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Delaney","last_name":"Farrell","first_name":"Delaney","recid":1941514},"control_number":2852759,"dois":[{"source":"Frontiers","value":"10.3389/fphy.2024.1474615"}],"document_type":["article"],"texkeys":["Farrell:2024rfa"],"abstracts":[{"source":"Frontiers","value":"<sec><title>Introduction</title><p>This paper investigates the impact of differential rotation on the bulk properties and onset of rotational instabilities in neutron stars at finite temperatures up to 50 MeV.</p></sec><sec><title>Methods</title><p>Utilizing the relativistic Brueckner-Hartree-Fock (RBHF) formalism in full Dirac space, the study constructs equation of state (EOS) models for hot neutron star matter, including conditions relevant for high temperatures. These finite-temperature EOS models are applied to compute the bulk properties of differentially rotating neutron stars with varying structural deformations.</p></sec><sec><title>Results</title><p>The findings demonstrate that the stability of these stars against bar-mode deformation, a key rotational instability, is only weakly dependent on temperature. Differential rotation significantly affects the maximum mass and radius of neutron stars, and the threshold for the onset of bar-mode instability shows minimal sensitivity to temperature changes within the examined range.</p></sec><sec><title>Discussion</title><p>These findings are crucial for interpreting observational data from neutron star mergers and other high-energy astrophysical events. The research underscores the necessity of incorporating differential rotation and finite temperature effects in neutron star models to predict their properties and stability accurately.</p></sec>","abstract_source_suggest":{"input":"Frontiers"}}],"titles":[{"source":"Frontiers","title":"Differential rotation in neutron stars at finite temperatures"}],"imprints":[{"date":"2024-09-30"}],"curated":false}},{"id":"3010739","links":{"bibtex":"https://inspirehep.net/api/literature/3010739?format=bibtex","latex-eu":"https://inspirehep.net/api/literature/3010739?format=latex-eu","latex-us":"https://inspirehep.net/api/literature/3010739?format=latex-us","json":"https://inspirehep.net/api/literature/3010739?format=json","json-expanded":"https://inspirehep.net/api/literature/3010739?format=json-expanded","cv":"https://inspirehep.net/api/literature/3010739?format=cv","citations":"https://inspirehep.net/api/literature/?q=refersto%3Arecid%3A3010739"},"updated":"2025-10-02T17:19:01.218756+00:00","created":"2025-10-02T08:27:55.129836+00:00","metadata":{"publication_info":[{"pubinfo_freetext":"SCIENCE AND CULTURE (Indian Science News Association), vol. 79, pp. 485-500 (2013)","material":"publication"}],"authors":[{"raw_affiliations":[{"value":"Condensed Matter Physics Division Saha Institute of Nuclear Physics 1/AF Bidhannagar, Kolkata 700 064, India."}],"full_name_unicode_normalized":"ghosh, asim","full_name":"Ghosh, Asim","record":{"$ref":"https://inspirehep.net/api/authors/2140577"},"last_name":"Ghosh","affiliations":[{"record":{"$ref":"https://inspirehep.net/api/institutions/903178"},"value":"Saha Inst."}],"ids":[{"schema":"INSPIRE BAI","value":"A.Ghosh.44"}],"uuid":"d99c8670-37bb-4e58-b9e3-00bb71ff1cc3","first_name":"Asim","recid":2140577},{"raw_affiliations":[{"value":"Condensed Matter Physics Division Saha Institute of Nuclear Physics 1/AF Bidhannagar, Kolkata 700 064, India."}],"full_name_unicode_normalized":"mukherjee, sudip","full_name":"Mukherjee, Sudip","record":{"$ref":"https://inspirehep.net/api/authors/1955474"},"last_name":"Mukherjee","affiliations":[{"record":{"$ref":"https://inspirehep.net/api/institutions/903178"},"value":"Saha Inst."}],"ids":[{"schema":"INSPIRE BAI","value":"S.Mukherjee.23"}],"uuid":"afb5bde9-02ab-4561-8d6b-5e84eb6a69cc","first_name":"Sudip","recid":1955474}],"citation_count":4,"citation_count_without_self_citations":3,"citeable":true,"$schema":"https://inspirehep.net/schemas/records/hep.json","references":[{"reference":{"misc":["References (Partial):"]},"raw_refs":[{"schema":"text","source":"arXiv","value":"References (Partial):"}]},{"reference":{"label":"1","publication_info":{"journal_volume":"6","artid":"4220","year":1972,"page_start":"4220","journal_title":"Phys.Rev.B"},"authors":[{"full_name":"Cannella, V."},{"full_name":"Mydosh, J.A."}]},"raw_refs":[{"schema":"text","source":"arXiv","value":"[1] V. 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At low temperatures, and in cases where barriers to relaxation are tall and narrow, quantum mechanics can enhance the ability to traverse the free energy surface [2]. The LiHoxY1xF4 family of materials represents the simplest quantum spin model, the Ising magnet in a transverse field, and it has been an especially useful system to probe the interplay of disorder, glassiness, random magnetic fields, and quantum entanglement [3–10].” Figure 13: Title, abstract and some excerpts from a paper extending and clarifying the method used in ref. [8]"}]},{"reference":{"label":"10","publication_info":{"journal_volume":"81","artid":"5916","year":1998,"page_start":"5916","journal_title":"Phys.Rev.Lett."},"title":{"title":"Research on spin glasses [1] has not only led to deep insights into disordered materials and the glassy state but has generated novel approaches to problems ranging from computer architecture through protein folding to economics. 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[84] Das A and Chakrabarti B K 2005 Quantum Annealing and Related Optimization Methods ed A Das and B K Chakrabarti (Berlin: Springer) p 217 [85] Das A, Chakrabarti B and Stinchcombe R B 2005 Phys. Rev. E 72 026701"}]}],"referenced_authors_bais":["Amitabha.Chakrabarti.1","E.Tosatti.1","H.Nishimori.1","G.Santoro.1","Paul.S.Ray.1","T.Kadowaki.1","R.Car.2","S.Kirkpatrick.1","F.Rosenbaum.1","D.Bitko.1","D.Sherrington.1","B.Chakrabarti.1","R.Martonak.2","G.Aeppli.1","James.J.Brooke.1"],"figures":[{"filename":"bbc.png","material":"preprint","caption":"BBC news blog on the purchase deal of the latest 512 qubit quantum annealer of D-Wave Inc. by the NASA-Google consortium (website: http://www.bbc.co.uk/news/science-environment-22554494).","label":"bbc.pdf","source":"arxiv","key":"b32f1e1801b92455e0b63f9cba638793","url":"https://inspirehep.net/files/b32f1e1801b92455e0b63f9cba638793"},{"filename":"sci-ame.png","material":"preprint","caption":"A Scientific American news blog on the NASA-Google  investment in D-Wave quantum (annealing) computer. It explains briefly the working principle involved, using the Wikipedia entry on quantum annealing (Fig. \\ref{wiki.pdf}; website: http://blogs.scientificamerican.com/guest-blog/2013/05/17/is-it-quantum-computing-or-not/).","label":"sci-ame.pdf","source":"arxiv","key":"fdabb9149042b2569da762401495cded","url":"https://inspirehep.net/files/fdabb9149042b2569da762401495cded"},{"filename":"wiki.png","material":"preprint","caption":"Part of the entry on quantum annealing in Wikipedia (as in September 2013; website: http://en.wikipedia.org/wiki/Quantum-annealing ).","label":"wiki.pdf","source":"arxiv","key":"79f58d1f3068e392535e3cc099c06c0d","url":"https://inspirehep.net/files/79f58d1f3068e392535e3cc099c06c0d"},{"filename":"ray-89.png","material":"preprint","caption":"Title, abstract and some excerpts from the first published paper arguing that quantum tunneling across the free energy barriers in Sherrienton-Kirkpatrick spin glass model can lead to efficient search possibilities for its ground state(s). It may be noted that computationally hard problems can often be mapped into such long-range spin glass models and the advantage of quantum tunneling in such quantum spin glass models has lead  ultimately to the development of the quantum annealer/computer discussed