PPT-Beam Induced heating and bunch length dependence
Author : dsuser1 | Published Date : 2020-06-17
Jan Uythoven with input from RAssmann MBarnes FCaspers SClaudet HDay LGentini AGrudiev EMétral BSalvant CZannini Heating due to Beam Impedance
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Beam Induced heating and bunch length dependence: Transcript
Jan Uythoven with input from RAssmann MBarnes FCaspers SClaudet HDay LGentini AGrudiev EMétral BSalvant CZannini Heating due to Beam Impedance. Y.Susaki,KEK-ACCL. 13 Jan, 2010. Low Emittance Rings 2010, CERN. Positron beam emits synchrotron radiation. Electrons are produced at the chamber wall by photoemission. Electrons are attracted and interact with the positron beam. Outline. The CLIC feasibility issues in CTF3 – 2010 Objectives. Present . status & outlook. Drive Beam Generation. RF power production & structure tests. Two Beam Issues. Other issues. Operating scenario for 2010, conclusions. Yue Hao. Collider-Accelerator Department. Brookhaven National Laboratory. Jan 10, 2009 EIC Meeting at Stony Brook. Outline. Beam-beam effect on the Electron beam. Beam distribution disruption. Mismatch with the design lattice. . for Linac-4. A.V.Feschenko. Institute For Nuclear Research (INR), Moscow 117312, Russia. 2. For . f. =352.2 . MHz. phase resolution of . 1. . is equivalent to time resolution of . 8 . ps. .. SuperKEKB. Y.Susaki,KEK. -ACCL. 9. Feb, . 2010. KEK seminar. Positron beam emits synchrotron radiation. Electrons are produced at the chamber wall by photoemission. The electrons . are attracted and interact with the positron beam. schemes. plus comments on BCMS and 8b+4e. S. Gilardoni BE/ABP. In collaboration with: H. . Bartosik. , H. . Damerau. , B. Goddard,. V. . Kain. , G. . . Rumolo. , . G. . Sterbini. h=7. b. sp. ≈ 330 ns (4 - 6 b.) . . for Linac-4. A.V.Feschenko. Institute For Nuclear Research (INR), Moscow 117312, Russia. 2. For . f. =352.2 . MHz. phase resolution of . 1. . is equivalent to time resolution of . 8 . ps. .. . . KIM . Joon. . Yeon. , KIM Do . Gyun. , BHANG . Hyoung. Chan, KIM . Jong. Won. 1. , YUN Chong Chul. 2. Seoul National University, Department of Physics & Astronomy. . 1. National Cancer Center. . BI IL/CLIC Beam Dynamics Workshop . –. 25. th. . of June 2009. CLIC Beam Instrumentation Challenges. Introduction. Beam . instrumentation. Challenges. Update . from CLIC Beam Instrumentation workshop in June 2009. David Johnson, Todd Johnson. US-Japan Collaboration Meeting. 14-March-2018. Lasers for Accelerators. Lasers have been used for laser profile monitors; SNS, BNL, JPARC, …and . H. -. . g. -> H. Wakefield issues). ATF TB Mtg. 201502. K.Kubo. Intensity dependence of IP . b. eam size. Studies using on-mover structures. Beam size at IP. Orbit change. OTR . chamber wake. Some new . reports. Updated . Louise Cowie . on behalf of the XARA . team at Daresbury Lab. High Gradient Workshop 2019. CLARA . S-band linear acceleration up to 250 MeV. Bunch charge 20-250 . pC. High repetition rate up to 400 Hz. S. Gilardoni BE/ABP. In collaboration with: H. . Bartosik. , H. . Damerau. , B. Goddard,. V. . Kain. , G. . . Rumolo. , . G. . Sterbini. h=7. b. sp. ≈ 330 ns (4 - 6 b.) . . h=21. b. sp.≈100 ns (18 b.) . Slides and animations from Marco Lonza. Sincrotrone Trieste - Elettra. Hermann . Schmickler. CAS 2013 - Trondheim. 2. Outline. . Introduction. Basics of feedback systems. Feedback system components.
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