戻る
「早戻しボタン」を押すと検索画面に戻ります。 [閉じる]

コーパス検索結果 (1語後でソート)

通し番号をクリックするとPubMedの該当ページを表示します
1  shown to determine the relaxation above the critical point.
2 onfigurations on either side of a mechanical critical point.
3 luid in the region close to the liquid-vapor critical point.
4 ula: see text] enclosing the nematic quantum critical point.
5  Many adaptive systems sit near a tipping or critical point.
6 cluding multi-stable behavior separated by a critical point.
7 als, revealing the existence of a mechanical critical point.
8 om being twice differentiable at an isolated critical point.
9 the complex phase diagram near the pseudogap critical point.
10 e4Sb12 is a known ferromagnet near a quantum critical point.
11 ce, through liquid-vapor coexistence, to the critical point.
12 y temperature and pressure ranges beyond the critical point.
13 ctivity being poised near an unusual kind of critical point.
14  that is typical of self-organization near a critical point.
15 rial near an itinerant ferromagnetic quantum critical point.
16  closer to the bifurcation by a shift in the critical point.
17 g it on the paramagnetic side of the quantum critical point.
18  parameter with the "time distance" from the critical point.
19 ls) in supercritical carbon dioxide near the critical point.
20 m in the free energy becomes singular at the critical point.
21 he dynamically generated length scale at the critical point.
22  electronic symmetry breaking at a concealed critical point.
23 nounced peaks and damping around the quantum critical point.
24 Chol mixture and predict the location of the critical point.
25 ompositions that are in close proximity to a critical point.
26 e scale invariance of an Ising magnet at the critical point.
27 trong fluctuations associated with a quantum critical point.
28 fective shear viscosity that diverges at the critical point.
29 g oscillatory approaches towards a depinning critical point.
30 al spin-singlet superconductivity across the critical point.
31 field even at T=0 K, that means at a quantum critical point.
32 hat are controlled by proximity to a quantum critical point.
33 e cluster growth can emerge at a non-trivial critical point.
34 omagnet CoNb2O6 (cobalt niobate) through its critical point.
35 the phase diagram is controlled by a quantum critical point.
36 the vicinity of an antiferromagnetic quantum critical point.
37 ctuation-dominated antiferromagnetic quantum critical point.
38 ersality class, like the ordinary liquid-gas critical point.
39 perties arise from the presence of a quantum-critical point.
40 ty of the superconducting state to a quantum critical point.
41 ing a phase transition to self-tune to their critical point.
42  malfunction of the entire road network at a critical point.
43 ch persists even in the approach to the bulk critical point.
44 sition and the proximity of this system to a critical point.
45 ons allows us to assess the closeness to the critical point.
46 r fluctuations shifts the system towards its critical point.
47 tatistical understanding of the liquid-vapor critical point.
48 pan multiple length scales in proximity to a critical point.
49  multiscale signatures of criticality near a critical point.
50 rical resistivity across the nematic quantum critical point.
51  instability in the molecular motion at this critical point.
52 or tuning appropriate materials to a quantum critical point.
53 why a system decreases the distance from the critical point.
54 Ginzburg-Landau, valid around a second-order critical point.
55 (WFM) which coexist with narrower minima and critical points.
56        A case is presented to illustrate the critical points.
57 hat characterize physical systems near their critical points.
58 for an asymptotically exact treatment of the critical points.
59  characteristic behavior of pressure-induced critical points.
60  of a system's constituents that emerge at a critical point(1).
61 lassic thermodynamic signatures of a quantum critical point(3-5), as observed in heavy-fermion(6) and
62                                      At this critical point, accessed by applying pressure to the str
63                                    Above the critical point, agents exploit incremental refinements t
64 rvation of T-linear resistivity at a nematic critical point also raises the question of whether stron
65 IM) and electron localization function (ELF) critical point analysis is reported for two types of lem
66 ation to accelerate both near the metastable critical point and almost everywhere below the fluid-flu
67  until now, a holistic understanding of this critical point and an empirical quantification of its dr
68 ics matched those expected near a liquid-gas critical point and described by the nearest-neighbor Isi
69         The presence or absence of a quantum critical point and its location in the phase diagram of
70       We discuss links between the dynamical critical point and quantum phase transitions, showing th
71 elds drive the system away from this quantum critical point and restore normal metallic behavior.
