltaics, particularly the optical and resistive losses of the front metal grid.
135 sorbers can enable the exchange of undesired resistive losses with the useful optical absorbance in t
136 ulting in superior power performance and low resistive losses.
137  Ex vivo, migration of neutrophils through a resistive matrix is reduced in the absence of flotillin
138  MEA remains stable when tested under highly resistive media using a continuous flow set up, as well
139 re 1-kilobit crossbar device based upon SiOx resistive memories with integrated diodes has been made.
140 rate the technological deployment of organic resistive memories.
141 in nature of the graphene edge to assemble a resistive memory ( approximately 3 A thick) stacked in a
142     Here we present an analogue non-volatile resistive memory (an electronic synapse) with foundry fr
143                          A fully transparent resistive memory (TRRAM) based on Hafnium oxide (HfO2) w
144                        Recently, ultra-dense resistive memory arrays built from various two-terminal
145                The two-terminal, nonvolatile resistive memory can also be configured in crossbar arra
146                             Here we report a resistive memory device based on a spin-coated active la
147 ns (MFTJ) allowing us to create a four-state resistive memory device.
148                                 Non-volatile resistive memory devices based on ultrathin 2D nanomater
149                                              Resistive memory devices, and in particular memories bas
150 ayers, electrodes and/or device structure of resistive memory devices.
151 anomaterials for fabrication of non-volatile resistive memory devices.
152 nd SThM techniques to nanoscale and vertical resistive memory devices.
153 ics predicts that the equilibrium state of a resistive metal ring will contain a dissipationless curr
154  unwanted charge current shunting by the low resistive NM layer utilizing the newly discovered phenom
155                               Underneath the resistive oceanic lithosphere, the magnetotelluric data
156  properties, which are not consistent with a resistive (ohmic) medium, as often assumed.
157 olers instead of cryogenics for trapping and resistive on-column heating for reinjection.
158 us operating principles, such as capacitive, resistive, or optical sensing.
159 decrease is due to the formation of the more resistive PdH(x) in the presence of H(2).
160 keys rapidly adapted to a novel assistive or resistive perturbation along the direction of the reach.
161 rmotile V is caused by shear thinning of the resistive population of strongly bound myosin heads.
162  minimum, and this is at least partly due to resistive power dissipation.
163 tegration of the stretchable, highly tunable resistive pressure sensor and the fully stretchable orga
164           Here we present an ultra-sensitive resistive pressure sensor based on an elastic, microstru
165 r than all previously reported capacitive or resistive pressure sensors.
166 r torus instability; and coronal jets from a resistive process involving magnetic reconnection.
167  to categorically distinguish capacitive and resistive properties of objects.
168 ler peak velocities, velocity time integral, resistive, pulsatility, acceleration indices (RI, PI, AI
169 create a mapping of the particle position to resistive pulse amplitude at the same instant in time.
170 mputational results were used to compute the resistive pulse current-time response for conical-shaped
171                                     During a resistive pulse experiment, the ionic current through a
172  of the inherent signal amplification of the resistive pulse method.
173 d to detect target DNA in solution through a resistive pulse nanopore detection technique.
174 m-radius particles, and the magnitude of the resistive pulse scaled approximately in proportion to th
175 n solution and on magnetic particles using a resistive pulse sensing (RPS) nanopore.
176                           The use of tunable resistive pulse sensing (TRPS) enabled continuous in sit
177    Here, we demonstrate the use of a tunable resistive pulse sensing (TRPS) technology to monitor the
178 r, we use dynamic light scattering (DLS) and resistive pulse sensing (TRPS) to observe a distinct red
179 -based sensor (aptasensor) utilising Tunable Resistive Pulse Sensing (TRPS).
180 suring zeta potential of nanoparticles using resistive pulse sensing are significantly improved by in
181 ntages, feasibility and limitations of using resistive pulse sensing for sample analysis are discusse
182                      Here we propose tunable resistive pulse sensing for simultaneous size and surfac
183           Particle-by-particle analysis with resistive pulse sensing is performed to detect these cha
184                                           In resistive pulse sensing of microRNA biomarkers, selectiv
185 ection method based on immunoaggregation and resistive pulse sensing technology.
186 s combined approach of optical detection and resistive pulse sensing will join with other attempts at
187 r concentrations (nanomoles of target) using resistive pulse sensing, confirmed by fluorescence and p
188  size spherical shape virus ever measured by resistive pulse sensing.