here.","label":"ray-89.pdf","source":"arxiv","key":"5c0e429a06e51e60b3a195a883655eff","url":"https://inspirehep.net/files/5c0e429a06e51e60b3a195a883655eff"},{"filename":"thirumalai-89.png","material":"preprint","caption":"Title, abstract and some excerpts from \\cite{Thirumalai-89}, arguing (in almost the same language as in ref. \\cite{ray-89}; see Fig. \\ref{ray-89.pdf}) for the possible advantage of quantum tunneling between well characterised (classically) localized states in the same long-range transverse Ising spin glass model.","label":"thirumalai-89.pdf","source":"arxiv","key":"354869d531fdf11614947bed721982a8","url":"https://inspirehep.net/files/354869d531fdf11614947bed721982a8"},{"filename":"appolloni-89.png","material":"preprint","caption":"Title and  abstract of ref. \\cite{apolloni-89} indicating the formulation of a quantum stochastic optimization trick.","source":"arxiv","key":"c4254aa2cacc5781a0bf0c2e3f85e57f","url":"https://inspirehep.net/files/c4254aa2cacc5781a0bf0c2e3f85e57f"},{"filename":"wu-91.png","material":"preprint","caption":"Title, abstract and some excerpts from the first paper (from Univ. Chicago and Bell Labs. groups) reporting on the  experimental realization of a sample described precisely by a transverse Ising spin glass model, with tunable  transverse field, and observations  in agreement with the results  of Ray et al. (1989).","label":"wu-91.pdf","source":"arxiv","key":"fe27e7e43059b09be42c295fbb23ce1b","url":"https://inspirehep.net/files/fe27e7e43059b09be42c295fbb23ce1b"},{"filename":"finnila-94.png","material":"preprint","caption":"Title and  abstract of the first published paper demonstrating the ground state cluster search for a Lennard-Jones system  with `quantum annealing' [in the title; Of course, the first claim for `A numerical implementation of quantum annealing' in a single particle Hamiltonian for minimizing a real function of Boolean variables was published by B. Apolloni, C. Carvalho and D. De Falco in a conference (held in July 1988) proceedings, `Stochastic Processes, Physics \\& Geometry', Eds. S. Albeverio et al., World Scientific, Singapore, 1990, pp. 97-111].","label":"finnila-94.pdf","source":"arxiv","key":"48a96b9886ddf9f8e42da3a823c249de","url":"https://inspirehep.net/files/48a96b9886ddf9f8e42da3a823c249de"},{"filename":"nishimori-98.png","material":"preprint","caption":"Title and  abstract of a   quantum annealing paper demonstrating clear advantages of quantum annealing in well characterized computationally hard problems of Ising models with frustrating interactions. The demonstrations of clear advantages in some well studied spin models made major impact on the subsequent developments.","label":"nishimori-98.pdf","source":"arxiv","key":"a4b353cd44519fb1c10f6f1ef58cf29b","url":"https://inspirehep.net/files/a4b353cd44519fb1c10f6f1ef58cf29b"},{"filename":"aeppli-99.png","material":"preprint","caption":"Title and  abstract of the first experimental demonstration of the advantages of quantum annealing in extracting ground state of disordered magnets. This experimental demonstration had put the quantum annealing trick on firm physical ground.","label":"aeppli-99.pdf","source":"arxiv","key":"d772c04b4fbbba6e561324e5423cc5be","url":"https://inspirehep.net/files/d772c04b4fbbba6e561324e5423cc5be"},{"filename":"farhi-01.png","material":"preprint","caption":"Title and abstract of zero temperature quantum annealing algorithm for NP-hard problems.","label":"farhi-01.pdf","source":"arxiv","key":"cf1c6522b6bc264f2d842d712467ae7f","url":"https://inspirehep.net/files/cf1c6522b6bc264f2d842d712467ae7f"},{"filename":"santoro-02.png","material":"preprint","caption":"Title and abstract of a paper on application of quantum annealing in estimating the remaining fraction of undesired solutions in some optimization searches in Ising spin-glasses.","label":"santoro-02.pdf","source":"arxiv","key":"c600723cf9651ee161b0ea4e9b096c04","url":"https://inspirehep.net/files/c600723cf9651ee161b0ea4e9b096c04"},{"filename":"aeppli-PRL-2008.png","material":"preprint","caption":"Title, abstract and some excerpts from a paper extending and clarifying the method used in ref. \\cite{brooke-99} (see fig. \\ref{aeppli-99.pdf}) for quantum glasses.","label":"aeppli-PRL-2008.pdf","source":"arxiv","key":"c16c4bd7f6c2a2d46744267155348af6","url":"https://inspirehep.net/files/c16c4bd7f6c2a2d46744267155348af6"},{"filename":"Santoro-06.png","material":"preprint","caption":"Title, abstract and some excerpts for the first review on adiabatic quantum computation/annealing.","label":"Santoro-06.pdf","source":"arxiv","key":"27f936826dabc017e2e482fce119c7d6","url":"https://inspirehep.net/files/27f936826dabc017e2e482fce119c7d6"},{"filename":"das-rmp.png","material":"preprint","caption":"Title, abstract and some excerpts from a review on quantum annealing and quantum computation.","label":"das-rmp.pdf","source":"arxiv","key":"7238a910fcd7afff5667faaedd871a7e","url":"https://inspirehep.net/files/7238a910fcd7afff5667faaedd871a7e"},{"filename":"Morita-08.png","material":"preprint","caption":"Title, abstract and some excerpts  from a review on quantum annealing, discussing rigorous mathematical bounds for  errors and convergence times in different optimization cases.","label":"Morita-08.pdf","source":"arxiv","key":"1ff0e9a6ed4517b2b77d011a7516f43f","url":"https://inspirehep.net/files/1ff0e9a6ed4517b2b77d011a7516f43f"},{"filename":"D-wave.png","material":"preprint","caption":"From the Wikipedia entry on `D-Wave Systems Inc.' (as in September 2013;  website: http://en.wikipedia.org/wiki/D-Wave-Systems).","label":"D-wave.pdf","source":"arxiv","key":"a4ad1675794fb2f317daec68d6f22be4","url":"https://inspirehep.net/files/a4ad1675794fb2f317daec68d6f22be4"},{"filename":"Johnson-12.png","material":"preprint","caption":"Title and abstract of the first paper by D-Wave group giving the basic architecture of their quantum annealing precessor.","label":"Johnson-12.pdf","source":"arxiv","key":"e261364cf1227ea77b3fd737b387b141","url":"https://inspirehep.net/files/e261364cf1227ea77b3fd737b387b141"},{"filename":"ortiz-12.png","material":"preprint","caption":"Title, abstract and excerpts from the first major paper supporting the claim of D-Wave quantum computer used in searching the low energy conformations of lattice protein model, reported by the Harvard University group.","label":"ortiz-12.pdf","source":"arxiv","key":"9f8229c19e5abbbb1f198cac67a6100f","url":"https://inspirehep.net/files/9f8229c19e5abbbb1f198cac67a6100f"},{"filename":"arXiv.png","material":"preprint","caption":"Title, abstract and some excerpts of a  paper (from NASA Ames Research centre, Jet Propulsion Lab, CALTECH and University of Southern California) explaining  the basic principle of quantum annealing,  D-Wave computers and the possibilities of searching  solutions  of hard computational problems in space science and technology (website: http://arxiv.org/abs/1204.2821).","label":"arXiv.pdf","source":"arxiv","key":"25a654f019cb9a32dbe31156915369a5","url":"https://inspirehep.net/files/25a654f019cb9a32dbe31156915369a5"},{"filename":"yamamoto.png","material":"preprint","caption":"Title  and some excerpts of a   paper (from National Institute of Informatics, Tokyo and Stanford University, California) comparing different quantum algorithms (including quantum annealing) in hardware platforms.","label":"yamamoto.pdf","source":"arxiv","key":"b05115a937ae24356e5023af7630399b","url":"https://inspirehep.net/files/b05115a937ae24356e5023af7630399b"},{"filename":"Somma-12.png","material":"preprint","caption":"Title, abstract  and some excerpts of a paper discussing possible speed-ups in quantum annealing computers.","label":"Somma-12.pdf","source":"arxiv","key":"1306ebe316c78a8a2d12fdfbff4500ae","url":"https://inspirehep.net/files/1306ebe316c78a8a2d12fdfbff4500ae"},{"filename":"titiloye-12.png","material":"preprint","caption":"Title, abstract  and some excerpts from a paper discussing