{"id":2046,"date":"2022-02-10T12:00:57","date_gmt":"2022-02-10T03:00:57","guid":{"rendered":"http:\/\/www-p.sci.ocha.ac.jp\/phys-hep\/?page_id=2046"},"modified":"2026-04-13T17:01:41","modified_gmt":"2026-04-13T08:01:41","slug":"%e4%bf%ae%e5%a3%ab%e3%83%bb%e5%8d%9a%e5%a3%ab%e8%ab%96%e6%96%87%e3%83%aa%e3%82%b9%e3%83%882022%e5%b9%b43%e6%9c%88","status":"publish","type":"page","link":"https:\/\/www-p.sci.ocha.ac.jp\/phys-hep\/thesis.html","title":{"rendered":"\u4fee\u58eb\u30fb\u535a\u58eb\u8ad6\u6587\u30ea\u30b9\u30c8"},"content":{"rendered":"\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n
\n
R06\/2024<\/span><\/div>\n<\/td>\n<\/tr>\n
\u4fee\u58eb<\/td>\n\u80fd\u52e2 \u5343\u6676<\/td>\nTwo Higgs doublet model with a complex singlet scalar\u306b\u5bfe\u3059\u308b\u591a\u91cd\u81e8\u754c\u70b9\u539f\u7406\u306e\u9069\u7528\u53ef\u80fd\u6027\u306b\u3064\u3044\u3066<\/td>\n<\/tr>\n
\n
R06\/2024<\/span><\/div>\n<\/td>\n<\/tr>\n
\u4fee\u58eb<\/td>\n\u5c0f\u6797 \u304a\u304d<\/td>\n\u30df\u30e5\u30fc\u30aa\u30f3\u30b3\u30e9\u30a4\u30bf\u3099\u30fc\u306b\u304a\u3051\u308bdoubly-charged lepton\u306e\u63a2\u7d22\u53ef\u80fd\u6027<\/td>\n<\/tr>\n
\u4fee\u58eb<\/td>\n\u9f4a\u85e4 \u7dbe\u4e43<\/td>\nSearching for signatures of 2HDM with Z4 symmetry at a muon collider<\/td>\n<\/tr>\n
\n
R05\/2023<\/span><\/div>\n<\/td>\n<\/tr>\n
\u535a\u58eb<\/td>\n\u51fa\u5ddd \u667a\u9999\u5b50<\/td>\nElectroweak baryogenesis in a complex singlet extension of the Standard Model with degenerate scalars<\/td>\n<\/tr>\n
\u4fee\u58eb<\/td>\n\u5927\u9688 \u5f69\u83dc<\/td>\n\u62e1\u5f35\u3055\u308c\u305f\u30d2\u30c3\u30b0\u30b9\u30fb\u30bb\u30af\u30bf\u30fc\u3092\u6301\u3064\u7d20\u7c92\u5b50\u6a21\u578b\u306b\u304a\u3051\u308b\u6697\u9ed2\u7269\u8cea-\u6838\u5b50\u6563\u4e71\u306e\u6291\u5236\u6a5f\u69cb\u306e\u5206\u6790<\/td>\n<\/tr>\n
\u4fee\u58eb<\/td>\n\u7b39\u8cab \u767e\u82b1<\/td>\nAsymmetric Dark Matter\u6a21\u578b\u306b\u304a\u3051\u308b\u8d64\u5916\u56fa\u5b9a\u70b9\u3068\u305d\u306e\u73fe\u8c61\u8ad6\u7684\u5e30\u7d50\u306e\u7814\u7a76<\/td>\n<\/tr>\n
\n
R04\/2022<\/span><\/div>\n<\/td>\n<\/tr>\n
\u4fee\u58eb<\/td>\n\u72ac\u5bae \u7406\u6075<\/td>\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<\/td>\n<\/tr>\n
\u4fee\u58eb<\/td>\n\u6749\u539f \u68a8\u592e<\/td>\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<\/td>\n<\/tr>\n
\u4fee\u58eb<\/td>\n\u5824 \u60a0\u7a00<\/td>\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<\/td>\n<\/tr>\n
\n
R03\/2021<\/span><\/div>\n<\/td>\n<\/tr>\n
\u4fee\u58eb<\/td>\n\u65b0\u4e95 \u5e78<\/td>\n\u30a4\u30f3\u30d5\u30ec\u30fc\u30b7\u30e7\u30f3\u5b87\u5b99\u306b\u304a\u3051\u308b\u30d5\u30a7\u30eb\u30df\u30aa\u30f3\u5834\u306e\u9577\u8ddd\u96e2\u76f8\u95a2<\/td>\n<\/tr>\n
\u4fee\u58eb<\/td>\n\u4e95\u4e0a \u78a7<\/td>\n\u6697\u9ed2\u7269\u8cea\u3068\u3057\u3066\u306e\u30a2\u30af\u30b7\u30aa\u30f3\u306b\u95a2\u3059\u308b\u7814\u7a76<\/td>\n<\/tr>\n
\u4fee\u58eb<\/td>\n\u6e21\u9089 \u590f\u5948<\/td>\n\u5927\u7d71\u4e00\u7406\u8ad6\u306b\u304a\u3051\u308b\u967d\u5b50\u5d29\u58ca\u6291\u5236\u6a5f\u69cb<\/td>\n<\/tr>\n
\u535a\u58eb<\/td>\n\u4e45\u4fdd\u7530 \u7f8e\u7dd2<\/td>\n\u9ad8\u6b21\u5143\u6f14\u7b97\u5b50\u3092\u6301\u3064\u30d1\u30e9\u30c6\u30a3\u30cb\u5f62\u5f0f\u306b\u304a\u3051\u308b\u30d2\u30c3\u30b0\u30b9\u30a4\u30f3\u30d5\u30ec\u30fc\u30b7\u30e7\u30f3\u306e\u7814\u7a76<\/td>\n<\/tr>\n
