{"id":626,"date":"2016-03-22T20:55:40","date_gmt":"2016-03-22T11:55:40","guid":{"rendered":"http:\/\/www-p.sci.ocha.ac.jp\/phys-hep\/?page_id=626"},"modified":"2024-12-04T14:07:43","modified_gmt":"2024-12-04T05:07:43","slug":"%e5%9b%bd%e5%86%85%e5%a4%96%e3%81%ae%e4%bc%9a%e8%ad%b0%e3%80%81%e7%a0%94%e7%a9%b6%e4%bc%9a%e3%80%81%e3%82%bb%e3%83%9f%e3%83%8a%e3%83%bc%e7%ad%89%e3%81%a7%e3%81%ae%e8%ac%9b%e6%bc%94","status":"publish","type":"page","link":"https:\/\/www-p.sci.ocha.ac.jp\/phys-hep\/talks_ws.html","title":{"rendered":"\u56fd\u5185\u5916\u306e\u4f1a\u8b70\u3001\u7814\u7a76\u4f1a\u3001\u30bb\u30df\u30ca\u30fc\u7b49\u3067\u306e\u8b1b\u6f14"},"content":{"rendered":"

2024\u5e74<\/h4>\n
    \n
  1. \u66fa\u00a0 \u57fa\u54f2
    \n\u30d5\u30ec\u30fc\u30d0\u30fc\u7269\u7406\u306e\u57fa\u790e
    \nFlavor Physics Workshop 2024, Dec\/2-5, \u30db\u30c6\u30eb\u660e\u5c71\u8358<\/li>\n
  2. \u72ac\u5bae\u7406\u6075
    \nDark Matter Considering Temperature Evolution of Mass Due to the Electroweak Phase Transition
    \nMeeting of New Higgs Working Group, Oct. 12, Osaka University<\/li>\n
  3. \u72ac\u5bae\u7406\u6075
    \nRelic Abundance of Dark Matter with Temperature-Dependent Mass during Phase Transitions
    \nThe 4th DMNet symposium : Revealing Dark matter in the Universe with Multidisciplinary Approaches in Particle Physics and Astrophysics, 5th\u20137th Sep. 2024, IBS Science and Culture Center(Poster Session)<\/li>\n
  4. \u51fa\u5ddd\u667a\u9999\u5b50
    \nElectroweak baryogenesis in a complex singlet extension of the Standard Model
    \nFourth Mini-workshop on the Early Universe, 3rd-6th Sep. 2024, Yatsugatake Commons, Yamanashi prefecture<\/li>\n
  5. \u5c0f\u6797\u304a\u304d
    \nSearching for signatures of 2HDM with Z4 symmetry at a muon collider
    \n\u57fa\u7814\u7814\u7a76\u4f1a\u3000\u7d20\u7c92\u5b50\u7269\u7406\u5b66\u306e\u9032\u5c552024\u30012024\/8\/19-23\u3001\u4eac\u90fd\u5927\u5b66 \u57fa\u790e\u7269\u7406\u5b66\u7814\u7a76\u6240(\u30dd\u30b9\u30bf\u30fc\u767a\u8868)<\/li>\n
  6. \u72ac\u5bae\u7406\u6075
    \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
    \n\u57fa\u7814\u7814\u7a76\u4f1a\u3000\u7d20\u7c92\u5b50\u7269\u7406\u5b66\u306e\u9032\u5c552024\u30012024\/8\/19-23\u3001\u4eac\u90fd\u5927\u5b66 \u57fa\u790e\u7269\u7406\u5b66\u7814\u7a76\u6240(\u30dd\u30b9\u30bf\u30fc\u767a\u8868)<\/li>\n
  7. \u51fa\u5ddd\u667a\u9999\u5b50
    \nA complex singlet extension of the Standard Model with a singlet fermion dark matter
    \nSeminar at Kanazawa University, 5th Jul. 2024<\/li>\n
  8. \u51fa\u5ddd\u667a\u9999\u5b50
    \nElectron electric dipole moment and electroweak baryogenesis in a complex singlet extension of the Standard Model
    \n37th Regular Meeting of New Higgs Working Group, Jan. 20, Osaka University<\/li>\n<\/ol>\n

    2023\u5e74<\/h4>\n
      \n
    1. \u51fa\u5ddd\u667a\u9999\u5b50
      \n\u8907\u7d20\u30b9\u30ab\u30e9\u30fc\u62e1\u5f35\u6a21\u578b\u306b\u304a\u3051\u308b\u96fb\u5f31\u30d0\u30ea\u30aa\u30b8\u30a7\u30cd\u30b7\u30b9\u3001\u5948\u826f\u5973\u5b50\u5927\u5b66\u7d20\u7c92\u5b50\u8ad6\u7814\u7a76\u5ba4\u30bb\u30df\u30ca\u30fc\u30012023\/Dec\/22\u3001\u5948\u826f\u5973\u5b50\u5927\u5b66<\/li>\n
    2. \u5c0f\u6797\u304a\u304d
      \nSearching for signatures of 2HDM with Z4 symmetry at a muon collider
      \nKEK-NAOJ Student Workshop 2023, 2023\/12\/16-17, Online<\/li>\n
    3. \u72ac\u5bae\u7406\u6075
      \nTwo-component dark matter model with degenerate scalars
      \nKEK-NAOJ Student Workshop 2023, 2023\/12\/16-17, Online<\/li>\n
    4. \u72ac\u5bae\u7406\u6075
      \nTwo-component dark matter model with degenerate scalars
      \n\u7b2c12\u56de \u89b3\u6e2c\u7684\u5b87\u5b99\u8ad6\u30ef\u30fc\u30af\u30b7\u30e7\u30c3\u30d7, 2023\/12\/11-13, \u4f50\u8cc0\u5927\u5b66<\/li>\n
    5. \u51fa\u5ddd\u667a\u9999\u5b50
      \n\u8907\u7d20\u30b9\u30ab\u30e9\u30fc\u62e1\u5f35\u6a21\u578b\u306eCP\u4f4d\u76f8\u306b\u3088\u308b\u91cd\u529b\u6ce2\u304a\u3088\u3073\u96fb\u6c17\u53cc\u6975\u5b50\u30e2\u30fc\u30e1\u30f3\u30c8\u3078\u306e\u5bc4\u4e0e
      \n\u7b2c12\u56de \u89b3\u6e2c\u7684\u5b87\u5b99\u8ad6\u30ef\u30fc\u30af\u30b7\u30e7\u30c3\u30d7, 2023\/12\/11-13, \u4f50\u8cc0\u5927\u5b66<\/li>\n
    6. \u72ac\u5bae\u7406\u6075
      \nTwo-component dark matter model with degenerate scalars
      \nFlavor Physics workshop 2023, 2023\/11\/22\u301c25,\u00a0 \u71b1\u6d77\u30fb\u4f0a\u8c46\u5c71\u6e29\u6cc9\u30cf\u30fc\u30c8\u30d4\u30a2\u71b1\u6d77 (\u9759\u5ca1\u770c\u71b1\u6d77\u5e02\u4f0a\u8c46\u5c71)<\/li>\n
    7. \u51fa\u5ddd\u667a\u9999\u5b50
      \nElectric dipole moment and electroweak baryogenesis in a complex scalar extension of the Standard Model
      \nSeminar at Tianqin Senter in SUN YAT-SEN University (\u4e2d\u5c71\u5927\u5b66,\u5929\u7434\u4e2d\u5fc3) , 24th Nov, 2023, SUN YAT-SEN University, Guangdong, China<\/li>\n
    8. \u51fa\u5ddd\u667a\u9999\u5b50
      \nElectron electric dipole moment and electroweak baryogenesis in a complex scalar extension of the Standard Model
      \nKEK Theory Meeting on Particle Physics Phenomenology (KEK-PH2023), Nov\/7-10, KEK<\/li>\n
    9. \u51fa\u5ddd\u667a\u9999\u5b50
      \nElectric dipole moment and electroweak baryogenesis in a complex scalar extension of the Standard Model
      \nSeminar at Science and technology advanced institute (STAI), Van Lang University , 8th Sep, 2023, Van Lang University (Ho Chi Minh city, Vietnam)<\/li>\n
    10. \u9f4a\u85e4\u7dbe\u4e43
      \nSearching for signatures of 2HDM with Z4 symmetry at a muon collider