72 ecause of the strong coupling nature of this critical point and the "sign problem" plaguing numerical
73 llization in the vicinity of this metastable critical point and throughout the metastable fluid-fluid
74 ion of the chain encodes the position of the critical point and universal critical exponents, as well
75 tron-electron scattering) on approaching the critical point and, at the critical point itself, a stri
76 effects have revealed new classes of quantum critical points and are uncovering a plethora of new qua
77 its a rich phase diagram with at least three critical points and four thermodynamically distinct amor
78                                   We discuss critical points and pitfalls relating to optimization of
79  phase field, whereas disclinations arise as critical points and singularities in the phase field.
80 od minimizers without getting stuck in local critical points and such minimizers are often satisfacto
81 t weighting of material may be considered as critical points and were addressed in the present paper.
82 tate at low temperatures, locate the quantum critical point, and constrain the critical exponents.
83 phase transitions and the associated quantum critical points are a major field of research, but one i
84        nabla(2)rho values for the Cu-N2 bond critical points are analogous to those for polar closed-
85           We demonstrate that the additional critical points are part of the Ising universality class
86                                    A quantum critical point arises at a continuous transformation bet
87 ission is predicted to remain just below the critical point around Reff = 1.
88 ts a heavy-fermion antiferromagnetic quantum critical point as a function of either pressure or P/As
89 mes captured by simple models that feature a critical point as an attractor for the dynamics(10-15),
90 ence, and the contrast persisted through the critical point as shown by characteristic circle-to-stri
91 ts achieve an exceptional prediction for the critical point as well as agreement with previously publ
92 ty of multicomponent condensates have higher critical points as pure systems or, if pure LLPS is unfe
93 cs of typical gradient descent have the same critical points as the constrained problem.
94 d (ii) the vicinity of the classical jamming critical point, as the cross-over temperature gets lower
95  such as whether the brain is working near a critical point, as well as for applications including ad
96 tion of the observed intermediate, and their critical points, as well.
97 ong liquids turn out to lie the closest to a critical point associated with a rigidity or jamming tra
98                     We show that the quantum critical point associated with the melting of the spin-g
99 dditional examples of local types of quantum critical points associated with superconductivity, howev
100 angular correlation lengths at 298 K and the critical point at 227 K in supercooled water.
101 ching optimal doping, and suggests a quantum critical point at a hole doping of p(crit) approximately
102  both models have a metastable liquid-liquid critical point at deeply supercooled conditions and that
103       The hypothesis that water has a second critical point at deeply supercooled conditions was form
104 y of a field-tuned antiferromagnetic quantum critical point at Hc approximately 50 tesla.
105 se diagram of water exhibits a liquid-liquid critical point at positive pressure.
106 tions show that the existence of the quantum critical point at temperatures approaching zero affects
107 composition, they pass through a miscibility critical point at the transition temperature.
108 ions we propose that TatA assembly reaches a critical point at which oligomerization can be reversed
109 compensatory phase and heart failure and the critical point at which the transition occurs are emerge
110 ransition in the supercooled regime with the critical point at ~207 K and 50 MPa.
111                               Estimating the critical points at which complex systems abruptly flip f
112 ing systems might operate in the vicinity of critical points, at the borderline between order and dis
113   Adding a rotating driving field, we find a critical point attached to the number of driving cycles
114  well correlated with proximity to a quantum critical point, but the relative importance of quantum c
115 ment of T(c) near to a ferroelectric quantum critical point can arise due to the virtual exchange of
116 from the well-known fact that water near its critical point can solubilize silica.
117                These regimes correspond to a critical point changing type from an unstable node to an
118 n shows signs of metallic transport near the critical point characterized by a resistance , indicativ
119 In membranes quenched far from a miscibility critical point, circular domains nucleate and then progr
120 ial on the border of a ferroelectric quantum critical point comprising ferroelectric, quantum critica
121                  We further find that near a critical point (contact angle being ca. 153 degrees ) th
122                        As a consequence, the critical points correspond to minimum norm infima of the
123                                          The critical point corresponds to a self-dual structure with
124 nse of nano-architectures comprised of Drude-Critical Points (DCP) media (e.g., gold and silver) is p
125            Fluids cooled to the liquid-vapor critical point develop system-spanning fluctuations in d
126 n these contributions; and distance from the critical point (DFC) can be controlled through biologica
127 synthetic dinoflagellate were treated with a critical point drying protocol, transferred to a carbon
128                                    This is a critical point due to the difficulty of quantitative NH(
129 in response to ecdysone hormone signaling at critical points during development.
