{"id":1204,"date":"2023-11-17T15:30:44","date_gmt":"2023-11-17T06:30:44","guid":{"rendered":"http:\/\/www-p.sci.ocha.ac.jp\/phys-hep\/?page_id=1204"},"modified":"2026-01-16T14:05:12","modified_gmt":"2026-01-16T05:05:12","slug":"%e7%a0%94%e7%a9%b6%e5%ae%a4%e3%82%bc%e3%83%9f","status":"publish","type":"page","link":"https:\/\/www-p.sci.ocha.ac.jp\/phys-hep\/lab-seminar.html","title":{"rendered":"\u7814\u7a76\u5ba4\u30bc\u30df(\u6587\u732e\u7d39\u4ecb)"},"content":{"rendered":"<h2>2026\u5e74<\/h2>\n<h3>1\u670816\u65e5<\/h3>\n<ol>\n<li>\u6587\u732e\u7d39\u4ecb(\u53e4\u91cc \u5bdb\u4e4b\u30fb\u5ca9\u624b\u5927\u5b66)<br \/>\nResonant Annihilation of WIMP Dark Matter for Halo Gamma Ray Signal<br \/>\n<a href=\"https:\/\/arxiv.org\/abs\/2512.01404\">https:\/\/arxiv.org\/abs\/2512.01404<\/a><\/li>\n<li>\u7814\u7a76\u9032\u6357\u5831\u544a<\/li>\n<\/ol>\n<h2>2025\u5e74<\/h2>\n<h3>12\u670812\u65e5<\/h3>\n<ol>\n<li>\u6587\u732e\u7d39\u4ecb(\u6ff1\u5d8b \u8389\u5e06)<br \/>\nEvidence of Relationships Among Fundamental Constants of the Standard Model<br \/>\n<a href=\"https:\/\/arxiv.org\/abs\/2509.07713\">https:\/\/arxiv.org\/abs\/2509.07713<\/a><\/li>\n<li>\u7814\u7a76\u9032\u6357\u5831\u544a<\/li>\n<\/ol>\n<h3>11\u670821\u65e5<\/h3>\n<ol>\n<li>\u6587\u732e\u7d39\u4ecb(\u83ca\u5730 \u548c\u594f)<br \/>\nCould the 650 GeV Excess be a Pseudoscalar of a 3-Higgs Doublet Model?<br \/>\n<a href=\"https:\/\/arxiv.org\/abs\/2509.06232\">https:\/\/arxiv.org\/abs\/2509.06232<\/a><\/li>\n<li>\u7814\u7a76\u9032\u6357\u5831\u544a<\/li>\n<\/ol>\n<h3>11\u670814\u65e5<\/h3>\n<ol>\n<li>\u6587\u732e\u7d39\u4ecb(\u5185\u7530\u7483\u5b50)<br \/>\nWhat is the Hierarchy Problem?<br \/>\n<a href=\"https:\/\/arxiv.org\/abs\/2505.00694\">https:\/\/arxiv.org\/abs\/2505.00694<\/a><\/li>\n<li>\u7814\u7a76\u9032\u6357\u5831\u544a<\/li>\n<\/ol>\n<h3>11\u67087\u65e5<\/h3>\n<ol>\n<li>\u6587\u732e\u7d39\u4ecb(\u85e4\u539f\u6709\u91cc\u5b50)<br \/>\nSearch for charged Higgs bosons through vector-like top quark pair production at the LHC<br \/>\n<a href=\"https:\/\/arxiv.org\/abs\/2407.01348\">https:\/\/arxiv.org\/abs\/2407.01348<\/a><\/li>\n<li>\u7814\u7a76\u9032\u6357\u5831\u544a<\/li>\n<\/ol>\n<h3>10\u670824\u65e5<\/h3>\n<ol>\n<li>\u6587\u732e\u7d39\u4ecb(\u9ad9\u934b\u7f8e\u6dbc)<br \/>\nInverse Seesaw Mechanism and Axion Portal Fermionic Dark Matter<br \/>\n<a href=\"https:\/\/arxiv.org\/abs\/2502.13002\">https:\/\/arxiv.org\/abs\/2502.13002<\/a><\/li>\n<li>\u7814\u7a76\u9032\u6357\u5831\u544a<\/li>\n<\/ol>\n<h3>10\u670817\u65e5<\/h3>\n<ol>\n<li>\u6587\u732e\u7d39\u4ecb(\u80fd\u52e2\u5343\u6676)<br \/>\nExplaining 650 GeV and 95 GeV Anomalies in the 2-Higgs Doublet Model Type-I<br \/>\n<a href=\"https:\/\/arxiv.org\/abs\/2509.06017\">https:\/\/arxiv.org\/abs\/2509.06017<\/a><\/li>\n<li>\u7814\u7a76\u9032\u6357\u5831\u544a<\/li>\n<\/ol>\n<h3>10\u670810\u65e5<\/h3>\n<ol>\n<li>\u6587\u732e\u7d39\u4ecb(\u72ac\u5bae \u7406\u6075)<br \/>\nOne-loop analysis of dark matter constraints in a complex scalar extension of the Standard Model<br \/>\n<a href=\"https:\/\/arxiv.org\/abs\/2506.23199\">https:\/\/arxiv.org\/abs\/2506.23199<\/a><\/li>\n<li>\u7814\u7a76\u9032\u6357\u5831\u544a<\/li>\n<\/ol>\n<h3>6\u670820\u65e5<\/h3>\n<ol>\n<li>\u6587\u732e\u7d39\u4ecb(\u5185\u7530 \u7483\u5b50)<br \/>\nDiscovery of a Glueball-like particle X(2370) at BESIII<br \/>\n<a href=\"https:\/\/arxiv.org\/abs\/2503.13286\">https:\/\/arxiv.org\/abs\/2503.13286<\/a><\/li>\n<li>\u7814\u7a76\u9032\u6357\u5831\u544a<\/li>\n<\/ol>\n<h3>6\u670813\u65e5<\/h3>\n<ol>\n<li>\u6587\u732e\u7d39\u4ecb(\u83ca\u5730 \u548c\u594f)<br \/>\nRecent Highlights from the Belle II Experiment<br \/>\n<a href=\"https:\/\/arxiv.org\/abs\/2502.10539\">https:\/\/arxiv.org\/abs\/2502.10539<\/a><\/li>\n<li>\u7814\u7a76\u9032\u6357\u5831\u544a<\/li>\n<\/ol>\n<h3>6\u67086\u65e5<\/h3>\n<ol>\n<li>\u6587\u732e\u7d39\u4ecb(\u6ff1\u5d8b \u8389\u5e06)<br \/>\nObservation of a pseudoscalar excess at the top quark pair production threshold<br \/>\n<a href=\"https:\/\/arxiv.org\/abs\/2503.22382\">https:\/\/arxiv.org\/abs\/2503.22382<\/a><\/li>\n<li>\u7814\u7a76\u9032\u6357\u5831\u544a<\/li>\n<\/ol>\n<h3>5\u670823\u65e5<\/h3>\n<ol>\n<li>\u6587\u732e\u7d39\u4ecb(\u53e4\u91cc \u5bdb\u4e4b\u30fb\u5ca9\u624b\u5927\u5b66)<br \/>\nVh production via vector boson scattering at lepton colliders in the Feynman-diagram gauge<\/li>\n<li>\u7814\u7a76\u9032\u6357\u5831\u544a<\/li>\n<\/ol>\n<h3>5\u670816\u65e5<\/h3>\n<ol>\n<li>\u6587\u732e\u7d39\u4ecb(\u85e4\u539f\u6709\u91cc\u5b50)<br \/>\nNeutrino properties from muonium-antimuonium mixing<br \/>\n<a href=\"https:\/\/arxiv.org\/abs\/2504.05378\">https:\/\/arxiv.org\/abs\/2504.05378<\/a><\/li>\n<li>\u7814\u7a76\u9032\u6357\u5831\u544a<\/li>\n<\/ol>\n<h3>5\u67089\u65e5<\/h3>\n<ol>\n<li>\u6587\u732e\u7d39\u4ecb(\u9ad9\u934b\u7f8e\u6dbc)<br \/>\nDirect Detection of Ultralight Dark Matter via Charged Lepton Flavor Violation<br \/>\n<a href=\"https:\/\/arxiv.org\/abs\/2503.07722\">https:\/\/arxiv.org\/abs\/2503.07722<\/a><\/li>\n<li>\u7814\u7a76\u9032\u6357\u5831\u544a<\/li>\n<\/ol>\n<h3>5\u67082\u65e5<\/h3>\n<ol>\n<li>\u6587\u732e\u7d39\u4ecb(\u80fd\u52e2\u5343\u6676)<br \/>\nPrinciple of multi-critical-points in the ALP-Higgs model and the corresponding phase transition<br \/>\n<a href=\"https:\/\/arxiv.org\/abs\/2402.12085\">https:\/\/arxiv.org\/abs\/2402.12085<\/a><\/li>\n<li>\u7814\u7a76\u9032\u6357\u5831\u544a<\/li>\n<\/ol>\n<h2>2024\u5e74<\/h2>\n<h3>12\u67086\u65e5<\/h3>\n<ol>\n<li>\u6587\u732e\u7d39\u4ecb(\u85e4\u539f\u6709\u91cc\u5b50)<br \/>\nInterpretation of excess in H \u2192 Z\u03b3 using a light axion-like particle<br \/>\n<a href=\"https:\/\/arxiv.org\/abs\/2402.05678\">https:\/\/arxiv.org\/abs\/2402.05678<\/a><\/li>\n<li>\u7814\u7a76\u9032\u6357\u5831\u544a<\/li>\n<\/ol>\n<h3>11\u670822\u65e5<\/h3>\n<ol>\n<li>\u6587\u732e\u7d39\u4ecb(\u9ad9\u934b\u7f8e\u6dbc)<br \/>\nW-mass and Muon g-2in Inert 2HDM Extended by Singlet Complex Scalar<br \/>\n<a href=\"https:\/\/arxiv.org\/abs\/2407.00181\">https:\/\/arxiv.org\/abs\/2407.00181<\/a><\/li>\n<li>\u7814\u7a76\u9032\u6357\u5831\u544a<\/li>\n<\/ol>\n<h3>11\u670815\u65e5<\/h3>\n<ol>\n<li>\u6587\u732e\u7d39\u4ecb(\u53e4\u91cc \u5bdb\u4e4b\u30fb\u5ca9\u624b\u5927\u5b66)<br \/>\nManifestly Covariant Canonical Formulation of Yang-Mills Field Theories: Physical State Subsidiary Conditions and Physical S Matrix Unitarity<br \/>\n<a href=\"https:\/\/inspirehep.net\/literature\/5749\">https:\/\/inspirehep.net\/literature\/5749<\/a><br \/>\n\u53c2\u8003\u8cc7\u6599:<a href=\"http:\/\/www2.yukawa.kyoto-u.ac.jp\/~taichiro.kugo\/M1lecture\/\u30b2\u30fc\u30b8\u5834\u306e\u7406\u8ad6\u3068\u7d4c\u8def\u7a4d\u520620210828.pdf\">http:\/\/www2.yukawa.kyoto-u.ac.jp\/~taichiro.kugo\/M1lecture\/\u30b2\u30fc\u30b8\u5834\u306e\u7406\u8ad6\u3068\u7d4c\u8def\u7a4d\u520620210828.pdf<\/a><\/li>\n<li>\u7814\u7a76\u9032\u6357\u5831\u544a<\/li>\n<\/ol>\n<h3>11\u67088\u65e5<\/h3>\n<ol>\n<li>\u6587\u732e\u7d39\u4ecb(\u9234\u6728 \u5c07\u592a \u30fb\u5ca9\u624b\u5927\u5b66)<br \/>\nMuon Collider Physics Summary<br \/>\n<a href=\"https:\/\/arxiv.org\/abs\/2203.07256\">https:\/\/arxiv.org\/abs\/2203.07256<\/a><\/li>\n<li>\u7814\u7a76\u9032\u6357\u5831\u544a<\/li>\n<\/ol>\n<h3>11\u67081\u65e5<\/h3>\n<ol>\n<li>\u6587\u732e\u7d39\u4ecb(\u7d30\u8c37 \u98af\u9a0e \u30fb\u5ca9\u624b\u5927\u5b66)<br \/>\nAutomatic generation of helicity amplitudes in Feynman-Diagram gauge<br \/>\n<a href=\"https:\/\/arxiv.org\/abs\/2405.01256\">https:\/\/arxiv.org\/abs\/2405.01256<\/a><\/li>\n<li>\u7814\u7a76\u9032\u6357\u5831\u544a<\/li>\n<\/ol>\n<h3>10\u670825\u65e5<\/h3>\n<ol>\n<li>\u6587\u732e\u7d39\u4ecb(\u80fd\u52e2\u5343\u6676)<br \/>\nCoscattering in the Extended Singlet-Scalar Higgs Portal<br \/>\n<a href=\"https:\/\/arxiv.org\/abs\/2404.19057\">https:\/\/arxiv.org\/abs\/2404.19057<\/a><\/li>\n<li>\u7814\u7a76\u9032\u6357\u5831\u544a<\/li>\n<\/ol>\n<h3>10\u670818\u65e5<\/h3>\n<ol>\n<li>\u6587\u732e\u7d39\u4ecb(\u9f4a\u85e4\u7dbe\u4e43)<br \/>\nA \u03bc-\u03c4-philic scalar doublet under Zn flavor symmetry<br \/>\n<a