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The astrophysical S-factor of the 12C(p,γ0)13N reaction at energies from 25 keV to 5 MeV within the framework of a modified potential cluster model with forbidden states is considered. The experimental phase shifts resonant\begin{document}$ {\delta _{^2{S_{1/2}}}} $\end{document} ![]()
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, \begin{document}$ {\delta _{^2{P_{3/2}}}} $\end{document} ![]()
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, and non-resonant \begin{document}$ {\delta _{^2{D_{3/2}}}} $\end{document} ![]()
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at the energies up to Ec.m. =3 MeV are reproduced with high accuracy, which provides the appropriate agreement with the experimental data for the S-factor of 1950 -2023 years. Two sets of asymptotic constant are used: Set I refers to Cw = 1.30(2), and Set II refers to Cw = 1.37(1). Set I leads to the astrophysical factor S(25) = 1.34 ± 0.02 keV·b, which is in agreement with data by Skowronski et al., 2023 – 1.34 ± 0.09 keV·b; Set II gives S(25) = 1.49 ± 0.02 keV·b, which is in agreement with data by Kettner et al., 2023 – 1.48 ± 0.09 keV·b. The reaction rates of 12C(p,γ0)13N at temperatures T9 from 0.001 to 10 are calculated. The detailed comparison with some models, the R-matrix approach, and NACRE II data for reaction rates is considered.
The astrophysical S-factor of the 12C(p,γ0)13N reaction at energies from 25 keV to 5 MeV within the framework of a modified potential cluster model with forbidden states is considered. The experimental phase shifts resonant
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In this paper we give an algebraic construction of the fused model for ABJM spin chain and find the corresponding boost operator. We also investigate the open spin Hamiltonian for fused model and point out the general common structures of the boundary terms.
In this paper we give an algebraic construction of the fused model for ABJM spin chain and find the corresponding boost operator. We also investigate the open spin Hamiltonian for fused model and point out the general common structures of the boundary terms.
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The\begin{document}$ ^{252} {\rm{Cf}}$\end{document} ![]()
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isotope produced at Oak Ridge National Laboratory is a promising target material for the synthesis of new superheavy nuclei through fusion reaction experiments. Within the framework of the dinuclear system model, the reaction systems with the \begin{document}$ ^{252} {\rm{Cf}}$\end{document} ![]()
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target and the \begin{document}$ ^{48} {\rm{Ca}}$\end{document} ![]()
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, \begin{document}$ ^{45} {\rm{Sc}}$\end{document} ![]()
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, \begin{document}$ ^{50} {\rm{Ti}}$\end{document} ![]()
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, \begin{document}$ ^{51} {\rm{V}}$\end{document} ![]()
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, \begin{document}$ ^{54} {\rm{Cr}}$\end{document} ![]()
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, \begin{document}$ ^{55} {\rm{Mn}}$\end{document} ![]()
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projectiles are investigated for the synthesis of new isotopes \begin{document}$ ^{295-297} {\rm{Og}}$\end{document} ![]()
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, \begin{document}$ ^{292-294} {\rm{119}}$\end{document} ![]()
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, \begin{document}$ ^{297-299} {\rm{120}}$\end{document} ![]()
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, \begin{document}$ ^{298-300} {\rm{121}}$\end{document} ![]()
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, \begin{document}$ ^{301-303} {\rm{122}}$\end{document} ![]()
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and \begin{document}$ ^{302-304} {\rm{123}}$\end{document} ![]()
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. The decreasing trend of the maximal evaporation residue cross sections with the increasing proton number of the compound nucleus are discussed in the capture, fusion and survival stages. Additionally, the radioactive beam-induced reactions based on the \begin{document}$ ^{252} {\rm{Cf}}$\end{document} ![]()
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target are investigated to reach the predicted neutron shell closure N = 184, with the maximal evaporation residue cross section predicted to be 21 fb for synthesizing \begin{document}$ ^{302} {\rm{Og}}$\end{document} ![]()
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. The predicted results fall below the current detection limitation, indicating the necessity for advancement in both accelerator and detection techniques, as well as exploration of alternative reaction mechanisms.
The
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In this work, we develop a general perturbative procedure to find the off-equatorial plane deflections in the weak deflection limit in general stationary and axisymmetric spacetimes, allowing the existence of the generalized Carter constant. Deflections of both null and timelike rays, with the finite distance effect of the source and detector taken into account, are obtained as dual series of\begin{document}$M/r_0$\end{document} ![]()
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and \begin{document}$r_0/r_{s,d}$\end{document} ![]()
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. These deflections allow a set of exact gravitational lensing equations from which the images' apparent angular positions are solved. The method and general results are then applied to the Kerr-Newmann, Kerr-Sen, and rotating Simpson-Visser spacetimes to study the effect of the spin and characteristic (effective) charge of the spacetimes and the source altitude on the deflection angles and image apparent angles. It is found that, in general, both the spacetime spin and charge only affect the deflections from the second non-trivial order, while the source altitude influences the deflection from the leading order. Because of this, it is found that, in gravitational lensing in realistic situations, it is hard to measure the effects of the spacetime spin and charge from the images' apparent locations. We also presented the off-equatorial deflections in the rotating Bardeen, Hayward, Ghosh, and Tinchev black hole spacetimes.
