TY - JOUR

T1 - Supersymmetric quantum mechanics of magnetic monopoles

T2 - A case study

AU - de Vries, Erik Jan

AU - Schroers, Bernd J.

PY - 2009/7/11

Y1 - 2009/7/11

N2 - We study, in detail, the supersymmetric quantum mechanics of charge-(1, 1) monopoles in N = 2 supersymmetric Yang-Mills-Higgs theory with gauge group SU (3) spontaneously broken to U (1) × U (1). We use the moduli space approximation of the quantised dynamics, which can be expressed in two equivalent formalisms: either one describes quantum states by Dirac spinors on the moduli space, in which case the Hamiltonian is the square of the Dirac operator, or one works with anti-holomorphic forms on the moduli space, in which case the Hamiltonian is the Laplacian acting on forms. We review the derivation of both formalisms, explicitly exhibit their equivalence and derive general expressions for the supercharges as differential operators in both formalisms. We propose a general expression for the total angular momentum operator as a differential operator, and check its commutation relations with the supercharges. Using the known metric structure of the moduli space of charge-(1, 1) monopoles we show that there are no quantum bound states of such monopoles in the moduli space approximation. We exhibit scattering states and compute corresponding differential cross sections. © 2009 Elsevier B.V. All rights reserved.

AB - We study, in detail, the supersymmetric quantum mechanics of charge-(1, 1) monopoles in N = 2 supersymmetric Yang-Mills-Higgs theory with gauge group SU (3) spontaneously broken to U (1) × U (1). We use the moduli space approximation of the quantised dynamics, which can be expressed in two equivalent formalisms: either one describes quantum states by Dirac spinors on the moduli space, in which case the Hamiltonian is the square of the Dirac operator, or one works with anti-holomorphic forms on the moduli space, in which case the Hamiltonian is the Laplacian acting on forms. We review the derivation of both formalisms, explicitly exhibit their equivalence and derive general expressions for the supercharges as differential operators in both formalisms. We propose a general expression for the total angular momentum operator as a differential operator, and check its commutation relations with the supercharges. Using the known metric structure of the moduli space of charge-(1, 1) monopoles we show that there are no quantum bound states of such monopoles in the moduli space approximation. We exhibit scattering states and compute corresponding differential cross sections. © 2009 Elsevier B.V. All rights reserved.

UR - http://www.scopus.com/inward/record.url?scp=64049087180&partnerID=8YFLogxK

U2 - 10.1016/j.nuclphysb.2009.01.003

DO - 10.1016/j.nuclphysb.2009.01.003

M3 - Article

SN - 0550-3213

VL - 815

SP - 368

EP - 403

JO - Nuclear Physics B

JF - Nuclear Physics B

IS - 3

ER -