ライフサイエンスコーパス: initial state

1 hysteretic dynamics and a slow return to the initial state.

2 rious time points during the recovery of the initial state.

3 nal Schiff base, followed by recovery of the initial state.

4 al state to the uncorrected state and to the initial state.

5 scillating 180 degrees out of phase with the initial state.

6 tion state is less or more strained than the initial state.

7 tions are present even without Mg(2+) in the initial state.

8 e a system to one of its attractors from any initial state.

9 [Li(3)](+) that slowly reversed back to the initial state.

10 fects each genome differently based on their initial state.

11 ring the system parameters and the channel's initial state.

12 is relieved, representations revert to their initial state.

13 ned primarily by the binding energies of the initial state.

14 olving and robust to small variations in the initial state.

15 se ligands is required for the return to the initial state.

16 ntensity minima, the molecules remain in the initial state.

17 and preparation of the molecule into a pure initial state.

18 he conductance by about 50 % compared to the initial state.

19 n's activity in a manner that depends on its initial state.

20 py and entropy differences between final and initial state.

21 d of the experiment but was altered from its initial state.

22 ic signatures in late-time dynamics from all initial states.

23 des over up to 30 cycles for a wide range of initial states.

24 cles with optimal performance based on their initial states.

25 quantum bits (qubits), independent of their initial states.

26 teristic spatiotemporal response for generic initial states(7,9,10).

27 te(7,8) and adiabatic evolution from a known initial state(9,10).

28 f Watson-Crick pairs increases the number of initial states able to proceed to full hybridization, wi

29 mal configurations give insight into how the initial state affects the outcome of an epidemic, they a

30 me it takes for the plasma to recover to its initial state after perturbation by a wakefield.

31 Kinship distributions return to their initial state after the shock and as the original age st

32 rasing redundant information and recover the initial states after chip-to-chip teleportation.

33 rence values are independent of the system's initial state, although they do depend on the model's pa

34 either end of the microtubule network in the initial state and are subsequently released from this ac

35 halted and the system fully restores to its initial state and below which the system abruptly collap

36 onse to an action sensitively depends on its initial state and can display unpredictable, even chaoti

37 released, cortex either bypassed the normal initial state and immediately generated the pattern that

38 dynamical phase transitions on system size, initial state and other parameters.

39 ntly higher excess chemical potential in the initial state and stabilizes at the same time the charge

40 eriorhodopsin in which the structures of the initial state and the early intermediates (K, L and M1)

41 , and the greater the difference between the initial state and the end state of an object, the greate

42 We also analyze how the purity of the initial state and the Markovian or non-Markovian regimes

43 In the scheme, both the initial state and the measurement basis in the quantum p

44 chanism that produces one photon in the same initial state and the other in some standard polarizatio

45 he reduced coupling constant epsilon0 of the initial state and the system size L.

46 fference in ring-strain energies between the initial state and the transition state for ring-opening

47 e a scheme that can be used to determine the initial state and to classically command the system to e

48 andy repetition of the operations on various initial states and demonstrate by the reconstruction of

49 e subharmonic response is independent of the initial state, and experimentally map out a phase bounda

50 e itself provides a "synchronously prepared" initial state, and its relaxation to the resting state a

51 rent design choices, such as various mixers, initial states, and QRAO-specific implementations of the

52 y coat distinct materials to form prescribed initial states, and use thermal annealing to evolve thes

53 dral angles predicted by OPUS-RotaNN2 as its initial states, and uses OPUS-Fold2 to refine the side-c

54 r microscopic equilibration for a variety of initial states, and we apply single-site control to meas

55 Coexisting PBAs and total independence from initial states are found for subsets of parameter space.

56 GST-14-3-3 limited dephosphorylation (66% of initial state at 60 min) compared with GST alone (27% of

57 able historical effects between years in the initial state, at both phenotypic and karyotypic levels;

58 The global thermodynamic parameters from the initial state (backfolded Ly49 and m157) to the final st

59 the Hp-Hb binding appears to trap IsdH in an initial state before heme transfer.

