... link to RLJ home ... see also Google Scholar, and Bath Uni Opus repository. [68] R. L. Jack, M. Kaiser, and J. Zimmer, arXiv:1709.04771. Symmetries and geometrical properties of dynamical fluctuations in molecular dynamics
[67] M. Kaiser, R. L. Jack, and J. Zimmer, arXiv:1708.01453. Canonical structure and orthogonality of forces and currents in irreversible Markov chains
[66] L. O. Hedges, H. A. Kim, and R. L. Jack, J. Comp. Phys. Stochastic level-set method for shape optimisation,
arXiv:1612.04681.
[65] T. Nemoto, R. L. Jack, and V. Lecomte, Phys. Rev. Lett. Finite-size scaling of a first-order dynamical phase transition: adaptive population dynamics and an effective model,
arXiv:1611.08239.
[64] M. Kaiser, R. L. Jack, and J. Zimmer, J. Stat. Phys.
Acceleration of convergence to equilibrium in Markov chains by breaking detailed balance,
arXiv:1611.06509.
[63] A. Razali, C. J. Fullerton, J. Hallett, R. L. Jack, and C. P. Royall, Soft Matter
Effects of vertical confinement on gelation and sedimentation of colloidsm
arXiv:1610.01123.
[62] C. J. Fullerton and R. L. Jack, J. Chem. Phys.
Optimising self-assembly through time-dependent interactions,
arXiv:1609.05008.
[61] M. Burman, D. Carpenter, and R. L. Jack, J. Phys. A
Emergence of particle clusters in a one-dimensional model: connection to condensation processes,
arXiv:1608.04304.
[60] C. Law, D. J. Ashton, N. B. Wilding and R. L. Jack, J. Chem. Phys.
Coarse-grained depletion potentials for anisotropic colloids:
application to lock-and-key systems,
arXiv:1607.00960.
[59] R. L. Jack and L. Berthier, J. Chem. Phys.
The melting of stable glasses is governed by nucleation-and-growth dynamics,
arXiv:1603.05017.
... see also our followup note... [59a] R. L. Jack and L. Berthier, J. Chem. Phys.
Note: Physical mechanisms for the bulk melting of stable glasses
[58] D. Coslovich and R. L. Jack, J. Stat. Mech. (2016) 074012.
[DOI]
Structure of inactive states of a binary Lennard-Jones mixture,
arXiv:1602.07589.
[57] R. L. Jack and R. M. L. Evans, J. Stat. Mech. (2016) 093305.
[DOI]
Absence of dissipation in trajectory ensembles biased by currents,
arXiv:1602.03815.
[56] T. Nemoto, F. Bouchet, R. L. Jack and V. Lecomte, Phys. Rev. E
Population dynamics method with a multi-canonical feedback control,
arXiv:1601.06648.
[55] T. Speck and R. L. Jack, Phys. Rev. E
Ideal bulk pressure of active Brownian particles,
arXiv:1512.00830.
[54] P. K. Jana, C. Wang, R. L. Jack, L. Chi and A. Heuer, Phys. Rev. E
Anomalous approach to thermodynamic equilibrium: structure formation of molecules
after vapor deposition
[53] R. L. Jack and J. P. Garrahan, Phys. Rev. Lett.
Phase transition for quenched coupled replicas in a plaquette spin model of glasses,
arXiv:1508.06470.
[52] I. R. Thompson and R. L. Jack, Phys. Rev. E
Dynamical phase transitions in one-dimensional hard-particle systems,
arXiv:1506.01492.
[51] R. M. Turner, R. L. Jack and J. P. Garrahan, Phys. Rev. E
Overlap and activity glass transitions in plaquette spin models with hierarchical dynamics,
arXiv:1504.05076
[50] L. Berthier and R. L. Jack, Phys. Rev. Lett.
Evidence for a disordered critical point in a glass-forming liquid,
arXiv:1503.08576.
[49] D. J. Ashton, R. L. Jack, and N. B. Wilding, Phys. Rev. Lett.
Porous liquid phases for indented colloids with depletion interactions,
arXiv:1501.07472.
[48] R. L. Jack and P. Sollich, Eur. Phys. J.: Special Topics
Effective interactions and large deviations in stochastic processes,
arXiv:1501.01154.
(Special issue from CECAM workshop: Scale Bridging Techniques in Molecular Simulation, Berlin 2014.)
[47] D. J. Ashton, S. J. Ivell, R. P. A. Dullens, R. L. Jack, N. B. Wilding, D. G. A. L. Aarts, Soft Matter
Self-assembly and crystallisation of indented colloids at a planar wall,
arXiv:1412.1596.
[DOI]
[46] R. L. Jack, I. R. Thompson and P. Sollich, Phys. Rev. Lett.
