{"id":3191,"date":"2020-08-26T16:07:26","date_gmt":"2020-08-26T07:07:26","guid":{"rendered":"http:\/\/localhost:8888\/accl\/?page_id=3191"},"modified":"2023-04-10T13:34:48","modified_gmt":"2023-04-10T04:34:48","slug":"previoussemi15","status":"publish","type":"page","link":"https:\/\/kekacclserver.kek.jp\/accl\/seminar\/previoussemi15","title":{"rendered":"\u5e73\u621015\u5e74\u5ea6\u30002003.4 ~ 2004.3"},"content":{"rendered":"

Accel. Lab. Seminars \u2013 Heisei 15th<\/p>\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
\u65e5\u4ed8
Date<\/td>\n		\u66dc\u65e5
Day<\/td>\n		\u6642\u9593
Time<\/td>\n		\u5834\u6240
Venue<\/td>\n		\u8b1b\u5e2b (\u6240\u5c5e)
Speaker (Affiliation)<\/td>\n		\u8b1b\u6f14\u984c\u76ee
Title<\/td>\n		\u4e16\u8a71\u4eba
Contact<\/td>\n		\u5185\u5bb9
Abstract<\/td>\n<\/tr>\n
2004\/03\/24\n<\/td>\nWed.\n<\/td>\n14:30-\n<\/td>\n2\u53f7\u9928\uff16\u968e\u30bb\u30df\u30ca\u30fc\u5ba4\n<\/td>\n\u5916\u5c71\u6bc5\n<\/td>\nJ-PARC\u306e\u30ea\u30f3\u30b0\u306b\u304a\u3051\u308bcollective effect\u306e\u8a55\u4fa1\n<\/td>\n\n<\/td>\nJ-PARC\u306e3GeV RCS\uff08rapid cycling synchrotron\uff09\u3001
\n50GeV MR\uff08main ring\uff09\u306e\u30a4\u30f3\u30d4\u30fc\u30c0\u30f3\u30b9\u8a55\u4fa1\u306e\u73fe\u72b6\u306b\u3064\u3044\u3066\u5831\u544a\u3059\u308b\u3002
\nKicker, RF cavity, vacuum pipe, BPM \u7b49\u306e\u30a4\u30f3\u30d4\u30fc\u30c0\u30f3\u30b9\u3092\uff0c
\n\u89e3\u6790\u7684\u8a08\u7b97\uff0c\u6570\u5024\u8a08\u7b97\uff0c\u30ef\u30a4\u30e4\u30fc\u6cd5\u306b\u3088\u308b\u6e2c\u5b9a\u3092\u9069\u5b9c\u4f7f\u3044\u308f\u3051\u3066\u6c42\u3081\u305f\u3002
\n\u7c21\u5358\u306a\u30d3\u30fc\u30e0\u5b89\u5b9a\u6027\u306e\u8a55\u4fa1\uff08Keil-Schnell \u516c\u5f0f\u306a\u3069\u306b\u3088\u308b\u3082\u306e\uff09\u306e\u7d50\u679c\u3082
\n\u5408\u308f\u305b\u3066\u5831\u544a\u3059\u308b\u3002
\n\u96fb\u5b50\u96f2\u306e\u52b9\u679c\u306b\u3064\u3044\u3066\u3001KEK-PS MR \u3067\u306e\u6e2c\u5b9a\u7d50\u679c\u3068\u7406\u8ad6\u8a08\u7b97\u3068\u306e\u6bd4\u8f03\u3092\u542b\u3081\u3066
\n\u8a00\u53ca\u3059\u308b\u4e88\u5b9a\u3002\n<\/td>\n<\/tr>\n
2004\/03\/17\n<\/td>\nWed.\n<\/td>\n13:30-\n<\/td>\nKEKB \u52a0\u901f\u5668\u5236\u5fa1\u68df\u4f1a\u8b70\u5ba4\n<\/td>\nMatthias Clausen\u6c0f, DESY, Germany\n<\/td>\nTrends in Cryogenic and Utility Controls at DESY\n<\/td>\n\u5c71\u672c\u6607\n<\/td>\nMatthias Cluasen\u6c0f\u306fDESY\u306eCryogenic contorl group \u306e\u30b0\u30eb\u30fc\u30d7\u30ea\u30fc\u30c0\u3068\u3057\u3001
\nHERA, TESLA Test Facility, \u3084 XFEL\u306a\u3069\u306eDESY\u306e\u4e3b\u8981\u306a\u30d7\u30ed\u30b8\u30a7\u30af\u30c8\u306b\u643a\u308f\u3063
\n\u3066\u304a\u3089\u308c\u308b\u3002Clausen\u6c0f\u306f\u307e\u305fEPICS\u5171\u540c\u7814\u7a76\u306e\u306a\u304b\u3067\u3082\u6d3b\u52d5\u7684\u306a\u30e1\u30f3\u30d0\u306e\u4e00\u4eba\u3067
\n\u3042\u3063\u3066\u3001\u305d\u306e\u8c4a\u5bcc\u306a\u7d4c\u9a13\u306b\u57fa\u3065\u3044\u3066\u5171\u540c\u7814\u7a76\u306e\u9032\u3080\u3079\u304d\u65b9\u5411\u306b\u3064\u3044\u3066\u306e\u8b70\u8ad6\u3092
\n\u30ea\u30fc\u30c9\u3057\u3066\u3044\u308b\u3002\u4eca\u56de\u306f\u3001DESY\u306eCryogenic system \u3084Utitily system\u306e\u5236\u5fa1\u306e
\n\u73fe\u72b6\u3068\u4eca\u5f8c\u3092\u984c\u6750\u306b\u3001\u5236\u5fa1\u30b7\u30b9\u30c6\u30e0\u306e\u4eca\u5f8c\u306e\u65b9\u5411\u6027\u306b\u3064\u3044\u3066\u304a\u8a71\u3044\u305f\u3060\u304f\u3002
