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See detailAbelian symmetries in multi-Higgs-doublet models
Ivanov, Igor ULg; Keus, Venus ULg; Vdovin, Evgeny

in Journal of Mathematical Physics (2012)

N-Higgs-doublet models (NHDM) are a popular framework to construct electroweak symmetry breaking mechanisms beyond the Standard model. Usually, one builds an NHDM scalar sector which is invariant under a ... [more ▼]

N-Higgs-doublet models (NHDM) are a popular framework to construct electroweak symmetry breaking mechanisms beyond the Standard model. Usually, one builds an NHDM scalar sector which is invariant under a certain symmetry group. Although several such groups have been used, no general analysis of symmetries possible in the NHDM scalar sector exists. Here, we describe a strategy that identifies all abelian groups which are realizable as symmetry groups of the NHDM Higgs potential. We consider both the groups of Higgs-family transformations only and the groups which also contain generalized CP transformations. We illustrate this strategy with the examples of 3HDM and 4HDM and prove several statements for arbitrary N. [less ▲]

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See detailMaximal subalgebras of vector fields for equivariant quantizations
Boniver, Fabien; Mathonet, Pierre ULg

in Journal of Mathematical Physics (2001), 42(2), 582-589

The elaboration of new quantization methods has recently developed the interest in the study of subalgebras of the Lie algebra of polynomial vector fields over a Euclidean space. In this framework, these ... [more ▼]

The elaboration of new quantization methods has recently developed the interest in the study of subalgebras of the Lie algebra of polynomial vector fields over a Euclidean space. In this framework, these subalgebras define maximal equivariance conditions that one can impose on a linear bijection between observables that are polynomial in the momenta and differential operators. Here, we determine which finite dimensional graded Lie subalgebras are maximal. In order to characterize these, we make use of results of Guillemin, Singer, and Sternberg and Kobayashi and Nagano. [less ▲]

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See detailSUPERSPACE FORMULATION OF N=2 PSEUDOMECHANICS AND SUPERPOTENTIALS
Bouquiaux, Laurence ULg; Dauby, Pierre ULg; HUSSIN, V.

in Journal of Mathematical Physics (1987), 28(2), 477-484

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See detailUpper bounds for the many-channel Marchenko transformation operator and its derivatives
Rochus, Pierre ULg

in Journal of Mathematical Physics (1979), 20

We specify the class of perturbative complex matrix potentials for which the corresponding many-channel Marchenko type transformation operators are bounded and integrable. Our reference matrix potential ... [more ▼]

We specify the class of perturbative complex matrix potentials for which the corresponding many-channel Marchenko type transformation operators are bounded and integrable. Our reference matrix potential contains Coulomb interactions, different threshold energies, and centrifugal potentials with different angular momenta. Estimates for the transformation operator and its derivatives are obtained; they enable us to improve our recent results and are necessary for the establishment of a unique solution to the ''generalized Marchenko fundamental equation.'' From the existence of an integrable transformation operator, the analyticity of the Jost solution as a function of k1 is deduced in the upper-half of the physical k1 plane. [less ▲]

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See detailUpper bounds for the many-channel Marchenko transformation operator and its derivatives
Rochus, Pierre ULg

in Journal of Mathematical Physics (1979), 20(5), 781--792

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See detailThe translation kernel in the n-dimensional scattering problem
Coz, Marcel; Rochus, Pierre ULg

in Journal of Mathematical Physics (1977), 18

Radial wavefunctions are defined for the n-dimensional scattering problem (n>~1) with spherical symmetry by conditions of regularity at the origin or by conditions of behavior at infinity. The existence ... [more ▼]

Radial wavefunctions are defined for the n-dimensional scattering problem (n>~1) with spherical symmetry by conditions of regularity at the origin or by conditions of behavior at infinity. The existence of translation kernels can therefore be discussed in both instances. The problem of representing regular solutions appears to be essentially different from that of representing irregular solutions. The essential difference originates from the type of domain used in the representation: It is bounded in the first case and unbounded in the second. If one can still compare the ranges of validity of the two types of representation when one is dealing with a scalar situation, upon proceeding to a matrix situation, a comparison is no longer possible. [less ▲]

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See detailTranslation kernels for velocity dependent interactions
Coz, M.; Rochus, Pierre ULg

in Journal of Mathematical Physics (1977), 18(11), 2232--2240

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See detailThe translation kernel in the $n$-dimensional scattering problem
Coz, Marcel; Rochus, Pierre ULg

in Journal of Mathematical Physics (1977), 18(11), 2223--2231

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See detailPartial differential matrix equations for the inverse problem of scattering theory
Coz, M.; Rochus, Pierre ULg

in Journal of Mathematical Physics (1976), 17

Sufficient conditions for the existence of a continuous translation operator are found in the case of a system of differential equations in which the matrix potential has the singularity of the ... [more ▼]

Sufficient conditions for the existence of a continuous translation operator are found in the case of a system of differential equations in which the matrix potential has the singularity of the centripetal term. The sufficient conditions are found in terms of moments of the nuclear potential. The method used employs the Riemann Green's function. Threshold energies introduce a threshold energy dependence into the translation kernel and lead to a requirement of an exponential decrease for terms of the matrix potential. [less ▲]

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