In this paper, the authors consider in a semiclassical regime a nonlinear Schrödinger equation in R3 with both an electric and a magnetic field. More precisely, the nonlinear Schrödinger equation under study is of the form (−iℏ∇−A)2u+Vu=f(|u|2)u, where A is a vector potential for the magnetic field, V is a strictly positive electric potential, f:[0,∞)→R is an increasing differentiable function and u:R3→R. The main result of this work states that if A, V and f satisfy some conditions, which are too technical to be stated here, then there exists ℏ0>0 such that for each ℏ with 0<ℏ<ℏ0 there exists a solution u of the above NLS equation that satisfies ∫R3∣∣[(−iℏ∇−A)u](x)∣∣2dx+∫R3V(x)∣∣u(x)∣∣2dx<∞. This statement greatly extends some of the results already contained in previous work of the same authors [J. Math. Anal. Appl. 275 (2002), no. 1, 108--130; MR1941775 (2003k:81062)]. In particular, the boundedness assumption on the electric field and on the vector potential is removed. As pointed out in this paper, the physically meaningful case of a constant magnetic field is now included in the present framework.
Cingolani, S., Secchi, S. (2005). Semiclassical states for NLS equations with magnetic potentials having polynomial growths. JOURNAL OF MATHEMATICAL PHYSICS, 46(5), 053503.1-053503.19 [10.1063/1.1874333].
Semiclassical states for NLS equations with magnetic potentials having polynomial growths
SECCHI, SIMONE
2005
Abstract
In this paper, the authors consider in a semiclassical regime a nonlinear Schrödinger equation in R3 with both an electric and a magnetic field. More precisely, the nonlinear Schrödinger equation under study is of the form (−iℏ∇−A)2u+Vu=f(|u|2)u, where A is a vector potential for the magnetic field, V is a strictly positive electric potential, f:[0,∞)→R is an increasing differentiable function and u:R3→R. The main result of this work states that if A, V and f satisfy some conditions, which are too technical to be stated here, then there exists ℏ0>0 such that for each ℏ with 0<ℏ<ℏ0 there exists a solution u of the above NLS equation that satisfies ∫R3∣∣[(−iℏ∇−A)u](x)∣∣2dx+∫R3V(x)∣∣u(x)∣∣2dx<∞. This statement greatly extends some of the results already contained in previous work of the same authors [J. Math. Anal. Appl. 275 (2002), no. 1, 108--130; MR1941775 (2003k:81062)]. In particular, the boundedness assumption on the electric field and on the vector potential is removed. As pointed out in this paper, the physically meaningful case of a constant magnetic field is now included in the present framework.I documenti in IRIS sono protetti da copyright e tutti i diritti sono riservati, salvo diversa indicazione.