href=\"https:\/\/arxiv.org\/abs\/1904.10908v2\">https:\/\/arxiv.org\/abs\/1904.10908v2<\/a><\/li>\n<li>\u7814\u7a76\u9032\u6357\u5831\u544a<\/li>\n<\/ol>\n<h3>10\u670811\u65e5<\/h3>\n<ol>\n<li>\u6587\u732e\u7d39\u4ecb(\u5c0f\u6797\u304a\u304d)<br \/>\nDoubly Charged Lepton Search Potential of the FCC-Based Energy-Frontier Electron-Proton Colliders<br \/>\n<a href=\"https:\/\/arxiv.org\/abs\/1912.07351\">https:\/\/arxiv.org\/abs\/1912.07351<\/a><\/li>\n<li>\u7814\u7a76\u9032\u6357\u5831\u544a<\/li>\n<\/ol>\n<h3>10\u67084\u65e5<\/h3>\n<ol>\n<li>\u6587\u732e\u7d39\u4ecb(\u72ac\u5bae \u7406\u6075)<br \/>\nEnhanced Dark Matter Abundance in First-Order Phase Transitions<br \/>\n<a href=\"https:\/\/arxiv.org\/abs\/2409.02179\">https:\/\/arxiv.org\/abs\/2409.02179<\/a><\/li>\n<li>\u7814\u7a76\u9032\u6357\u5831\u544a<\/li>\n<\/ol>\n<h3>7\u670819\u65e5<\/h3>\n<ol>\n<li>\u6587\u732e\u7d39\u4ecb(\u9234\u6728 \u5c07\u592a\u30fb\u5ca9\u624b\u5927\u5b66)<br \/>\nExcited Lepton Production at LEP and HERA<br \/>\n<a href=\"https:\/\/link.springer.com\/article\/10.1007\/BF01571391\">Z. Phys. C 29, 115-122 (1985) <\/a><\/li>\n<li>\u7814\u7a76\u9032\u6357\u5831\u544a<\/li>\n<\/ol>\n<h3>7\u670812\u65e5<\/h3>\n<ol>\n<li>\u6587\u732e\u7d39\u4ecb(\u7d30\u8c37 \u98af\u9a0e \u30fb\u5ca9\u624b\u5927\u5b66)<br \/>\n(1) Determination of the relative sign of the Higgs boson couplings to W and Z bosons using WH production via vector-boson fusion with the ATLAS detector<br \/>\n<a href=\"https:\/\/arxiv.org\/abs\/2402.00426\">https:\/\/arxiv.org\/abs\/2402.00426<\/a><br \/>\n(2) Study of WH production through vector boson scattering and extraction of the relative sign of the W and Z couplings to the Higgs boson in proton-proton collisions at \\sqrt{s}=13 TeV<br \/>\n<a href=\"https:\/\/arxiv.org\/abs\/2405.16566\">https:\/\/arxiv.org\/abs\/2405.16566<\/a><\/li>\n<li>\u7814\u7a76\u9032\u6357\u5831\u544a<\/li>\n<\/ol>\n<h3>7\u67085\u65e5<\/h3>\n<ol>\n<li>\u6587\u732e\u7d39\u4ecb(\u53e4\u91cc \u5bdb\u4e4b\u30fb\u5ca9\u624b\u5927\u5b66)<br \/>\nW-boson pair production at lepton colliders in the Feynman-diagram gauge<br \/>\n<a href=\"https:\/\/arxiv.org\/abs\/2406.08869\">https:\/\/arxiv.org\/abs\/2406.08869<\/a><\/li>\n<li>\u7814\u7a76\u9032\u6357\u5831\u544a<\/li>\n<\/ol>\n<h3>6\u670828\u65e5<\/h3>\n<ol>\n<li>\u6587\u732e\u7d39\u4ecb(\u85e4\u539f\u6709\u91cc\u5b50)<br \/>\nSearching for Lepton Flavor Violation with the CMS Experiment<br \/>\n<a href=\"https:\/\/arxiv.org\/abs\/2403.12817\">https:\/\/arxiv.org\/abs\/2403.12817<\/a><\/li>\n<li>\u7814\u7a76\u9032\u6357\u5831\u544a<\/li>\n<\/ol>\n<h3>6\u670821\u65e5<\/h3>\n<ol>\n<li>\u6587\u732e\u7d39\u4ecb(\u9ad9\u934b\u7f8e\u6dbc)<br \/>\nSearching for Lepton Flavor Violation with the CMS Experiment<br \/>\n<a href=\"https:\/\/arxiv.org\/abs\/2403.12817\">https:\/\/arxiv.org\/abs\/2403.12817<\/a><\/li>\n<li>\u7814\u7a76\u9032\u6357\u5831\u544a<\/li>\n<\/ol>\n<h3>6\u670814\u65e5<\/h3>\n<ol>\n<li>\u6587\u732e\u7d39\u4ecb(\u80fd\u52e2\u5343\u6676)<br \/>\nAnalysis of the gg\u2192H\u2192hh\u21924\u03c4 process in the 2HDM lepton specific model at the LHC<br \/>\n<a href=\"https:\/\/arxiv.org\/abs\/2401.07289\">https:\/\/arxiv.org\/abs\/2401.07289<\/a><\/li>\n<li>\u7814\u7a76\u9032\u6357\u5831\u544a<\/li>\n<\/ol>\n<h3>5\u670831\u65e5<\/h3>\n<ol>\n<li>\u6587\u732e\u7d39\u4ecb(\u9f4a\u85e4\u7dbe\u4e43)<br \/>\nPortals into Higgs vacuum stability<br \/>\n<a href=\"https:\/\/arxiv.org\/abs\/2207.07737\">https:\/\/arxiv.org\/abs\/2207.07737<\/a><\/li>\n<li>\u7814\u7a76\u9032\u6357\u5831\u544a<\/li>\n<\/ol>\n<h3>5\u670824\u65e5<\/h3>\n<ol>\n<li>\u6587\u732e\u7d39\u4ecb(\u5c0f\u6797\u304a\u304d)<br \/>\nSearch For a Leptoquark and Vector-like Lepton in a Muon Collider<br \/>\n<a href=\"https:\/\/arxiv.org\/abs\/2309.07583\">https:\/\/arxiv.org\/abs\/2309.07583<\/a><\/li>\n<li>\u7814\u7a76\u9032\u6357\u5831\u544a<\/li>\n<\/ol>\n<h3>5\u670817\u65e5<\/h3>\n<ol>\n<li>\u6587\u732e\u7d39\u4ecb(\u72ac\u5bae \u7406\u6075)<br \/>\nDark matter transient annihilations in the early Universe<br \/>\n<a href=\"https:\/\/arxiv.org\/abs\/2109.07479\">https:\/\/arxiv.org\/abs\/2109.07479<\/a><\/li>\n<li>\u7814\u7a76\u9032\u6357\u5831\u544a<\/li>\n<\/ol>\n<h3>5\u670810\u65e5<\/h3>\n<ol>\n<li>\u6587\u732e\u7d39\u4ecb\u51fa\u5ddd\u667a\u9999\u5b50)<br \/>\nImplications of Nano-Hertz Gravitational Waves on Electroweak Phase Transition in the Singlet Dark Matter Model<br \/>\n<a href=\"https:\/\/arxiv.org\/abs\/2307.01072\">https:\/\/arxiv.org\/abs\/2307.01072<\/a><\/li>\n<li>\u7814\u7a76\u9032\u6357\u5831\u544a<\/li>\n<\/ol>\n<h2>2023\u5e74<\/h2>\n<h3>12\u67081\u65e5<\/h3>\n<ol>\n<li>\u6587\u732e\u7d39\u4ecb(\u5c71\u672c\u5357\u7dd2)<br \/>\nSearching for Majorana Neutrinos at a Same-Sign Muon Collider<br \/>\n<a href=\"https:\/\/arxiv.org\/abs\/2304.04483\">https:\/\/arxiv.org\/abs\/2304.04483<\/a><\/li>\n<li>\u7814\u7a76\u9032\u6357\u5831\u544a<\/li>\n<\/ol>\n<h3>11\u670824\u65e5<\/h3>\n<ol>\n<li>\u6587\u732e\u7d39\u4ecb(\u80fd\u52e2\u5343\u6676)<br \/>\nSearch for WIMPs at future \u03bc^+\u03bc^+ colliders<br \/>\n<a href=\"https:\/\/arxiv.org\/abs\/2310.07162\">https:\/\/arxiv.org\/abs\/2310.07162<\/a><\/li>\n<li>\u7814\u7a76\u9032\u6357\u5831\u544a<\/li>\n<\/ol>\n<h3>11\u670817\u65e5<\/h3>\n<ol>\n<li>\u6587\u732e\u7d39\u4ecb(\u9f4a\u85e4\u7dbe\u4e43)<br \/>\nObservability of the Higgs boson decay to a photon and a dark photon<br \/>\n<a href=\"https:\/\/arxiv.org\/abs\/2304.04165\">https:\/\/arxiv.org\/abs\/2304.04165<\/a><\/li>\n<li>\u7814\u7a76\u9032\u6357\u5831\u544a<\/li>\n<\/ol>\n<h3>11\u670810\u65e5<\/h3>\n<ol>\n<li>\u6587\u732e\u7d39\u4ecb(\u5c0f\u6797\u304a\u304d)<br \/>\nA forgotten fermion: the hypercharge -3\/2 doublet, its phenomenology and connections to dark matter<br \/>\n<a href=\"https:\/\/arxiv.org\/abs\/2301.12120\">https:\/\/arxiv.org\/abs\/2301.12120<\/a><\/li>\n<li>\u7814\u7a76\u9032\u6357\u5831\u544a<\/li>\n<\/ol>\n<h3>10\u670827\u65e5<\/h3>\n<ol>\n<li>\u6587\u732e\u7d39\u4ecb(\u7b39\u8cab \u767e\u82b1)<br \/>\nRenormalisation group analysis of scalar Leptoquark couplings addressing flavour anomalies: emergence of lepton-flavour universality<br \/>\n<a href=\"https:\/\/arxiv.org\/abs\/2307.15117\">https:\/\/arxiv.org\/abs\/2307.15117<\/a><\/li>\n<li>\u7814\u7a76\u9032\u6357\u5831\u544a<\/li>\n<\/ol>\n<h3>10\u670820\u65e5<\/h3>\n<ol>\n<li>\u6587\u732e\u7d39\u4ecb(\u5927\u9688 \u5f69\u83dc)<br \/>\nCollider Signatures of Type-X 2HDM + scalar singlet dark matter at HL-LHC<br \/>\n<a href=\"https:\/\/arxiv.org\/abs\/2112.15536\">https:\/\/arxiv.org\/abs\/2112.15536<\/a><\/li>\n<li>\u7814\u7a76\u9032\u6357\u5831\u544a<\/li>\n<\/ol>\n<h3>10\u670813\u65e5<\/h3>\n<ol>\n<li>\u6587\u732e\u7d39\u4ecb(\u72ac\u5bae \u7406\u6075)<br \/>\nPhenomenology of a two-component dark matter model<br \/>\n<a href=\"https:\/\/arxiv.org\/abs\/2201.11485\">https:\/\/arxiv.org\/abs\/2201.11485<\/a><\/li>\n<li>\u7814\u7a76\u9032\u6357\u5831\u544a<\/li>\n<\/ol>\n<h3>10\u67086\u65e5<\/h3>\n<ol>\n<li>\u6587\u732e\u7d39\u4ecb(\u51fa\u5ddd\u667a\u9999\u5b50)<br \/>\nSinglet-doublet Dirac fermion dark matter from Peccei-Quinn symmetry<br \/>\n<a href=\"https:\/\/arxiv.org\/abs\/2309.15052\">https:\/\/arxiv.org\/abs\/2309.15052<\/a><\/li>\n<li>\u7814\u7a76\u9032\u6357\u5831\u544a<\/li>\n<\/ol>\n<h3>7\u67087\u65e5<\/h3>\n<ol>\n<li>\u6587\u732e\u7d39\u4ecb(\u7b39\u8cab \u767e\u82b1)<br \/>\nExploring the cosmological dark matter coincidence using infrared fixed points<br \/>\n<a href=\"https:\/\/arxiv.org\/abs\/2210.11011\">https:\/\/arxiv.org\/abs\/2210.11011<\/a><\/li>\n<li>\u8a71\u984c\u63d0\u4f9b(\u83c5\u672c\u6676\u592b)<br \/>\nNANOGrav 15-years<\/li>\n<li>\u7814\u7a76\u9032\u6357\u5831\u544a<\/li>\n<\/ol>\n<h3>6\u670830\u65e5<\/h3>\n<ol>\n<li>\u6587\u732e\u7d39\u4ecb(\u5c71\u672c\u5357\u7dd2)<br \/>\nDark Matter searches at CMS and ATLAS<br \/>\n<a href=\"https:\/\/arxiv.org\/abs\/2301.10141\">https:\/\/arxiv.org\/abs\/2301.10141<\/a><\/li>\n<li>\u7814\u7a76\u9032\u6357\u5831\u544a<\/li>\n<\/ol>\n<h3>6\u670823\u65e5<\/h3>\n<ol>\n<li>\u6587\u732e\u7d39\u4ecb(\u80fd\u52e2\u5343\u6676)<br \/>\nA search for decays of the Higgs boson to invisible particles in events with a top-antitop quark pair or a vector boson in proton-proton collisions at \\sqrt{s} = 13 TeV<br \/>\n<a