ライフサイエンスコーパス: field theory

1 t allows expression of the cancer phenotype (field theory).

2 nctional theory together with dynamical mean-field theory.

3 erturbatively using methods from statistical field theory.

4 hese properties is achieved by using crystal field theory.

5 functional integrals as used in statistical field theory.

6 sional Van der Waals magnets using continuum field theory.

7 xtures was calculated using a molecular mean-field theory.

8 system, are obtained using a molecular mean-field theory.

9 ation effects were calculated using reaction field theory.

10 ion (Feynman diagrams) borrowed from quantum field theory.

11 predictions with available results from mean-field theory.

12 discuss its equilibrium properties via mean-field theory.

13 O)-bearing lipids by using single chain mean field theory.

14 Na+ and Cs+, was investigated using constant field theory.

15 T fusion using nuclear forces from effective field theory.

16 cting matter fermion sector in a parton mean-field theory.

17 ty and agree with predictions from a generic field theory.

18 acroscopic PRC (imPRC) within the exact mean-field theory.

19 nitio framework of nuclear lattice effective field theory.

20 tes formed by droplet microfluidics and mean-field theory.

21 uch as complete active space self-consistent field theory.

22 t can be understood within the Abelian Higgs field theory.

23 rahams) model], using cluster dynamical mean-field theory.

24 formed using cluster correction using random field theory.

25 or fields, which appears within relativistic field theory.

26 ples calculations and a self-consistent mean-field theory.

27 expensive algorithms such as self-consistent field theory.

28 and a generic lever rule acquired from mean-field theory.

29 cture for the dimensional cross-over to mean-field theory.

30 ree-nucleon interactions in chiral effective field theory.

31 us as a field in a nonrelativistic conformal field theory.

32 CDW ~ 20 , far beyond the prediction of mean-field theory.

33 nite temperature with cluster dynamical mean-field theory.

34 show how to describe dissipation in a scalar field theory.

35 imate using a classical Ising model and mean field theory.

36 c fluctuation expansion based on statistical field theory.

37 articles not present in relativistic quantum field theory.

38 l Hubbard model using cluster dynamical mean field theory.

39 ons were assigned with the aid of the ligand-field theory.

40 e calculations performed with Dynamical Mean-Field Theory.

41 Bell-Jackiw) anomaly investigated in quantum field theory.

42 emission spectroscopy and the dynamical mean-field theory.

43 earlier results obtained from dynamical mean-field theory.

44 for the application of metrology to quantum field theory.

45 rons is further refined using dynamical mean-field theory.

46 ed ensembles match predictions from rigorous field theories.

47 a result was previously only expected by the field theories.

48 ns as point charges consistent with the mean-field theories.

49 sociated QPTs and their underlying conformal field theories.

50 ars, from the quantum gap problem to quantum-field theories.

51 y numerical simulation of particle models or field theories.

52 m, in agreement with the predictions of near-field theories.

53 pen an avenue for quantum simulation of SUSY field theories.

54 s, to electromagnetism, classic, and quantum field theories.

55 On the basis of mean field theory, a transferable potential was designed to e

56 tify how time reversal symmetry is broken in field theories across scales.

57 alities such as the anti-de Sitter/conformal field theory (AdS/CFT) correspondence, where a higher-di

58 A thorough analysis, based on crystal field theory, allowed an unambiguous determination of al

59 However, predictions from neural field theory, an established mathematical framework for

60 Building on a dynamical-mean field-theory analysis of the ecological dynamics, an app

61 self-similar dynamics in nonequilibrium O(n) field theories and Bose gases, we find qualitatively dis

62 s allow us to go beyond standard topological field theories and engineer systems with Topological Qua

63 y establishing a direct link between quantum field theory and an experimentally measurable quantity,

64 in which a particle model is converted to a field theory and appropriate field operators are average

65 een cold-atom experiments and nonequilibrium field theory and are applicable to any study of universa

66 t are more compliant than those of both mean-field theory and computer simulations.

67 parameterize the model using self-consistent field theory and confirm its ability to make predictions

68 tional methodology based on multiplet ligand field theory and maximally localized Wannier orbitals be

69 hite, observed by AFM and reproduced by mean-field theory and MD simulation.