\n\u53c2\u8003 (http:\/\/www-kryo.desy.de\/)\n<\/td>\n<\/tr>\n
2004\/03\/09\n<\/td>\nTue.\n<\/td>\n13:30 – 15:00\n<\/td>\n3 \u53f7\u9928 7 \u968e \u4f1a\u8b70\u5ba4\n<\/td>\n\u5cf6\u7530 \u7f8e\u5e06\uff08COE)\n<\/td>\n\u5149\u6563\u4e71\u30e2\u30c7\u30eb\u3092\u7528\u3044\u305f\u76ae\u819a\u3068\u523a\u9752\u306e\u8272\u89e3\u6790\u306b\u95a2\u3059\u308b\u7814\u7a76\n<\/td>\n\u53e4\u5ddd\n<\/td>\n\u50b7\u8de1\u3084\u75e3\u306a\u3069\u3092\u76ee\u7acb\u305f\u306a\u304f\u3059\u308b\u6700\u7d42\u624b\u6bb5\u3068\u3057\u3066\u3001\u533b\u7642\u7528\u523a\u9752\u306b\u3088\u308b\u6cbb\u7642\u304c\u6709
\n\u52b9\u3067\u3042\u308b\u3002\u305d\u306e\u305f\u3081\u8272\u306e\u30b3\u30f3\u30c8\u30ed\u30fc\u30eb\u304c\u91cd\u8981\u3067\u3042\u308b\u304c\u3001\u7d4c\u9a13\u3068\u52d8\u306b\u3088\u3063\u3066\u884c
\n\u308f\u308c\u3066\u3044\u308b\u305f\u3081\u4f55\u5ea6\u3082\u624b\u8853\u3092\u7e70\u308a\u8fd4\u3057\u3066\u3044\u308b\u306e\u304c\u73fe\u72b6\u3067\u3042\u308b\u3002\u76ae\u819a\u4e2d\u306b\u5165\u5c04
\n\u3057\u305f\u53ef\u8996\u5149\u306f\u8907\u96d1\u306b\u6563\u4e71\u304a\u3088\u3073\u5438\u53ce\u3092\u7e70\u308a\u8fd4\u3057\u3001\u305d\u306e\u4f1d\u64ad\u7d4c\u8def\u306f\u6ce2\u9577\u306b\u3088\u3063
\n\u3066\u7570\u306a\u308b\u3002\u307e\u305f\u3001\u751f\u4f53\u3067\u3042\u308b\u305f\u3081\u3001\u500b\u4eba\u5dee\u3084\u90e8\u4f4d\u5dee\u304c\u591a\u304f\u672a\u77e5\u306e\u30d1\u30e9\u30e1\u30fc\u30bf\u30fc
\n\u304c\u591a\u3044\u3002\u3053\u308c\u3089\u306e\u554f\u984c\u3092\u8e0f\u307e\u3048\u3066\u3001\u672c\u7814\u7a76\u3067\u306f\u3001\u5065\u5e38\u8005\u306e\u76ae\u819a\u306e\u8272\u306e\u30e1\u30ab\u30cb
\n\u30ba\u30e0\u306e\u89e3\u660e\u3068\u3001\u5c11\u91cf\u306e\u523a\u9752\u306e\u6295\u4e0e\u3067\u8272\u30b3\u30f3\u30c8\u30ed\u30fc\u30eb\u3092\u884c\u3046\u65b9\u6cd5\u3092\u63d0\u6848\u3059\u308b\u3002\n<\/td>\n<\/tr>\n
2004\/03\/05\n<\/td>\nFri.\n<\/td>\n14:00-15:00\n<\/td>\n\uff12\u53f7\u9928\u4e8c\u968e\u4f1a\u8b70\u5ba4\n<\/td>\nMarc Ross (SLAC)\n<\/td>\nLC availability Simulation\n<\/td>\n\u6d66\u5ddd\n<\/td>\nThe simulation that was given the MTBFs, MTTRs, numbers and redundancies of components, and access requirements for repair can calculate average availability and the integrated luminosity per year. Luminosity is mostly either design or zero in this simulation. We should collect data on MTBFs and MTTRs of components in existing machines to guide our budgeting process and make up a reasonable set of MTBFs that give a reasonable overall availability. We allowed 25% downtime total. 10% was kept as contingency and MTBFs were tuned so the simulation gave 15% downtime.\n<\/td>\n<\/tr>\n
2004\/03\/04\n<\/td>\nThu.\n<\/td>\n13:30-15:00\n<\/td>\n\u4e00\u53f7\u9928\u8ac7\u8a71\u5ba4\n<\/td>\n\u8302\u4e2d\u4fca\u660e\u3000\u4ed6\uff08\u4e09\u83f1\u91cd\u5de5\u5148\u9032\u6280\u8853\u7814\u7a76\u30bb\u30f3\u30bf\u30fc\uff09\n<\/td>\n\u5b87\u5b99\u30fb\u5730\u4e0a\u9593\u30de\u30a4\u30af\u30ed\u6ce2\u4f1d\u642c\u30b7\u30df\u30e5\u30ec\u30fc\u30b7\u30e7\u30f3\u30b3\u30fc\u30c9\u306e\u958b\u767a\n<\/td>\n\u9ad8\u5c71\u3000\u5065\n<\/td>\nNASA, JAXA\u7b49\u306e\u5c06\u6765\u8a08\u753b\u3068\u3057\u3066\u592a\u967d\u5149\u3092\u5b87\u5b99\u3067\u53d7\u5149\u3057\u3001\u96fb\u78c1\u6ce2\u30a8\u30cd\u30eb\u30ae\u30fc\u306b\u5909\u63db\u3057\u3066