189                                            A resistive pulse sensor is then used to measure the sizes
190                         A novel method using resistive pulse sensors for electrokinetic surface charg
191                                   The use of resistive pulse sensors for submicron particle size meas
192 tion, which is difficult to resolve with the resistive pulse signal alone.
193 n-dependent and asymmetric triangular-shaped resistive pulse.
194 unable surface charge and chemical state for resistive-pulse and rectification sensing.
195                         This paper describes resistive-pulse detection of cancer biomarker (Vascular
196                                 Furthermore, resistive-pulse experiments are conducted to study the c
197 as an analytical tool enhancing the speed of resistive-pulse experiments, with a potential to simulta
198                  To improve the precision of resistive-pulse measurements, we have used a focused ion
199             Temperature studies coupled with resistive-pulse nanopore sensing enable the quantificati
200                                              Resistive-pulse sensing is a label-free method for chara
201 nanopipettes have recently been employed for resistive-pulse sensing of Au nanoparticles (AuNP) and n
202 zation of hepatitis B virus (HBV) capsids by resistive-pulse sensing through single track-etched coni
203                                         With resistive-pulse sensing, the nanopores fully resolved pu
204 molecule counting experiment called nanopore resistive-pulse sensing.
205 in using nanopores in synthetic membranes as resistive-pulse sensors for molecular and macromolecule
206                 Second, they are amenable to resistive-pulse type measurement systems when embedded i
207 ted using the Coulter counter principle (or "resistive-pulse" method) in which the time-dependent nan
208 n of nanoparticles based on the amplitude of resistive pulses caused by their translocation through n
209 d in terms of the width and amplitude of the resistive pulses generated from the two Coulter counters
210 o resolve the positional dependencies of the resistive pulses.
211 t a detailed study of the characteristics of resistive-pulses of charged and uncharged polymer partic
212  quantitation and sizing of nanoparticles by resistive pulsing sensing (RPS) was investigated.
213     Solution-processed mechanically flexible resistive random access memories are fabricated using Ag
214  device with NiOx interlayers in series with resistive random access memory (ReRAM) device demonstrat
215                                            A resistive random access memory (RRAM) device with a tuna
216 tly imaging the active switching region in a resistive random access memory (RRAM) device, a nanoscal
217       As a new class of non-volatile memory, resistive random access memory (RRAM) offers not only su
218 r as a substrate, we fabricated a disposable resistive random access memory (RRAM) which has good dat
219 that may be applicable to the fabrication of resistive random access memory (RRAM).
220                  As a suitable candidate for resistive random access memory technology, reduced graph
221 ip memory (with hypothetical on-chip digital resistive random access memory).
222 corroborate the reliability of the device as resistive random access memory.
223 ching mechanisms that operate in redox-based resistive random-access memories (ReRAM) is key to contr
224                                              Resistive random-access memory (ReRAM) has been of wide
225         It consists of more than one million resistive random-access memory cells and more than two m
226 e development of new device concepts such as resistive random-access memory.
227                                          The resistive relative humidity sensor was developed using a
228                                          The resistive reserve ratio was significantly lower in the S
229                                          The resistive reserve ratio was similar in stable angina and
230                                          The resistive reserve ratio, a measure of the vasodilatory c
231 2 molecule for unusually high CO2 uptake and resistive sensing.
232  tuning pore geometry for the application in resistive-sensing and multipronged characterization of p
233 o a sensing space on top of a tunnel magneto-resistive sensor.
234     The system alternates or combines direct resistive sintering (DRS) and indirect resistive sinteri
235 irect resistive sintering (DRS) and indirect resistive sintering (IRS).
236 h as electrical discharge sintering (EDS) or resistive sintering (RS), have been intensively investig
237 debate about the nature of the field-induced resistive state and its implications for the 'normal sta
238                                 We model the resistive state as a vortex liquid with short-range d-wa
239  vortex can switch the whole junction into a resistive state at currents well below the Josephson cri
240 set' the magnetic anisotropy orientation and resistive state in the film, as well as to lower the mag
241 and stored in single devices as non-volatile resistive state transitions.
242 herefore, we propose that, in switching to a resistive state, the nanotube oxidizes by extracting oxy
243 e involved in switching the device to a high resistive state.
