Collider Rings and IR Design for MEIC

Size: px
Start display at page:

Download "Collider Rings and IR Design for MEIC"

Transcription

1 Collider Rings and IR Design for MEIC Alex Bogacz for MEIC Collaboration Center for Advanced Studies of Accelerators EIC Collaboration Meeting The Catholic University of America Washington, DC, July 29-31, 21

2 Figure-8 Collider Rings x [cm] Figure-8 Collider Ring - Footprint z [cm] total ring circumference ~1 m 6 deg. crossing Collider Ring size is a compromise between synchrotron radiation and space charge 3-11 GeV electrons 2-6 GeV ions (with 6 Tesla dipoles) 1 GeV ions (with 8 Tesla dipoles)

3 Collider Rings with Relaxed IR Optics Larger Figure-8 Rings (~1 m circumference) 6 Tesla bends for ions at 6 GeV Additional straights to accommodate spin rotators and RF Horizontal IR crossing, dispersion free straights Relaxed IR Design: Chromaticity Compensating Optics max m Uncompensated dispersion in the straights Anti-symmetric dispersion pattern across the IR Dedicated Symmetric Inserts around the IR x y 1cm 2cm Electron Collider Ring based on emittance preserving Optics

4 PHASE_X&Y Ion Ring - 9 FODO Cell E = 6 GeV phase adv/cell: Df x,y = Q_X Q_Y Arc dipoles: $Lb=3 cm $B=58.2 kgauss $ang=5 deg. $rho = 34.4 meter Arc quadrupoles $Lq=65 cm $G= 1.5 kg/cm 9 offers intrinsic cell-to-cell cancellation of beta chromaticity off momentum beta wave propagates with twice the betatron frequency (18 after two cells - cancellation)

5 2 2 Quarter Arc Achromat 12 deg. Arc B/2 B/2 B/2 B/ dis. sup. cells 1 FODO cells 2 dis. sup. cells 28 3 meter dipoles

6 2 2 Ion Ring - Arc Optics 24 deg. Arc 26 quarter Arc 12 meter Straight 2 meter quarter Arc 12 meter

7 PHASE_X&Y Electron Ring FODO Cell E = 11 GeV phase adv/cell: Df x,y = Q_X Q_Y Arc dipoles: $Lb=11 cm $B=12.5 kgauss $ang=2.14 deg. $rho = 29.4 meter Arc quadrupoles $Lq=4 cm $G= 9 kg/cm 135 FODO offers emittance preserving optics H minimum Synchrotron radiation power per meter less than 2 kw/m

8 15.15 Quarter Arc Achromat 12 deg. Arc 12 2 dis. sup. cells 26 FODO cells 2 dis. sup. cells 2B/3 B/3 2B/3 B/ meter dipoles

9 15.15 Electron Ring - Arc Optics 24 deg. Arc 26 quarter Arc 12 meter Straight 2 meter quarter Arc 12 meter

10 Flexible Momentum Compaction Cell E = 11 GeV 135 FODO Theoretical Emittance Minimum FMC Cell H minimum e x e x 2

11 EM Calorimeter HTCC RICH EM Calorimeter Hadron Calorimeter Muon Detector Detector and IR layout low-q 2 electron detection dipole large aperture electron quads central detector with endcaps small angle hadron detection dipole ion quads ultra forward hadron detection dipole small diameter electron quads ~5 mrad crossing Solenoid yoke + Muon Detector Solenoid yoke + Hadronic Calorimeter RICH Tracking 5 m solenoid Pawel Nadel-Turonski

12 8 5 IR Optics (electrons) () 2 ff m IR f 2 1 f f x y 1cm 2cm max g FF f Natural Chromaticity: x = -47 y = FF doublets l = 3.5m

13 Size_X[cm] Size_Y[cm] IR Optics (electrons at 5 GeV) e e x N y N m m x y 1cm 2cm e g () N 19 Ax_bet Ay_bet Ax_disp Ay_disp 19 Q4 Q3 Q2 Q1 Q1 G[kG/cm] = -2.8 Q2 G[kG/cm] = 3.1 Q3 G[kG/cm] = -2. Q4 G[kG/cm] = x 31-6 y m m

14 Synchrotron Radiation Background x W 5 mm P + 4.6x mm 5 mrad Photons incident on various surfaces from the last 4 quads FF1 24 FF2 3 mm e Rate per bunch incident on the surface > 1 kev Beam current = 2.32 A 2.9x1 1 particles/bunch Rate per bunch incident on the detector beam pipe assuming 1% reflection coefficient and solid angle acceptance of 4.4 % M. Sullivan July 2, 21 F$JLAB_E_3_5M_1A Michael Sullivan, SLAC

15 3 5 IR Optics (ions) () 2 ff m IR f 2 1 f f x y 1cm 2cm max g FF f Natural Chromaticity: x = -88 y = FF triplet : Q3 Q2 Q1 l = 7m