      \n\u300c\u57fa\u7814\u7814\u7a76\u4f1a\u3000\u7d20\u7c92\u5b50\u7269\u7406\u5b66\u306e\u9032\u5c552023\u300d\u30012023\/8\/28-9\/1\u3001\u4eac\u90fd\u5927\u5b66 \u57fa\u790e\u7269\u7406\u5b66\u7814\u7a76\u6240(\u30dd\u30b9\u30bf\u30fc\u767a\u8868)<\/li>\n
    11. \u51fa\u5ddd\u667a\u9999\u5b50
      \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\u3001\u300c\u57fa\u7814\u7814\u7a76\u4f1a\u3000\u7d20\u7c92\u5b50\u7269\u7406\u5b66\u306e\u9032\u5c552023\u300d\u30012023\/8\/28-9\/1\u3001\u4eac\u90fd\u5927\u5b66 \u57fa\u790e\u7269\u7406\u5b66\u7814\u7a76\u6240(\u30dd\u30b9\u30bf\u30fc\u767a\u8868)<\/li>\n
    12. \u51fa\u5ddd\u667a\u9999\u5b50
      \n\u6697\u9ed2\u7269\u8cea-\u6838\u5b50\u6563\u4e71\u6291\u5236\u30e1\u30ab\u30cb\u30ba\u30e0\u3092\u6301\u3064\u8907\u7d20\u30b7\u30f3\u30b0\u30ec\u30c3\u30c8\u30b9\u30ab\u30e9\u30fc\u62e1\u5f35\u6a21\u578b\u306e\u5206\u6790\u304a\u3088\u3073\u96fb\u5f31\u76f8\u8ee2\u79fb\u3068\u306e\u95a2\u9023
      \n\u6771\u4eac\u7406\u79d1\u5927\u5b66\u963f\u90e8\u7814\u7a76\u5ba4\u3067\u306e\u30bb\u30df\u30ca\u30fc\u30012023\/Jun\/12, \u6771\u4eac\u7406\u79d1\u5927\u5b66<\/li>\n
    13. \u51fa\u5ddd\u667a\u9999\u5b50
      \nElectric dipole moment and electroweak baryogenesis in a complex singlet extension of the Standard Model with degenerate scalars
      \nThe 6th International Workshop on Higgs as a Probe of New Physics 2023 (HPNP2023), Jun\/5-9, Osaka University<\/li>\n
    14. \u51fa\u5ddd\u667a\u9999\u5b50
      \n\u65b0\u7269\u7406\u6291\u5236\u30e1\u30ab\u30cb\u30ba\u30e0\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\u304a\u3088\u3073\u305d\u306e\u73fe\u8c61\u8ad6\u7684\u5e30\u7d50
      \n\u6a2a\u6d5c\u56fd\u7acb\u5927\u5b66\u7d20\u7c92\u5b50\u7406\u8ad6\u7814\u7a76\u5ba4\u3067\u306e\u30bb\u30df\u30ca\u30fc\u30012023\/Apr\/7, \u6a2a\u6d5c\u56fd\u7acb\u5927\u5b66<\/li>\n
    15. Gi-Chol Cho
      \nDegenerate scalar scenario in a singlet scalar extension of the Standard Model(\u62db\u5f85\u8b1b\u6f14)
      \nNITEP\u7d20\u7c92\u5b50\u73fe\u8c61\u8ad6\u7814\u7a76\u4f1a2022, Mar\/16-18, \u5927\u962a\u516c\u7acb\u5927\u5b66<\/li>\n
    16. Chikako Idegawa
      \n\u8907\u7d20\u30b7\u30f3\u30b0\u30ec\u30c3\u30c8\u30b9\u30ab\u30e9\u30fc\u62e1\u5f35\u6a21\u578b\u306b\u304a\u3051\u308b \u591a\u91cd\u81e8\u754c\u70b9\u539f\u7406\u306e\u9069\u7528\u304a\u3088\u3073\u96fb\u5f31\u76f8\u8ee2\u79fb\u3068\u306e\u95a2\u9023
      \nNITEP\u7d20\u7c92\u5b50\u73fe\u8c61\u8ad6\u7814\u7a76\u4f1a2022, Mar\/16-18, \u5927\u962a\u516c\u7acb\u5927\u5b66<\/li>\n<\/ol>\n

      2022\u5e74<\/h4>\n
        \n
      1. Momoka Sasanuki
        \nCKM anomaly and Minimal supersymmetric standard model with R-parity violation
        \n13th Ewha-JWU-Ochanomizu Joint Symposium 2022, Dec. 5-7,\u00a0 Ewha Womans University, Seoul, Korea<\/li>\n
      2. Chikako Idegawa
        \nElectroweak phase transition and Gravitational waves in a complex singlet extension of the Standard Model with degenerate scalars
        \n13th Ewha-JWU-Ochanomizu Joint Symposium 2022, Dec. 5-7,\u00a0 Ewha Womans University, Seoul, Korea<\/li>\n
      3. Chikako Idegawa
        \nCP-violating effects on gravitational waves in a complex singlet extension of the Standard Model with degenerate scalars
        \nKEK Theory Meeting on Particle Physics Phenomenology (KEK-PH2022) and International Joint Workshop on the Standard Model and beyond,
        \nNov. 30- Dec. 2, KEK<\/li>\n
      4. Chikako Idegawa
        \nCPV effects on GW in a singlet extension with mass degenerated scalars
        \n35th Regular Meeting of New Higgs Working Group, Nov. 18, Osaka University<\/li>\n
      5. \u6749\u539f\u68a8\u592e
        \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\u30dd\u30c6\u30f3\u30b7\u30e3\u30eb\u306e\u5206\u6790 (\u30dd\u30b9\u30bf\u30fc\u767a\u8868)
        \nFlavor Physics workshop 2022, 2022\/11\/7\u301c10, \u30cb\u30e5\u30fc\u516b\u666f\u5712(\u9759\u5ca1\u770c\u4f0a\u8c46\u306e\u56fd\u5e02)<\/li>\n
      6. \u51fa\u5ddd\u667a\u9999\u5b50
        \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\u96fb\u5f31\u76f8\u8ee2\u79fb\u3078\u306e\u52b9\u679c
        \nFlavor Physics workshop 2022, 2022\/11\/7\u301c10, \u30cb\u30e5\u30fc\u516b\u666f\u5712(\u9759\u5ca1\u770c\u4f0a\u8c46\u306e\u56fd\u5e02)<\/li>\n
      7. \u51fa\u5ddd\u667a\u9999\u5b50
        \n\u65b0\u7269\u7406\u6291\u5236\u30e1\u30ab\u30cb\u30ba\u30e0\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
        \n2022\/10\/20, \u6771\u4eac\u5973\u5b50\u5927\u5b66\u7406\u8ad6\u7269\u7406\u7814\u7a76\u5ba4\u30bb\u30df\u30ca\u30fc, \u6771\u4eac\u5973\u5b50\u5927\u5b66<\/li>\n
      8. \u51fa\u5ddd\u667a\u9999\u5b50
        \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\u91cd\u529b\u6ce2\u3078\u306e\u5bc4\u4e0e
        \n\u57fa\u7814\u7814\u7a76\u4f1a \u7d20\u7c92\u5b50\u7269\u7406\u5b66\u306e\u9032\u5c552022\u30012022\/8\/29-9\/2\u3001\u4eac\u90fd\u5927\u5b66\u57fa\u790e\u7269\u7406\u5b66\u7814\u7a76\u6240<\/li>\n
      9. \u51fa\u5ddd\u667a\u9999\u5b50
        \n\u7e2e\u9000\u30b9\u30ab\u30e9\u30fc\u30b7\u30ca\u30ea\u30aa\u306b\u304a\u3051\u308b\u6697\u9ed2\u7269\u8cea\u3068\u96fb\u5f31\u76f8\u8ee2\u79fb
        \n\u5ca9\u624b\u5927\u5b66\u6559\u80b2\u5b66\u90e8\u7406\u79d1\u6559\u80b2\u79d1\u7269\u7406\u5b66\u6559\u5ba4\u7b2c12\u56de\u7d20\u7c92\u5b50\u30fb\u5b87\u5b99\u30bb\u30df\u30ca\u30fc\u30012022\/5\/30 (https:\/\/physics.edu.iwate-u.ac.jp\/seminar<\/a>)<\/li>\n<\/ol>\n

        2021\u5e74<\/h4>\n
          \n
        1. \u51fa\u5ddd\u667a\u9999\u5b50
          \nEW phase transition with degenerate scalars