In this work, we develop a general perturbative procedure to find the off-equatorial plane deflections in the weak deflection limit in general stationary and axisymmetric spacetimes, allowing the existence of the generalized Carter constant. Deflections of both null and timelike rays, with the finite distance effect of the source and detector taken into account, are obtained as dual series of
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In this paper, we investigate the topological charge and the conditions for the existence of the photon sphere (PS) in Kiselev-AdS black holes within\begin{document}$f(R, T)$\end{document} ![]()
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gravity. Furthermore, we establish their topological classifications. We employ two different methods based on Duan’s topological current ϕ-mapping theory viz analysis of temperature and the generalized Helmholtz free energy methods to study the topological classes of our black hole. By considering the mentioned black hole, we discuss the critical and zero points (topological charges and topological numbers) for different parameters. Our findings reveal that the Kiselev parameter ω and the \begin{document}$f(R, T)$\end{document} ![]()
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gravity parameter γ influence the number of topological charges of black holes, leading to novel insights into topological classifications. We observe that for given values of the free parameters, there exist total topological charges (\begin{document}$Q_{total} = -1$\end{document} ![]()
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) for T-method and total topological numbers (\begin{document}$W = +1$\end{document} ![]()
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) for the generalized Helmholtz free energy method. Our research findings elucidate that, in contrast to the scenario where \begin{document}$\omega = 1/3$\end{document} ![]()
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, in other cases, increasing the parameter γ increases the number of total topological charges for the black hole. Interestingly, for the phantom field (\begin{document}$\omega = -4/3$\end{document} ![]()
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), we observed that decreasing the parameter γ increases the number of topological charges. Additionally, we study the results for the photon sphere. The studied models reveal that the simultaneous presence of γ and ω effectively expands the permissible range for γ. In other words, the model can exhibit black hole behavior over a larger domain. Additionally, it is evident that with the stepwise reduction of ω, the region covered by singularity also diminishes and becomes more restricted. However, An interesting point about all three ranges is the elimination of the forbidden region in this model. In other words, it appears that in this model and the investigated areas, there is no region where both the ϕ function and the metric function simultaneously lack solutions. Also, at the end, we fully checked the curvatures singularities, and energy conditions for the mentioned black hole.
In this paper, we investigate the topological charge and the conditions for the existence of the photon sphere (PS) in Kiselev-AdS black holes within
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We investigate the critical collapse of spherically symmetric scalar fields in asymptotically anti-de Sitter spacetime, focusing on two scenarios: real and complex scalar fields with potentials. By fine-tuning the amplitude of the initial scalar field under different cosmological constants, we find a linear relationship between the critical amplitude of the first collapse and the cosmological constant in both scenarios. Furthermore, we observe that the slope of this linear relationship varies linearly with the coupling strength.
We investigate the critical collapse of spherically symmetric scalar fields in asymptotically anti-de Sitter spacetime, focusing on two scenarios: real and complex scalar fields with potentials. By fine-tuning the amplitude of the initial scalar field under different cosmological constants, we find a linear relationship between the critical amplitude of the first collapse and the cosmological constant in both scenarios. Furthermore, we observe that the slope of this linear relationship varies linearly with the coupling strength.
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Bremsstrahlung photons emitted during nucleon-nucleus reactions in compact star are investigated. Influence of density of stellar medium on intensity of emission is studied at first time in quantum approach. Bremsstrahlung model is generalized, where new term describing influence of stellar medium is added to interactions between nucleons of nucleus (in frameworks of nuclear model of deformed oscillatoric shells). Polytropic EOS, Chandrasekar EOS and Harrison-Wheeler EOS are applied for calculations. Unified EOS of neutron-star matter of Haensel and Potekhin based on FPS an SLy EOSs is used for tests. Bremsstrahlung calculations are tested on existed measurements of bremsstrahlung in the scattering of protons off the 197Au nuclei at energy of proton beam of\begin{document}$ E_{\rm p}=190 $\end{document} ![]()
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MeV. Many properties of bremsstrahlung emitted from nuclear processes in stellar medium of compact stars are studied at first time. In particular, the spectra of photons in the scattering of protons and neutrons off 4He, 8Be, 12C, 16O, 24Mg, 40Ca, 56Fe are estimated in dependence on density of stellar medium. Medium of white dwarfs has small influence on the bremsstrahlung emission from nuclear processes, while bremsstrahlung emission is intensive in neutron stars and it is changed essentially in dependence on stellar density and structure.
Bremsstrahlung photons emitted during nucleon-nucleus reactions in compact star are investigated. Influence of density of stellar medium on intensity of emission is studied at first time in quantum approach. Bremsstrahlung model is generalized, where new term describing influence of stellar medium is added to interactions between nucleons of nucleus (in frameworks of nuclear model of deformed oscillatoric shells). Polytropic EOS, Chandrasekar EOS and Harrison-Wheeler EOS are applied for calculations. Unified EOS of neutron-star matter of Haensel and Potekhin based on FPS an SLy EOSs is used for tests. Bremsstrahlung calculations are tested on existed measurements of bremsstrahlung in the scattering of protons off the 197Au nuclei at energy of proton beam of
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This paper investigates off-equatorial plane deflections and gravitational lensing of both null signals and massive particles in Kerr spacetime in the weak deflection limit, with the finite distance effect of the source and detector taken into account. This is the effect caused by the fact that both the source and detector are located at finite distances from the lens, while many researchers often use the deflection angle for infinite distances from sources and detectors. The deflection in both the\begin{document}$ \phi $\end{document} ![]()
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and \begin{document}$ \theta $\end{document} ![]()
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directions is computed as power series of \begin{document}$ M/r_0 $\end{document} ![]()
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and \begin{document}$ r_0/r_{\mathrm{s,d}} $\end{document} ![]()
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, where \begin{document}$ M,\,r_{\mathrm{s,d}} $\end{document} ![]()
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are the spacetime mass and source and detector radii respectively, and \begin{document}$ r_0 $\end{document} ![]()
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is the minimal radial coordinate of the trajectory. The coefficients of these series are simple trigonometric functions of \begin{document}$ \theta_ \mathrm{e} $\end{document} ![]()
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, the extreme value of the \begin{document}$ \theta $\end{document} ![]()
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coordinate of the trajectory. A set of exact gravitational lensing equations is used to solve for \begin{document}$ r_0 $\end{document} ![]()
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and \begin{document}$ \theta_ \mathrm{e} $\end{document} ![]()
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for given deviation angles \begin{document}$ \delta\theta $\end{document} ![]()
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and \begin{document}$ \delta\phi $\end{document} ![]()
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of the source, and two lensed images are always obtained. The apparent angles and their magnifications of these images, and the time delays between them are solved and their dependence on various parameters, especially spacetime spin \begin{document}$ \hat{a} $\end{document} ![]()
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are analyzed in great detail. It is found that there generally exist two critical spacetime spin values that separate the case of test particles reaching the detector from different sides of the \begin{document}$ z $\end{document} ![]()
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axis from the cases in which the images appear from the same side in the celestial plane. Three potential applications of these results are discussed.
