{"id":614,"date":"2016-03-22T20:17:59","date_gmt":"2016-03-22T11:17:59","guid":{"rendered":"http:\/\/www-p.sci.ocha.ac.jp\/phys-hep\/?page_id=614"},"modified":"2025-09-26T13:48:43","modified_gmt":"2025-09-26T04:48:43","slug":"%e7%89%a9%e7%90%86%e5%ad%a6%e4%bc%9a%e3%81%a7%e3%81%ae%e8%ac%9b%e6%bc%94%ef%bc%88%ef%bc%91%ef%bc%89","status":"publish","type":"page","link":"https:\/\/www-p.sci.ocha.ac.jp\/phys-hep\/talks_jps.html","title":{"rendered":"\u65e5\u672c\u7269\u7406\u5b66\u4f1a\u306b\u304a\u3051\u308b\u8b1b\u6f14"},"content":{"rendered":"<h2>2025\u5e74<\/h2>\n<h3>\u65e5\u672c\u7269\u7406\u5b66\u4f1a\u7b2c80\u56de\u5e74\u6b21\u5927\u4f1a(\u5e83\u5cf6\u5927\u5b66(\u6771\u5e83\u5cf6\u30ad\u30e3\u30f3\u30d1\u30b9)\u30012025\u5e749\u670816\u65e5\u301c19\u65e5)<\/h3>\n<ol>\n<li>\u80fd\u52e2\u5343\u6676, \u66fa\u57fa\u54f2, \u51fa\u5ddd\u667a\u9999\u5b50<br \/>\nTwo Higgs doublet model with a complex singlet scalar\u306b\u304a\u3051\u308b\u591a\u91cd\u81e8\u754c\u70b9\u539f\u7406\u306e\u9069\u7528\u53ef\u80fd\u6027\u306b\u3064\u3044\u3066 (18aEK102-2)<\/li>\n<\/ol>\n<h3>\u65e5\u672c\u7269\u7406\u5b66\u4f1a2025\u5e74\u6625\u5b63\u5927\u4f1a(\u30aa\u30f3\u30e9\u30a4\u30f3\u958b\u50ac\u30012025\u5e743\u670818\u65e5\u301c21\u65e5)<\/h3>\n<h2>2024\u5e74<\/h2>\n<h3>\u65e5\u672c\u7269\u7406\u5b66\u4f1a\u7b2c79\u56de\u5e74\u6b21\u5927\u4f1a(\u5317\u6d77\u9053\u5927\u5b66\u30012024\u5e749\u670816\u65e5\u301c19\u65e5)<\/h3>\n<ol>\n<li>\u72ac\u5bae\u7406\u6075, \u51fa\u5ddd\u667a\u9999\u5b50, \u8239\u4e45\u4fdd\u516c\u4e00<br \/>\n\u6e29\u5ea6\u4f9d\u5b58\u6027\u3092\u8003\u616e\u3057\u305f\u6697\u9ed2\u7269\u8cea\u306e\u8cea\u91cf\u3067\u306e\u521d\u671f\u5b87\u5b99\u306e\u76f8\u8ee2\u79fb\u306b\u3088\u308b\u6b8b\u5b58\u91cf (17pWB101-5)<\/li>\n<li>\u9f4a\u85e4\u7dbe\u4e43, \u5c0f\u6797\u304a\u304d, \u66fa\u57fa\u54f2, \u99ac\u6e21\u5065\u592a\u90ce<br \/>\nSearching for signatures of 2HDM with Z4 symmetry in \u03bc- \u03bc+ and \u03bc+ \u03bc+ collisions (19aWB101-9)<\/li>\n<\/ol>\n<h3>\u65e5\u672c\u7269\u7406\u5b66\u4f1a2024\u5e74\u6625\u5b63\u5927\u4f1a(\u30aa\u30f3\u30e9\u30a4\u30f3\u958b\u50ac\u30012024\u5e743\u670818\u65e5\u301c21\u65e5)<\/h3>\n<ol>\n<li>\u9f4a\u85e4\u7dbe\u4e43, \u5c0f\u6797\u304a\u304d, \u66fa\u57fa\u54f2, \u99ac\u6e21\u5065\u592a\u90ce<br \/>\nSearch for two-Higgs doublet model with Z4 symmetry at muon collider (20aS2-4)<\/li>\n<li>\u83c5\u672c\u6676\u592b<br \/>\n\u30c0\u30a4\u30aa\u30cb\u30e5\u30fc\u30e0\u306b\u8a98\u8d77\u3055\u308c\u305f\u30d5\u30a7\u30eb\u30df\u30aa\u30f3\u6570\u306e\u7834\u308c (20aS2-11)<\/li>\n<li>\u72ac\u5bae\u7406\u6075, \u51fa\u5ddd\u667a\u9999\u5b50, \u66fa\u57fa\u54f2<br \/>\nTwo-component dark matter model with degenerate scalars (21aS2-6)<\/li>\n<\/ol>\n<h2>2023\u5e74<\/h2>\n<h3>\u65e5\u672c\u7269\u7406\u5b66\u4f1a\u7b2c78\u56de\u5e74\u6b21\u5927\u4f1a(\u6771\u5317\u5927\u5b66\u30012023\u5e749\u670816\u65e5\u301c19\u65e5)<\/h3>\n<ol>\n<li>\u5c0f\u6797\u304a\u304d, \u66fa\u57fa\u54f2, \u9f4a\u85e4\u7dbe\u4e43, \u99ac\u6e21\u5065\u592a\u90ce<br \/>\n\u30df\u30e5\u30fc\u30aa\u30f3\u30b3\u30e9\u30a4\u30c0\u30fc\u306b\u304a\u3051\u308bZ4\u4e0d\u5909\u306a2HDM\u306e\u691c\u8a3c\u53ef\u80fd\u6027 (18aS31-3)<\/li>\n<li>\u51fa\u5ddd\u667a\u9999\u5b50, \u702c\u540d\u6ce2\u6804\u554f<br \/>\n\u9ad8\u6b21\u5143\u6f14\u7b97\u5b50\u3092\u6301\u3064\u8907\u7d20\u30b7\u30f3\u30b0\u30ec\u30c3\u30c8\u30b9\u30ab\u30e9\u30fc\u62e1\u5f35\u6a21\u578b\u306b\u304a\u3051\u308b\u96fb\u6c17\u53cc\u6975\u5b50\u30e2\u30fc\u30e1\u30f3\u30c8\u3068\u96fb\u5f31\u30d0\u30ea\u30aa\u30f3\u6570\u751f\u6210 (16pRA21-11)<\/li>\n<\/ol>\n<h3>\u65e5\u672c\u7269\u7406\u5b66\u4f1a2023\u5e74\u6625\u5b63\u5927\u4f1a(\u30aa\u30f3\u30e9\u30a4\u30f3\u958b\u50ac\u30012023\u5e743\u670822\u65e5\u301c25\u65e5)<\/h3>\n<h2>2022\u5e74<\/h2>\n<h3>\u65e5\u672c\u7269\u7406\u5b66\u4f1a2022\u5e74\u79cb\u5b63\u5927\u4f1a(\u5ca1\u5c71\u7406\u79d1\u5927\u5b66\u30012022\u5e749\u67086\u65e5\u301c8\u65e5)<\/h3>\n<ol>\n<li>\u51fa\u5ddd\u667a\u9999\u5b50, \u66fa\u57fa\u54f2, \u702c\u540d\u6ce2\u6804\u554f<br \/>\n\u7e2e\u9000\u30b9\u30ab\u30e9\u30fc\u3092\u6301\u3064\u8907\u7d20\u30b9\u30ab\u30e9\u30fc\u62e1\u5f35\u6a21\u578b\u306b\u304a\u3051\u308bCP\u5bfe\u79f0\u6027\u3092\u7834\u308b\u4f4d\u76f8\u306e\u52b9\u679c\u3068\u305d\u306e\u91cd\u529b\u6ce2\u3078\u306e\u5bc4\u4e0e (6aA133-3)<\/li>\n<li>\u6749\u539f\u68a8\u592e, \u66fa\u57fa\u54f2, \u51fa\u5ddd\u667a\u9999\u5b50<br \/>\n\u8907\u7d20\u30b7\u30f3\u30b0\u30ec\u30c3\u30c8\u30b9\u30ab\u30e9\u30fc\u62e1\u5f35\u6a21\u578b\u306b\u304a\u3051\u308b\u30b9\u30ab\u30e9\u30fc\u30fb\u30dd\u30c6\u30f3\u30b7\u30e3\u30eb\u306e\u5206\u6790 (6pA133-3)<\/li>\n<li>\u72ac\u5bae\u7406\u6075, \u51fa\u5ddd\u667a\u9999\u5b50, \u66fa\u57fa\u54f2<br \/>\n\u30d2\u30c3\u30b0\u30b9\u30fb\u30dd\u30fc\u30bf\u30eb\u578b\u6697\u9ed2\u7269\u8cea\u6a21\u578b\u306b\u304a\u3051\u308b\u771f\u7a7a\u306e\u5b89\u5b9a\u6027 (6pA133-4)<\/li>\n<li>\u5824\u60a0\u7a00, \u66fa\u57fa\u54f2, \u51fa\u5ddd\u667a\u9999\u5b50<br \/>\n\u30d5\u30a7\u30eb\u30df\u30aa\u30f3\u6697\u9ed2\u7269\u8cea\u6a21\u578b\u306b\u304a\u3051\u308b\u30b7\u30b0\u30ca\u30eb\u6291\u5236\u6a5f\u69cb\u3068\u73fe\u8c61\u8ad6\u7684\u5e30\u7d50 (7pA133-11)<\/li>\n<\/ol>\n<h3>\u65e5\u672c\u7269\u7406\u5b66\u4f1a\u7b2c77\u56de\u5e74\u6b21\u5927\u4f1a(\u30aa\u30f3\u30e9\u30a4\u30f3\u958b\u50ac\u30012022\u5e743\u670815\u65e5\u301c19\u65e5)<\/h3>\n<h2>2021\u5e74<\/h2>\n<h3>\u65e5\u672c\u7269\u7406\u5b66\u4f1a2021\u5e74\u79cb\u5b63\u5927\u4f1a(\u30aa\u30f3\u30e9\u30a4\u30f3\u958b\u50ac\u30012021\u5e749\u670814\u65e5\u301c17\u65e5)<\/h3>\n<ol>\n<li>\u51fa\u5ddd\u667a\u9999\u5b50, \u66fa\u57fa\u54f2, \u702c\u540d\u6ce2\u6804\u554f<br \/>\n\u7e2e\u9000\u30b9\u30ab\u30e9\u30fc\u3092\u6301\u3064\u8907\u7d20\u30b7\u30f3\u30b0\u30ec\u30c3\u30c8\u30b9\u30ab\u30e9\u30fc\u62e1\u5f35\u6a21\u578b\u306b\u304a\u3051\u308b\u96fb\u5f31\u76f8\u8ee2\u79fb(14aS2-1)<\/li>\n<\/ol>\n<h3>\u65e5\u672c\u7269\u7406\u5b66\u4f1a\u7b2c76\u56de\u5e74\u6b21\u5927\u4f1a(\u30aa\u30f3\u30e9\u30a4\u30f3\u958b\u50ac\u30012021\u5e743\u670812\u65e5\u301c15\u65e5)<\/h3>\n<h2>2020\u5e74<\/h2>\n<h3>\u65e5\u672c\u7269\u7406\u5b66\u4f1a2020\u5e74\u79cb\u5b63\u5927\u4f1a(\u30aa\u30f3\u30e9\u30a4\u30f3\u958b\u50ac\u30012020\u5e749\u670814\u65e5\u301c17\u65e5)<\/h3>\n<ol>\n<li>\u51fa\u5ddd\u667a\u9999\u5b50, \u66fa\u57fa\u54f2<br \/>\n\u30b7\u30f3\u30b0\u30ec\u30c3\u30c8\u8907\u7d20\u30b9\u30ab\u30e9\u30fc\u62e1\u5f35\u6a21\u578b\u306b\u304a\u3051\u308b\u4e00\u6b21\u76f8\u8ee2\u79fb\u306e\u6761\u4ef6(16pSB-11)<\/li>\n<\/ol>\n<h3>\u65e5\u672c\u7269\u7406\u5b66\u4f1a\u7b2c75\u56de\u5e74\u6b21\u5927\u4f1a(\u540d\u53e4\u5c4b\u5927\u5b66\u30012020\u5e743\u670816\u65e5\u301c19\u65e5)(\u73fe\u5730\u958b\u50ac\u4e2d\u6b62)<\/h3>\n<ol>\n<li>\u51fa\u5ddd\u667a\u9999\u5b50, \u66fa\u57fa\u54f2<br \/>\n\u30b7\u30f3\u30b0\u30ec\u30c3\u30c8\u8907\u7d20\u30b9\u30ab\u30e9\u30fc\u62e1\u5f35\u6a21\u578b\u306b\u304a\u3051\u308b\u4e00\u6b21\u76f8\u8ee2\u79fb\u306e\u6761\u4ef6\u3068\u73fe\u8c61\u8ad6\u7684\u5e30\u7d50 (16pH11-7)<\/li>\n<li>\u51fa\u5ddd\u667a\u9999\u5b50, \u6a3d\u5c4b\u767e\u512a, \u66fa\u57fa\u54f2, \u65e5\u8272\u53f2\u5948, \u7c73\u6751\u7f8e\u7d00<br \/>\n\u8907\u7d20\u30b7\u30f3\u30b0\u30ec\u30c3\u30c8\u30b9\u30ab\u30e9\u30fc\u62e1\u5f35\u6a21\u578b\u306b\u304a\u3051\u308bCP\u5bfe\u79f0\u6027\u306e\u7834\u308c\u3068\u6697\u9ed2\u7269\u8cea\u554f\u984c (16pH11-8)<\/li>\n<li>\u4e45\u4fdd\u7530\u7f8e\u7dd2, \u4ed63\u540d<br \/>\nHiggs inflation in metric and Palatini formalisms: Required suppression of higher dimensional operators (17aH31-6)<\/li>\n<li>\u901f\u6c34\u9999\u5948, \u66fa\u57fa\u54f2, \u4ed61\u540d<br \/>\nGrand Unification of a simple extension of Minimal Dark Matter and collider signatures (19aH11-7)<\/li>\n<li>\u83c5\u672c\u6676\u592b, \u4ed66\u540d<br \/>\n\u975e\u5e73\u8861\u71b1\u529b\u5b66\u306e\u91cd\u529b\u30a2\u30ca\u30ed\u30b8\u30fc\u30e2\u30c7\u30eb I (17pH12-13)<\/li>\n<li>\u83c5\u672c\u6676\u592b, \u4ed66\u540d<br \/>\n\u975e\u5e73\u8861\u71b1\u529b\u5b66\u306e\u91cd\u529b\u30a2\u30ca\u30ed\u30b8\u30fc\u30e2\u30c7\u30eb II (17pH12-14)<\/li>\n<\/ol>\n<h2>2019\u5e74<\/h2>\n<h3>\u65e5\u672c\u7269\u7406\u5b66\u4f1a\u7b2c74\u56de\u5e74\u6b21\u5927\u4f1a(\u4e5d\u5dde\u5927\u5b66\u4f0a\u90fd\u30ad\u30e3\u30f3\u30d1\u30b9\u30012019\u5e743\u670814\u65e5\u301c17\u65e5)<\/h3>\n<ol>\n<li>\u901f\u6c34\u9999\u5948, \u66fa\u57fa\u54f2, \u4ed61\u540d<br \/>\nCoupling unification in an extension of the minimal dark matter model and collider signatures (14pK211-1)<\/li>\n<li>\u4e45\u4fdd\u7530\u7f8e\u7dd2\u3001\u4ed63\u540d<br \/>\nOn the fine-tuning of Higgs inflation in metric and Palatini formulations (15aK407-6)<\/li>\n<li>\u65e5\u8272\u53f2\u5948, \u7c73\u6751\u7f8e\u7d00, \u66fa\u57fa\u54f2<br \/>\nConstraints on light scalar in singlet Higgs extension of the SM at Belle-II (17aK212-5)<\/li>\n<li>\u66fa\u57fa\u54f2, \u963f\u90e8\u7965\u6b69,\u4ed61\u540d<br \/>\nSuppression of dark matter-nucelon scattering in singlet Higgs extension of the SM and its signature at collider experiments (17aK212-7)<\/li>\n<\/ol>\n<h2>2018\u5e74<\/h2>\n<h3>\u65e5\u672c\u7269\u7406\u5b66\u4f1a2018\u5e74\u79cb\u5b63\u5927\u4f1a(\u4fe1\u5dde\u5927\u5b66\u30012018\u5e749\u670814\u65e5\u301c17\u65e5)<\/h3>\n<ol>\n<li>\u00a0\u901f\u6c34\u9999\u5948, \u66fa\u57fa\u54f2, \u4ed61\u540d<br \/>\n\u62e1\u5f35\u3055\u308c\u305fminimal dark matter model\u306b\u304a\u3051\u308bgauge\u7d50\u5408\u5b9a\u6570\u306e\u7d71\u4e00 (14pS43-6)<\/li>\n<li>\u7c73\u6751\u7f8e\u7d00, \u66f9\u57fa\u54f2\u3001\u4ed61\u540d<br \/>\n\u5149\u5b50-\u967d\u5b50\u885d\u7a81\u306b\u304a\u3051\u308b\u30b9\u30d4\u30f31\u7c92\u5b50\u3092\u5a92\u4ecb\u3068\u3057\u305f\u6697\u9ed2\u7269\u8cea\u306e\u63a2\u7d22\u306b\u3064\u3044\u3066 (14pS43-4)<\/li>\n<li>\u963f\u90e8\u7965\u6b69, \u66f9\u57fa\u54f2<br \/>\n\u30b9\u30ab\u30e9\u30fc\u30c0\u30fc\u30af\u30de\u30bf\u30fc\u6a21\u578b\u306e\u6838\u5b50\u6563\u4e71\u6291\u5236\u6761\u4ef6\u3068\u73fe\u8c61\u8ad6\u7684\u5236\u9650 (14pS43-1)<\/li>\n<li>\u83c5\u672c\u6676\u592b,\u4ed64\u540d<br \/>\n\u56de\u8ee2\u3059\u308b\u5f37\u5236\u632f\u308a\u5b50\u306e\u30c0\u30a4\u30ca\u30df\u30af\u30b9\u3092\u5fdc\u7528\u3057\u305f\u30ec\u30d7\u30c8\u30f3\u6570\u751f\u6210\u6a5f\u69cb (14aS43-11)<\/li>\n<\/ol>\n<h3>\u65e5\u672c\u7269\u7406\u5b66\u4f1a\u7b2c73\u56de\u5e74\u6b21\u5927\u4f1a(\u6771\u4eac\u7406\u79d1\u5927\u5b66\u91ce\u7530\u30ad\u30e3\u30f3\u30d1\u30b9\u30012018\u5e743\u670822\u65e5\u301c25\u65e5)<\/h3>\n<ol>\n<li>\u66f9\u57fa\u54f2, \u798f\u7530\u88d5\u9999,\u4ed61\u540d<br \/>\nConstraints on lepton-flavor violating contact interactions at e+ e- linear collider (22aK306-8)<\/li>\n<li>\u7c73\u6751\u7f8e\u7d00, \u8d8a\u91ce\u8309\u4f9d\u7f85, \u66f9\u57fa\u54f2<br \/>\n\u5149\u5b50 \u967d\u5b50\u885d\u7a81\u306b\u304a\u3051\u308b\u30c0\u30fc\u30af\u30d5\u30a9\u30c8\u30f3\u751f\u6210\u5d29\u58ca (22aK306-10 )<\/li>\n<li>\u77e2\u8429\u91cf\u5b50, \u4ed61\u540d<br \/>\n\u8d85\u5bfe\u79f0\u7c92\u5b50\u306e\u30e9\u30b0\u30e9\u30f3\u30b8\u30a2\u30f3\u3092\u7528\u3044\u305f\u8d85\u91cd\u529b\u7406\u8ad6\u306e\u69cb\u6210 (22pK202-12)<\/li>\n<li>\u963f\u90e8\u7965\u6b69, \u66f9\u57fa\u54f2<br \/>\n\u30b9\u30ab\u30e9\u30fc\u30c0\u30fc\u30af\u30de\u30bf\u30fc\u3068\u6838\u5b50\u306e\u6563\u4e71\u6291\u5236\u6a5f\u69cb\u306b\u3064\u3044\u3066 (22pK306-8)<\/li>\n<li>\u901f\u6c34\u9999\u5948, \u66f9\u57fa\u54f2, \u4ed61\u540d<br \/>\nCoupling unification in minimal dark matter models (22pK306-9)<\/li>\n<li>\u5c71\u4e0b\u516c\u5b50, \u83c5\u672c\u6676\u592bA, \u4ed63\u540d<br \/>\nQED\u4e26\u3073\u306b\u96a0\u308c\u305f\u30bb\u30af\u30bf\u30fc\u3092\u542b\u3080QED\u306b\u304a\u3051\u308b\u5916\u90e8\u78c1\u5834\u4e2d\u306e\u96fb\u78c1\u6ce2\u504f\u5149\u30e2\u30fc\u30c9 (25aK306-9)<\/li>\n<\/ol>\n<h2>2017\u5e74<\/h2>\n<h3>\u65e5\u672c\u7269\u7406\u5b66\u4f1a2017\u5e74\u79cb\u5b63\u5927\u4f1a(\u5b87\u90fd\u5bae\u5927\u5b66\u5cf0\u30ad\u30e3\u30f3\u30d1\u30b9\u30012017\u5e749\u670812\u65e5\u301c15\u65e5)<\/h3>\n<ol>\n<li>\n<div