successes of  quantum  annealing algorithms for graph-coloring problems.","label":"titiloye-12.pdf","source":"arxiv","key":"2d0ae375e08290d20227ee6b0db6a4a3","url":"https://inspirehep.net/files/2d0ae375e08290d20227ee6b0db6a4a3"},{"filename":"boixo-12.png","material":"preprint","caption":"Title and abstract of a paper reporting on quantum signatures in D-Wave machines and on their `surprising robustness against noise and imperfections'.","label":"boixo-12.pdf","source":"arxiv","key":"54423295c2f8bb9c1910bba66a3f5cc9","url":"https://inspirehep.net/files/54423295c2f8bb9c1910bba66a3f5cc9"},{"filename":"bian-13.png","material":"preprint","caption":"Title and  abstract from ref. \\cite{Bian-13} claiming a precise success (though very limited in scope) in a problem of party size calculation (with conflicting choices  among the  party members), using the D-wave computer.","label":"bian-13.pdf","source":"arxiv","key":"fcc391564c4176d2a6932f8bbc435b81","url":"https://inspirehep.net/files/fcc391564c4176d2a6932f8bbc435b81"},{"filename":"bioxo-13.png","material":"preprint","caption":"Title, abstract and some excerpts from a paper by scientists from University of Southern California, University of  California, ETH Zurich and Microsoft Research, reporting on the precise quantum nature of the  performance of the D-Wave computer, compared with that of classical or  conventional  computers (website: http://arxiv.org/abs/1304.4595).","label":"bioxo-13.pdf","source":"arxiv","key":"5cb95416621b165a25ebb2ae4fc1e89d","url":"https://inspirehep.net/files/5cb95416621b165a25ebb2ae4fc1e89d"},{"filename":"bose-13.png","material":"preprint","caption":"A very recent news note by Bose \\cite{bose-13} conveying the excitement.","label":"bose-13.pdf","source":"arxiv","key":"1d5d8a960ed09b8b62e9a2f39bccaee1","url":"https://inspirehep.net/files/1d5d8a960ed09b8b62e9a2f39bccaee1"},{"filename":"nature.png","material":"preprint","caption":"Nature news blog regarding the recent reporting by scientists confirming the quantum nature of computation in D-Wave computers  (website: http://blogs.nature.com/news/2013/04/further-proof-for-controversial-quantum-computer.html).","label":"nature.pdf","source":"arxiv","key":"d0751c09adc97657b8a4034c19786fd4","url":"https://inspirehep.net/files/d0751c09adc97657b8a4034c19786fd4"}],"inspire_categories":[{"term":"Other","source":"arxiv"},{"term":"Quantum Physics","source":"arxiv"}],"preprint_date":"2013-11-29","author_count":2,"first_author":{"emails":["asim.ghosh@saha.ac.in"],"full_name":"Ghosh, Asim","last_name":"Ghosh","first_name":"Asim","recid":2140577},"public_notes":[{"source":"arXiv","value":"To be published in SCIENCE AND CULTURE (Indian Science News Association), 2013"}],"control_number":3010739,"earliest_date":"2013-11-29","document_type":["article"],"texkeys":["Ghosh:2013jac"],"abstracts":[{"source":"arXiv","value":"Major breakthrough in quantum computation has recently been achieved using quantum annealing to develop analog quantum computers instead of gate based computers. After a short introduction to quantum computation, we retrace very briefly the history of these developments and discuss the Indian researches in this connection and provide some interesting documents (in the Figs.) obtained from a chosen set of high impact papers (and also some recent news etc. blogs appearing in the Internet). This note is also designed to supplement an earlier note by Bose (Science and Culture, 79, pp. 337-378, 2013).","abstract_source_suggest":{"input":"arXiv"}}],"primary_arxiv_category":["physics.hist-ph"],"titles":[{"source":"arXiv","title":"Quantum Annealing and Computation: A Brief Documentary Note"}],"facet_author_name":["2140577_Abhik Ghosh","1955474_S. Mukherjee"],"core":true,"license":[{"license":"arXiv nonexclusive-distrib 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Design and test of wire-scanners for SwissFEL[ED/OL]. 2016-11-01. https://arxiv.org/abs/1611.00151.. , arXiv: https://scholar.google.com/scholar?1611.00151.&"}]},{"reference":{"dois":["10.18429/JACoW-IPAC2018-WEPAF047"],"label":"8","publication_info":{"year":2018},"misc":["and commissioning of the wire scanner system for the European XFEL.,: 1919 -1922"],"authors":[{"full_name":"T, Lensch"},{"full_name":"Status, Liu S."}]},"raw_refs":[{"schema":"text","value":"[8] Lensch T, Liu S. Status and commissioning of the wire scanner system for the European XFEL. 2018 ,: 1919 -1922 , DOI: 10.18429/JACoW-IPAC2018-WEPAF047"}],"record":{"$ref":"https://inspirehep.net/api/literature/1690536"}},{"reference":{"dois":["10.3390/app7050479"],"label":"9","misc":["Ko I S","Construction and commissioning of PAL-XFEL facility"],"authors":[{"full_name":"S, Kang H."},{"full_name":"H, Heo"}]},"raw_refs":[{"schema":"text","value":"[9] Ko I S, Kang H S, Heo H, et al. 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Design and measurement of signal processing system for cavity beam position monitor"],"authors":[{"full_name":"P, Wang B."},{"full_name":"B, Leng Y."}]},"raw_refs":[{"schema":"text","value":"[18] Wang B P, Leng Y B, Yu L Y, et al. Design and measurement of signal processing system for cavity beam position monitor. , DOI: 10.13538/j.1001-8042/nst.2013.02.007 , 2013 , 24(2) , DOI: 10.13538/j.1001-8042/nst.2013.02.007 , DOI: https://scholar.google.com/scholar? &q=Design and measurement of signal processing system for cavity beam position monitor& author=Wang B P&author=Leng Y B&author=Yu10.13538/j.1001-8042/nst.2013.02.007\">Nuclear Science and Techniques</a>& volume=24& issue=2&"}]},{"reference":{"dois":["10.11889/j.0253-3219.2021.hjs.44.040101"],"label":"19","publication_info":{"year":2021},"misc":["曹珊珊, 冷用斌","基于腔式探头的高分辨率束团电荷量测量方法研究[J]. 核技术,, 44(4): 040101"]},"raw_refs":[{"schema":"text","value":"[19] 曹珊珊, 冷用斌, 袁任贤, 等. 基于腔式探头的高分辨率束团电荷量测量方法研究[J]. 核技术, 2021, 44(4): 040101... , DOI: 10.11889/j.0253-3219.2021.hjs.44.040101"}]},{"reference":{"dois":["10.1016/j.nima.2021.165627"],"label":"20","misc":["Study of the optimal amplitude extraction algorithm for cavity BPM"],"authors":[{"full_name":"J, Chen"},{"full_name":"S, Cao S."},{"full_name":"B, Leng Y."}]},"raw_refs":[{"schema":"text","value":"[20] Chen J, Cao S S, Leng Y B, et al. 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CrossRef"}]}],"number_of_pages":8,"referenced_authors_bais":["Jia.Wen.Xia.1","R.C.Field.1","L.ZhaoKai.1","T.Lensch.2","Hai.Xing.Miao.1","Yong.Bin.Leng.1","R.Shafer.1","G.Penco.1","J.A.Kadyk.44","J.Ding.11","S.Liu.32","R.C.Jared.1","Jian.Ping.Chen.1","Guo.Yi.Zhu.1","P.Heimgartner.1","Y.Liu.29","H.Lv.4","H.M.Xie.1","U.Hahn.1","R.Fulton.11","L.Lai.1","D.Haixiao.1","J.J.Chen.1","W.Xu.31","R.Ischebeck.1","S.Trovati.1","Wei.Zhou.1","M.Ferianis.1","W.Kozanecki.1","John.S.Haggerty.1","Peng.Peng.Yu.1","Y.Yan.13","C.Yu.11","T.Wu.1","C.O.Loch.1","Hao.Hao.Wang.1","V.Schlott.1","J.Chen.88","G.J.Wan.1","P.Valitutti.1","G.Schmidt.1","H.Zhao.2","R.Jones.116","F.Ridoutt.1","Y.Zhou.42","Bo.Gao.2","W.Koska.1","Yong.Zhang.3","Y.M.Ye.1","M.Meschkat.1","F.Chen.4","X.J.Wu.1","G.L.Orlandi.1","S.Cao.16","G.Chen.6","Q.Mi.1"],"inspire_categories":[{"term":"Instrumentation","source":"curator"}],"author_count":8,"first_author":{"full_name":"WAN, Jun","last_name":"WAN","first_name":"Jun","recid":1949471},"control_number":3129967,"dois":[{"source":"CHINA SCIENCE PUBLISHING & MEDIA LTD","value":"10.11889/j.0253-3219.2022.hjs.45.050101"}],"earliest_date":"2022","document_type":["article"],"texkeys":["WAN:2022rky","WAN:2024lde"],"languages":["zh"],"abstracts":[{"source":"CHINA SCIENCE PUBLISHING & MEDIA LTD","value":"<sec><title>Background</title><p>The Shanghai high repetition rate XFEL and extreme light facility (SHINE) accelerates electrons up to 8 GeV using cryogenic-superconducting high-frequency cavity. Wire scanner system is applied to the beam profile measurement of SHINE due to its advantages such as fewer secondary particles generation compared with that of complete beam block, hence reduce the risk of superconducting cavity.