          \n\u65b0\u30d2\u30c3\u30b0\u30b9\u52c9\u5f37\u4f1a\u7b2c31\u56de\u5b9a\u4f8b\u4f1a\u30012021\/11\/27\u3001\u5927\u962a\u5927\u5b66<\/li>\n
        2. \u51fa\u5ddd\u667a\u9999\u5b50
          \nElectroweak phase transition\u00a0 in a complex singlet extension of the Standard Model with degenerate scalars
          \n\u4e5d\u5dde\u5927\u5b66\u7d20\u7c92\u5b50\u8ad6\u7814\u7a76\u5ba4\u30bb\u30df\u30ca\u30fc\u30012021\/11\/16, online<\/li>\n
        3. \u66fa\u00a0 \u57fa\u54f2
          \n\u5c0f\u3055\u306a\u7d20\u7c92\u5b50\u3001\u5927\u304d\u306a\u5b87\u5b99
          \n\u653e\u9001\u5927\u5b66\u8db3\u7acb\u5b66\u7fd2\u30bb\u30f3\u30bf\u30fc\u3067\u306e\u9762\u63a5\u6388\u696d\u30012021\u5e7411\u670813\u65e5\u300114\u65e5<\/li>\n
        4. \u51fa\u5ddd\u667a\u9999\u5b50
          \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
          \n\u7d20\u7c92\u5b50\u73fe\u8c61\u8ad6\u7814\u7a76\u4f1a2021, 2021\/11\/6-8, \u5927\u962a\u5e02\u7acb\u5927\u5b66<\/li>\n
        5. \u66fa\u00a0 \u57fa\u54f2
          \n\u93e1\u306e\u5411\u3053\u3046\u306e\u7269\u7406\u5b66\u301c\u529b\u3068\u5bfe\u79f0\u6027
          \n\u653e\u9001\u5927\u5b66\u6587\u4eac\u5b66\u7fd2\u30bb\u30f3\u30bf\u30fc\u3067\u306e\u9762\u63a5\u6388\u696d\u30012021\u5e7410\u670830\u65e5\u300131\u65e5<\/li>\n
        6. Chikako Idegawa
          \n1st order phase transition in CxSM with degenerate scalars
          \nSummer camp on ILC accelerator physics and detectors 2021 Sep\/21-24, Online<\/li>\n
        7. Gi-Chol Cho
          \nProbing a degenerate-scalar scenario in a pseudoscalar dark-matter model
          \nSummer camp on ILC accelerator physics and detectors 2021 Sep\/21-24, Online<\/li>\n
        8. \u51fa\u5ddd\u667a\u9999\u5b50
          \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
          \n\u57fa\u7814\u7814\u7a76\u4f1a\u300c\u7d20\u7c92\u5b50\u7269\u7406\u5b66\u306e\u9032\u5c55\u300d2021,2021\/9\/6~9\/10 , Online<\/li>\n
        9. Chikako Idegawa
          \n1st order phase transition in Complex singlet extension of the Standard Model
          \nAsia-Pacific Workshop on Particle Physics and\u00a0Cosmology 2021, Oct\/2-6, Online<\/li>\n
        10. \u66fa \u57fa\u54f2
          \n\u7269\u7406\u5b66\u306f\u3058\u3081\u306e\u4e00\u6b69
          \n\u653e\u9001\u5927\u5b66\u8db3\u7acb\u5b66\u7fd2\u30bb\u30f3\u30bf\u30fc\u3067\u306e\u9762\u63a5\u6388\u696d\u30012021\u5e745\u670815\u65e5\u300116\u65e5<\/li>\n
        11. \u66fa \u57fa\u54f2
          \n\u5c0f\u3055\u306a\u7d20\u7c92\u5b50\u3001\u5927\u304d\u306a\u5b87\u5b99
          \n\u653e\u9001\u5927\u5b66\u6587\u4eac\u5b66\u7fd2\u30bb\u30f3\u30bf\u30fc\u3067\u306e\u9762\u63a5\u6388\u696d\u30012021\u5e745\u67081\u65e5\u30012\u65e5<\/li>\n
        12. Chikako Idegawa
          \n1st order phase transition in Complex singlet extension of the Standard Model
          \nThe 5th International Workshop on \u201dHiggs as a Probe of New Physics\u201d Special Edition 2021 (HPNP2021), Mar\/25-27, Online<\/li>\n<\/ol>\n

          2020\u5e74<\/h4>\n
            \n
          1. \u66fa \u57fa\u54f2
            \n\u5c0f\u3055\u306a\u7d20\u7c92\u5b50\u3001\u5927\u304d\u306a\u5b87\u5b99
            \n\u653e\u9001\u5927\u5b66\u8db3\u7acb\u5b66\u7fd2\u30bb\u30f3\u30bf\u30fc\u3067\u306e\u9762\u63a5\u6388\u696d\u30012020\u5e7411\u670814\u65e5\u300115\u65e5<\/li>\n<\/ol>\n
              \n
            1. \u66fa \u57fa\u54f2
              \n\u93e1\u306e\u5411\u3053\u3046\u306e\u7269\u7406\u5b66\u301c\u529b\u3068\u5bfe\u79f0\u6027\u301c
              \n\u653e\u9001\u5927\u5b66\u6587\u4eac\u5b66\u7fd2\u30bb\u30f3\u30bf\u30fc\u3067\u306e\u9762\u63a5\u6388\u696d\u30012020\u5e7410\u670817\u65e5\u300118\u65e5<\/li>\n<\/ol>\n
                \n
              1. \u51fa\u5ddd\u667a\u9999\u5b50
                \n\u30b7\u30f3\u30b0\u30ec\u30c3\u30c8\u8907\u7d20\u30b9\u30ab\u30e9\u30fc\u6a21\u578b\u306b\u304a\u3051\u308b\u4e00\u6b21\u76f8\u8ee2\u79fb\u306e\u6761\u4ef6
                \n\u7d20\u7c92\u5b50\u82e5\u624b\u30aa\u30f3\u30e9\u30a4\u30f3\u7814\u7a76\u4f1a2020\u30012020\u5e748\u670826-28\u65e5<\/li>\n
              2. Kana Hayami
                \nGrand Unification of a simple extension of the Standard Model with Minimal Dark Matter and Color Octet Scalars
                \n\u57fc\u7389\u5927\u5b66\u3067\u306e\u30bb\u30df\u30ca\u30fc\u30012020\u5e746\u670819\u65e5<\/li>\n
              3. Mio Kubota
                \nHiggs Infration in metric and Palatini formalisms: Required suppression of higher dimensional operators
                \nThe 23rd New Physics Forum, Feb\/10, 2020, Ochanomizu University<\/li>\n<\/ol>\n

                2019\u5e74<\/h4>\n
                  \n
                1. Gi-Chol Cho
                  \nSuppression of DM-nucleon scattering and degenerate scalars in an extension of the SM
                  \nThe 27th regular meeting of the New Higgs Working Group (NHWG27), Dec\/13-14, 2019<\/li>\n
                2. \u66fa\u00a0 \u57fa\u54f2
                  \n\u93e1\u306e\u5411\u3053\u3046\u306e\u7269\u7406\u5b66\u301c\u529b\u3068\u5bfe\u79f0\u6027\u301c
                  \n\u653e\u9001\u5927\u5b66\u6587\u4eac\u5b66\u7fd2\u30bb\u30f3\u30bf\u30fc\u3067\u306e\u9762\u63a5\u6388\u696d\u30012019\u5e7410\u670826\u65e5\u300127\u65e5<\/li>\n
                3. \u66fa\u00a0 \u57fa\u54f2
                  \nLepton-flavor violation via four-Fermi contact interactions at e+ e- linear collider (\u5927\u962a\u5e02\u7acb\u5927\u5b66\u3067\u306e\u30bb\u30df\u30ca\u30fc\u30012019\u5e747\u670816\u65e5)<\/li>\n
                4. \u66fa\u00a0 \u57fa\u54f2