70 rify our predictions with previous effective field theory and model calculations of the (6)He[Formula

71 owerful model, based on self-consistent mean-field theory and molecular dynamics simulations, for lip

72 obial experiments with concepts from lattice-field theory and non-equilibrium statistical mechanics t

73 Lastly, we discuss applications in quantum field theory and quantum gravity, and implications for p

74 t of the universality predicted by classical-field theory and quantum Monte Carlo calculations.

75 d Hubbard model with cellular dynamical mean-field theory and show that both of these observations fo

76 rmal field theories in the algebraic quantum field theory and subfactor theory framework are formulat

77 Our measurements agree with a beyond-mean-field theory and support the expectation that the dynami

78 We present both an analytic mean field theory and supporting simulations showing that the

79 Here we derive the complete mean field theory and the lowest order second moment correcti

80 amental Belinfante's spin momentum, known in field theory and unobservable in propagating fields.

81 ar equations of state from relativistic mean field theory and weakly repulsive equations of state wit

82 ured by the analytical predictions of a mean field theory, and can be verified by calorimetric measur

83 nent had I-V relations described by constant field theory, and the conductance was reduced by acid an

84 erformed using Benjamini-Hochberg and random field theory, and the resulting accuracies were compared

85 er parameter(s) are described by a continuum field theory, and these dominate the physics near such p

86 Correction terms to the mean-field theory are computed and discussed.

87 nctions calculated within the dynamical mean-field theory are in excellent agreement with the experim

88 In contrast, the same problem expressed as a field theory (auxiliary field or coherent states) isolat

89 rges naturally from anti-de Sitter/conformal-field-theory based semi-holography.

90 A simple ligand field theory-based design principle for electrocatalysts

91 ere the metal cation is Cu(2+)), and polymer field theory-based simulations.

92 The serving algorithm of discrete field theories belongs to the family of structure-preser

93 tter realization of the anomalies in quantum field theories but also demonstrates the topological cla

94 mions that play an important role in quantum field theory but have never been observed as fundamental

95 Dynamical mean field theory calculation combined with density functiona

96 tems as exemplified by recent dynamical mean field theory calculations for delta-plutonium.

97 Self-consistent field theory calculations indicate the stability of HCP

98 Molecular field theory calculations recapitulated these findings a

99 Self-consistent mean-field theory calculations show that these, and other ass

100 Dynamical mean-field theory calculations suggest that the former anomal

101 density functional theory and dynamical mean field theory calculations to design a new class of Mott

102 gether with the findings from molecular mean-field theory calculations, suggests the coexistence of p

103 ensity functional theory, and dynamical mean-field theory calculations, we visualize a fourfold degen

104 l is dual to a (1 + 1)-dimensional conformal field theory (CFT) with central charge that depends on t

105 In each major theory of the origin of cancer-field theory, chemical carcinogenesis, infection, mutati

106 demonstrate the universality of relativistic field theory concepts, and offer a new platform for thei

107 l metamaterials will be governed by a scalar field theory, conformal elasticity, in which the nonunif

108 Effective field theory considering phonon renormalization in the s

109 the temporal lobes (temporal cortex: random field theory corrected; left amygdala: B, -0.237; P < .0

110 Utilizing dynamical mean-field theory, correlation signatures and damping in the

111 The anti-de Sitter (AdS)/conformal field theory correspondence or duality(1) is the princip

112 We used the anti-de-Sitter/conformal field theory correspondence to identify a class of non-F

113 Self-consistent field theory data presented here qualitatively reproduce

114 The images corrected by random field theory demonstrated improved classification accura

115 try to prior predictions from dynamical mean-field theory demonstrates that the hole concentration p

116 We derive the low-energy field theory describing a non-BCS fermionic superfluid p

117 of Wen-Zee terms in the topological quantum field theory describing the phase.

118 An approach to bridging the phenomenological field theory description of phase separation in binary m

119 We use a self-consistent mean-field theory, designed to investigate membrane reshaping

120 we use the density functional dynamical mean-field theory (DFDMFT) scheme to comprehensively explain

121 ensity functional theory plus dynamical mean-field theory (DFT + DMFT) to iron and find that at high

122 s paper presents one such model, the dynamic field theory (DFT) of spatial cognition, showing new sim

123 ociated with deviation from the classic mean-field theory, dielectric critical exponent anomalies and

124 me implements non-equilibrium dynamical mean field theory (DMFT) and uses a digital quantum simulator

125 ely consistent with our DFT + dynamical mean field theory (DMFT) results, both showing a continuous t

126 sion spectroscopy (ARPES) and dynamical mean field theory (DMFT).