</p></sec><sec><title>Purpose</title><p>This study aims to design data acquisition system for wire scanner system and realize synchronous acquisition of beam loss signal and relative position between the wire and beam.</p></sec><sec><title>Methods</title><p>The data acquisition system for wire scanner was designed to include radio frequency (RF) daughter board with analog signal digitizer, digital motherboard, firmware, data processing software. A Zynq-UltraScale+ based system on chip (SoC) was employed as system central component, and a field programmable gate array (FPGA) was used for system control and data transmission whilst the advanced RISC machine (ARM) integrating Linux was implemented for data acquisition and communication. Finally, experimental test of this data acquisition system was performed on the testbed to verify its feasibility and functionalities.</p></sec><sec><title>Results</title><p>The data acquisition system can correctly read back position of grating ruler, and achieve synchronous acquisition of sample beam loss signal and signal of cavity beam position monitor.</p></sec><sec><title>Conclusions</title><p>The data acquisition system meets the requirements of SHINE wire scanner system. It will be applied to the prototype of SHINE wire scanner system.</p></sec>","abstract_source_suggest":{"input":"CHINA SCIENCE PUBLISHING & MEDIA LTD"}}],"refereed":true,"titles":[{"source":"CHINA SCIENCE PUBLISHING & MEDIA LTD","title":"Development of data acquisition system for prototype of SHINE wire scanner system"}],"facet_author_name":["2129791_J.F. Chen","2715667_Shanshan Cao","1949471_Guang-Jun Wan","2726059_Bo Gao","1978078_Fangzhou Chen","1962552_Longwei Lai","2161504_Guang-Jie Chen","1486078_Yong-Bin Leng"],"core":false,"imprints":[{"date":"2024-10-25"}],"_oai":{"sets":["Literature"],"id":"oai:inspirehep.net:3129967","updated":"2026-04-15T08:51:29.862754"},"curated":true,"journal_title_variants":["Nucl. 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Coupled-bunch instabilities in storage rings and feedback systems. , DOI: 10.1007/978-3-319-14394-1_20, DOI: 10.1007/978-3-319-14394-1_20, DOI: 10.1007/978-3-319-14394-1_20 , 2016 ,: 605 -628 , DOI: 10.1007/978-3-319-14394-1_20 , DOI: https://scholar.google.com/scholar? &q=Coupled-bunch instabilities in storage rings and feedback systems& author=Teytelman10.1007/978-3-319-14394-1_20\">Cham</a>& pages=605 -628"}]},{"reference":{"label":"10","publication_info":{"journal_volume":"54","page_end":"308","year":2011,"page_start":"305","journal_title":"Sci.China Phys.Mech.Astron."},"misc":["bunch-by-bunch transverse feedback system at SSRF[J]. Science China Physics Mechanic &","Suppl 2): 305-308"],"authors":[{"full_name":"Digital, Yuan R.X."}]},"raw_refs":[{"schema":"text","value":"[10] Yuan R X. Digital bunch-by-bunch transverse feedback system at SSRF[J]. Science China Physics Mechanic & Astronomy, 2011, 54(Suppl 2): 305-308.."}],"record":{"$ref":"https://inspirehep.net/api/literature/1206090"}},{"reference":{"label":"11","publication_info":{"year":2003},"misc":["and algorithms for control and diagnostics of coupled-bunch instabilities in circular accelerators[D]. Stanford University PhD thesis",": 47-54"],"authors":[{"full_name":"Architectures, Teytelman D."}],"report_numbers":["SLAC-R-633"]},"raw_refs":[{"schema":"text","value":"[11] Teytelman D. Architectures and algorithms for control and diagnostics of coupled-bunch instabilities in circular accelerators[D]. Stanford University PhD thesis, SLAC-R-633, 2003: 47-54.."}],"record":{"$ref":"https://inspirehep.net/api/literature/625822"}},{"reference":{"label":"12","publication_info":{"year":2009},"misc":["Measurements of coupled-bunch instabilities in BEPCII[C]. Proceeding of PAC09"],"authors":[{"full_name":"D, Teytelman"},{"full_name":"J, Cao"},{"full_name":"J, Yue"}]},"raw_refs":[{"schema":"text","value":"[12] Teytelman D, Cao J, Yue J, et al. Measurements of coupled-bunch instabilities in BEPCII[C]. Proceeding of PAC09, 2009.."}]},{"reference":{"label":"13","publication_info":{"year":2017},"misc":["Feedback commissioning and diagnostics in BEPCII e+ ring[R]. December"],"authors":[{"full_name":"D, Teytelman"},{"full_name":"J, Cao"},{"full_name":"J, Yue"}]},"raw_refs":[{"schema":"text","value":"[13] Teytelman D, Cao J, Yue J, et al. Feedback commissioning and diagnostics in BEPCII e+ ring[R]. December 2017.."}]},{"reference":{"label":"14","publication_info":{"journal_volume":"32","page_end":"104","year":2008,"page_start":"102","journal_title":"Chin.Phys.C"},"misc":["曹建社, 马力","Libera BPM 在 BEPCII","调束中的应用[J]. 中国物理 C","32(增 1): 102-104"]},"raw_refs":[{"schema":"text","value":"[14] 曹建社, 马力, 麻惠州, 等. Libera BPM 在 BEPCII 调束中的应用[J]. 中国物理 C, 2008, 32(增 1): 102-104.."}]},{"reference":{"label":"15","publication_info":{"year":2013},"misc":["张闯, 马力. 北京正负电子对撞机重大改造工程加速器的设计与研制[M]. 上海: 上海科学技术出版社"]},"raw_refs":[{"schema":"text","value":"[15] 张闯, 马力. 北京正负电子对撞机重大改造工程加速器的设计与研制[M]. 上海: 上海科学技术出版社, 2013.."}]}],"number_of_pages":6,"referenced_authors_bais":["Ren.Xian.Yuan.1","D.Teytelman.1","Dou.Wang.1","Yong.Bin.Leng.1","K.Ye.2","M.Tobiyama.1","D.Gong.6","Luyang.Yu.1","Ji.Yuan.Zhai.1","E.Kikutani.1","L.Han.9","Jie.Gao.1"],"inspire_categories":[{"term":"Accelerators","source":"curator"}],"author_count":8,"first_author":{"full_name":"LAN, Qinghong","last_name":"LAN","first_name":"Qinghong","recid":2829193},"control_number":3142353,"dois":[{"source":"CHINA SCIENCE PUBLISHING & MEDIA LTD","value":"10.11889/j.0253-3219.2019.hjs.42.030401"}],"earliest_date":"2019","document_type":["article"],"texkeys":["LAN:2019nyk","LAN:2024sbm"],"languages":["zh"],"abstracts":[{"source":"CHINA SCIENCE PUBLISHING & MEDIA LTD","value":"<sec><title>Background</title><p>Digital bunch-by-bunch feedback control is the best way to control bunch instability. It will be applied to the super collider to suppress the beam oscillation within a dozen or even several cycles. The damping time of circular electron positron collider (CEPC) and FCC-ee ( Future Circle Collider e<sup>-</sup>e<sup>+</sup> ) is very short, but it is impossible to realize through using traditional digital feedback system.</p></sec><sec><title>Purpose</title><p>This study aims to cure the coupled-bunch instability by using a dual-feedback control system to reduce the damping time for BEPCII (Beijing Electron Positron Collider II).</p></sec><sec><title>Methods</title><p>Several feedback systems operate simultaneously and act on the same time beam in storage ring can superimpose the damping effect and then reduce the damping time of the system. With the favorable condition of two stripline kicker located on the outer ring, we make a experimental research about double feedback system in BEPCII synchrotron mode. Among the double feedback system, one system is the self-make digital bunch-by-bunch transverse feedback system based commercial card, the other system is the commercial feedback system produced by the Dimtel company.</p></sec><sec><title>Results</title><p>The damping time of commercial feedback system is measured as 0.93 ms, the damping time of self-make digital bunch-by-bunch transverse feedback system based commercial card is measured as 2.98 ms, and the damping time of double feedback system is measured as 0.70 ms.</p></sec><sec><title>Conclusions</title><p>Several feedback systems work simultaneously can effectively reduce the damping time turn by turn.</p></sec>","abstract_source_suggest":{"input":"CHINA SCIENCE PUBLISHING & MEDIA LTD"}}],"refereed":true,"titles":[{"source":"CHINA SCIENCE PUBLISHING & MEDIA LTD","title":"Research of the double feedback system operating in BEPCII"}],"facet_author_name":["1978140_Yanfeng Sui","2022315_Jun-Kang He","1077154_Junhui Yue","1273018_Jianshe Cao","1273279_Jingxia Zhao","1284105_Dayu Yin","1483013_Huizhou Ma","2829193_J.Q. Lan"],"core":true,"imprints":[{"date":"2024-10-25"}],"_oai":{"sets":["Literature"],"id":"oai:inspirehep.net:3142353","updated":"2026-04-14T08:21:37.388803"},"curated":true,"journal_title_variants":["Nucl.Tech.","Nucl. 