130 >0.95) are found between QTAIM metrics (bond critical point electron densities and delocalization ind
131        The Yb-Fe interaction energy and bond critical point electron density are slightly larger than
132 city was estimated as the difference between critical point elevations of recent and historic logisti
133                  In these systems, a quantum critical point emerges as external parameters (such as c
134 s that have been found to operate close to a critical point exhibit joint activations of large number
135 e precision of this experimental approach, a critical point for applications to metabolomics.
136 ional activation in eukaryotes, and thus the critical point for gene regulation, is unknown.
137 othesis predicts that cortex operates near a critical point for optimum information processing.
138 dered difficult to determine the location of critical points for real-world networks, and it is even
139                                   One of the critical points for the success of this research directi
140 mple of two interacting networks we find two critical points, four triple points, ten allowed transit
141 upercooled water is interpreted by adding a "critical point-free" scenario to the two competing scena
142 CeRhIn5 shifts its antiferromagnetic quantum critical point from 2.3 GPa to 1.3 GPa and induces a res
143                         Upon approaching the critical point from high temperature, the intensity of t
144 ypothesized the existence of a liquid-liquid critical point from which a dividing line separates two
145 ve Laplacian of electron density at the bond critical point further confirm the dative nature of the
146                                            A critical point has now been reached at which the analysi
147                                          The critical point Hc = 1/2 corresponds to a widely studied
148 nd CeRhIn5 is a rare example where a quantum critical point, hidden by a dome of superconductivity, h
149 nsitions are found, each of them ending in a critical point: (i) a fluid-fluid transition at higher d
150 rgue that the transverse-field-tuned quantum critical point in [Formula: see text] corresponds to bre
151 e scaling behavior associated with a quantum critical point in a correlated metal.
152 sponse functions converge on approaching the critical point in a single line, the Widom line.
153 sion of clinical studies, which are now at a critical point in determining their fate in RHT manageme
154 t a second-order differential at an isolated critical point in k-space, which we clearly distinguish
155  this process is initiated is likely to be a critical point in regulating endocytic activity spatiall
156  findings support the proposed liquid-liquid critical point in supercooled water in the No-Man's Land
157 s suggests that activation of caspase 8 is a critical point in the death decision process.
158  of the membrane, most dramatically near the critical point in the membrane phase diagram.
159 hat characterize the proximity of the second critical point in the miscibility phase diagram.
160 ility requires careful consideration at this critical point in the pandemic of coronavirus disease 20
161 quids, which become indistinguishable at the critical point in the supercooled phase.
162 om one phase to another, which occurs at the critical point in the two-channel structures with one-di
163  patients with mixed uptake, who may be at a critical point in their disease evolution.
164 ing the presence and the nature of a quantum critical point in their phase diagram is a central enigm
165 cussion of anomalies observed at the quantum critical point in this system.
166                                      The AIM critical points in 1 are relatively insensitive to the r
167 trol of superconductivity by tunable quantum critical points in CeRhIn5.
168  we review opportunities for intervention at critical points in developmental trajectories.
169 is complex should attack the pathogen at two critical points in its cycle.
170                          The multiplicity of critical points in our model allows it to adapt to diffe
171 peutics might be chosen that target genes at critical points in the commonly perturbed pathway(s) of
172 connectivity changes during infancy, marking critical points in the development of the brain's functi
173 among patients with cancer and fluctuates at critical points in the disease trajectory.
174 existence of phase boundaries and underlying critical points in the stripe and skyrmion phases.
175 types in the peripheral blood and identifies critical points in the transition from health to leukemi
176 ritical fluctuations associated to a quantum critical point, in the cuprates they remain undetected u
177 inuous quantum phase transitions, or quantum critical points, in a host of antiferromagnetic heavy-fe
178             In a fluid, when moving from the critical point into the single-phase region, the thermod
179 he development of the entropy as the quantum critical point is approached and to study the thermodyna
180                                         As a critical point is approached from either high or low tem
181                            In addition, as a critical point is approached from low temperature, the l
182 ppressed, i.e., as the ferroelectric quantum critical point is approached in a way reminiscent to beh
183 d absolute zero as the ferroelectric quantum critical point is approached.
184  deeply supercooled conditions and that this critical point is consistent with the three-dimensional
185 d to higher pressure, and the confined water critical point is correlatively shifted to lower tempera
186 order parameter that exhibits scaling at the critical point is generically missing in these systems.