\n\u5730\u4e0a\u306b\u9001\u96fb\u3059\u308b\u5b87\u5b99\u767a\u96fb\u69cb\u60f3\u304c\u3042\u308b\u3002\u9759\u6b62\u8ecc\u9053\u306b\u304a\u3044\u305f\u767a\u96fb\u885b\u661f\u4e0a\u306e\u30bd\u30fc\u30e9\u30fc\u30d1\u30cd\u30eb
\n\u306b\u3088\u308a\u4e00\u65e6\u96fb\u6c17\u30a8\u30cd\u30eb\u30ae\u30fc\u306b\u5909\u63db\u3057\u3001\u3055\u3089\u306b\u9069\u5f53\u306a\u5909\u63db\u88c5\u7f6e\u3067\u5909\u63db\u3055\u308c\u305fC-band, X-
\nband\u306e\u30de\u30a4\u30af\u30ed\u6ce2\u3092\u5730\u4e0a\u306b\u9001\u308a\u3001\u305d\u3053\u306b\u7f6e\u3044\u305f\u30ec\u30af\u30c6\u30ca\u30a2\u30f3\u30c6\u30ca\u3067\u53d7\u4fe1\u3057\u3001\u6700\u7d42\u7684\u306b
\nACPower\u3068\u3057\u3066\u5f97\u308b\u4e8b\u3092\u76ee\u7684\u3068\u3057\u3066\u3044\u308b\u3002\u6280\u8853\u7684\u30d5\u30a3\u30b8\u30d3\u30ea\u30c6\u30a4\u30fc\u306b\u3064\u3044\u3066\u306f1970\u5e74
\n\u4ee3\u5f8c\u534a\u304b\u3089\u7c73\u56fd\u3067\u8abf\u67fb\u3055\u308c\u3001\u73fe\u5728\u3067\u3082\u7c73\u3068\u65e5\u3092\u4e2d\u5fc3\u3068\u3057\u3066\u7814\u7a76\u304c\u9032\u884c\u4e2d\u3067\u3042\u308b\u3002\u52ff\u8ad6\u3001
\n\u793e\u4f1a\u7684\u53d7\u5bb9\u6027\u306b\u3064\u3044\u3066\u306f\u307e\u3060\u591a\u304f\u306e\u8b70\u8ad6\u306e\u4f59\u5730\u3092\u6b8b\u3059\u3002\u5b9f\u969b\u3001\u60f3\u5b9a\u3055\u308c\u3066\u3044\u308b\u904b\u7528\u30b9
\n\u30b1\u30fc\u30eb\u306e\u30de\u30a4\u30af\u30ed\u6ce2\u304c\u5730\u4e0a500km\u306e\u5b87\u5b99\u570f\u304b\u3089\u5730\u4e0a\u307e\u3067\u3069\u3046\u4f1d\u642c\u3059\u308b\u304b\u306e\u30c7\u30fc\u30bf\u306f\u3053
\n\u308c\u307e\u3067\u5b58\u5728\u3057\u306a\u3044\u3002\u6700\u8fd1\u3001\u6211\u304c\u30b0\u30eb\u30fc\u30d7\u306f\u3053\u306e\u4f1d\u9001\u8def\u306b\u5b58\u5728\u3059\u308b\u65e5\u5909\u5316\u3001\u5b63\u7bc0\u5909\u5316\u3057\u3001
\n\u4e14\u3064\u9ad8\u5ea6\u4f9d\u5b58\u6027\u3092\u6301\u3063\u305f\u8a98\u96fb\u7387\u3001\u5730\u78c1\u6c17\u7b49\u306e\u5927\u6c17\u74b0\u5883\u30d1\u30e9\u30e1\u30fc\u30bf\u30fc\u3092\u53d6\u308a\u8fbc\u3093\u3067\u3001\u76f4
\n\u5f84100m\u306e\u30d1\u30e9\u30dc\u30ca\u30a2\u30f3\u30c6\u30ca\u304b\u3089\u767a\u5c04\u3055\u308c\u305f\u96fb\u78c1\u6ce2\u306e\u4f1d\u642c\u3092\u8ffd\u3046\u30b7\u30df\u30e5\u30ec\u30fc\u30b7\u30e7\u30f3\u30b3\u30fc
\n\u30c9\u3092\u958b\u767a\u3057\u305f\u3002\u3053\u308c\u306b\u3088\u308a\u3001\u53d7\u4fe1\u7528\u30ec\u30af\u30c6\u30ca\u30a2\u30f3\u30c6\u30ca\u306e\u5fc5\u8981\u30b5\u30a4\u30ba\u3084\u7acb\u3061\u5165\u308a\u7981\u6b62\u9818
\n\u57df\u306e\u5927\u304d\u3055\u306b\u3064\u3044\u3066\u898b\u7a4d\u3082\u308a\u304c\u306a\u3055\u308c\u308b\u3002\u958b\u767a\u3057\u305f\u30b3\u30fc\u30c9\u306fMaxwell\u65b9\u7a0b\u5f0f\u3092Alterna
\nting Direct Implicit Method\u3092\u4f7f\u3063\u3066\u96e2\u6563\u5316\u3057\u3001\u900f\u904e\u6cd5\u3092\u7528\u3044\u305f\u5883\u754c\u6761\u4ef6\u306e\u51e6\u7406\u306b
\n\u3088\u3063\u3066\u5de8\u5927\u7a7a\u9593\u3067\u306e\u4f1d\u642c\u3092\u8ffd\u3046\u4e8b\u3092\u53ef\u80fd\u306b\u3057\u305f\u3002\u30bb\u30df\u30ca\u30fc\u3067\u306f\u30b3\u30fc\u30c9\u306e\u4e0a\u8a18\u7279\u5fb4\u3092\u89e3
\n\u8aac\u3059\u308b\u3068\u5171\u306b\u3001\u30b3\u30fc\u30c9\u691c\u8a3c\u3001\u30b9\u30fc\u30d1\u30fc\u30b3\u30f3\u30d4\u30e5\u30fc\u30bf\u30fc\u3092\u7528\u3044\u305f\u8a08\u7b97\u4f8b\u3092\u7c21\u5358\u306b\u7d39\u4ecb\u3059\u308b\u3002