244 stance (NDR) and its derivative intermediate resistive states (IRSs) of nanocomposite memory systems
245 hat electrically pre-switched devices in low-resistive states comprise reduced disordered phases with
246 ety of designs are demonstrated, including a resistive strain gauge and an ionic cable.
247 oxygen loss, which leads to the formation of resistive surface layers on the cathode particles.
248                 A solid-state three-terminal resistive switch based on gate-voltage-tunable reversibl
249                                  Metal oxide resistive switches are increasingly important as possibl
250                                              Resistive switches are non-volatile memory cells based o
251 he conductance of silicon-rich silica (SiOx) resistive switches is quantised in half-integer multiple
252 ctrochemical devices, such as fuel cells and resistive switches, but these effects have remained larg
253  such as transistors, memories, sensors, and resistive switches.
254 varied behaviors including Ohmic conduction, resistive switching (memristor), and vestiges of quantum
255        The resetting behaviors of Pt/TiO2/Pt resistive switching (RS) cell in unipolar RS operations
256           In this paper, we present a unique resistive switching (RS) mechanism study of Pt/TiO2/Pt c
257     Ferroelectric polarization stability and resistive switching are strongly affected by a molecular
258                         Prevailing models of resistive switching arising from electrochemical formati
259 um oxide (HfO2) with excellent transparency, resistive switching capability, and environmental stabil
260 n solid-state memory devices, enabling their resistive switching capacity.
261                                  Oxide-based resistive switching devices are promising candidates for
262 ons as electrochemical storage materials and resistive switching devices follow from this abrupt chan
263                                    Nanoscale resistive switching devices, sometimes termed memristors
264 rtant step towards engineering more reliable resistive switching devices.
265                                              Resistive switching effects in dielectric-based devices
266 nd light illumination, can induce pronounced resistive switching effects.
267                          Polarization-driven resistive switching in ferroelectric tunnel junctions (F
268 intentional interface layer as the origin of resistive switching in Pt/Nb:SrTiO3 junctions.
269 l method to monitor the development of local resistive switching in TiO2-based devices.
270 he defect-based mechanisms that give rise to resistive switching is a major impediment for engineerin
271                                              Resistive switching is attractive because of, inter alia
272  deposition (iCVD) for polymerization of the resistive switching layer and inkjet printing of the ele
273 ting potential applications for SiO(x)-based resistive switching materials.
274              A detailed understanding of the resistive switching mechanisms that operate in redox-bas
275 he active and inert electrodes confining the resistive switching memory cell.
276                               An oxide-based resistive switching memory is engineered to emulate syna
277                       Pt/Ta2 O5 /HfO2- x /Ti resistive switching memory with a new circuit design is
278 aviors by integrating silicon oxide (SiO(x)) resistive switching memory with Si diodes.
279      We report lead-free ferroelectric based resistive switching non-volatile memory (NVM) devices wi
280                                              Resistive switching offers a promising route to universa
281 to gain new insights into the scaling of the resistive switching phenomenon and observe the formation
282 rm metallic filaments and participate in the resistive switching process, illustrating that there is
283                                          The resistive switching SET transition is modeled as hydroge
284                         In contrast to other resistive switching systems this quantisation is intrins
285  electrical behaviour demonstrated excellent resistive switching with high retention time, cyclic end
286 indings reveal the microscopic origin behind resistive switching, and also provide general guidance f
287                                  The bipolar resistive switching, with a concurrent capacitive contri
288  and related oxides studied for red-ox based resistive switching.
289 ms by which the interface layer controls the resistive switching.
290 0 K, validating the role of Joule heating in resistive switching.
291 ctroresistance effect is distinct from known resistive-switching or tunnel electro resistance.
292 cell body and the detachment/retraction of a resistive tail, thereby allowing these regions to underg
293 , we have found that long ONI wires are less resistive than OPI wires.
294                    We reversibly switch from resistive to conductive behaviour at charged walls in se
295 l tensile moduli suggest that the RDT is not resistive to pathologic disc displacement.
296 timal growth conditions to realize maximally resistive topological insulators.
297 iance from the Myotonometer measurements and resistive torques from the repeated passive stretch at v
298 slight curvilinearity, which is explained by resistive vessel distensibility.
299  LTM assembly that utilizes the principle of resistive wire heating and a temperature sensor to accur
300 e molecular-scale electronic components from resistive wires to reversible switches.

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