16 Size_X[cm] Size_Y[cm] IR Optics (ions) at 6 GeV e e x N y N m m x y 1cm 2cm e g () N 5 Ax_bet Ay_bet Ax_disp Ay_disp 5 FF triplet : Q3 Q2 Q1 Q1 G[kG/cm] = -9.7 Q2 G[kG/cm] = 6.9 Q3 G[kG/cm] = x 31-6 y m m

17 IR Chromaticity Compensation ions Df x 2 Df y Arc end Df x p Df x,y p Df x,y p Chromaticity Compensation with four families of sextupoles

18 Chromaticity Compensation electrons Df x 2 Df y Df x,y p Df x,y p Df x p Chromaticity Compensation with four families of sextupoles

19 31 32 Collider Ring Tune Diagram Working point above half integer a la KEKB: Q x =36.56 Q y =

20 Tune Chromaticity Correction Large momentum acceptance and dynamic aperture Dp p -3 Hisham Sayed, Old Dominion Univ.

21 Arc - Spin Rotator - IR electrons Arc 8 m drift space for low Q 2 tagging IR Chromaticity Compensation Block Spin Rotator

22 Electron and Ion IRs - Overlay ions electrons Chromaticity Compensation Block electrons Spin rotator

23 Summary Complete design of Figure-8 Collider Rings (~ 1 m circumference) Emittance preserving Arcs based on 135 FODO lattice (11 GeV electrons) Periodic dispersion Arcs based on 9 FODO lattice (6 GeV ions) Relaxed IR Design: max m xy, 1 / 2cm Chromatic compensation with sextupoles IR chromaticity Dispersive Straights - disp. leakage from the Arcs (by design) Anti-symmetric dispersion pattern across the IR Dedicated Optics Symmetric inserts Beta Chromaticity compensation (immediate vicinity of the ) Dp Large Momentum Acceptance open, DA tracking p -3

LHeC Recirculator with Energy Recovery Beam Optics Choices

LHeC Recirculator with Energy Recovery Beam Optics Choices LHeC Recirculator with Energy Recovery Beam Optics Choices Alex Bogacz in collaboration with Frank Zimmermann and Daniel Schulte Alex Bogacz 1 Alex Bogacz 2 Alex Bogacz 3 Alex Bogacz 4 Alex Bogacz 5 Alex

More information

Muon RLA Design Status and Simulations

Muon RLA Design Status and Simulations Muon RLA Design Status and Simulations Muons Inc., Vasiliy Morozov, Yves Roblin Jefferson Lab NuFact'11, Univ. of Geneva, Aug. 1-6, 211 1 Linac and RLAs IDS 244 MeV.9 GeV RLA with 2-pass Arcs 192 m 79

More information

TeV Scale Muon RLA Complex Large Emittance MC Scenario

TeV Scale Muon RLA Complex Large Emittance MC Scenario TeV Scale Muon RLA Complex Large Emittance MC Scenario Alex Bogacz and Kevin Beard Muon Collider Design Workshop, BNL, December 1-3, 29 Outline Large Emittance MC Neuffer s Collider Acceleration Scheme

More information

EIC at JLab - design considerations and detector overview

EIC at JLab - design considerations and detector overview EIC at JLab - design considerations and detector overview Pawel Nadel-Turonski Jefferson Lab, Newport News, VA EIC Exclusive Workshop,, Rutgers Outline 1. Introduction 2. Exclusive kinematics and Detector

More information

Full-Acceptance Detector Integration at MEIC

Full-Acceptance Detector Integration at MEIC Full-Acceptance Detector Integration at MEIC Vasiliy Morozov for MEIC Study Group Electron Ion Collider Users Meeting, Stony Brook University June 27, 2014 Lattice design of geometrically-matched collider

More information

Preliminary Detector Design for the EIC at JLab

Preliminary Detector Design for the EIC at JLab Preliminary Detector Design for the EIC at JLab Pawel Nadel-Turonski Jefferson Lab, Newport News, VA, Outline 1. Introduction 2. Interaction Region 3. Detector Requirements and Challenges 4. Brief Overview

More information

Lattice Design and Performance for PEP-X Light Source

Lattice Design and Performance for PEP-X Light Source Lattice Design and Performance for PEP-X Light Source Yuri Nosochkov SLAC National Accelerator Laboratory With contributions by M-H. Wang, Y. Cai, X. Huang, K. Bane 48th ICFA Advanced Beam Dynamics Workshop

More information

{ } Double Bend Achromat Arc Optics for 12 GeV CEBAF. Alex Bogacz. Abstract. 1. Dispersion s Emittance H. H γ JLAB-TN

{ } Double Bend Achromat Arc Optics for 12 GeV CEBAF. Alex Bogacz. Abstract. 1. Dispersion s Emittance H. H γ JLAB-TN JLAB-TN-7-1 Double Bend Achromat Arc Optics for 12 GeV CEBAF Abstract Alex Bogacz Alternative beam optics is proposed for the higher arcs to limit emittance dilution due to quantum excitations. The new

More information

Compressor Ring. Contents Where do we go? Beam physics limitations Possible Compressor ring choices Conclusions. Valeri Lebedev.