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DOI: 10.7498/aps. 71.20211561."}]},{"reference":{"dois":["10.7538/yzk. 2019.youxian.0322"],"publication_info":{"journal_volume":"54","page_end":"1124","year":2020,"page_start":"1118","journal_title":"Atomic Energ.Sci.Technol."},"label":"11","authors":[{"full_name":"Fengqi"}],"misc":["YIN Qian, GUO Gang, ZHANG","Experimental research on single-event effect in SRAMs with different feature sizes[J]","2019.youxian.0322"]},"raw_refs":[{"schema":"text","value":"11 YIN Qian, GUO Gang, ZHANG Fengqi, et al. Experimental research on single-event effect in SRAMs with different feature sizes[J]. Atomic Energy Science and Technology, 2020, 54(6): 1118–1124. DOI: 10.7538/yzk. 2019.youxian.0322."}]},{"reference":{"dois":["10.12126/see.2020.03.014"],"label":"12","publication_info":{"year":2020},"authors":[{"full_name":"Yancun"}],"misc":["ZHANG Qingxiang, YU Dengyun, LI","Single event sensitivity evaluation by using mediumenergy proton accelerated by CYCIAE-100 cyclotron[J]. Spacecraft Environment Engineering,, 37(3): 293- 298"]},"raw_refs":[{"schema":"text","value":"12 ZHANG Qingxiang, YU Dengyun, LI Yancun, et al. Single event sensitivity evaluation by using mediumenergy proton accelerated by CYCIAE-100 cyclotron[J]. Spacecraft Environment Engineering, 2020, 37(3): 293– 298. DOI: 10.12126/see.2020.03.014."}]},{"reference":{"publication_info":{"journal_volume":"10","page_end":"612","year":2012,"page_start":"608","journal_title":"Electron.Eng."},"label":"13","authors":[{"full_name":"Ding"}],"misc":["SHI Shuting, GUO Gang, WANG","Technique of single event upset mapping[J]. Information and"]},"raw_refs":[{"schema":"text","value":"13 SHI Shuting, GUO Gang, WANG Ding, et al. Technique of single event upset mapping[J]. Information and Electronic Engineering, 2012, 10(5): 608–612."}]},{"reference":{"dois":["10.3390/ electronics11203413"],"publication_info":{"journal_volume":"11","artid":"3413","year":2022,"page_start":"3413","journal_title":"Electronics"},"label":"14","authors":[{"full_name":"H, Sun H."},{"full_name":"G, Guo"},{"full_name":"N, Sun R."}],"misc":["Study on single event upsets in a 28 nm technology static random access memory device based on micro-beam irradiation[J]","DOI: 10.3390/ electronics11203413"]},"raw_refs":[{"schema":"text","value":"14 Sun H H, Guo G, Sun R N, et al. Study on single event upsets in a 28 nm technology static random access memory device based on micro-beam irradiation[J]. Electronics, 2022, 11(20): 3413. DOI: 10.3390/ electronics11203413"}]}],"keywords":[{"source":"author","value":"Space radiation"},{"source":"author","value":"Single event effects"},{"source":"author","value":"Simulation test"}],"number_of_pages":6,"inspire_categories":[{"term":"Instrumentation","source":"curator"}],"author_count":10,"first_author":{"full_name":"CHEN, Qiming","last_name":"CHEN","first_name":"Qiming","recid":1939727},"control_number":3127159,"dois":[{"source":"CHINA SCIENCE PUBLISHING & MEDIA LTD","value":"10.11889/j.0253-3219.2023.hjs.46.080008"}],"earliest_date":"2023","document_type":["article"],"texkeys":["CHEN:2023luy","CHEN:2024meg"],"languages":["zh"],"abstracts":[{"source":"CHINA SCIENCE PUBLISHING & MEDIA LTD","value":"<sec><title>Background</title><p>The space environment contains numerous high-energy particles, and a single high-energy particle passing through a spacecraft shell bombards the electronic devices within, triggering single-particle effects such as device logic state upset and function failures, which, in turn, affect spacecraft operation reliability and mission accomplishment.</p></sec><sec><title>Purpose</title><p>Notably, ground accelerator irradiation tests provide an important and effective means for simulating space single event effects and for predicting the risks of single event effect rates for electronic devices in space applications. Generally, electronic devices can be used in spacecraft only if their resistance radiation indicators meet astronautical application requirements.</p></sec><sec><title>Methods</title><p>Spacecraft are typically exposed to space radiation particles, primarily heavy ions and protons; therefore, single event effect simulation testing for electronic devices relies predominantly on heavy ion and proton accelerators. To address the requirements of single event effect testing, technologies such as large-area beam expansion and homogenization, high-precision beam current diagnosis, and efficient test terminals have been developed to fulfill the requirements of various test tasks.</p></sec><sec><title>Results</title><p>Particular focus is placed on the CIAE's (China Institute of Atomic Energy) heavy ion single event and proton single event effect simulation test techniques and the heavy ion microbeam technique for radiation sensitive area identification for electronic devices. Subsequently, the aforementioned techniques are applied to a single event effect risk evaluation for astronautical electronic devices.</p></sec><sec><title>Conclusions</title><p>In the future, the demand for radiation-resistant devices is expected to continue to increase in the aerospace, nuclear industry, and other radiation application fields. It is, therefore, necessary to further exploit the irradiation potential of existing domestic single event effect simulation equipment and establish new accelerator platforms with improved capacity for single event effect simulation testing.</p></sec>","abstract_source_suggest":{"input":"CHINA SCIENCE PUBLISHING & MEDIA LTD"}}],"refereed":true,"titles":[{"source":"CHINA SCIENCE PUBLISHING & MEDIA LTD","title":"Accelerator simulation test technology and its application for single event effect evaluation in space"}],"facet_author_name":["1877454_J.Z. Zhang","1939727_Qianqian Chen","1978527_Jie Liu","2723791_Gang Guo","1929379_Q.Q. 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WIMP dark matter candidates and searches-current status and future prospects. , DOI: 10.1088/1361-6633/aab913 , 2018 , 81(6) , DOI: 10.1088/1361-6633/aab913 , DOI: https://scholar.google.com/scholar? &q=WIMP dark matter candidates and searches-current status and future prospects& author=Roszkowski L&author=Sessolo E M&author=Trojanowski10.1088/1361-6633/aab913\">Reports on Progress in Physics Physical Society (Great Britain)</a>& volume=81& issue=6&"}],"record":{"$ref":"https://inspirehep.net/api/literature/1610814"}},{"reference":{"dois":["10.1038/nphys4039"],"label":"3","misc":["status of direct dark matter detection experiments"],"authors":[{"full_name":"L, Liu J."},{"full_name":"X, Chen"}]},"raw_refs":[{"schema":"text","value":"[3] Liu J L, Chen X, Ji X D. 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Low background stainless steel for the pressure vessel in the PandaX-II dark matter experiment. , DOI: 10.1088/1748-0221/11/09/t09004 , 2016 , 11(9) , DOI: 10.1088/1748-0221/11/09/t09004 , DOI: https://scholar.google.com/scholar? &q=Low background stainless steel for the pressure vessel in the PandaX-II dark matter experiment& author=Zhang T&author=Fu C&author=Ji10.1088/1748-0221/11/09/t09004\">Journal of Instrumentation</a>& volume=11& issue=9&"}],"record":{"$ref":"https://inspirehep.net/api/literature/1488102"}},{"reference":{"dois":["10.1146/annurev-nucl-102115-044842"],"label":"5","misc":["Li J M, et al. The China Jinping underground laboratory and its early science"],"authors":[{"full_name":"P, Cheng J."},{"full_name":"J, Kang K."}]},"raw_refs":[{"schema":"text","value":"[5] Cheng J P, Kang K J, Li J M, et al. 