\n\n<\/td>\n<\/tr>\n
2004\/02\/25\n<\/td>\nWed.\n<\/td>\n10:00-\n<\/td>\nKEKB\u5236\u5fa1\u68df\u4f1a\u8b70\u5ba4\n<\/td>\nR.Dostovalov (BINP)\n<\/td>\nVacuum Studies in the BINP\n<\/td>\n\u672b\u6b21\n<\/td>\n\u30c1\u30a7\u30f3\u30d0\u30fc\u8868\u9762\u304b\u3089\u306e\u5149\u96fb\u5b50\u653e\u51fa\u6e2c\u5b9a\u306a\u3069
\nBINP\u3067\u884c\u308f\u308c\u3066\u3044\u308b\u771f\u7a7a\u95a2\u9023\u306e\u7814\u7a76\u306b\u3064\u3044\u3066\n<\/td>\n<\/tr>\n
2004\/02\/24\n<\/td>\nTue.\n<\/td>\n14:00\n<\/td>\n\uff12\u53f7\u9928\u4e8c\u968e\u4f1a\u8b70\u5ba4\n<\/td>\nJie Gao (LAL \/ CNRS\u3001\u30aa\u30eb\u30bb\u30fc)\n<\/td>\nAnalytical estimation of the dynamic aperture limited by wigglers in a storage ring
\n\n<\/td>\n		\u6d66\u5ddd\u9806\u6cbb\n<\/td>\nBy solving first analytically the problem of dynamic aperture limited by a single multipole located in a storage ring, we derived the corresponding analytical formulae including the combined effect from different multipoles, which are checked with numerical simulation results. As a specific case, we apply the general multipole limited dynamic aperture formulae to the dynamic apertures limited by single or multi wigglers in a storage ring, and the analytical results are checked with numerical values.
\n
\n\u84c4\u7a4d\u30ea\u30f3\u30b0\u5185\u306b\u591a\u6975\u6210\u5206\u3092\u4eee\u5b9a\u3057\u305f\u5834\u5408\u306e\u52d5\u7684\u30a2\u30d1\u30fc\u30c1\u30e3\u3078\u306e\u5f71\u97ff\u3092\u89e3\u6790\u7684\u306b\u89e3\u304f\u3053\u3068\u306b\u3088\u308a\u3001\u591a\u6975\u6210\u5206\u306b\u5bfe\u5fdc\u3059\u308b\u5f0f\u3092\u5c0e\u3044\u305f\u3002\u3053\u306e\u5f0f\u3068\u6570\u5024\u8a08\u7b97\u306b\u3088\u308b\u7d50\u679c\u3092\u6bd4\u8f03\u3057\u305f\u3002\u7279\u5225\u306a\u5834\u5408\u3068\u3057\u3066\u3001\u30de\u30eb\u30c1\u30a6\u30a4\u30b0\u30e9\u30fc\u304c\u84c4\u7a4d\u30ea\u30f3\u30b0\u5185\u306b\u3042\u308b\u3070\u3042\u3044\u306b\u3064\u3044\u3066\u691c\u8a0e\u3057\u305f\u3002\n<\/td>\n<\/tr>\n
2004\/02\/23\n<\/td>\nMon.\n<\/td>\n13:30-\n<\/td>\n3\u53f7\u99287\u968e\u4f1a\u8b70\u5ba4\n<\/td>\nLiu Bo, Pei Shilun\n<\/td>\nLiu Bo\u3000”Introduction to the Elctron Gun System for BEPCII “<\/p>\n

Pei Shilun “Some Topics of BEPCII Linac”\n<\/td>\n

\u5927\u6ca2\n<\/td>\n\n<\/td>\n<\/tr>\n
2004\/02\/18\n<\/td>\nWed.\n<\/td>\n14:00-15:00\n<\/td>\n\uff14\u53f7\u9928\uff11\u968e\u30bb\u30df\u30ca\u30fc\u30db\u30fc\u30eb\n<\/td>\nProf. Georg Hoffstaetter (Cornell University)\n<\/td>\nThe Cornell ERL Project\n<\/td>\n\u8acf\u8a2a\u7530\u525b\n<\/td>\nSynchrotron light sources based on Energy Recovery Linacs (ERLs) show
\npromise to deliver X-ray beams with both brilliance and X-ray pulse
\nduration superior to the values that can be achieved with storage
\nring technology. Cornell University, in collaboration with Jefferson
\nLaboratory, has proposed the construction of a prototype ERL. This
\n100MeV, 100mA CW superconducting electron accelerator will be used to
\nstudy and resolve the many accelerator physics and technology issues
\nof this type of machine. Furthermore, a study that incorporates
\nCornell’s CESR e+\/e- ring into a 5 GeV ERL X-ray facility is under
\ndevelopment. Such a facility is planed to be formally proposed after
\nsuccess of the prototype ERL.
