We add a random bulk term, modelling the interaction with the impurities of the medium, to a standard functional in the gradient theory of phase transitions consisting of a gradient term with a double well potential. We show that in d � 2 there exists, for almost all the realizations of the random bulk term, a unique random macroscopic minimizer. This result is in sharp contrast to the case when the random bulk term is absent. In the latter case there are two minimizers which are (in law) invariant under translations in space
Energy functionals describing phase transitions in crystalline solids are often non-quasiconvex and ...
Energy functionals describing phase transitions in crystalline solids are often non-quasiconvex and ...
We consider the Gamma-limit of a family of functionals which model the interaction of a material tha...
We add a random bulk term, modelling the interaction with the impurities of the medium, to a standa...
We add a random bulk term, modelling the interaction with the impurities of the medium, to a standa...
We add a random bulk term, modelling the interaction with the impurities of the medium, to a standa...
Abstract. We add a random bulk term, modelling the interaction with the impurities of the medium, to...
Abstract. We add a random bulk term, modelling the interaction with the impurities of the medium, to...
We add a random bulk term, modeling the interaction with the impurities of the medium,to a standa...
We add a random bulk term, modeling the interaction with the impurities of the medium,to a standa...
We add a random bulk term, modeling the interaction with the impurities of the medium, to a standard...
We add a random bulk term, modeling the interaction with the impurities of the medium, to a standard...
We add a random bulk term, modeling the interaction with the impurities of the medium, to a standard...
We add a random bulk term, modeling the interaction with the impurities of the medium, to a standard...
We add a random bulk term, modeling the interaction with the impurities of the medium, to a standard...
Energy functionals describing phase transitions in crystalline solids are often non-quasiconvex and ...
Energy functionals describing phase transitions in crystalline solids are often non-quasiconvex and ...
We consider the Gamma-limit of a family of functionals which model the interaction of a material tha...
We add a random bulk term, modelling the interaction with the impurities of the medium, to a standa...
We add a random bulk term, modelling the interaction with the impurities of the medium, to a standa...
We add a random bulk term, modelling the interaction with the impurities of the medium, to a standa...
Abstract. We add a random bulk term, modelling the interaction with the impurities of the medium, to...
Abstract. We add a random bulk term, modelling the interaction with the impurities of the medium, to...
We add a random bulk term, modeling the interaction with the impurities of the medium,to a standa...
We add a random bulk term, modeling the interaction with the impurities of the medium,to a standa...
We add a random bulk term, modeling the interaction with the impurities of the medium, to a standard...
We add a random bulk term, modeling the interaction with the impurities of the medium, to a standard...
We add a random bulk term, modeling the interaction with the impurities of the medium, to a standard...
We add a random bulk term, modeling the interaction with the impurities of the medium, to a standard...
We add a random bulk term, modeling the interaction with the impurities of the medium, to a standard...
Energy functionals describing phase transitions in crystalline solids are often non-quasiconvex and ...
Energy functionals describing phase transitions in crystalline solids are often non-quasiconvex and ...
We consider the Gamma-limit of a family of functionals which model the interaction of a material tha...