127 ntial approximation (CPA) and dynamical mean field theory (DMFT).

128 sponse, which is contained in dynamical mean-field theory (DMFT).

129 al theory (DFT) combined with dynamical-mean-field theory (DMFT).

130 ing state-of-the-art embedded dynamical mean field theory (eDMFT).

131 investigate a chiral spin-chain, whose mean field theory effectively captures the behavior of Dirac

132 Non-Abelian topological quantum field theories exhibit the mathematical features necessa

133 esting that Poisson-Boltzmann and other mean-field theories fail for higher valency cations where ion

134 This continuum density field theory features two-dimensional parity symmetry br

135 se theorems to the full framework of quantum field theory, finding that theories with classical gravi

136 To explain these findings we present a mean-field theory for [Formula: see text], which is based on

137 on, we develop a non-stationary dynamic mean-field theory for driven networks.

138 isfactorily described by the self-consistent field theory for end-grafted polymer brushes.

139 The spectra reproduce the high-field theory for free hydrogen, with quadratic Zeeman sp

140 ses of the hybrids, we have developed a mean field theory for mixtures of soft, flexible chains and h

141 Furthermore, we derive an effective field theory for the field-induced critical point which

142 We develop a mean-field theory for the network, which shows how irregular

143 nteracting, 2D antiplane cracks obeys a mean-field theory for which the mean field on a crack inserte

144 We report a simple model, unconnected to field theory, for a compacted dimension realized in a me

145 ar, the learning algorithm learns a discrete field theory from a set of data of planetary orbits simi

146 The learning algorithm trains a discrete field theory from a set of observational data on a space

147 To explain these findings, we propose a mean-field theory from which we obtain a scaling relation bet

148 bifold of a given unitary rational conformal field theory generates a unitary modular category.

149 Here we connect concepts from lattice field theory, graph theory, and transition rate theory t

150 In parallel, topological field theory has opened the doors to the formulation and

151 e apparent that N = 2 supersymmetric quantum field theory has something to do with cluster algebras.

152 iginally developed in the context of quantum field theory, has been investigated on distinct photonic

153 ct of the connection: supersymmetric quantum field theories have associated hyperkahler moduli spaces

154 Effective field theories have emerged as the dominant approach to

155 Inspired by field theory, here we develop a second-quantized MBD for

156 alogue of the Schwinger mechanism in quantum field theory; here they appear as a quantum phase transi

157 on-semisimple analogs of topological quantum field theories in 2 + 1 dimensions.

158 such an approach by mapping strongly coupled field theories in D dimensions into weakly coupled quant

159 for machine learning and serving of discrete field theories in physics is developed.

160 The unitary rational orbifold conformal field theories in the algebraic quantum field theory and

161 by the uranium center using ab initio ligand field theory in combination with the angular overlap mod

162 sful in verifying key predictions of quantum field theory in curved spacetime(7-11).

163 en concentrations follow predictions of mean-field theory in disordered films and show suppression of

164 imation of parameters that appear in quantum field theory including proper times and accelerations.

165 retically modelled within the Dynamical Mean Field Theory, including the core-hole interaction.

166 nitio calculations based on chiral effective-field theory interactions and the quasi-particle random-

167 We use high-fidelity chiral effective field theory interactions(17,18) and find good agreement

168 sented by a Berry-phase term in an effective field theory, intrinsically intertwine the different ord

169 mplex recovers the usual topological quantum field theory invariants of W.

170 a's approach to the formulation of conformal field theories is combined with the formal calculus deve

171 graph construction method based on electric field theory is applied which specifically deals with co

172 the fundamental principles on which quantum field theory is constructed.

173 Self-consistent field theory is employed, and both standard and alternat

174 of his Green's functions methods in quantum field theory is placed in historical context.