\n\n<\/td>\n<\/tr>\n
2004\/01\/29\n<\/td>\nThu.\n<\/td>\n10:00-11:30\n<\/td>\n\uff11\u53f7\u9928\u4f1a\u8b70\u5ba4\n<\/td>\n\u516b\u4e95\u3000\u6d44(\u9577\u5ca1\u6280\u8853\u79d1\u5b66\u5927\u5b66\u30bb\u30f3\u30bf\u30fc\u9577)\u3001\u6c5f\u3000\u5049\u83ef\uff08\u9577\u5ca1\u6280\u79d1\u5927\uff09\n<\/td>\n\u30d1\u30eb\u30b9\u30d1\u30ef\u30fc\u6280\u8853\u306e\u9032\u5c55
\n\uff08\uff11\uff09\u9577\u5ca1\u6280\u8853\u79d1\u5b66\u5927\u5b66\u6975\u9650\u30a8\u30cd\u30eb\u30ae\u30fc\u5bc6\u5ea6\u5de5\u5b66\u7814\u7a76\u30bb\u30f3\u30bf\u30fc\u306e\u5168\u4f53\u7684\u6982\u8981\u3068\u3000\u3000
\n\u3000\u3000\u3000\u7814\u7a76\u6210\u679c\u3000\u3000\u3000\u3000\u3000\u3000\u3000\u3000\u3000\u3000\u3000\u3000\u3000\u3000\u3000\u3000\u3000\u516b\u4e95\u3000\u6d44\uff08\u30bb\u30f3\u30bf\u30fc\u9577\uff09
\n\uff08\uff12\uff09\u534a\u5c0e\u4f53\u30b9\u30a4\u30c3\u30c1\u3092\u7528\u3044\u305f\u30d1\u30eb\u30b9\u30d1\u30ef\u30fc\u96fb\u6e90\u3000\u3000\u6c5f\u3000\u5049\u83ef\uff08\u9577\u5ca1\u6280\u79d1\u5927\uff09\n<\/td>\n		\u9ad8\u5c71\n<\/td>\n\u30d1\u30ef\u30fc\u534a\u5c0e\u4f53\u30c7\u30d0\u30a4\u30b9\u3068\u3057\u3066\u30b7\u30ea\u30b3\u30f3\u30c0\u30a4\u30aa\u30fc\u30c9\u304c\u6700\u521d\u306b\u5b9f\u7528\u5316\u3055\u308c\u30011957\u5e74\u306b\u7c73\u56fd
\n\u3067\u767a\u660e\u3055\u308c\u305f\u30b5\u30a4\u30ea\u30b9\u30bf\u306b\u3088\u308a\u30d1\u30ef\u30fc\u30a8\u30ec\u30af\u30c8\u30ed\u30cb\u30af\u30b9\u306e\u672c\u683c\u7684\u5c55\u958b\u306e\u6642\u4ee3\u304c\u59cb\u307e\u3063
\n\u305f\u3068\u8a00\u3063\u3066\u826f\u3044\u3002\u4ee5\u964dGTO(\u30b2\u30fc\u30c8\u30bf\u30fc\u30f3\u30aa\u30d5\u30b5\u30a4\u30ea\u30b9\u30bf\uff09\u3001MOSFET, SI\u30b5\u30a4\u30ea\u30b9\u30bf\u3001
\nIGBT\u304c\u767b\u5834\u3059\u308b\u306b\u53ca\u3073\u3001\u7d20\u5b50\u5358\u4f53\u306e\u30a8\u30cd\u30eb\u30ae\u30fc\u5909\u63db\u5bb9\u91cf\uff08V\u30fbA\uff09\u3068\u52d5\u4f5c\u5468\u6ce2\u6570\uff08Hz\uff09
\n\u306e\u30d5\u30ed\u30f3\u30c6\u30a4\u30a2\u30fc\u306f\u5e74\u3005\u9032\u5316\u3057\u3066\u3044\u307e\u3059\u3002\u52a0\u901f\u5668\u306b\u7528\u3044\u3089\u308c\u308b\u5404\u7a2e\u96fb\u6e90\u3092\u69cb\u6210\u3059\u308b\u30d1
\n\u30ef\u30fc\u30b3\u30f3\u30dd\u30fc\u30cd\u30f3\u30c8\u304c\u3053\u308c\u3089\u30d1\u30ef\u30fc\u534a\u5c0e\u4f53\u30c7\u30d0\u30a4\u30b9\u306b\u7f6e\u304d\u63db\u3048\u3089\u308c\u3064\u3064\u3042\u308b\u4e8b\u306f\u7686\u3055
\n\u3093\u304c\u65e5\u5e38\u7684\u306b\u898b\u805e\u304d\u3057\u3066\u304a\u3089\u308c\u308b\u901a\u308a\u3067\u3059\u3002\u4eca\u56de\u306e\u30bb\u30df\u30ca\u30fc\u3067\u306f\u8b1b\u5e2b\u306e\u65b9\u3005\u306eKEK\u898b
\n\u5b66\u306e\u6a5f\u4f1a\u3092\u6349\u3048\u3001\u6240\u5c5e\u3055\u308c\u308b\u6a5f\u95a2\u3067\u306e\u30d1\u30ef\u30fc\u534a\u5c0e\u4f53\u30c7\u30d0\u30a4\u30b9\u3092\u4f7f\u3063\u305f\u96fb\u6e90\u306e\u958b\u767a\u3068\u305d
\n\u306e\u8208\u5473\u3042\u308b\u5fdc\u7528\u306b\u3064\u3044\u3066\u8b1b\u6f14\u3092\u304a\u9858\u3044\u3057\u307e\u3057\u305f\u3002\n<\/td>\n<\/tr>\n
2004\/01\/21\n<\/td>\nWed.\n<\/td>\n15:00-\n<\/td>\n2\u53f7\u9928 2F\u3000\u4f1a\u8b70\u5ba4\n<\/td>\nMauro Paoluzzi\n<\/td>\nRF Acceleration System for CERN-LEIR\n<\/td>\n\u5927\u68ee\n<\/td>\nCERN-LEIR\u7a7a\u6d1e\u3068\u9ad8\u5468\u6ce2\u6e90\u306b\u3064\u3044\u3066\u8ff0\u3079\u308b\u3002\u7279\u8cea\u306b\u3064\u3044\u3066\u306e\u8aac\u660e\u53ca\u3073\u5c0f\u578b\u30e2\u30c7\u30eb\u3067\u306e\u6e2c\u5b9a\u306b\u3064\u3044\u3066\u8b70\u8ad6\u3059\u308b\u3002(\u653e\u533b\u7814\u306eHIMAC\u91d1\u5c5e\u78c1\u6027\u4f53\u7a7a\u6d1e\u306e\u6e2c\u5b9a\u7d50\u679c\u306b\u57fa\u3065\u304d)2\u3064