                  \n\u5c0f\u3055\u306a\u7d20\u7c92\u5b50\u3001\u5927\u304d\u306a\u5b87\u5b99
                  \n\u653e\u9001\u5927\u5b66\u8db3\u7acb\u5b66\u7fd2\u30bb\u30f3\u30bf\u30fc\u3067\u306e\u9762\u63a5\u6388\u696d\u30012019\u5e745\u670811\u65e5\u300112\u65e5<\/li>\n
                5. \u66fa\u00a0 \u57fa\u54f2
                  \n\u5c0f\u3055\u306a\u7d20\u7c92\u5b50\u3001\u5927\u304d\u306a\u5b87\u5b99
                  \n\u653e\u9001\u5927\u5b66\u6587\u4eac\u5b66\u7fd2\u30bb\u30f3\u30bf\u30fc\u3067\u306e\u9762\u63a5\u6388\u696d\u30012019\u5e744\u670820\u65e5\u300121\u65e5<\/li>\n
                6. Sachiho Abe
                  \nSuppression of dark matter-nucleon scattering in singlet Higgs extension of the SM and its signature at collider experiments
                  \n(The 4th International Workshop on “Higgs as a Probe of New Physics 2019”, Feb\/18-22, Osaka University)<\/li>\n
                7. Mio Kubota
                  \nOn the fine-tuning of Higgs inflation in metric and Palatini formulations
                  \n(The 4th International Workshop on “Higgs as a Probe of New Physics 2019”, Feb\/18-22, Osaka University)<\/li>\n
                8. Kana Hayami
                  \nCoupling unification in an extension of the minimal dark matter model and collider signatures
                  \n(The 4th International Workshop on “Higgs as a Probe of New Physics 2019”, Feb\/18-22, Osaka University)<\/li>\n
                9. Miki Yonemura
                  \nConstraints on a light scalar in a singlet Higgs extension of the SM at Belle-II
                  \n(The 4th International Workshop on “Higgs as a Probe of New Physics 2019”, Feb\/18-22, Osaka University)<\/li>\n<\/ol>\n

                  2018\u5e74<\/h4>\n
                    \n
                  1. \u66fa\u00a0 \u57fa\u54f2
                    \n\u93e1\u306e\u5411\u3053\u3046\u306e\u7269\u7406\u5b66\u301c\u529b\u3068\u5bfe\u79f0\u6027\u301c
                    \n\u653e\u9001\u5927\u5b66\u6587\u4eac\u5b66\u7fd2\u30bb\u30f3\u30bf\u30fc\u3067\u306e\u9762\u63a5\u6388\u696d\u30012018\u5e7410\u670826\u65e5\u300127\u65e5<\/li>\n
                  2. \u901f\u6c34 \u9999\u5948
                    \n\u62e1\u5f35\u3055\u308c\u305f minimal dark matter model \u306b\u304a\u3051\u308b gauge \u7d50\u5408\u5b9a\u6570\u306e\u7d71\u4e00
                    \n(\u57fa\u7814\u7814\u7a76\u4f1a\u300c\u7d20\u7c92\u5b50\u7269\u7406\u5b66\u306e\u9032\u5c55 2018\u300d\u3067\u306e\u30dd\u30b9\u30bf\u30fc\u767a\u8868\u30012018\u5e748\u67086\u65e5\u301c10\u65e5\u3001\u4eac\u90fd\u5927\u5b66\u57fa\u790e\u7269\u7406\u5b66\u7814\u7a76\u6240)<\/li>\n
                  3. \u963f\u90e8 \u7965\u6b69
                    \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
                    \n(\u57fa\u7814\u7814\u7a76\u4f1a\u300c\u7d20\u7c92\u5b50\u7269\u7406\u5b66\u306e\u9032\u5c55 2018\u300d\u3067\u306e\u30dd\u30b9\u30bf\u30fc\u767a\u8868\u30012018\u5e748\u67086\u65e5\u301c10\u65e5\u3001\u4eac\u90fd\u5927\u5b66\u57fa\u790e\u7269\u7406\u5b66\u7814\u7a76\u6240)<\/li>\n
                  4. \u7c73\u6751 \u7f8e\u7d00
                    \n\u5149\u5b50-\u967d\u5b50\u885d\u7a81\u306b\u304a\u3051\u308b\u30b9\u30d4\u30f3 1 \u7c92\u5b50\u3092\u5a92\u4ecb\u3068\u3057\u305f\u6697\u9ed2\u7269\u8cea\u306e\u63a2\u7d22\u306b\u3064\u3044\u3066
                    \n(\u57fa\u7814\u7814\u7a76\u4f1a\u300c\u7d20\u7c92\u5b50\u7269\u7406\u5b66\u306e\u9032\u5c55 2018\u300d\u3067\u306e\u30dd\u30b9\u30bf\u30fc\u767a\u8868\u30012018\u5e748\u67086\u65e5\u301c10\u65e5\u3001\u4eac\u90fd\u5927\u5b66\u57fa\u790e\u7269\u7406\u5b66\u7814\u7a76\u6240)<\/li>\n
                  5. \u66fa\u00a0 \u57fa\u54f2
                    \nLepton-flavor violation via four-Fermi contact interactions at e+e- linear collider
                    \nAsian Linear Collider Workshop 2018 (ALCW 2018)
                    \nMay\/28-June\/01, 2018, Fukuoka, Japan (URL)<\/a><\/li>\n
                  6. \u66fa\u00a0 \u57fa\u54f2
                    \nA suppression mechanism of dark matter-nucleon scattering in singlet extension of the SM (\u5de5\u5b66\u9662\u5927\u5b66\u3067\u306e\u30bb\u30df\u30ca\u30fc\u30012018\u5e744\u670818\u65e5)<\/li>\n
                  7. \u66fa\u00a0 \u57fa\u54f2
                    \n\u5c0f\u3055\u306a\u7d20\u7c92\u5b50\u3001\u5927\u304d\u306a\u5b87\u5b99
                    \n\u653e\u9001\u5927\u5b66\u6587\u4eac\u5b66\u7fd2\u30bb\u30f3\u30bf\u30fc\u3067\u306e\u9762\u63a5\u6388\u696d\u30012018\u5e744\u670814\u65e5\u300115\u65e5<\/li>\n
                  8. \u5c71\u4e0b\u516c\u5b50
                    \nSearch for Dark Neutrino via Vacuum Magnetic Birefringence Experiment
                    \n(KEK Theory Meeting on Particle Physics Phenomenology (KEK-PH2018)\u30012018\u5e742\u670813\u65e5\u301c16\u65e5)<\/li>\n<\/ol>\n

                    2017\u5e74<\/h4>\n
                      \n
                    1. \u5c71\u4e0b\u516c\u5b50
                      \nImplications for the Vacuum Magnetic Birefringence Experiment from the Parity Violating Interactions between Fermionic Dark Matter and Extra U(1) Mediator
                      \n(\u56fd\u7acb\u6e05\u83ef\u5927\u5b66\/NCTS \u3067\u306e\u30bb\u30df\u30ca\u30fc\u30012017\u5e7412\u670821\u65e5)<\/li>\n
                    2. \u5c71\u4e0b\u516c\u5b50
                      \nImplications for the Vacuum Magnetic Birefringence Experiment from the Parity Violating Interactions between Fermionic Dark Matter and Extra U(1) Mediator
                      \n(\u56fd\u7acb\u53f0\u6e7e\u5927\u5b66\u3067\u306e\u30bb\u30df\u30ca\u30fc\u30012017\u5e7412\u670818\u65e5)<\/li>\n