Compressor Ring. Contents Where do we go? Beam physics limitations Possible Compressor ring choices Conclusions. Valeri Lebedev. Compressor Ring Valeri Lebedev Fermilab Contents Where do we go? Beam physics limitations Possible Compressor ring choices Conclusions Muon Collider Workshop Newport News, VA Dec. 8-1, 8 Where do we go?

More information

ILC Damping Ring Alternative Lattice Design **

ILC Damping Ring Alternative Lattice Design ** ILC Damping Ring Alternative Lattice Design ** Yi-Peng Sun *,1,2, Jie Gao 1, Zhi-Yu Guo 2 1 Institute of High Energy Physics, CAS, Beijing 2 Key Laboratory of Heavy Ion Physics, Peking University, Beijing

More information

Synchrotron Based Proton Drivers

Synchrotron Based Proton Drivers Synchrotron Based Pron Drivers Weiren Chou Fermi National Accelerar Laborary P.O. Box 500, Batavia, IL 60510, USA Abstract. Pron drivers are pron sources that produce intense short pron bunches. They have

More information

Practical Lattice Design

Practical Lattice Design Practical Lattice Design Dario Pellegrini (CERN) dario.pellegrini@cern.ch USPAS January, 15-19, 2018 1/17 D. Pellegrini - Practical Lattice Design Lecture 5. Low Beta Insertions 2/17 D. Pellegrini - Practical

More information

Beam Optics design for CEPC collider ring

Beam Optics design for CEPC collider ring Beam Optics design for CEPC collider ring, Yuan Zhang, Yuanyuan Wei, Sha Bai, Dou Wang, Huiping Geng, Chenghui Yu, Jie Gao IHEP, Beijing 1st workshop on applications of high energy Circular Electron-Positron

More information

Beam Dynamics. D. Brandt, CERN. CAS Bruges June 2009 Beam Dynamics D. Brandt 1

Beam Dynamics. D. Brandt, CERN. CAS Bruges June 2009 Beam Dynamics D. Brandt 1 Beam Dynamics D. Brandt, CERN D. Brandt 1 Some generalities D. Brandt 2 Units: the electronvolt (ev) The electronvolt (ev)) is the energy gained by an electron travelling, in vacuum, between two points

More information

NEXT GENERATION B-FACTORIES

NEXT GENERATION B-FACTORIES NEXT GENERATION B-FACTORIES M. Masuzawa, KEK, Tsukuba, Japan Abstract The KEKB and PEP-II B factories have achieved world record luminosities while doubling or tripling their original design luminosities.

More information

ILC Damping Ring Alternative Lattice Design (Modified FODO)

ILC Damping Ring Alternative Lattice Design (Modified FODO) ILC Damping Ring Alternative Lattice Design (Modified FODO) Yi-Peng Sun 1,2, Jie Gao 1, Zhi-Yu Guo 2 Wei-Shi Wan 3 1 Institute of High Energy Physics, CAS, China 2 State Key Laboratory of Nuclear Physics

More information

Choosing the Baseline Lattice for the Engineering Design Phase

Choosing the Baseline Lattice for the Engineering Design Phase Third ILC Damping Rings R&D Mini-Workshop KEK, Tsukuba, Japan 18-20 December 2007 Choosing the Baseline Lattice for the Engineering Design Phase Andy Wolski University of Liverpool and the Cockcroft Institute

More information

Accelerator Physics Final Exam pts.

Accelerator Physics Final Exam pts. Accelerator Physics Final Exam - 170 pts. S. M. Lund and Y. Hao Graders: C. Richard and C. Y. Wong June 14, 2018 Problem 1 P052 Emittance Evolution 40 pts. a) 5 pts: Consider a coasting beam composed of

More information

Pretzel scheme of CEPC

Pretzel scheme of CEPC Pretzel scheme of CEPC H. Geng, G. Xu, Y. Zhang, Q. Qin, J. Gao, W. Chou, Y. Guo, N. Wang, Y. Peng, X. Cui, T. Yue, Z. Duan, Y. Wang, D. Wang, S. Bai, F. Su HKUST, Hong Kong IAS program on High Energy

More information

Operational Experience with HERA

Operational Experience with HERA PAC 07, Albuquerque, NM, June 27, 2007 Operational Experience with HERA Joachim Keil / DESY On behalf of the HERA team Contents Introduction HERA II Luminosity Production Experiences with HERA Persistent