\u535a\u58eb<\/td>\n\u901f\u6c34 \u9999\u5948<\/td>\n\u6700\u5c0f\u6697\u9ed2\u7269\u8cea\u6a21\u578b\u306b\u57fa\u3064\u3099\u304f\u5927\u7d71\u4e00\u7406\u8ad6\u306e\u69cb\u7bc9\u3068\u691c\u8a3c\u53ef\u80fd\u6027<\/td>\n<\/tr>\n
\u535a\u58eb<\/td>\n\u7c73\u6751 \u7f8e\u7d00<\/td>\n\u30d9\u30af\u30c8\u30eb\u578b\u5a92\u4ecb\u7c92\u5b50\u6a21\u578b\u306b\u3088\u308b\u6697\u9ed2\u7269\u8cea\u63a2\u7d22\u306e\u7814\u7a76<\/td>\n<\/tr>\n
\n
R02\/2020<\/span><\/div>\n<\/td>\n<\/tr>\n
\u4fee\u58eb<\/td>\n\u51fa\u5ddd \u667a\u9999\u5b50<\/td>\n1st order phase transition in Complex singlet extension of the Standard Model<\/td>\n<\/tr>\n
\u4fee\u58eb<\/td>\n\u9060\u85e4\u3000\u3081\u3050\u307f<\/td>\n5 \u6b21\u5143\u53cd\u30c9\u30fb\u30b8\u30c3\u30bf\u30fc\u6642\u7a7a\u306b\u57cb\u3081\u8fbc\u307e\u308c\u305f4 \u6b21\u5143\u30c9\u30fb\u30b8\u30c3\u30bf\u30fc\u6642\u7a7a\u306e\u53ef\u80fd\u6027<\/td>\n<\/tr>\n
\n
R01\/2019<\/span><\/div>\n<\/td>\n<\/tr>\n
\u4fee\u58eb<\/td>\n\u65e5\u8272 \u53f2\u5948<\/td>\nA scalar particle in a complex scalar extension of the Standard Model<\/td>\n<\/tr>\n
\u4fee\u58eb<\/td>\n\u6a3d\u5c4b \u767e\u512a<\/td>\nHiggs sector\u306eCP\u5bfe\u79f0\u6027\u3068custodial\u5bfe\u79f0\u6027\u306e\u95a2\u4fc2\u306b\u3064\u3044\u3066<\/td>\n<\/tr>\n
\n
H30\/2018<\/span><\/div>\n<\/td>\n<\/tr>\n
\u4fee\u58eb<\/td>\n\u963f\u90e8 \u7965\u6b69<\/td>\nA scalar particle in a complex scalar extension of the Standard Model<\/td>\n<\/tr>\n
\u4fee\u58eb<\/td>\n\u4e8c\u74f6 \u68a2\u9999<\/td>\nFIMP Dark Matter \u3068Clockwork Mechanism \u306b\u3064\u3044\u3066<\/td>\n<\/tr>\n
\u4fee\u58eb<\/td>\n\u901f\u6c34 \u9999\u5948<\/td>\nMinimal Dark Matter \u6a21\u578b\u3068SO(10)\u5927\u7d71\u4e00\u7406\u8ad6<\/td>\n<\/tr>\n
\n
H29\/2017<\/span><\/div>\n<\/td>\n<\/tr>\n
\u535a\u58eb<\/td>\n\u5c71\u4e0b \u516c\u5b50<\/td>\n\u30ab\u30eb\u30fc\u30c4\u30a1=\u30af\u30e9\u30a4\u30f3\u30fb\u30b0\u30e9\u30d3\u30c8\u30f3\u306e\u73fe\u8c61\u8ad6\u7684\u7814\u7a76<\/td>\n<\/tr>\n
\u4fee\u58eb<\/td>\n\u4e45\u4fdd\u7530 \u7f8e\u7dd2<\/td>\nMinimal Dark Matter\u306b\u3064\u3044\u3066<\/td>\n<\/tr>\n
\u4fee\u58eb<\/td>\n\u8d8a\u91ce \u8309\u4f9d\u7f85<\/td>\nLHC\u3067\u306e\u5149\u5b50\u30fb\u967d\u5b50\u885d\u7a81\u306b\u3088\u308b\u30c0\u30fc\u30af\u30d5\u30a9\u30c8\u30f3\u306e\u751f\u6210\u5d29\u58ca\u306e\u7814\u7a76<\/td>\n<\/tr>\n
\u4fee\u58eb<\/td>\n\u798f\u7530 \u88d5\u9999<\/td>\n\u30ec\u30d7\u30c8\u30f3\u30fb\u30d5\u30ec\u30fc\u30d0\u30fc\u3092\u7834\u308b4\u4f53\u30d5\u30a7\u30eb\u30df\u76f8\u4e92\u4f5c\u7528\u306e\u7814\u7a76<\/td>\n<\/tr>\n
\u4fee\u58eb<\/td>\n\u7c73\u6751 \u7f8e\u7d00<\/td>\n\u96fb\u5b50\u967d\u96fb\u5b50\u7cfb\u3067\u306e\u30c0\u30fc\u30af\u30bb\u30af\u30bf\u30fc\u306e\u63a2\u7d22<\/td>\n<\/tr>\n
\n
H28\/2016<\/span><\/div>\n<\/td>\n<\/tr>\n
\u4fee\u58eb<\/td>\n\u4e0b \u83ef\u5948\u5b50<\/td>\nSearch for charged lepton flavor violation at the ILC<\/td>\n<\/tr>\n
\u4fee\u58eb<\/td>\n\u9577\u5cf6\u77b3<\/td>\nLHC\u306b\u304a\u3051\u308b\u30b9\u30c8\u30c3\u30dd\u30cb\u30a6\u30e0\u63a2\u7d22\u53ef\u80fd\u6027\u306b\u3064\u3044\u3066<\/td>\n<\/tr>\n
\n
H27\/2015<\/span><\/div>\n<\/td>\n<\/tr>\n
\u535a\u58eb<\/td>\n\u5927\u91ce\u6176\u5b50<\/td>\nRandall-Sundrum\u6a21\u578b\u306b\u304a\u3051\u308b\u30e9\u30c7\u30a3\u30aa\u30f3\u306e\u73fe\u8c61\u8ad6\u7684\u7814\u7a76<\/td>\n<\/tr>\n
