{"@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/1872272492444159488.json","@type":"Article","productIdentifier":[{"identifier":{"@type":"DOI","@value":"10.48550/arxiv.2201.06664"}}],"dc:title":[{"@value":"$μ$TRISTAN"}],"description":[{"notation":[{"@value":"The ultra-cold muon technology developed for the muon $g-2$ experiment at J-PARC provides a low emittance $μ^+$ beam which can be accelerated and used for realistic collider experiments. We consider the possibility of new collider experiments by accelerating the $μ^+$ beam up to 1 TeV. Allowing the $μ^+$ beam to collide with a high intensity $e^-$ beam at the TRISTAN energy, $E_{e^-}= 30$ GeV, in the storage ring with the same size as TRISTAN (the circumference of 3 km), one can realize a collider experiment with the center-of-mass energy $\\sqrt s = 346$ GeV, which allows productions of the Higgs bosons through the vector boson fusion processes. We estimate the deliverable luminosity with existing accelerator technologies to be at the level of $5 \\times 10^{33}$ cm$^{-2}$ s$^{-1}$, with which the collider can be a good Higgs boson factory. The $μ^+ μ^+$ colliders up to $\\sqrt s = 2$ TeV are also possible by using the same storage ring. They have a capability of producing the superpartner of the muon up to TeV masses."}]},{"notation":[{"@value":"23 pages, 7 figures, version to appear in PTEP"}]}],"creator":[{"@id":"https://cir.nii.ac.jp/crid/1892272492444159491","@type":"Researcher","foaf:name":[{"@value":"Hamada, Yu"}]},{"@id":"https://cir.nii.ac.jp/crid/1420282801198551168","@type":"Researcher","personIdentifier":[{"@type":"KAKEN_RESEARCHERS","@value":"50543451"},{"@type":"NRID","@value":"1000050543451"},{"@type":"NRID","@value":"9000003376141"},{"@type":"NRID","@value":"9000398130160"},{"@type":"NRID","@value":"9000388539007"},{"@type":"NRID","@value":"9000006550171"},{"@type":"NRID","@value":"9000411544525"},{"@type":"NRID","@value":"9000006701747"},{"@type":"NRID","@value":"9000411544574"},{"@type":"NRID","@value":"9000351499324"},{"@type":"NRID","@value":"9000241861941"},{"@type":"NRID","@value":"9000411544565"},{"@type":"NRID","@value":"9000388528685"},{"@type":"RESEARCHMAP","@value":"https://researchmap.jp/read0149927"}],"foaf:name":[{"@value":"Kitano, Ryuichiro"}]},{"@id":"https://cir.nii.ac.jp/crid/1892272492444159489","@type":"Researcher","foaf:name":[{"@value":"Matsudo, Ryutaro"}]},{"@id":"https://cir.nii.ac.jp/crid/1892272492444159490","@type":"Researcher","foaf:name":[{"@value":"Takaura, Hiromasa"}]},{"@id":"https://cir.nii.ac.jp/crid/1892272492444159492","@type":"Researcher","foaf:name":[{"@value":"Yoshida, Mitsuhiro"}]}],"publication":{"dc:publisher":[{"@value":"arXiv"}],"prism:publicationDate":"2022-01-01"},"foaf:topic":[{"@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=FOS:%20Physical%20sciences","dc:title":"FOS: Physical sciences"}],"relatedProduct":[{"@id":"https://cir.nii.ac.jp/crid/2051151842061958272","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isVersionOf"],"jpcoar:relatedTitle":[{"@value":"μTRISTAN"}]}],"dataSourceIdentifier":[{"@type":"OPENAIRE","@value":"doi_________::2a565903ab869d86f4e38c4fda1cdfac"}]}