This paper investigates off-equatorial plane deflections and gravitational lensing of both null signals and massive particles in Kerr spacetime in the weak deflection limit, with the finite distance effect of the source and detector taken into account. This is the effect caused by the fact that both the source and detector are located at finite distances from the lens, while many researchers often use the deflection angle for infinite distances from sources and detectors. The deflection in both the
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Background: The lightest uranium isotope\begin{document}$ {\rm^{214}U} $\end{document} ![]()
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has been produced using the Heavy Ion Research Facility in Lanzhou, China. It is found that the α-decay reduced width (\begin{document}$ \delta^{2} $\end{document} ![]()
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) of \begin{document}$ {\rm^{214}U} $\end{document} ![]()
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is significantly larger than other nuclei by a factor of two. However, the extraction of \begin{document}$ \delta^{2} $\end{document} ![]()
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depends on the penetration probability (P) through the barrier, and P is related to the theoretical method of obtaining it and the form of the α-core potential. Purpose: The aim of the present study is to investigate whether the selections of the α-core potential and the method of calculating P can affect the above conclusion. Method: Four different phenomenological α-core potentials and two microscopic double-folding potentials, together with the Wentzel-Kramers-Brillouin (WKB) approximation and the transfer matrix (TM) approach are used to obtain P. Results: The value of P obtained with WKB is about 20% ~ 40% smaller than the one obtained with TM approach, and consequently the deduced \begin{document}$ \delta^{2} $\end{document} ![]()
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is overestimated. The choice of α-core potential can significantly affect the value of the \begin{document}$ \delta^{2} $\end{document} ![]()
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. With spherical form for the α-core potentials, the \begin{document}$ \delta^{2} $\end{document} ![]()
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of \begin{document}$ {\rm^{214}U} $\end{document} ![]()
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obtained with both WKB and TM approaches are about twice as large as that of the surrounding nuclei. While with the deformed double-folding potential, the ratio between \begin{document}$ \delta^{2} $\end{document} ![]()
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of \begin{document}$ {\rm^{214}U} $\end{document} ![]()
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and that of the surrounding nuclei is found slightly below 2. Conclusions: Effects of nuclear deformation and the α-core potential should be considered when studying the α-decay reduced width in the \begin{document}$ N_{p}N_{n} $\end{document} ![]()
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systematic.
Background: The lightest uranium isotope
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Heavy-ion fusion reaction is relevant to a number of important issues not only in stellar environment but also in the synthesis of new nuclides and superheavy elements. In this work, the role of Pauli blocking and isospin effect in sub-barrier fusion reactions is investigated within the well established coupled-channels method. An isospin-dependent Pauli blocking potential is proposed to better address the deep sub-barrier fusion hindrance problem. It is found that the Pauli blocking effect manifests itself strongly for isospin symmetric targets and is reduced for targets with large isospin asymmetries. The agreement between experimental and theoretical fusion cross sections is improved for both 12C-target and 16O-target systems.
Heavy-ion fusion reaction is relevant to a number of important issues not only in stellar environment but also in the synthesis of new nuclides and superheavy elements. In this work, the role of Pauli blocking and isospin effect in sub-barrier fusion reactions is investigated within the well established coupled-channels method. An isospin-dependent Pauli blocking potential is proposed to better address the deep sub-barrier fusion hindrance problem. It is found that the Pauli blocking effect manifests itself strongly for isospin symmetric targets and is reduced for targets with large isospin asymmetries. The agreement between experimental and theoretical fusion cross sections is improved for both 12C-target and 16O-target systems.
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Using\begin{document}$ (1.0087\pm0.0044)\times10^{10} $\end{document} ![]()
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\begin{document}$ J/\psi $\end{document} ![]()
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events collected by the BESIII detector at the BEPCII collider, we search for the lepton number violation decay \begin{document}$ \phi \to \pi^+ \pi^+ e^- e^- $\end{document} ![]()
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via \begin{document}$ J/\psi\to \phi\eta $\end{document} ![]()
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. No signal is found and the upper limit on the branching fraction of \begin{document}$ \phi \to \pi^+ \pi^+ e^- e^- $\end{document} ![]()
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is set to be \begin{document}$ 1.3\times10^{-5} $\end{document} ![]()
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at the 90% confidence level.
Using
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In this paper, we base our analysis on the assumption that the existence of a photon sphere is an intrinsic feature of any ultra-compact gravitational structure with spherical symmetry. Utilizing the concept of a topological photon sphere, we categorize the behaviors of various gravitational models based on the structure of their photon spheres. This innovative approach enables us to define boundaries for black hole parameters, subsequently allowing us to classify the model as either a black hole or a naked singularity. Indeed, we will demonstrate that the presence of this interplay between the gravitational structure and the existence of a photon sphere is a unique advantage that can be utilized from both perspectives. Our observations indicate that a gravitational model typically exhibits the behavior of a horizonless structure (or a naked singularity) when a minimum effective potential (a stable photon sphere) appears within the studied spacetime region. Additionally, in this study, we tried to investigate the effect of this structure on the behavior of the photon sphere by choosing models that are affected by the Perfect Fluid Dark Matter (PFDM). Finally, by analyzing a model with multiple event horizons, we show that the proposed method remains applicable even in such scenarios.