\u535a\u58eb<\/td>\n\u9f4b\u85e4\u9ebb\u7531\u7f8e<\/td>\n\u975e\u53ef\u63db\u7a7a\u9593\u4e0a\u306e\u6d41\u4f53\u529b\u5b66<\/td>\n<\/tr>\n
\u535a\u58eb<\/td>\n\u897f\u5c3e\u54b2\u5b50<\/td>\nA unified scenario of three kinds of Dark Matters in the Galaxy into a Kaluza-Klein Neutrino<\/td>\n<\/tr>\n
\u535a\u58eb<\/td>\n\u77e2\u8429\u91cf\u5b50<\/td>\n\u30a3\u30f3\u30b9\u30e9\u30fc\u30fb\u6cb3\u53e3\u5e7e\u4f55\u306b\u3088\u308b\u30e9\u30b0\u30e9\u30f3\u30b8\u30e5\u5f62\u5f0f ~\u5b9a\u5f0f\u5316\u304b\u3089\u5834\u306e\u7406\u8ad6\u3001\u5f26\u7406\u8ad6\u3078\u306e\u5fdc\u7528\u307e\u3067~<\/td>\n<\/tr>\n
\u4fee\u58eb<\/td>\n\u4f50\u3005\u6728\u5f69\u4e43<\/td>\n\u76f4\u63a5\u63a2\u7d22\u5b9f\u9a13\u306b\u304a\u3051\u308b\u30a8\u30ad\u30be\u30c1\u30c3\u30af\u30af\u30a9\u30fc\u30af\u3092\u4ecb\u3057\u305f\u6697\u9ed2\u7269\u8cea-\u6838\u5b50\u6563\u4e71\u65ad\u9762\u7a4d\u306b\u95a2\u3059\u308b\u7814\u7a76<\/td>\n<\/tr>\n
\u4fee\u58eb<\/td>\n\u4e8c\u968e\u5802\u745e\u5e0c<\/td>\nLHC Run-2\u3067\u306e\u6e96\u5b9f\u5149\u5b50\u6563\u4e71\u904e\u7a0b\u306b\u304a\u3051\u308b\u30c1\u30e3\u30fc\u30b8\u30fc\u30ce\u306e\u63a2\u7d22\u53ef\u80fd\u6027\u306b\u3064\u3044\u3066<\/td>\n<\/tr>\n
\u4fee\u58eb<\/td>\n\u5c71\u7530\u7f8e\u5e78<\/td>\nRundall-Sundrum\u6a21\u578b\u306b\u304a\u3051\u308bradion\u306e\u96fb\u5f31\u30b2\u30fc\u30b8\u30dc\u30bd\u30f3\u5bfe\u3078\u306e\u5d29\u58ca\u306b\u95a2\u3059\u308b\u7814\u7a76<\/td>\n<\/tr>\n
\n
H26\/2014<\/span><\/div>\n<\/td>\n<\/tr>\n
\u535a\u58eb<\/td>\n\u7c73\u5c71\u4eac\u5b50<\/td>\nThe Lattice Approach to Five Dimensional Gauge Theories<\/td>\n<\/tr>\n
\u4fee\u58eb<\/td>\n\u5c71\u4e0b\u516c\u5b50<\/td>\nLHC\u306b\u304a\u3051\u308b\u6e96\u5b9f\u5149\u5b50\u4ea4\u63db\u904e\u7a0b\u304b\u3089\u306e\u30ab\u30eb\u30fc\u30c4\u30a1=\u30af\u30e9\u30a4\u30f3\u30fb\u30b0\u30e9\u30d3\u30c8\u30f3\u306e\u5bc4\u4e0e\u306b\u3064\u3044\u3066<\/td>\n<\/tr>\n
\u4fee\u58eb<\/td>\n\u98ef\u5009\u6731\u97f3<\/td>\n\u8d85\u5bfe\u79f0 One Higgs Doublet Model \u306b\u304a\u3051\u308b\u30b2\u30fc\u30b8\u7d50\u5408\u5b9a\u6570\u306e\u7d71\u4e00\u53ef\u80fd\u6027\u306b\u3064\u3044\u3066<\/td>\n<\/tr>\n
\n
H25\/2013<\/span><\/div>\n<\/td>\n<\/tr>\n
\u535a\u58eb<\/td>\n\u5742\u4e0b\u3042\u3044<\/td>\nShape Transformations of Free and Confined Lipid Vesicles:
\nThree-Dimensional Analysis of Confocal Microscopy and Dynamically-Triangulated Membrane Simulation<\/td>\n<\/tr>\n
\u535a\u58eb<\/td>\n\u677e\u5c3e\u5149<\/td>\nR\u30d1\u30ea\u30c6\u30a3\u3092\u7834\u308b\u8d85\u5bfe\u79f0\u6a19\u6e96\u6a21\u578b\u306e\u73fe\u8c61\u8ad6\u7684\u7814\u7a76<\/td>\n<\/tr>\n
\u4fee\u58eb<\/td>\n\u56db\u8c37\u4f73\u7a42<\/td>\nConstraints on extra U(1) models from perturbative gauge coupling unification<\/td>\n<\/tr>\n
\u4fee\u58eb<\/td>\n\u658e\u85e4\u90a3\u83dc<\/td>\n\u975e\u7dda\u5f62\u5149\u5b66\u7d20\u5b50\u3092\u7528\u3044\u305f\u91cd\u529b\u6ce2\u4fe1\u53f7\u306e\u5897\u5e45<\/td>\n<\/tr>\n
\n
H24\/2012<\/span><\/div>\n<\/td>\n<\/tr>\n
\u4fee\u58eb<\/td>\n\u5927\u91ce\u6176\u5b50<\/td>\nProduction and decay of heavy radion in Randall-Sundrum model at the LHC<\/td>\n<\/tr>\n
\u4fee\u58eb<\/td>\n\u5c0f\u4fe3\u5df4\u82b3<\/td>\nB\u2192K\u03c0 decay in R-parity violating supersymmetric standard model<\/td>\n<\/tr>\n
\u4fee\u58eb<\/td>\n\u6a29\u85e4\u91cc\u5948<\/td>\n\u306d\u3058\u308c\u578b\u91cd\u529b\u6ce2\u691c\u51fa\u5668TOBA\u306e\u958b\u767a<\/td>\n<\/tr>\n