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.J.Murphy.1","Murdock.G.D.Gilchriese.1","X.Ren.1","S.Catalanotti.1","Andrzej.M.Szelc.1","B.Baibussinov.1","Frank.L.H.Wolfs.1","K.T.Knopfle.1","V.S.Gallo.1","Zhi.Deng.1","L.Ounalli.2","M.Vanderbroucke.1"],"inspire_categories":[{"term":"Experiment-Nucl","source":"curator"}],"author_count":9,"first_author":{"affiliations_identifiers":[{"schema":"ROR","value":"https://ror.org/0220qvk04"}],"full_name":"ZHANG, Tao","last_name":"ZHANG","first_name":"Tao","recid":1419200},"control_number":3127150,"dois":[{"source":"CHINA SCIENCE PUBLISHING & MEDIA LTD","value":"10.11889/j.0253-3219.2022.hjs.45.110201"}],"earliest_date":"2022","document_type":["article"],"texkeys":["ZHANG:2022qmd","ZHANG:2024vzx"],"languages":["zh"],"abstracts":[{"source":"CHINA SCIENCE PUBLISHING & MEDIA LTD","value":"<sec><title>Background</title><p>The expected signal rate of rare decay experiments, such as instance dark matter and neutrino less double beta decay experiments, is extremely low, which requires that the detector building materials have extremely low radioactivity. Low radioactive background control is one of the essential works in the rare decay experiments. <sup>226</sup>Ra and <sup>228</sup>Ra produced in the early decay chain of <sup>238</sup>U and <sup>232</sup>Th have low boiling point and high vapor pressure, removing the element Ra can break the <sup>238</sup>U decay chain and keep a low radioactivity of <sup>232</sup>Th-late for a long time.</p></sec><sec><title>Purpose</title><p>This study aims to investigate vacuum melting technique for low background titanium to reduce the impurity of isotopes that have negative impact on rare decay experiments and creating a low background environment for the detector running.</p></sec><sec><title>Methods</title><p>Firstly, the low background material samples were acquired by manual separation of radionuclides using physical and chemical methods. Then, radioactive impurity elements, such as K, Cs, Ra, Pb, Po and Rn with low boiling point and high vapor pressure, were volatilized in environment with high temperature and high vacuum level. Finally, radioactivity of these testing samples were measured by two sets of high-purity germanium γ spectrometer with measurement time extended to 7 days.</p></sec><sec><title>Results</title><p>Measurement results show signs of removal of radioactive isotopes by smelting-vacuum method, and the impurity in pure titanium smelted in vacuum electron beam furnace can reach the levels of (0.13±0.69) mBq∙kg<sup>-1</sup> for <sup>232</sup>Th-<sup>228</sup>Ac, and (0.07±0.29) mBq∙kg<sup>-1</sup> for <sup>238</sup>U-<sup>222</sup>Rn, respectively.</p></sec><sec><title>Conclusions</title><p>The smelting-vacuum method could provide reliable low background material for the container of the next generation PandaX detector.</p></sec>","abstract_source_suggest":{"input":"CHINA SCIENCE PUBLISHING & MEDIA LTD"}}],"refereed":true,"titles":[{"source":"CHINA SCIENCE PUBLISHING & MEDIA LTD","title":"Investigation of vacuum melting technique for low background titanium"}],"facet_author_name":["2141548_Han-Yang Liu","1882979_Yukun Yao","1924504_B. Li","2044104_Y.T. Pei","1066360_Siguang Wang","1311908_Jianglai Liu","1329734_Yue Meng","1405838_Ke Han","1419200_Tao Zhang"],"core":false,"imprints":[{"date":"2024-10-25"}],"_oai":{"sets":["Literature"],"id":"oai:inspirehep.net:3127150","updated":"2026-04-16T05:40:39.656291"},"curated":true,"journal_title_variants":["Nucl.Tech.","Nucl. 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In a specific energy range, the cross section of neutron reaction varies drastically with the neutron energy, and resonance occurs. The resonance spectrum of nuclides is unique, and qualitative and quantitative analysis of nuclides can be carried out based on this. Among them, the resonance energy range of medium-heavy nuclei is in the eV~keV energy range, which is an important part of neutron resonance analysis.</p></sec><sec><title>Purpose</title><p>Due to the lack of conclusive articles on neutron resonance in medium-heavy nuclei, this paper summarizes the current research on neutron resonance.</p></sec><sec><title>Methods</title><p>By querying a large number of journal papers and books related to neutron resonance, the theory and application of neutron resonance of medium and heavy nuclear are summarized.</p></sec><sec><title>Results &amp; Conclusions</title><p>At present, there have been many research results, and they have been widely used in temperature measurement, imaging, non-destructive analysis, nuclear data measurement, and other aspects. In this regard, by reviewing the literature and books on neutron resonance, the research status of neutron resonance at domestic and overseas are summarized and analyzed, and its development tendency is forecast.</p></sec>","abstract_source_suggest":{"input":"CHINA SCIENCE PUBLISHING & MEDIA LTD"}}],"refereed":true,"titles":[{"source":"CHINA SCIENCE PUBLISHING & MEDIA LTD","title":"Research and application of neutron resonance in medium-heavy nuclei"}],"facet_author_name":["2141999_M.X. Tuo","1887251_J.R. Niu","1923061_Rongsheng Shi","1991467_Qing Wang","2025631_Frank Liu","2205925_L.C. Deng","3129968_Keliang MU"],"core":false,"imprints":[{"date":"2024-10-25"}],"_oai":{"sets":["Literature"],"id":"oai:inspirehep.net:3129966","updated":"2026-04-15T09:10:04.019520"},"curated":true,"journal_title_variants":["Nucl. 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It is designed as a cylindrical barrel divided into 32 sectors with a total of 43 008 towers. Each tower is composed of 220 layers of lead and 221 layers of scintillator alternately.</p></sec><sec><title>Purpose</title><p>This study aims to simulate multiple parameters of Shashlik ECAL for NICA-MPD that affect the performance of ECAL.</p></sec><sec><title>Methods</title><p>First of all, the module of ECAL tower was built based on the principle of Shashlik ECAL. Then, the GEENT4 software was employed to simulate the performance of every single tower of ECAL according to its structure composition. Considering the influence of the design parameters of the scintillator and absorber on energy deposition, energy resolution, and energy leakage after electrons were incident on the tower and the subsequent scintillator luminescence process, the influence of the reflective layer on the number of photons was in the wavelength shifted fiber and detector. Finally, factors that affected energy deposition, energy leakage, energy resolution, and photon number in the wavelength shift (WLS) and sensor, and the influence of the thickness, number of layers, and size of the scintillator and absorber in the module on energy deposition, energy leakage, and energy resolution were simulated and analyzed.</p></sec><sec><title>Results</title><p>The simulation results show that the best side length of cross-section of each tower is 4 cm. When the total thickness of absorber and scintillator is 1.8 mm and the thickness of lead absorber is 0.3 mm, the energy resolution meets the experimental requirements of 5%@3 GeV. When the radiation length reaches 13<italic>X</italic><sub>0</sub>, maximum energy deposition and obtains better energy resolution can be achieved. Adding a reflective layer to the tower side can increase the number of photons in the fiber by 10%~19% whereas adding a reflective coating to the fiber end can effectively increase the number of photons reaching the detector by 50%.</p></sec><sec><title>Conclusions</title><p>The photon numbers in the wavelength shift fiber and the detector are affected by the reflection layer on both the tower side and the end face of the fiber. The importance and necessity of adding reflector are verified by this study.