                    3. \u66fa\u00a0 \u57fa\u54f2
                      \nDimension, Scale and Particle Physics
                      \n(8th Ewha-JWU-Ochanomizu Joint Symposium 2017, 2017\/Dec\/12-14, Ewha University, Seoul, Korea)<\/li>\n
                    4. \u7c73\u6751\u7f8e\u7d00
                      \nSearching for signatures of the Dark Sector in Collider Experiments
                      \n(8th Ewha-JWU-Ochanomizu Joint Symposium 2017, 2017\/Dec\/12-14, Ewha University, Seoul, Korea)<\/li>\n
                    5. \u901f\u6c34\u9999\u83dc
                      \nSearch for the Possibility of Grand Unification and Higgs Inflation
                      \n(8th Ewha-JWU-Ochanomizu Joint Symposium 2017, 2017\/Dec\/12-14, Ewha University, Seoul, Korea)<\/li>\n
                    6. \u5c71\u4e0b\u516c\u5b50
                      \n\u96a0\u308c\u305fU(1)\u30b2\u30fc\u30b8\u5834\u3092\u5a92\u4ecb\u3068\u3057\u3066\u5149\u3068\u30d1\u30ea\u30c6\u30a3\u3092\u7834\u3063\u305f\u76f8\u4e92\u4f5c\u7528\u3092\u3059\u308b\u30d5\u30a7\u30eb\u30df\u30aa\u30f3\u306e4\u5149\u5b50\u6709\u52b9\u30e9\u30b0\u30e9\u30f3\u30b8\u30a2\u30f3\u3068\u771f\u7a7a\u8907\u5c48\u6298\u5b9f\u9a13\u3067\u306e\u63a2\u7d22\u306b\u3064\u3044\u3066
                      \n(\u4eac\u90fd\u7523\u696d\u5927\u5b66\u76ca\u5ddd\u587e\u3067\u306e\u30bb\u30df\u30ca\u30fc\u30012017\u5e7411\u670820\u65e5)<\/li>\n
                    7. \u5c71\u4e0b\u516c\u5b50
                      \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
                      \n(\u5927\u962a\u30ef\u30fc\u30af\u30b7\u30e7\u30c3\u30d7 2017\u300c\u5730\u4e0a\u5b9f\u9a13\u3067\u691c\u8a3c\u53ef\u80fd\u306a\u65b0\u7269\u7406\u300d\u30012017\u5e7411\u670811\u65e5\u301c13\u65e5\u3001\u5927\u962a\u5927\u5b66)<\/li>\n
                    8. \u66fa\u00a0 \u57fa\u54f2
                      \nLepton flavor violation via four-Fermi contact interactions at future lepton colliders
                      \n(\u5927\u962a\u30ef\u30fc\u30af\u30b7\u30e7\u30c3\u30d7 2017\u300c\u5730\u4e0a\u5b9f\u9a13\u3067\u691c\u8a3c\u53ef\u80fd\u306a\u65b0\u7269\u7406\u300d\u30012017\u5e7411\u670811\u65e5\u301c13\u65e5\u3001\u5927\u962a\u5927\u5b66)<\/li>\n
                    9. \u66fa\u00a0 \u57fa\u54f2
                      \nLepton flavor violation via four-Fermi contact interactions at future lepton colliders
                      \n(The 7th KIAS workshop on particle physics and cosomology, The 2nd KEK-NCTS-KIAS joint workshop on particle physics phenomenology\u3067\u306e\u8b1b\u6f14\u30012017\u5e7411\u67086\u65e5\u301c10\u65e5\u3001\u30bd\u30a6\u30eb(\u97d3\u56fd))<\/li>\n
                    10. \u66fa\u00a0 \u57fa\u54f2
                      \n\u6a19\u6e96\u7406\u8ad6\u5165\u9580(\u524d\u7de8\u30fb\u5f8c\u7de8)
                      \n(Flavor Physics Workshop 2017\u3067\u306e\u8b1b\u6f14\u30012017\u5e7410\u670830\u65e5\u301c11\u67082\u65e5\u3001\u4e09\u6d66\u6d77\u5cb8)<\/li>\n
                    11. \u5c71\u4e0b\u516c\u5b50
                      \nImplications for the Vacuum Magnetic Birefringence Experiment from the Parity Violating Interactions between Fermionic Dark Matter and Extra U(1) Mediator
                      \n(IBS-CTPU(\u97d3\u56fd)\u3067\u306e\u30bb\u30df\u30ca\u30fc\u30012017\u5e749\u670828\u65e5)<\/li>\n
                    12. \u5c71\u4e0b\u516c\u5b50
                      \nImplications for the Vacuum Magnetic Birefringence Experiment from the Parity Violating Interactions between Fermionic Dark Matter and Extra U(1) Mediator
                      \n(KIAS(\u97d3\u56fd)\u3067\u306e\u30bb\u30df\u30ca\u30fc\u30012017\u5e749\u670825\u65e5)<\/li>\n
                    13. \u5c71\u4e0b\u516c\u5b50
                      \nImplications for the Vacuum Magnetic Birefringence Experiment from the Parity Violating Interactions between Fermionic Dark Matter and Extra U(1) Mediator
                      \n(APCTP(\u97d3\u56fd)\u3067\u306e\u30bb\u30df\u30ca\u30fc\u30012017\u5e749\u670822\u65e5)<\/li>\n
                    14. \u5c71\u4e0b\u516c\u5b50
                      \nImplications for the Vacuum Magnetic Birefringence Experiment from
                      \nthe Parity Violating Interactions between Fermionic Dark Matter and Extra U(1) Mediator
                      \n(\u30dd\u30b9\u30bf\u30fc\u767a\u8868\u3001\u57fa\u7814\u7814\u7a76\u4f1a\u300c\u7d20\u7c92\u5b50\u7269\u7406\u5b66\u306e\u9032\u5c552017\u300d\u3001\u4eac\u90fd\u5927\u5b66\u57fa\u790e\u7269\u7406\u5b66\u7814\u7a76\u6240\u30012017\u5e747\u670831\u65e5\u301c8\u67084\u65e5)<\/li>\n
                    15. \u5c71\u4e0b\u516c\u5b50
                      \nImplications for the Vacuum Magnetic Birefringence Experiment from the Parity Violating Interactions between Fermionic Dark Matter and Extra U(1) Mediator
                      \n(\u53e3\u982d\u767a\u8868\u3001”DSU 2017 (The 13th International Workshop on the Dark Side of the Universe\u3001KIAS\u3001\u97d3\u56fd\u30012017\u5e747\u670810\u65e5\u301c7\u670814\u65e5)”<\/li>\n
                    16. \u5c71\u4e0b\u516c\u5b50
                      \nImplications for the Vacuum Magnetic Birefringence Experiment from the Parity Violating Interactions between Fermionic Dark Matter and Extra U(1) Mediator
                      \n(\u57fc\u7389\u5927\u5b66\u3067\u306e\u30bb\u30df\u30ca\u30fc\u30012017\u5e747\u67087\u65e5)<\/li>\n
                    17. \u5c71\u4e0b\u516c\u5b50
                      \nSimplified dark matter models with a spin-2 mediator at the LHC