\n\u306e\u7a7a\u6d1e\u30fc\u30a2\u30f3\u30d7\u7d50\u5408\u65b9\u5f0f\u306e\u5468\u6ce2\u6570\u5fdc\u7b54\u306b\u3064\u3044\u3066\u5831\u544a\u3057\u3001\u73fe\u5728\u306e\u65b9\u5f0f\u306b\u3064\u3044\u3066\u8a55\u4fa1\u3059\u308b\u3002\u53c8\u3001\u30d7\u30ed\u30b8\u30a7\u30af\u30c8\u306e\u72b6\u6cc1\u306b\u3064\u3044\u3066\u3082\u5831\u544a\u3055\u308c\u308b\u3002
\n\n<\/td>\n<\/tr>\n
2004\/01\/20\n<\/td>\nTue.\n<\/td>\n15:00-16:00\n<\/td>\n4th building, Seminar Hall\n<\/td>\nH. Sagawa(KEK)\n<\/td>\nUpdate of CP Violation Study on B0->pi+pi- Decay\n<\/td>\nIchiro Adachi (phs: 4640)\n<\/td>\nBelle’s previous results for B0->pi+pi- decays based on a 78\/fb
\n suggested large direct CP asymmetry and\/or mixing-induced asymmetry.
\n Here we report a measurement with an improved analysis that
\n incorporates an additional 62\/fb for a total of 140\/fb.\n<\/td>\n<\/tr>\n
2004\/01\/16\n<\/td>\nFri.\n<\/td>\n15:00-\n<\/td>\n2\u53f7\u9928 2F\u3000\u4f1a\u8b70\u5ba4\n<\/td>\nMauro Paoluzzi\n<\/td>\nRF Acceleration System for CERN-PSB\n<\/td>\n\u5927\u68ee\n<\/td>\nCO2\u53ca\u3073CO4(\u57fa\u672c\u6ce2\u30682\u6b21\u9ad8\u8abf\u6ce2\u9ad8\u5468\u6ce2\u7cfb\uff09\u306e\u914d\u7f6e\u53ca\u3073\u4e3b\u306a\u7279\u6027\u3068\u6e2c\u5b9a\u7d50\u679c\u306b\u3064\u3044\u3066\u8ff0\u3079\u308b\u3002\u53c8\u3001\u9ad8\u5468\u6ce2\u30d5\u30a7\u30fc\u30c9\u30d0\u30c3\u30af\u304c\u4e3b\u306a\u5185\u5bb9\u3068\u306a\u308b\u304c\u3001\u30d5\u30a7\u30e9\u30a4\u30c8\u306a\u3044\u3067\u306eHLM\u306b\u8d77\u56e0\u3059\u308b\u52b9\u679c\u306b\u3064\u3044\u3066\u3082\u5831\u544a\u3055\u308c\u308b\u3002\n<\/td>\n<\/tr>\n
2003\/12\/22\n<\/td>\nMon.\n<\/td>\n13:30-\n<\/td>\n2Gokan 2F Meeting room\n<\/td>\n\u543e\u90f7\u667a\u7d00\n<\/td>\nMesh\u8a08\u7b97\u306b\u3088\u308bCSR\u306e\u89e3\u6790\n<\/td>\n\u5927\u898b\n<\/td>\nERL\u3084FEL\u306a\u3069\u306e\u6b21\u4e16\u4ee3\u5149\u6e90\u306b\u304a\u3044\u3066\u3001Coherent \u653e\u5c04\uff08CSR\uff09\u306e\u5f71\u97ff\u306f\u91cd\u8981\u306a\u8981\u7d20\u306e
\n\u3072\u3068\u3064\u3067\u3042\u308b\u3002
\n\u3053\u3053\u3067\u306fMesh\u8a08\u7b97\u306b\u3088\u308bCSR\u89e3\u6790\u306e\u624b\u6cd5\u3092\u793a\u3059\u3002
\n\u9ad8\u30a8\u30cd\u30eb\u30ae\u30fc\u3067\u306fsynchrotron radiation\u306f\u9ad8\u5468\u6ce2\u306e\u6210\u5206\u3092\u542b\u3080\u305f\u3081\u306b\u3001\u96fb\u78c1\u5834\u306eMesh\u8a08\u7b97\u306f\u56f0\u96e3\u3067\u3042\u308b\u304c\u3001
\nFrequency\u3000Domain\u306b\u304a\u3044\u3066\u653e\u5c04\u306e\u5468\u6ce2\u6570\u6210\u5206\u306e\u4e2d\u304b\u3089\u4f4e\u5468\u6ce2\u306e\u307f\u3092\u53d6\u308a\u51fa\u3059\u3053\u3068\u3067\u3001
\nCSR\u306eMesh\u8a08\u7b97\u304c\u53ef\u80fd\u3068\u306a\u308b\u3002
\n\u30d3\u30fc\u30e0\u30d1\u30a4\u30d7\u3092\u5883\u754c\u6761\u4ef6\u3068\u3057\u3066\u4e0e\u3048\u3001Frequency\u3000Domain\u306b\u304a\u3051\u308bMaxwell\u65b9\u7a0b\u5f0f\u3092\u6570\u5024\u7684\u306b
\n\u89e3\u304f\u3053\u3068
\n\u306b\u3088\u308a\u3001CSR\u306e\u5834\u3092\u89e3\u6790\u3059\u308b\u3053\u3068\u304c\u53ef\u80fd\u3067\u3042\u308b\u3053\u3068\u3092\u793a\u3059\u3002
\n\u3053\u3053\u3067\u306f\u30d3\u30fc\u30e0\u30d1\u30a4\u30d7\u306e\u65ad\u9762\u306f\u9577\u65b9\u5f62\u3068\u3057\u3066\u8a08\u7b97\u3092\u884c\u3063\u305f\u304c\u3001\u3053\u306e\u624b\u6cd5\u306f\u4efb\u610f\u306e\u5f62\u72b6\u306e\u30d1\u30a4\u30d7\u306b
\n\u9069\u7528\u3067\u304d\u308b\u3002
\n\n<\/td>\n<\/tr>\n
2003\/11\/27\n<\/td>\nThu.\n<\/td>\n13:30-\n<\/td>\n2Gokan 2F Meeting room\n<\/td>\n\u91d1\u9280\u5c71\u6c0f\n<\/td>\nLattice design and Beam blowup in a 200 MeV Energy Recovery Linac Test Facility\n<\/td>\n\u5927\u898b\n<\/td>\nWe present an overview of the lattice design and beam parameters for the 200 MeV ERL test facility at KEK. Beam blowup due to the superconducting rf cavities and coherent synchrotron radiation in the designed test facility is also investigated.