\u4fee\u58eb<\/td>\n\u9f4b\u85e4\u9ebb\u7531\u7f8e<\/td>\nNambu\u98a8\u6d41\u4f53\u529b\u5b66\u3092\u7528\u3044\u305f\u5f26\u3068\u819c\u7406\u8ad6\u306e\u8003\u5bdf<\/td>\n<\/tr>\n
\u4fee\u58eb<\/td>\n\u9577\u5ca1\u53cb\u7f8e<\/td>\nRHIC\u3068LHC\u306b\u304a\u3051\u308bQGP\u6d41\u4f53\u4e2d\u3067\u306e\u30c1\u30e3\u30fc\u30e2\u30cb\u30a6\u30e0\u306e\u9023\u7d9a\u7684\u89e3\u96e2\u73fe\u8c61<\/td>\n<\/tr>\n
\n
H23\/2011<\/span><\/div>\n<\/td>\n<\/tr>\n
\u535a\u58eb<\/td>\n\u897f\u7530\u6075\u91cc\u5948<\/td>\nDevelopment of advanced technology on optical system of gravitational
\nwave detector KAGRA<\/td>\n<\/tr>\n
\u4fee\u58eb<\/td>\n\u6728\u4f50\u306f\u308b\u9999<\/td>\n\u96fb\u78c1\u6c17\u529b\u3082\u91cd\u529b\u3068\u540c\u3058\u304f\u30a8\u30f3\u30c8\u30ed\u30d4\u30fc\u529b\u304b?<\/td>\n<\/tr>\n
\u4fee\u58eb<\/td>\n\u7a42\u8c37\u91ce\u8a13\u5b50<\/td>\nAdS\/CFT\u5bfe\u5fdc\u306b\u3088\u308b\u71b1\u4f1d\u5c0e\u306e\u89e3\u6790<\/td>\n<\/tr>\n
\n
H22\/2010<\/span><\/div>\n<\/td>\n<\/tr>\n
\u4fee\u58eb<\/td>\n\u76f8\u7530\u6709\u7f8e\u5b50<\/td>\nConstraints on R-parity violating couplings from leptonic decays of D_s and B^+ mesons<\/td>\n<\/tr>\n
\u4fee\u58eb<\/td>\n\u677e\u5c3e\u5149<\/td>\nDark Matter in radiative U(1) B-L symmetry breaking model<\/td>\n<\/tr>\n
\u4fee\u58eb<\/td>\n\u6c5f\u5c3b\u60a0\u7f8e\u5b50<\/td>\n\u5c0f\u578b\u91cd\u529b\u6ce2\u89b3\u6e2c\u885b\u661fDECIGO Pathfinder\u7528\u8a66\u9a13\u30de\u30b9\u975e\u63a5\u89e6\u5236\u5fa1\u6a5f\u69cb\u306e\u958b\u767a<\/td>\n<\/tr>\n
\u4fee\u58eb<\/td>\n\u9234\u6728\u7406\u6075\u5b50<\/td>\n\u5c0f\u578b\u91cd\u529b\u6ce2\u89b3\u6e2c\u885b\u661fDECIGO Pathfinder\u7528\u8a66\u9a13\u30de\u30b9\u30e2\u30b8\u30e5\u30fc\u30eb\u306e\u958b\u767a<\/td>\n<\/tr>\n
\n
H21\/2009<\/span><\/div>\n<\/td>\n<\/tr>\n
\u535a\u58eb<\/td>\n\u91d1\u7551\u559c\u7f8e<\/td>\nPhenomenology of Kaluza-Klein gluon in Warped Extra Dimension Model<\/td>\n<\/tr>\n
\u535a\u58eb<\/td>\n\u6df1\u702c\u967d\u5b50<\/td>\nMeson mass in the second quantized string model of QCD<\/td>\n<\/tr>\n
\u535a\u58eb<\/td>\n\u5357\u5d0e\u6893<\/td>\n\u975e\u5bfe\u79f0\u5468\u671f\u578b\u30dd\u30c6\u30f3\u30b7\u30e3\u30eb\u306b\u3088\u308b\u5b87\u5b99\u306e\u30d0\u30ea\u30aa\u30f3\u6570\u751f\u6210\u6a5f\u69cb\u306e\u7814\u7a76<\/td>\n<\/tr>\n
\u4fee\u58eb<\/td>\n\u9593\u3000\u4eac\u5b50<\/td>\n\u9060\u65b9\u5929\u4f53\u306e\u5206\u5e03\u304b\u3089\u89e3\u660e\u3059\u308b\u5b87\u5b99\u306e\u4e00\u69d8\u6027<\/td>\n<\/tr>\n
\u4fee\u58eb<\/td>\n\u51fa\u96f2\u6c99\u7406<\/td>\nAdS\/CFT\u5bfe\u5fdc\u306e\u30cf\u30c9\u30ed\u30f3\u7269\u6027\u7cfb\u3078\u306e\u5fdc\u7528<\/td>\n<\/tr>\n
\u4fee\u58eb<\/td>\n\u5b89\u6c5f\u7531\u4f73<\/td>\n\u6709\u52b9\u30dd\u30c6\u30f3\u30b7\u30e3\u30eb\u306e\u65b9\u6cd5\u3092\u7528\u3044\u305f\u30d2\u30c3\u30b0\u30b9\u7c92\u5b50\u306e\u8cea\u91cf\u306b\u5bfe\u3059\u308b\u5236\u9650\u306e\u5c0e\u51fa<\/td>\n<\/tr>\n
\u4fee\u58eb<\/td>\n\u7c73\u5c71\u4eac\u5b50<\/td>\n\u30e9\u30f3\u30c9\u30fc\u30eb\u30fb\u30b5\u30f3\u30c9\u30e9\u30e0\u30e2\u30c7\u30eb\u306b\u304a\u3051\u308b\u30ab\u30eb\u30c4\u30a1\u30fc\u30fb\u30af\u30e9\u30a4\u30f3\u30b0\u30eb\u30fc\u30aa\u30f3\u306e\u73fe\u8c61\u8ad6\u7684\u7814\u7a76<\/td>\n<\/tr>\n
\n
H20\/2008<\/span><\/div>\n<\/td>\n<\/tr>\n