More information

Lattice design and dynamic aperture optimization for CEPC main ring

Lattice design and dynamic aperture optimization for CEPC main ring Lattice design and dynamic aperture optimization for CEPC main ring Yiwei Wang, Feng Su, Sha Bai, Yuan Zhang, Dou Wang, Huiping Geng, Chenghui Yu, Jie Gao HKUST IAS conference, 23-26 Jan 2017 Outline Fully

More information

6 Bunch Compressor and Transfer to Main Linac

6 Bunch Compressor and Transfer to Main Linac II-159 6 Bunch Compressor and Transfer to Main Linac 6.1 Introduction The equilibrium bunch length in the damping ring (DR) is 6 mm, too long by an order of magnitude for optimum collider performance (σ

More information

Transverse dynamics Selected topics. Erik Adli, University of Oslo, August 2016, v2.21

Transverse dynamics Selected topics. Erik Adli, University of Oslo, August 2016, v2.21 Transverse dynamics Selected topics Erik Adli, University of Oslo, August 2016, Erik.Adli@fys.uio.no, v2.21 Dispersion So far, we have studied particles with reference momentum p = p 0. A dipole field

More information

COMBINER RING LATTICE

COMBINER RING LATTICE CTFF3 TECHNICAL NOTE INFN - LNF, Accelerator Division Frascati, April 4, 21 Note: CTFF3-2 COMBINER RING LATTICE C. Biscari 1. Introduction The 3 rd CLIC test facility, CTF3, is foreseen to check the feasibility

More information

The TESLA Dogbone Damping Ring

The TESLA Dogbone Damping Ring The TESLA Dogbone Damping Ring Winfried Decking for the TESLA Collaboration April 6 th 2004 Outline The Dogbone Issues: Kicker Design Dynamic Aperture Emittance Dilution due to Stray-Fields Collective

More information

HE-LHC Optics Development

HE-LHC Optics Development SLAC-PUB-17224 February 2018 HE-LHC Optics Development Yunhai Cai and Yuri Nosochkov* SLAC National Accelerator Laboratory, Menlo Park, CA, USA Mail to: yuri@slac.stanford.edu Massimo Giovannozzi, Thys

More information

SLS at the Paul Scherrer Institute (PSI), Villigen, Switzerland

SLS at the Paul Scherrer Institute (PSI), Villigen, Switzerland SLS at the Paul Scherrer Institute (PSI), Villigen, Switzerland Michael Böge 1 SLS Team at PSI Michael Böge 2 Layout of the SLS Linac, Transferlines Booster Storage Ring (SR) Beamlines and Insertion Devices

More information

First propositions of a lattice for the future upgrade of SOLEIL. A. Nadji On behalf of the Accelerators and Engineering Division

First propositions of a lattice for the future upgrade of SOLEIL. A. Nadji On behalf of the Accelerators and Engineering Division First propositions of a lattice for the future upgrade of SOLEIL A. Nadji On behalf of the Accelerators and Engineering Division 1 SOLEIL : A 3 rd generation synchrotron light source 29 beamlines operational

More information

Modeling CESR-c. D. Rubin. July 22, 2005 Modeling 1

Modeling CESR-c. D. Rubin. July 22, 2005 Modeling 1 Modeling CESR-c D. Rubin July 22, 2005 Modeling 1 Weak strong beambeam simulation Motivation Identify component or effect that is degrading beambeam tuneshift Establish dependencies on details of lattice

More information

Superconducting Magnets for Future Electron-Ion Collider. Yuhong Zhang Thomas Jefferson National Accelerator Facility, USA

Superconducting Magnets for Future Electron-Ion Collider. Yuhong Zhang Thomas Jefferson National Accelerator Facility, USA Superconducting Magnets for Future Electron-Ion Collider Yuhong Zhang Thomas Jefferson National Accelerator Facility, USA Mini-workshop on Accelerator, IAS, HKUST, Hong Kong, January 18-19, 2018 1 Outline

More information

Linear Collider Collaboration Tech Notes

Linear Collider Collaboration Tech Notes LCC 0035 07/01/00 Linear Collider Collaboration Tech Notes More Options for the NLC Bunch Compressors January 7, 2000 Paul Emma Stanford Linear Accelerator Center Stanford, CA Abstract: The present bunch

More information

Introduction to EIC/detector concept

Introduction to EIC/detector concept Introduction to EIC/detector concept Tanja Horn 4 th Workshop on Exclusive Reactions at High Momentum Transfer Tanja Horn, CUA Colloquium Newport News, VA 19 May 2010 1 Why an electron-ion Collider? Easier

More information

ILC Spin Rotator. Super B Workshop III. Presenter: Jeffrey Smith, Cornell University. with