175 A remarkable prediction of quantum field theory is that there are quantum electromagnetic f

176 Self-consistent field theory is used to determine structural and energet

177 al-density-approximation plus dynamical mean-field theory (LDA+DMFT) we characterize its paramagnetic

178 of electrostatics in water is based on mean-field theories like the Poisson-Boltzmann formalism and

179 done within the framework of local molecular-field theory (LMFT), which provides a well-controlled me

180 an iterative scheme, where at each step mean field theory methods at finite "temperatures" are used f

181 preciable deviations from the classical mean-field theory (MFT) of this type of front propagation.

182 In contrast, simple mean field theory (MFT) predicts that x = 3 and x = 2.

183 cate that curvature coupling, along with the field theory model for composition free energy, gives do

184 of giant unilamellar vesicles using a Landau field theory model for phase coexistence coupled to elas

185 tion of a strong segregation self-consistent field theory model with a multilayer optical framework.

186 rmation as elucidated by our self-consistent field theory modeling, from which we exclude Langmuir ad

187 On the basis of the ligand field theory, most fluorescence spectral peaks could be

188 re, we propose a unifying framework for mean-field theories of asymmetric kinetic Ising systems from

189 Mean field theories of ion distributions, such as the Gouy-Ch

190 Using the nonlinear field theories of mechanics supplemented by the theory o

191 ties of the material would then need quantum field theories of objects such as textures and strings,

192 ear interactions were derived from effective field theories of quantum chromodynamics.

193 t this is equivalent to the respective class field theories of the curves being isomorphic as dynamic

194 archical geometric model founded on the mean-field theory of 2D polygonal tessellations to predict ex

195 ysis of the Landau-Ginzburg-Wilson effective field theory of a classical incommensurate CDW in the pr

196 ic facilitation in the framework of the mean-field theory of glasses.

197 Here we develop an advanced phase-field theory of melting coupled to mechanics, which reso

198 endent cutoff, in agreement with recent mean-field theory of slip avalanches in elasto-plastic materi

199 We develop a full microscopic replica field theory of the dynamical transition in glasses.

200 Although the mean-field theory of the glass transition--like that of other

201 e suggest Gaussian approximation to the mean-field theory of the second-order phase transition to exp

202 This is a scalar phi(4) field theory (or phase-field model) that minimally viola

203 me of our findings can be understood by mean-field theory, others show breakdown of this picture, hig

204 The approach of learning discrete field theories overcomes the difficulties associated wit

205 Mean field theories predict an asymptotic scaling state with

206 low the interaction energy scale, where mean-field theory predicts an ordering transition.

207 Quantum field theory properly incorporates quantum theory and re

208 Thus, we directly observe these fundamental field theory properties as microscopic mechanical proper

209 ve phenomena in strongly-interacting quantum field theories (QFTs).

210 sing extensive simulations and quenched mean-field theory (QMF), focusing on structures with a connec

211 le' properties of light and of a fundamental field-theory quantity, which was previously considered a

212 Self-consistent field theory rationalizes the thermodynamic stability of

213 Quantum field theory reconciles quantum mechanics and special re

214 Self-consistent field theory reinforces these observations and predicts

215 argued, on the basis of comparison with mean-field theory results for chiral diblock copolymer melts,

216 Complementary self-consistent field theory (SCFT) predicts multilayer brush morphologi

217 mergent phases, we implement self-consistent field theory (SCFT) simulations and a strong-stretching

218 description, as captured in self-consistent field theory (SCFT).

219 oughput computation based on self-consistent field theory (SCFT).

220 lations performed using self-consistent mean field theory (SCMFT) account for the preferred self-asse

221 The resulting Pauli-Fierz quantum field theory serves as a cornerstone for the development

222 mplectic capacities from rational symplectic field theory (SFT).

223 Effective field theory shows that this topology stabilized order i

224 fluid helium as a finite-temperature quantum field theory simulator for rotating curved spacetimes(19

225 ese intuitive expectations are based on mean field theories, such as the Poisson-Boltzmann formalism,

226 Quantum field theory suggests that electromagnetic fields natura

227 Self-consistent mean field theory suggests this rich self-assembly behavior i

228 complex networks, we successfully build mean-field theory that accurately predicts both milling state

229 ctrostatic analysis based in local molecular field theory that affords a clean separation of long-ran

230 Quantum electrodynamics (QED), the quantum field theory that describes the interaction between ligh

231 bipolar bolalipids was studied using a mean field theory that explicitly includes molecular details