Hyperuniformity and phase separation in biased ensembles of trajectories for diffusive systems,
arXiv:1409.3986.
[45] J. K. Weber, R. L. Jack, C. R. Schwantes and V. S. Pande, Biophys. J.
Dynamical Phase Transitions Reveal Amyloid-like States on Protein Folding Landscapes.
(Featured in new and notable section of Biophys J) [44] S. Whitelam and R. L. Jack, Ann. Rev. Phys. Chem
Statistical Mechanics of Dynamic Pathways to Self-assembly,
arXiv:1407.2505.
(Invited review article) [43] R. L. Jack, and J. Zimmer, J. Phys. A
Geometrical interpretation of fluctuating hydrodynamics in diffusive systems,
arXiv:1407.1679.
[42] R. L. Jack, A. J. Dunleavy and C. P. Royall, Phys. Rev. Lett.
Information-theoretic measurements of coupling between structure and dynamics in glass-formers,
arXiv:1402.6867.
[41] C. J. Fullerton and R. L. Jack, Phys. Rev. Lett.
Investigating amorphous order in stable glasses by random pinning,
arXiv:1312.0766.
[40] I. Williams, E. C. Oguz, R. L. Jack, P. Bartlett, H. Loewen and C. P. Royall, J. Chem. Phys.
The effect of boundary adaptivity on hexagonal ordering and bistability in circularly confined quasi hard discs,
arXiv:1311.4781.
[DOI]
[39] R. L. Jack and P. Sollich, J. Phys. A Large deviations of the dynamical activity in the East model:
analysing structure in biased trajectories,
arXiv:1308.6124.
[38] R. L. Jack, Phys. Rev E Counting metastable states in a kinetically constrained model using a patch repetition
analysis,
arXiv:1309.6247.
[37] R. L. Jack and C. J. Fullerton, Phys. Rev E Dynamical correlations in a glass-former with randomly pinned particles,
arXiv:1306.5640.
[36] D. J. Ashton, R. L. Jack, N. B. Wilding, Soft Matter
Self-assembly of colloidal polymers via depletion-mediated lock and
key binding,
arXiv:1304.3675.
[35] J. K. Weber, R. L. Jack and V. S. Pande, J. Am. Chem. Soc.
Emergence of glass-like behavior in Markov state models of
protein folding dynamics.
[34] C. J. Fullerton and R. L. Jack, J. Chem. Phys.
Dynamical phase transitions in supercooled liquids: interpreting measurements of dynamical activity,
arXiv:1302.6880.
[33] D. Klotsa and R. L. Jack, J. Chem. Phys. Controlling crystal self-assembly using a real-time feedback scheme,
arXiv:1210.2636.
[32] Y. S. Elmatad and R. L. Jack, J. Chem. Phys.
Space-time phase transitions in the East model with a softened kinetic constraint,
arXiv:1210.1614.
(Part of a JCP special topical issue.) [31] R. L. Jack and L. Berthier, Phys. Rev. E Random pinning in glassy spin models with plaquette interactions,
arXiv:1112.1536.
[30] J. Grant and R. L. Jack, Phys. Rev. E Quantifying reversibility in a phase-separating lattice gas: an analogy with self-assembly,
arXiv:1110.6068.
[29] R. L. Jack, L. O. Hedges, J. P. Garrahan and D. Chandler, Phys. Rev. Lett. Preparation and relaxation of very stable glassy states of a simulated liquid,
arXiv:1109.2715.
[28] J. Grant, R. L. Jack and S. Whitelam, J. Chem. Phys. Analyzing mechanisms and microscopic reversibility of self-assembly,
arXiv:1108.4542.
[27] M. F. Hagan, O. M. Elrad and R. L. Jack, J. Chem. Phys.
Mechanisms of kinetic trapping in self-assembly and phase transformation,
arXiv:1105.2830.
[26] D. Klotsa and R. L. Jack, Soft Matter
Predicting the self-assembly of a model colloidal crystal,
arXiv:1103.2037.
[25] L. Berthier, G. Biroli, J.-P. Bouchaud and R. L. Jack, arXiv:1009.4765. Overview of different characterisations of dynamic heterogeneity,
(Book chapter in Dynamical heterogeneities in glasses, colloids, and granular media
(Oxford Univ. Press))
[24] Y. S. Elmatad, R. L. Jack, J. P. Garrahan and D. Chandler, Proc. Natl. Acad. Sci. USA
Finite-temperature critical point of a glass transition,
arXiv:1003.3161.
[23] R. L. Jack and P. Sollich, Prog. Theor. Phys. Supp.
Large deviations and ensembles of trajectories in stochastic models,
arXiv:0911.0211.