\n
\n\u6a5f\u69cb\u30bb\u30df\u30ca\u30fc\u60c5\u5831<\/a>\n<\/td>\n<\/tr>\n
2003\/11\/25\n<\/td>\nTue.\n<\/td>\n15:00-\n<\/td>\n#3Bld. 1F Meeting room\n<\/td>\nDr. Gennady A. Naumenko (Tomsk Polytechnic University, Russia)\n<\/td>\nBeam Test Proposal of an Optical Diffraction Radiation Beam Size Monitor at the SLAC FFTB and
\nPreliminary Experimental Plan at ATF for this Proposal\n<\/td>\n		\u6d66\u5ddd\n<\/td>\nTreatments of the usage of diffraction radiation from the relativistic electrons moving through
\na conductive slit for the transverse beam size measurement encounter hard limitation of the method
\nsensitivity for the electron energy much larger than 1 GeV. These limitations are connected with
\na small response of ODR yield on the beam size in comparison with SR background and with a large
\nnear field zone effect for very high Lorenz-factor, such as it is at SLAC FFTB. We consider here
\na possibility of application of the artificial phase shift on a slit target, which is very sensitive
\nto the transverse electron position and may allow increasing significantly the method sensitivity.
\nFor near field zone problem on resolution the model for calculation of ODR from a real size slit
\ntarget in near field zone was developed. Usage of this model actually shows a large distortion
\nof ODR angular distribution in near field zone for high value of Lorenz-factor. To another side,
\nthis model shows the possibility of near field zone effect removing using an optical system in
\nthe ODR path. This allows us to realize the measurements of a small transverse size of supper
\nrelativistic electron beams. Some tests of this technique at ATF are possible.
\nOHP<\/a><\/td>\n<\/tr>\n
2003\/11\/6\n<\/td>\nThu.\n<\/td>\n13:30-\n<\/td>\n2\u53f7\u99282\u968e\u4f1a\u8b70\u5ba4\n<\/td>\nG.Rumolo (GSI)\u6c0f\n<\/td>\nELECTRON CLOUD IN THE GSI-SIS18
\n AND ROLE OF ELASTICALLY REFLECTED ELECTRONS
\n\n<\/td>\n		\u5927\u898b\n<\/td>\nAccording to the GSI future project, the existing synchrotron SIS18 will
\nbe upgraded to be used as an injector for the planned larger synchrotron
\nSIS100. All possible operation scenarios require the acceleration in the
\nSIS18 of 4×10^(10) U^(73+) (either packed in 4 80ns long bunches with a
\n100ns spacing, or in one single uniform long -500 ns- bunch) up to 1
\nGeV\/u.
\nAn electron cloud can therefore form in the machine, as the intensities
\nwill be pushed to these unprecedented high values.
\nWe study numerically the SEY threshold for the onset of the electron cloud
\nbuild up and the possible resulting bunch instabilities.
\nWe stress the importance of low energy reflected electrons in the process,
\nreferring to recent measurements which have led to a new SEY
\nparametrization in which the probability of reflection becomes 1 for
\nvanishing energy of the incident electron.
\nThe importance of rediffused electrons in simulations is also finally
\nshortly addressed as subject presently under study.