\u535a\u58eb<\/td>\n\u82d4\u5c71\u572d\u4ee5\u5b50<\/td>\nDevelopment of displacement- and frequency-noise free interferometer for gravitational wave detection<\/td>\n<\/tr>\n
\u4fee\u58eb<\/td>\n\u897f\u7530\u6075\u91cc\u5948<\/td>\n\u7b2c\u4e09\u4e16\u4ee3\u91cd\u529b\u6ce2\u691c\u51fa\u5668\u306e\u305f\u3081\u306e\u8f3b\u5c04\u5727\u3092\u7528\u3044\u305f\u30d5\u30a9\u30c8\u30c0\u30a4\u30aa\u30fc\u30c9\u306e\u91cf\u5b50\u52b9\u7387\u6e2c\u5b9a\u6cd5\u306e\u63d0\u6848<\/td>\n<\/tr>\n
\u4fee\u58eb<\/td>\n\u6cb3\u91ce\u907c\u5b50<\/td>\n\u30cf\u30c9\u30ed\u30f3\u30b3\u30e9\u30a4\u30c0\u30fc\u306b\u304a\u3051\u308b\u91cd\u3044\u30ec\u30d7\u30c8\u30f3\u751f\u6210\u306b\u95a2\u3059\u308b\u7814\u7a76<\/td>\n<\/tr>\n
\u4fee\u58eb<\/td>\n\u5409\u6fa4\u3000\u78a7<\/td>\n\u96fb\u5b50\u30fb\u967d\u96fb\u5b50\u30ea\u30cb\u30a2\u30b3\u30e9\u30a4\u30c0\u30fc\u306b\u304a\u3051\u308b\u7b2c4\u4e16\u4ee3\u30ec\u30d7\u30c8\u30f3\u306e\u63a2\u7d22<\/td>\n<\/tr>\n
\n
H19\/2007<\/span><\/div>\n<\/td>\n<\/tr>\n
\u535a\u58eb<\/td>\n\u5ddd\u6dfb\u53f2\u5b50<\/td>\nExperimental Demonstration of a Control Scheme for a Tuned RSE
\nInterferometer for Next-generation Gravitational-wave Detectors<\/td>\n<\/tr>\n
\u535a\u58eb<\/td>\n\u962a\u7530\u7d2b\u5e06\u91cc<\/td>\n\u91cd\u529b\u6ce2\u691c\u51fa\u5668\u306b\u304a\u3051\u308b\u30dd\u30f3\u30c7\u30ed\u30e2\u30fc\u30c6\u30a3\u30d6\u30b9\u30af\u30a4\u30fc\u30b8\u30f3\u30b0\u3092\u5229\u7528\u3057\u305f\u8f3b\u5c04\u5727\u96d1\u97f3\u9664\u53bb\u306e\u7814\u7a76<\/td>\n<\/tr>\n
\u535a\u58eb<\/td>\n\u7167\u6cbc\u5e78\u5b50<\/td>\n\u30b9\u30c8\u30ea\u30f3\u30b0\u7406\u8ad6\u3092\u7528\u3044\u305f\u30cf\u30c9\u30ed\u30f3\u7269\u7406\u306e\u89e3\u6790<\/td>\n<\/tr>\n
\u4fee\u58eb<\/td>\n\u9752\u6728\u667a\u7f8e<\/td>\n\u8d85\u5bfe\u79f0E6\u5927\u7d71\u4e00\u6a21\u578b\u306b\u5bfe\u3059\u308b\u96fb\u5f31\u7cbe\u5bc6\u5b9f\u9a13\u304b\u3089\u306e\u5236\u9650<\/td>\n<\/tr>\n
\u4fee\u58eb<\/td>\n\u57a3\u5185\u307e\u3069\u304b<\/td>\nBars-Hanson\u5f26\u6a21\u578b\u3068\u975e\u53ef\u63dbBorn-Infeld\u4f5c\u7528<\/td>\n<\/tr>\n
\n
H18\/2006<\/span><\/div>\n<\/td>\n<\/tr>\n
\u535a\u58eb<\/td>\n\u8868\u3000\u6587<\/td>\nTeV\u30b9\u30b1\u30fc\u30eb\u8d85\u5bfe\u79f0\u6027\u30b7\u30fc\u30bd\u30fc\u6a21\u578b\u306e\u73fe\u8c61\u8ad6\u7684\u7814\u7a76<\/td>\n<\/tr>\n
\u4fee\u58eb<\/td>\n\u91d1\u7551\u559c\u7f8e<\/td>\nLeptogenesis at the TeV scale in the Brane World<\/td>\n<\/tr>\n
\u4fee\u58eb<\/td>\n\u6df1\u702c\u967d\u5b50<\/td>\nMass spectrum of Mesons in Second Quantizatized Dual String Model of QCD<\/td>\n<\/tr>\n
\u4fee\u58eb<\/td>\n\u5357\u5d0e\u3000\u6893<\/td>\nTwo small Numbers, Baryon number in the Universe and the Cosmological Constant, are interrelated?<\/td>\n<\/tr>\n
\u4fee\u58eb<\/td>\n\u6d45\u539f\u65e9\u82d7<\/td>\n\u9280\u6cb3\u306e\u69cb\u9020\u306e\u9032\u5316\u306b\u3064\u3044\u3066\u306e\u8003\u5bdf<\/td>\n<\/tr>\n
\u4fee\u58eb<\/td>\n\u52a9\u5ddd\u3000\u592e<\/td>\nPhenomenology of the next-to-minimal supersymmetric standard model<\/td>\n<\/tr>\n
\n
H17\/2005<\/span><\/div>\n<\/td>\n<\/tr>\n
\u4fee\u58eb<\/td>\n\u82d4\u5c71\u572d\u4ee5\u5b50<\/td>\n\u91cd\u529b\u6ce2\u691c\u51fa\u306e\u305f\u3081\u306e\u5909\u4f4d\u96d1\u97f3\u30d5\u30ea\u30fc\u5e72\u6e09\u8a08\u306e\u958b\u767a<\/td>\n<\/tr>\n
\u4fee\u58eb<\/td>\n\u897f\u5c3e\u54b2\u5b50<\/td>\nIs the Lightest Kaluza-Klein Neutrino a Candidate for Cold Dark Matter?
