Abstract:The ladder Bethe-Salpeter Equation of a bound (1/2) + system, composed by a fermion and a scalar boson, is solved in Minkowski space, for the first time. The formal tools are the same already successfully adopted for two-scalar and two-fermion systems, namely the Nakanishi integral representation of the Bethe-Salpeter amplitude and the light-front projection of the fulfilled equation. Numerical results are presented and discussed for two interaction kernels: i) a massive scalar exchange and ii) a massive vecto… Show more
“…Those steps have been explored for the BSEs in Refs. [64][65][66][67][68][69][70][71][72][73][74][75][76][77][78]. For the fermion self-energy, it is necessary to introduce two NWFs, since one has to deal with two scalar functions.…”
Section: The Renormalized Propagator Of a Fermionmentioning
confidence: 99%
“…[44,[58][59][60][61][62][63]) and BSE (see, e.g., Refs. [64][65][66][67][68][69][70][71][72][73][74][75][76][77][78], where systems with and without spin degrees of freedom are investigated).…”
Section: Introductionmentioning
confidence: 99%
“…y − A 7 (s, s , ω, v, ξ, w) , (D.128)with Δ , C(i) AV , C(i) AS and C γ from Eqs (69),(70),(71),(73),(74). and(78), and the following equations that relate the NWFs to the KL weights (see Eq.…”
The approach based on the Nakanishi integral representation of n-leg transition amplitudes is extended to the treatment of the self-energies of a fermion and an (IR-regulated) vector boson, in order to pave the way for constructing a comprehensive application of the technique to both gap- and Bethe-Salpeter equations, in Minkowski space. The achieved result, namely a 6-channel coupled system of integral equations, eventually allows one to determine the three Källén–Lehman weights for fully dressing the propagators of fermion and photon. A first consistency check is also provided. The presented formal elaboration points to embed the characteristics of the non-perturbative regime at a more fundamental level. It yields a viable tool in Minkowski space for the phenomenological investigation of strongly interacting theories, within a QFT framework where the dynamical ingredients are made transparent and under control.
“…Those steps have been explored for the BSEs in Refs. [64][65][66][67][68][69][70][71][72][73][74][75][76][77][78]. For the fermion self-energy, it is necessary to introduce two NWFs, since one has to deal with two scalar functions.…”
Section: The Renormalized Propagator Of a Fermionmentioning
confidence: 99%
“…[44,[58][59][60][61][62][63]) and BSE (see, e.g., Refs. [64][65][66][67][68][69][70][71][72][73][74][75][76][77][78], where systems with and without spin degrees of freedom are investigated).…”
Section: Introductionmentioning
confidence: 99%
“…y − A 7 (s, s , ω, v, ξ, w) , (D.128)with Δ , C(i) AV , C(i) AS and C γ from Eqs (69),(70),(71),(73),(74). and(78), and the following equations that relate the NWFs to the KL weights (see Eq.…”
The approach based on the Nakanishi integral representation of n-leg transition amplitudes is extended to the treatment of the self-energies of a fermion and an (IR-regulated) vector boson, in order to pave the way for constructing a comprehensive application of the technique to both gap- and Bethe-Salpeter equations, in Minkowski space. The achieved result, namely a 6-channel coupled system of integral equations, eventually allows one to determine the three Källén–Lehman weights for fully dressing the propagators of fermion and photon. A first consistency check is also provided. The presented formal elaboration points to embed the characteristics of the non-perturbative regime at a more fundamental level. It yields a viable tool in Minkowski space for the phenomenological investigation of strongly interacting theories, within a QFT framework where the dynamical ingredients are made transparent and under control.
“…Together with the practicity of our approach and the reduced error estimate, we believe that the algorithm discussed herein is also suitable to study other Green functions. Moreover, the SPM has been proven useful in connecting Euclidean and Minkowskian quantities [48][49][50], a key goal in modern hadron physics [51,52].…”
We propose a practical procedure to extrapolate the space-like quark propagator onto the complex plane, which follows the Schlessinger Point Method and the spectral representation of the propagator. As a feasible example, we employ quark propagators for different flavors, obtained from the solutions of the corresponding Dyson-Schwinger equation. Thus, the analytical structure of the quark propagator is studied, capitalizing on the current-quark mass dependence of the observed features.
“…The above properties of NIR were exploited to provide solutions of many particular quantum field toy model problems [9]. Especially, the NIR was used in two body bound state calculation in various models [10], [11], [12], [13], [14], [16], [17]. Encouraging results for the electromagnetic form factors were obtained [18] within the formalism as well.…”
Using a nonperturbative framework of Dyson-Schwinger equations a class of Nakanishi's like integral representations for the transverse part of the quark-photon vertex is derived. For this but also for its own purpose the two and single variable integral representations for untruncated quarkantiquark-photon vertex is proposed as well. To exhibit the adequacy of proposed representation, the Dyson-Schwinger equation for the vertex is transformed into the equivalent set of coupled integrodifferential equations for Nakanishi weight functions-functions that appear linearly in the numerator of given integral representation. Their knowledge then provide self-consistent nonperturbative solution for the vertex in the entire Minkowski space.
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