187 Furthermore, we find that switching near the critical point is intrinsically stochastic and provide e
188 themselves to be poised in the vicinity of a critical point is lacking.
189                       Physics of the quantum critical point is one of the most perplexing topics in c
190 ndamental to all chemical processes, and the critical point is particularly important for supercritic
191           For smaller N, only the gap at the critical point is relevant, where it scales polynomially
192     The presence of a metastable fluid-fluid critical point is thought to dramatically influence the
193 re continuous phase transitions, or "quantum critical points" is a central topic of study in condense
194                                       At the critical point itself cerium lacks any compressive stren
195 n approaching the critical point and, at the critical point itself, a strictly T-linear resistivity t
196 tion (LLT) and a corresponding liquid-liquid critical point (LLCP) in supercooled liquid water remain
197 wo forms of liquid water and terminates at a critical point located at deeply supercooled conditions.
198 -liquid phase equilibria where the effective critical point may be reduced by tuning the structure of
199 etime at 227 K suggests that the supercooled critical point may correspond to a phase transition temp
200 at spin-fluctuations near a magnetic quantum critical point may provide an explanation for the superc
201                                          The critical-point model was used for the permittivity of si
202 t likely terminating into a crossover with a critical point near 30 GPa and 200 K.
203 -order liquid-liquid phase transition with a critical point near 48 GPa and 3,200 K that intersects t
204                          By operating near a critical point, neural circuits can maximize information
205                               At the quantum critical point, non-Fermi-liquid behaviour appears, whic
206 ly in a monotonic way even moving around the critical point, not only along isotherms or isobars.
207 tics have on the two-dimensional miscibility critical point observed in cell-derived giant plasma mem
208 pplied to the magnetic-field induced quantum critical point observed in YbRh(2)Si(2), for which we al
209 lts suggest that the transitional stage is a critical point of action of Act1 in the elimination of a
210 ticles was long predicted to appear near the critical point of an Ising chain.
211 ignaling in glioblastoma cells, clarifying a critical point of cross-talk between molecular signaling
212 A boundary-value problem for movement of the critical point of disconnection is established for an an
213 ested that each species may have a different critical point of failure.
214           The emergency department (ED) is a critical point of identification and treatment for some
215 ived ecto-mesenchymal cells, Tak1 provides a critical point of intersection in a complex dialogue bet
216 udies demonstrate that the PI3K pathway is a critical point of miRNA regulation of immune cell develo
217  equality for a quenching process across the critical point of second-order phase transitions, where
218 hen the global network dynamics operate at a critical point of state transition.
219                                       At the critical point of the dynamics, the rescaled average ava
220 ess, superconductivity occurs at the quantum critical point of the tin-doped metal.
221 the electronic conductivity, we estimate the critical point of the transition at temperatures near 2,
222  classes of Mobius transformations, with the critical point of the transition corresponding to the pa
223                               At the quantum critical point of the transition, finite-size effects le
224  (defects) and the traversal rate across the critical point of transition.
225                                       Hence, critical points of accessible systems (i.e., with just a
226 sing and regulated secretion of IL-1beta are critical points of control of the biological activity of
227                            We identify three critical points of failure in current informatic workflo
228                                     Defining critical points of modulation across heterogeneous clini
229                                    All three critical points of the evolutionary explanation proposed
230                                    Here, the critical points of the method were extensively revised,
231 advantage of the proximity of the metastable critical point on the crystallization rates.
232 e gamma-phase to the alpha-phase ending in a critical point (p C, V C, T C), unique among the element
233 troscopic evidence for two potential quantum critical points, p = 0.19 for the pseudogap phase and p
234 n the hyperfine shifts and the bond and ring critical point properties computed using atoms-in-molecu
235 atoms-in-molecules analysis reveals U-M bond critical point properties typical of metallic bonding an
236  16), and only small changes are seen in the critical point properties when the pi-electron count is
237 tuations around an antiferromagnetic quantum critical point (QCP) are believed to lead to unconventio
238 2)) allows one to study the putative quantum critical point (QCP) at low temperature and to understan
239 er superconductivity is favored at a quantum critical point (QCP) characterized by a divergent quasip
240                                    A quantum critical point (QCP) is currently being conjectured for
241 vity in a dome around the associated quantum critical point (QCP) near p(c) ~ 23 kbar.