60 d gum Arabic returns the ESR spectrum to its initial state before irradiation.

61 Particularly, the initial state (benzyl alcohol oxonium ion) is less stabi

62 er described by an exponential decay from an initial state, but by an escape from a potential well.

63 course, communities began to return to their initial state, but the return was often incomplete.

64 etermine whether M can be converted into the initial state by light.

65 Mature topography developed from this initial state by targeted axonal growth within the home

66 However, these initial states can be disrupted by rapid evolution of th

67 nic increase in conformational order from an initial state comprised primarily of monomers and small

68 The initial state comprises all necessary mineral nutrients

69 omerization and return of the protein to the initial state constitute the rate-limiting events in the

70 of protein conformational changes given the initial state crystal structure together with a small nu

71 tional change of a protein complex given its initial-state crystal structure together with a small se

72 appears to originate from nonlinearities and initial state dependence in the carbon cycle.

73 namics by elucidating and accounting for the initial-state-dependent prescaling effects.

74 t pap expression in uropathogenic E. coli is initial-state-dependent, as previously reported.

75 us visual perception belongs to the class of initial-state-dependent, robust, transient neural dynami

76 Because the initial states do not have this property, they can be sa

77 ntaneously stroke up by snapping back to its initial state, driven by elastic restoring force, withou

78 ropy of the titania support itself (i.e., an initial state effect) is deeply intertwined with the H*

79 ble system, which is highly sensitive to the initial state, enabling detection of quantum state displ

80 otoactivation, PAiRFPs slowly revert back to initial state, enabling multiple photoactivation-relaxat

81 Neonatal imitation illuminates how the initial state engenders and supports rapid social learni

82 he CO(2) reduction rate is controlled by the initial state entropy, which depends on the applied pote

83 tates at zero temperature as well as thermal initial state evolution at room temperature.

84 g the effects of surface adsorbates from the initial state for application-oriented nanointegration p

85 ansduction, and simultaneously recovered the initial state for catalytic signal amplification of ROS,

86 The initial states for transient and stable pores are differ

87 served in confined systems of rather chaotic initial states, for example, lattes formed by pouring es

88 Moreover, the initial state formed rapidly after the initiation of ref

89 ly pumped spin polarization is a nearly pure initial state from the ensemble.

90 lement transfer, the effect of selecting the initial state has also been studied.

91 Moreover, we have shown that the initial state (i.e., the first job) can have a significa

92 regardless of the charge distribution of the initial state, i.e., whether the positive charge is smea

93 eptor retained the binding properties of its initial state in retinal membranes.

94 entic O intermediate, before recovery of the initial state in the photocycle.

95 re-shell excitations from both B 1s and C 1s initial states in all three isomers of the dicarba-closo

96 They also inform the strategic design of initial states in social networks to maximally promote c

97 apply to any quantum system in an arbitrary initial state, in particular including non-equilibrium s

98 hat the phase factor regulating the system's initial state induces sharp drops in the propagation spe

99 type of bias represents an innate asymmetric initial state (initial expectation bias) while the other

100 antity which translates information about an initial state into the stationary state.

101 lectronic absorption technique for which the initial state is a deeply buried core level.

102 cific mutants indicates that recovery of the initial state is influenced by (1) residues such as Glu-

103 e weaknesses: a) the assumption of a singlet initial state is irreconcilable with known reaction path

104 useful when the a priori information on the initial state is not available.

105 e remains a longstanding challenge since the initial state is not recovered rapidly.

106 he 362 nm photoproduct is 13-cis whereas the initial state is predominantly all-trans.

107 n of the charge in the TS as compared to the initial state is probably at the origin of the observati

108 s paper, a method that is independent of the initial state is proposed.

109 step of the bacteriorhodopsin photocycle the initial state is regenerated from the O intermediate in

110 and instead occurs later in the cycle as the initial state is restored from the O intermediate.