232 ompare with except those from dynamical mean-field theory that suggest epsilon-plutonium is mechanica

233 ic structure method, based on dynamical mean-field theory, that enables interpolation between the ban

234 According to quantum field theory the signal photon is then in a coherent sup

235 iginally developed in the context of quantum field theory, the concept of supersymmetry can be used t

236 In advanced field theories, there can be more than four dimensions t

237 the diffuse distributions predicted by mean field theory, thereby confirming a common prediction of

238 thermostatistics to extend the range of mean-field theory, thereby eliminating the need for a separat

239 onnects the microscopic couplings in quantum field theories to macroscopic observations of neutron st

240 tion into a design strategy by applying mean-field theory to a structure-based computational model to

241 a general framework based on local molecular field theory to accurately determine the contributions f

242 Hubbard model with plaquette dynamical mean-field theory to address these unusual features and relat

243 Here we develop a mean-field theory to address this challenge, and demonstrate

244 We use stochastic neural field theory to analyze the stimulus-dependent tuning of

245 s of fundamental physics models from quantum field theory to cosmology.

246 In this study, we first use mean-field theory to demonstrate that a combination of homeos

247 We use lattice effective field theory to describe the low-energy interactions of

248 We use self-consistent field theory to determine structural and energetic prope

249 arametric maps, implementing Gaussian random field theory to estimate inter-voxel dependencies.

250 We use phase-field theory to model and describe these non-equilibrium

251 uch as complete active space self-consistent field theory to multiple molecular fragments via a produ

252 serving algorithm uses the learned discrete field theory to predict new observations of the field fo

253 in a variety of fields, ranging from quantum field theory to quantum information science to condensed

254 We develop a mean-field theory to show that, in order to understand the fi

255 troscopy and state-of-the-art dynamical mean-field theory to show the importance of the crystal latti

256 se numerical simulations and self-consistent field theory to study the deformation behaviour of a sin

257 We employ self-consistent field theory to study the thermodynamics of membrane-par

258 We use the dynamic field theory to test the proposal that infants encode lo

259 reasons are given for preferring the unified field theory to the building block model.

260 r-theory computations using chiral effective field theory, to constrain the neutron-star equation of

261 how this new theory, the tissue organization field theory (TOFT), can help chart a path to progress f

262 Here, we present a dynamic mean-field theory together with comprehensive computer simula

263 loer theory is a kind of topological quantum field theory (TQFT), assigning graded groups to closed,

264 onventionally, calculations in QED and other field theories treat incoming particles as single-moment

265 Using mean-field theory, we derive a low-dimensional description of

266 By means of a perturbative field theory, we derive relevant observables in closed f

267 By employing parton mean-field theory, we discuss the nature of these correlated

268 In quantum field theory, we learn that fermions come in three varie

269 sing molecular dynamics simulations and mean-field theory, we show that at a critical strain amplitud

270 Using nonequilibrium dynamical mean field theory, we show that suitably designed chirped pul

271 lo simulations of lattice-polymers with mean-field theory, we show that the sequence of heterotypic b

272 inciples band structure calculation and mean-field theory, we unambiguously establish that the superc

273 Our observations are compared with mean-field theory where the coupling strength between atomic-

274 re for them, is based on topological quantum field theories, which rely on the existence in Nature of

275 electron materials, based on Dynamical Mean Field Theory, which can predict the change of the crysta

276 t analogy to the well-known Onsager reaction field theory, which has been successful in predicting vi

277 then demonstrate that the complete effective field theory-which includes all the soft modes and the r

278 sition to dynamical arrest predicted by mean-field theories while also being strongly influenced by i

279 ds are described via elasticity, a classical field theory whose form is constrained by translational

280 ate coupling within a cluster dynamical mean-field theory with a numerically exact quantum impurity s

281 pic model of SCO materials combining crystal field theory with elastic intermolecular interactions.

282 ll these lattices is a conformally invariant field theory with holographic properties (characteristic

283 cattering probabilities in a massive quantum field theory with quartic self-interactions (phi(4) theo

284 tified expectation values in a certain SU(2)-field theory with values of the Jones polynomial that ar

285 Using dynamical mean-field theory, with cross-region currents as order parame

286 romagnetic behaviour occurs), classical mean-field theory yields the Curie-Weiss law for the magnetic