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in the SeibergWitten Low Energy Limit
, 2001
"... We analyse open and mixed sector treelevel amplitudes consisting of two p − p ′ openstring and one or two p ′ − p ′ openstring vertex operators in the purely openstring sector, and two p − p ′ or p ′ − p ′ openstring and one closed string vertex operators, for N = 2 strings with a constant ma ..."
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with momentum (ζ = ik). However, on taking the SeibergWitten (SW) low energy limit[2], there are considerable differences in the results one obtains and the interpretations of the results: the 4point function is local indicating the possible topological nature of the theory. The 3point function vanishes (on
LowEnergy Limit of Yang–Mills
, 2006
"... If the fundamental quarks of QCD are replaced by massless adjoint quarks the pattern of the chiral symmetry breaking drastically changes compared to the standard one. It becomes SU(Nf) →SO(Nf). While for Nf = 2 the chiral Lagrangian describing the “pion ” dynamics is wellknown, this is not the case ..."
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If the fundamental quarks of QCD are replaced by massless adjoint quarks the pattern of the chiral symmetry breaking drastically changes compared to the standard one. It becomes SU(Nf) →SO(Nf). While for Nf = 2 the chiral Lagrangian describing the “pion ” dynamics is wellknown, this is not the case at Nf> 2. We outline a general strategy for deriving chiral Lagrangians for the coset spaces Mk = SU(k)/SO(k), and study in detail the case of Nf = k = 3. We obtain two and fourderivatives terms in the chiral Lagrangian on the coset space M3 = SU(3)/SO(3), as well as the Wess–Zumino– Novikov–Witten term, in terms of an explicit parameterization of the quotient manifold. Then we discuss stable topological solitons supported by this Lagrangian. Aspects of relevant topological considerations scattered in the literature are reviewed. The same analysis applies to SO(N) gauge theories with Nf Weyl flavors in the vector representation. 1
UMSNHPhys/0213 On the lowenergy limit of the
, 2003
"... We derive an explicit formula for the low energy limits of the oneloop onshell massive N photon amplitudes, for arbitrary N and all helicity assignments, in scalar and spinor QED. The twoloop corrections to the same amplitudes are obtained for up to the ten point case. All photon amplitudes with ..."
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We derive an explicit formula for the low energy limits of the oneloop onshell massive N photon amplitudes, for arbitrary N and all helicity assignments, in scalar and spinor QED. The twoloop corrections to the same amplitudes are obtained for up to the ten point case. All photon amplitudes
The Low Energy Limit of the Chern–Simons Theory Coupled to
, 1997
"... We study the nonrelativistic limit of the theory of a quantum Chern–Simons field minimally coupled to Dirac fermions. To get the nonrelativistic effective Lagrangian one has to incorporate vacuum polarization and anomalous magnetic moment effects. Besides that, an unsuspected quartic fermionic inter ..."
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We study the nonrelativistic limit of the theory of a quantum Chern–Simons field minimally coupled to Dirac fermions. To get the nonrelativistic effective Lagrangian one has to incorporate vacuum polarization and anomalous magnetic moment effects. Besides that, an unsuspected quartic fermionic
The Low Energy Limit of the Noncommutative WessZumino Model
, 2001
"... The noncommutative WessZumino model is used as a prototype for studying the low energy behavior of a renormalizable noncommutative field theory. We start by deriving the potentials mediating the fermionfermion and bosonboson interactions in the nonrelativistic regime. The quantum counterparts of t ..."
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The noncommutative WessZumino model is used as a prototype for studying the low energy behavior of a renormalizable noncommutative field theory. We start by deriving the potentials mediating the fermionfermion and bosonboson interactions in the nonrelativistic regime. The quantum counterparts
The Low Energy Limit of the Noncommutative WessZumino Model
, 2001
"... It has recently been shown that the noncommutative WessZumino model is renormalizable to all orders of perturbation theory and that the infrared singularities arising form the IR/UV mixing are all integrable. In this work we investigate the low energy behavior of this model by deriving the effectiv ..."
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It has recently been shown that the noncommutative WessZumino model is renormalizable to all orders of perturbation theory and that the infrared singularities arising form the IR/UV mixing are all integrable. In this work we investigate the low energy behavior of this model by deriving
ON THE LOWENERGY LIMIT OF STRING AND MTHEORY ∗
, 2000
"... We discuss the possible applications of string theory for the construction of generalizations of the SU(3) × SU(2) × U(1) standard model of strong and electroweak interactions. This includes an investigation of effective d = 4 dimensional supergravity theories that could be derived from higher dim ..."
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We discuss the possible applications of string theory for the construction of generalizations of the SU(3) × SU(2) × U(1) standard model of strong and electroweak interactions. This includes an investigation of effective d = 4 dimensional supergravity theories that could be derived from higher dimensional string theories (d = 10) and Mtheory (d = 11). It is shown how the question of unification of gauge and gravitational coupling constants could find a solution within this framework. The mechanism of hidden sector supersymmetry breakdown and its consequences for the pattern for soft supersymmetry breaking terms are discussed in detail. 1
Results 1  10
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4,281,970