class=\"width260\">\u798f\u7530\u88d5\u9999, \u6cb3\u91ce\u80fd\u77e5, \u66fa\u57fa\u54f2<\/div>\n<div>\u96fb\u5b50\u30fb\u967d\u96fb\u5b50\u30b3\u30e9\u30a4\u30c0\u30fc\u306b\u3088\u308b\u30ec\u30d7\u30c8\u30f3\u30fb\u30d5\u30ec\u30fc\u30d0\u30fc\u3092\u7834\u308b4\u4f53\u30d5\u30a7\u30eb\u30df\u76f8\u4e92\u4f5c\u7528\u306e\u63a2\u7d22 (13pS31-2)<\/div>\n<\/li>\n<li>\u5c71\u4e0b\u516c\u5b50\u3001 \u83c5\u672c\u6676\u592b\u3001\u4ed63\u540d<br \/>\n\u30d1\u30ea\u30c6\u30a3\u304c\u7834\u308c\u305f\u5834\u5408\u306b\u4e00\u822c\u5316\u3055\u308c\u305f\u30cf\u30a4\u30bc\u30f3\u30d9\u30eb\u30b0=\u30aa\u30a4\u30e9\u30fc\u516c\u5f0f (13pS31-8)<\/li>\n<li>\u5c71\u4e0b\u516c\u5b50\u3001 \u83c5\u672c\u6676\u592b\u3001\u4ed63\u540d<br \/>\n\u771f\u7a7a\u8907\u5c48\u6298\u5b9f\u9a13\u3092\u901a\u3057\u305fDark sector\u306e\u63a2\u7d22\u53ef\u80fd\u6027\u306b\u3064\u3044\u3066 (13pS31-9)<\/li>\n<li>\u5c71\u4e0b\u516c\u5b50\u3001\u4ed63\u540d<br \/>\n\u30b9\u30d4\u30f32\u306e\u7c92\u5b50\u3092\u5a92\u4ecb\u3068\u3057\u305f\u6697\u9ed2\u7269\u8cea\u6a21\u578b\u3078\u306eLHC\u304b\u3089\u306e\u5236\u9650 (14aT21-9)<\/li>\n<li>\u9f4b\u85e4\u9ebb\u7531\u7f8e\u3001\u4ed61\u540d<br \/>\n\u5357\u90e8\u306e\u30c0\u30a4\u30ca\u30df\u30af\u30b9\u306b\u5bfe\u3059\u308b\u30b7\u30f3\u30d7\u30ec\u30af\u30c6\u30a3\u30c3\u30af\u7a4d\u5206\u6cd5\u306e\u5fdc\u7528 (15aS33-9)<\/li>\n<\/ol>\n<h3>\u65e5\u672c\u7269\u7406\u5b66\u4f1a\u7b2c72\u56de\u5e74\u6b21\u5927\u4f1a(\u5927\u962a\u5927\u5b66\u8c4a\u4e2d\u30ad\u30e3\u30f3\u30d1\u30b9\u30012017\u5e743\u670817\u65e5\u301c20\u65e5)<\/h3>\n<ol>(\u767a\u8868\u306a\u3057)<\/ol>\n<h2>2016\u5e74<\/h2>\n<h3>\u65e5\u672c\u7269\u7406\u5b66\u4f1a2016\u5e74\u79cb\u5b63\u5927\u4f1a(\u5bae\u5d0e\u5927\u5b66\u6728\u82b1\u30ad\u30e3\u30f3\u30d1\u30b9\u30012016\u5e749\u670821\u65e5\u301c24\u65e5\u3001\u91d1\u6ca2\u5927\u5b66\u89d2\u9593\u30ad\u30e3\u30f3\u30d1\u30b9\u30019\u670813\u65e5\u301c16\u65e5)<\/h3>\n<ol>\n<li>\u4e0b\u83ef\u5948\u5b50\u3001\u66f9\u57fa\u54f2<br \/>\nSearch for lepton flavor violation in an e<sup>&#8211;<\/sup> e<sup>&#8211;<\/sup> collider (21aSC-2)<\/li>\n<li>\u5c71\u4e0b\u516c\u5b50\u3001\u66f9\u57fa\u54f2\u3001\u4ed64\u540d<br \/>\n\u30b9\u30d4\u30f32\u306e\u7c92\u5b50\u3092\u5a92\u4ecb\u3068\u3057\u305f\u6697\u9ed2\u7269\u8cea\u6a21\u578b\u3078\u306e\u5236\u9650\u3068LHC\u3067\u306e\u63a2\u7d22\u53ef\u80fd\u6027\u306b\u3064\u3044\u3066 (21pSC-9)<\/li>\n<li>\u9f4b\u85e4\u9ebb\u7531\u7f8e\u3001\u83c5\u672c\u6676\u592b\u3001\u4ed63\u540d<br \/>\n\u975e\u53ef\u63db\u7a7a\u9593\u4e0a\u306e\u6d41\u4f53\u30b7\u30df\u30e5\u30ec\u30fc\u30b7\u30e7\u30f3 (16aAH-5)<\/li>\n<\/ol>\n<div class=\"width260\"><\/div>\n<div class=\"width260\"><\/div>\n<h3>\u65e5\u672c\u7269\u7406\u5b66\u4f1a\u7b2c71\u56de\u5e74\u6b21\u5927\u4f1a( \u6771\u5317\u5b66\u9662\u5927\u5b66\u30012016\u5e743\u670819\u65e5\uff5e22\u65e5)<\/h3>\n<ol>\n<li>\u5c71\u4e0b\u516c\u5b50\u3001\u83c5\u672c\u6676\u592b\u3001\u4ed63\u540d<br \/>\n\u518d\u52a0\u71b1\u904e\u7a0b\u306b\u304a\u3051\u308b\u30a4\u30f3\u30d5\u30e9\u30c8\u30f3\u3068\u8907\u7d20\u30b9\u30ab\u30e9\u30fc\u3092\u7528\u3044\u305f\u30d0\u30ea\u30aa\u30f3\u6570\u751f\u6210\u6a5f\u69cb (21pAL-4)<\/li>\n<\/ol>\n<h2>2015\u5e74<\/h2>\n<h3>\u65e5\u672c\u7269\u7406\u5b66\u4f1a2015\u5e74\u79cb\u5b63\u5927\u4f1a( \u5927\u962a\u5e02\u7acb\u5927\u5b66\u30012015\u5e749\u670825\u65e5\uff5e28\u65e5)<\/h3>\n<ol>\n<li>\u9f4b\u85e4\u9ebb\u7531\u7f8e\u3001\u83c5\u672c\u6676\u592b\u3001\u4ed64\u540d<br \/>\n\u975e\u53ef\u63db\u7a7a\u9593\u4e0a\u306e\u6d41\u4f53\u306b\u5bfe\u3059\u308b\u6570\u5024\u89e3\u6790 (28pSC-4)<\/li>\n<li>\u77e2\u8429\u91cf\u5b50\u3001\u83c5\u672c\u6676\u592b<br \/>\n\u6cb3\u53e3\u5e7e\u4f55\u306b\u3088\u308b\u30e9\u30b0\u30e9\u30f3\u30b8\u30e5\u5f62\u5f0f\u306e\u8d85\u5f26\u7406\u8ad6\u3078\u306e\u5fdc\u7528 (28pSC-7)<\/li>\n<\/ol>\n<h3>\u65e5\u672c\u7269\u7406\u5b66\u4f1a\u7b2c70\u56de\u5e74\u6b21\u5927\u4f1a( \u65e9\u7a32\u7530\u5927\u5b66\u30012015\u5e743\u670821\u65e5\uff5e24\u65e5)<\/h3>\n<ol>\n<li>\u9f4b\u85e4\u9ebb\u7531\u7f8e,\u83c5\u672c\u6676\u592b\u3001\u4ed64\u540d<br \/>\n\u975e\u53ef\u63db\u7a7a\u9593\u4e0a\u306e\u6d41\u4f53\u30b7\u30df\u30e5\u30ec\u30fc\u30b7\u30e7\u30f3 (21pDA-13)<\/li>\n<li>\u99ac\u5872\u4e00\u6674\u3001\u4ed63\u540d<br \/>\n\u30a4\u30f3\u30d5\u30ec\u30fc\u30b7\u30e7\u30f3\u306b\u95a2\u3059\u308b\u89b3\u6e2c\u91cf\u306e\u6d41\u4f53\u6a21\u578b\u53ca\u3073F(R)\u91cd\u529b\u7406\u8ad6\u306b\u304a\u3051\u308b\u63cf\u50cf (21aDM-2)<\/li>\n<\/ol>\n<h2>2014\u5e74<\/h2>\n<h3>\u65e5\u672c\u7269\u7406\u5b66\u4f1a2014\u5e74\u79cb\u5b63\u5927\u4f1a( \u4f50\u8cc0\u5927\u5b66\u672c\u5e84\u30ad\u30e3\u30f3\u30d1\u30b9\u30012014\u5e749\u670818\u65e5\uff5e21\u65e5)<\/h3>\n<ol>\n<li>\u5c71\u4e0b\u516c\u5b50,\u66f9\u3000\u57fa\u54f2\u3001\u4ed62\u540d<br \/>\nLHC\u306b\u304a\u3051\u308b\u524d\u65b9\u691c\u51fa\u5668\u3092\u7528\u3044\u305f\u4f59\u5270\u6b21\u5143\u6a21\u578b\u306e\u691c\u8a3c (19aSD-6)<\/li>\n<li>\u9f4b\u85e4\u9ebb\u7531\u7f8e,\u99ac\u5872\u4e00\u6674,\u83c5\u672c\u6676\u592b<br \/>\nHydrodynamics on non-commutative space (20aSF-11)<\/li>\n<li>\u99ac\u5872\u4e00\u6674,\u4ed63\u540d<br \/>\n\u91cf\u5b50\u88dc\u6b63\u3092\u542b\u3080R2\u91cd\u529b\u7406\u8ad6\u3067\u306e\u30a4\u30f3\u30d5\u30ec\u30fc\u30b7\u30e7\u30f3\u5b87\u5b99\u8ad6 (18aSA-1)<\/li>\n<li>\u658e\u85e4\u90a3\u83dc,\u4ed6<br \/>\n\u5927\u578b\u4f4e\u6e29\u91cd\u529b\u6ce2\u671b\u9060\u93e1(KAGRA)\u30d7\u30ed\u30b8\u30a7\u30af\u30c8\u306e\u73fe\u72b6 (20aSB-1)<\/li>\n<li>\u6c5f\u5c3b\u60a0\u7f8e\u5b50,\u6a29\u85e4\u91cc\u5948,\u9234\u6728\u7406\u6075\u5b50,\u897f\u7530\u6075\u91cc\u5948,\u4ed6<br \/>\n\u30b9\u30da\u30fc\u30b9\u91cd\u529b\u6ce2\u30a2\u30f3\u30c6\u30caDECIGO\u8a08\u753b(55):DECIGO\/DPF\u306e\u6982\u8981 (21aSB-4)<\/li>\n<li>\u4e8c\u968e\u5802\u745e\u5e0c,\u4ed6<br \/>\n\u30b9\u30da\u30fc\u30b9\u91cd\u529b\u6ce2\u30a2\u30f3\u30c6\u30caDECIGO\u8a08\u753b(57):\u8a66\u9a13\u30de\u30b9 (21aSB-6)<\/li>\n<\/ol>\n<h3>\u65e5\u672c\u7269\u7406\u5b66\u4f1a\u7b2c69\u56de\u5e74\u6b21\u5927\u4f1a( \u6771\u6d77\u5927\u5b66\u30012014\u5e743\u670827\u65e5\uff5e30\u65e5)<\/h3>\n<ol>\n<li>\u5927\u91ce\u6176\u5b50\u3001\u66f9\u57fa\u54f2<br \/>\nRadion in Randall-Sundrum