SAYANTAN GHOSH

Mr. SAYANTAN GHOSH

orcid

Research Focus & Metrics

Academic Career Length

4Years (2023-Present)

(Calculated once Scilit publication data is synced: current year − year of first publication + 1)

Representative Publications

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1 October 2023 in Journal of Cosmology and Astroparticle Physics
Verified
Journal Article
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PRPinku Routaray
Pinku Routaray
SMSailesh Ranjan Mohanty
Sailesh Ranjan Mohanty
HDH. C. Das
H. C. Das
SGSAYANTAN GHOSH
SAYANTAN GHOSH
PKProbit Jyoti Kalita
Probit Jyoti Kalita
BKBharat Kumar
Bharat Kumar
The fastest and heaviest pulsar, PSR J0952-0607, with a mass of M = 2.35±0.17 M ⊙, has recently been discovered in the disk of the Milky Way Galaxy. In response to this discovery, a new RMF model, 'NITR' has been developed. The NITR model's naturalness has been confirmed by assessing its validity for various finite nuclei and nuclear matter properties, including incompressibility, symmetry energy, and slope parameter values of 225.11, 31.69, and 43.86 MeV, respectively. These values satisfy the empirical/experimental limits currently available. The maximum mass and canonical radius of a neutron star (NS) calculated using the NITR model parameters are 2.355 M ⊙ and 13.13 km, respectively, which fall within the range of PSR J0952-0607 and the latest NICER limit. This study aims to test the consistency of the NITR model by applying it to various systems. As a result, its validity is extensively calibrated, and all the nuclear matter and NS properties of the NITR model are compared with two established models such as IOPB-I and FSUGarnet. In addition, the NITR model equation of state (EOS) is employed to obtain the properties of a dark matter admixed NS (DMANS) using two approaches (I) single-fluid and (II) two-fluid approaches. In both cases, the EOS becomes softer due to DM interactions, which reduces various macroscopic properties such as maximum mass, radius, tidal deformability, etc. The various observational data such as NICER and HESS are used to constrain the amount of DM in both cases. Moreover, we discuss the impact of dark matter (DM) on the nonradial f-mode frequency of the NS in a single fluid case only and try to constrain the amount of DM using different theoretical limits available in the literature.

19 April 2023 in Galaxies
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Journal Article
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SSSouhardya Sen
Souhardya Sen
SKShubham Kumar
Shubham Kumar
AKAthul Kunjipurayil
Athul Kunjipurayil
PRPinku Routaray
Pinku Routaray
SGSAYANTAN GHOSH
SAYANTAN GHOSH
BKBharat Kumar
Bharat Kumar
We study radial oscillations in non-rotating neutron stars by considering the unified equation of states (EoSs), which support the 2 M⊙ star criterion. We solve the Sturm–Liouville problem to compute the 20 lowest radial oscillation modes and their eigenfunctions for a neutron star modeled with eight selected unified EoSs from distinct Skyrme–Hartree–Fock, relativistic mean field and quarkyonic models. We compare the behavior of the computed eigenfrequency for an NS modeled with hadronic to one with quarkyonic EoSs while varying the central densities. The lowest-order f-mode frequency varies substantially between the two classes of the EoS at 1.4 M⊙ but vanishes at their respective maximum masses, consistent with the stability criterion ∂M/∂ρc>0. Moreover, we also compute large frequency separation and discover that higher-order mode frequencies are significantly reduced by incorporating a crust in the EoS.

