{"@context":{"@vocab":"https://cir.nii.ac.jp/schema/1.0/","rdfs":"http://www.w3.org/2000/01/rdf-schema#","dc":"http://purl.org/dc/elements/1.1/","dcterms":"http://purl.org/dc/terms/","foaf":"http://xmlns.com/foaf/0.1/","prism":"http://prismstandard.org/namespaces/basic/2.0/","cinii":"http://ci.nii.ac.jp/ns/1.0/","datacite":"https://schema.datacite.org/meta/kernel-4/","ndl":"http://ndl.go.jp/dcndl/terms/","jpcoar":"https://github.com/JPCOAR/schema/blob/master/2.0/"},"@id":"https://cir.nii.ac.jp/crid/1360580232136308864.json","@type":"Article","productIdentifier":[{"identifier":{"@type":"DOI","@value":"10.1007/jhep12(2022)145"}},{"identifier":{"@type":"URI","@value":"https://link.springer.com/content/pdf/10.1007/JHEP12(2022)145.pdf"}},{"identifier":{"@type":"URI","@value":"https://link.springer.com/article/10.1007/JHEP12(2022)145/fulltext.html"}},{"identifier":{"@type":"DOI","@value":"10.48550/arxiv.2206.13523"}}],"resourceType":"学術雑誌論文(journal article)","dc:title":[{"@value":"First evaluation of meson and τ lepton spectra and search for heavy neutral leptons at ILC beam dump"}],"description":[{"type":"abstract","notation":[{"@value":"<jats:title>A<jats:sc>bstract</jats:sc>\n                     </jats:title><jats:p>A beam dump experiment can be seamlessly added to the proposed Inter- national Linear Collider (ILC) program because the high energy electron beam should be dumped after the collision point. The ILC beam dump experiment will provide an excellent opportunity to search for new long-lived particles. Since many of them can be produced by a rare decay of standard model particles, we evaluate spectra of the mesons and <jats:italic>τ</jats:italic> lepton at the decay based on the PHITS and PYTHIA8 simulations. As a motivated physics case, we study the projected sensitivity of heavy neutral leptons at the ILC beam dump experiment. The heavy neutral leptons can also be produced via deep inelastic scattering and <jats:italic>Z</jats:italic> boson decay at the ILC main detector, which we include in the projection. With the multi-track signal, the reach would be greatly extended in mass and coupling, even compared with the other proposed searches.</jats:p>"}]}],"creator":[{"@id":"https://cir.nii.ac.jp/crid/1380580232136308877","@type":"Researcher","foaf:name":[{"@value":"Mihoko M. Nojiri"}]},{"@id":"https://cir.nii.ac.jp/crid/1380580232136308608","@type":"Researcher","foaf:name":[{"@value":"Yasuhito Sakaki"}]},{"@id":"https://cir.nii.ac.jp/crid/1380580232136308873","@type":"Researcher","foaf:name":[{"@value":"Kohsaku Tobioka"}]},{"@id":"https://cir.nii.ac.jp/crid/1380580232136308867","@type":"Researcher","foaf:name":[{"@value":"Daiki Ueda"}]}],"publication":{"publicationIdentifier":[{"@type":"EISSN","@value":"10298479"}],"prism:publicationName":[{"@value":"Journal of High Energy Physics"}],"dc:publisher":[{"@value":"Springer Science and Business Media LLC"}],"prism:publicationDate":"2022-12-27","prism:volume":"2022","prism:number":"12","prism:startingPage":"145"},"reviewed":"false","dc:rights":["https://creativecommons.org/licenses/by/4.0","https://creativecommons.org/licenses/by/4.0"],"url":[{"@id":"https://link.springer.com/content/pdf/10.1007/JHEP12(2022)145.pdf"},{"@id":"https://link.springer.com/article/10.1007/JHEP12(2022)145/fulltext.html"}],"createdAt":"2022-12-29","modifiedAt":"2023-03-25","foaf:topic":[{"@id":"https://cir.nii.ac.jp/all?q=New%20Light%20Particles","dc:title":"New Light Particles"},{"@id":"https://cir.nii.ac.jp/all?q=FOS:%20Physical%20sciences","dc:title":"FOS: Physical sciences"},{"@id":"https://cir.nii.ac.jp/all?q=QC770-798","dc:title":"QC770-798"},{"@id":"https://cir.nii.ac.jp/all?q=High%20Energy%20Physics%20-%20Experiment","dc:title":"High Energy Physics - Experiment"},{"@id":"https://cir.nii.ac.jp/all?q=High%20Energy%20Physics%20-%20Phenomenology","dc:title":"High Energy Physics - Phenomenology"},{"@id":"https://cir.nii.ac.jp/all?q=High%20Energy%20Physics%20-%20Experiment%20(hep-ex)","dc:title":"High Energy Physics - Experiment (hep-ex)"},{"@id":"https://cir.nii.ac.jp/all?q=High%20Energy%20Physics%20-%20Phenomenology%20(hep-ph)","dc:title":"High Energy Physics - Phenomenology (hep-ph)"},{"@id":"https://cir.nii.ac.jp/all?q=Neutrino%20Interactions","dc:title":"Neutrino Interactions"},{"@id":"https://cir.nii.ac.jp/all?q=Nuclear%20and%20particle%20physics.