Di Sun
Current Organizations / Institutes
The organizations/institutes from the scholar's latest article
Di Sun has a total of 48 co-authors. Here are the top co-authors by number of shared publications:
- Jing-Yu Tang
University of Science and Technology of China
4 shared publications - Jun-Heng Hu
Sino-French Institute of Nuclear Engineering and Technology, Sun Yat-Sen University, Zhuhai, CHINA
4 shared publications - Ting Liu
Sino-French Institute of Nuclear Engineering and Technology, Sun Yat-Sen University, Zhuhai, CHINA
4 shared publications - Zhen-Dong An
Institute of Modern Physics
4 shared publications - Chen-Chen Guo
Sino-French Institute of Nuclear Engineering and Technology, Sun Yat-Sen University, Zhuhai, CHINA
3 shared publications - Hao Liang
Sino-French Institute of Nuclear Engineering and Technology, Sun Yat-Sen University, Zhuhai, CHINA
3 shared publications
Latest Publications
- 29 July 2026
- Published by Springer Nature in Nuclear Science and Techniques
- Vol. 37 (10) , 211
Neutron capture cross-section of indium from 1 eV to 1 MeV at the CSNS Back-n
- 29 July 2026
- Published by Springer Nature in Nuclear Science and Techniques
- Vol. 37 (10) , 211
Neutron capture cross-section of indium from 1 eV to 1 MeV at the CSNS Back-n
- Open Access
- 26 June 2026
- Published by American Astronomical Society in The Astrophysical Journal Supplement Series
- Vol. 285 (1) , 13
Direct Determination of Neutron Capture Relevant to the s -process of 127 I and 133 Cs at the CSNS Back-n Facility
The cross sections of 127 I( n , γ ) 128 I and 133 Cs( n , γ ) 134 Cs play a critical role in the s -process of nuclear astrophysics, the iodine–xenon chronometer on early meteorite evolution, and understanding the performance of CsI crystal detectors for Dark Matter Detection Experiment and Coherent Elastic Neutrino-Nucleus Scattering (CE ν NS) experiments. The neutron capture cross sections of 127 I and 133 Cs were measured from 1 eV to 1 MeV using the time-of-flight method at China Spallation Neutron Source Back-n facility. The neutron capture yield was derived via the pulse-height weighting technique based on the total energy detection principle of C 6 D 6 detectors. In the resolved resonance region (RRR), some new resonance peaks of 133 Cs( n , γ ) were observed for the first time. Resonance parameters for the neutron capture cross section were extracted using the SAMMY code from 1 eV to 4 keV, while averaged capture cross sections in the unresolved resonance region (URR) from 4 keV to 1 MeV were analyzed with TALYS. Results were compared with evaluated libraries and previous work in both RRR and URR. Astrophysical Maxwellian-averaged cross sections (MACS) were calculated for kT = 5–100 keV. At kT = 30 keV, the MACS of both 127 I( n , γ ) 128 I and 133 Cs( n , γ ) 134 Cs were slightly higher than those of the KADoNiS v0.3 recommended value. And the reaction rates were derived over the astrophysically relevant temperature range of s -process nucleosynthesis models. The uncertainties of present reaction rates are significantly reduced.
