- Particle physics theoretical and experimental studies
- High-Energy Particle Collisions Research
- Quantum Chromodynamics and Particle Interactions
- Particle Detector Development and Performance
- Radiation Detection and Scintillator Technologies
- Quantum, superfluid, helium dynamics
- Dark Matter and Cosmic Phenomena
- High-pressure geophysics and materials
- Superconducting Materials and Applications
- Nuclear physics research studies
- Neutrino Physics Research
- Atomic and Subatomic Physics Research
- Advanced Algorithms and Applications
- Geophysics and Gravity Measurements
- Medical Imaging Techniques and Applications
- Muon and positron interactions and applications
- Neural Networks and Applications
- Semiconductor materials and devices
- Photonic and Optical Devices
- Spectral Theory in Mathematical Physics
- Plasma Diagnostics and Applications
- Radioactive Decay and Measurement Techniques
- Atomic and Molecular Physics
- Magnetic Field Sensors Techniques
- Astrophysical Phenomena and Observations
Nanjing University of Posts and Telecommunications
2025
Institute of High Energy Physics
2019-2024
Bulgarian Academy of Sciences
2024
Institute of High Energy Physics
2023
Chinese Academy of Sciences
2022
Tokyo Institute of Technology
2010-2021
AviChina Industry & Technology (China)
2021
University of Chinese Academy of Sciences
2018-2020
In view of the High Luminosity upgrade CERN LHC, forward CMS Muon spectrometer will be extended with two new stations improved Resistive Plate Chambers (iRPC) covering pseudorapidity range from 1.8 to 2.4. Compared present RPC system, gap thickness is reduced lower avalanche charge, and an innovative 2D strip readout geometry proposed. These improvements allow iRPC detector cope higher background rates. A Front-End-Board (FEB) designed signals a threshold as low 30 fC integrated Time Digital...
Self-Organizing Map (SOM) neural networks can project complex, high-dimensional data onto a two-dimensional plane for visualization, enabling an intuitive understanding of the distribution and symmetric structures such data, thereby facilitating clustering anomaly detection complex data. However, this algorithm is sensitive to initial weight matrix suffers from insufficient feature extraction. To address these issues, paper proposes improved SOM based on virtual winning neurons...
We have performed an exclusive measurement of the K−+He3→Λpn reaction at incident kaon momentum 1GeV/c. In Λp invariant mass spectrum, a clear peak was observed below threshold K¯+N+N, as signal kaonic nuclear bound state, K¯NN. The binding energy, decay width, and S-wave Gaussian form factor this state were to be BK=42±3(stat.)−4+3(syst.)MeV, ΓK=100±7(stat.)−9+19(syst.)MeV, QK=383±11(stat.)−1+4(syst.)MeV/c, respectively. total production cross section K¯NN, determined by its mode,...
An experiment to search for the $K^-pp$ bound state was performed via in-flight $^3$He($K^-,n)$ reaction using 5.3 $\times$ $10^9$ kaons at 1 GeV/$c$ J-PARC hadron experimental facility. In semi-inclusive neutron missing-mass spectrum $\theta_{n}^{lab}=0^\circ$, no significant peak observed in region corresponding binding energy larger than 80 MeV, where a bump structure has been reported $\Lambda p$ final different reactions. Assuming be isotropically decaying into p$, mass-dependent upper...
Abstract The CMS detector, including its muon system, has been operating at the CERN LHC in increasingly challenging conditions for about 15 years. detector was designed to provide excellent triggering and track reconstruction muons produced proton–proton collisons an instantaneous luminosity ( $$\mathcal {L}$$ <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:mi>L</mml:mi> </mml:math> ) of $$1 \times 10^{34}$$ <mml:mrow> <mml:mn>1</mml:mn> <mml:mo>×</mml:mo> <mml:msup>...
During Phase-2 of the LHC, known as High Luminosity LHC (HL-LHC), accelerator will increase its instantaneous luminosity to 5 × 1034 cm−2 s−1, delivering an integrated 3000 fb−1 over 10 years operation starting from 2027. In view HL-LHC, CMS muon system be upgraded sustain efficient triggering and reconstruction performance. Resistive Plate Chambers (RPCs) serve dedicated detectors for due their excellent timing resolution, extend acceptance up pseudorapidity values |η|=2.4. Before Long...
Data on the production of η mesons light nuclei near threshold are surveyed.The photoproduction 3 He and elastic scattering from this nucleus modelled in a multiple scheme positions poles both here neighbouring studied an optical potential approach.The 7 Li is compared to that within cluster model.The decay η-mesic through pion or nucleon emission also considered.
We observed a distinct peak in the $\Lambda p$ invariant mass spectrum of $^{3}{\rm He}(K^-, \, \Lambda p)n$, well below threshold $m_K + 2 m_p$. By selecting relatively large momentum-transfer region $q = 350 \sim 650$ MeV/$c$, one can clearly separate from quasi-free process, $\overline{K}N \rightarrow \overline{K}N$ followed by non-resonant absorption two spectator-nucleons $\overline{K}NN N $. found that simplest fit to gives us Breit-Wigner pole position at $B_{\rm {\it Kpp}} 47 \pm 3...
The J-PARC E15 experiment aims to search for the lightest kaonic nuclear states, namely K - pp, using in-flight (K , n) reaction on 3 He . In this experiment, missing mass in and invariant of decay such as pp → Λp pπ p will be measured simultaneously. article, experimental feature present status are presented.
While the current Belle II data acquisition (DAQ) system has proven to be reliable in first collisions delivered since May 2018, an upgrade increase bandwidth of readout is foreseen deployed over next few years for higher target luminosity SuperKEKB running. Currently, front-end electronics (FEE) individual subdetectors are connected online event building via a unified optical link called Belle2Link, offering unidirectional as well bidirectional slow control access. The FEE received by...