SearcharxivSearch

arXiv subjects

Swapan Das

Publications and source records attributed to Swapan Das.

At least 19 recordsLinked to original sources

On the reconstruction of the Rotation Curve for Milky Way and its spacetime implications: a Machine Learning approach

We propose a machine learning-assisted analytical reconstruction of the Milky Way rotation curve and discuss its implications in a relativistic spacetime context. The rotation curve is reconstructed using 73 observational data points over the range 0.1-95.56 kpc, and we compare the performances of Ridge regression, LASSO regression, and feed-forward neural networks using a physically motivated functional basis. Ridge regression yields the most stable prediction with R2 = 0.9824 +/- 0.0064 and RMSE = 3.75 km/s, while retaining analytical interpretability. We embed the reconstructed velocity profile into a static, spherically symmetric spacetime, enabling the determination of the redshift function and the mass function through Einstein's equations. We verify that all energy conditions are satisfied, the sound speed remains subluminal, the circular orbits are stable, and the gravitational energy is negative, confirming the attractive nature of gravity. This framework provides a statistically validated, data-driven alternative to conventional dark matter halo models and establishes a direct connection between kinematical observables and relativistic spacetime geometry.

astro-ph.GA

Transparency of the $γ(n,p) π^-$ reaction in nuclei

The transparency of the hadrons produced in the $γ(n,p) π^-$ reaction in nuclei is calculated using the Glauber model modified by including the Fermi motion of the nucleon in the nucleus. Since the calculated results underestimates the measured transparency for $^4$He nucleus, the Glauber model is further modified by incorporating the short-range correlation of the nucleon and the color transparency of the hadron in the nucleus. The nuclear transparency of the $γ(n,p) π^-$ reaction is calculated for $θ_{π^-}$(c.m.) = 50$^{\circ}$, 70$^{\circ}$ and 90$^{\circ}$. The calculated results are compared with the data reported for $^4$He nucleus.

nucl-th

Resonance nucleon scattering amplitude in the photonuclear reaction

The cross section of the photonuclear reaction in the nucleon-resonance region is calculated to search the resonance-nucleon scattering amplitude in the nucleus. It is assumed that the resonance $R$ is produced and decayed in the elementary photon-nucleon $(γN)$ reaction in the nucleus as $γN \to R \to γN$. The resonance interacts with the nucleons while propagating through the nucleus. Therefore, the calculated photonuclear reaction cross section is compared with the data to extract the resonance-nucleon scattering parameters in the nucleus.

nucl-th

Nuclear transparency of the charged hadron produced in the inclusive electronuclear reaction

The nuclear transparency of the charged hadron produced in the inclusive $(e,e^\prime)$ reaction on the nucleus has been calculated using Glauber model for the nuclear reaction. The color transparency (CT) of the produced hadron and the short-range correlation (SRC) of the nucleons in the nucleus have been incorporated in the Glauber model to investigate their effects on the nuclear transparency of the hadron. The calculated nuclear transparencies for the proton and pion are compared with the data.

nucl-th

Nuclear effects on the $ρ$ meson produced in the inclusive photonuclear reaction

The hadronic properties of the $ρ$ meson produced in the inclusive photonuclear reaction have been investigated. The elementary reaction occurring in the nucleus is assumed as $γN \to ρ^0 N$. The $ρ$ meson, while propagating through the nucleus, interacts with the nuclear particles, and therefore, the properties of the $ρ$ meson can be modified because of this interaction. Being a short-lived particle, the $ρ$ meson decays to various elementary particles, such as, $e^+e^-$, $π^+π^-$, .... etc. The $e^+e^-$ invariant mass, i.e., the $ρ$ meson mass, distribution spectra have been calculated to extract the information about the parameters, viz., mass and width, of the $ρ$ meson in the nucleus. The calculated results have been compared with the data reported from Jefferson Laboratory.