- 26 June 2026
- Published by American Astronomical Society in The Astrophysical Journal Supplement Series
- Vol. 285 (1) , 13
Open AccessDirect Determination of Neutron Capture Relevant to the s -process of 127 I and 133 Cs at the CSNS Back-n Facility
The cross sections of 127 I( n , γ ) 128 I and 133 Cs( n , γ ) 134 Cs play a critical role in the s -process of nuclear astrophysics, the iodine–xenon chronometer on early meteorite evolution, and understanding the performance of CsI crystal detectors for Dark Matter Detection Experiment and Coherent Elastic Neutrino-Nucleus Scattering (CE ν NS) experiments. The neutron capture cross sections of 127 I and 133 Cs were measured from 1 eV to 1 MeV using the time-of-flight method at China Spallation Neutron Source Back-n facility. The neutron capture yield was derived via the pulse-height weighting technique based on the total energy detection principle of C 6 D 6 detectors. In the resolved resonance region (RRR), some new resonance peaks of 133 Cs( n , γ ) were observed for the first time. Resonance parameters for the neutron capture cross section were extracted using the SAMMY code from 1 eV to 4 keV, while averaged capture cross sections in the unresolved resonance region (URR) from 4 keV to 1 MeV were analyzed with TALYS. Results were compared with evaluated libraries and previous work in both RRR and URR. Astrophysical Maxwellian-averaged cross sections (MACS) were calculated for kT = 5–100 keV. At kT = 30 keV, the MACS of both 127 I( n , γ ) 128 I and 133 Cs( n , γ ) 134 Cs were slightly higher than those of the KADoNiS v0.3 recommended value. And the reaction rates were derived over the astrophysically relevant temperature range of s -process nucleosynthesis models. The uncertainties of present reaction rates are significantly reduced.
- Open Access
- 30 December 2025
- Published by American Physical Society (APS) in Physical Review Research
- Vol. 7 (4)
Measurement of the Ag ( n , γ ) cross section up to stellar s-process temperatures at the CSNS Back-n
The ( n , γ ) cross section of silver is crucial for the nucleosynthesis process of nuclear astrophysics, the design of silver-indium-cadmium absorber rod in the nuclear reactors, and neutron resonance capture analysis for determining the elemental and isotopic composition of cultural heritage. The high-precision Ag ( n , γ ) cross section was measured from 1 eV to 1 MeV at the Back-n facility of the Chinese Spallation Neutron Source using the time-of-flight method and pulse height weighting technique. The resonance parameters were accurately extracted in the resolved resonance region by the multilevel multichannel R -matrix code . The code was used to describe the average cross sections in the unresolved resonance region, and the Maxwellian-averaged cross sections (MACSs) of Ag 107 and Ag 109 were further given in the 5–100 keV range. The MACS values at k T = 30 keV for Ag 107 ( 887 ± 89 mb ) and Ag 109 ( 903 ± 90 mb ) are slightly higher than the recommended values in the Karlsruhe Astrophysical Database of Stellar Nucleosynthesis.
- 30 December 2025
- Published by American Physical Society (APS) in Physical Review Research
- Vol. 7 (4)
Open AccessMeasurement of the Ag ( n , γ ) cross section up to stellar s-process temperatures at the CSNS Back-n
The ( n , γ ) cross section of silver is crucial for the nucleosynthesis process of nuclear astrophysics, the design of silver-indium-cadmium absorber rod in the nuclear reactors, and neutron resonance capture analysis for determining the elemental and isotopic composition of cultural heritage. The high-precision Ag ( n , γ ) cross section was measured from 1 eV to 1 MeV at the Back-n facility of the Chinese Spallation Neutron Source using the time-of-flight method and pulse height weighting technique. The resonance parameters were accurately extracted in the resolved resonance region by the multilevel multichannel R -matrix code . The code was used to describe the average cross sections in the unresolved resonance region, and the Maxwellian-averaged cross sections (MACSs) of Ag 107 and Ag 109 were further given in the 5–100 keV range. The MACS values at k T = 30 keV for Ag 107 ( 887 ± 89 mb ) and Ag 109 ( 903 ± 90 mb ) are slightly higher than the recommended values in the Karlsruhe Astrophysical Database of Stellar Nucleosynthesis.
- Open Access
- 12 December 2025
- Published by Elsevier in Physics Letters B
- Vol. 872
Direct measurement of the 103Rh(n,γ) and 103Rh(γ,n) cross section up to stellar temperatures at the CSNS Back-n and SSRF SLEGS
- 12 December 2025
- Published by Elsevier in Physics Letters B
- Vol. 872
Open AccessDirect measurement of the 103Rh(n,γ) and 103Rh(γ,n) cross section up to stellar temperatures at the CSNS Back-n and SSRF SLEGS