                      \n(\u53e3\u982d\u767a\u8868\u3001”LHCTheory ERC meeting”\u3001\u30eb\u30fc\u30f4\u30a1\u30f3\u30fb\u30ab\u30c8\u30ea\u30c3\u30af\u5927\u5b66\u3001\u30d9\u30eb\u30ae\u30fc\u3001\u00a02017\u5e743\u670822\u65e5\u301c3\u670824\u65e5)<\/li>\n<\/ol>\n

                      2016\u5e74<\/h4>\n
                        \n
                      1. \u4e0b\u83ef\u5948\u5b50
                        \nSearch for charged lepton flavor violation at the ILC
                        \n(\u53e3\u982d\u767a\u8868\u30fb\u30dd\u30b9\u30bf\u30fc\u767a\u8868\u3001\u201dEwha-JWU-Ocha Joint Symposium 2016\u201d\u3001\u68a8\u82b1\u5973\u5b50\u5927\u30012016\u5e7412\u67086\u65e5\u301c8\u65e5)<\/li>\n
                      2. \u66fa\u00a0 \u57fa\u54f2
                        \nPerturbative unification of gauge couplings in supersymmetric E6 models
                        \n(\u30dd\u30b9\u30bf\u30fc\u767a\u8868\u3001\u201dEwha-JWU-Ocha Joint Symposium 2016\u201d\u3001\u68a8\u82b1\u5973\u5b50\u5927\u5b66\u3001\u97d3\u56fd\u30012016\u5e7412\u67086\u65e5\u301c8\u65e5)<\/li>\n
                      3. \u5c71\u4e0b\u516c\u5b50
                        \nDark matter constraints on simplified models with s-channel spin-2 mediators (AEPSHEP2016\u3067\u306e\u30dd\u30b9\u30bf\u30fc\u767a\u8868\u30012016\u5e7410\u670812\u65e5\u301c25\u65e5\u3001\u5317\u4eac)<\/li>\n
                      4. \u5c71\u4e0b\u516c\u5b50
                        \nRatchet Baryogenesis with an Analogy to the Forced Pendulum(AEPSHEP2016\u3067\u306e\u30dd\u30b9\u30bf\u30fc\u767a\u8868\u30012016\u5e7410\u670812\u65e5\u301c25\u65e5\u3001\u5317\u4eac)<\/li>\n
                      5. \u5c71\u4e0b\u3000\u516c\u5b50
                        \nConstruction of a Model of Monopolium and its Search via Multi-Photon Channels at LHC(\u57fa\u7814\u7814\u7a76\u4f1a\u300c\u7d20\u7c92\u5b50\u7269\u7406\u5b66\u306e\u9032\u5c552016\u300d\u3067\u306e\u30dd\u30b9\u30bf\u30fc\u767a\u8868\u30012016\u5e749\u67085\u65e5\u301c9\u65e5)<\/li>\n
                      6. \u5c71\u4e0b\u3000\u516c\u5b50
                        \nSearch for Kaluza-Klein gravitons in extra dimension models via forward detectors at the LHC (Laboratory of Subatomic Physics & Cosmology Grenoble\u3067\u306e\u30bb\u30df\u30ca\u30fc\u30012016\u5e743\u670811\u65e5)<\/li>\n<\/ol>\n

                        2015\u5e74<\/h4>\n
                          \n
                        1. \u5c71\u4e0b\u3000\u516c\u5b50
                          \nRatchet Baryogenesis during reheating
                          \n(\u30d0\u30fc\u30b8\u30cb\u30a2\u5de5\u79d1\u5927\u5b66\u3067\u306e\u30bb\u30df\u30ca\u30fc\u30012015\u5e7410\u670821\u65e5)<\/li>\n
                        2. \u5c71\u4e0b\u3000\u516c\u5b50
                          \nRatchet Baryogenesis during reheating
                          \n(\u53e3\u982d\u767a\u8868\u3001”SUSY 2015″, 2015\u5e748\u670823-29\u65e5)<\/li>\n
                        3. \u66f9\u3000\u57fa\u54f2
                          \nGauge coupling unification in supersymmetric E6 models
                          \n(\u5c71\u5f62\u5927\u5b66\u3067\u306e\u30bb\u30df\u30ca\u30fc\u30012015\u5e748\u670827\u65e5)<\/li>\n
                        4. \u77e2\u8429\u3000\u91cf\u5b50
                          \nEnergy-momentum current of gravity in Finsler-Kawaguchi Lagrangian formulation
                          \n(\u53e3\u982d\u767a\u8868\u3001”Gravity and Beyond (GRaB100)”, National Taiwan University, July\/6-10, 2015)<\/li>\n
                        5. \u77e2\u8429\u3000\u91cf\u5b50
                          \nFinite-temperature behavior of an impurity in the spin-1\/2 XXZ chain
                          \n(\u53e3\u982d\u767a\u8868\u3001”Integrable Systems and Quantum symmetries (ISQS-23)”
                          \n\u30c1\u30a7\u30b3, 6\u670823\u65e5\u301c27\u65e5)<\/li>\n
                        6. \u9f4b\u85e4\u3000\u9ebb\u7531\u7f8e
                          \nHydrodynamics on non-commutative space
                          \n(\u53e3\u982d\u767a\u8868\u3001”Gravity and Beyond (GRaB100)”, National Taiwan University, July\/6-10, 2015)<\/li>\n
                        7. \u5927\u91ce\u3000\u6176\u5b50
                          \nRadion in Randall-Sundrum model at the LHC and photon collider
                          \n(\u5927\u962a\u5e02\u7acb\u5927\u5b66\u3067\u306e\u30bb\u30df\u30ca\u30fc\u30012015\u5e747\u67087\u65e5)<\/li>\n
                        8. \u5c71\u4e0b\u3000\u516c\u5b50
                          \nSearch for Kaluza-Klein gravitons in extra dimension models via forward detectors at the LHC
                          \n(\u5bcc\u5c71\u5927\u5b66\u3067\u306e\u30bb\u30df\u30ca\u30fc\u30012015\u5e745\u670829\u65e5)<\/li>\n
                        9. \u66f9 \u57fa\u54f2
                          \nGauge coupling unification in supersymmetric E6 models
                          \n(KIAS(\u97d3\u56fd\u9ad8\u7b49\u79d1\u5b66\u9662)\u3067\u306e\u30bb\u30df\u30ca\u30fc\u3001\u30bd\u30a6\u30eb\u3001\u97d3\u56fd\u30012015\u5e74 4\u670827\u65e5)<\/li>\n
                        10. \u66f9 \u57fa\u54f2
                          \nSearching for signatures of extra dimensions at the LHC
                          \n(\u62db\u5f85\u8b1b\u6f14\u3001”JPS-KPS Joint Symposium: Present and Future of Collider Physics”, Daejeon Convention Center, Korea, Apr\/24\/2015)<\/li>\n
                        11. \u99ac\u5872\u3000\u4e00\u6674
                          \nDescriptions of inflation in scalar field theories, perfect fluid, and F(R) gravity
