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Three Generations of SM Gauge Symmetry from Non-SUSY Compactification on CP2 × S2
Jyoti Bhattacharyya
Posted: 18 April 2025
Science Mapping Nuclear Reaction Cross Section Calculations
Hasan Özdoğan,
Gençay Sevim,
Yiğit Ali Üncü
Posted: 17 April 2025
Energy Renormalization in a Berry Geometrical Phase: Low-Energy Perturbations of the Strong Interaction and the QCD MASS Gap
Mark Gibbons
Posted: 14 April 2025
Correlating the 0νββ-Decay Amplitudes of 136Xe with the Ordinary Muon Capture (OMC) Rates of 136Ba
Aagrah Agnihotri,
Vikas Kumar,
Jouni Suhonen
Posted: 21 March 2025
Beta Decay Properties of Waiting-Point N=50 and 82 Isotopes
Necla Çakmak,
Najm Abdullah Saleh
Posted: 17 March 2025
Machine Learning Approach to Shield Optimization at Muon Collider
Luca Castelli
Posted: 28 January 2025
Characterizing Nuclear Pasta with Alpha Shapes
Jorge Lopez,
Daniela Ramírez Chávez,
Dmitriy Morozov
Posted: 28 January 2025
Calculation of α Decay Half-Lives for Tl, Bi and at Isotopes
Myeong-Hwan Mun,
Kyoungsu Heo,
Myung-Ki Cheoun
Posted: 22 January 2025
Newly Patented Charged Particle Confinement Device for Fusion that is a Hybrid Method of Fusion Between Tokamak and Inertial Electrostatic Confinement (IEC) Reactors
Pierre Moss II
Posted: 09 January 2025
Chiral Symmetry in Dense Matter with Meson Condensation
Takumi Muto,
Toshiki Maruyama,
Toshitaka Tatsumi
Posted: 30 December 2024
Design and Simulation of Muon Detector using Wavelength-Shifting Fiber Readout for Border Security
Anzori Sh. Georgadze
Posted: 30 December 2024
Feasibility Study of a PET Detector with Wavelength-Shifting Fiber Readout
Anzori Sh. Georgadze
Posted: 30 December 2024
Portable Magnetic Field Mapping Measurement System based on Large-Scale Dipole Magnets in HIAF
Xiang Zhang,
Zi Di Wu,
Li an Jin,
Jing Yang,
Xian Jin Ou,
Dong Sheng Ni,
Yue Cheng,
Li Xia Zhao,
Tong Jin Tong,
Wei Gang Dong
The High-Intensity Heavy-Ion Accelerator Facility (HIAF) is a significant national science and technology infrastructure project, constructed by IMP, to provide primary and radioactive intense beams for nuclear and related research. Large aperture, high-precision, and warm-ion superconducting dipole magnets are extensively utilised to achieve high beam intensities. However, the traditional Hall point measurement platform faces limitations such as magnet volume, measurement environment, and the range of good field regions in the measurement of large dipole magnets, especially huge superconducting dipole magnets, leading to poor operability, low measurement efficiency, and significant errors in secondary positioning accuracy. This paper introduces a new magnetic field mapping measurement system, which introduces ultrasonic motors capable of operating under strong magnetic fields (<7T), and can realize portable, efficient and high-precision magnetic field measurement. After system debugging, the SRing dipole magnet prototype was measured. The system's accuracy and efficiency were verified through comparison with traditional Hall probe measurement systems. On this basis, magnetic field distribution and integral excitation curve measurements of all 11 HFRS warm-iron superconducting dipole magnets and 3 HFRS anti-irradiation dipole magnets were carried out and completed, achieving the testing objectives.
The High-Intensity Heavy-Ion Accelerator Facility (HIAF) is a significant national science and technology infrastructure project, constructed by IMP, to provide primary and radioactive intense beams for nuclear and related research. Large aperture, high-precision, and warm-ion superconducting dipole magnets are extensively utilised to achieve high beam intensities. However, the traditional Hall point measurement platform faces limitations such as magnet volume, measurement environment, and the range of good field regions in the measurement of large dipole magnets, especially huge superconducting dipole magnets, leading to poor operability, low measurement efficiency, and significant errors in secondary positioning accuracy. This paper introduces a new magnetic field mapping measurement system, which introduces ultrasonic motors capable of operating under strong magnetic fields (<7T), and can realize portable, efficient and high-precision magnetic field measurement. After system debugging, the SRing dipole magnet prototype was measured. The system's accuracy and efficiency were verified through comparison with traditional Hall probe measurement systems. On this basis, magnetic field distribution and integral excitation curve measurements of all 11 HFRS warm-iron superconducting dipole magnets and 3 HFRS anti-irradiation dipole magnets were carried out and completed, achieving the testing objectives.