(Proceedings of workshop, "Frontiers in non-equilibrium physics", Kyoto 2009.) [22] P. Sollich and R. L. Jack, Prog. Theor. Phys. Supp.
Duality symmetries in driven one-dimensional hopping models,
arXiv:0911.0208.
(Proceedings of workshop, "Frontiers in non-equilibrium physics", Kyoto 2009.) [21] R. L. Jack and J. P. Garrahan, Phys. Rev. E
Metastable states and space-time phase transitions in a spin-glass model,
arXiv:0910.1111.
[20] R. L. Jack and P. Sollich, J. Stat. Mech. (2009), P11011.
Duality symmetries and effective dynamics in disordered hopping models,
arXiv:0908.3492.
[19] K. van Duijvendijk, R. L. Jack and F. van Wijland, Phys. Rev. E
Second-order dynamic transition in a p=2 spin-glass model,
arXiv:0905.4878.
[18] L. O. Hedges, R. L. Jack, J. P. Garrahan and D. Chandler, Science Dynamic order-disorder in atomistic models of structural glass formers.
[PDF]
[17] J. P. Garrahan, R. L. Jack, V. Lecomte, E. Pitard, K. van Duijvendijk and F. van Wijland, J. Phys A First-order dynamical phase transition in models of glasses: an approach based on ensembles of histories,
arXiv:0810.5298.
[16] R. L. Jack, P. Sollich and P. Mayer, Phys. Rev. E
Subdiffusive motion in kinetically constrained models,
arXiv:0809.2897.
[15] R. L. Jack, D. Kelsey, J. P. Garrahan and D. Chandler, Phys. Rev. E Negative differential mobility of weakly driven particles in
models of glass formers,
arXiv:0803.2002.
[14] R. L. Jack and P. Sollich, J. Phys. A Duality between random trap and barrier models,
arXiv:0710.1665.
(David Sherrington Festschrift.) [13] L. Berthier and R. L. Jack, Phys Rev. E Structure and dynamics in glass-formers: predictability at large
lengthscales,
arXiv:0706.1044.
[12] R. L. Jack, M. F. Hagan and D. Chandler, Phys. Rev. E Fluctuation-dissipation ratios in the dynamics of self-assembly,
arXiv:0705.3660.
[11] J. P. Garrahan, R. L. Jack, V. Lecomte, E. Pitard, K. van Duijvendijk and F. van Wijland, Phys. Rev. Lett. Dynamic first-order phase transition in kinetically constrained
models of glasses,
cond-mat/0701757.
[10] R. L. Jack, L. Berthier and J. P. Garrahan, J. Stat. Mech. (2006) P12005. Fluctuation-dissipation relations in plaquette spin systems
with multi-stage relaxation,
cond-mat/0609257.
[9] D. Chandler, J. P. Garrahan, R. L. Jack, L. Maibaum and A. C. Pan, Phys. Rev. E Lengthscale dependence of dynamic four-point susceptibilities
in glass formers,
cond-mat/0605084.
[8] R. L. Jack, J. P. Garrahan and D. Chandler, J. Chem. Phys.
Space-time thermodynamics and subsystem observables in a kinetically constrained model of glassy systems,
cond-mat/0604068.
[7] R. L. Jack, P. Mayer and P. Sollich,
J. Stat. Mech. (2006), P03006. Mappings between reaction-diffusion and kinetically constrained systems:
cond-mat/0601529.
A+A <-> A and the FA model have upper critical dimension dc = 2, [6] R. L. Jack and J. P. Garrahan,
J. Chem. Phys. Caging and mosaic lengthscales in
plaquette spin models of glasses,
cond-mat/0507370.
[5] R. L. Jack, L. Berthier and J. P. Garrahan,
Phys. Rev. E Static and dynamic lengthscales in a simple glassy plaquette
model ,
cond-mat/0502120.
[4] R. L. Jack, J. P. Garrahan and D. Sherrington,
Phys. Rev. E Glassy behaviour in an exactly solved spin system with a
ferromagnetic transition ,
cond-mat/0410028.
[3] R. L. Jack, D. K. K. Lee and N. R. Cooper,
Phys. Rev. B
Quantum and Classical Dissipative Effects on Tunnelling in Quantum Hall
Bilayers
cond-mat/0409547.
[2] R. L. Jack, D. K. K. Lee and N. R. Cooper,
Phys. Rev. Lett.Dissipation and Tunnelling in Quantum Hall Bilayers,
cond-mat/0403392.
[1] R. L. Jack and D. K. K. Lee, Phys. Rev. B Bosons in fluctuating gauge fields: Bose metal and phase
separation
cond-mat/0203274.
[0] R. L. Jack, Ph.D. thesis, University of London. (pdf) Back to Robert Jack's homepage
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