%20Atomic%20energy.%20Radioactivity","dc:title":"Nuclear and particle physics. Atomic energy. Radioactivity"},{"@id":"https://cir.nii.ac.jp/all?q=Specific%20BSM%20Phenomenology","dc:title":"Specific BSM Phenomenology"}],"project":[{"@id":"https://cir.nii.ac.jp/crid/1040018351901133312","@type":"Project","projectIdentifier":[{"@type":"KAKEN","@value":"23K20847"},{"@type":"JGN","@value":"JP23K20847"},{"@type":"URI","@value":"https://kaken.nii.ac.jp/grant/KAKENHI-PROJECT-23K20847/"}],"notation":[{"@language":"ja","@value":"軽い新粒子で切り込むクォークとレプトンの世代構造"},{"@language":"en","@value":"Explore quark and lepton flavor structure via light new particles"}]},{"@id":"https://cir.nii.ac.jp/crid/1040282256879604352","@type":"Project","projectIdentifier":[{"@type":"KAKEN","@value":"16H06492"},{"@type":"JGN","@value":"JP16H06492"},{"@type":"URI","@value":"https://kaken.nii.ac.jp/grant/KAKENHI-PLANNED-16H06492/"}],"notation":[{"@language":"ja","@value":"電弱対称性の破れと世代構造の統一的真空像"},{"@language":"en","@value":"Unified picture of electroweak symmetry breaking and family structure"}]},{"@id":"https://cir.nii.ac.jp/crid/1040574036135615872","@type":"Project","projectIdentifier":[{"@type":"KAKEN","@value":"22H05113"},{"@type":"JGN","@value":"JP22H05113"},{"@type":"URI","@value":"https://kaken.nii.ac.jp/grant/KAKENHI-PLANNED-22H05113/"}],"notation":[{"@language":"ja","@value":"機械学習による素粒子物理学の革新的な発展"},{"@language":"en","@value":"Innovative advances in particle physics through machine learning"}]},{"@id":"https://cir.nii.ac.jp/crid/1040852814763274752","@type":"Project","projectIdentifier":[{"@type":"KAKEN","@value":"21H05466"},{"@type":"JGN","@value":"JP21H05466"},{"@type":"URI","@value":"https://kaken.nii.ac.jp/grant/KAKENHI-PUBLICLY-21H05466/"}],"notation":[{"@language":"ja","@value":"電子陽電子ビームを用いた固定標的実験によるダークマター探索"},{"@language":"en","@value":"Searching for dark matter at fixed target experiments using electron positron beams"}]}],"relatedProduct":[{"@id":"https://cir.nii.ac.jp/crid/1360002217433126784","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"A facility to search for hidden particles at the CERN SPS: the SHiP physics case"}]},{"@id":"https://cir.nii.ac.jp/crid/1360013168759250432","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Leptophilic gauge bosons at ILC beam dump experiment"}]},{"@id":"https://cir.nii.ac.jp/crid/1360013172545612416","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Searching for new light particles at the international linear collider main beam dump"}]},{"@id":"https://cir.nii.ac.jp/crid/1360017279824598016","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Search for lepton flavor violating decay at FASER"}]},{"@id":"https://cir.nii.ac.jp/crid/1360017286451684864","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Charged-current deep-inelastic scattering of muon neutrinos (\n<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\"><mml:msub><mml:mi>ν</mml:mi><mml:mi>μ</mml:mi></mml:msub></mml:math>\n) off \n<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\"><mml:mmultiscripts><mml:mi>Fe</mml:mi><mml:mprescripts/><mml:none/><mml:mn>56</mml:mn></mml:mmultiscripts></mml:math>"}]},{"@id":"https://cir.nii.ac.jp/crid/1360017287022499328","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"High-Energy Electroproduction and the Constitution of the Electric Current"}]},{"@id":"https://cir.nii.ac.jp/crid/1360017287073668480","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Sensitivity reach on heavy neutral leptons and \n<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mi>τ</mml:mi></mml:math>\n-neutrino mixing \n<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mo stretchy=\"false\">|</mml:mo><mml:msub><mml:mi>U</mml:mi><mml:mrow><mml:mi>τ</mml:mi><mml:mi>N</mml:mi></mml:mrow></mml:msub><mml:msup><mml:mo stretchy=\"false\">|</mml:mo><mml:mn>2</mml:mn></mml:msup></mml:math>\n at the HL-LHC"}]},{"@id":"https://cir.nii.ac.jp/crid/1360017288934304256","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Sterile neutrino production at small mixing in the early universe"}]},{"@id":"https://cir.nii.ac.jp/crid/1360017288934984320","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Constraints on heavy-lepton mixings from deep-inelastic charged-lepton scattering"}]},{"@id":"https://cir.nii.ac.jp/crid/1360017288935006208","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Measurement of Shadowing in Photon-Nucleus Total Cross Sections from 20 to 185 GeV"}]},{"@id":"https://cir.nii.ac.jp/crid/1360292620180626432","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Further limits on heavy neutrino couplings"}]},{"@id":"https://cir.nii.ac.jp/crid/1360298760965894784","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Sterile neutrinos"}]},{"@id":"https://cir.nii.ac.jp/crid/1360298761980258688","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"GeV-scale neutrinos: interactions with mesons and DUNE sensitivity"}]},{"@id":"https://cir.nii.ac.jp/crid/1360302865739764864","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Sub-GeV dark matter search at ILC beam dumps"}]},{"@id":"https://cir.nii.ac.jp/crid/1360574093585797504","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Analysis of the (<i>N</i>,<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mrow><mml:msup><mml:mrow><mml:mi mathvariant=\"italic\">xN</mml:mi></mml:mrow><mml:mrow><mml:mo>′</mml:mo></mml:mrow></mml:msup></mml:mrow></mml:math>) reactions by quantum molecular dynamics plus statistical decay model"}]},{"@id":"https://cir.nii.ac.jp/crid/1360574094883402496","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"New electron beam-dump experiments to search for MeV to few-GeV dark matter"}]},{"@id":"https://cir.nii.ac.jp/crid/1360574096331910784","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"How to find neutral leptons of the νMSM?"}]},{"@id":"https://cir.nii.ac.jp/crid/1360579811551995008","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Heavy QCD axion at Belle II: Displaced and prompt signals"}]},{"@id":"https://cir.nii.ac.jp/crid/1360580229778848000","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"New physics searches at the ILC positron and electron beam dumps"}]},{"@id":"https://cir.nii.ac.jp/crid/1360580235269771520","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Polarized deep inelastic scattering at high energies and parity violating structure functions"}]},{"@id":"https://cir.nii.ac.jp/crid/1360580235942283520","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Improved big bang nucleosynthesis constraints on heavy neutral leptons"}]},{"@id":"https://cir.nii.ac.jp/crid/1360580235943674496","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Dark scalars and heavy neutral leptons at DarkQuest"}]},{"@id":"https://cir.nii.ac.jp/crid/1360580239279479680","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Implementation of muon pair production in PHITS and verification by comparing with the muon shielding experiment at SLAC"}]},{"@id":"https://cir.nii.ac.jp/crid/1360580239280097280","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Charm Photoproduction"}]},{"@id":"https://cir.nii.ac.jp/crid/1360846642119598208","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Features of Particle and Heavy Ion Transport code System (PHITS) version 3.02"}]},{"@id":"https://cir.nii.ac.jp/crid/1360848657371513216","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Beam dump experiment at future electron–positron colliders"}]},{"@id":"https://cir.nii.ac.jp/crid/1360855569088539520","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"General