ILC Spin Rotator. Super B Workshop III. Presenter: Jeffrey Smith, Cornell University. with ILC Spin Rotator Super B Workshop III Presenter: Jeffrey Smith, Cornell University with Peter Schmid, DESY Peter Tenenbaum and Mark Woodley, SLAC Georg Hoffstaetter and David Sagan, Cornell Based on NLC

More information

Lattice Design for the Taiwan Photon Source (TPS) at NSRRC

Lattice Design for the Taiwan Photon Source (TPS) at NSRRC Lattice Design for the Taiwan Photon Source (TPS) at NSRRC Chin-Cheng Kuo On behalf of the TPS Lattice Design Team Ambient Ground Motion and Civil Engineering for Low Emittance Electron Storage Ring Workshop

More information

Compressor Lattice Design for SPL Beam

Compressor Lattice Design for SPL Beam EUROPEAN ORGANIZATION FOR NUCLEAR RESEARCH CERN A&B DIVISION AB-Note-27-34 BI CERN-NUFACT-Note-153 Compressor Lattice Design for SPL Beam M. Aiba Abstract A compressor ring providing very short proton

More information

S1: Particle Equations of Motion S1A: Introduction: The Lorentz Force Equation

S1: Particle Equations of Motion S1A: Introduction: The Lorentz Force Equation S1: Particle Equations of Motion S1A: Introduction: The Lorentz Force Equation The Lorentz force equation of a charged particle is given by (MKS Units):... particle mass, charge... particle coordinate...

More information

III. CesrTA Configuration and Optics for Ultra-Low Emittance David Rice Cornell Laboratory for Accelerator-Based Sciences and Education

III. CesrTA Configuration and Optics for Ultra-Low Emittance David Rice Cornell Laboratory for Accelerator-Based Sciences and Education III. CesrTA Configuration and Optics for Ultra-Low Emittance David Rice Cornell Laboratory for Accelerator-Based Sciences and Education Introduction Outline CESR Overview CESR Layout Injector Wigglers

More information

Status of Optics Design

Status of Optics Design 17th B2GM, February 5, 2014 Status of Optics Design Y. Ohnishi /KEK 17th B2GM KEK, February 5, 2014 Contents! Lattice parameters! Dynamic aperture under influence of beam-beam effect! Lattice preparation

More information

Bernhard Holzer, CERN-LHC

Bernhard Holzer, CERN-LHC Bernhard Holzer, CERN-LHC * Bernhard Holzer, CERN CAS Prague 2014 Lattice Design... in 10 seconds... the Matrices Transformation of the coordinate vector (x,x ) in a lattice x(s) x = M 0 x'(s) 1 2 x' 0

More information

New LSS optics for the LHC (status)

New LSS optics for the LHC (status) New LSS optics for the LHC (status) 23-03-2012 R.B. Appleby The University of Manchester/Cockcroft Institute, UK Many thanks to Riccardo, Bernhard, Stephane Motivation The optics limitations of the nominal

More information

S. Guiducci. Table 1 PADME beam from Linac. Energy (MeV) 550. Number of positrons per pulse Pulse length (ns)

S. Guiducci. Table 1 PADME beam from Linac. Energy (MeV) 550. Number of positrons per pulse Pulse length (ns) K K DA ΦNE TECHNICAL NOTE INFN - LNF, Accelerator Division Frascati, 11/01/2017 Note: G-73 PRELIMINARY CONSIDERATIONS ON THE USE OF DAΦNE POSITRON RING AS A PULSE STRETCHER FOR THE DAΦNE LINAC S. Guiducci

More information

MEIC Status. Andrew Hutton For the MEIC Collaboration

MEIC Status. Andrew Hutton For the MEIC Collaboration MEIC Status Andrew Hutton For the MEIC Collaboration MEIC Collaborators I am presenting the work of a large group of passionate scientists and engineers who have been working together for several years

More information

FODO Cell Introduction to OptiM

FODO Cell Introduction to OptiM FODO Cell Introduction to OptiM S. Alex Bogacz Jefferson Lab 1 FODO Optics cell Most accelerator lattices are designed in modular ways Design and operational clarity, separation of functions One of the

More information

MEIC Electron-Ion Collider - Space-Charge Issues

MEIC Electron-Ion Collider - Space-Charge Issues MEIC Electron-Ion Collider - Space-Charge Issues on behalf of MEIC Collaboration 1 MEIC (Medium-energy Electron Ion Collider) Collaboration A. Bogacz, P. Brindza, A. Camsonne, E. Daly, Y. Derbenev, D.

