ライフサイエンスコーパス: oscillator

1 -level systems arising from quantum harmonic oscillators).

2 te cage and behaves as a heavy atom rattling oscillator.

3 rcadian processes or by a parasite-intrinsic oscillator.

4 lso pivotal in mediating light inputs to the oscillator.

5 oroplasts are gated by the nuclear circadian oscillator.

6 s extra perturbations to this basic epidemic oscillator.

7 ak the time-translation symmetry of a driven oscillator.

8 urons, including a subset called the evening oscillator.

9 ion of the molecular clock, a cell-intrinsic oscillator.

10 rtional to the number of charges on the nano-oscillator.

11 ting microwave cavity having the role of the oscillator.

12 ese quantum states in the case of a harmonic oscillator.

13 ring or synthetically constructed biological oscillator.

14 se rhythms are modulated by a circadian-type oscillator.

15 tical component of the mammalian respiratory oscillator.

16 e systems, including an autonomous molecular oscillator.

17 o changes in the frequency of the mechanical oscillator.

18 is also feeds back to regulate the circadian oscillator.

19 ypes of the composition and behaviour of the oscillator.

20 er convey photoperiod sensing to the central oscillator.

21 source of inhibitory drive to the expiratory oscillator.

22 nce in cycle period, on par with a circadian oscillator.

23 res associated with circadian and cell cycle oscillators.

24 emented as a simple Kuramoto model with four oscillators.

25 al response of individual hydroxy group (OH) oscillators.

26 ch as spin systems or macroscopic mechanical oscillators.

27 hip-scale quantum micro- and nano-mechanical oscillators.

28 typically require high-power lasers as local oscillators.

29 ive measurements of the motion of mechanical oscillators.

30 lecular mechanisms of stramenopile circadian oscillators.

31 lisecond scale may be modelled using coupled oscillators.

32 by using quantum dot microlasers as optical oscillators.

33 applicability to a number of other physical oscillators.

34 g capacitively coupled Vanadium Dioxide nano-oscillators.

35 ntralization in simulations of phase-coupled oscillators.

36 re very large numbers of nanoscale nonlinear oscillators.

37 artmentalised chemical networks and designed oscillators.

38 stablished processes such as coupling to X-H oscillators.

39 ches coupled to anharmonic metal-carboxylate oscillators.

40 large-scale phase synchronization of neural oscillators.

41 neuromorphic hardware based on magnetic nano-oscillators.

42 ir bundles may be regarded as nonisochronous oscillators.

43 stent with those generated by weakly coupled oscillators.

44 cent applicative developments of spin torque oscillators.

45 genstates that forms grid states of a single oscillator(2).

46 mobile electronics(1,2) and spin torque nano-oscillators(3-7) for neuromorphic computing(8).

47 ch motor cortex is best modelled as a neural oscillator, a conjecture that aligns well with current p

48 Synchronization of oscillators, a phenomenon found in a wide variety of nat

49 New findings demonstrate that the oscillator adjusts phase and period in response to abiot

50 RRs), essential components of circadian core oscillators, affect root meristem cell proliferation med

51 otor activity, the molecular clock in either oscillator alone is sufficient to rescue circadian locom

52 Recently, spin torque nano-oscillators also found use in microwave-assisted magneti

53 The circadian oscillator, an internal time-keeping device found in mos

54 rong but nonresonant interaction between the oscillator and an atom.

55 ct 1 Transistor-1 Resistor implementation of oscillator and bidirectional capacitive coupling allow s

56 this protocol with a trapped-ion mechanical oscillator and determined an increase by a factor of up

57 ntly limited by the phase noise of the local oscillator and Dick noise, but demonstrate the possible

58 zed mechanism that integrates the cell-cycle oscillator and embryo mechanics.

59 egg helped identify the cyclin-based mitotic oscillator and how this approach quickly merged with gen

60 n between glyphosate activity, the circadian oscillator and potentially auxin signalling.

61 Fs in mediating light input to the circadian oscillator and show how their regulation by GI is requir

62 our numerical simulations of a chaotic Hopf oscillator and suggest that chaos may be responsible for

63 how how it scales with the parameters of the oscillator and the driving.

