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 c fluctuation expansion based on statistical field theory.

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

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

5 ation effects were calculated using reaction field theory.

6 articles not present in relativistic quantum field theory.

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

8 discuss its equilibrium properties via mean-field theory.

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

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

11 l Hubbard model using cluster dynamical mean field theory.

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

13 e calculations performed with Dynamical Mean-Field Theory.

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

15 emission spectroscopy and the dynamical mean-field theory.

16 earlier results obtained from dynamical mean-field theory.

17 for the application of metrology to quantum field theory.

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

19 nctional theory together with dynamical mean-field theory.

20 erturbatively using methods from statistical field theory.

21 hese properties is achieved by using crystal field theory.

22 functional integrals as used in statistical field theory.

23 ed ensembles match predictions from rigorous field theories.

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

47 Molecular field theory calculations recapitulated these findings a

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

106 Quantum field theory properly incorporates quantum theory and re

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

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

109 Quantum field theory reconciles quantum mechanics and special re

110 Self-consistent field theory reinforces these observations and predicts

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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