More information

SABER Optics. Y. Nosochkov, K. Bane, P. Emma, R. Erickson. SABER Workshop, SLAC, March 15-16, /25

SABER Optics. Y. Nosochkov, K. Bane, P. Emma, R. Erickson. SABER Workshop, SLAC, March 15-16, /25 SABER Optics Y. Nosochkov, K. Bane, P. Emma, R. Erickson SABER Workshop, SLAC, March 15-16, 2006 1/25 Outline White paper optics design Beam tracking for SABER and for the old South Arc Magnet overlap

More information

Longitudinal Top-up Injection for Small Aperture Storage Rings

Longitudinal Top-up Injection for Small Aperture Storage Rings Longitudinal Top-up Injection for Small Aperture Storage Rings M. Aiba, M. Böge, Á. Saá Hernández, F. Marcellini and A. Streun Paul Scherrer Institut Introduction Lower and lower horizontal emittances

More information

JLEIC forward detector design and performance

JLEIC forward detector design and performance Jefferson Lab E-mail: ryoshida@jlab.org A major part of the physics program at the Electron-Ion Collider being planned in the US is the exploration of nucleon and nuclear structure. This program means

More information

Overview of Acceleration

Overview of Acceleration Overview of Acceleration R B Palmer, Scott Berg, Steve Kahn (presented by Steve Kahn) Nufact-04 RF Frequency Acc types and System Studies Linacs RLA s FFAG s Injection/Extraction US Study 2a acceleration

More information

Luminosity Considerations for erhic

Luminosity Considerations for erhic Luminosity Considerations for erhic Fuhua Wang MIT-Bates Linear Accelerator Center Second Electron-Ion Collider Workshop Jefferson Lab March 15-17, 2004 1 Thanks BNL: V.Ptitsyn, C.Montag, S. Peggs, T.Roser

More information

Conceptual design of an accumulator ring for the Diamond II upgrade

Conceptual design of an accumulator ring for the Diamond II upgrade Journal of Physics: Conference Series PAPER OPEN ACCESS Conceptual design of an accumulator ring for the Diamond II upgrade To cite this article: I P S Martin and R Bartolini 218 J. Phys.: Conf. Ser. 167

More information

Status of SuperKEKB Design: Lattice and IR

Status of SuperKEKB Design: Lattice and IR Status of SuperKEKB Design: Lattice and IR Y. Ohnishi July 7, 2009 3rd Open Mee8ng of the Belle II collabora8on Tanabata : Festival of the Weaver? KEK Contents Nano-beam scheme: Design concept Machine

More information

LOW EMITTANCE MODEL FOR THE ANKA SYNCHROTRON RADIATION SOURCE

LOW EMITTANCE MODEL FOR THE ANKA SYNCHROTRON RADIATION SOURCE Karlsruhe Institute of Technology (KIT, Karlsruhe, Germany) Budker Institute of Nuclear Physics (BINP, Novosibirsk, Russia) LOW EMITTANCE MODEL FOR THE ANKA SYNCHROTRON RADIATION SOURCE (A.Papash - on

More information

Presented at the 5th International Linear Collider Workshop (LCWS 2000), Oct 24-28, 2000, Batavia, IL

Presented at the 5th International Linear Collider Workshop (LCWS 2000), Oct 24-28, 2000, Batavia, IL SLAC-PUB-10800 New NLC Final Focus Pantaleo Raimondi and Andrei Seryi Stanford Linear Accelerator Center, Stanford University, Stanford, California 94309 USA Abstract. A novel design of the Final Focus

More information

Abstract. 1. Introduction

Abstract. 1. Introduction The New Upgrade of SESAME D.Einfeld1, R.H.Sarraf2, M.Attal3, H.Hashemi4, A.Elsisi5, A.Amro6, H.Hassanzadegan4, K.Tavakoli3, B.Kalantari7, S. Varnasery8, E. Al-Dmour8, D. Foudeh6, H.Tarawneh9, A.Aladwan7

More information

Accelerator Physics Issues of ERL Prototype

Accelerator Physics Issues of ERL Prototype Accelerator Physics Issues of ERL Prototype Ivan Bazarov, Geoffrey Krafft Cornell University TJNAF ERL site visit (Mar 7-8, ) Part I (Bazarov). Optics. Space Charge Emittance Compensation in the Injector

More information

arxiv: v1 [physics.acc-ph] 21 Oct 2014

arxiv: v1 [physics.acc-ph] 21 Oct 2014 SIX-DIMENSIONAL WEAK STRONG SIMULATIONS OF HEAD-ON BEAM BEAM COMPENSATION IN RHIC arxiv:.8v [physics.acc-ph] Oct Abstract Y. Luo, W. Fischer, N.P. Abreu, X. Gu, A. Pikin, G. Robert-Demolaize BNL, Upton,

More information

e + e Factories M. Sullivan Presented at the Particle Accelerator Conference June 25-29, 2007 in Albuquerque, New Mexico e+e- Factories

e + e Factories M. Sullivan Presented at the Particle Accelerator Conference June 25-29, 2007 in Albuquerque, New Mexico e+e- Factories e + e Factories M. Sullivan Presented at the Particle Accelerator Conference June 25-29, 2007 in Albuquerque, New Mexico 1 Outline Factory Running KEKB PEP-II DAFNE CESR-c BEPCII 2 Summary Factory Running