64 reaction-diffusion model based on relaxation oscillators and couple this to a model for the mechanics

65 ock and cell cycle as interdependent coupled oscillators and identify DNA replication as a critical p

66 Synchrony between the different circadian oscillators and resonance with the solar day is largely

67 yme-free catalytic systems, all DNA chemical oscillators and the most complex molecular computers yet

68 face plasmon resonances coupled to nonlinear oscillators and the propagation of the electromagnetic w

69 or in communicating populations, a synthetic oscillator, and a trans-differentiation network.

70 itulate important in vivo phenomena, such as oscillators, and (2) perform complex tasks for synthetic

71 ng signals to contributing peripheral tissue oscillators, and are mediated by underlying changes in t

72 ynthetic dimensions, compact opto-electronic oscillators, and microwave-to-optical converters.

73 sets, called the Extended Circadian Harmonic Oscillator application, or ECHO.

74 This coupled cellular oscillator architecture permits stable and replicable en

75 ditionally stable motifs of the Phase Switch Oscillator are organized into an ordered sequence, such

76 Oscillators are at the heart of optical lasers, providin

77 erent taxa, the core components of circadian oscillators are not conserved and differ between bacteri

78 hemically coupled Belousov-Zhabotinsky micro-oscillators are studied in experiments and simulations.

79 nts provides the coupling force between both oscillators, arising as a fundamental requirement for sp

80 This simple "sizer-oscillator" arrangement reproduces the experimentally ob

81 his work demonstrates the capability of nano-oscillators as an useful tool for measuring the binding

82 is solution in brain-like systems of coupled oscillators as well as in high-density electrocortigraph

83 d the dynamics of a ring of quasi-sinusoidal oscillators at and beyond first order.

84 Synchronization of coupled oscillators at the transition between classical physics

85 lecular dynamics simulations using the Drude oscillator-based polarizable force field, quantum chemic

86 tion is normally entrained to the cell-cycle oscillator but can run autonomously of it-potentially ex

87 cern that what is measured is perhaps not an oscillator but is instead a sequence of evoked responses

88 The oscillator can have three stable states of period-3 vibr

89 uous-variable system-for example, a harmonic oscillator-can take advantage of hardware-efficient quan

90 emonstrate the implementation of a synthetic oscillator capable of keeping robust time in the mouse g

91 Lack of either results in a defective oscillator causing severely compromised output pathways,

92 On one hand, the circadian oscillators CCA1 and LHY regulate diurnal expression of

93 Along with free-running oscillator circuits, we measure repression response time

94 ak coupling can poise the system of unstable oscillators closer to the bifurcation by a shift in the

95 Although these cellular oscillators communicate, isolated mammalian cellular clo

96 In plants, the circadian oscillator contributes to the regulation of many aspects

97 cal model of the eardrums as noisy nonlinear oscillators coupled by the air within an animal's mouth.

98 from the transistor and progressing to ring oscillators, current-mirror circuits to toggle switches

99 Solutions are obtained within 5 oscillator cycles, and the time-to-solution has been dem

100 n the nucleus that are part of the circadian oscillator demonstrates a new role for the circadian sys

101 ng approximately nine generations, a dCas12a oscillator design with 40-nt CRISPR RNAs performed much

102 synchronization and robustness of a genetic oscillator distributed between two strains to spatial se

103 escribe the classical motion of a mechanical oscillator do not have a well defined energy, but are qu

104 ork of coupled degenerate optical parametric oscillators (DOPOs) to effectively find the ground state

105 onstrate the operation of a spin torque nano-oscillator driven by this SOT.

106 scape from a metastable state of a nonlinear oscillator driven close to triple its eigenfrequency.