nucl-th

Forward coherent $ω$ and $ϕ$ mesons production in the photon induced reaction on nuclei

The differential cross sections of the forward coherent $ω$ and $ϕ$ mesons photoproduction from nuclei have been calculated using the Glauber model for the nuclear reaction. The measured cross section of the elementary reaction, i.e., $γN \to ω(ϕ) N$ reaction, are used as input in the Glauber model. The experimentally determined free-space scattering parameters of the quoted mesons have been used to evaluate the meson nucleus interactions. The sensitivity of the cross section to the Fermi-motion of the nucleon and the nucleon-nucleon short-range correlation in the nucleus are studied. The calculated results are compared with the measured cross sections.

nucl-th

Absorption of $ω$ and $ϕ$ mesons in the inclusive photonuclear reaction

The $ω$ and $ϕ$ mesons dominantly decay outside the nucleus because the decay-lengths of them are much larger than the dimension of the nucleus. Therefore, the medium modification of the above mesons is studied through their absorption in the nucleus. CLAS collaboration at Jefferson Laboratory (Jlab) has investigated the absorption of the $ω$ and $ϕ$ mesons by measuring the nuclear transparency ratios for them in the $γA \to ω(ϕ) X \to e^+e^-X$ reaction. The nuclear transparency ratios for both $ω$ and $ϕ$ mesons in the above reactions have been calculated, and those are compared with the experimental findings, reported from Jlab, to estimate the $ω$ meson nucleon and $ϕ$ meson nucleon cross sections in the nucleus.

nucl-th

Pion exchange interaction in the $γp \to p e^+e^-$ reaction

The $ρ^0-ω$ interference has been studied in the dilepton invariant mass distribution spectra in the photonuclear reaction, but that is not done for the gamma-nucleon reaction. Recent past, the $e^+e^-$ invariant mass distribution spectrum in the $γp$ reaction, i.e., $γp \to pe^+e^-$ reaction, was measured at Jefferson Laboratory to look for the $ρ^0 -ω$ interference in the multi-GeV region. To study the mechanism of this reaction, the differential cross section of the $e^+e^-$ invariant mass distribution is calculated in the quoted energy region. The reaction is assumed to proceed as $γp \to Vp$; $V \to e^+e^-$, where $V$ denotes a vector meson, i.e., either $ρ^0$ or $ω$ meson. The photoproduction of the vector meson is described by the Vector Meson Dominance (VMD) model which consists of diagonal and off-diagonal processes. The diagonal process is described as $γ\to V; ~Vp \to Vp$. The low energy $ω$ meson photoproduction data is well described by the off-diagonal process which is illustrated as $γ\to ρ^0; ~ρ^0 p \to ωp$. The reaction $ρ^0p \to ωp$ proceeds due to one pion exchange interaction. The differential cross sections of the $γp \to pe^+e^-$ reaction due to the above processes of VMD model are compared, and the significance of the pion exchange interaction is investigated in the energy region of $γ$ beam available at Jefferson Laboratory.

nucl-th

Shadowing in the low energy photonuclear reaction

The photonuclear reaction in the multi-GeV region occurs because of the electromagnetic and hadronic interaction. The later originates due to the hadronic fluctuation, i.e., vector meson, of the photon. The total cross section of the reaction is shadowed because of the vector meson nucleus (hadronic) interaction. To estimate it quantitatively, the cross section of the photonuclear reaction was calculated in the low energy region ($\sim 1-3$ GeV) using simple vector meson dominance (SVMD) model, i.e., the low lying vector mesons ($ρ^0$, $ω$ and $ϕ$ mesons) were considered. The nuclear shadowing is reinvestigated using generalized vector meson (GVMD) model, where the higher $ρ$ meson effective state ($ρ^\prime$ meson) is taken into account along with the low lying vector mesons. Using GVMD model, the shadowing and the total cross section of the photonuclear reaction are calculated in the above mentioned energy region. The calculated results have been compared with the measured spectra.