111 As in Y83F, the recovery of the initial state is slowed several fold in Y83N.

112 nnually variability of salinity in the ocean initial states is either included or excluded, the salin

113 h represents the time taken to return to the initial state, is quantized as an integer multiple of th

114 Before recovery of the initial state, it will come to be represented entirely b

115 strate that quench dynamics from a polarized initial state lead to spin squeezing that improves with

116 ysis of vibronic coherences reveals that the initial state mixing is actively driven by a 193 cm(-1)

117 The initial state occupancies can be optimized from the fit

118 xpected if preparatory activity provides the initial state of a dynamical system whose evolution prod

119 ors in a society increasingly depends on the initial state of a few influential individuals.

120 on the role of the preparation stage of the initial state of a particle and on the interplay of cons

121 ption, but also allows a rapid return to the initial state of acetylation when targeting is removed.

122 LAR is a stable phenotype and not merely an initial state of AR.

123 This initial state of brain activity interacts nonlinearly wi

124 to a nontrivial equilibrium dependent on the initial state of cells in the highest telomere class.

125 verpotential, electrolyte concentration, and initial state of charge.

126 lt suggests that the OFC may reconstitute an initial state of collective influence when individual ac

127 In addition, the initial state of layer 5 pyramidal tract neurons contain

128 Finally, the initial state of nanoswitch was reset by addition of cyc

129 A positive correlation between the initial state of NE wrinkles, the unfolding of NE wrinkl

130 herently tunnel back and forth between their initial state of oscillatory motion (corresponding to an

131 p-coumaric acid (pCA) chromophore in pG, the initial state of PYP, results in the formation of pB, a

132 is introduced that allows discriminating the initial state of quenching, viz., the loose ion pair and

133 heir direction and magnitude correlated with initial state of release mechanisms.

134 tosolic Ca2+ concentration ([Ca2+]iini), the initial state of sarcoplasmic reticulum (SR) Ca2+ load (

135 ation of the (31)P nuclear spin to obtain an initial state of sufficient purity to create a non-class

136 model with history-dependent updates to the initial state of the accumulator.

137 als or crystals to glasses, depending on the initial state of the assembly and the illumination time.

138 We reasoned that changing the initial state of the brain (i.e., from quiescence to a m

139 e plasticity stable, i.e. insensitive to the initial state of the devices.

140 n the presence of its environment and by the initial state of the environment itself.

141 e can estimate the model parameters, and the initial state of the first transformed cell.

142 e text] to [Formula: see text], provided the initial state of the input qubit is known.

143 a particular state that depends only on the initial state of the inverse and forward models and on t

144 l inputs have been implicated in setting the initial state of the motor cortex(5,6), but they may als

145 h their final configuration dependent on the initial state of the network.

146 an INHIBIT gate, depending on the inputs and initial state of the photochromes.

147 cycles or that the outcome may depend on the initial state of the population - scenarios impossible w

148 er, while attack speed was unaffected by the initial state of the prey, accuracy dropped significantl

149 The synchronization is independent of the initial state of the system and is solely the result of

150 ding the timing of certain processes and the initial state of the system are satisfied.

151 bject depends on the assumptions made on the initial state of the system.

152 ach equivalence class, for any choice of the initial state of the system.

153 We find that a high-energy initial state of this system settles into frustrated, me

154 thway by which amphiphiles transform from an initial state of vesicles or micelles into such tubules

155 vidual systems are characterized by both the initial states of Abeta peptides and the P:L molar ratio

156 We show that, except for a set of initial states of measure zero, the environment always a

157 scription of the dynamics, provided that the initial states of the system and the environment are ind

158 uration of only one of the two complexes, at initial state or by switching, this approach enables a "

159 g achievable in the presence of noise in the initial state or the channel in some situations is impos

160 is impossible in the absence of noise in the initial state or the channel.