\n\n<\/td>\n<\/tr>\n
2003\/11\/4\n<\/td>\nTue.\n<\/td>\n10:00-\n<\/td>\n\uff12\u53f7\u9928\uff16\u968e\uff16\uff10\uff11\u5ba4 \n<\/td>\n\u4f50\u85e4\u3000\u5065\u6b21 (\u5927\u962a\u5927\u5b66\u6838\u7269\u7406\u7814\u7a76\u30bb\u30f3\u30bf\u30fc) \n<\/td>\n\u30b7\u30f3\u30af\u30ed\u30fb\u30b5\u30a4\u30af\u30ed\u30c8\u30ed\u30f3\u306e\u6e26\u5dfb\u304d\u52a0\u901f\u904b\u52d5\u306e\u65b0\u305f\u306a\u89e3\u6cd5\n<\/td>\n\u753a\u7530\n<\/td>\n\n<\/td>\n<\/tr>\n
2003\/10\/28\n<\/td>\nTue.\n<\/td>\n10:30-\n<\/td>\nKEKB\u5236\u5fa1\u68df\u4f1a\u8b70\u5ba4
\n\n<\/td>\n		Dr. Shen GuoBao
\n\n<\/td>\n		my experience with EPICS in SSRC, China\n<\/td>\n\u5c71\u672c\n<\/td>\n\n<\/td>\n<\/tr>\n
2003\/07\/30\n<\/td>\nWed.\n<\/td>\n15:00-\n<\/td>\n2\u53f7\u99282\u968e\u4f1a\u8b70\u5ba4\n<\/td>\n\u751f\u51fa\u52dd\u5ba3\n<\/td>\nBINP\u8a2a\u554f\u9332\n<\/td>\n\u5927\u898b\n<\/td>\n7\/16-20\u306bBINP(Novosibirsk)\u3092\u8a2a\u554f\u3057\u305f\u306e\u3067\u3001\u5199\u771f\u3092\u4e2d\u5fc3\u306b\u3001
\n\u5f7c\u7b49\u306e\u52a0\u901f\u5668\u5de5\u5834\u30fbLinac\u30fbERL\u7b49\u306e\u7d39\u4ecb\u3092\u3057\u305f\u3044\u3068\u601d\u3044\u307e\u3059\u3002\n<\/td>\n<\/tr>\n
2003\/07\/10\n<\/td>\nThu\n<\/td>\n10:00-11:00\n<\/td>\n1\u53f7\u9928\u8ac7\u8a71\u5ba4\n<\/td>\nWeiren Chou (FNAL)\n<\/td>\nRF barrier studies at FNAL\n<\/td>\n\u9ad8\u5c71\u5065\n<\/td>\n\n<\/td>\n<\/tr>\n
2003\/06\/04\n<\/td>\nWed.\n<\/td>\n15:30-\n<\/td>\n2\u53f7\u99282\u968e\u4f1a\u8b70\u5ba4\n<\/td>\n\u5927\u897f\u5e78\u5584\n<\/td>\nFour \u30d3\u30fc\u30e0\u30b9\u30ad\u30fc\u30e0\u306e beam-beam simulation\n<\/td>\n\u5927\u898b\n<\/td>\n\u73fe\u5728B\u30d5\u30a1\u30af\u30c8\u30ea\u30fc\u30de\u30b7\u30f3\u3067\u3042\u308bKEKB\u52a0\u901f\u5668\u306f\u3001\u305d\u306e\u30c7\u30b6\u30a4\u30f3\u30eb\u30df\u30ce\u30b7\u30c6\u30a3\u30fc\u3067\u3042\u308b10^34 \/cm^2\/s\u3092\u9054\u6210\u3057\u3066\u3044\u308b\u3002\u5c06\u6765\u3001\u3055\u3089\u306b\uff11\uff10\u500d\u304b\u3089\uff11\uff10\uff10\u500d\u306e\u8d85\u9ad8\u30eb\u30df\u30ce\u30b7\u30c6\u30a3\u30fc\u3092\u76ee\u6307\u3057\u305fKEKB\u52a0\u901f\u5668\u306e\u30a2\u30c3\u30d7\u30b0\u30ec\u30fc\u30c9\u8a08\u753b\u304c\u3042\u308b\u3002\u3053\u3046\u3057\u305f\u8d85\u9ad8\u30eb\u30df\u30ce\u30b7\u30c6\u30a3\u30fc\u3092\u5b9f\u73fe\u3059\u308b\u305f\u3081\u306b\u306f\u73fe\u5b58\u306e\u30c7\u30b6\u30a4\u30f3\u30fb\u30b3\u30f3\u30bb\u30d7\u30c8\u3092\u8e0f\u8972\u3059\u308b\u3053\u3068\u4ee5\u5916\u306b\u3001\u305d\u308c\u3068\u306f\u7570\u306a\u308b\u30c7\u30b6\u30a4\u30f3\u30fb\u30b3\u30f3\u30bb\u30d7\u30c8\u306e\u53ef\u80fd\u6027\u3092\u8ffd\u6c42\u3059\u308b\u5fc5\u8981\u304c\u3042\u308b\u3002\u305d\u306e\u4e2d\u306e\u4e00\u3064\u306bfourbeams\u304c\u3042\u308b\u3002\u305d\u306e\u30b9\u30ad\u30fc\u30e0\u3092beam-beam\u3000simulation\u306b\u3088\u3063\u3066\u8abf\u3079\u305f\u306e\u3067\u3001\u305d\u306e\u7d50\u679c\u3092\u5831\u544a\u3059\u308b\u3002\n<\/td>\n<\/tr>\n
2003\/04\/16\n<\/td>\nWed.\n<\/td>\n13:30-\n<\/td>\n3\u53f7\u99287\u968e\u4f1a\u8b70\u5ba4\n<\/td>\nDr. Vladimir Foguel (BINP\/KEK)\n<\/td>\nDevelopment of the IGBT Induction Modulator for JLC\n<\/td>\n\u9673\u3000\u6804\u6d69\n<\/td>\nJLC\u8a08\u753b\u306e\u305f\u3081\u306b\u73fe\u5728\u958b\u767a\u4e2d\u306eIGBT\u534a\u5c0e\u4f53\u30b9\u30a4\u30c3\u30c1\u3092\u4f7f\u3063\u305f\u8a98\u5c0e\u578b\u5909\u8abf\u5668\u306b\u3064
\n\u3044\u3066\u5305\u62ec\u7684\u306a\u8a71\u3092\u3057\u307e\u3059\u3002
\n\n<\/td>\n<\/tr>\n<\/tbody>\n<\/table>\n

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