href=\"https:\/\/arxiv.org\/abs\/2303.01214\">https:\/\/arxiv.org\/abs\/2303.01214<\/a><\/li>\n<li>\u7814\u7a76\u9032\u6357\u5831\u544a<\/li>\n<\/ol>\n<h3>6\u670816\u65e5<\/h3>\n<ol>\n<li>\u6587\u732e\u7d39\u4ecb(\u9f4a\u85e4\u7dbe\u4e43)<br \/>\nA nearly Dirichlet Higgs for lower-scale warped extra dimensions<br \/>\n<a href=\"https:\/\/arxiv.org\/abs\/2305.09567\">https:\/\/arxiv.org\/abs\/2305.09567<\/a><\/li>\n<li>\u7814\u7a76\u9032\u6357\u5831\u544a<\/li>\n<\/ol>\n<h3>6\u67089\u65e5<\/h3>\n<ol>\n<li>\u6587\u732e\u7d39\u4ecb(\u5c0f\u6797\u304a\u304d)<br \/>\nY=0 Scalar Triplet Beyond the W Mass: (g-2)_\u03bc, h\u2192 \u03bc^+ \u03bc^- and CKM Unitarity<br \/>\n<a href=\"https:\/\/arxiv.org\/abs\/2305.03081\">https:\/\/arxiv.org\/abs\/2305.03081<\/a><\/li>\n<li>\u7814\u7a76\u9032\u6357\u5831\u544a<\/li>\n<\/ol>\n<h3>6\u67082\u65e5<\/h3>\n<ol>\n<li>\u56fd\u969b\u4f1a\u8b70\u3067\u306e\u767a\u8868\u30ea\u30cf\u30fc\u30b5\u30eb(\u51fa\u5ddd \u667a\u9999\u5b50)<\/li>\n<li>\u7814\u7a76\u9032\u6357\u5831\u544a<\/li>\n<\/ol>\n<h3>5\u670826\u65e5<\/h3>\n<ol>\n<li>\u6587\u732e\u7d39\u4ecb(\u5927\u9688 \u5f69\u83dc)<br \/>\nPhenomenological signatures of additional scalar bosons at the LHC<br \/>\n<a href=\"https:\/\/arxiv.org\/abs\/1606.01674\">https:\/\/arxiv.org\/abs\/1606.01674<\/a><\/li>\n<li>\u7814\u7a76\u9032\u6357\u5831\u544a<\/li>\n<\/ol>\n<h3>5\u670819\u65e5<\/h3>\n<ol>\n<li>\u6587\u732e\u7d39\u4ecb(\u72ac\u5bae \u7406\u6075)<br \/>\nAsymptotic safety and gauged baryon number<br \/>\n<a href=\"https:\/\/arxiv.org\/abs\/2206.02686\">https:\/\/arxiv.org\/abs\/2206.02686<\/a><\/li>\n<li>\u7814\u7a76\u9032\u6357\u5831\u544a<\/li>\n<\/ol>\n<h3>5\u670812\u65e5<\/h3>\n<ol>\n<li>\u6587\u732e\u7d39\u4ecb(\u51fa\u5ddd \u667a\u9999\u5b50)<br \/>\nGravitational waves and proton decay: complementary windows into GUTs<br \/>\n<a href=\"https:\/\/arxiv.org\/abs\/2005.13549\">https:\/\/arxiv.org\/abs\/2005.13549<\/a><\/li>\n<li>\u7814\u7a76\u9032\u6357\u5831\u544a<\/li>\n<\/ol>\n<h2>2022\u5e74<\/h2>\n<h3>1\u670827\u65e5<\/h3>\n<ol>\n<li>\u4fee\u8ad6\u767a\u8868\u4f1a\u30ea\u30cf\u30fc\u30b5\u30eb<\/li>\n<li>\u7814\u7a76\u9032\u6357\u5831\u544a<\/li>\n<\/ol>\n<h3>1\u670820\u65e5<\/h3>\n<ol>\n<li>\u7814\u7a76\u9032\u6357\u5831\u544a<\/li>\n<\/ol>\n<h3>1\u670813\u65e5<\/h3>\n<ol>\n<li>\u6587\u732e\u7d39\u4ecb(\u66fa\u00a0 \u57fa\u54f2)<br \/>\nPrecision test of the muon-Higgs coupling at a high-energy muon collider<br \/>\n<a href=\"https:\/\/arxiv.org\/abs\/2212.01323\">https:\/\/arxiv.org\/abs\/2212.01323<\/a><\/li>\n<li>\u6587\u732e\u7d39\u4ecb(\u99ac\u6e21\u5065\u592a\u90ce)<br \/>\nQED and QCD helicity amplitudes in parton-shower gauge<br \/>\n<a href=\"https:\/\/arxiv.org\/abs\/2003.03003\">https:\/\/arxiv.org\/abs\/2003.03003<\/a><br \/>\nHelicity amplitudes without gauge cancellation for electroweak processes<br \/>\n<a href=\"https:\/\/arxiv.org\/abs\/2203.10440\">https:\/\/arxiv.org\/abs\/2203.10440<\/a><br \/>\nHelicity amplitudes in light-cone and Feynman-diagram gauges<br \/>\n<a href=\"https:\/\/arxiv.org\/abs\/2211.14562\">https:\/\/arxiv.org\/abs\/2211.14562<\/a><\/li>\n<\/ol>\n<h3>12\u670823\u65e5<\/h3>\n<ol>\n<li>\u5f8c\u671f\u6210\u679c\u767a\u8868\u4f1a (3\/3)<\/li>\n<\/ol>\n<h3>12\u670816\u65e5<\/h3>\n<ol>\n<li>\u5f8c\u671f\u6210\u679c\u767a\u8868\u4f1a (2\/3)<\/li>\n<\/ol>\n<h3>12\u67089\u65e5<\/h3>\n<ol>\n<li>\u5f8c\u671f\u6210\u679c\u767a\u8868\u4f1a (1\/3)<\/li>\n<\/ol>\n<h3>12\u67082\u65e5<\/h3>\n<ol>\n<li>\u6587\u732e\u7d39\u4ecb(\u5409\u5dba \u51db)<br \/>\nProbing Light Charged Higgs Bosons in the 2-Higgs Doublet Model Type-II with Vector-Like Quarks<br \/>\n<a href=\"https:\/\/arxiv.org\/abs\/2211.07259\">https:\/\/arxiv.org\/abs\/2211.07259<\/a><\/li>\n<li>\u7814\u7a76\u9032\u6357\u5831\u544a<\/li>\n<\/ol>\n<h3>11\u670825\u65e5<\/h3>\n<ol>\n<li>\u6587\u732e\u7d39\u4ecb(\u9f4a\u85e4\u7dbe\u4e43)<br \/>\nCollider probe of heavy additional Higgs bosons solving the muon g-2<br \/>\n<a href=\"https:\/\/arxiv.org\/abs\/2210.13508\">https:\/\/arxiv.org\/abs\/2210.13508<\/a><\/li>\n<li>\u7814\u7a76\u9032\u6357\u5831\u544a<\/li>\n<\/ol>\n<h3>11\u670818\u65e5<\/h3>\n<ol>\n<li>\u6587\u732e\u7d39\u4ecb(\u5c0f\u6797\u304a\u304d)<br \/>\nThe Role of a Heavy Neutrino in the Gamma-Ray Burst GRB-221009A<br \/>\n<a href=\"https:\/\/arxiv.org\/abs\/2210.14178\">https:\/\/arxiv.org\/abs\/2210.14178<\/a><\/li>\n<li>\u7814\u7a76\u9032\u6357\u5831\u544a<\/li>\n<\/ol>\n<h3>11\u670811\u65e5<\/h3>\n<ol>\n<li>\u6587\u732e\u7d39\u4ecb(\u7b39\u8cab \u767e\u82b1)<br \/>\nInfra-Red Fixed Points in an Asymptotically Non-Free Theory<br \/>\n<a href=\"https:\/\/arxiv.org\/abs\/hep-ph\/9703321v3\">https:\/\/arxiv.org\/abs\/hep-ph\/9703321<\/a><\/li>\n<li>\u7814\u7a76\u9032\u6357\u5831\u544a<\/li>\n<\/ol>\n<h3>11\u67084\u65e5<\/h3>\n<ol>\n<li>\u6587\u732e\u7d39\u4ecb(\u5927\u9688 \u5f69\u83dc)<br \/>\nThe Two Higgs Doublet Model and the Multiple Point Principle<br \/>\n<a href=\"https:\/\/arxiv.org\/abs\/hep-ph\/0412333\">https:\/\/arxiv.org\/abs\/hep-ph\/0412333<\/a><\/li>\n<li>\u7814\u7a76\u9032\u6357\u5831\u544a<\/li>\n<\/ol>\n<h3>10\u670828\u65e5<\/h3>\n<ol>\n<li>\u6587\u732e\u7d39\u4ecb(\u5824 \u60a0\u7a00)<br \/>\nDirac dark matter, neutrino masses, and dark baryogenesis<br \/>\n<a href=\"https:\/\/arxiv.org\/abs\/2205.05762\">https:\/\/arxiv.org\/abs\/2205.05762<\/a><\/li>\n<li>\u7814\u7a76\u9032\u6357\u5831\u544a<\/li>\n<\/ol>\n<h3>10\u670821\u65e5<\/h3>\n<ol>\n<li>\u7814\u7a76\u9032\u6357\u5831\u544a<\/li>\n<\/ol>\n<h3>10\u670814\u65e5<\/h3>\n<ol>\n<li>\u6587\u732e\u7d39\u4ecb(\u6749\u539f \u68a8\u592e)<br \/>\nHigh scale boundary conditions with an additional complex singlet<br \/>\n<a href=\"https:\/\/arxiv.org\/abs\/1802.02391\">https:\/\/arxiv.org\/abs\/1802.02391<\/a><\/li>\n<li>\u7814\u7a76\u9032\u6357\u5831\u544a<\/li>\n<\/ol>\n<h3>10\u67087\u65e5<\/h3>\n<ol>\n<li>\u6587\u732e\u7d39\u4ecb(\u72ac\u5bae \u7406\u6075)<br \/>\nVacuum stability in the Standard Model with vector-like fermions<br \/>\n<a href=\"https:\/\/arxiv.org\/abs\/2207.10332\">https:\/\/arxiv.org\/abs\/2207.10332<\/a><\/li>\n<li>\u7814\u7a76\u9032\u6357\u5831\u544a<\/li>\n<\/ol>\n<h3>9\u670830\u65e5<\/h3>\n<ol>\n<li>\u6587\u732e\u7d39\u4ecb(\u51fa\u5ddd \u667a\u9999\u5b50)<br \/>\nElectroweak Baryogenesis in Non-minimal Composite Higgs Models<br \/>\n<a href=\"https:\/\/arxiv.org\/abs\/1110.2876\">https:\/\/arxiv.org\/abs\/1110.2876<\/a><\/li>\n<li>\u7814\u7a76\u9032\u6357\u5831\u544a<\/li>\n<\/ol>\n<h3>9\u670816\u65e5<\/h3>\n<ol>\n<li>\u6587\u732e\u7d39\u4ecb(\u5409\u5dba \u51db)<br \/>\n\u300c\u5b87\u5b99\u3068\u3044\u3046\u540d\u306e\u7389\u306d\u304e\u300d\u30fc\u30af\u30a9\u30fc\u30af\u9054\u3068\u5b87\u5b99\u306e\u7d20\u6027\u30fc<\/li>\n<li>\u7814\u7a76\u9032\u6357\u5831\u544a<\/li>\n<\/ol>\n<h3>7\u670822\u65e5<\/h3>\n<ol>\n<li>\u7814\u7a76\u9032\u6357\u5831\u544a<\/li>\n<li>\u524d\u671f\u7814\u7a76\u6d3b\u52d5\u632f\u308a\u8fd4\u308a (2)<\/li>\n<\/ol>\n<h3>7\u670815\u65e5<\/h3>\n<ol>\n<li>\u6587\u732e\u7d39\u4ecb(\u5927\u9688 \u5f69\u83dc)<br \/>\nSemi-dark Higgs decays: sweeping the Higgs neutrino floor<br \/>\n<a href=\"https:\/\/arxiv.org\/abs\/2206.01214\">https:\/\/arxiv.org\/abs\/2206.01214<\/a><\/li>\n<li>\u7814\u7a76\u9032\u6357\u5831\u544a<\/li>\n<\/ol>\n<h3>7\u67088\u65e5<\/h3>\n<ol>\n<li>\u7814\u7a76\u9032\u6357\u5831\u544a<\/li>\n<li>\u524d\u671f\u7814\u7a76\u6d3b\u52d5\u632f\u308a\u8fd4\u308a (1)<\/li>\n<\/ol>\n<h3>7\u67081\u65e5<\/h3>\n<ol>\n<li>\u6587\u732e\u7d39\u4ecb(\u9f4a\u85e4\u7dbe\u4e43)<br \/>\nSemi-Annihilation of Fermionic Dark Matter<br \/>\n<a href=\"https:\/\/arxiv.org\/abs\/2206.05811\">https:\/\/arxiv.org\/abs\/2206.05811<\/a><\/li>\n<li>\u7814\u7a76\u9032\u6357\u5831\u544a<\/li>\n<\/ol>\n<h3>6\u670824\u65e5<\/h3>\n<ol>\n<li>\u6587\u732e\u7d39\u4ecb(\u5c0f\u6797\u304a\u304d)<br \/>\nPossibility of multi-step electroweak phase transition in the two Higgs doublet models<br \/>\n<a href=\"https:\/\/arxiv.org\/abs\/2106.03439\">https:\/\/arxiv.org\/abs\/2106.03439<\/a><\/li>\n<li>\u7814\u7a76\u9032\u6357\u5831\u544a<\/li>\n<\/ol>\n<h3>6\u670817\u65e5<\/h3>\n<ol>\n<li>\u6587\u732e\u7d39\u4ecb(\u7b39\u8cab \u767e\u82b1)<br \/>\nImportance of vector leptoquark-scalar