Abstract:We obtain in analytical form the dressed propagator of the massive Rarita-Schwinger field taking into account all spin components and discuss shortly its properties.
“…The obtained dressed propagator (20) solves an algebraic part of the problem, the following step is renormalization. Note that the investigation of the dressed propagator is an alternative for more conventional methods based on equations of motion (see, i.e.…”
Section: Discussionmentioning
confidence: 99%
“…The appearance of p 2 factor is typical for fermions -see below and this apparent branch point p 2 is canceled in total expression for the dressed Rarita-Schwinger propagator (20). Thus we obtained the simple analytical expression (20) for the interacting Rarita-Schwinger field propagator which accounts all spin components.…”
Section: Dressed Propagator Of the Rarita-schwinger Fieldmentioning
We obtain in analytical form the dressed propagator of the massive RaritaSchwinger field taking into account all spin components. We found that the nearest analogy for dressing the Rarita-Schwinger field in spin-1/2 sector is dressing the two Dirac fermions of opposite parity with presence of mutual transitions. The calculation of the self-energy contributions confirms that besides the leading spin-3/2 component the Rarita-Schwinger field contains also two spin-1/2 components of different parity.
“…The obtained dressed propagator (20) solves an algebraic part of the problem, the following step is renormalization. Note that the investigation of the dressed propagator is an alternative for more conventional methods based on equations of motion (see, i.e.…”
Section: Discussionmentioning
confidence: 99%
“…The appearance of p 2 factor is typical for fermions -see below and this apparent branch point p 2 is canceled in total expression for the dressed Rarita-Schwinger propagator (20). Thus we obtained the simple analytical expression (20) for the interacting Rarita-Schwinger field propagator which accounts all spin components.…”
Section: Dressed Propagator Of the Rarita-schwinger Fieldmentioning
We obtain in analytical form the dressed propagator of the massive RaritaSchwinger field taking into account all spin components. We found that the nearest analogy for dressing the Rarita-Schwinger field in spin-1/2 sector is dressing the two Dirac fermions of opposite parity with presence of mutual transitions. The calculation of the self-energy contributions confirms that besides the leading spin-3/2 component the Rarita-Schwinger field contains also two spin-1/2 components of different parity.
“…The Rarita-Schwinger propagator in vacuum was recently discussed in Ref. [12], where some elements of the basis used in the present approach were introduced (of course, without the terms relevant for the nuclear medium). For the in-medium calculation of the isobar self energy we also use the interaction lagrangian (14), but with the off-shell parameter a put to zero.…”
Section: B Relativistic Propagator Of the Isobarmentioning
A formalism for representing the fully relativistic propagator of the Rarita-Schwinger field in the nuclear medium is developed. Using a convenient basis for expanding the propagator it is shown that it can be represented by 40 energy and momentum dependent quantities which can be decomposed into an 2×2 and an 6×6 matrix. In this way calculations reduce to matrix multiplication. Using the presented formalism the full relativistically covariant contribution of the pion-nucleon loop to the isobar self energy and propagator in isospin-symmetric spin-saturated nuclear medium is computed. Utilizing this propagator the photoabsorption cross-section on in-medium nucleons in the isobar region is calculated and the result compared with experimental data.
“…They simplify essentially all calculations and clarify their physical meaning. Recall that these projection operators were successfully used in calculations of the ∆-isobar propagator both in vacuum [13,14] and media [17].…”
We derive accurately the fermion resonance propagator by means of Dyson summation of the self-energy contribution. It turns out that the relativistic fermion resonance differs essentially from its boson analog.
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