\n~New method of directly searching Cold Dark Matter in Large Hadron Collider~<\/td>\n<\/tr>\n
\n
H16\/2004<\/span><\/div>\n<\/td>\n<\/tr>\n
\u535a\u58eb<\/td>\n\u5c0f\u6a4b\u6709\u5b50<\/td>\n2\u6210\u5206\u884c\u5217\u6a21\u578b\u4e26\u3073\u306b\u975e\u53ef\u63db\u30c1\u30e3\u30fc\u30f3\u30fb\u30b5\u30a4\u30e2\u30f3\u7406\u8ad6\u306e\u30b5\u30a4\u30d0\u30fc\u30b0\u30fb\u30a6\u30a3\u30c3\u30c6\u30f3\u5199\u50cf\u3092\u7528\u3044\u305f\u91cf\u5b50\u30db\u30fc\u30eb\u52b9\u679c\u306e\u7814\u7a76<\/td>\n<\/tr>\n
\u535a\u58eb<\/td>\n\u672c\u591a\u7f8e\u5948\u5b50<\/td>\nCP violation and flavor changing interactions in supersymmetric theories<\/td>\n<\/tr>\n
\u4fee\u58eb<\/td>\n\u5c0f\u91ce\u82b3\u7f8e<\/td>\n\u30b9\u30cb\u30e5\u30fc\u30c8\u30ea\u30ce\u8cea\u91cf\u306b\u5bfe\u3059\u308b\u96fb\u5b50\u967d\u96fb\u5b50\u885d\u7a81\u5b9f\u9a13\u304b\u3089\u306e\u5236\u9650<\/td>\n<\/tr>\n
\u4fee\u58eb<\/td>\n\u5ddd\u6dfb\u53f2\u5b50<\/td>\n\u91cd\u529b\u6ce2\u691c\u51fa\u7528\u5e2f\u57df\u53ef\u5909\u578b\u30ec\u30fc\u30b6\u30fc\u5e72\u6e09\u8a08\u4fe1\u53f7\u53d6\u5f97\u6cd5\u306e\u958b\u767a<\/td>\n<\/tr>\n
\u4fee\u58eb<\/td>\n\u962a\u7530\u7d2b\u5e06\u91cc<\/td>\n\u30ec\u30fc\u30b6\u5e72\u6e09\u8a08\u91cd\u529b\u6ce2\u691c\u51fa\u5668\u306e\u305f\u3081\u306e\u91cf\u5b50\u96d1\u97f3\u306e\u7814\u7a76<\/td>\n<\/tr>\n
\u4fee\u58eb<\/td>\n\u7167\u6cbc\u5e78\u5b50<\/td>\n\u30b9\u30c8\u30ea\u30f3\u30b0\u306b\u3088\u308b\u30da\u30f3\u30bf\u30af\u30aa\u30fc\u30af\u306e\u7814\u7a76<\/td>\n<\/tr>\n
\n
H15\/2003<\/span><\/div>\n<\/td>\n<\/tr>\n
\u4fee\u58eb<\/td>\n\u8868\u3000\u6587<\/td>\n\u30ea\u30c8\u30eb\u30d2\u30c3\u30b0\u30b9\u6a21\u578b\u306b\u304a\u3051\u308b\u73fe\u8c61\u8ad6\u7684\u7814\u7a76<\/td>\n<\/tr>\n
\u4fee\u58eb<\/td>\n\u6749\u5b89\u7531\u7f8e\u5b50<\/td>\n\u03b3\u03b3\u30b3\u30e9\u30a4\u30c0\u30fc\u306b\u304a\u3051\u308b\u30d2\u30c3\u30b0\u30b93\u70b9\u30ab\u30c3\u30d7\u30ea\u30f3\u30b0\u306e\u63a2\u7d22<\/td>\n<\/tr>\n
\u4fee\u58eb<\/td>\n\u91ce\u53e3\u4e9c\u5e0c\u5b50<\/td>\n\u30b2\u30fc\u30b8\u7406\u8ad6\u3068\u91cd\u529b\u7406\u8ad6\u306e\u9593\u306e\u53cc\u5bfe\u6027\u306e\u529b\u5b66\u7684\u8d77\u6e90<\/td>\n<\/tr>\n
\u4fee\u58eb<\/td>\n\u677e\u6c38\u771f\u7406\u5b50<\/td>\nAttempt to solve TeV gamma paradox by discrete dimension model<\/td>\n<\/tr>\n
\u4fee\u58eb<\/td>\n\u5b89\u7530\u6643\u5b50<\/td>\n\u9280\u6cb3\u7cfb\u4e2d\u5fc3\u9818\u57df\u306b\u304a\u3051\u308b\u661f\u9593\u7269\u8cea\u306e\u7269\u7406\u72b6\u614b<\/td>\n<\/tr>\n
\n
H14\/2002<\/span><\/div>\n<\/td>\n<\/tr>\n
\u535a\u58eb<\/td>\n\u5c0f\u539f\u307f\u3069\u308a<\/td>\nThe problem of fermion mass matrices in SUSY GUT\u2019s<\/td>\n<\/tr>\n
\u535a\u58eb<\/td>\n\u9577\u5d8b\u771f\u8a18\u5b50<\/td>\nProof of Factorization and Analysis of B -> DK mode in the PQCD method<\/td>\n<\/tr>\n
\u535a\u58eb<\/td>\n\u5bae\u6bdb\u660e\u5b50<\/td>\n\u884c\u5217\u6a21\u578b\u306e\u30aa\u30fc\u30d3\u30d5\u30a9\u30fc\u30eb\u30c9\u30b3\u30f3\u30d1\u30af\u30c8\u5316<\/td>\n<\/tr>\n
\u4fee\u58eb<\/td>\n\u897f\u539f\u7406\u7d75<\/td>\n\u30cf\u30c9\u30ed\u30f3\u30b3\u30e9\u30a4\u30c0\u30fc\u306b\u304a\u3051\u308b\u30b9\u30af\u30a9\u30fc\u30af\u5bfe\u751f\u6210\u63a2\u7d22<\/td>\n<\/tr>\n
\n
H13\/2001<\/span><\/div>\n<\/td>\n<\/tr>\n
\u4fee\u58eb<\/td>\n\u7530\u4e2d\u9ebb\u5229\u6c5f<\/td>\ntop quark decay \u306b\u304a\u3051\u308b W-boson\u306e\u504f\u6975\u6e2c\u5b9a -\u6a19\u6e96\u6a21\u578b\u306e\u73fe\u8c61\u8ad6\u7684\u691c\u8a3c-<\/td>\n<\/tr>\n
\u4fee\u58eb<\/td>\n\u5c0f\u6a4b\u6709\u5b50<\/td>\n\u884c\u5217\u6a21\u578b\u306b\u3088\u308b\u91cf\u5b50\u30db\u30fc\u30eb\u52b9\u679c\u306e\u8a18\u8ff0<\/td>\n<\/tr>\n
\u4fee\u58eb<\/td>\n\u548c\u6cc9\u60a6\u5b50<\/td>\nConstructing a 4D theory from a 3D ones \u2013 A phenomenological consequence \u2013<\/td>\n<\/tr>\n
