TY - Generic
T1 - Critical opalescence across the doping-driven Mott transition in optical lattices of ultracold atoms
JF - Physical Review B
Y1 - 2019
ER -
TY - Generic
T1 - Critical opalescence across the doping-driven Mott transition in optical lattices of ultracold atoms
JF - Phys. Rev. B
Y1 - 2019
A1 - Walsh, C.
A1 - Sémon, P.
A1 - Sordi, G.
A1 - A.-M. S. Tremblay
ER -
TY - Generic
T1 - Local Entanglement Entropy and Mutual Information across the Mott Transition in the Two-Dimensional Hubbard Model
JF - Physical Review Letters
Y1 - 2019
ER -
TY - Generic
T1 - Local Entanglement Entropy and Mutual Information across the Mott Transition in the Two-Dimensional Hubbard Model
JF - Phys. Rev. Lett.
Y1 - 2019
A1 - Walsh, C.
A1 - Sémon, P.
A1 - Poulin, D.
A1 - Sordi, G.
A1 - A.-M. S. Tremblay
ER -
TY - Generic
T1 - Specific heat maximum as a signature of Mott physics in the two-dimensional Hubbard model
JF - Phys. Rev. B
Y1 - 2019
A1 - Sordi, G.
A1 - Walsh, C.
A1 - Sémon, P.
A1 - A.-M. S. Tremblay
ER -
TY - Generic
T1 - Specific heat maximum as a signature of Mott physics in the two-dimensional Hubbard model
JF - Physical Review B
Y1 - 2019
ER -
TY - Generic
T1 - Thermodynamic and information-theoretic description of the Mott transition in the two-dimensional Hubbard model
JF - Physical Review B
Y1 - 2019
ER -
TY - Generic
T1 - Thermodynamic and information-theoretic description of the Mott transition in the two-dimensional Hubbard model
JF - Phys. Rev. B
Y1 - 2019
A1 - Walsh, C.
A1 - Sémon, P.
A1 - Poulin, D.
A1 - Sordi, G.
A1 - A.-M. S. Tremblay
ER -
TY - Generic
T1 - Effects of interaction strength, doping, and frustration on the antiferromagnetic phase of the two-dimensional Hubbard model
JF - Phys. Rev. B
Y1 - 2017
A1 - Fratino, L.
A1 - Charlebois, M.
A1 - Sémon, P.
A1 - Sordi, G.
A1 - A.-M. S. Tremblay
ER -
TY - Generic
T1 - Signatures of the Mott transition in the antiferromagnetic state of the two-dimensional Hubbard model
JF - Phys. Rev. B
Y1 - 2017
A1 - Fratino, L.
A1 - Sémon, P.
A1 - Charlebois, M.
A1 - Sordi, G.
A1 - A.-M. S. Tremblay
ER -
TY - Generic
T1 - Antagonistic effects of nearest-neighbor repulsion on the superconducting pairing dynamics in the doped Mott insulator regime
JF - Phys. Rev. B
Y1 - 2016
A1 - Reymbaut, A.
A1 - Charlebois, M.
A1 - Asiani, M. Fellous
A1 - Fratino, L.
A1 - Sémon, P.
A1 - Sordi, G.
A1 - A.-M. S. Tremblay
ER -
TY - Generic
T1 - Pseudogap and superconductivity in two-dimensional doped charge-transfer insulators
JF - Phys. Rev. B
Y1 - 2016
A1 - Fratino, L.
A1 - Sémon, P.
A1 - Sordi, G.
A1 - A.-M. S. Tremblay
ER -
TY - Generic
T1 - Ergodicity of the hybridization-expansion Monte Carlo algorithm for broken-symmetry states
JF - Phys. Rev. B
Y1 - 2014
A1 - Sémon, P.
A1 - Sordi, G.
A1 - A.-M. S. Tremblay
ER -
TY - Generic
T1 - c-axis resistivity, pseudogap, superconductivity, and Widom line in doped Mott insulators
JF - Phys. Rev. B
Y1 - 2013
A1 - Sordi, G.
A1 - Sémon, P.
A1 - Haule, K.
A1 - A.-M. S. Tremblay
ER -
TY - Generic
T1 - Pseudogap temperature as a Widom line in doped Mott insulators
JF - Scientific Reports
Y1 - 2012
A1 - Sordi, G.
A1 - Sémon, P.
A1 - Haule, K.
A1 - A.-M. S. Tremblay
ER -
TY - Generic
T1 - Strong Coupling Superconductivity, Pseudogap, and Mott Transition
JF - Phys. Rev. Lett.
Y1 - 2012
A1 - Sordi, G.
A1 - Sémon, P.
A1 - Haule, K.
A1 - A.-M. S. Tremblay
ER -
TY - Generic
T1 - Mott physics and first-order transition between two metals in the normal-state phase diagram of the two-dimensional Hubbard model
JF - Phys. Rev. B
Y1 - 2011
A1 - Sordi, G.
A1 - Haule, K.
A1 - A.-M. S. Tremblay
ER -
TY - Generic
T1 - Finite Doping Signatures of the Mott Transition in the Two-Dimensional Hubbard Model
JF - Physical Review Letters
Y1 - 2010
A1 - Sordi, G.
A1 - Haule, K.
A1 - A.-M. S. Tremblay
AB - Experiments on layered materials call for a study of the influence of short-range spin correlations on the Mott transition. To this end, we solve the cellular dynamical mean-field equations for the Hubbard model on a plaquette with continuous-time quantum Monte Carlo calculations. The normal-state phase diagram as a function of temperature T, interaction strength U, and filling n reveals that upon increasing n towards the insulator, there is a surface of first-order transition between two metals at nonzero doping. For T above the critical end line there is a maximum in scattering rate.

ER -