107 ontinuous position measurement of a harmonic oscillator, due to backaction arising from quantum fluct

108 ns-morning oscillators (M cells) and evening oscillators (E cells)-are largely responsible for these

109 and small molecules with self-assembled nano-oscillators, each consisting of a nanoparticle tethered

110 s from a model of two coupled nonisochronous oscillators, each displaying a supercritical Hopf bifurc

111 ecular clock in both the morning and evening oscillators eliminates circadian locomotor activity, the

112 intrinsic spectral responses of isolated OH oscillators embedded in two cold (~20 K), hydrogen-bonde

113 he frequency autocorrelation) of a single OH oscillator, embedded in a water cluster held in a temper

114 of two opposite-phase coherent states in an oscillator encode a qubit protected against phase-flip e

115 The coupled oscillators exhibit stable limit-cycle oscillations and

116 Coupled oscillators exhibiting rich spatio-temporal dynamics hav

117 d in model organisms(1,2), whether a similar oscillator exists in humans remains unknown.

118 In their absence, the circadian oscillator fails to synchronize to the light-dark cycles

119 n addition, the dynamics of strongly coupled oscillators far from criticality suggested that individu

120 complex modulation of the conditional pF(L) oscillator for active expiration.

121 e development of a bioanalytical Wien-bridge oscillator for the fused measurement to lactate and gluc

122 ts based on spin waves, such as phase locked oscillators for neuromorphic computing, where the device

123 has been demonstrated to scale directly with oscillator frequency.

124 They are not only essential for the oscillator function but are also pivotal in mediating li

125 elation of phase fluctuations in any type of oscillator fundamentally defines its spectral shape.

126 s (Arabidopsis thaliana) plants in which the oscillator gene CIRCADIAN CLOCK ASSOCIATED1 (CCA1) was o

127 , we present the possibility for a synthetic oscillator generalizable across many organisms and readi

128 On the other hand, expression of circadian oscillator genes including CCA1 and LHY is associated wi

129 and to generate superpositions of a harmonic oscillator ground state and a number state of the form [

130 uster synchronization in networks of coupled oscillators ground on simplifying assumptions, which oft

131 Although this oscillator has been well-characterized in model organism

132 The clockwork of plant circadian oscillators has been resolved through investigations in

133 Until now, laser oscillators have been available only in the infrared to

134 Such oscillators have been refined in bacteria in vitro, howe

135 Synthetic gene oscillators have the potential to control timed function

136 ncy entrainment of two coupled physiological oscillators: i) the stimulus function and ii) the [Ca(2+

137 mechanism by which Suc affects the circadian oscillator in a GI-dependent manner was unknown.

138 Some studies hypothesize that an oscillator in auditory cortex could underlie important t

139 inating reaction rate using a protease-based oscillator in E. coli, we achieve D-xylonate productivit

140 We further reconstituted the calcium oscillator in HEK293 cells, supporting the model that Ca

141 tood as the damping of a stochastic harmonic oscillator in q space, which indicates that the suppress

142 e deployment of a precise engineered genetic oscillator in real-life settings.

143 Ablation of the Hes1 oscillator in stem cells interfered with stable MyoD osc

144 he endogenous period of the master circadian oscillator in the SCN.

145 ysis, we identified a role for the circadian oscillator in WUE.

146 l a unique platform for realizing mechanical oscillators in both classical and quantum regimes.

147 ay a role in synchronized motions of coupled oscillators in fluids, and understanding the mechanism w

148 ges the organization of endogenous circadian oscillators in human adipocytes, independent of SCN sign

149 chromatin modifications of central circadian oscillators in mammals and plants.

150 ddress the frequency spectrum of spin torque oscillators in the regime of large-amplitude steady osci

151 Furthermore, putative single-cell oscillators in the SFO and OVLT are strongly rhythmic an

152 scribes a set of interacting linear harmonic oscillators in thermal equilibrium.

153 the hypothalamus and it regulates circadian oscillators in tissues throughout the body to prevent in

154 sent a random network of heterogeneous phase oscillators in which the links mediating the interaction

155 exhibits a complete set of modes of coupled oscillators, including out-of-phase synchronization and

156 On E15.5, the fraction of competent oscillators increased dramatically corresponding with st

157 neuronal output pathway: distinct circadian oscillators independently drive a common pre-motor cente

158 viding insight in to how the plant circadian oscillator integrates with the biology of the cell and e

159 ion is accompanied by an increase of surface oscillator intensity with decreasing surface-to-volume r

160 The Arabidopsis circadian oscillator is a gene network which orchestrates rhythmic

161 The circadian oscillator is an important regulator of much of plant ph

162 We propose that the plant circadian oscillator is dynamically plastic, in constant adjustmen

163 quantum fluctuations that exist even if the oscillator is in its lowest possible energy state.