box diagrams in Pati-Salam unification with vector-like families<br \/>\n<a href=\"https:\/\/arxiv.org\/abs\/2201.04638\">https:\/\/arxiv.org\/abs\/2201.04638<\/a><\/li>\n<li>\u7814\u7a76\u9032\u6357\u5831\u544a<\/li>\n<\/ol>\n<h3>6\u670810\u65e5<\/h3>\n<ol>\n<li>\u6587\u732e\u7d39\u4ecb(\u5927\u9688 \u5f69\u83dc)<br \/>\nSemi-dark Higgs decays: sweeping the Higgs neutrino floor<br \/>\n<a href=\"https:\/\/arxiv.org\/abs\/2206.01214\">https:\/\/arxiv.org\/abs\/2206.01214<\/a><\/li>\n<li>\u7814\u7a76\u9032\u6357\u5831\u544a<\/li>\n<\/ol>\n<h3>6\u67083\u65e5<\/h3>\n<ol>\n<li>\u6587\u732e\u7d39\u4ecb(\u5824 \u60a0\u7a00)<br \/>\nA Simple Model of Dark Matter and CP Violation<br \/>\n<a href=\"https:\/\/arxiv.org\/abs\/2202.02954\">https:\/\/arxiv.org\/abs\/2202.02954<\/a><\/li>\n<li>\u7814\u7a76\u9032\u6357\u5831\u544a<\/li>\n<\/ol>\n<h3>5\u670827\u65e5<\/h3>\n<ol>\n<li>\u6587\u732e\u7d39\u4ecb(\u6749\u539f \u68a8\u592e)<br \/>\nWeak scale from Planck scale &#8212; Mass Scale Generation in Classically Conformal Two Scalar System &#8212;<br \/>\n<a href=\"https:\/\/arxiv.org\/abs\/1905.05656\">https:\/\/arxiv.org\/abs\/1905.05656<\/a><\/li>\n<li>\u7814\u7a76\u9032\u6357\u5831\u544a<\/li>\n<\/ol>\n<h3>5\u670813\u65e5<\/h3>\n<ol>\n<li>\u6587\u732e\u7d39\u4ecb(\u51fa\u5ddd \u667a\u9999\u5b50)<br \/>\nCP-violating effects on gravitational waves from electroweak phase transition in the CxSM with degenerate scalars<br \/>\nhttps:\/\/arxiv.org\/abs\/2205.12046<\/li>\n<li>\u7814\u7a76\u9032\u6357\u5831\u544a<\/li>\n<\/ol>\n<h3>5\u67086\u65e5<\/h3>\n<ol>\n<li>\u6587\u732e\u7d39\u4ecb(\u72ac\u5bae \u7406\u6075)<br \/>\n\u6f38\u8fd1\u7684\u5b89\u5168\u6027\u306b\u3088\u308b\u91cd\u529b\u306e\u91cf\u5b50\u8ad6\u3078\u306e\u30a2\u30d7\u30ed\u30fc\u30c1(\u592a\u7530\u4fe1\u7fa9\u8457\u3001\u4e38\u5584)<\/li>\n<li>\u7814\u7a76\u9032\u6357\u5831\u544a<\/li>\n<\/ol>\n<h2>2021\u5e74<\/h2>\n<h3>1\u670821\u65e5<\/h3>\n<ol>\n<li>\u6587\u732e\u7d39\u4ecb(\u7b39\u8cab \u767e\u82b1)<br \/>\nFlavour violating charged lepton decays in Little Randall-Sundrum Model<br \/>\n<a href=\"https:\/\/arxiv.org\/abs\/2201.01062\">https:\/\/arxiv.org\/abs\/2201.01062<\/a><\/li>\n<li>\u4fee\u8ad6\u767a\u8868\u4f1a\u30ea\u30cf\u30fc\u30b5\u30eb(\u6e21\u9089 \u590f\u5948)<\/li>\n<li>\u7814\u7a76\u9032\u6357\u5831\u544a<\/li>\n<\/ol>\n<h3>1\u670814\u65e5<\/h3>\n<ol>\n<li>\u6587\u732e\u7d39\u4ecb(\u5927\u9688 \u5f69\u83dc)<br \/>\nSearching for Flavor-Violating ALPs in Higgs Decays<br \/>\n<a href=\"https:\/\/arxiv.org\/abs\/2105.05866\">https:\/\/arxiv.org\/abs\/2105.05866<\/a><\/li>\n<li>\u7814\u7a76\u9032\u6357\u5831\u544a<\/li>\n<\/ol>\n<h3>1\u67087\u65e5<\/h3>\n<ol>\n<li>\u7814\u7a76\u9032\u6357\u5831\u544a<\/li>\n<\/ol>\n<h3>12\u670817\u65e5<\/h3>\n<ol>\n<li>\u6587\u732e\u7d39\u4ecb(\u72ac\u5bae \u7406\u6075)<br \/>\nThe Fermi constant from muon decay versus electroweak fits and CKM unitarity<br \/>\n<a href=\"https:\/\/arxiv.org\/abs\/2102.02825\">https:\/\/arxiv.org\/abs\/2102.02825<\/a><\/li>\n<li>\u6587\u732e\u7d39\u4ecb(\u4e95\u4e0a \u78a7)<br \/>\nAn exceptionally light axion: Strong CP and Dark Matter<br \/>\n<a href=\"https:\/\/arxiv.org\/abs\/2111.03149\">https:\/\/arxiv.org\/abs\/2111.03149<\/a><\/li>\n<li>\u7814\u7a76\u9032\u6357\u5831\u544a<\/li>\n<\/ol>\n<h3>12\u670810\u65e5<\/h3>\n<ol>\n<li>\u6587\u732e\u7d39\u4ecb(\u6749\u539f \u68a8\u592e)<br \/>\nThe muon g-2 in an Aligned 2-Higgs Doublet Model with Right-Handed Neutrinos<br \/>\n<a href=\"https:\/\/arxiv.org\/abs\/2111.12185\">https:\/\/arxiv.org\/abs\/2111.12185<\/a><\/li>\n<li>\u7814\u7a76\u9032\u6357\u5831\u544a<\/li>\n<\/ol>\n<h3>12\u67083\u65e5<\/h3>\n<ol>\n<li>\u6587\u732e\u7d39\u4ecb(\u5824 \u60a0\u7a00)<br \/>\nThe CN2HDM<br \/>\n<a href=\"https:\/\/arxiv.org\/abs\/2110.06680\">https:\/\/arxiv.org\/abs\/2110.06680<\/a><\/li>\n<li>\u7814\u7a76\u9032\u6357\u5831\u544a<\/li>\n<\/ol>\n<h3>11\u670826\u65e5<\/h3>\n<ol>\n<li>\u6587\u732e\u7d39\u4ecb(\u6e21\u9089 \u590f\u5948)<br \/>\nNonlocal SU(5) GUT<br \/>\n<a href=\"https:\/\/arxiv.org\/abs\/2012.10161\">https:\/\/arxiv.org\/abs\/2012.10161<\/a><\/li>\n<li>\u7814\u7a76\u9032\u6357\u5831\u544a<\/li>\n<\/ol>\n<h3>11\u670812\u65e5<\/h3>\n<ol>\n<li>\u6587\u732e\u7d39\u4ecb(\u51fa\u5ddd \u667a\u9999\u5b50)<br \/>\nElectroweak phase transition in a complex singlet extension of the Standard Model with degenerate scalars<br \/>\n<a href=\"https:\/\/arxiv.org\/abs\/2105.11830\">https:\/\/arxiv.org\/abs\/2105.11830<\/a><\/li>\n<li>\u7814\u7a76\u9032\u6357\u5831\u544a<\/li>\n<\/ol>\n<h3>11\u67085\u65e5<\/h3>\n<ol>\n<li>\u6587\u732e\u7d39\u4ecb(\u901f\u6c34 \u9999\u5948)<br \/>\nSeesaw determination of the dark matter relic density<br \/>\n<a href=\"https:\/\/arxiv.org\/abs\/2104.00042\">https:\/\/arxiv.org\/abs\/2104.00042<\/a><\/li>\n<li>\u7814\u7a76\u9032\u6357\u5831\u544a<\/li>\n<\/ol>\n<h3>10\u670829\u65e5<\/h3>\n<ol>\n<li>\u6587\u732e\u7d39\u4ecb(\u7b39\u8cab \u767e\u82b1)<br \/>\nThe CKM unitarity problem: A trace of new physics at the TeV scale?<br \/>\n<a href=\"https:\/\/arxiv.org\/abs\/1906.02714\">https:\/\/arxiv.org\/abs\/1906.02714<\/a><\/li>\n<li>\u7814\u7a76\u9032\u6357\u5831\u544a<\/li>\n<\/ol>\n<h3>10\u670822\u65e5<\/h3>\n<ol>\n<li>\u6587\u732e\u7d39\u4ecb(\u5927\u9688 \u5f69\u83dc)<br \/>\nDiscovering Axion-Like Particles with Photon Fusion at the ILC<br \/>\n<a href=\"https:\/\/arxiv.org\/abs\/2108.11927\">https:\/\/arxiv.org\/abs\/2108.11927<\/a><\/li>\n<li>\u7814\u7a76\u9032\u6357\u5831\u544a<\/li>\n<\/ol>\n<h3>10\u670815\u65e5<\/h3>\n<ol>\n<li>\u6587\u732e\u7d39\u4ecb(\u5824 \u60a0\u7a00)<br \/>\nTimelike Transition Form Factor for CP-odd Higgs Boson Production<br \/>\n<a href=\"https:\/\/arxiv.org\/abs\/2110.00286\">https:\/\/arxiv.org\/abs\/2110.00286<\/a><\/li>\n<li>\u7814\u7a76\u9032\u6357\u5831\u544a<\/li>\n<\/ol>\n<h3>10\u67088\u65e5<\/h3>\n<ol>\n<li>\u6587\u732e\u7d39\u4ecb(\u4e95\u4e0a \u78a7)<br \/>\nStimulated Laser Light Shining Through Wall Search for Axion Detection<br \/>\n<a href=\"https:\/\/arxiv.org\/abs\/2109.14663\">https:\/\/arxiv.org\/abs\/2109.14663<\/a><\/li>\n<li>\u7814\u7a76\u9032\u6357\u5831\u544a<\/li>\n<\/ol>\n<h3>10\u67081\u65e5<\/h3>\n<ol>\n<li>\u6587\u732e\u7d39\u4ecb(\u72ac\u5bae \u7406\u6075)<br \/>\nTest of the 4-th quark generation from the Cabibbo-Kobayashi-Maskawa matrix<br \/>\n<a href=\"https:\/\/arxiv.org\/abs\/2101.05386\">https:\/\/arxiv.org\/abs\/2101.05386<\/a><\/li>\n<li>\u7814\u7a76\u9032\u6357\u5831\u544a<\/li>\n<\/ol>\n<h3>9\u670824\u65e5<\/h3>\n<ol>\n<li>\u6587\u732e\u7d39\u4ecb(\u6e21\u9089 \u590f\u5948)<br \/>\nFAKE GUT<br \/>\n<a class=\"c-link\" href=\"https:\/\/arxiv.org\/abs\/1906.02977\" target=\"_blank\" rel=\"noopener noreferrer\" data-sk=\"tooltip_parent\">https:\/\/arxiv.org\/abs\/1906.02977<\/a><\/li>\n<li>\u7814\u7a76\u9032\u6357\u5831\u544a<\/li>\n<\/ol>\n<h3>9\u670810\u65e5<\/h3>\n<ol>\n<li>\u6587\u732e\u7d39\u4ecb(\u6749\u539f \u68a8\u592e)<br \/>\nConstraints on Pseudo-Nambu-Goldstone dark matter from direct detection experiment and neutron star reheating temperature<br \/>\n<a class=\"c-link\" href=\"https:\/\/arxiv.org\/abs\/2108.11381\" target=\"_blank\" rel=\"noopener noreferrer\" data-sk=\"tooltip_parent\">https:\/\/arxiv.org\/abs\/2108.11381<\/a><\/li>\n<li>\u7814\u7a76\u9032\u6357\u5831\u544a<\/li>\n<\/ol>\n<h3>7\u670830\u65e5<\/h3>\n<ol>\n<li>\u6587\u732e\u7d39\u4ecb(\u51fa\u5ddd \u667a\u9999\u5b50)<br \/>\nImpact of a complex singlet: From dark matter to baryogenesis<br \/>\n<a href=\"https:\/\/arxiv.org\/abs\/1502.07574\">https:\/\/arxiv.org\/abs\/1502.07574<\/a><\/li>\n<li>\u7814\u7a76\u9032\u6357\u5831\u544a<\/li>\n<\/ol>\n<h3>7\u670816\u65e5<\/h3>\n<ol>\n<li>\u6587\u732e\u7d39\u4ecb(\u901f\u6c34 \u9999\u5948)<br \/>\nThe CKM unitarity problem: A trace of new physics at the TeV scale?