In this paper, we base our analysis on the assumption that the existence of a photon sphere is an intrinsic feature of any ultra-compact gravitational structure with spherical symmetry. Utilizing the concept of a topological photon sphere, we categorize the behaviors of various gravitational models based on the structure of their photon spheres. This innovative approach enables us to define boundaries for black hole parameters, subsequently allowing us to classify the model as either a black hole or a naked singularity. Indeed, we will demonstrate that the presence of this interplay between the gravitational structure and the existence of a photon sphere is a unique advantage that can be utilized from both perspectives. Our observations indicate that a gravitational model typically exhibits the behavior of a horizonless structure (or a naked singularity) when a minimum effective potential (a stable photon sphere) appears within the studied spacetime region. Additionally, in this study, we tried to investigate the effect of this structure on the behavior of the photon sphere by choosing models that are affected by the Perfect Fluid Dark Matter (PFDM). Finally, by analyzing a model with multiple event horizons, we show that the proposed method remains applicable even in such scenarios.
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The Preformed Cluster Model (PCM) is applied to investigate the heavy particle radioactivity (HPR) and spontaneous fission (SF) processes for even-Z superheavy nuclear systems. Different proximity potentials are used to calculate decay half-lives of Z=112-120 nuclei. The fragmentation potential and preformation distribution suggest that spontaneous fission is the major contributor upto Z=114 and HPR starts competing for heavier nuclei. The heavy cluster emission is supported by Pb-magicity whereas SF is reinforced due to the deformations of fission fragments. The heavy cluster decay half-lives (Log\begin{document}$ _{10} $\end{document} ![]()
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TC) are calculated using PCM and are compared with the estimates of Analytical Super Asymmetric Fission (ASAF) Model. The calculated Log\begin{document}$ _{10} $\end{document} ![]()
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TC show nice agreement with the ASAF measurements for the use of Prox-00 and Mod Prox-00 versions of potentials. However, Prox-77, Prox-88, and Prox-BW-91 are not appropriate to address the Log\begin{document}$ _{10} $\end{document} ![]()
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TC for Z\begin{document}$ \geq $\end{document} ![]()
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116 nuclei. In order to resolve this, Z-dependence in the radius parameters is included. Interestingly, half-lives match the ASAF data after the inclusion of Z-dependence. The branching ratios are also calculated for superheavy nuclei and compared with the estimates of Unified description (UD) formula, Universal (UNIV) curve, Universal decay law (UDL), Horoi formula and ASAF measurements. Further, the spontaneous fission half-lives (\begin{document}$ T_{SF} $\end{document} ![]()
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) of \begin{document}$ ^{282} $\end{document} ![]()
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Cn, \begin{document}$ ^{284} $\end{document} ![]()
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Cn, \begin{document}$ ^{284} $\end{document} ![]()
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Fl and \begin{document}$ ^{286} $\end{document} ![]()
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Fl superheavy nuclei are also estimated through various proximity potentials. Among all, Prox-00 is appropriate to address the experimental data nicely. Using same, the spontaneous fission half-lives are estimated through PCM for Z=116-120 isotopes at different neck-length parameters. Finally, the scaled total kinetic energy (TKE) values are compared nicely with the available data.
The Preformed Cluster Model (PCM) is applied to investigate the heavy particle radioactivity (HPR) and spontaneous fission (SF) processes for even-Z superheavy nuclear systems. Different proximity potentials are used to calculate decay half-lives of Z=112-120 nuclei. The fragmentation potential and preformation distribution suggest that spontaneous fission is the major contributor upto Z=114 and HPR starts competing for heavier nuclei. The heavy cluster emission is supported by Pb-magicity whereas SF is reinforced due to the deformations of fission fragments. The heavy cluster decay half-lives (Log
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The current study explores the production of charged Higgs particles through photon-photon collisions within the context of the Two Higgs Doublet Model, including one-loop-level scattering amplitudes of Electroweak and QED radiation. The cross-section has been scanned for plane (\begin{document}$m_{\phi^{0}}, \sqrt{s}$\end{document} ![]()
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) investigating the process of \begin{document}$\gamma\gamma \rightarrow H^{+}H^{-}$\end{document} ![]()
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. Three particular numerical scenarios i.e., low-\begin{document}$m_{H}$\end{document} ![]()
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, non-alignment, and short-cascade are employed. The decay channels for charged Higgs particles are examined using \begin{document}$h^{0}$\end{document} ![]()
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for low-\begin{document}$m_{H^{0}}$\end{document} ![]()
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and \begin{document}$H^{0}$\end{document} ![]()
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for non-alignment and short-cascade scenario incorporating the new experimental and theoretical constraints along with the analysis for cross-sections. It reveals that at low energy, it is consistently higher for all scenarios. However, as \begin{document}$\sqrt{s}$\end{document} ![]()
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increases, it reaches a peak value at 1\begin{document}$~$\end{document} ![]()
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TeV for all benchmark scenarios. The branching ratio of the decay channels indicates that for non-alignment, the mode of decay \begin{document}$W^{\pm} h^{0}$\end{document} ![]()
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takes control, and for short cascade, the prominent decay mode remains \begin{document}$t\overline {b}$\end{document} ![]()
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, while in the low-\begin{document}$m_{H}$\end{document} ![]()
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the dominant decay channel is of \begin{document}$W^{\pm} h^{0}$\end{document} ![]()
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. In our research, we employ contemporary machine-learning methodologies to investigate the production of high-energy Higgs bosons within a 3.0 TeV \begin{document}$\gamma\gamma$\end{document} ![]()
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collider. We have used multivariate approaches such as Boosted Decision Trees (BDT), LikelihoodD, and Multilayer Perceptron (MLP) to show the observability of heavy-charged Higgs Bosons versus the most significant Standard Model backgrounds. The purity of the signal efficiency and background rejection are measured for each cut value.