</p></sec>","abstract_source_suggest":{"input":"CHINA SCIENCE PUBLISHING & MEDIA LTD"}}],"refereed":true,"titles":[{"source":"CHINA SCIENCE PUBLISHING & MEDIA LTD","title":"Performance simulation of a Shashlik sampling electromagnetic calorimeter for NICA-MPD"}],"facet_author_name":["2131185_X. Ji","1879431_De-Xian Wei","1894893_H.D. Zeng","1986615_Chundong Hu","1952877_K. Zhu","1944541_G. Qu","1958004_XUE. Peng","1471023_Kai-yu Cheng","2430946_Xiaodong Wang"],"core":true,"imprints":[{"date":"2024-10-25"}],"_oai":{"sets":["Literature"],"id":"oai:inspirehep.net:3132209","updated":"2026-04-10T08:19:15.046666"},"curated":true,"journal_title_variants":["Nucl. 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It is one of the scientific infrastructures with the highest altitude in China and its core goal is to explore high-energy cosmic ray. As an important component of LHAASO, the ground shower particle array (KM2A) has a huge total area of one square kilometer. Unlike most high-energy physics experiments, the KM2A has a total of about 6 500 channels, and a total input bandwidth of about 546 MB∙s-1. There is no hardware trigger function in KM2A.</p></sec><sec><title>Purpose</title><p>This study aims to design and implement a software for KM2A to complete the trigger and real-time data processing.</p></sec><sec><title>Methods</title><p>Data transmission scheme based on standard Ethernet and TCP / IP protocol was employed to receive all packet data including all detector units at the same time. Online processing and calculation of data packets were achieved by using the configured trigger algorithm. Data with physical significance were extracted and packaged to form different events with physical labels, then these events were sent to different receivers according to the configured output rules. By using distributed technology and task division, this software was able to finish real-time data processing through selectable algorithm scheduling.</p></sec><sec><title>Results &amp; Conclusions</title><p>The software is able to trigger KM2A in real time, reduce the amount of data, and lessen the burden of transmission and storage. It has been put into use in the data center of 4 410 m altitude experiment site, and has been running well so far.</p></sec>","abstract_source_suggest":{"input":"CHINA SCIENCE PUBLISHING & MEDIA LTD"}}],"titles":[{"source":"CHINA SCIENCE PUBLISHING & MEDIA LTD","title":"Online real-time distributed data process of LHAASO ground shower particle array"}],"imprints":[{"date":"2024-10-25"}],"curated":true}},{"id":"1610865","links":{"bibtex":"https://inspirehep.net/api/literature/1610865?format=bibtex","latex-eu":"https://inspirehep.net/api/literature/1610865?format=latex-eu","latex-us":"https://inspirehep.net/api/literature/1610865?format=latex-us","json":"https://inspirehep.net/api/literature/1610865?format=json","json-expanded":"https://inspirehep.net/api/literature/1610865?format=json-expanded","cv":"https://inspirehep.net/api/literature/1610865?format=cv","citations":"https://inspirehep.net/api/literature/?q=refersto%3Arecid%3A1610865"},"updated":"2023-03-07T02:03:44.418134+00:00","created":"2017-07-21T00:00:00+00:00","metadata":{"publication_info":[{"journal_volume":"99","pubinfo_freetext":"Phys. 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Total photon energy distributions and their ratios for photons with energy $>$ 1 GeV for {\\KK}MC-hh with the cuts specified in the text for the EW-CORR labels and notational and illustrative conventions as given in the caption for Fig.~\\ref{fig-1}.The ratio plot features ``CEEX2'' as the reference distribution as noted in the respective title.","source":"arxiv","key":"c195c51208fee08b8e577d8460f6288d","url":"https://inspirehep.net/files/c195c51208fee08b8e577d8460f6288d"},{"filename":"muon-pt-ratio-3-16-17.png","caption":"\\baselineskip=11pt Muon transverse momentum distributions and their ratios for {\\KK}MC-hh with the cuts specified in the text for the EW-CORR labels ``CEEX2\" (red -- medium dark shade), ``CEEX2 (no IFI)\" (violet -- light dark shade), ``EEX1'' (blue -- dark shade), and ``EEX1 (no IFI)'' (green -- light shade), showered by HERWIG 6.5. The labels are explained in the text. The ratio plot features ``CEEX2'' as the reference distribution as noted in the respective title.","source":"arxiv","key":"4d617c38e97177e71610fadfc6cb5a1f","url":"https://inspirehep.net/files/4d617c38e97177e71610fadfc6cb5a1f"},{"filename":"muon-eta-3-16-17.png","caption":"\\baselineskip=11pt Muon $\\eta$ distributions and their ratios for {\\KK}MC-hh with the cuts specified in the text for the EW-CORR labels and notational and illustrative conventions as given in the caption for Fig.~\\ref{fig-1}. 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The labels are explained in the text. The ratio plot features ``CEEX2'' as the reference distribution as noted in the respective title.","source":"arxiv","key":"a5d6ea9164fdbdbcacd4aa8482b4e66e","url":"https://inspirehep.net/files/a5d6ea9164fdbdbcacd4aa8482b4e66e"},{"filename":"muon-eta-6-18-18.png","caption":"\\baselineskip=11pt Muon $\\eta$ distributions and their ratios for {\\KK}MC-hh with the cuts specified in the text for the EW-CORR labels and notational and illustrative conventions as given in the caption for Fig.~\\ref{fig-1}. The events were showered by HERWIG 6.5.The ratio plot features ``CEEX2'' as the reference distribution as noted in the respective title.","source":"arxiv","key":"66d7de90ec84e98930cde1ead8f31183","url":"https://inspirehep.net/files/66d7de90ec84e98930cde1ead8f31183"},{"filename":"dimuon-mass-6-18-18.png","caption":"\\baselineskip=11pt Dimuon invariant mass distributions and their ratios for {\\KK}MC-hh with the cuts specified in the text for the EW-CORR labels and notational and illustrative conventions as given in the caption for Fig.~\\ref{fig-1}. The events were showered by HERWIG 6.5.The ratio plot features ``CEEX2'' as the reference distribution as noted in the respective title.","source":"arxiv","key":"f4f44d9ba92dd546939dfbf3144564b0","url":"https://inspirehep.net/files/f4f44d9ba92dd546939dfbf3144564b0"},{"filename":"photon-total-energy-ratio-3-16-17.png","caption":"\\baselineskip=11pt Total photon energy distributions and their ratios for photons with energy $&gt;$ 1 GeV for {\\KK}MC-hh with the cuts specified in the text for the EW-CORR labels and notational and illustrative conventions as given in the caption for Fig.~\\ref{fig-1}.The ratio plot features ``CEEX2'' as the reference distribution as noted in the respective title.","source":"arxiv","key":"231b797cb24a06dc5cae13bf8950e195","url":"https://inspirehep.net/files/231b797cb24a06dc5cae13bf8950e195"},{"filename":"photon-energy-ratio-6-18-18.png","caption":"\\baselineskip=11pt Total photon energy distributions and their ratios for photons with energy $>$ 1 GeV for {\\KK}MC-hh with the cuts specified in the text for the EW-CORR labels and notational and illustrative conventions as given in the caption for Fig.~\\ref{fig-1}.The ratio plot features ``CEEX2'' as the reference distribution as noted in the respective title.","source":"arxiv","key":"4db949783bdc6e89206d6bb407cc80cb","url":"https://inspirehep.net/files/4db949783bdc6e89206d6bb407cc80cb"},{"filename":"dimu-mss-pt4-24-18eta2p4.png","caption":"\\baselineskip=8pt Dimuon mass and transverse momentum distributions and their respective ratios, using the PDG quark masses as explained in the text, for {\\KK}MC-hh with the cuts specified in the text for the EW-CORR labels and notational and illustrative conventions as given in the caption for Fig.~\\ref{fig-1}.The ratio plot features ``CEEX2'' as the reference distribution as noted in the respective title.","source":"arxiv","key":"74f4497db8020d3c8bd434dc69f7163d","url":"https://inspirehep.net/files/74f4497db8020d3c8bd434dc69f7163d"},{"filename":"photon-pt-ratio-6-18-18.png","caption":"\\baselineskip=11pt Total photon transverse momentum distributions and their ratios for photons with energy $>$ 1 GeV for {\\KK}MC-hh with the cuts specified in the text for the EW-CORR labels and notational and illustrative conventions as given in the caption for Fig.