\u4fee\u58eb<\/td>\n\u672c\u591a\u7f8e\u5948\u5b50<\/td>\n\u8d85\u5bfe\u79f0\u30de\u30e8\u30ed\u30f3\u6a21\u578b\u3068\u30cb\u30e5\u30fc\u30c8\u30ea\u30ce\u73fe\u8c61\u8ad6<\/td>\n<\/tr>\n
\n
H12\/2000<\/span><\/div>\n<\/td>\n<\/tr>\n
\u535a\u58eb<\/td>\n\u6d2a\u6c5f\u7f8e<\/td>\nB physics and the puzzle of \u03b7\u2019<\/td>\n<\/tr>\n
\u535a\u58eb<\/td>\n\u6d45\u5ddd\u6075\u7406<\/td>\nProbing the CP property of the Higgs sector at future colliders<\/td>\n<\/tr>\n
\u535a\u58eb<\/td>\n\u897f\u6751\u307e\u3069\u304b<\/td>\nLocal Symmetries in the AdS\/CFT Correspondence<\/td>\n<\/tr>\n
\u535a\u58eb<\/td>\n\u5c0f\u6adb\u5e78\u5b50<\/td>\nConformal Anomaly via AdS\/CFT duality<\/td>\n<\/tr>\n
\u4fee\u58eb<\/td>\n\u6e05\u6c34\u660e\u5b50<\/td>\nW \u30dc\u30bd\u30f3\u306e\u96fb\u6c17\u53cc\u6975\u5b50\u80fd\u7387\u306b\u5bfe\u3059\u308b\u8d85\u5bfe\u79f0\u6027\u7c92\u5b50\u306e\u52b9\u679c\u3068\u5149\u5b50-\u5149\u5b50\u885d\u7a81\u5b9f\u9a13<\/td>\n<\/tr>\n
\u4fee\u58eb<\/td>\n\u9ad8\u5c71\u6075\u7f8e<\/td>\n\u30ac\u30f3\u30de\u7dda\u30d0\u30fc\u30b9\u30c8\u306e\u6b8b\u5149\u306e\u767a\u751f\u6a5f\u69cb<\/td>\n<\/tr>\n
\n
H11\/1999<\/span><\/div>\n<\/td>\n<\/tr>\n
\u535a\u58eb<\/td>\n\u9752\u6728\u771f\u7531\u7f8e<\/td>\nA New Supersymmetric Extension of the Standard Model with an Additional U(1) Gauge Symmetry<\/td>\n<\/tr>\n
\u535a\u58eb<\/td>\n\u4eca\u4e95\u5e03\u7f8e<\/td>\n\u533a\u5206\u7684\u306b\u4e00\u69d8\u306a\u5f26\u7406\u8ad6\u306e\u7814\u7a76<\/td>\n<\/tr>\n
\u535a\u58eb<\/td>\n\u9060\u85e4\u7406\u4f73<\/td>\nDerivations of the Effective Actions for D-branes<\/td>\n<\/tr>\n
\u4fee\u58eb<\/td>\n\u9577\u5d8b\u771f\u8a18\u5b50<\/td>\n\u7a00\u5d29\u58caB\u2192Xs \u03b3\u3078\u306e\u30d9\u30af\u30c8\u30eb\u30e9\u30a4\u30af\u30fb\u30af\u30a9\u30fc\u30af\u6a21\u578b\u306e\u5f71\u97ff<\/td>\n<\/tr>\n
\u4fee\u58eb<\/td>\n\u6a4b\u672c\u4f38\u5b50<\/td>\n\u30df\u30e5\u30fc\u30aa\u30f3\u30b3\u30e9\u30a4\u30c0\u30fc\u306b\u304a\u3051\u308b\u8377\u96fb\u30d2\u30c3\u30b0\u30b9\u7c92\u5b50\u306e\u5bfe\u751f\u6210<\/td>\n<\/tr>\n
\u4fee\u58eb<\/td>\n\u5bae\u6bdb\u660e\u5b50<\/td>\n\u8d85\u5f26\u7406\u8ad6\u306b\u3088\u308bDp-brane\u306e\u6563\u4e71\u3068M\u7406\u8ad6\u306b\u3088\u308bD-particle\u306e\u76f8\u4e92\u4f5c\u7528<\/td>\n<\/tr>\n
\u4fee\u58eb<\/td>\n\u77e2\u6570\u3072\u308d\u307f<\/td>\n\u819c(\u30e1\u30f3\u30d6\u30ec\u30a4\u30f3)\u306b\u5bfe\u3059\u308b\u6c4e\u95a2\u6570\u65b9\u7a0b\u5f0f\u306e\u5c0e\u51fa<\/td>\n<\/tr>\n
\u4fee\u58eb<\/td>\n\u5c71\u672c\u7f8e\u5e06<\/td>\nAdS\/CFT\u5bfe\u5fdc\u3092\u7528\u3044\u305f\u91cf\u5b50\u7570\u5e38(Anomaly)\u306e\u7814\u7a76<\/td>\n<\/tr>\n
\n
H10\/1998<\/span><\/div>\n<\/td>\n<\/tr>\n
\u535a\u58eb<\/td>\n\u9580\u5409\u670b\u5b50<\/td>\nQuantum cosmology in dilaton gravity<\/td>\n<\/tr>\n
\u4fee\u58eb<\/td>\n\u5c0f\u6adb\u5e78\u5b50<\/td>\nSchild Type Superstring Action and Matrix Model<\/td>\n<\/tr>\n
\u4fee\u58eb<\/td>\n\u52a0\u85e4\u7531\u91cc\u5b50<\/td>\nDerivation of Charged Black Hole Entropy from D0-branes in Matrix Theory<\/td>\n<\/tr>\n
\n
H09\/1997<\/span><\/div>\n<\/td>\n<\/tr>\n
\u535a\u58eb<\/td>\n\u4e0a\u6749\u667a\u5b50<\/td>\nStudy of Baryogenesis due to CP violating Domain Wall at the Electroweak Phase Transition<\/td>\n<\/tr>\n
\u535a\u58eb<\/td>\n\u9f4b\u85e4\u667a\u7f8e<\/td>\n\u30b2\u30fc\u30b8\u5834\u306e3\u70b9\u7d50\u5408\u306b\u304a\u3051\u308bCP\u5bfe\u79f0\u6027\u306e\u7834\u308c<\/td>\n<\/tr>\n
\u4fee\u58eb<\/td>\n\u6d45\u5ddd\u6075\u7406<\/td>\nPhenomenological Study in Electron-Proton Collider HERA<\/td>\n<\/tr>\n
\u4fee\u58eb<\/td>\n\u6d2a\u6c5f\u7f8e<\/td>\nParticle Physics Phenomenology in Connection with the Future B Factories<\/td>\n<\/tr>\n
\n
H08\/1996<\/span><\/div>\n<\/td>\n<\/tr>\n