theory of weak processes involving neutrinos. I. Leptonic pseudoscalar-meson decays, with associated tests for, and bounds on, neutrino masses and lepton mixing"}]},{"@id":"https://cir.nii.ac.jp/crid/1360855569830955008","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Search for heavy neutrino decays in the BEBC beam dump experiment"}]},{"@id":"https://cir.nii.ac.jp/crid/1360855569919340416","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Relativistic nuclear collisions at<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mn>1</mml:mn><mml:mn>0</mml:mn><mml:mi>A</mml:mi></mml:math>GeV energies from<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mi>p</mml:mi><mml:mo>+</mml:mo><mml:mi mathvariant=\"normal\">Be</mml:mi></mml:math>to Au+Au with the hadronic cascade model"}]},{"@id":"https://cir.nii.ac.jp/crid/1360855570397266688","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Search for neutral heavy leptons produced in Z decays"}]},{"@id":"https://cir.nii.ac.jp/crid/1360855571518427392","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"New constraints on heavy neutral leptons from Super-Kamiokande data"}]},{"@id":"https://cir.nii.ac.jp/crid/1360861292465474432","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Searching for a sterile neutrino that mixes predominantly with \n<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:msub><mml:mi>ν</mml:mi><mml:mi>τ</mml:mi></mml:msub></mml:math>\n at \n<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mi>B</mml:mi></mml:math>\n factories"}]},{"@id":"https://cir.nii.ac.jp/crid/1360861711791889536","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"An allowed window for heavy neutral leptons below the kaon mass"}]},{"@id":"https://cir.nii.ac.jp/crid/1360861711809477632","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Expression of interest for the CODEX-b detector"}]},{"@id":"https://cir.nii.ac.jp/crid/1360861711980023680","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Constraints from the CHARM experiment on heavy neutral leptons with tau mixing"}]},{"@id":"https://cir.nii.ac.jp/crid/1361131417125049472","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Search for heavy neutrinos in π → μν decay"}]},{"@id":"https://cir.nii.ac.jp/crid/1361137043995102208","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Physics beyond colliders at CERN: beyond the Standard Model working group report"}]},{"@id":"https://cir.nii.ac.jp/crid/1361137045024291200","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Nuclear shadowing in electro-weak interactions"}]},{"@id":"https://cir.nii.ac.jp/crid/1361137045794529664","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Double-Cascade Events from New Physics in Icecube"}]},{"@id":"https://cir.nii.ac.jp/crid/1361418520616851840","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"New potentialities of the Liège intranuclear cascade model for reactions induced by nucleons and light charged particles"}]},{"@id":"https://cir.nii.ac.jp/crid/1361699993677507840","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Sterile neutrino searches via displaced vertices at LHCb"}]},{"@id":"https://cir.nii.ac.jp/crid/1361699994938577280","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Approximations to multiple Coulomb scattering"}]},{"@id":"https://cir.nii.ac.jp/crid/1361699995320430080","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Extending sensitivity for low-mass neutral heavy lepton searches"}]},{"@id":"https://cir.nii.ac.jp/crid/1361975844185884416","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Long-lived particles at the energy frontier: the MATHUSLA physics case"}]},{"@id":"https://cir.nii.ac.jp/crid/1361981468882774144","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Sensitivity bounds on heavy neutrino mixing \n<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mo