242 des with the putative existence of a quantum critical point (QCP) near x approximately 0.14, as propo
243 modynamic properties when tuned to a quantum critical point (QCP), although the origins of such stran
244 metal, close to an antiferromagnetic quantum critical point (QCP).
245 tem that undergoes a transition at a quantum critical point (QCP).
246 s enter the critical dynamics near a quantum critical point (QCP).
247 m phase transition that happens at a quantum critical point (QCP).
248 rmetallics Yb2Pd2Sn, which shows two quantum critical points (QCP) under pressure and has been propos
249 comes almost gapless at the magnetic quantum critical point realized at Hc.
250 ctions that define a line emanating from the critical point, referred to as Widom line.
251                                       Such a critical point requires a line of classical phase transi
252 sed polymerases are above, near, and below a critical point, respectively.
253 ings demonstrate that proximity to a quantum critical point results in critical damping of the emerge
254 incompatible with existing pseudogap quantum critical point scenarios.
255 posits the existence of a new line above the critical point separating two physically distinct states
256                           For systems near a critical point small changes to component behaviour can
257 roach especially for on-site applications at critical points such as traffic stops and the workplace.
258                   For m = 1 we find that the critical point t(c) = 1 which is the maximum possible va
259 tion close to T = 0 is governed by a quantum critical point (T = 0, P = P(c)) at which the energy req
260 f density maxima of water, or emanate from a critical point terminating a liquid-liquid transition.
261 ion antiferromagnet CeRhIn5 toward a quantum critical point that becomes hidden by a dome of unconven
262 ressure presents a new type of naked quantum critical point that is free of disorder and symmetry-bre
263 ties of supercooled water may be caused by a critical point that terminates a line of liquid-liquid s
264        The state-transition model identified critical points that accurately predict AML development
265 al La(2-x)Ce(x)CuO(4) with a line of quantum critical points that surrounds the superconducting phase
266 uum theory (diffusion) and at a self-similar critical point (the Ising model).
267 o a percolation transition, wherein around a critical point, the addition of a small number of connec
268                        Near carbon dioxide's critical point, the addition to ethylene exhibits critic
269 seudogap phase of cuprates ends at a quantum critical point, the associated fluctuations of which are
270                           After crossing the critical point, the condensates manifest delayed growth
271                             Below the higher critical point, the condensation energy, obtained direct
272 ble presence of an incipient nematic quantum critical point, the doping dependence of the nematic flu
273        However, in the vicinity of a quantum critical point, the existence of quasiparticles comes un
274                           Across the quantum critical point, the low-temperature Hall coefficient und
275          In membranes close to a miscibility critical point, the two liquid phases in the membrane ar
276  of simple amorphous solids is governed by a critical point, the unjamming transition where the press
277 al systems (flocks and schools), sits near a critical point; the contributions individuals make to co
278 at the ability to systematically control the critical point, thereby preparing spatially inhomogeneou
279 y decision-makers with scientific experts at critical points throughout the regulatory process.
280                   These results indicate the critical point thymic function regulation by IGF-1 invol
281          These findings suggest that BNPP is critical point to future research.
282 s deduced from the immediate vicinity of the critical point to obtain predictions can lead to results
283                                          The critical point to this approach is the introduction of a
284 ted with both intra- and intermolecular bond critical points, topological bond orders, atomic charges
285            The beams' deformation beyond the critical point triggers a dynamic transition of the part
286 phase diagram topologies, including multiple critical points, triple points, and first-order transiti
287 hases and the possible presence of a quantum-critical point underneath the superconducting dome.
288 lains around 90% of the empirically observed critical point variation, making it therefore predictabl
289 turbations for a system in the vicinity of a critical point, we propose this information may be harne
290                                    This is a critical point when considering these molecules as thera
291     It exhibits two peaks, each located at a critical point where the Fermi surface of YBa2Cu3Oy is k
292                          The jury trial is a critical point where the state and its citizens come tog
293                             We are at a time-critical point where we can implement new capacity to re
294  the sample close to the topological quantum critical point, where the gate voltage reversibly drives
295                       The associated quantum critical point, which is "concealed" by the nematic phas
296 model ends in a finite-temperature dynamical critical point, which may be present in natural systems.
297 tinal circuits continued to operate near the critical point whose quantitative characteristics matche
298 es exhibit a consolution curve with an upper critical point, whose temperature and concentration decr
299 A subset of unstable vectors soften near the critical point, with a marked suppression in their chara
300 pment of wearable sensing tools represents a critical point within the security field, in order to pr

 
Page Top