1 March 2024 in Journal of Cosmology and Astroparticle Physics
Verified
Journal Article
Closed access
SMSailesh Ranjan Mohanty
Sailesh Ranjan Mohanty
SGSAYANTAN GHOSH
SAYANTAN GHOSH
PRPinku Routaray
Pinku Routaray
HDH. C. Das
H. C. Das
BKBharat Kumar
Bharat Kumar
Anisotropy in pressure within a star emerges from exotic internal processes. In this study, we incorporate pressure anisotropy using the Quasi-Local model. Macroscopic properties, including mass (M), radius (R), compactness (C), dimensionless tidal deformability (Λ), the moment of inertia (I), and oscillation frequency (f), are explored for the anisotropic neutron star. Magnitudes of these properties are notably influenced by anisotropy degree. Universal I–f–C relations for anisotropic stars are explored in this study. The analysis encompasses various EOS types, spanning from relativistic to non-relativistic regimes. Results show the relation becomes robust for positive anisotropy, weakening with negative anisotropy. The distribution of f-mode across M–R parameter space as obtained with the help of C–f relation was analyzed for different anisotropic cases. Using tidal deformability data from GW170817 and GW190814 events, a theoretical limit for canonical f-mode frequency is established for isotropic and anisotropic neutron stars. For isotropic case, canonical f-mode frequency for GW170817 event is f 1.4 = 2.606+0.457 -0.484kHz; for GW190814 event, it is f 1.4 = 2.097+0.124 -0.149kHz. These relationships can serve as reliable tools for constraining nuclear matter EOS when relevant observables are measured.

26 June 2024 in Physical Review D
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Journal Article
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SMSailesh Ranjan Mohanty
Sailesh Ranjan Mohanty
SGSAYANTAN GHOSH
SAYANTAN GHOSH
BKBharat Kumar
Bharat Kumar
Neutron stars (NSs) are incredibly versatile for studying various important aspects of high-energy and compact-object physics. These celestial objects contain extreme matter at incredibly high densities in their interiors, leading to the risk of instabilities that may cause them to collapse into a black hole (BH). This paper focuses on exploring the stability and gravitational collapse of NSs. For a more realistic approach we have considered the pressure to be locally anisotropic. We utilize the BL model to describe the anisotropy inside the NS. The presence of quarks in the core of an NS can heavily affect its stability. Hence, along with pure hadronic EOSs, we have also considered hadron-quark phase transition (HQPT) EOSs for this paper’s analysis. We subject the anisotropic NSs to radial perturbations to study their stability against radial oscillations. NSs exhibiting imaginary eigenfrequencies are identified as unstable, and their inevitable destiny is gravitational collapse, resulting in the formation of a BH. We consider the interior of these unstable anisotropic NSs to be a nonideal fluid in a nonadiabatic background in order to study its dynamical evolution during the collapse. We examine the temporal evolution of key properties of NSs, such as mass, density, heat flux, and anisotropy during the process of gravitational collapse. We present an innovative and viable approach to detect such high-energy gravitational collapse events, providing valuable insights into the properties of the static NS before its collapse.

26 September 2024 in Nuclear Physics B
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Journal Article
Open access
SGSAYANTAN GHOSH
SAYANTAN GHOSH
SSShahebaj Shaikh
Shahebaj Shaikh
PKProbit Jyoti Kalita
Probit Jyoti Kalita
PRPinku Routaray
Pinku Routaray
BKBharat Kumar
Bharat Kumar
BABijay Kumar Agrawal
Bijay Kumar Agrawal

1 April 2024 in Journal of Cosmology and Astroparticle Physics
Verified
Journal Article
Closed access
PKProbit Jyoti Kalita
Probit Jyoti Kalita
PRPinku Routaray
Pinku Routaray
SGSAYANTAN GHOSH
SAYANTAN GHOSH
BKBharat Kumar
Bharat Kumar
BABijay Kumar Agrawal
Bijay Kumar Agrawal
Non-radial oscillations of Neutron Stars (NSs) provide a means to learn important details regarding their interior composition and equation of state. We consider the effects of Δ-baryons on non-radial f-mode oscillations and other NS properties within the Density-Dependent Relativistic Mean Field formalism. Calculations are performed for Δ-admixed NS matter with and without hyperons. Our study of the non-radial f-mode oscillations revealed a distinct increase in frequency due to the addition of the Δ-baryons with upto 20% increase in frequency being seen for canonical NSs. Other bulk properties of NSs, including mass, radii, and dimensionless tidal deformability (Λ) were also affected by these additional baryons. Comparing our results with available observational data from pulsars (NICER) and gravitational waves (LIGO-VIRGO collaboration), we found strong agreement, particularly concerning Λ.