161 urtate cycloids are also traced by different initial states outside and inside of the rolling circle,

162 e at 60 min) compared with GST alone (27% of initial state; p < 0.01).

163 ther residues may be important in tuning the initial state pK(a) values of these groups and in mediat

164 systems towards this goal requires flexible initial state preparation, precise time evolution and ex

165 In the initial state, RG binds to DNA and unwinds ~2 turns of t

166 these quantum criterion is influenced by the initial state's purity (whether pure or mixed) and the n

167 We observe that a decrease in the initial state's purity corresponds to a reduction in bot

168 stallised oxide nanolites depending on their initial state, showing an increase of one order of magni

169 average prediction (2015-2019) from the 2013 initial state shows a transition to the positive phase o

170 ally thick liquid clouds with warming of the initial state--slows radiative cooling of the surface an

171 alent crosslinks preserves the memory of the initial state, so that much of the large deformation is

172 ique which projects the infinite dimensional initial state space to a finite-dimensional Euclidean sp

173 We also succeeded in measurements of L minus initial state spectra of BR-T, which are the first FTIR

174 ts selected by a fluctuation analysis of the initial state structures.

175 tructures has been attempted by preparing an initial state that favors the assembly of the required t

176 We have also applied our methods to initial states that are partially mixed.

177 The rate of the recovery of the initial state (the rate of the O --> BR transition) and

178 se observations are robust to changes in the initial state, the gas density, and the system size.

179 ticipated factors, such as the length of the initial state, the specific pattern that should be maint

180 With realistic salinity initial states, the tendency to decay of the subsurface

181 schemes train a loss function by sending an initial state through a parametrized quantum circuit, an

182 This allows the evolution of the initial state through unitary quantum gates, while using

183 and confirm that they are robust for generic initial states, thus showing the characteristic time-cry

184 a sequence of actions that takes us from an initial state to a desired goal state.

185 quantum mechanical particle can pass from an initial state to a final state along two possible paths,

186 sed effectively for endpoint changes from an initial state to a final state, such as in logic gates.

187 -dependent evolution from an easy-to-prepare initial state to a low energy state of a target Ising Ha

188 bset of its nodes, it can be driven from any initial state to any desired state in finite time.

189 ich can presumably exploit a fully entangled initial state to better explore the complex energy lands

190 a value determined by the properties of the initial state to purify.

191 tion of large-scale complex networks from an initial state to the desired state.

192 of cardiolipin during the reaction from the initial state to the equilibrium state.

193 port on all aspects of the evolution from an initial state to the final state.

194 erve the atomic structure evolution from the initial state to the low-resistance state (LRS) in the Z

195 ization that the step of activation from the initial state to the saddle point in PEL and the followi

196 ical dynamic scheme, our approach drives any initial state to the target state with 100% effectivenes

197 nd preserves the quantum correlations of the initial state up to a scaling factor.

198 upported by restoration of the system to the initial state upon subsequent oxygen treatment.

199 ion for predicting dissociation from a given initial state using kinetic equations.

200 reset the state of the entangled pair to its initial state using only local operations.

201 A dynamic NMR study of the initial state was performed, providing a detailed descri

202 For a range of initial states, we experimentally drive the ion-trap sys

203 For different initial states, we reveal universal scaling in the exper

204 Following fibrillation induction, 6 initial states were selected, and biphasic shocks (5-70

205 A primary ion qubit is prepared in an initial state, which is then encoded into an entangled s

206 egrees of freedom, preparation of a fiducial initial state with ion motion close to the ground state,

207 ctonic forcing drive landscapes away from an initial state with minimal topographic dissection, large

208 is observed by preparing an optimal quantum initial state with no excitation of the slowest decaying

209 on of three latitudinal tissue bands from an initial state with only two distinct cell types.

210 ly influence the efficiency of resetting the initial state, with higher stability devices ( 10 pN) re

211 ticed how two pendulums, regardless of their initial state, would synchronize. It is now known that t