                          \n(\u30dd\u30b9\u30bf\u30fc\u767a\u8868\u3001”Sakata Memorial KMI Workshop on “Origin of Mass and Strong Coupling Gauge Theories” (SCGT15), Sakata-Hirata Hall, Nagoya University, Nagoya, Japan”\u30012015\u5e743\u67083-6\u65e5)<\/li>\n
                        12. \u99ac\u5872\u3000\u4e00\u6674
                          \nLarge-scale magnetic fields, non-Gaussianity, and gravitational waves from inflation
                          \n(\u53e3\u982d\u767a\u8868\u3001”Sakata Memorial KMI Workshop on “Origin of Mass and Strong Coupling Gauge Theories” (SCGT15), Sakata-Hirata Hall, Nagoya University, Nagoya, Japan”\u30012015\u5e743\u67083-6\u65e5)<\/li>\n
                        13. \u99ac\u5872\u3000\u4e00\u6674
                          \nCosmological Issues in F(T) Gravity Theory
                          \n(\u62db\u5f85\u8b1b\u6f14\u3001”The International Conference on Relativistic Astrophysics, Department of Mathematics, University of the Punjab, Lahore, Pakistan”\u3001 2015\u5e742\u670810-14\u65e5)<\/li>\n
                        14. \u99ac\u5872\u3000\u4e00\u6674
                          \nLarge-scale magnetic fields, non-Gaussianity, and primordial gravitational waves from inflation
                          \n(\u53e3\u982d\u767a\u8868\u3001”KEK-CPWS The 4th UTQuest Workshop, KEK Theory
                          \nCenter Cosmophysics Group Workshop, B-mode Cosmology, -Intermediate Scale Inflation and Hidden Sector -, KEK, Tsukuba, Japan”\u30012015\u5e742\u670819-21\u65e5)<\/li>\n<\/ol>\n

                          2014\u5e74<\/h4>\n
                            \n
                          1. \u5927\u91ce\u3000\u6176\u5b50
                            \nRadion in Randall-Sundrum model at the LHC and photon collider
                            \n(\u5cf6\u6839\u5927\u5b66\u3067\u306e\u30bb\u30df\u30ca\u30fc\u30012014\u5e7412\u670822\u65e5)<\/li>\n
                          2. \u99ac\u5872\u3000\u4e00\u6674
                            \nInflationary cosmology in $R^2$ gravity with quantum corrections
                            \n(\u53e3\u982d\u767a\u8868\u3001”The 24th Workshop on General Relativity and Gravitation
                            \n(JGRG24),
                            \nKavli IPMU, the University of Tokyo”\u30012014\u5e7411\u670810-14\u65e5)<\/li>\n
                          3. \u99ac\u5872\u3000\u4e00\u6674
                            \nInflationary models and the recent observations
                            \n(\u62db\u5f85\u8b1b\u6f14\u3001”2nd International Workshop on Particle Physics and Cosmology after Higgs and Planck, National Center for Theoretical Sciences, Hsinchu and
                            \nFo-Guang-Shan, Kaohsiung, Taiwan”\u30012014\u5e7410\u67088-11\u65e5)<\/li>\n
                          4. \u99ac\u5872\u3000\u4e00\u6674
                            \nInflationary models and recent cosmological observations
                            \n(\u62db\u5f85\u8b1b\u6f14\u3001”Workshop on COSMOLOGY AND THE QUANTUM VACUUM
                            \nCentro de Ciencias de Benasque Pedro Pascual, Av. Francia 17, Benasque 22440, Spain”\u30012014\u5e749\u67087-13\u65e5)<\/li>\n
                          5. \u5c71\u4e0b\u3000\u516c\u5b50
                            \nSearch for extra dimensions via forward detectors at the LHC
                            \n(SUSY2014, Manchester, England, July 21-26)<\/li>\n
                          6. \u99ac\u5872\u3000\u4e00\u6674
                            \nLarge-scale magnetic fields, non-Gaussianity, and primordial gravitational waves in inflationary cosmology
                            \n(\u62db\u5f85\u8b1b\u6f14\u3001”\u30b8\u30e7\u30a4\u30f3\u30c8\u30bb\u30df\u30ca\u30fc(\u65e9\u7a32\u7530\u5927\u5b66)”\u30012014\u5e747\u670814\u65e5)<\/li>\n
                          7. \u66f9\u3000\u57fa\u54f2
                            \nCollider phenomenology in warped extra dimension models
                            \n(\u62db\u5f85\u8b1b\u6f14\u3001”\u677e\u6c5f\u73fe\u8c61\u8ad6\u7814\u7a76\u4f1a2014″\u30012014\u5e742\u67088-9\u65e5)<\/li>\n<\/ol>\n

                            2013\u5e74<\/h4>\n
                              \n
                            1. \u5927\u91ce\u6176\u5b50
                              \nRadion in Randall-Sundrum model at the LHC and photon collider
                              \n(\u30dd\u30b9\u30bf\u30fc\u767a\u8868\u3001\u56fd\u969b\u4f1a\u8b70”KMI International Symposium 2013 – on Quest for the origin of particles and the Universe”\u30012013\u5e7412\u670811-13\u65e5)<\/li>\n
                            2. \u66f9\u3000\u57fa\u54f2
                              \n\u7d20\u7c92\u5b50\u6a19\u6e96\u6a21\u578b\u306e\u7cbe\u5bc6\u691c\u8a3c\u3068\u30c6\u30e9\u30b9\u30b1\u30fc\u30eb\u7269\u7406
                              \n(\u96c6\u4e2d\u8b1b\u7fa9\u3001\u9996\u90fd\u5927\u5b66\u6771\u4eac\u30012013\u5e7412\u67089, 10\u65e5)<\/li>\n
                            3. \u5742\u4e0b\u3042\u3044
                              \nCompartmentalization by confinement in multi-lamellar vesicles
                              \n(\u30dd\u30b9\u30bf\u30fc\u767a\u8868\u3001\u56fd\u969b\u4f1a\u8b70”International Soft Matter Conference 2013″\u30012013\u5e749\u670815-19\u65e5\u3001\u30ed\u30fc\u30de)<\/li>\n
                            4. \u5927\u91ce\u6176\u5b50
                              \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
                              \n(\u30dd\u30b9\u30bf\u30fc\u767a\u8868\u3001\u57fa\u7814\u7814\u7a76\u4f1a\u300c\u7d20\u7c92\u5b50\u7269\u7406\u5b66\u306e\u9032\u5c552013\u300d2013\u5e748\u67085\u65e5-9\u65e5\u3001\u4eac\u90fd\u5927\u5b66)<\/li>\n