nucl-th

Modification of $Δ(1232)$ in the neutrino nucleus reaction

The remarkable observations in the pion induced and charge exchange reactions on a nucleus are the significant shift and broadening of the $Δ(1232)$-peak relative to free pion nucleon scattering. For the forward going massless leptons, the weak process $(ν_l,l)$ on a nucleon, according to Adler's partially conserved axial current theorem, is connected to the pion nucleon scattering. This mechanism is also applicable to the nucleus. Therefore, the modification of the $Δ$-peak in a nucleus can be seen in the $(ν_l,l)$ reaction since it is connected to the pion nucleus scattering. To investigate this issue quantitatively, the double differential cross sections of the forward going ejectile $l$ energy distribution in the $(ν_l,l)$ reaction are calculated in the $Δ$-excitation region for both proton and nucleus. The measured pion nucleon and pion nucleus scattering cross sections in the quoted energy region are used in these reactions as input. Since the $(ν_l,l)$ reaction is connected to the pion induced scattering, the features of the previous reaction is shown analogous to those of the later.

nucl-th

Gravastars in $f(R,\mathcal{T})$ gravity

We propose a unique stellar model under the $f(R,\mathcal{T})$ gravity by using the conjecture of Mazur-Mottola [P. Mazur and E. Mottola, Report number: LA-UR-01-5067., P. Mazur and E. Mottola, Proc. Natl. Acad. Sci. USA 101, 9545 (2004)] which is known as gravastar and a viable alternative to the black hole as available in literature. This gravastar is described by the three different regions, viz., (I) Interior core region, (II) Intermediate thin shell, and (III) Exterior spherical region. The pressure within the interior region is equal to the constant negative matter density which provides a repulsive force over the thin spherical shell. This thin shell is assumed to be formed by a fluid of ultra relativistic plasma and the pressure, which is directly proportional to the matter-energy density according to Zel'dovich's conjecture of stiff fluid [Y.B. Zel'dovich, Mon. Not. R. Astron. Soc. 160, 1 (1972)], does counter balance the repulsive force exerted by the interior core region. The exterior spherical region is completely vacuum and assumed to be de Sitter spacetime which can be described by the Schwarzschild solution. Under this specification we find out a set of exact and singularity-free solution of the collapsing star which presents several other physically valid features within the framework of alternative gravity.

gr-qc

Semihadronic and hadronic decays of $ρ^0$ and $ω$ mesons coherently photoproduced in the isoscalar nuclei

The interference of the $ρ^0$ and $ω$ mesons has been studied in the hadronic and leptonic decay channels, i.e., dipion and dilepton decay channels respectively, but this interference is not studied yet in the semihadronic or semileptonic decay channel, e.g., $V \to π^0γ$. $V$ denotes either $ρ^0$ or $ω$ meson. To look for the quoted interference in the $π^0γ$ decay channel as well as the contribution of $ρ$ meson to the cross section, the correlated $π^0γ$ invariant mass distribution spectra are calculated in the photonuclear reaction in the multi-GeV region. It is assumed that these bosons arise in the final state due to the decay of $ρ^0$ and $ω$ mesons which are photoproduced coherently in the isoscalar nucleus. The elementary reaction in the nucleus is considered to proceed as $γN \to VN$; $V \to π^0γ$. The forward propagation of the $ρ$ and $ω$ mesons and the near forward emission of pion are considered, so that they can be described by the eikonal form. The meson nucleus interactions are evaluated using $t\varrho$ approximation. Replacing the decay vertex $V \to π^0γ$ by $V \to π^+π^-$ in the above formalism, it is also used to study the $ρ-ω$ interference in the $π^+π^-$ decay channel.

nucl-th

Hadron interferences in the proton induced coherent $η$ meson production reaction on a scalar-isovector nucleus