model at the LHC and photon collider (30pSB-10)<\/li>\n<li>\u99ac\u5872\u4e00\u6674\u3001\u4ed62\u540d<br \/>\n\u30e2\u30b8\u30e5\u30e9\u30a4\u30a4\u30f3\u30d5\u30ec\u30fc\u30b7\u30e7\u30f3\u3067\u306e\u5927\u57df\u7684\u78c1\u5834\u751f\u6210\u4e26\u3073\u306b\u66f2\u7387\u63fa\u3089\u304e\u306e\u975e\u30ac\u30a6\u30b9\u6027\u3068\u30c6\u30f3\u30bd\u30eb\/\u30b9\u30ab\u30e9\u30fc\u6bd4 (28aTT-3)<\/li>\n<li>\u658e\u85e4\u90a3\u83dc\u3001\u4ed6<br \/>\n\u5927\u578b\u4f4e\u6e29\u91cd\u529b\u6ce2\u671b\u9060\u93e1(KAGRA)\u30d7\u30ed\u30b8\u30a7\u30af\u30c8\u306e\u73fe\u72b6 (27aTL-1)<\/li>\n<li>\u6c5f\u5c3b\u60a0\u7f8e\u5b50\u3001\u6a29\u85e4\u91cc\u5948\u3001\u9234\u6728\u7406\u6075\u5b50\u3001\u4ed6<br \/>\n\u30b9\u30da\u30fc\u30b9\u91cd\u529b\u6ce2\u30a2\u30f3\u30c6\u30caDECIGO\u8a08\u753b(50):DECIGO\u306e\u30b5\u30a4\u30a8\u30f3\u30b9 (28aTL-1)<\/li>\n<li>\u4e8c\u968e\u5802\u745e\u5e0c\u3001\u4ed6<br \/>\n\u30b9\u30da\u30fc\u30b9\u91cd\u529b\u6ce2\u30a2\u30f3\u30c6\u30caDECIGO\u8a08\u753b(51):\u5e72\u6e09\u8a08\u30fb\u4fe1\u53f7\u51e6\u7406 (28aTL-2)<\/li>\n<li>\u4e8c\u968e\u5802\u745e\u5e0c\u3001\u4ed6<br \/>\n\u30b9\u30da\u30fc\u30b9\u91cd\u529b\u6ce2\u30a2\u30f3\u30c6\u30caDECIGO\u8a08\u753b(52):\u8a66\u9a13\u30de\u30b9 (28aTL-3)<\/li>\n<li>\u658e\u85e4\u90a3\u83dc\u3001\u4ed6<br \/>\n\u91cd\u529b\u6ce2\u6e2c\u5b9a\u5668\u306b\u304a\u3051\u308b\u30b9\u30af\u30a4\u30fc\u30b8\u30f3\u30b0\u3068\u5149\u30d0\u30cd\u306e\u79fb\u52d5 (28aTL-9)<\/li>\n<\/ol>\n<h2>2013\u5e74<\/h2>\n<h3>\u65e5\u672c\u7269\u7406\u5b66\u4f1a2013\u5e74\u79cb\u5b63\u5927\u4f1a( \u9ad8\u77e5\u5927\u5b66\u30012013\u5e749\u670820\u65e5\uff5e23\u65e5)<\/h3>\n<ol>\n<li>\u677e\u5c3e\u5149\u3001\u66f9\u57fa\u54f2\u3001\u4ed61\u540d<br \/>\nImplication of large A\u03bd in non-decoupling MSSM scenario at collider experiments (20pSE-9)<\/li>\n<li>\u9234\u6728\u5065\u53f8\u3001\u4ed62\u540d<br \/>\n\u975e\u53ef\u63db\u7a7a\u9593\u4e0a\u306e\u6709\u9650\u6e29\u5ea6\u30db\u30ed\u30b0\u30e9\u30d5\u30a3\u30c3\u30afQCD\u306b\u304a\u3051\u308b\u30d0\u30ea\u30aa\u30f3\u6570\u30ab\u30ec\u30f3\u30c8(20pSK-3)<\/li>\n<li>\u5897\u7530\u66a2<br \/>\n\u958b\u5f26\u306e\u5834\u306e\u7406\u8ad6\u306b\u304a\u3051\u308b\u4e8c\u91cd\u30d6\u30ec\u30fc\u30f3\u89e3\u5468\u308a\u306e\u7269\u7406\u7684\u52b1\u8d77\u306b\u3064\u3044\u3066(21aSF-4)<\/li>\n<li>\u56db\u8c37\u4f73\u7a42\u3001\u66f9\u57fa\u54f2<br \/>\nConstraints on extra U(1) models from perturbative gauge coupling unification (21aSK-13)<\/li>\n<li>\u5927\u91ce\u6176\u5b50\u3001\u66f9\u57fa\u54f2\u3001\u4ed61\u540d<br \/>\n\u30e9\u30c7\u30a3\u30aa\u30f3\u8cea\u91cf\u306b\u5bfe\u3059\u308b\u30d2\u30c3\u30b0\u30b9\u63a2\u7d22\u5b9f\u9a13\u304b\u3089\u306e\u5236\u9650 (23aSF-11)<\/li>\n<li>\u658e\u85e4\u90a3\u83dc\u3001\u4ed6<br \/>\n\u5927\u578b\u4f4e\u6e29\u91cd\u529b\u6ce2\u671b\u9060\u93e1(KAGRA)\u30d7\u30ed\u30b8\u30a7\u30af\u30c8\u306e\u73fe\u72b6 (22pSR-1)<\/li>\n<li>\u658e\u85e4\u90a3\u83dc\u3001\u83c5\u672c\u6676\u592b\u3001\u4ed6<br \/>\n\u30c7\u30c1\u30e5\u30fc\u30f3\u3092\u3057\u305f\u5e72\u6e09\u8a08\u306b\u304a\u3051\u308b\u30aa\u30d5\u30bb\u30c3\u30c8\u554f\u984c\u306e\u89e3\u6c7aIII (22pSR-11)<\/li>\n<li>\u4e8c\u968e\u5802\u745e\u5e0c\u3001\u4ed6<br \/>\n\u30b9\u30da\u30fc\u30b9\u91cd\u529b\u6ce2\u30a2\u30f3\u30c6\u30caDECIGO\u8a08\u753b(46):\u5e72\u6e09\u8a08\u30fb\u4fe1\u53f7\u51e6\u7406 (23aSR-10)<\/li>\n<li>\u4e8c\u968e\u5802\u745e\u5e0c\u3001\u4ed6<br \/>\n\u30b9\u30da\u30fc\u30b9\u91cd\u529b\u6ce2\u30a2\u30f3\u30c6\u30caDECIGO\u8a08\u753b(47):\u8a66\u9a13\u30de\u30b9\u30e2\u30b8\u30e5\u30fc\u30eb (23aSR-11)<\/li>\n<\/ol>\n<h3>\u65e5\u672c\u7269\u7406\u5b66\u4f1a\u7b2c68\u56de\u5e74\u6b21\u5927\u4f1a( \u5e83\u5cf6\u5927\u5b66\u30012013\u5e743\u670826\u65e5\uff5e29\u65e5)<\/h3>\n<ol>\n<li>\u7c73\u5c71\u4eac\u5b50\u3001\u4ed62\u540d<br \/>\nProgress in Gauge-Higgs Unification on the Lattice (26pRE-6)<\/li>\n<li>\u5927\u91ce\u6176\u5b50,\u66f9\u57fa\u54f2<br \/>\nConstratins on radion mass from search for Higgs boson at the LHC (27pRE-15)<\/li>\n<li>\u5742\u4e0b\u3042\u3044\u3001\u4ed63\u540d<br \/>\n\u7403\u72b6\u30d9\u30b7\u30af\u30eb\u306b\u5185\u5305\u3055\u308c\u305f\u30d9\u30b7\u30af\u30eb\u306e\u5f62\u72b6\u6c7a\u5b9a\u6a5f\u69cb\u306e\u89e3\u660e (28pXC-6)<\/li>\n<li>\u6a29\u85e4\u91cc\u5948,\u658e\u85e4\u90a3\u83dc\u3001\u4ed6<br \/>\n\u5927\u578b\u4f4e\u6e29\u91cd\u529b\u6ce2\u671b\u9060\u93e1(KAGRA)\u30d7\u30ed\u30b8\u30a7\u30af\u30c8\u306e\u73fe\u72b6(3) (26aBE-1)<\/li>\n<li>\u658e\u85e4\u90a3\u83dc\u3001\u4ed6<br \/>\n\u91cd\u529b\u6ce2\u691c\u51fa\u5668\u306b\u304a\u3051\u308b\u5149\u30b9\u30af\u30a4\u30fc\u30b8\u30f3\u30b0\u6280\u8853\u306e\u5fdc\u7528 (26pBE-10)<\/li>\n<li>\u6a29\u85e4\u91cc\u5948\u3001\u4ed6<br \/>\n\u30b9\u30da\u30fc\u30b9\u91cd\u529b\u6ce2\u30a2\u30f3\u30c6\u30caDECIGO\u8a08\u753b(41):DPF\u5e72\u6e09\u8a08\u30fb\u8a66\u9a13\u30de\u30b9 (27aBE-10)<\/li>\n<li>\u77e2\u8429\u91cf\u5b50\u3001\u4ed6<br \/>\n\u56db\u5143\u6570\u5909\u6570\u3092\u7528\u3044\u305f\u91cd\u529b\u7406\u8ad6 (29aBB-5)<\/li>\n<\/ol>\n","protected":false},"excerpt":{"rendered":"<p>2025\u5e74 \u65e5\u672c\u7269\u7406\u5b66\u4f1a\u7b2c80\u56de\u5e74\u6b21\u5927\u4f1a(\u5e83\u5cf6\u5927\u5b66(\u6771\u5e83\u5cf6\u30ad\u30e3\u30f3\u30d1\u30b9)\u30012025\u5e749\u670816\u65e5\u301c19\u65e5) \u80fd\u52e2\u5343\u6676, \u66fa\u57fa\u54f2, \u51fa\u5ddd\u667a\u9999\u5b50 Two Higgs doublet model with a complex si &hellip; <a href=\"https:\/\/www-p.sci.ocha.ac.jp\/phys-hep\/talks_jps.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-614","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\/614","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=614"}],"version-history":[{"count":26,"href":"https:\/\/www-p.sci.ocha.ac.jp\/phys-hep\/wp-json\/wp\/v2\/pages\/614\/revisions"}],"predecessor-version":[{"id":2652,"href":"https:\/\/www-p.sci.ocha.ac.jp\/phys-hep\/wp-json\/wp\/v2\/pages\/614\/revisions\/2652"}],"wp:attachment":[{"href":"https:\/\/www-p.sci.ocha.ac.jp\/phys-hep\/wp-json\/wp\/v2\/media?parent=614"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}