164 The field of miniature mechanical oscillators is rapidly evolving, with emerging applicati

165 omite formation is controlled by a molecular oscillator known as the segmentation clock(1,2).

166 errogation of the atomic system by the local-oscillator laser (Dick noise(5)) and by the standard qua

167 he BotC neurons interact with the expiratory oscillator located in the parafacial respiratory group (

168 n requires the recruitment of the expiratory oscillator located on the ventral surface of the medulla

169 o distinct clusters of clock neurons-morning oscillators (M cells) and evening oscillators (E cells)-

170 osophila, two corresponding circadian neural oscillators-M (morning) cells and E (evening) cells-exhi

171 We conclude that an intrinsic oscillator maintains Plasmodium's rhythmic life cycle.

172 Even wider ramifications of the Hechtian oscillator may implicate AGPs in osmosensing or gravisen

173 ated logic circuits such as seven-stage ring-oscillators, meeting the industrially needed device dens

174 use segmentation clock, suggesting that this oscillator might be conserved in humans(3).

175 imilar in the case of rhythmic input, but an oscillator might better provide the computational roles

176 , we characterised a low-frequency metabolic oscillator (MO-1) in skin from live wild-type and Nrf2(-

177 sed on spin density analysis, HOMA (harmonic oscillator model of aromaticity), NICS (nucleus-independ

178 t chemical shifts, NICS(1)(zz), and harmonic oscillator model of electron delocalization (HOMED) anal

179 In a previous large-scale nonlinear oscillator model of neuronal network dynamics, we showed

180 ed the feasibility of applying a limit-cycle oscillator model of the human circadian pacemaker to est

181 We report a phase oscillator model that permitted derivation of the ideal

182 itation can be represented using the Lorentz oscillator model, and discuss how these Lorentz paramete

183 illuminated with a classical double-harmonic-oscillator model, from which it is revealed that the com

184 ith theoretical calculations using a coupled oscillator model.

185 ons between arbitrary states of two harmonic oscillator modes and can be used to enact a deterministi

186 Oscillators near 3,400 cm(-1), however, occur with a sec

187 X-ray optical cavity and other parts of the oscillator needed for its realization, opening the way t

188 ack loop driving fungal and animal circadian oscillators, negative elements (FREQUENCY [FRQ], PERIODS

189 This work considers a second-order Kuramoto oscillator network periodically driven at one node to mo

190 ical component of the hypothalamic circadian oscillator network that times overt rhythms of physiolog

191 t is composed of a fully-connected 4-node LC oscillator network with low-cost electronic components a

192 lf-sustained Bmal1-dependent transcriptional oscillator network.

193 g analysis which suggests that large coupled oscillator networks may be used to solve computationally

194 useful for applications of coherent, coupled oscillator networks, for example in an all-optical coher

195 below the SQL after subtraction of the local-oscillator noise.

196 ven weak thermal fluctuations could make the oscillator nonlinear(10-13).

197 used in many devices such as high-frequency oscillators, nonvolatile memories, and magnetic field se

198 iscover that the system can act as a coupled oscillator, notably showing spontaneous in-phase synchro

199 noise and the spectrum on spin torque vortex oscillators, notably varying the measurement time durati

200 The posttranslational oscillator of the Kai system can be entrained by transie

201 mplitude and period variation in single cell oscillators of Neurospora crassa.

202 analog experiment in which seven electronic oscillators of three kinds are connected with two kinds

203 encoding various components of the circadian oscillator on whole plant, long-term WUE.

204 dynamics based on a system of coupled phase oscillators on a mammalian whole-brain network at the me

205 tested forty-four 2-um channel 5-stage ring oscillators on the same flexible substrate (1,056 TFTs).