The coherent $η$ meson energy $E_η$ distribution spectra in the proton nucleus reaction have been calculated to investigate the $π^0 - η$ mesons' interference, in addition to the study of resonance $N^*$ dynamics in the nucleus. The elementary reaction occurring in the nucleus is assumed to proceed as $ pN \to pN^* $; $ N^* \to Nη$. Born terms in the intermediate state is also considered. In a scalar-isovector nucleus, this reaction occurs because of $π^0$ and $η$ meson exchange interactions for the forward going proton and $η$ meson; other meson exchange potentials do not contribute in this process. The sensitivity of the cross section to the hadron nucleus interactions, and the beam energy dependence of the cross section are studied for this reaction.

nucl-th

$π^0$ and $η$ meson exchange interactions in the coherent $η$ meson production in the nucleus

The energy transfer spectra have been calculated for the coherent $η$ meson production in the proton nucleus reaction. The elementary reaction occurring in the nucleus is considered as $ pN \to pN^*(1535) $; $ N^*(1535) \to Nη$. The $N^*(1535)$ excitation for the forward going proton and $η$ meson is occurred due to the $π^0$ and $η$ meson exchange interactions, other mesons do not contribute in this process. The cross sections are calculated for the $π^0$ and $η$ meson exchange interactions, and the effect of their interference on the cross section is also studied. The initial and final state interactions as well as the $N^*(1535)$ nucleus interaction are addressed by the optical potentials. The distorted wave functions for proton and $η$ meson are described by the eikonal form. The sensitivity of the cross section to the hadron nucleus potential is presented.

nucl-th

Effect of in-medium parameters of rho meson in its photoproduction reactions on nuclei

There exist model calculations showing the modification of the hadronic parameters of $ρ$ meson in the nuclear environment. From these parameters, we extract the $ρ$ meson nucleus optical potential and show the medium effect due to this potential on the $ρ$ meson mass distribution spectra in the photonuclear reaction. The calculated results reproduced reasonably the measured $e^+e^-$ invariant mass, i.e., $ρ$ meson mass, distribution spectra in the $( γ, ρ^0 \to e^+e^- )$ reaction on nuclei.

nucl-th

Resonance dynamics in the coherent $η$ meson production in the $(p,p^\prime)$ reaction on the spin-isospin saturated nucleus

For the forward going proton and $η$ meson, the coherent $η$ meson production in the $(p,p^\prime)$ reaction on the spin-isospin saturated nucleus occurs only due to the $η$ meson exchange interaction between the beam proton and nucleus. In this process, the nucleon in the nucleus can be excited to resonances $N^*$ and the $η$ meson in the final state can arise due to $N^* \to Nη$. We investigate the dynamics of resonances, including nucleon Born terms, and their interferences in the coherently added cross section of this reaction. We discuss the importance of $N(1520)$ resonance and show the sensitivity of the cross section to the hadron nucleus interaction.

nucl-th

Broadening of $ρ(\to e^+e^-)$ meson produced coherently in the photonuclear reaction

The $e^+e^-$ invariant mass distribution spectra are calculated to estimate the hadron parameters of the $ρ$ meson produced coherently in the photonuclear reaction. The elementary reaction occurring in the nucleus is considered to proceed as $ γN \to ρ^0 N ; ~ ρ^0 \to e^+e^- $. We describe the elementary $ρ$ meson photoproduction by the experimentally determined reaction amplitude $ f_{ γN \to ρ^0 N } $. The $ρ$ meson propagator is presented by the eikonal form, and the $ρ$ meson nucleus optical potential $V_{Oρ}$ appearing in it is estimated using the "$t\varrho$" approximation. The $ρ$ meson nucleon scattering amplitude $ f_{ ρN } $ extracted from the measurements is used to generate this potential. The calculated $e^+e^-$ invariant mass distribution spectra are compared with those measured at Jefferson Laboratory. The calculated results for the transparency ratio are also presented.

nucl-th