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Johan Bijnens

Researcher at Lund University

Publications -  349
Citations -  12148

Johan Bijnens is an academic researcher from Lund University. The author has contributed to research in topics: Chiral perturbation theory & Quantum chromodynamics. The author has an hindex of 54, co-authored 341 publications receiving 10497 citations. Previous affiliations of Johan Bijnens include California Institute of Technology & CERN.

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On the tensor formulation of effective vector lagrangians and duality transformations

TL;DR: In this paper, the equivalence between effective Lagrangians for massive vector mesons using a vector field and an antisymmetric tensor field was proved using duality transformations.
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Vector Formfactors in Hard Pion Chiral Perturbation Theory

TL;DR: In this paper, the authors used three-flavour hard pion Chiral Perturbation Theory (HPChPT) in both the heavy meson and a relativistic formulation to calculate the chiral logarithms m(2) log (m(2)/mu(2)) contributing to the formfactors of the B-(s) -> pi, K, eta and D-(s, K) transitions at momentum transfer q( 2) away from the endpoint q(max)(2) = (m (B) - m(M
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Hard pion chiral perturbation theory for B -> pi and D -> pi formfactors

TL;DR: In this article, the authors used one-loop Heavy Meson Chiral Perturbation Theory (HMChPT) as well as a relativistic formulation to calculate the chiral logarithm m(pi) log (m(pi)(2)/mu(2)) contributing to the formfactors of the semileptonic B -> pi decays at momentum transfer q(2) away from q(max)(2) = m(B) -m(π))(2).
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Pion light-by-light contributions to the muon g − 2

TL;DR: In this paper, the pion loop light-by-light contribution to the muon anomalous magnetic moment was studied in the framework of some models studied earlier, such as pure pion loops, full VMD and hidden local symmetry for inclusion of vector mesons.
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Fermion masses from symmetry

TL;DR: In this article, the authors present a model with continuous or discrete abelian generation group G, which predicts all orders of magnitude for fermion masses ad mixings correctly as a function of only one small parameter φSM ≈ 110.