206 g suggests that in progenitor cells the HES5 oscillator operates close to its bifurcation boundary wh

207 In this paper, we present a study of an oscillator operating in the 5- to 12-keV photon-energy r

208 ween chromatin modifiers and circadian clock oscillators orchestrates diurnal gene expression that go

209 ems with inducible RNA steps to compare with oscillator period times.

210 The ability to tune the oscillator phase provides new pathways for both engineer

211 neural circuitry by which distinct circadian oscillators produce specific outputs to precisely contro

212 ptical cavity, it is possible to build X-ray oscillators producing intense, fully coherent, transform

213 Circadian oscillator proteins are known to regulate the expression

214 lated behavior with a model consisting of an oscillator receiving its own delayed activity as input.

215 A subset of Pdf(+) neurons (the morning oscillator) regulates morning activity and communicates

216 The Drosophila circadian oscillator relies on a negative transcriptional feedback

217 a dyad as a unit consisting of two connected oscillators, representing intrinsic processes of percept

218 ses, which are crucial in the context of the oscillator's long term stability.

219 However, the attainable knowledge of an oscillator's motion is limited by quantum fluctuations t

220 because of the very large gain per pass, the oscillator saturates and reaches full coherence in four

221 systems (Hindmarsh-Rose neurons or Kuramoto oscillators), set to operate in a dynamic regime recogni

222 As the dimensions of a mechanical oscillator shrink to the molecular scale, such as in a c

223 f the time delay in the coupling between the oscillators, spiral wave core splitting at higher values

224 The exciton exhibits giant oscillator strength and absorption (over 30% for monolay

225 ed with intrinsic exciton properties such as oscillator strength and linewidth.

226 use of their large exciton binding energies, oscillator strength and valley degree of freedom, have e

227 Moreover, we can tune the relative oscillator strength by tuning the bilayer graphene bandg

228 ngendering low optical bandgaps and improved oscillator strength for their lowest-energy transition (

229 nteractions, leading to a small but non-zero oscillator strength in the charge-transfer state between

230 rization and the concomitant increase of the oscillator strength make excitation in the near-UV possi

231 ture is not identified probably due to lower oscillator strength of plasmon compared to the coronene.

232 S(2), that is, energy-level anticrossing and oscillator strength redistribution under a vertical elec

233 er Chl(D1) and Phe(D1) as well as one weaker oscillator strength state with molecular orbitals deloca

234 ty via redistributing high-energy absorptive oscillator strength throughout the visible spectral doma

235 idence of superradiance (including increased oscillator strength, bathochromic shift, reduced linewid

236 te singlet to excited-state triplets to gain oscillator strength, enabling triplets to be directly ge

237 Strikingly, we observe two high oscillator strength, low-lying states, in which molecula

238 reased singlet-triplet energy gaps, improved oscillator strengths and core rigidity compared to previ

239 d-state singlet-triplet energy gap with high oscillator strengths and minor reorganization energies.

240 Manipulating the oscillator strengths of radical cation transitions allow

241 The oscillator strengths of the DHP precursors to the helice

242 ecombination ( k(rad)) is calculated through oscillator strengths using SKSO basis.

243 However, in nonlinear oscillators, such as spin torque nano-oscillators, the f

244 ells do not seem to have intrinsic circadian oscillators, suggesting that rhythmic function might be

245 hermore, the effect of internal phase of the oscillator system on far-field thermal radiation is expe

246 eve precision measurements in other harmonic oscillator systems.

247 ty in [Formula: see text] Using tunnel diode oscillator (TDO) measurements, we find indications for p

248 al respiratory group, pFRG) is a conditional oscillator that drives active expiration during periods

249 The circadian clock is an intrinsic oscillator that imparts 24 h rhythms on immunity.

250 an extended solution of the fixed amplitude oscillator that incorporates the amplitude change coeffi

251 en tube tip growth based on a novel Hechtian oscillator that integrates a periplasmic arabinogalactan

252 lates its own synthesis by a Hechtian growth oscillator that regulates overall tip growth.