The current study explores the production of charged Higgs particles through photon-photon collisions within the context of the Two Higgs Doublet Model, including one-loop-level scattering amplitudes of Electroweak and QED radiation. The cross-section has been scanned for plane (
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In this paper, we delve into the optical properties of a quantum-corrected black hole (BH) in loop quantum gravity, surrounded by a plasma medium. We first determine the photon and shadow radii resulting from quantum corrections and the plasma medium in the environment surrounding a quantum-corrected BH. We find that the photon sphere and the BH shadow radii decrease due to the quantum correction parameter α acting as a repulsive gravitational charge. We further delve into the gravitational weak lensing by applying the general formalism used to model the deflection angle of the light traveling around the quantum-corrected BH placed in the plasma medium. We show, in conjunction with the fact that the combined effects of the quantum correction and non-uniform plasma frequency parameter can decrease the deflection angle, that the light traveling through the uniform plasma can be strongly deflected compared to the non-uniform plasma environment surrounding the quantum-corrected BH. Finally, we consider the magnification of the lensed image brightness under the effect of the quantum correction parameter α, together with the uniform and non-uniform plasma effects.
In this paper, we delve into the optical properties of a quantum-corrected black hole (BH) in loop quantum gravity, surrounded by a plasma medium. We first determine the photon and shadow radii resulting from quantum corrections and the plasma medium in the environment surrounding a quantum-corrected BH. We find that the photon sphere and the BH shadow radii decrease due to the quantum correction parameter α acting as a repulsive gravitational charge. We further delve into the gravitational weak lensing by applying the general formalism used to model the deflection angle of the light traveling around the quantum-corrected BH placed in the plasma medium. We show, in conjunction with the fact that the combined effects of the quantum correction and non-uniform plasma frequency parameter can decrease the deflection angle, that the light traveling through the uniform plasma can be strongly deflected compared to the non-uniform plasma environment surrounding the quantum-corrected BH. Finally, we consider the magnification of the lensed image brightness under the effect of the quantum correction parameter α, together with the uniform and non-uniform plasma effects.
Universal thermodynamic relations with constant corrections for five-dimensional de Sitter spacetime
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This paper expands on the method proposed by Goon and Penco for studying the universality of thermodynamic relations with corrections in de Sitter black holes. Furthermore, based on our analysis of Non-linear magnetic-charged black hole in the dS spacetime, five-dimensional de Sitter Hairy spacetime and Five-dimensional Charged-dS rotating dS black hole, we demonstrate the universality of the thermodynamic relation in de Sitter black holes.we which gives a universal conjecture relation between the shifted thermodynamic quantities for arbitrary black hole background. We believe that these universal relations will shed new light on the region of the quantum gravity.
This paper expands on the method proposed by Goon and Penco for studying the universality of thermodynamic relations with corrections in de Sitter black holes. Furthermore, based on our analysis of Non-linear magnetic-charged black hole in the dS spacetime, five-dimensional de Sitter Hairy spacetime and Five-dimensional Charged-dS rotating dS black hole, we demonstrate the universality of the thermodynamic relation in de Sitter black holes.we which gives a universal conjecture relation between the shifted thermodynamic quantities for arbitrary black hole background. We believe that these universal relations will shed new light on the region of the quantum gravity.
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A formalism has been developed for calculating the signal of violation of time-reversal invariance, provided that space-reflection (parity) invariance is conserved during the scattering of tensor-polarized deuterons on vector-polarized ones. The formalism is based on the Glauber theory with the full consideration of spin dependence of\begin{document}$ NN $\end{document} ![]()
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elastic scattering amplitudes and spin structure of colliding deuterons. The numerical calculations have been carried out in the range of laboratory proton energies of \begin{document}$ T_p = 0.1 $\end{document} ![]()
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–1.2 GeV using the SAID database for spin amplitudes and in the energy region of the SPD NICA experiment corresponding to the invariant mass of the interacting nucleon pairs \begin{document}$ \sqrt{s_{NN}} = 2.5 $\end{document} ![]()
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–25 GeV, using two phenomenological models of \begin{document}$ pN $\end{document} ![]()
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elastic scattering. It is found that only one type of the time-reversal non-invariant parity conserving \begin{document}$ NN $\end{document} ![]()
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interaction gives a non-zero contribution to the signal in question, that is important for isolating an unknown constant of this interaction from the corresponding data.
A formalism has been developed for calculating the signal of violation of time-reversal invariance, provided that space-reflection (parity) invariance is conserved during the scattering of tensor-polarized deuterons on vector-polarized ones. The formalism is based on the Glauber theory with the full consideration of spin dependence of
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We consider a Lagrangian to describe gravity using a nonlinear term depending on the Gauss-Bonnet invariant. We examine the conditions for a bouncing and the existence of an ulterior accelerated phase of the Universe.
We consider a Lagrangian to describe gravity using a nonlinear term depending on the Gauss-Bonnet invariant. We examine the conditions for a bouncing and the existence of an ulterior accelerated phase of the Universe.