<br \/>\n<a href=\"https:\/\/arxiv.org\/abs\/1906.02714\">https:\/\/arxiv.org\/abs\/1906.02714<\/a><\/li>\n<li>\u7814\u7a76\u9032\u6357\u5831\u544a<\/li>\n<\/ol>\n<h3>7\u67089\u65e5<\/h3>\n<ol>\n<li>\u6587\u732e\u7d39\u4ecb(\u7c73\u6751 \u7f8e\u7d00)<br \/>\nNeutrino As The Dark Force<br \/>\n<a href=\"https:\/\/arxiv.org\/abs\/2106.08339\">https:\/\/arxiv.org\/abs\/2106.08339<\/a><\/li>\n<li>\u7814\u7a76\u9032\u6357\u5831\u544a<\/li>\n<\/ol>\n<h3>7\u67082\u65e5<\/h3>\n<ol>\n<li>\u6587\u732e\u7d39\u4ecb(\u4e45\u4fdd\u7530 \u7f8e\u7dd2)<br \/>\nCosmological Perturbations in Palatini Formalism<br \/>\n<a href=\"https:\/\/arxiv.org\/abs\/2010.07867\">https:\/\/arxiv.org\/abs\/2010.07867<\/a><\/li>\n<li>\u7814\u7a76\u9032\u6357\u5831\u544a<\/li>\n<\/ol>\n<h3>6\u670825\u65e5<\/h3>\n<ol>\n<li>\u6587\u732e\u7d39\u4ecb(\u7b39\u8cab \u767e\u82b1)<br \/>\n<span dir=\"auto\">Modified lepton couplings and the Cabibbo-angle anomaly<\/span><br \/>\n<a href=\"https:\/\/arxiv.org\/abs\/2009.03877\">https:\/\/arxiv.org\/abs\/2009.03877<\/a><\/li>\n<li>\u7814\u7a76\u9032\u6357\u5831\u544a<\/li>\n<\/ol>\n<h3>6\u670818\u65e5<\/h3>\n<ol>\n<li>\u6587\u732e\u7d39\u4ecb(\u5927\u9688 \u5f69\u83dc)<br \/>\nSearch for new light particles at ILC main beam dump<br \/>\n<a href=\"https:\/\/arxiv.org\/abs\/2009.13790\">https:\/\/arxiv.org\/abs\/2009.13790<\/a><\/li>\n<li>\u7814\u7a76\u9032\u6357\u5831\u544a<\/li>\n<\/ol>\n<h3>6\u670811\u65e5<\/h3>\n<ol>\n<li>\u6587\u732e\u7d39\u4ecb(\u5824 \u60a0\u7a00)<br \/>\n<span dir=\"auto\">An update on the two singlet Dark Matter model<\/span><br \/>\n<a class=\"c-link c-message_attachment__title_link\" href=\"https:\/\/arxiv.org\/abs\/2105.09044\" target=\"_blank\" rel=\"noreferrer noopener\" data-qa=\"message_attachment_title_link\"><span dir=\"auto\">https:\/\/arxiv.org\/abs\/2105.09044<\/span><\/a><\/li>\n<li>\u7814\u7a76\u9032\u6357\u5831\u544a<\/li>\n<\/ol>\n<h3>6\u67084\u65e5<\/h3>\n<ol>\n<li>\u6587\u732e\u7d39\u4ecb(\u6749\u539f \u68a8\u592e)<br \/>\nA misleading\u00a0CP<br \/>\nviolation measurement at DUNE induced by a Majorana phase<br \/>\n<a href=\"https:\/\/arxiv.org\/abs\/2011.01254\">https:\/\/arxiv.org\/abs\/2011.01254<\/a><\/li>\n<li>\u7814\u7a76\u9032\u6357\u5831\u544a<\/li>\n<\/ol>\n<h3>5\u670828\u65e5<\/h3>\n<ol>\n<li>\u6587\u732e\u7d39\u4ecb(\u72ac\u5bae \u7406\u6075)<br \/>\nEffects of a background scalar field induced by the Lorentz symmetry violation on Non Relativistic Quantum Mechanics<br \/>\n<a href=\"https:\/\/arxiv.org\/abs\/2105.04644\">https:\/\/arxiv.org\/abs\/2105.04644<\/a><\/li>\n<li>\u7814\u7a76\u9032\u6357\u5831\u544a<\/li>\n<\/ol>\n<h3>5\u670821\u65e5<\/h3>\n<ol>\n<li>\u6587\u732e\u7d39\u4ecb(\u6e21\u9089 \u590f\u5948)<br \/>\nSU(5)Unification without Proton Decay<br \/>\n<a href=\"https:\/\/arxiv.org\/abs\/1706.08535\">https:\/\/arxiv.org\/abs\/1706.08535<\/a><\/li>\n<li>\u7814\u7a76\u9032\u6357\u5831\u544a<\/li>\n<\/ol>\n<h3>5\u670814\u65e5<\/h3>\n<ol>\n<li>\u6587\u732e\u7d39\u4ecb(\u4e95\u4e0a \u78a7)<br \/>\nAxion Dark Matter: What is it and Why Now?<br \/>\n<a href=\"https:\/\/arxiv.org\/abs\/2105.01406\">https:\/\/arxiv.org\/abs\/2105.01406<\/a><\/li>\n<li>\u7814\u7a76\u9032\u6357\u5831\u544a<\/li>\n<\/ol>\n<h3>5\u67087\u65e5<\/h3>\n<ol>\n<li>\u6587\u732e\u7d39\u4ecb(\u65b0\u4e95 \u5e78)<br \/>\n\u52a0\u901f\u81a8\u5f35\u5b87\u5b99\u306b\u304a\u3051\u308b\u30d5\u30a7\u30eb\u30df\u30aa\u30f3\u5834\u306e\u9577\u8ddd\u96e2\u76f8\u95a2<\/li>\n<li>\u7814\u7a76\u9032\u6357\u5831\u544a<\/li>\n<\/ol>\n<h3>4\u670830\u65e5<\/h3>\n<ol>\n<li>\u6587\u732e\u7d39\u4ecb(\u51fa\u5ddd \u667a\u9999\u5b50)<br \/>\nCP Violation in the \u03c4 Lepton Yukawa Coupling and Flavour Symmetries<br \/>\n<a href=\"https:\/\/arxiv.org\/abs\/2103.16569\">https:\/\/arxiv.org\/abs\/2103.16569<\/a><\/li>\n<li>\u7814\u7a76\u9032\u6357\u5831\u544a<\/li>\n<\/ol>\n<h3>4\u670823\u65e5<\/h3>\n<ol>\n<li>\u6587\u732e\u7d39\u4ecb(\u901f\u6c34 \u9999\u5948)<br \/>\nQuasi-Dirac neutrinos in the linear seesaw model<br \/>\n<a href=\"https:\/\/arxiv.org\/abs\/2104.08023\">https:\/\/arxiv.org\/abs\/2104.08023<\/a><\/li>\n<li>\u7814\u7a76\u9032\u6357\u5831\u544a(slack\u306b\u3066)<\/li>\n<\/ol>\n<h3>4\u670816\u65e5<\/h3>\n<ol>\n<li>\u6587\u732e\u7d39\u4ecb(\u7c73\u6751 \u7f8e\u7d00)<br \/>\nClosing in on t-channel simplified dark matter models<br \/>\n<a href=\"https:\/\/arxiv.org\/abs\/2010.07559\">https:\/\/arxiv.org\/abs\/2010.07559<\/a><\/li>\n<li>\u7814\u7a76\u9032\u6357\u5831\u544a(\u4e45\u4fdd\u7530\u3001\u7c73\u6751\u3001\u901f\u6c34\u3001\u51fa\u5ddd\u3001\u65b0\u4e95\u3001\u4e95\u4e0a\u3001\u6e21\u9089\u3001\u72ac\u5bae\u3001\u6749\u539f\u3001\u5824\u3001\u5927\u9688\u3001\u7b39\u8cab)<\/li>\n<\/ol>\n<h3>4\u67089\u65e5<\/h3>\n<ol>\n<li>\u6587\u732e\u7d39\u4ecb(\u4e45\u4fdd\u7530 \u7f8e\u7dd2)<br \/>\nWhy primordial Non-Gaussianity is Very Small?<br \/>\n<a href=\"https:\/\/arxiv.org\/abs\/2104.01953\">https:\/\/arxiv.org\/abs\/2104.01953<\/a><\/li>\n<li>\u7814\u7a76\u9032\u6357\u5831\u544a(\u7c73\u6751\u3001\u901f\u6c34\u3001\u51fa\u5ddd\u3001\u65b0\u4e95\u3001\u72ac\u5bae\u3001\u6749\u539f\u3001\u5824\u3001\u5927\u9688\u3001\u7b39\u8cab)<\/li>\n<\/ol>\n<h3>2\u670819\u65e5<\/h3>\n<ol>\n<li>\u7814\u7a76\u9032\u6357\u5831\u544a(\u4e45\u4fdd\u7530 \u7f8e\u7dd2)<\/li>\n<li>\u7814\u7a76\u9032\u6357\u5831\u544a(\u7c73\u6751 \u7f8e\u7d00)<\/li>\n<li>\u7814\u7a76\u9032\u6357\u5831\u544a(\u51fa\u5ddd \u667a\u9999\u5b50)<\/li>\n<li>\u7814\u7a76\u9032\u6357\u5831\u544a(\u901f\u6c34 \u9999\u5948)<\/li>\n<li>\u7814\u7a76\u9032\u6357\u5831\u544a(\u6e21\u9089 \u590f\u5948)<\/li>\n<\/ol>\n<h3>2\u670812\u65e5<\/h3>\n<ol>\n<li>\u7814\u7a76\u9032\u6357\u5831\u544a(\u4e95\u4e0a \u78a7)<br \/>\n\u30a2\u30af\u30b7\u30aa\u30f3\u306b\u3064\u3044\u3066<\/li>\n<li>\u7814\u7a76\u9032\u6357\u5831\u544a(\u9060\u85e4 \u3081\u3050\u307f)<br \/>\n\u591a\u69d8\u4f53\u3068\u30c0\u30a4\u30d0\u30fc\u30b8\u30a7\u30f3\u30b9\u95a2\u6570\u306b\u3064\u3044\u3066<\/li>\n<\/ol>\n<h3>2\u67085\u65e5<\/h3>\n<ol>\n<li>\u6587\u732e\u7d39\u4ecb(\u901f\u6c34\u9999\u5948)<br \/>\nNonlocal SU(5) GUT<br \/>\n<a href=\"https:\/\/arxiv.org\/abs\/2012.10161\">https:\/\/arxiv.org\/abs\/2012.10161<\/a><\/li>\n<li>\u7814\u7a76\u9032\u6357\u5831\u544a(\u51fa\u5ddd\u667a\u9999\u5b50)<br \/>\nA fast C++ implementation of thermal functions<br \/>\n<a href=\"https:\/\/arxiv.org\/abs\/1802.02720\">https:\/\/arxiv.org\/abs\/1802.02720<\/a><\/li>\n<\/ol>\n<h3>1\u670822\u65e5<\/h3>\n<ol>\n<li>\u7814\u7a76\u9032\u6357\u5831\u544a(\u4e45\u4fdd\u7530 \u7f8e\u7dd2)<\/li>\n<li>\u6587\u732e\u7d39\u4ecb(\u7c73\u6751\u7f8e\u7d00)<br \/>\nTest of the 4-th quark generation from the Cabibbo-Kobayashi-Maskawa matrix<br \/>\n<a href=\"https:\/\/arxiv.org\/abs\/2101.05386\">https:\/\/arxiv.org\/abs\/2101.05386<\/a><\/li>\n<\/ol>\n<h3>1\u670815\u65e5<\/h3>\n<ol>\n<li>\u7814\u7a76\u9032\u6357\u5831\u544a(\u5824 \u60a0\u7a00)<\/li>\n<li>\u7814\u7a76\u9032\u6357\u5831\u544a(\u5fd7\u6469 \u975c\u9999)<\/li>\n<\/ol>\n<h3>1\u67088\u65e5<\/h3>\n<ol>\n<li>\u6587\u732e\u7d39\u4ecb(\u6e21\u9089 \u590f\u5948)<br \/>\nTests of the Atomki anomaly in lepton pair decays of heavy mesons<br \/>\n<a href=\"https:\/\/arxiv.org\/abs\/2101.01865\">https:\/\/arxiv.org\/abs\/2101.01865<\/a><\/li>\n<li>\u7814\u7a76\u9032\u6357\u5831\u544a(\u6749\u539f \u68a8\u592e)<\/li>\n<\/ol>\n<h2>2020\u5e74<\/h2>\n<h3>12\u670818\u65e5<\/h3>\n<ol>\n<li>\u6587\u732e\u7d39\u4ecb(\u4e95\u4e0a \u78a7)<br \/>\nNeutrino refractive effects during their decoupling era in the early universe<br \/>\n<a href=\"https:\/\/arxiv.org\/abs\/2011.05456\">https:\/\/arxiv.org\/abs\/2011.05456<\/a><\/li>\n<li>\u6587\u732e\u7d39\u4ecb(\u9060\u85e4 \u3081\u3050\u307f)<br \/>\nPentaquark Baryons in String Theory<br \/>\n<a href=\"https:\/\/arxiv.org\/abs\/hep-ph\/0405259\">https:\/\/arxiv.org\/abs\/hep-ph\/0405259<\/a><\/li>\n<li>\u8f2a\u8b1b(\u901f\u6c34 \u9999\u5948)<br \/>\n<a href=\"https:\/\/www.amazon.co.jp\/Concepts-Elementary-Particle-Physics-Oxford\/dp\/0198812183\" target=\"_blank\" rel=\"noopener\">Concepts of Elementary Particle Physics (M.E.Peskin)<\/a><br \/>\n&#8220;20. Neutrino Masses and Mixings&#8221;<\/li>\n<li>\u8f2a\u8b1b(\u66fa \u57fa\u54f2)<br \/>\n<a href=\"https:\/\/www.amazon.co.jp\/Concepts-Elementary-Particle-Physics-Oxford\/dp\/0198812183\" target=\"_blank\" rel=\"noopener\">Concepts of Elementary Particle Physics (M.E.Peskin)<\/a><br \/>\n&#8220;21. The Higgs Boson&#8221;<\/li>\n<\/ol>\n<h3>12\u67084\u65e5<\/h3>\n<ol>\n<li>\u8f2a\u8b1b(\u7c73\u6751\u7f8e\u7d00)<br \/>\n<a