253 ansforms the Phase Switch into an autonomous oscillator that robustly toggles through the cell cycle

254 computational models of diffusively coupled oscillators that account for nuclear import, nuclear pos

255 in mutants implies the existence of multiple oscillators that act to normalize memory formation acros

256 s12a (dCas12a) to construct dynamic RNA ring oscillators that cycle continuously between states over

257 lation reactions catalyzed by the cell-cycle oscillator, the biochemical network controlling mitotic

258 nesis require coordination of the cell-cycle oscillator, the dynamics of the cytoskeleton, and the cy

259 Upon the binding of ligands onto the nano-oscillator, the oscillation amplitude will change.

260 linear oscillators, such as spin torque nano-oscillators, the frequency spectrum can become particula

261 including the components of these molecular oscillators, the function and mechanisms of action of ce

262 l qubits or larger dimensional modes such as oscillators, the individual elements in realistic device

263 to light: heterogeneity in the population of oscillators, the structure of the typical light phase re

264 results from the interaction of two distinct oscillators: the pre-Botzinger Complex (preBotC), which

265 by underlying changes in the local cellular oscillators themselves.

266 iance in the framework of the nonlinear auto-oscillator theory and deduce the actual frequency spectr

267 e obtained, while quasi-rigid rotor harmonic oscillator thermal contributions are important in improv

268 ioning, which is regulated by the cell-cycle oscillator through cortical contractility and cytoplasmi

269 nant sensors is implemented using a feedback oscillator to dynamically track variations in the resona

270 blue light in the response of the circadian oscillator to nicotinamide.

271 on as direct outputs from the core circadian oscillator to regulate the expression of PIF-DTGs throug

272 at ELF3 and GI are essential that enable the oscillator to synchronize the endogenous cellular mechan

273 es the way for incorporating hourglass based oscillators to be used as building block of future mecha

274 avior of a functional network of conditional oscillators to control zG layer performance and aldoster

275 l pattern from the interaction among coupled oscillators to generate a range of locomotion gait patte

276 Our work focuses on the use of coupled oscillators to represent neurons in areas generating pat

277 ory inhibition that restrains the expiratory oscillator under resting condition and regulates the for

278 TEMENT Interactions between multiple coupled oscillators underlie a three-part respiratory cycle comp

279 F, SCF-Cyclin F, and APC/C in regulating the oscillator underlying human cell cycles.

280 ytterbium (Yb)-doped femtosecond fiber laser oscillator using commercially-available parts (plus stan

281 nection between the circadian and cell cycle oscillators via CRY-modulated turnover of TLK2.

282 ene transcripts within the central circadian oscillator was upregulated and oscillated robustly in th

283 tigate temporal regulation in this molecular oscillator, we combined mouse genetic approaches and ana

284 ionships between metabolic and microvascular oscillators were examined during phenylephrine-induced v

285 log computing system with coupled non-linear oscillators which is capable of solving complex combinat

286 light phase response curve, the fraction of oscillators which receive direct light input and changes

287 adian rhythms are generated by the circadian oscillator, which provides a cellular measure of the tim

288 t reveal this noise-induced evolution of the oscillator while preserving the encoded information(3-7)

289 ormulation, discovering larger sets of known oscillators while avoiding the need for less interpretab

290 g of the self-sustaining molecular circadian oscillator, while research in nutrition science has yiel

291 It is driven by an oscillator whose various components are localized in the

292 Specifically, we consider oscillators whose phase dynamics and spatial dynamics ar

293 found by numerical simulations in a Duffing oscillator with a slowly periodically parametric excitat

294 fying coherent displacements of a mechanical oscillator with initial magnitudes well below these zero

295 e motional energy of a driven nanomechanical oscillator with sufficient sensitivity to resolve the qu

296 demonstrate an integrated circuit of thirty oscillators with highly reconfigurable coupling to compu

297 dentify a set of ultraprecise synthetic gene oscillators, with circuit variants spanning a 30-fold ra

298 We also established that the circadian oscillator within guard cells can contribute to long-ter

299 Here we show that the amplitude of intrinsic oscillators within macrophages and neutrophils is limite

300 stion as to what the spectrum of a single OH oscillator would be in the absence of thermal fluctuatio

301 Most OH oscillators yield single, isolated features that occur w