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By combining the Skyrme-Hartree-Fock method with complex momentum representation (CMR), the resonant states of\begin{document}$ {}^{17}_\Lambda $\end{document} ![]()
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O, \begin{document}$ {}^{41}_{\Lambda} $\end{document} ![]()
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Ca, \begin{document}$ {}^{49}_{\Lambda} $\end{document} ![]()
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Ca, and \begin{document}$ {}^{57}_\Lambda $\end{document} ![]()
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Ni are investigated. The phase shifts for hyperon-nucleus elastic scattering are determined with continuum level density (CLD) and the scatting length as well as the resonance energy are obtained by utilizing the effective range expansion. Our method abbreviated as CMR-CLD exhibits good consistency with traditional approaches and provides some ground work for investigating scattering and resonance problems in deformed hypernuclei and multi-hyperon hypernuclei.
By combining the Skyrme-Hartree-Fock method with complex momentum representation (CMR), the resonant states of
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The coupled reaction channel approach has proven to be quite effective in explaining the mechanism of nucleon transfer in heavy-ion reactions. Nevertheless, significant ambiguities remain regarding the selection of potential parameters and the states of the nuclei that should be coupled together for a specific reaction channel. We have analyzed the excitation functions for one- and two-neutron transfer in\begin{document}$ ^{6,7} $\end{document} ![]()
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Li-induced reactions on various targets using the coupled reaction channel formalism. Spectroscopic amplitudes are taken from existing literature and shell model calculations. The one-neutron transfer cross sections from \begin{document}$ ^{6} $\end{document} ![]()
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Li+\begin{document}$ ^{93} $\end{document} ![]()
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Nb and \begin{document}$ ^{7} $\end{document} ![]()
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Li+\begin{document}$ ^{115} $\end{document} ![]()
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In reactions are reasonably well reproduced by coupled reaction channel calculations. A reasonable match for the measured cross sections has also been obtained for the two-neutron transfer in \begin{document}$ ^{7} $\end{document} ![]()
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Li+\begin{document}$ ^{181} $\end{document} ![]()
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Ta reaction by employing the extreme cluster model.
The coupled reaction channel approach has proven to be quite effective in explaining the mechanism of nucleon transfer in heavy-ion reactions. Nevertheless, significant ambiguities remain regarding the selection of potential parameters and the states of the nuclei that should be coupled together for a specific reaction channel. We have analyzed the excitation functions for one- and two-neutron transfer in
Layout optimization and Performance of Large Array of imaging atmospheric Cherenkov Telescope (LACT)
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Large Array of imaging atmospheric Cherenkov Telescope (LACT) is an array of 32 Cherenkov telescopes with 6-meter diameter mirrors to be constructed at the LHAASO site. In this work, we present a study on the layout optimization and performance analysis of LACT. We investigate two observation modes: large zenith angle observations for ultra-high energy events and small zenith angle observations for lower energy thresholds. For large zenith angles (60°), simulations show that an 8-telescope subarray can achieve an effective area of\begin{document}$ 3 \; \rm km^2 $\end{document} ![]()
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and excellent angular resolution. For small zenith angles, we optimize the layout of 4-telescope cells and the full 32-telescope array. The threshold of the full array is about 200 GeV, which is particularly crucial for studying transient phenomena, including gamma-ray bursts (GRBs) and active galactic nuclei (AGNs). This study provides important guidance for the final LACT layout design and performance estimates under different observational conditions, demonstrating LACT's potential for deep observations of ultra-high energy γ-ray sources and morphological studies of PeVatrons, as well as time-domain γ-ray astronomy.
Large Array of imaging atmospheric Cherenkov Telescope (LACT) is an array of 32 Cherenkov telescopes with 6-meter diameter mirrors to be constructed at the LHAASO site. In this work, we present a study on the layout optimization and performance analysis of LACT. We investigate two observation modes: large zenith angle observations for ultra-high energy events and small zenith angle observations for lower energy thresholds. For large zenith angles (60°), simulations show that an 8-telescope subarray can achieve an effective area of
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The present work discusses methods for estimating the moments of inertia of fission fragments resulting from the spontaneous fission of the isotope Cf-252. In particular, two main approaches are mentioned: statistical and microscopic. Furthermore, the classical and superfluid approaches to calculating the moments of inertia are examined, along with their implementation in a variety of nuclear models. In this context, the impact of diverse oscillation modes and nucleon exchange on the moments of inertia and spin distributions of fission fragments is assessed. The authors highlight the necessity for a comparative analysis of theoretical predictions with experimental data, which would facilitate a more comprehensive understanding of the internal structure of nuclei and fission mechanisms.
The present work discusses methods for estimating the moments of inertia of fission fragments resulting from the spontaneous fission of the isotope Cf-252. In particular, two main approaches are mentioned: statistical and microscopic. Furthermore, the classical and superfluid approaches to calculating the moments of inertia are examined, along with their implementation in a variety of nuclear models. In this context, the impact of diverse oscillation modes and nucleon exchange on the moments of inertia and spin distributions of fission fragments is assessed. The authors highlight the necessity for a comparative analysis of theoretical predictions with experimental data, which would facilitate a more comprehensive understanding of the internal structure of nuclei and fission mechanisms.
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The Jiangmen Underground Neutrino Observatory (JUNO) is a multi-purpose neutrino experiment under construction in South of China. This paper presents an updated estimate of JUNO’s sensitivity to the neutrino mass ordering using the reactor antineutrinos emitted from eight nuclear reactor cores in the Taishan and Yangjiang nuclear power plants. This measurement is planned by studying the fine interference pattern caused by quasi-vacuum oscillations in the oscillated antineutrino spectrum at a baseline of 52.5 km and is completely independent of the CP violating phase and the neutrino mixing angle θ23. The sensitivity is obtained through a joint analysis of JUNO and TAO detectors utilizing the best available knowledge to date about the location and overburden of the JUNO experimental site, the local and global nuclear reactors, the JUNO and TAO detectors responses, the expected event rates and spectra of signal and backgrounds, and the systematic uncertainties of the analysis inputs. It is found that a 3σ median sensitivity to reject the wrong mass ordering hypothesis can be reached with an exposure of about 6.5 years × 26.6 GW thermal power.