~\\ref{fig-1}.The ratio plot features ``CEEX2'' as the reference distribution as noted in the respective title.","source":"arxiv","key":"3cf6d6afc44864979a42234c24e02f8c","url":"https://inspirehep.net/files/3cf6d6afc44864979a42234c24e02f8c"},{"filename":"photon-pt-6-18-18.png","caption":"\\baselineskip=11pt Total photon transverse momentum distributions and their ratios for photons with energy $>$ 1 GeV for {\\KK}MC-hh with the cuts specified in the text for the EW-CORR labels and notational and illustrative conventions as given in the caption for Fig.~\\ref{fig-1}.The ratio plot features ``CEEX2'' as the reference distribution as noted in the respective title.","source":"arxiv","key":"a0e280276cc3939f4d8f4f6aa2b8f1fb","url":"https://inspirehep.net/files/a0e280276cc3939f4d8f4f6aa2b8f1fb"},{"filename":"totphtn-rpdty4-24-18-eta2p4.png","caption":"\\baselineskip=8pt Photon total momentum rapidity distributions and their respective ratios, using the PDG quark masses as explained in the text, for photons with energy $>$ 1 GeV for {\\KK}MC-hh with the cuts specified in the text for the EW-CORR labels and notational and illustrative conventions as given in the caption for Fig.~\\ref{fig-1}. The ratio plot features ``CEEX2'' as the reference distribution as noted in the respective title.","source":"arxiv","key":"ed03ee87054524c26339be6a6f06a4f2","url":"https://inspirehep.net/files/ed03ee87054524c26339be6a6f06a4f2"},{"filename":"dimuon-rapidity-6-18-18.png","caption":"\\baselineskip=11pt Dimuon rapidity distributions and their ratios for {\\KK}MC-hh with the cuts specified in the text for the EW-CORR labels and notational and illustrative conventions as given in the caption for Fig.~\\ref{fig-1}.The ratio plot features ``CEEX2'' as the reference distribution as noted in the respective title.","source":"arxiv","key":"8c76a5c3b39fc8da2cb42d23c9c0d1aa","url":"https://inspirehep.net/files/8c76a5c3b39fc8da2cb42d23c9c0d1aa"},{"filename":"dimuon-mass-ratio-6-18-18.png","caption":"\\baselineskip=11pt Dimuon invariant mass distributions and their ratios for {\\KK}MC-hh with the cuts specified in the text for the EW-CORR labels and notational and illustrative conventions as given in the caption for Fig.~\\ref{fig-1}. The events were showered by HERWIG 6.5.The ratio plot features ``CEEX2'' as the reference distribution as noted in the respective title.","source":"arxiv","key":"540904885dc232178c335e725076d74b","url":"https://inspirehep.net/files/540904885dc232178c335e725076d74b"},{"filename":"muon-eta-ratio-6-18-18.png","caption":"\\baselineskip=11pt Muon $\\eta$ distributions and their ratios for {\\KK}MC-hh with the cuts specified in the text for the EW-CORR labels and notational and illustrative conventions as given in the caption for Fig.~\\ref{fig-1}. The events were showered by HERWIG 6.5.The ratio plot features ``CEEX2'' as the reference distribution as noted in the respective title.","source":"arxiv","key":"7818c55621bb10f7eadb5226f9977f42","url":"https://inspirehep.net/files/7818c55621bb10f7eadb5226f9977f42"},{"filename":"muon-pt-ratio-6-18-18.png","caption":"\\baselineskip=11pt Muon transverse momentum distributions and their ratios for {\\KK}MC-hh with the cuts specified in the text for the EW-CORR (electroweak-correction) labels ``CEEX2\" (red -- medium dark shade), ``CEEX2 (no IFI)\" (violet -- light dark shade), ``EEX1'' (blue -- dark shade), and ``EEX1 (no IFI)'' (green -- light shade), showered by HERWIG 6.5. The labels are explained in the text. The ratio plot features ``CEEX2'' as the reference distribution as noted in the respective title.","source":"arxiv","key":"775fe7cfcddf5982922122fec2560303","url":"https://inspirehep.net/files/775fe7cfcddf5982922122fec2560303"}],"legacy_version":"20190517005046.0","inspire_categories":[{"term":"Phenomenology-HEP"}],"first_author":{"affiliations_identifiers":[{"schema":"ROR","value":"https://ror.org/01n78t774"}],"full_name":"Jadach, S.","last_name":"Jadach","first_name":"S.","recid":1004601},"control_number":1610865,"dois":[{"source":"bibmatch","value":"10.1103/PhysRevD.99.076016"},{"material":"publication","source":"arXiv","value":"10.1103/PhysRevD.99.076016"}],"document_type":["article"],"texkeys":["Jadach:2017sqv"],"abstracts":[{"source":"APS","value":"With an eye toward the precision physics of the LHC, such as the recent measurement of MW by the ATLAS Collaboration, we present here systematic studies relevant to the assessment of the expected size of multiple photon radiative effects in heavy gauge boson production with decay to charged lepton pairs. We use the new version 4.22 of KKMC-hh so that we have coherent exclusive exponentiation (CEEX) electroweak (EW) exact O(α2L) corrections in a hadronic monte carlo and control over the corresponding EW initial-final interference (IFI) effects as well. In this way, we illustrate the interplay between cuts of the type used in the measurement of MW at the LHC and the sizes of the expected responses of the attendant higher order corrections. We find that there are per cent to per mille level effects in the initial-state radiation, fractional per mille level effects in the IFI and per mille level effects in the overall O(α2L) corrections that any treatment of EW corrections at the per mille level should consider. Our results have direct applicability to current LHC experimental data analyses.","abstract_source_suggest":{"input":"APS"}},{"source":"arXiv","value":"With an eye toward the precision physics of the LHC, such as the recent measurement of $M_W$ by the ATLAS Collaboration, we present here systematic studies relevant to the assessment of the expected size of multiple photon radiative effects in heavy gauge boson production with decay to charged lepton pairs. We use the new version 4.22 of ${\\cal KK}$MC-hh so that we have CEEX EW exact ${\\cal O}(\\alpha^2 L)$ corrections in a hadronic MC and control over the corresponding EW initial-final interference (IFI) effects as well. In this way, we illustrate the interplay between cuts of the type used in the measurement of $M_W$ at the LHC and the sizes of the expected responses of the attendant higher order corrections. We find that there are per cent to per mille level effects in the initial-state radiation, fractional per mille level effects in the IFI and per mille level effects in the over-all ${\\cal O}(\\alpha^2 L)$ corrections that any treatment of EW corrections at the per mille level should consider. Our results have direct applicability to current LHC experimental data analyses.","abstract_source_suggest":{"input":"arXiv"}}],"primary_arxiv_category":["hep-ph"],"titles":[{"source":"APS","title":"Systematic Studies of Exact ${\\cal O}(\\alpha^2L)$ CEEX EW Corrections in a Hadronic MC for Precision $Z/\\gamma^*$ Physics at LHC Energies"},{"source":"arXiv","title":"Systematic Studies of Exact ${\\cal O}(\\alpha^2L)$ CEEX EW Corrections in a Hadronic MC for Precision $Z/\\gamma^*$ Physics at LHC Energies"}],"imprints":[{"date":"2019-05-01"}],"curated":true}}],"total":7731},"links":{"self":"https://inspirehep.net/api/literature/?q=title&size=10&page=1","next":"https://inspirehep.net/api/literature/?q=title&size=10&page=2","bibtex":"https://inspirehep.net/api/literature/?q=title&size=10&page=1&format=bibtex","latex-eu":"https://inspirehep.net/api/literature/?q=title&size=10&page=1&format=latex-eu","latex-us":"https://inspirehep.net/api/literature/?q=title&size=10&page=1&format=latex-us","json":"https://inspirehep.net/api/literature/?q=title&size=10&page=1&format=json","json-expanded":"https://inspirehep.net/api/literature/?q=title&size=10&page=1&format=json-expanded","cv":"https://inspirehep.net/api/literature/?q=title&size=10&page=1&format=cv"}}