\u535a\u58eb<\/td>\n\u5ddd\u6751\u660c\u5b50<\/td>\nSwimming of Micro-organisms from Field Theoretical Viewpoint<\/td>\n<\/tr>\n
\u4fee\u58eb<\/td>\n\u9752\u6728\u771f\u7531\u7f8e<\/td>\n\u8d85\u5bfe\u79f0\u6027\u6a21\u578b\u306b\u304a\u3051\u308b\u96fb\u5f31\u30d0\u30ea\u30aa\u30f3\u751f\u6210<\/td>\n<\/tr>\n
\u4fee\u58eb<\/td>\n\u4eca\u4e95\u5e03\u7f8e<\/td>\n\u5f26\u306e\u51dd\u7e2e\u306e\u30c0\u30a4\u30ca\u30df\u30c3\u30af\u30b9<\/td>\n<\/tr>\n
\n
H07\/1995<\/span><\/div>\n<\/td>\n<\/tr>\n
\u535a\u58eb<\/td>\n\u5c71\u53e3\u3042\u3065\u3055<\/td>\nThe Electroweak Baryogenesis and The Phase Transition Dynamics<\/td>\n<\/tr>\n
\u4fee\u58eb<\/td>\n\u9060\u85e4\u7406\u4f73<\/td>\n\u5927\u6c17\u30cb\u30e5\u30fc\u30c8\u30ea\u30ce\u554f\u984c\u306b\u304a\u3051\u308b\u5730\u7403\u306e\u7269\u8cea\u52b9\u679c\u306e\u5f71\u97ff<\/td>\n<\/tr>\n
\u4fee\u58eb<\/td>\n\u9580\u5409\u670b\u5b50<\/td>\n\u8d85\u5bfe\u79f0\u6027\u306e\u7834\u308c\u306e\u52d5\u529b\u5b66<\/td>\n<\/tr>\n
\u4fee\u58eb<\/td>\n\u5317\u539f\u7f8e\u5948\u5b50<\/td>\nCP\u975e\u4fdd\u5b58\u306e\u30b2\u30fc\u30b8\u30dc\u30bd\u30f33\u70b9\u7d50\u5408WWZ\u3068\u8d85\u5bfe\u79f0\u6027\u6a21\u578b<\/td>\n<\/tr>\n
\n
H06\/1994<\/span><\/div>\n<\/td>\n<\/tr>\n
\u535a\u58eb<\/td>\n\u6728\u6751\u4e45\u7f8e\u5b50<\/td>\nHadron Multiplicity and Angular Distribution in the Perturbative QCD<\/td>\n<\/tr>\n
\u4fee\u58eb<\/td>\n\u4e0a\u6749\u667a\u5b50<\/td>\nThe change from quantum state to classical state in the inflationary universe<\/td>\n<\/tr>\n
\u4fee\u58eb<\/td>\n\u6589\u85e4\u667a\u7f8e<\/td>\n\u30d9\u30af\u30c8\u30eb\u30e9\u30a4\u30af\u306a\u30af\u30a9\u30fc\u30af\u306e\u5c0e\u5165\u306b\u3088\u308bCP\u306e\u7834\u308c<\/td>\n<\/tr>\n
\u4fee\u58eb<\/td>\n\u9999\u6708\u6df1\u96ea<\/td>\n2-from\u91cd\u529b\u304b\u3089Einstein\u91cd\u529b\u3078<\/td>\n<\/tr>\n
\u4fee\u58eb<\/td>\n\u91d1\u4e45\u4fdd\u6587\u5b50<\/td>\nThrust distribution of two-jet like processes at a photon-photon collider<\/td>\n<\/tr>\n
\n
H05\/1993<\/span><\/div>\n<\/td>\n<\/tr>\n
\u535a\u58eb<\/td>\n\u4e38\u4e95\u7f8e\u4fdd<\/td>\n\u91cd\u3044\u30de\u30e8\u30e9\u30ca\u30cb\u30e5\u30fc\u30c8\u30ea\u30ce\u306e\u691c\u8a3c:W\u30dc\u30bd\u30f3\u5bfe\u751f\u6210\u904e\u7a0b\u306e\u8f3b\u5c04\u88dc\u6b63\u3092\u4ecb\u3057\u3066<\/td>\n<\/tr>\n
\u4fee\u58eb<\/td>\n\u5ddd\u6751\u660c\u5b50<\/td>\n\u5fae\u751f\u7269\u306e\u904a\u6cf3\u3068\u305d\u306e\u4ee3\u6570\u69cb\u9020<\/td>\n<\/tr>\n
\n
H04\/1992<\/span><\/div>\n<\/td>\n<\/tr>\n
\u4fee\u58eb<\/td>\n\u5c71\u53e3\u3042\u3065\u3055<\/td>\nThe Electroweak Baryogenesis and the Dynamics of Phase Transition<\/td>\n<\/tr>\n
\u4fee\u58eb<\/td>\n\u9577\u68ee\u85e4\u6c5f<\/td>\n\u91cf\u5b50\u91cd\u529b\u3078\u306e\u4f4d\u76f8\u7684\u91cd\u529b\u7406\u8ad6\u304b\u305f\u306e\u30a2\u30d7\u30ed\u30fc\u30c1<\/td>\n<\/tr>\n
\n
H03\/1991<\/span><\/div>\n<\/td>\n<\/tr>\n
\n
H02\/1990<\/span><\/div>\n<\/td>\n<\/tr>\n
\u4fee\u58eb<\/td>\n\u6728\u6751\u4e45\u7f8e\u5b50<\/td>\n\u30c8\u30c3\u30d7\u30af\u30a9\u30fc\u30af\u306b\u4f9d\u308b\u30c0\u30a4\u30ca\u30df\u30ab\u30eb\u306a\u5bfe\u79f0\u6027\u306e\u7834\u308c\u3068B^0-B^0bar\u6df7\u5408<\/td>\n<\/tr>\n
\u4fee\u58eb<\/td>\n\u4e2d\u9053\u6676\u9999<\/td>\n4\u6b21\u5143\u306e\u30c8\u30dd\u30ed\u30b8\u30ab\u30eb\u306a\u91cf\u5b50\u91cd\u529b\u7406\u8ad6<\/td>\n<\/tr>\n
\u4fee\u58eb<\/td>\n\u5c0f\u4e45\u4fdd\u4f50\u77e5\u5b50<\/td>\n\u819c\u306e\u6563\u4e71\u632f\u5e45\u306e\u9ad8\u30a8\u30cd\u30eb\u30ae\u30fc\u3067\u306e\u632f\u821e\u3044<\/td>\n<\/tr>\n
\n
S64\/1989<\/span><\/div>\n<\/td>\n<\/tr>\n
\u4fee\u58eb<\/td>\n\u4e38\u4e95\u7f8e\u4fdd<\/td>\n\u5f26\u306e\u5834\u306e\u7406\u8ad6\u306b\u304a\u3051\u308b\u767a\u5c55\u65b9\u7a0b\u5f0f<\/td>\n<\/tr>\n<\/tbody>\n<\/table>\n
\n