stretchy=\"false\">|</mml:mo><mml:msub><mml:mi>U</mml:mi><mml:mrow><mml:mi>μ</mml:mi><mml:mi>N</mml:mi></mml:mrow></mml:msub><mml:msup><mml:mo stretchy=\"false\">|</mml:mo><mml:mn>2</mml:mn></mml:msup></mml:math>\n and \n<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mo stretchy=\"false\">|</mml:mo><mml:msub><mml:mi>U</mml:mi><mml:mrow><mml:mi>τ</mml:mi><mml:mi>N</mml:mi></mml:mrow></mml:msub><mml:msup><mml:mo stretchy=\"false\">|</mml:mo><mml:mn>2</mml:mn></mml:msup></mml:math>\n from LHCb upgrade"}]},{"@id":"https://cir.nii.ac.jp/crid/1361981470023036288","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Baryogenesis via Neutrino Oscillations"}]},{"@id":"https://cir.nii.ac.jp/crid/1362262944017026688","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"From eV to EeV: Neutrino cross sections across energy scales"}]},{"@id":"https://cir.nii.ac.jp/crid/1362262946421607680","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Parton distributions for the LHC"}]},{"@id":"https://cir.nii.ac.jp/crid/1362544420425334144","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"The νMSM, dark matter and baryon asymmetry of the universe"}]},{"@id":"https://cir.nii.ac.jp/crid/1362825895728102784","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Tau neutrino deep inelastic charged current interactions"}]},{"@id":"https://cir.nii.ac.jp/crid/1363107369140067328","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"A possible symmetry of the <mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" altimg=\"si1.gif\" overflow=\"scroll\"><mml:mi>ν</mml:mi><mml:mtext>MSM</mml:mtext></mml:math>"}]},{"@id":"https://cir.nii.ac.jp/crid/1363388843231794816","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Neutrino production of M+ and E+ heavy leptons (I)"}]},{"@id":"https://cir.nii.ac.jp/crid/1363388843864763520","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Pair production and bremsstrahlung of charged leptons"}]},{"@id":"https://cir.nii.ac.jp/crid/1363670319171961472","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Heavy neutral leptons at FASER"}]},{"@id":"https://cir.nii.ac.jp/crid/1363670319784379392","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Search for Heavy Right Handed Neutrinos at the FCC-ee"}]},{"@id":"https://cir.nii.ac.jp/crid/1363951793656142208","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"New tests for and bounds on neutrino masses and lepton mixing"}]},{"@id":"https://cir.nii.ac.jp/crid/1363951793945843968","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"The EGS5 Code System"}]},{"@id":"https://cir.nii.ac.jp/crid/1364233268290654208","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"FASER’s physics reach for long-lived particles"}]},{"@id":"https://cir.nii.ac.jp/crid/1364233269635285632","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Phenomenology of GeV-scale heavy neutral leptons"}]},{"@id":"https://cir.nii.ac.jp/crid/1364233269844410496","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"General theory of weak processes involving neutrinos. II. Pure leptonic decays"}]},{"@id":"https://cir.nii.ac.jp/crid/1364233270507655296","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Benchmark study of the recent version of the PHITS code"}]},{"@id":"https://cir.nii.ac.jp/crid/1390569647110453120","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@language":"en","@value":"Benchmarking of PHITS on Pion Production for Medium-Energy Physics"}]}],"dataSourceIdentifier":[{"@type":"CROSSREF","@value":"10.1007/jhep12(2022)145"},{"@type":"KAKEN","@value":"PRODUCT-24361928"},{"@type":"KAKEN","@value":"PRODUCT-24592543"},{"@type":"KAKEN","@value":"PRODUCT-25102571"},{"@type":"KAKEN","@value":"PRODUCT-24728929"},{"@type":"OPENAIRE","@value":"doi_dedup___::94833ec0af30f943384c6ee7e6e6f3ef"},{"@type":"CROSSREF","@value":"10.1007/jhep01(2023)145_references_DOI_J6M4mBLPWuT2QbyzfORCOVo5F93"},{"@type":"CROSSREF","@value":"10.1007/jhep02(2024)129_references_DOI_J6M4mBLPWuT2QbyzfORCOVo5F93"}]}