The Jiangmen Underground Neutrino Observatory (JUNO) is a multi-purpose neutrino experiment under construction in South of China. This paper presents an updated estimate of JUNO’s sensitivity to the neutrino mass ordering using the reactor antineutrinos emitted from eight nuclear reactor cores in the Taishan and Yangjiang nuclear power plants. This measurement is planned by studying the fine interference pattern caused by quasi-vacuum oscillations in the oscillated antineutrino spectrum at a baseline of 52.5 km and is completely independent of the CP violating phase and the neutrino mixing angle θ23. The sensitivity is obtained through a joint analysis of JUNO and TAO detectors utilizing the best available knowledge to date about the location and overburden of the JUNO experimental site, the local and global nuclear reactors, the JUNO and TAO detectors responses, the expected event rates and spectra of signal and backgrounds, and the systematic uncertainties of the analysis inputs. It is found that a 3σ median sensitivity to reject the wrong mass ordering hypothesis can be reached with an exposure of about 6.5 years × 26.6 GW thermal power.
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We investigate the soft behavior of the tree-level Rutherford scattering processes mediated via t-channel one-graviton exchange. We consider two types of Rutherford scattering processes, e.g., a low-energy massless structureless projectile (up to spin-1) hits a static massive composite particle carrying various spins (up to spin-2), and a slowly-moving light projectile hits a heavy static composite target. The unpolarized cross sections in the first type are found to exhibit universal forms at the first two orders in\begin{document}$ 1/M $\end{document} ![]()
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expansion, yet differ at the next-to-next-to-leading order, though some terms at this order still remain universal or depend on the target spin in a definite manner. The unpolarized cross sections in the second type are universal at the lowest order in projectile velocity expansion and through all orders in \begin{document}$ 1/M $\end{document} ![]()
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, independent of the spins of both projectile and target. The universality partially breaks down at relative order-\begin{document}$ v^2/M^2 $\end{document} ![]()
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, albeit some terms at this order still depend on the target spin in a specific manner.
We investigate the soft behavior of the tree-level Rutherford scattering processes mediated via t-channel one-graviton exchange. We consider two types of Rutherford scattering processes, e.g., a low-energy massless structureless projectile (up to spin-1) hits a static massive composite particle carrying various spins (up to spin-2), and a slowly-moving light projectile hits a heavy static composite target. The unpolarized cross sections in the first type are found to exhibit universal forms at the first two orders in
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We investigate the bound-state equations in two-dimensional QCD in the\begin{document}$ N_c\to \infty $\end{document} ![]()
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limit. We consider two types of hadrons, an exotic "meson" (which is composed of a bosonic quark and a bosonic anti-quark), and an exotic "baryon" (composed of a fermionic quark and a bosonic antiquark). Using the Hamiltonian operator approach, we derive the corresponding bound-state equations for both types of hadrons from the perspectives of the light-front quantization and equal-time quantization, and confirm the known results. We also present a novel diagrammatic derivation for the exotic "meson" bound-state equation in the equal-time quantization. The bound-state equation for the exotic baryons in the equal-time quantization in two-dimensional QCD is new. We also numerically solve various bound-state equations, obtain the hadron spectrum and the bound-state wave functions of the lowest-lying states. We explicitly demonstrate the pattern that as the hadron is boosted to the infinite-momentum frame, the forward-moving bound-state wave function approaches the corresponding light-front wave function.
We investigate the bound-state equations in two-dimensional QCD in the
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We investigate the soft behavior of the tree-level Rutherford scattering process. We consider two types of Rutherford scattering, a low-energy massless point-like projectile (say, a spin-\begin{document}$ {1\over 2} $\end{document} ![]()
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or spin-\begin{document}$ 0 $\end{document} ![]()
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electron) hits a static massive composite target particle carrying various spins (up to spin-\begin{document}$ 2 $\end{document} ![]()
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), and a slowly-moving light projectile hits a heavy static composite target. For the first type, the unpolarized cross sections in the laboratory frame are found to exhibit universal forms in the first two orders of \begin{document}$ 1/M $\end{document} ![]()
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expansion, yet differ at the next-to-next-to-leading order (though some terms at this order still remain to be universal or depend on the target spin in a definite manner). For the second type, at the lowest order in electron velocity expansion, through all orders in \begin{document}$ 1/M $\end{document} ![]()
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, the unpolarized cross section is universal (also not sensitive to the projectile spin). The universality partially breaks down at relative order-\begin{document}$ v^2/M^2 $\end{document} ![]()
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, though some terms at this order are still universal or depend on the target spin in a specific manner. We also employ the effective field theory approach to reproduce the soft behavior of the differential cross sections for the target particle being a composite spin-\begin{document}$ {1\over 2} $\end{document} ![]()
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fermion.
