Parametric Study of CSR in the MEIC CCR

Slides:



Advertisements
Similar presentations
Nominal and no CSR (R 56-1 = 55 mm, R 56-2 = 59 mm, R 56-3 = 0) L1 phase = 21 deg, V 3.9 = 55 MV CSR OFF BC3 OFF Elegant Tracking  z1 = mm (post.
Advertisements

Optical parameters of dipoles for the DAFNE upgrade M. Preger 6/11/2007.
Short bunches in SPEAR J. Safranek for the SPEAR3 accelerator group November 2, 20101J. Safranek CLS THz Workshop.
Radiation Physics | ELBE | SRF Photo Injector for Electron- Laser Interaction LA 3 NET conference: Laser applications at accelerators, Mallorca,
Bunch compressor design for eRHIC Yichao Jing and Vladimir Litvinenko FLS2012, Newport News, VA 3/8/2012.
1 Energy-Phase Rotation with a proton absorber David Neuffer September 27, 2011.
Space Charge Electric-Field Calculations for Coherent Tune Shift Estimations using the Electron-cloud Modelling Algorithm ECLOUD Jim Crittenden Cornell.
C.Limborg-Deprey Beam Dynamics Justifying L01 November 3 rd 2004 Beam Dynamics Justifications of modification of.
Simulation of direct space charge in Booster by using MAD program Y.Alexahin, N.Kazarinov.
Simulation of direct space charge in Booster by using MAD program Y.Alexahin, A.Drozhdin, N.Kazarinov.
Page 1 Overview and Issues of the MEIC Interaction Region M. Sullivan MEIC Accelerator Design Review September 15-16, 2010.
Observations of Beam Filamentation at SLM5F02 in Simulation July 22, 2011 C. Tennant.
‘S2E’ Study of Linac for TESLA XFEL P. Emma SLAC  Tracking  Comparison to LCLS  Re-optimization  Tolerances  Jitter  CSR Effects.
Detector / Interaction Region Integration Vasiliy Morozov, Charles Hyde, Pawel Nadel-Turonski Joint CASA/Accelerator and Nuclear Physics MEIC/ELIC Meeting.
Beam Optics of the TTF2 Nina Golubeva DESY. Beam optics from the BC2 up to the undulators General introduction to linear optics: – constraints for different.
300keV emittances February 1, Scan _1835 FC0=1.13E-04 [A] Collimator=7.50E-06 [A] DF=1% Peak current = 100 [μA] RF = [dB] Power = 30.
实验十四 紫外线灭菌  一、实验背景及目的:  灭菌是一种杀灭微生物的措施。紫外线灭菌 是物理灭菌因素之一。  1. 了解紫外线灭菌的原理;  2. 学习、掌握紫外线灭菌的方法。 版权所有 未经作者同意 请勿使用.
親愛的吉姆舅舅: 今天吃完晚餐後,奶奶說,在家 裡情況變好以前,您要我搬到城裡跟 您住。奶奶有沒有跟您說,爸爸已經 好久沒有工作,也好久沒有人請媽媽 做衣服了? 我們聽完都哭了,連爸爸也哭了, 但是媽媽說了一個故事讓我們又笑了。 她說:您們小的時候,她曾經被您追 得爬到樹上去,真的嗎? 雖然我個子小,但是我很強壯,
The reading is 7.38 mm. The reading is 7.72 mm.
CLIC Frequency Multiplication System aka Combiner Rings Piotr Skowronski Caterina Biscari Javier Barranco 21 Oct IWLC 2010.
Preservation of Magnetized Beam Quality in a Non-Isochronous Bend
SABER Longitudinal Tracking Studies P. Emma, K. Bane Mar. 1, 2006
10 mm is the same as... 1 cm. 20 mm is the same as... 2 cm.
Some Aspects on Compton Scheme Positron Source Study Wanming Liu ANL Tsunehiko OMORI KEK.
输尿管软镜钬激光碎石术的体会 南华大学附属第二医院泌尿外科三区 钱 坤. 背 景  输尿管软镜作为一种新碎石手段,目前在部分医 院应用。其安全性、有效性得到一致的认可。  但是存在一些问题需要探讨:  手术适应症、禁忌症  影响碎石成功率的因素  手术并发症的防治.
Electron Cooling Simulation For JLEIC
fundamental equations of LHC performance
Time-Reversed Particle Simulations In GPT (or “There And Back Again”)
Large Booster and Collider Ring