href=\"https:\/\/www.amazon.co.jp\/Concepts-Elementary-Particle-Physics-Oxford\/dp\/0198812183\" target=\"_blank\" rel=\"noopener\">Concepts of Elementary Particle Physics (M.E.Peskin)<\/a><br \/>\n&#8220;19. CP Violation&#8221;<\/li>\n<\/ol>\n<h3>11\u670827\u65e5<\/h3>\n<ol>\n<li>\u6587\u732e\u7d39\u4ecb(\u5824 \u60a0\u7a00)<br \/>\nHADES: A long lived particle detector concept for the FCC-ee or CEPC<br \/>\n<a href=\"https:\/\/arxiv.org\/abs\/2011.01005\">https:\/\/arxiv.org\/abs\/2011.01005<\/a><\/li>\n<li>\u8f2a\u8b1b(\u4e45\u4fdd\u7530 \u7f8e\u7dd2)<br \/>\n<a href=\"https:\/\/www.amazon.co.jp\/Concepts-Elementary-Particle-Physics-Oxford\/dp\/0198812183\" target=\"_blank\" rel=\"noopener\">Concepts of Elementary Particle Physics (M.E.Peskin)<\/a><br \/>\n&#8220;19. CP Violation&#8221;<\/li>\n<\/ol>\n<h3>11\u670820\u65e5<\/h3>\n<ol>\n<li>\u6587\u732e\u7d39\u4ecb(\u6749\u539f \u68a8\u592e)<br \/>\nVaccum Fluctuation Approach to study Neutrino Interaction<br \/>\n<a href=\"https:\/\/arxiv.org\/abs\/2011.06251\">https:\/\/arxiv.org\/abs\/2011.06251<\/a><\/li>\n<li>\u6587\u732e\u7d39\u4ecb(\u5fd7\u6469 \u975c\u9999)<br \/>\nModel identification in \\mu-e conversion with invisible boson emission using muonic atoms<br \/>\n<a href=\"https:\/\/arxiv.org\/abs\/2005.07894\">https:\/\/arxiv.org\/abs\/2005.07894<\/a><\/li>\n<\/ol>\n<h3>11\u670813\u65e5<\/h3>\n<ol>\n<li>\u6587\u732e\u7d39\u4ecb(\u6e21\u9089 \u590f\u5948)<br \/>\nGhosts in the Wall<br \/>\n<a href=\"https:\/\/arxiv.org\/abs\/2010.14028\">https:\/\/arxiv.org\/abs\/2010.14028<\/a><\/li>\n<\/ol>\n<h3>11\u67086\u65e5<\/h3>\n<ol>\n<li>\u6587\u732e\u7d39\u4ecb(\u51fa\u5ddd \u667a\u9999\u5b50)<br \/>\nVacuum structure and electroweak phase transition in singlet scalar model<br \/>\n<a href=\"https:\/\/arxiv.org\/abs\/2010.15708\">https:\/\/arxiv.org\/abs\/2010.15708<\/a><\/li>\n<li>\u6587\u732e\u7d39\u4ecb(\u9060\u85e4 \u3081\u3050\u307f)<br \/>\nBrane Cosmologies without Orbifolds<br \/>\n<a href=\"https:\/\/arxiv.org\/abs\/hep-ph\/0003173\">https:\/\/arxiv.org\/abs\/hep-ph\/0003173<\/a><\/li>\n<li>\u8f2a\u8b1b(\u5824 \u60a0\u7a00)<br \/>\n<a href=\"https:\/\/www.amazon.co.jp\/Concepts-Elementary-Particle-Physics-Oxford\/dp\/0198812183\" target=\"_blank\" rel=\"noopener\">Concepts of Elementary Particle Physics (M.E.Peskin)<\/a><br \/>\n&#8220;18. Quark Mixing Angles and Weak Decays&#8221;<\/li>\n<\/ol>\n<h3>10\u670830\u65e5<\/h3>\n<ol>\n<li>\u6587\u732e\u7d39\u4ecb(\u901f\u6c34 \u9999\u5948)<br \/>\nDileptonic Scalar Dark Matter and Exotic Leptons<br \/>\n<a href=\"https:\/\/arxiv.org\/abs\/2010.05054\">https:\/\/arxiv.org\/abs\/2010.05054<\/a><\/li>\n<li>\u8f2a\u8b1b(\u6749\u539f \u68a8\u592e)<br \/>\n<a href=\"https:\/\/www.amazon.co.jp\/Concepts-Elementary-Particle-Physics-Oxford\/dp\/0198812183\" target=\"_blank\" rel=\"noopener\">Concepts of Elementary Particle Physics (M.E.Peskin)<\/a><br \/>\n&#8220;17. The W and Z bosons&#8221;<\/li>\n<\/ol>\n<h3>10\u670823\u65e5<\/h3>\n<ol>\n<li>\u6587\u732e\u7d39\u4ecb(\u5824 \u60a0\u7a00)<br \/>\nDecaying dark matter, the H0 tension, and the lithium problem<br \/>\n<a href=\"https:\/\/arxiv.org\/abs\/2010.09715\">https:\/\/arxiv.org\/abs\/2010.09715<\/a><\/li>\n<li>\u8f2a\u8b1b(\u5fd7\u6469 \u975c\u9999)<br \/>\n<a href=\"https:\/\/www.amazon.co.jp\/Concepts-Elementary-Particle-Physics-Oxford\/dp\/0198812183\" target=\"_blank\" rel=\"noopener\">Concepts of Elementary Particle Physics (M.E.Peskin)<\/a><br \/>\n&#8220;16. Gauge Theories with Spontaneous Symmetry Breaking&#8221;<\/li>\n<\/ol>\n<h3>10\u670816\u65e5<\/h3>\n<ol>\n<li>\u6587\u732e\u7d39\u4ecb(\u6e21\u9089 \u590f\u5948)<br \/>\nBaryogenesis through baryon capture by black holes<br \/>\n<a href=\"https:\/\/arxiv.org\/abs\/2009.04361\">https:\/\/arxiv.org\/abs\/2009.04361<\/a><\/li>\n<li>\u6587\u732e\u7d39\u4ecb(\u6749\u539f \u68a8\u592e)<br \/>\nThermally produced scalar singlet as leptonphilic dark matter<br \/>\n<a href=\"https:\/\/arxiv.org\/abs\/2009.03789\">https:\/\/arxiv.org\/abs\/2009.03789<\/a><\/li>\n<li>\u8f2a\u8b1b(\u6e21\u9089 \u590f\u5948)<br \/>\n<a href=\"https:\/\/www.amazon.co.jp\/Concepts-Elementary-Particle-Physics-Oxford\/dp\/0198812183\" target=\"_blank\" rel=\"noopener\">Concepts of Elementary Particle Physics (M.E.Peskin)<\/a><br \/>\n&#8220;15. The Current-Current Model of the Weak Interaction&#8221;<\/li>\n<\/ol>\n<h3>10\u67089\u65e5<\/h3>\n<ol>\n<li>\u6587\u732e\u7d39\u4ecb(\u4e95\u4e0a \u78a7)<br \/>\nTheoretical bounds on dark matter masses<br \/>\n<a href=\"https:\/\/arxiv.org\/abs\/2009.11575\">https:\/\/arxiv.org\/abs\/2009.11575<\/a><\/li>\n<li>\u6587\u732e\u7d39\u4ecb(\u5fd7\u6469 \u975c\u9999)<br \/>\nDark Matter as a Solution to Muonic Puzzles<br \/>\n<a href=\"https:\/\/arxiv.org\/abs\/2009.09867\">https:\/\/arxiv.org\/abs\/2009.09867<\/a><\/li>\n<li>\u8f2a\u8b1b(\u4e95\u4e0a \u78a7)<br \/>\n<a href=\"https:\/\/www.amazon.co.jp\/Concepts-Elementary-Particle-Physics-Oxford\/dp\/0198812183\" target=\"_blank\" rel=\"noopener\">Concepts of Elementary Particle Physics (M.E.Peskin)<\/a><br \/>\n&#8220;14. Chiral Symmetry&#8221;<\/li>\n<\/ol>\n<h3>10\u67082\u65e5<\/h3>\n<ol>\n<li>\u6587\u732e\u7d39\u4ecb(\u51fa\u5ddd \u667a\u9999\u5b50)<br \/>\n<span dir=\"auto\">Electroweak symmetry breaking in the inverse seesaw mechanism<\/span><br \/>\n<a href=\"https:\/\/arxiv.org\/abs\/2009.10116\">https:\/\/arxiv.org\/abs\/2009.10116<\/a><\/li>\n<li>\u6587\u732e\u7d39\u4ecb(\u9060\u85e4 \u3081\u3050\u307f)<br \/>\nTesting Swampland Conjecture with Machine Learning<br \/>\n<a href=\"https:\/\/arxiv.org\/abs\/2006.07290\">https:\/\/arxiv.org\/abs\/2006.07290<\/a><\/li>\n<li>\u8f2a\u8b1b (\u9060\u85e4 \u3081\u3050\u307f)<br \/>\n<a href=\"https:\/\/www.amazon.co.jp\/Concepts-Elementary-Particle-Physics-Oxford\/dp\/0198812183\" target=\"_blank\" rel=\"noopener\">Concepts of Elementary Particle Physics (M.E.Peskin)<\/a><br \/>\n&#8220;13. QCD at Hadron Colliders&#8221;<\/li>\n<\/ol>\n<h3>9\u670825\u65e5<\/h3>\n<ol>\n<li>\u6587\u732e\u7d39\u4ecb(\u901f\u6c34 \u9999\u5948)<br \/>\nFlavorgenesis<br \/>\n<a href=\"https:\/\/arxiv.org\/abs\/2009.03909\">https:\/\/arxiv.org\/abs\/2009.03909<\/a><\/li>\n<li>\u8f2a\u8b1b(\u51fa\u5ddd \u667a\u9999\u5b50)<br \/>\n<a href=\"https:\/\/www.amazon.co.jp\/Concepts-Elementary-Particle-Physics-Oxford\/dp\/0198812183\" target=\"_blank\" rel=\"noopener\">Concepts of Elementary Particle Physics (M.E.Peskin)<\/a><br \/>\n&#8220;12. Partons and Jets&#8221;<\/li>\n<\/ol>\n<h3>9\u670818\u65e5<\/h3>\n<ol>\n<li>\u6587\u732e\u7d39\u4ecb(\u4e45\u4fdd\u7530 \u7f8e\u7dd2)<br \/>\nPalatini Higgs and Coleman-Weinberg inflation with non-minimal coupling<br \/>\n<a href=\"https:\/\/arxiv.org\/abs\/2009.04406\" target=\"_blank\" rel=\"noopener\">https:\/\/arxiv.org\/abs\/2009.04406<\/a><\/li>\n<li>\u6587\u732e\u7d39\u4ecb(\u66fa \u57fa\u54f2)<br \/>\nElectron and muon anomalies in general flavor conserving two Higgs doublets models<br \/>\n<a href=\"http:\/\/arxiv.org\/abs\/2006.01934\" target=\"_blank\" rel=\"noopener\">https:\/\/arxiv.org\/abs\/2006.01934<\/a><\/li>\n<li>\u8f2a\u8b1b(\u901f\u6c34 \u9999\u5948)<br \/>\n<a href=\"https:\/\/www.amazon.co.jp\/Concepts-Elementary-Particle-Physics-Oxford\/dp\/0198812183\" target=\"_blank\" rel=\"noopener\">Concepts of Elementary Particle Physics (M.E.Peskin)<\/a><br \/>\n&#8220;11. Quantum Chromodynamics&#8221;<\/li>\n<\/ol>\n<h3>9\u670811\u65e5<\/h3>\n<ol>\n<li>\u6587\u732e\u7d39\u4ecb(\u5fd7\u6469 \u975c\u9999)<br \/>\nThe Effects of Primordial Black Holes on Dark Matter Models<br \/>\n<a href=\"https:\/\/arxiv.org\/abs\/2009.02424\" target=\"_blank\" rel=\"noopener\">https:\/\/arxiv.org\/abs\/2009.02424<\/a><\/li>\n<li>\u6587\u732e\u7d39\u4ecb(\u66fa \u57fa\u54f2)<br \/>\nPrecision Microwave Spectroscopy of the Positronium N=2 Fine Structure<br \/>\n<a href=\"https:\/\/journals.aps.org\/prl\/abstract\/10.1103\/PhysRevLett.125.073002\" target=\"_blank\" rel=\"noopener\">https:\/\/journals.aps.org\/prl\/abstract\/10.1103\/PhysRevLett.125.073002<\/a><\/li>\n<\/ol>\n<h3>7\u670824\u65e5<\/h3>\n<ol>\n<li>\u6587\u732e\u7d39\u4ecb(\u51fa\u5ddd \u667a\u9999\u5b50)<br \/>\nCP Violation in B Decays (and the Search for New Physics)<br \/>\n<a