                            5. \u77e2\u8429\u91cf\u5b50
                              \nA Solvable XXZ Model with an Impurity
                              \n(\u30dd\u30b9\u30bf\u30fc\u767a\u8868\u3001\u56fd\u969b\u4f1a\u8b70”Mathematical Statistical Physics”\u30012013\u5e747\u670829\u65e5-8\u67083\u65e5\u3001\u4eac\u5927\u57fa\u7814)<\/li>\n
                            6. \u5927\u91ce\u6176\u5b50
                              \nConstraints on radion in a warped extra dimension model from Higgs boson searches at the LHC
                              \n(\u300c\u52a0\u901f\u5668\u30fb\u7269\u7406\u5408\u540c ILC \u590f\u306e\u5408\u5bbf2013\u300d\u30012013\u5e747\u670820\u65e5-23\u65e5\u3001\u5bcc\u5c71)<\/li>\n
                            7. \u5927\u91ce\u6176\u5b50
                              \nConstraints on radion in a warped extra dimension model from Higgs boson searches at the LHC
                              \n(\u795e\u6238\u5927\u5b66\u3067\u306e\u30bb\u30df\u30ca\u30fc\u30012013\u5e746\u670819\u65e5)<\/li>\n
                            8. \u5927\u91ce\u6176\u5b50
                              \nConstraints on radion mass from search for Higgs boson at the LHC
                              \n(\u5317\u91cc\u5927\u5b66\u3067\u306e\u30bb\u30df\u30ca\u30fc\u30012013\u5e745\u670831\u65e5)<\/li>\n
                            9. \u66f9\u3000\u57fa\u54f2
                              \n\u7cbe\u5bc6\u6e2c\u5b9a\u304b\u3089\u30c6\u30e9\u30b9\u30b1\u30fc\u30eb\u3078
                              \n(\u65b0\u5b66\u8853\u9818\u57df\u300c\u5148\u7aef\u52a0\u901f\u5668LHC\u304c\u5207\u308a\u62d3\u304f\u30c6\u30e9\u30b9\u30b1\u30fc\u30eb\u306e\u7d20\u7c92\u5b50\u7269\u7406\u5b66\u300d\u7814\u7a76\u4f1a\u3001\u540d\u53e4\u5c4b\u5927\u5b66\u30012013\u5e745\u670823\u65e5\u301c25\u65e5)<\/li>\n
                            10. \u77e2\u8429\u91cf\u5b50
                              \n\u4e0d\u7d14\u7269\u306e\u3042\u308b\u53ef\u89e3 XXZ \u9396\u306b\u3064\u3044\u3066
                              \n(\u7acb\u6559\u5927\u5b66\u3067\u306e\u30bb\u30df\u30ca\u30fc\u30012013\u5e745\u670814\u65e5)<\/li>\n
                            11. \u66f9\u3000\u57fa\u54f2
                              \n\u96fb\u5f31\u7cbe\u5bc6\u6e2c\u5b9a\u306e\u7269\u7406
                              \n(\u672d\u5e4c\u30a6\u30a3\u30f3\u30bf\u30fc\u30b9\u30af\u30fc\u30eb2013\u3067\u306e\u8b1b\u7fa9\u3001\u5317\u6d77\u9053\u5927\u5b66\u30012013\u5e742\u670813-15\u65e5)<\/li>\n<\/ol>\n

                              2012\u5e74<\/h4>\n
                                \n
                              1. \u9577\u5ca1\u53cb\u7f8e
                                \nSequential melting of quarkonia in quark-gluon fluid at RHIC and LHC
                                \n(The 4th Asian Triangle Heavy Ion Conference, Pusan, Korea, Nov.14-17)<\/li>\n
                              2. \u5927\u91ce\u6176\u5b50
                                \nProduction and decay of a heavy radion in Rundall-Sundrum model at the LHC
                                \n(Hadron Collider Physics Symposium 2012, Kyoto, Nov. 12-16)<\/li>\n
                              3. \u677e\u5c3e\u5149
                                \nConstraints on R-parity violating couplings from B \u2192 D^(*)tau nu decays
                                \n(B workshop 2012, \u5ca9\u624b\u770c\u82b1\u5dfb\u5e02\u30012012\u5e7411\u67085-8\u65e5)<\/li>\n
                              4. \u5c0f\u4fe3\u5df4\u82b3
                                \nB\u2192K\u03c0 decay in R-parity violating supersymmetric standard model
                                \n(B workshop 2012, \u5ca9\u624b\u770c\u82b1\u5dfb\u5e02\u30012012\u5e7411\u67085-8\u65e5)<\/li>\n
                              5. \u7c73\u5c71\u4eac\u5b50
                                \nProgress in Gauge-Higgs Unification on the Lattice
                                \n(The STRONGnet 2012, Madrid, Spain, Oct.15-19)<\/li>\n
                              6. \u677e\u5c3e\u5149
                                \nConstraints on R-parity violating interactions in MSSM from leptonic decays of pseudoscalar mesons
                                \n(\u7b2c18\u56de \u6771\u4eac\u5927\u5b66\u7d20\u7c92\u5b50\u7269\u7406\u56fd\u969b\u7814\u7a76\u30bb\u30f3\u30bf\u30fc\u30b7\u30f3\u30dd\u30b8\u30a6\u30e0,\u9577\u91ce,2012\u5e742\u6708)<\/li>\n
                              7. Gi-Chol Cho
                                \nThe MSSM confronts the precision electroweak data and the muon g-2
                                \nseminar at Czech Technical University at Prague, Feb.21.2012<\/li>\n<\/ol>\n","protected":false},"excerpt":{"rendered":"

                                2024\u5e74 \u66fa\u00a0 \u57fa\u54f2 \u30d5\u30ec\u30fc\u30d0\u30fc\u7269\u7406\u306e\u57fa\u790e Flavor Physics Workshop 2024, Dec\/2-5, \u30db\u30c6\u30eb\u660e\u5c71\u8358 \u72ac\u5bae\u7406\u6075 Dark Matter Considering Temperature … \u7d9a\u304d\u3092\u8aad\u3080 →<\/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-626","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\/626","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=626"}],"version-history":[{"count":73,"href":"https:\/\/www-p.sci.ocha.ac.jp\/phys-hep\/wp-json\/wp\/v2\/pages\/626\/revisions"}],"predecessor-version":[{"id":2571,"href":"https:\/\/www-p.sci.ocha.ac.jp\/phys-hep\/wp-json\/wp\/v2\/pages\/626\/revisions\/2571"}],"wp:attachment":[{"href":"https:\/\/www-p.sci.ocha.ac.jp\/phys-hep\/wp-json\/wp\/v2\/media?parent=626"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}