More information

Emittance preserving staging optics for PWFA and LWFA

Emittance preserving staging optics for PWFA and LWFA Emittance preserving staging optics for PWFA and LWFA Physics and Applications of High Brightness Beams Havana, Cuba Carl Lindstrøm March 29, 2016 PhD Student University of Oslo / SLAC (FACET) Supervisor:

More information

Study of Alternative Optics for the NLC Prelinac Collimation section

Study of Alternative Optics for the NLC Prelinac Collimation section LCC 0057 03/01 Linear Collider Collaboration Tech Notes Study of Alternative Optics for the NLC Prelinac Collimation section March 2001 Yuri Nosochkov, Pantaleo Raimondi, Tor Raubenheimer Stanford Linear

More information

The Electron-Ion Collider

The Electron-Ion Collider The Electron-Ion Collider C. Tschalaer 1. Introduction In the past year, the idea of a polarized electron-proton (e-p) or electron-ion (e-a) collider of high luminosity (10 33 cm -2 s -1 or more) and c.m.

More information

Lattice Design of 2-loop Compact ERL. High Energy Accelerator Research Organization, KEK Miho Shimada and Yukinori Kobayashi

Lattice Design of 2-loop Compact ERL. High Energy Accelerator Research Organization, KEK Miho Shimada and Yukinori Kobayashi Lattice Design of 2-loop Compact ERL High Energy Accelerator Research Organization, KEK Miho Shimada and Yukinori Kobayashi Introduction Wepromote the construction of the compact Energy Recovery Linac(cERL)

More information

Introduction to particle accelerators

Introduction to particle accelerators Introduction to particle accelerators Walter Scandale CERN - AT department Lecce, 17 June 2006 Introductory remarks Particle accelerators are black boxes producing either flux of particles impinging on

More information

Introduction to Accelerator Physics 2011 Mexican Particle Accelerator School

Introduction to Accelerator Physics 2011 Mexican Particle Accelerator School Introduction to Accelerator Physics 2011 Mexican Particle Accelerator School Lecture 5/7: Dispersion (including FODO), Dispersion Suppressor, Light Source Lattices (DBA, TBA, TME) Todd Satogata (Jefferson

More information

E. Gianfelice-Wendt, for the Luminosity Upgrade Group, DESY, Hamburg, Germany

E. Gianfelice-Wendt, for the Luminosity Upgrade Group, DESY, Hamburg, Germany HERA UPGRADE PLANS E. Gianfelice-Wendt, for the Luminosity Upgrade Group, DESY, Hamburg, Germany Abstract HERA is a 6.3 km long p=e +=, double ring collider located at DESY (Hamburg). The proton and the

More information

D. Brandt, CERN. CAS Frascati 2008 Accelerators for Newcomers D. Brandt 1

D. Brandt, CERN. CAS Frascati 2008 Accelerators for Newcomers D. Brandt 1 Accelerators for Newcomers D. Brandt, CERN D. Brandt 1 Why this Introduction? During this school, you will learn about beam dynamics in a rigorous way but some of you are completely new to the field of

More information

FCC-ee Machine Layout and Beam Optics + Matching with synchrotron motion

FCC-ee Machine Layout and Beam Optics + Matching with synchrotron motion FCC-ee Machine Layout and Beam Optics + Matching with synchrotron motion KEK Accelerator Seminar 27 Apr. 2016 KEK, Tsukuba K. Oide Contributed by M. Aiba, S. Aumon, M. Benedikt, A. Blondel, A. Bogomyagkov,

More information

LIS section meeting. PS2 design status. Y. Papaphilippou. April 30 th, 2007

LIS section meeting. PS2 design status. Y. Papaphilippou. April 30 th, 2007 LIS section meeting PS2 design status Y. Papaphilippou April 30 th, 2007 Upgrade of the injector chain (R. Garoby, PAF) Proton flux / Beam power 50 MeV 160 MeV Linac2 Linac4 1.4 GeV ~ 5 GeV PSB SPL RCPSB

More information

Polarization Preservation and Control in a Figure-8 Ring

Polarization Preservation and Control in a Figure-8 Ring Spin Physics (SPIN2014) International Journal of Modern Physics: Conference Series Vol. 40 (2016) 1660090 (7 pages) c The Author(s) DOI: 10.1142/S2010194516600909 Polarization Preservation and Control

More information

ELIC: A High Luminosity And Efficient Spin Manipulation Electron-Light Ion Collider Based At CEBAF