href=\"https:\/\/arxiv.org\/abs\/2007.06061\" target=\"_blank\" rel=\"noopener\">https:\/\/arxiv.org\/abs\/2007.06061<\/a><\/li>\n<li>\u6587\u732e\u7d39\u4ecb(\u9060\u85e4 \u3081\u3050\u307f)<br \/>\nDark bubbles: decorating the wall<br \/>\n<a href=\"https:\/\/arxiv.org\/abs\/2001.07433\" target=\"_blank\" rel=\"noopener\">https:\/\/arxiv.org\/abs\/2001.07433<\/a><\/li>\n<li>\u8f2a\u8b1b(\u4e45\u4fdd\u7530 \u7f8e\u7dd2)<br \/>\n&#8220;Concepts of Elementary Particle Physics&#8221; (M.E.Peskin)<\/li>\n<\/ol>\n<h3>7\u670817\u65e5<\/h3>\n<ol>\n<li>\u6587\u732e\u7d39\u4ecb(\u901f\u6c34 \u9999\u5948)<br \/>\nRelaxing Cosmological Neutrino Mass Bounds with Unstable Neutrinos<br \/>\n<a href=\"https:\/\/arxiv.org\/abs\/2007.04994\" target=\"_blank\" rel=\"noopener\">https:\/\/arxiv.org\/abs\/2007.04994<\/a><\/li>\n<\/ol>\n<h3>7\u670810\u65e5<\/h3>\n<ol>\n<li>\u6587\u732e\u7d39\u4ecb(\u6749\u539f \u68a8\u592e)<br \/>\nSearching for GeV-scale Majorana Dark Matter: inter spem et metum and Stellar Cooling<br \/>\n<a href=\"https:\/\/arxiv.org\/abs\/2006.01348\" target=\"_blank\" rel=\"noopener\">https:\/\/arxiv.org\/abs\/2006.01348<\/a><\/li>\n<li>\u8f2a\u8b1b(\u5824 \u60a0\u7a00)<br \/>\n&#8220;Concepts of Elementary Particle Physics&#8221; (M.E.Peskin)<\/li>\n<\/ol>\n<h3>7\u67083\u65e5<\/h3>\n<ol>\n<li>\u6587\u732e\u7d39\u4ecb(\u5fd7\u6469 \u975c\u9999)<br \/>\nHidden Photon Dark Matter in the Light of XENON1T and Stellar Cooling<br \/>\n<a href=\"https:\/\/arxiv.org\/abs\/2006.11243\" target=\"_blank\" rel=\"noopener\">https:\/\/arxiv.org\/abs\/2006.11243<\/a><\/li>\n<li>\u6587\u732e\u7d39\u4ecb(\u5824 \u60a0\u7a00)<br \/>\nMissing in Axion: where are XENON1T&#8217;s big black holes?<br \/>\n<a href=\"https:\/\/arxiv.org\/abs\/2007.00650\" target=\"_blank\" rel=\"noopener\">https:\/\/arxiv.org\/abs\/2007.00650<\/a><\/li>\n<li>\u8f2a\u8b1b(\u5fd7\u6469 \u975c\u9999)<br \/>\n&#8220;Concepts of Elementary Particle Physics&#8221; (M.E.Peskin)<\/li>\n<\/ol>\n<h3>6\u670826\u65e5<\/h3>\n<ol>\n<li>\u6587\u732e\u7d39\u4ecb(\u4e95\u4e0a\u78a7)<br \/>\nDark Matter Search at Colliders and Neutrino Floor<br \/>\n<a href=\"https:\/\/arxiv.org\/abs\/2006.12768\" target=\"_blank\" rel=\"noopener\">https:\/\/arxiv.org\/abs\/2006.12768<\/a><\/li>\n<li>\u6587\u732e\u7d39\u4ecb(\u6e21\u9089\u590f\u5948)<br \/>\nNo short hair behaviors of ultra-compact stars<br \/>\n<a href=\"https:\/\/arxiv.org\/abs\/2005.14512\" target=\"_blank\" rel=\"noopener\">https:\/\/arxiv.org\/abs\/2005.14512<\/a><\/li>\n<li>\u8f2a\u8b1b(\u6749\u539f\u68a8\u592e)<br \/>\n&#8220;Concepts of Elementary Particle Physics&#8221; (M.E.Peskin)<\/li>\n<\/ol>\n<h3>6\u670819\u65e5<\/h3>\n<ol>\n<li>\u6587\u732e\u7d39\u4ecb(\u51fa\u5ddd\u667a\u9999\u5b50)<br \/>\nSearches for dark matter via charged Higgs pair production in the Inert Doublet Model at gamma-gamma collider<br \/>\n<a href=\"https:\/\/arxiv.org\/abs\/2006.06216\" target=\"_blank\" rel=\"noopener\">https:\/\/arxiv.org\/abs\/2006.06216<\/a><\/li>\n<li>\u6587\u732e\u7d39\u4ecb(\u4e45\u4fdd\u7530\u7f8e\u7dd2)<br \/>\nGravitational reheating and superheavy Dark Matter creation after inflation with non-minimal coupling<br \/>\n<a href=\"https:\/\/arxiv.org\/abs\/2006.02225\" target=\"_blank\" rel=\"noopener\">https:\/\/arxiv.org\/abs\/2006.02225<\/a><\/li>\n<li>\u8f2a\u8b1b(\u6e21\u9089\u590f\u5948)<br \/>\n&#8220;Concepts of Elementary Particle Physics&#8221; (M.E.Peskin)<\/li>\n<\/ol>\n<h3>6\u670812\u65e5<\/h3>\n<ol>\n<li>\u6587\u732e\u7d39\u4ecb(\u901f\u6c34\u9999\u5948)<br \/>\nA Higgs Doublet + Higgs Singlet Scheme with Negative Kinetic Term for Neutrino Mass Generation<br \/>\n<a href=\"https:\/\/arxiv.org\/abs\/2005.13016\" target=\"_blank\" rel=\"noopener\">https:\/\/arxiv.org\/abs\/2005.13016<\/a><\/li>\n<li>\u6587\u732e\u7d39\u4ecb(\u7c73\u6751\u7f8e\u7d00)<br \/>\nProbing heavy scalars with an effective Hbb\u00afg coupling at the LHC<br \/>\n<a href=\"https:\/\/arxiv.org\/abs\/2006.02218\" target=\"_blank\" rel=\"noopener\">https:\/\/arxiv.org\/abs\/2006.02218<\/a><\/li>\n<li>\u8f2a\u8b1b(\u4e95\u4e0a\u78a7)<br \/>\n&#8220;Concepts of Elementary Particle Physics&#8221; (M.E.Peskin)<\/li>\n<\/ol>\n<h3>6\u67085\u65e5<\/h3>\n<ol>\n<li>\u6587\u732e\u7d39\u4ecb(\u5824 \u60a0\u7a00)<br \/>\nThe X(3872) tetraquarks in B and B_s decays<br \/>\n<a href=\"https:\/\/arxiv.org\/abs\/2005.08764\" target=\"_blank\" rel=\"noopener\">https:\/\/arxiv.org\/abs\/2005.08764<\/a><\/li>\n<li>\u8f2a\u8b1b(\u9060\u85e4\u3081\u3050\u307f)<br \/>\n&#8220;Concepts of Elementary Particle Physics&#8221; (M.E.Peskin)<\/li>\n<\/ol>\n<h3>5\u670829\u65e5<\/h3>\n<ol>\n<li>\u6587\u732e\u7d39\u4ecb(\u6749\u539f\u68a8\u592e)<br \/>\nHiggs Portal From The Atmosphere To Hyper-K<br \/>\n<a href=\"https:\/\/arxiv.org\/abs\/2005.08980\" target=\"_blank\" rel=\"noopener\">https:\/\/arxiv.org\/abs\/2005.08980<\/a><\/li>\n<li>\u6587\u732e\u7d39\u4ecb(\u5fd7\u6469\u975c\u9999)<br \/>\nAnalytic model studies of polarized baryon production<br \/>\n<a href=\"https:\/\/arxiv.org\/abs\/2005.10514\" target=\"_blank\" rel=\"noopener\">https:\/\/arxiv.org\/abs\/2005.10514<\/a><\/li>\n<li>\u8f2a\u8b1b(\u51fa\u5ddd\u667a\u9999\u5b50)<br \/>\n&#8220;Concepts of Elementary Particle Physics&#8221; (M.E.Peskin)<\/li>\n<\/ol>\n<h3>5\u670822\u65e5<\/h3>\n<ol>\n<li>\u6587\u732e\u7d39\u4ecb(\u51fa\u5ddd\u667a\u9999\u5b50)<br \/>\nHiggs boson coupling as a probe of the sphaleron property<br \/>\n<a href=\"https:\/\/arxiv.org\/abs\/2005.05250\" target=\"_blank\" rel=\"noopener\">https:\/\/arxiv.org\/abs\/2005.05250<\/a><\/li>\n<li>\u6587\u732e\u7d39\u4ecb(\u6e21\u9089\u590f\u5948)<br \/>\nThird-family quark-lepton unification with a fundamental composite Higgs<br \/>\n<a href=\"https:\/\/arxiv.org\/abs\/2004.1137\" target=\"_blank\" rel=\"noopener\">https:\/\/arxiv.org\/abs\/2004.1137<\/a><\/li>\n<li>\u8f2a\u8b1b (\u901f\u6c34\u9999\u5948)<br \/>\n&#8220;Concepts of Elementary Particle Physics&#8221; (M.E.Peskin)<\/li>\n<\/ol>\n<h3>5\u670815\u65e5<\/h3>\n<ol>\n<li>\u6587\u732e\u7d39\u4ecb(\u66fa\u00a0 \u57fa\u54f2)<br \/>\nThe &#8220;96 GeV excess&#8221; at the LHC<br \/>\n<a href=\"https:\/\/arxiv.org\/abs\/2003.05422\" target=\"_blank\" rel=\"noopener\">https:\/\/arxiv.org\/abs\/2003.05422<\/a><\/li>\n<li>\u6587\u732e\u7d39\u4ecb(\u9060\u85e4\u3081\u3050\u307f)<br \/>\nEinstein Rings in Holography<br \/>\n<a href=\"https:\/\/arxiv.org\/abs\/1906.09113\" target=\"_blank\" rel=\"noopener\">https:\/\/arxiv.org\/abs\/1906.09113<\/a><\/li>\n<li>\u8f2a\u8b1b (\u4e45\u4fdd\u7530\u7f8e\u7dd2)<br \/>\n&#8220;Concepts of Elementary Particle Physics&#8221; (M.E.Peskin)<\/li>\n<\/ol>\n<h3>5\u67088\u65e5<\/h3>\n<ol>\n<li>\u6587\u732e\u7d39\u4ecb(\u4e95\u4e0a\u78a7)<br \/>\nRevisiting supernova constraints on a light CP-even scalar<br \/>\n<a href=\"https:\/\/arxiv.org\/abs\/2005.00490\" target=\"_blank\" rel=\"noopener\">https:\/\/arxiv.org\/abs\/2005.00490<\/a><\/li>\n<li>\u6587\u732e\u7d39\u4ecb(\u901f\u6c34\u9999\u5948)<br \/>\nHow long does the hydrogen atom live?