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The glassy random laser: replica symmetry breaking in the intensity fluctuations of emission spectra.Noise Enhances Action Potential Generation in Mouse Sensory Neurons via Stochastic ResonanceNoise in multiple sclerosis: unwanted and necessary.Small-cluster renormalization group in Ising and Blume-Emery-Griffiths models with ferromagnetic, antiferromagnetic, and quenched disordered magnetic interactions.Nonequilibrium and information: the role of cross correlations.Fluctuation relation for weakly ergodic aging systems.Statistical mechanical approach to secondary processes and structural relaxation in glasses and glass formers: a leading model to describe the onset of Johari-Goldstein processes and their relationship with fully cooperative processes.Thermodynamic first order transition and inverse freezing in a 3D spin glass.Spin-glass complexity.Chaos in temperature in the Sherrington-Kirkpatrick model.Analysis of the infinity-replica symmetry breaking solution of the Sherrington-Kirkpatrick model.Effective action method for the Langevin equation.Applying algorithmic complexity to define chaos in the motion of complex systems.Predictability in the large: an extension of the concept of Lyapunov exponentViolation of the fluctuation–dissipation theorem in glassy systems: basic notions and the numerical evidenceStrongly intermittent chaos and scaling in an earthquake modelFollowing states in temperature in the sphericals+p-spin glass modelGeneral Phase Diagram of Multimodal Ordered and Disordered Lasers in Closed and Open CavitiesSpectrum of large random asymmetric matricesIntermittency and predictability in turbulenceRandom transfer matrices for the overlap in disordered systemsDiffusion limited growth in systems with continuous symmetryBroken ergodicity and glassy behavior in a deterministic chaotic mapGrowth of Noninfinitesimal Perturbations in TurbulenceDynamics of spin systems with randomly asymmetric bonds: Langevin dynamics and a spherical modelDynamics of spin systems with randomly asymmetric bonds: Ising spins and Glauber dynamicsLyapunov exponent for products of Markovian random matricesLocalization properties of the one-dimensional Anderson model with a self-similar random potentialPair dispersion in synthetic fully developed turbulenceProducts of random matrices for disordered systemsComplexity in quantum systemsStatistical mechanics of shell models for two-dimensional turbulencePredictability in systems with many characteristic times: The case of turbulenceGrowth kinetics in a phase field model with continuous symmetryFirst-order phase transition and phase coexistence in a spin-glass modelStable solution of the simplest spin model for inverse freezingSpherical 2 + p spin-glass model: an exactly solvable model for glass to spin-glass transition
P50
Q35855065-7C2B14DC-F1E0-4E7D-B6D8-BAC8774CE885Q36104046-B111EE63-4C31-4412-8B5A-D6713CE8BD85Q38263875-1F4E0C98-20A3-4BA0-8D04-524677CD1074Q47739909-CF293020-1946-416D-A274-87C54EAA6412Q50936543-B9532093-C7A1-4AD1-803E-AA302F4A7233Q51248058-1ACDF2D1-F4B4-43B3-A7C6-DBF97A7FA42BQ51529095-B68AC7CE-4EC6-4D2D-8D02-61D9B711CB0CQ51707547-2BE5ADCC-6E18-4FF9-BC87-4849FF102E70Q51999207-5B02A768-72F1-460B-BD37-3A8ED1247F61Q52018551-B400C152-9800-4D57-913E-2905DFBCC7FDQ52040651-8769B52E-D2C6-4B6F-85DE-0F2116FCB332Q52341844-F266A449-37EF-4245-AE80-2D69522D4813Q52371473-B7059177-84EA-4263-B17A-621C035D6B39Q56144177-2238B9A3-52C5-48CA-8350-89D526C92FC5Q56337127-4A79F459-7474-412C-BFB2-B49B0811A4E3Q57134023-97DE4386-121B-4A69-A7AB-2A19134A2AD7Q59460101-B688E98C-1FA6-43CF-AE49-CC30C05A70F0Q60180824-A3AFAD2A-356C-46EC-BDAF-02DCFCF5213BQ74486202-DA85E13A-993F-4484-A30E-D95775B3E66AQ74535659-9717BC58-5C65-487F-9638-1ED7CD0FDB2FQ74543478-53279477-0303-414D-86A2-8143AA214227Q74560834-92D783E5-4C06-4299-877F-F6F34CE3F236Q74568899-52553A76-3F69-4D05-87AA-14BC5E1ADAFDQ74576291-8F0C1583-7C1F-42E7-B6C3-811CF585DDEDQ77827929-3AA24DB2-D5F1-45A5-B9DA-30EDC98AC830Q77831026-E663D219-F745-4104-B2A7-780F8B86965FQ77837114-8575AA97-EEFC-43DC-A9C2-1873A4D75B0FQ77985076-F42D7353-32D6-447B-80A1-BC987CFB1CC9Q77994749-6969697B-9DE3-4309-AE2F-CF8C8BCF7D53Q78060744-2A30D768-97FF-4F1C-9F08-B07B2FABB081Q78063455-1B7670EF-FF86-4164-B53C-2859857FB51EQ78066501-B4A8591A-4944-4C26-B96F-68B6CF6CDBB8Q78076211-19C265C7-6E33-4628-9C28-A23931B4537CQ78078496-A9A7583F-04C5-4BE6-B7C9-4D9DE50B1BD1Q78671712-DAAC47C4-4BA2-46E3-AF99-4066BFA392BDQ81291185-DF684E5A-BB17-454A-AEFA-DBAC3ADBE100Q94417812-D7ED3A5F-DB28-4B6C-9CE2-B303D0AC9272
P50
description
researcher
@en
wetenschapper
@nl
հետազոտող
@hy
name
Andrea Crisanti
@ast
Andrea Crisanti
@en
Andrea Crisanti
@es
Andrea Crisanti
@nl
type
label
Andrea Crisanti
@ast
Andrea Crisanti
@en
Andrea Crisanti
@es
Andrea Crisanti
@nl
prefLabel
Andrea Crisanti
@ast
Andrea Crisanti
@en
Andrea Crisanti
@es
Andrea Crisanti
@nl
P1053
C-1705-2016
P106
P1153
7006134060
P31
P3829
P496
0000-0002-9869-4420
P569
2000-01-01T00:00:00Z