General Particle Tracer (GPT) Simplified Simulations: Counter-wound Solenoids A. Hofler July 12, /14/2017.
BC2 Commissioning Parameters
Progress activities in short bunch compressors
ERL working modes Georg Hoffstaetter, Professor Cornell University / CLASSE / SRF group & ERL effort High Current mode High Coherence mode High Buch charge.
LCLS Commissioning Parameters
CEPC Injector Damping Ring
RM 2 7 +RM 2 4 RM 7 3 +RM 1 6 RM 5 2 +RM 2 4 RM 1 3 +RM5 2.
CEPC parameter optimization and lattice design
CNGS Proton beam line: news since NBI2002 OUTLINE 1. Overview
IMPACT Simulation of the Montague Resonance at PS
مديريت موثر جلسات Running a Meeting that Works
Metric Unit Conversion: Lengths
ERL EIC Workshop | Jefferson Laboratory | November 2, 2018
CMS vacuum chamber. Geometry for wakefield calculations
Experiments on CSR Effects at CTF II
Linac/BC1 Commissioning P
LCLS Tracking Studies CSR micro-bunching in compressors
Modified Beam Parameter Range
LCLS FEL Parameters Heinz-Dieter Nuhn, SLAC / SSRL April 23, 2002
CEPC Injector Linac beam dynamics
LCLS Commissioning Parameters
Low Energy Electron-Ion Collision
E.Bulyak, P.Gladkikh, M.Kuriki, T.Omori, L.Rinolfi,
Electron Optics & Bunch Compression
New VUV-FEL Simulation results
MEIC Electron Cooling: Do we have a Baseline Design and What is it?
Update on ERL Cooler Design Studies
Feasibility of Recuperation of Magnets in Decommissioned Storage Rings
Main Design Parameters RHIC Magnets for MEIC Ion Collider Ring
Fanglei Lin, Yuhong Zhang JLEIC R&D Meeting, March 10, 2016
Electron Cooling Work Plan for New Strong Cooling Baseline
Possible CCR Arc designs
MEIC Alternative Design Part V
Possibility of MEIC Arc Cell Using PEP-II Dipole
Simon Jolly UKNFIC Meeting 25th April 2008
HE-JLEIC: Do We Have a Baseline?
MEIC Alternative Design Part III
He Zhang, David Douglas, Yuhong Zhang MEIC R&D Meeting, 09/04/2014
MEIC beam path change with e-ring bypass lines
Presentation transcript:

Parametric Study of CSR in the MEIC CCR January 30, 2012

Parameters p = 54 MeV/c ex=y = 3 mm-mrad ez = (33.3, 66.6, 99.9) ps × 5.4 keV Qbunch = (0.5, 1.0, 1.5, 2.0) nC Run 50,000 particles in elegant Turn CSR on in dipoles (no csrdrift) Track for 10 turns

2.0 nC Track bunches with sz=(1.0, 2.0, 3.0) cm for 10 turns at 2.0 nC

1.5 nC Track bunches with sz=(1.0, 2.0, 3.0) cm for 10 turns at 1.5 nC

1.0 nC Track bunches with sz=(1.0, 2.0, 3.0) cm for 10 turns at 1.0 nC

0.5 nC Track bunches with sz=(1.0, 2.0, 3.0) cm for 10 turns at 0.5 nC

100 Turns 0.5 nC with 3 cm long bunch (rms) tracked for 100 turns with CSR sDE/E = 5.4 keV sDE/E = 49.8 keV

Increase Dipole Bend Radii Track for 1 turn (2.0 nC, 1 cm) sDE/E = 6.7 keV nominal sDE/E = 20.5 keV larger bend radii

1-d model