<br \/>\n<a href=\"https:\/\/arxiv.org\/abs\/2003.02270\" target=\"_blank\" rel=\"noopener\">https:\/\/arxiv.org\/abs\/2003.02270<\/a><\/li>\n<li>\u8f2a\u8b1b (\u4e45\u4fdd\u7530\u7f8e\u7dd2)<br \/>\n&#8220;Concepts of Elementary Particle Physics&#8221; (M.E.Peskin)<\/li>\n<\/ol>\n<h2>2019\u5e74<\/h2>\n<h3>1\u670817\u65e5<\/h3>\n<ol>\n<li>\u5352\u696d\u7814\u7a76\u9032\u6357\u5831\u544a\u30fb\u767a\u8868\u4f1a\u30ea\u30cf\u30fc\u30b5\u30eb (\u51fa\u5ddd\u667a\u9999\u5b50)<\/li>\n<\/ol>\n<h3>1\u670810\u65e5<\/h3>\n<ol>\n<li>\u7814\u7a76\u9032\u6357\u5831\u544a(\u7c73\u6751\u7f8e\u7d00)<\/li>\n<li>MadGraph\u306e\u4f7f\u3044\u65b9\u306e\u89e3\u8aac(\u7c73\u6751\u7f8e\u7d00)<\/li>\n<\/ol>\n<h2>2018\u5e74<\/h2>\n<h3>12\u670820\u65e5<\/h3>\n<ol>\n<li>\u7814\u7a76\u9032\u6357\u5831\u544a\u4f1a(\u5168\u54e1)<\/li>\n<\/ol>\n<h3>11\u670829\u65e5<\/h3>\n<ol>\n<li>\u6587\u732e\u7d39\u4ecb(\u4e8c\u74f6\u68a2\u9999)<br \/>\nClockwork Higgs portal model for freeze-in dark matter<br \/>\n<a href=\"https:\/\/arxiv.org\/abs\/1709.04105\">https:\/\/arxiv.org\/abs\/1709.04105<\/a><\/li>\n<\/ol>\n<h3>11\u670822\u65e5<\/h3>\n<ol>\n<li>\u6587\u732e\u7d39\u4ecb(\u65e5\u8272\u53f2\u5948)<br \/>\nTikZ-Feynman(feynman diagram\u63cf\u753b\u30c4\u30fc\u30eb)<br \/>\n<a href=\"https:\/\/arxiv.org\/abs\/1601.05437\">https:\/\/arxiv.org\/abs\/1612.05125<\/a><\/li>\n<\/ol>\n<h3>11\u670815\u65e5<\/h3>\n<ol>\n<li>\u30bb\u30df\u30ca\u30fc<br \/>\n\u8b1b\u5e2b:\u67f3\u751f\u6176\u6c0f(\u6210\u8e4a\u5927\u5b66)<br \/>\n\u8b1b\u6f14\u984c\u76ee:\u8efd\u3044\u30d2\u30c3\u30b0\u30b9\u30dc\u30bd\u30f3\u3092\u5c0e\u304f\u30c6\u30e9\u30b9\u30b1\u30fc\u30eb\u306b\u304a\u3051\u308b\u5f37\u7d50\u5408\u306e\u529b\u5b66<\/li>\n<\/ol>\n<h3>11\u67088\u65e5<\/h3>\n<ol>\n<li>\u9032\u6357\u5831\u544a(\u4e45\u4fdd\u7530\u7f8e\u7dd2)<br \/>\n<span lang=\"EN-US\">Difference in prediction between metric and Palatini gravities for Higgs Inflation<\/span><\/li>\n<\/ol>\n<h3>11\u67081\u65e5<\/h3>\n<ol>\n<li>\u6587\u732e\u7d39\u4ecb(\u6a3d\u5c4b\u767e\u512a)<br \/>\nTheory and Phenomenology of Composite 2-Higgs Doublet Models<br \/>\n<a href=\"https:\/\/arxiv.org\/abs\/1612.05125\">https:\/\/arxiv.org\/abs\/1612.05125<\/a><\/li>\n<\/ol>\n<h3>10\u670825\u65e5<\/h3>\n<ol>\n<li>\u9032\u6357\u5831\u544a(\u963f\u90e8\u7965\u6b69)<br \/>\nFeynrules\u306b\u3088\u308b\u30e2\u30c7\u30eb\u30d5\u30a1\u30a4\u30eb\u4f5c\u6210\u3068MadGraph, MadDM\u3078\u306eimplementation\u306e\u73fe\u72b6\u5831\u544a<\/li>\n<li>\u6587\u732e\u7d39\u4ecb(\u963f\u90e8\u7965\u6b69)<br \/>\nLoop corrections to dark matter direct detection in a pseudoscalar mediator dark matter model<br \/>\n<a href=\"https:\/\/arxiv.org\/abs\/1810.01039\">https:\/\/arxiv.org\/abs\/1810.01039<\/a><\/li>\n<\/ol>\n<h3>10\u670818\u65e5<\/h3>\n<ol>\n<li>\u30bb\u30df\u30ca\u30fc<br \/>\n\u8b1b\u5e2b:\u9752\u6728\u771f\u7531\u7f8e\u6c0f(\u91d1\u6ca2\u5927\u5b66)<br \/>\n\u8b1b\u6f14\u984c\u76ee:\u91cd\u529b\u6ce2\u306b\u3088\u308b\u96a0\u308c\u305f\u8cea\u91cf\u8d77\u6e90\u306e\u691c\u8a3c\u53ef\u80fd\u6027<\/li>\n<\/ol>\n<h3>10\u670811\u65e5<\/h3>\n<ol>\n<li>\u9032\u6357\u5831\u544a(\u901f\u6c34\u9999\u5948)<br \/>\nmatter parity \u306b\u3088\u308b\u7c92\u5b50\u306e\u5b89\u5b9a\u6027<\/li>\n<\/ol>\n<h3>10\u67084\u65e5<\/h3>\n<ol>\n<li>\u6587\u732e\u7d39\u4ecb(\u7c73\u6751\u7f8e\u7d00)<br \/>\nDark Matter Searches in Jet plus Missing Energy in \u03b3p collision at CERN LHC<br \/>\n<a href=\"https:\/\/arxiv.org\/abs\/1407.5356\">https:\/\/arxiv.org\/abs\/1407.5356<\/a><\/li>\n<\/ol>\n<h3>9\u670827\u65e5<\/h3>\n<ol>\n<li>\u30bb\u30df\u30ca\u30fc<br \/>\n\u8b1b\u5e2b:\u5c71\u4e2d\u771f\u4eba\u6c0f(\u4e5d\u5dde\u7523\u696d\u5927\u5b66)<br \/>\n\u8b1b\u6f14\u984c\u76ee:BBN and leptogenesis in the CMSSM<\/li>\n<\/ol>\n<h3>7\u670826\u65e5<\/h3>\n<ol>\n<li>\u6587\u732e\u7d39\u4ecb(\u901f\u6c34\u9999\u5948)<br \/>\nA new solution of the fermionic mass hierarchy of the standard model<br \/>\nhttps:\/\/arxiv.org\/abs\/1807.05683 [hep-ph]<\/li>\n<li>\u540d\u53e4\u5c4b\u5927\u5b66\u7d20\u7c92\u5b50\u8ad6\u7814\u7a76\u5ba4(E\u7814)\u3067\u306e\u30b0\u30ed\u30fc\u30d0\u30eb\u30a4\u30f3\u30bf\u30fc\u30f3\u30b7\u30c3\u30d7(3\u30f6\u6708)\u306b\u3064\u3044\u3066(\u7c73\u6751\u7f8e\u7d00)<\/li>\n<li>\u9032\u6357\u5831\u544a:LHC\u3067\u306egamma-proton\u6563\u4e71\u306b\u3088\u308b spin-1 mediator\u63a2\u7d22(\u7c73\u6751\u7f8e\u7d00)<\/li>\n<\/ol>\n<h3>7\u670812\u65e5<\/h3>\n<ol>\n<li>\u5927\u962a\u5927\u5b66\u7d20\u7c92\u5b50\u8ad6\u7814\u7a76\u5ba4\u3067\u306e\u30b0\u30ed\u30fc\u30d0\u30eb\u30a4\u30f3\u30bf\u30fc\u30f3\u30b7\u30c3\u30d7(3\u30f6\u6708)\u306b\u3064\u3044\u3066(\u4e45\u4fdd\u7530\u7f8e\u7dd2)<\/li>\n<li>\u9032\u6357\u5831\u544a:\u30a4\u30f3\u30d5\u30ec\u30fc\u30b7\u30e7\u30f3\u6a5f\u69cb\u306b\u3064\u3044\u3066(\u4e45\u4fdd\u7530\u7f8e\u7dd2)<\/li>\n<\/ol>\n<h3>7\u67085\u65e5<\/h3>\n<ol>\n<li>\u30bb\u30df\u30ca\u30fc<br \/>\n\u8b1b\u5e2b:\u85e4\u9593 \u5d07\u6c0f(\u30df\u30e5\u30f3\u30d8\u30f3\u5de5\u79d1\u5927\u5b66)<br \/>\n\u8b1b\u6f14\u984c\u76ee:\u81ea\u5df1\u76f8\u4e92\u4f5c\u7528\u306e\u5f37\u3044\u30de\u30e8\u30e9\u30ca\u30d5\u30a7\u30eb\u30df\u30aa\u30f3\u30c0\u30fc\u30af\u30de\u30bf\u30fc<\/li>\n<\/ol>\n<h3>6\u670821\u65e5<\/h3>\n<ol>\n<li>\u8a08\u7b97\u6a5f\u8b1b\u7fd2(\u963f\u90e8\u7965\u6b69)<br \/>\nWebPlotDigitizer\u306e\u4f7f\u3044\u65b9(<a href=\"https:\/\/automeris.io\/WebPlotDigitizer\/\">https:\/\/automeris.io\/WebPlotDigitizer\/<\/a>)<\/li>\n<li>\u6587\u732e\u7d39\u4ecb(\u963f\u90e8\u7965\u6b69)<br \/>\nBound-state effects for dark matter with Higgs-like mediators<br \/>\nhttps:\/\/arxiv.org\/abs\/1805.00353 [hep-ph]<\/li>\n<li>\u6587\u732e\u7d39\u4ecb(\u963f\u90e8\u7965\u6b69)<br \/>\nFlavor Changing Neutral Currents in the Asymmetric Left-Right Gauge Model<br \/>\nhttps:\/\/arxiv.org\/abs\/1806.04812 [hep-ph]<\/li>\n<\/ol>\n<h3>6\u670814\u65e5<\/h3>\n<ol>\n<li>\u6587\u732e\u7d39\u4ecb(\u4e8c\u74f6\u68a2\u9999)<br \/>\n&#8220;A UV Complete Framework of Freeze-in Massive Particle Dark Matter&#8221;<br \/>\nA. Biswas, D. Borah, A. Dasgupta, arXiv:1805.06903 [hep-ph]<\/li>\n<\/ol>\n<h3>6\u67087\u65e5<\/h3>\n<ol>\n<li>\u901f\u5831\u4f1a(\u6a3d\u5c4b\u767e\u512a)<br \/>\narXiv: 1804.09889, 1805.07101, 1805,06734, 1804.09835, 1805.12027<\/li>\n<li>\u901f\u5831\u4f1a(\u65e5\u8272\u53f2\u5948)<br \/>\narXiv: 1804.03145, 1804.09660, 1804.10790, 1805.05807, 1805.10294, 1805.10513<\/li>\n<\/ol>\n<h3>5\u670824\u65e5<\/h3>\n<ol>\n<li>\u7814\u7a76\u9032\u6357\u5831\u544a(\u901f\u6c34\u9999\u5948)<br \/>\nGrand unified theory in minimal dark matter model<\/li>\n<\/ol>\n<h3>5\u670817\u65e5<\/h3>\n<ol>\n<li>\u7814\u7a76\u9032\u6357\u5831\u544a(\u963f\u90e8\u7965\u6b69)<br \/>\n\u30c0\u30fc\u30af\u30de\u30bf\u30fc\u3092\u8a18\u8ff0\u3059\u308b\u7406\u8ad6\u3068\u76f4\u63a5\u63a2\u7d22\u5b9f\u9a13\u306e\u6bd4\u8f03<\/li>\n<\/ol>\n<h3>5\u670810\u65e5<\/h3>\n<ol>\n<li>\u6587\u732e\u7d39\u4ecb(\u4e8c\u74f6\u68a2\u9999)<br \/>\n\u201cPhenomenology of Self-Interacting Dark Matter in a Matter-Dominated Universe\u201d<br \/>\nN. Bernal, C. Cosme and T. Tenkanen, arXiv:1803.08064 [hep-ph]<\/li>\n<\/ol>\n<h3>4\u670826\u65e5<\/h3>\n<ol>\n<li>\u901f\u5831(\u65e5\u8272\u53f2\u5948)<br \/>\narXiv.org\u30672018\u5e742\u6708\u4ee5\u964d\u306b\u767a\u8868\u3055\u308c\u305f\u8ad6\u6587\u304b\u30896\u5831<\/li>\n<li>\u00a0\u901f\u5831(\u6a3d\u5c4b\u767e\u512a)<br \/>\narXiv.org\u30672017\u5e74\u4e0b\u534a\u671f\u306b\u767a\u8868\u3055\u308c\u305f\u8ad6\u6587\u304b\u30897\u5831<\/li>\n<\/ol>\n<h3>4\u670819\u65e5<\/h3>\n<ol>\n<li>\u6587\u732e\u7d39\u4ecb(\u66fa \u57fa\u54f2)<br \/>\n\u201cObservation of ttbarH production\u201d<br \/>\nThe CMS collaboration, arXiv:1804.02610 [hep-ex]<\/li>\n<li>\u8a71\u984c\u63d0\u4f9b (\u83c5\u672c\u6676\u592b)<br \/>\n\u201cDeep learning\u3068AdS\/CFT\u201d<\/li>\n<\/ol>\n","protected":false},"excerpt":{"rendered":"<p>2026\u5e74 1\u670816\u65e5 \u6587\u732e\u7d39\u4ecb(\u53e4\u91cc \u5bdb\u4e4b\u30fb\u5ca9\u624b\u5927\u5b66) Resonant Annihilation of WIMP Dark Matter for Halo Gamma Ray Signal https:\/\/arxiv &hellip; <a href=\"https:\/\/www-p.sci.ocha.ac.jp\/phys-hep\/lab-seminar.html\">\u7d9a\u304d\u3092\u8aad\u3080 <span class=\"meta-nav\">&rarr;<\/span><\/a><\/p>\n","protected":false},"author":26,"featured_media":0,"parent":0,"menu_order":0,"comment_status":"closed","ping_status":"closed","template":"","meta":{"footnotes":""},"class_list":["post-1204","page","type-page","status-publish","hentry"],"aioseo_notices":[],"_links":{"self":[{"href":"https:\/\/www-p.sci.ocha.ac.jp\/phys-hep\/wp-json\/wp\/v2\/pages\/1204","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/www-p.sci.ocha.ac.jp\/phys-hep\/wp-json\/wp\/v2\/pages"}],"about":[{"href":"https:\/\/www-p.sci.ocha.ac.jp\/phys-hep\/wp-json\/wp\/v2\/types\/page"}],"author":[{"embeddable":true,"href":"https:\/\/www-p.sci.ocha.ac.jp\/phys-hep\/wp-json\/wp\/v2\/users\/26"}],"replies":[{"embeddable":true,"href":"https:\/\/www-p.sci.ocha.ac.jp\/phys-hep\/wp-json\/wp\/v2\/comments?post=1204"}],"version-history":[{"count":176,"href":"https:\/\/www-p.sci.ocha.ac.jp\/phys-hep\/wp-json\/wp\/v2\/pages\/1204\/revisions"}],"predecessor-version":[{"id":2688,"href":"https:\/\/www-p.sci.ocha.ac.jp\/phys-hep\/wp-json\/wp\/v2\/pages\/1204\/revisions\/2688"}],"wp:attachment":[{"href":"https:\/\/www-p.sci.ocha.ac.jp\/phys-hep\/wp-json\/wp\/v2\/media?parent=1204"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}