Posted: 20 December 2024
Fractional Analytic QCD: The Recent Results
Anatoly Kotikov,
Ilnur Gabdrakhmanov,
Nikita Gramotkov,
Oleg Teryaev,
Daria Volkova,
Ivan Zemlyakov
In this work, we present an overview of fractional analytic QCD in the spacelike (Euclidean) and timelike regions, which significantly improves the coupling constant in perturbative QCD. The obtained results are applied to the description of the Higgs boson decay into a bottom-antibottom pair and the polarized Bjorken sum rule. For the latter, an additional modification is proposed to combine the fitting curve with the condition for photoproduction.We found good agreement between the experimental data obtained for the polarized Bjorken sum rule and the predictions of analytic QCD, as well as a strong difference between these data and the results obtained in the framework of perturbative QCD. To satisfy the limit of photoproduction and take into account GerasimovDrell-Hearn and Burkhardt-Cottingham sum rules, we develope new representation of the perturbative part of the polarized Bjorken sum rule. We present an overview of fractional analytic QCD and its application for Higgs-boson decay into a bottom-antibottom pair and the description of the polarized Bjorken sum rule. The results shown here have been recently obtained in Refs. [18,19,21,22]. This study is dedicated to the description of the polarized Bjorken sum rule, based on recently derived formulas within the analytic QCD approach. To accommodate the photoproduction limit and incorporate the Gerasimov-Drell-Hearn and Burkhardt-Cottingham sum rules, we develop a new representation for the twist-2 part of the Bjorken sum rule. The derived results were applied for processing of experimental data. We observed a good agreement between the experimental data and the predictions from analytic QCD. In contrast, there is a significant discrepancy between these data and the fitting curves within the standard perturbative approach.
In this work, we present an overview of fractional analytic QCD in the spacelike (Euclidean) and timelike regions, which significantly improves the coupling constant in perturbative QCD. The obtained results are applied to the description of the Higgs boson decay into a bottom-antibottom pair and the polarized Bjorken sum rule. For the latter, an additional modification is proposed to combine the fitting curve with the condition for photoproduction.We found good agreement between the experimental data obtained for the polarized Bjorken sum rule and the predictions of analytic QCD, as well as a strong difference between these data and the results obtained in the framework of perturbative QCD. To satisfy the limit of photoproduction and take into account GerasimovDrell-Hearn and Burkhardt-Cottingham sum rules, we develope new representation of the perturbative part of the polarized Bjorken sum rule. We present an overview of fractional analytic QCD and its application for Higgs-boson decay into a bottom-antibottom pair and the description of the polarized Bjorken sum rule. The results shown here have been recently obtained in Refs. [18,19,21,22]. This study is dedicated to the description of the polarized Bjorken sum rule, based on recently derived formulas within the analytic QCD approach. To accommodate the photoproduction limit and incorporate the Gerasimov-Drell-Hearn and Burkhardt-Cottingham sum rules, we develop a new representation for the twist-2 part of the Bjorken sum rule. The derived results were applied for processing of experimental data. We observed a good agreement between the experimental data and the predictions from analytic QCD. In contrast, there is a significant discrepancy between these data and the fitting curves within the standard perturbative approach.
Posted: 16 December 2024
Nuclear Evidences for Confirming the Physical Existence of 585 GeV Weak Fermion and Galactic Observations of TeV Radiation
Satya Seshavatharam U.V,
Gunavardhananaidu T,
Lakshminarayana S
Posted: 04 December 2024
Effective Models of QCD and Their Implications for Dark Matter Phenomenology
Swapnil Singh
Posted: 02 December 2024
Statistical Model of Nuclear Fission Using Hill-Wheeler Equation as Quantum Mechanical Distribution Function
Hirokazu Maruyama
Posted: 20 November 2024
On the Hypothesis of Exact Conservation of Charged Weak Hadronic Vector Current in the Standard Model
Derar Altarawneh,
Roman Höllwieser,
Markus Wellenzohn
Posted: 31 October 2024
Dynamics of Neutron Transfer in the Reaction 3He+9Be
Aidos K. Azhibekov,
Englik K. Almanbetova,
Mikhail A. Naumenko,
Kairat O. Mendibayev,
Sergey M. Lukyanov,
Talgat G. Issatayev,
Bakhytzhan A. Urazbekov,
Asset M. Kabyshev,
Kuralay Dyussebayeva,
Timur K. Zholdybayev
Posted: 30 October 2024
External Moderation of Reactor Core Neutrons for Optimized Production of Ultra-Cold Neutrons
Graham Medlin,
Ekaterina Korobkina,
Cole Gresham Teander,
Bernard Wehring,
Eduard Sharapov,
Ayman I. Hawari,
Paul Huffman,
Albert R. Young,
Grant Palmquist,
Matthew Morano
Posted: 14 October 2024
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