We investigate the soft behavior of the tree-level Rutherford scattering process. We consider two types of Rutherford scattering, a low-energy massless point-like projectile (say, a spin-
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Exploring the inverse problem tied to the Page curve phenomenon and island paradigm, we investigate the geometric conditions underpinning black hole evaporation where information is preserved and islands manifest, giving rise to the characteristic Page curve. Focusing on a broad class of static spherical symmetry black hole metrics in asymptotically Minkowski or (anti-)de Sitter spacetimes, we derive a pivotal constraint: the second derivative of blacken factor\begin{document}$ f^{\prime \prime}(r_h)<\frac{6 \kappa A^{\prime}(r_h)}{cG_N} $\end{document} ![]()
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for which the island exists and reproduce the Page curve. On the other hand, starting from the quantum focusing conjecture theory, we obtain another constraint on the blacken factor: \begin{document}$ f^{\prime \prime}(r_h)< \frac{6 \kappa^2 r_h A^{\prime}(r_h) e^{2\kappa r_{\star}(b)} }{cG_N f(b)} $\end{document} ![]()
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that the theory can be satisfied. In particular, by studying these two constraints, we find that a common properties. Specifically, we reveal that a universally criterion – manifested in the negativity of the second derivative of \begin{document}$ f(r) $\end{document} ![]()
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, i.e. \begin{document}$ f^{\prime \prime} (r)<0 $\end{document} ![]()
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, in proximity to the event horizon where \begin{document}$ r \sim r_h+ {\cal O} (G_N) $\end{document} ![]()
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, ensures the emergence of Page curves and follows the quantum focusing conjecture in a manner transcending specific theoretical models. Finally, we argue that the negativity of the second derivative of the blacken factor \begin{document}$ f(r) $\end{document} ![]()
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near the event horizon strongly indicates negative heat capacity, which implies that black holes with a negative heat capacities must have islands and satisfy the quantum focusing conjecture.
Exploring the inverse problem tied to the Page curve phenomenon and island paradigm, we investigate the geometric conditions underpinning black hole evaporation where information is preserved and islands manifest, giving rise to the characteristic Page curve. Focusing on a broad class of static spherical symmetry black hole metrics in asymptotically Minkowski or (anti-)de Sitter spacetimes, we derive a pivotal constraint: the second derivative of blacken factor
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Abstract:
Background: The search of the heavier elements has yielded many surprises and enhanced our knowledge in the direction of nuclear synthesis and associated dynamical aspects. Although new elements and their associated isotopes have been synthesized, the amount of information with the Z ≥ 102, remains somewhat scarce. Further, in the domain of transfermium elements, the nuclear shell structure is of significant relevance for ensuring nuclear stability. Hence, the shell effects become indispensable for such nuclei. Purpose: Persistent experimental and theoretical endeavors have been conducted to examine the reactions induced by heavy ions and the subsequent decay mechanisms in the realm of superheavy mass. In addition, the region of transfermium elements is itself of great interest because of the neutron / proton shell effects. Here, Our objective is to analyze the subsequent decay mechanisms of nuclides of Z = 102 nucleus, i.e. 248No* and 250No*. Methods: An extensive study is conducted using the dynamical cluster-decay model (DCM) based on Quantum Mechanical Fragmentation Theory (QMFT). The focus is on investigating compound nucleus (CN) and non-compound nucleus (nCN) mechanisms, including fusion-fission (ff), Quasi fission (QF), and fast fission (FF). The specific isotopes of interest are 248No* and 250No*, with attention given to the role of centre of mass energy\begin{document}$ (E_{c.m.}) $\end{document} ![]()
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and angular momentum \begin{document}$ (\ell) $\end{document} ![]()
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. The nuclear interaction potential is derived using the Skyrme energy density formalism (SEDF) with the GSkI force parameters. The capture cross-sections are calculated using the \begin{document}$ \ell $\end{document} ![]()
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-summed Wong Model. The determination of the probability of compound nucleus formation (PCN) uses a function that is dependent upon the center of mass energy. The lifetimes of the fusion-fission (ff) quasi fission (QF) channels are also investigated. Results: Here, CN and nCN decay mechanisms for two isotopes of Z=102 nobelium are analysed over the range of centre-of-mass \begin{document}$ (E_{c.m.}) $\end{document} ![]()
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by taking into account the quadrupole deformation \begin{document}$ (\beta_2) $\end{document} ![]()
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and optimum orientations \begin{document}$ (\theta_{opt.}) $\end{document} ![]()
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of decaying fragments. The fragmentation potential, preformation probability, neck length parameter and reaction cross-sections are explored. Further, the calculations are done for PCN to determine the mechanisms of decay of 248No* and 250No* isotopes. The fusion-fission lifetimes and quasi fission lifetimes are compared with the dinuclear system (DNS) approach. Conclusions: Among the considered isotopes of Z = 102 i.e., 248No* formed in 40Ca + 208Pb reaction and 250No* via to different entrance channels 44Ca+206Pb and 64Ni+186W show asymmetric fragmentation with the effect of \begin{document}$ \beta_2 $\end{document} ![]()
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deformation at the energies beyond the Coulomb barrier. It has been noted, the nCN (QF,FF) decay mechanisms compete with CN fission channels. The calculations based on DCM show a strong correlation with the experimental data. The most probable fragments such as 122Sn and 128Te are observed near the magic shell closure Z = 50 and N = 82. As the excitation energy increases, the lifetime of fusion-fission and quasi fission decreases.
Background: The search of the heavier elements has yielded many surprises and enhanced our knowledge in the direction of nuclear synthesis and associated dynamical aspects. Although new elements and their associated isotopes have been synthesized, the amount of information with the Z ≥ 102, remains somewhat scarce. Further, in the domain of transfermium elements, the nuclear shell structure is of significant relevance for ensuring nuclear stability. Hence, the shell effects become indispensable for such nuclei. Purpose: Persistent experimental and theoretical endeavors have been conducted to examine the reactions induced by heavy ions and the subsequent decay mechanisms in the realm of superheavy mass. In addition, the region of transfermium elements is itself of great interest because of the neutron / proton shell effects. Here, Our objective is to analyze the subsequent decay mechanisms of nuclides of Z = 102 nucleus, i.e. 248No* and 250No*. Methods: An extensive study is conducted using the dynamical cluster-decay model (DCM) based on Quantum Mechanical Fragmentation Theory (QMFT). The focus is on investigating compound nucleus (CN) and non-compound nucleus (nCN) mechanisms, including fusion-fission (ff), Quasi fission (QF), and fast fission (FF). The specific isotopes of interest are 248No* and 250No*, with attention given to the role of centre of mass energy
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