ELIC: A High Luminosity And Efficient Spin Manipulation Electron-Light Ion Collider Based At CEBAF ELIC: A High Luminosity And Efficient Spin Manipulation Electron-Light Ion Collider Based At CEBAF Lia Merminga and Yaroslav Derbenev Center for Advanced Studies of Accelerators, Jefferson Laboratory,

More information

Physics Opportunities at the MEIC at JLab

Physics Opportunities at the MEIC at JLab Physics Opportunities at the MEIC at JLab Pawel Nadel-Turonski Jefferson Lab QCD Evolution Workshop, JLab, May 16, 2012 1 The physics program of an EIC Map the spin and spatial structure of sea quarks

More information

Accelerator Physics. Tip World Scientific NEW JERSEY LONDON SINGAPORE BEIJING SHANGHAI HONG KONG TAIPEI BANGALORE. Second Edition. S. Y.

Accelerator Physics. Tip World Scientific NEW JERSEY LONDON SINGAPORE BEIJING SHANGHAI HONG KONG TAIPEI BANGALORE. Second Edition. S. Y. Accelerator Physics Second Edition S. Y. Lee Department of Physics, Indiana University Tip World Scientific NEW JERSEY LONDON SINGAPORE BEIJING SHANGHAI HONG KONG TAIPEI BANGALORE Contents Preface Preface

More information

ThomX Machine Advisory Committee. (LAL Orsay, March ) Ring Beam Dynamics

ThomX Machine Advisory Committee. (LAL Orsay, March ) Ring Beam Dynamics ThomX Machine Advisory Committee (LAL Orsay, March 20-21 2017) Ring Beam Dynamics A. Loulergue, M. Biagini, C. Bruni, I. Chaikovska I. Debrot, N. Delerue, A. Gamelin, H. Guler, J. Zang Programme Investissements

More information

HIRFL STATUS AND HIRFL-CSR PROJECT IN LANZHOU

HIRFL STATUS AND HIRFL-CSR PROJECT IN LANZHOU HIRFL STATUS AND HIRFL-CSR PROJECT IN LANZHOU J. W. Xia, Y. F. Wang, Y. N. Rao, Y. J. Yuan, M. T. Song, W. Z. Zhang, P. Yuan, W. Gu, X. T. Yang, X. D. Yang, S. L. Liu, H.W.Zhao, J.Y.Tang, W. L. Zhan, B.

More information

IP switch and big bend

IP switch and big bend 1 IP switch and big bend Contents 1.1 Introduction..................................................... 618 1.2 TheIPSwitch.................................................... 618 1.2.1 OpticsDesign...............................................

More information

The 2015 erhic Ring-Ring Design. Christoph Montag Collider-Accelerator Department Brookhaven National Laboratory

The 2015 erhic Ring-Ring Design. Christoph Montag Collider-Accelerator Department Brookhaven National Laboratory The 2015 erhic Ring-Ring Design Christoph Montag Collider-Accelerator Department Brookhaven National Laboratory The Relativistic Heavy Ion Collider RHIC Two superconducting storage rings 3833.845 m circumference

More information

Accelerator. Physics of PEP-I1. Lecture #7. March 13,1998. Dr. John Seeman

Accelerator. Physics of PEP-I1. Lecture #7. March 13,1998. Dr. John Seeman Accelerator Physics of PEP-1 Lecture #7 March 13,1998 Dr. John Seeman Accelerator Physics of PEPJ John Seeman March 13,1998 1) What is PEP-? Lecture 1 2) 3) Beam parameters for an luminosity of 3~1~~/cm~/sec

More information

Progress on the Large Hadron electron Collider. O. Brüning, E. Nissen, D. Pellegrini, D. Schulte, A. Valloni, F. Zimmermann 1

Progress on the Large Hadron electron Collider. O. Brüning, E. Nissen, D. Pellegrini, D. Schulte, A. Valloni, F. Zimmermann 1 O. Brüning, E. Nissen, D. Pellegrini, D. Schulte, A. Valloni, F. Zimmermann 1 CERN Meyrin, Switzerland E-mail: oliver.bruning@cern.ch, edward.nissen@cern.ch, dario.pellegrini@cern.ch, daniel.schulte@cern.ch,

More information

Accelerator Physics. Accelerator Development

Accelerator Physics. Accelerator Development Accelerator Physics The Taiwan Light Source (TLS) is the first large accelerator project in Taiwan. The goal was to build a high performance accelerator which provides a powerful and versatile light source

More information

A Very Large Lepton Collider in a VLHC tunnel

A Very Large Lepton Collider in a VLHC tunnel A Very Large Lepton Collider in a VLHC tunnel Tanaji Sen Fermilab, Batavia, IL Design strategy Intensity Limitations RF and Optics parameters: Arc, IR Lifetime Scaling the beam-beam parameter Luminosity,

More information

SuperB: Ring Issues. U. Wienands SLAC PEP-II. U. Wienands, SLAC-PEP-II SuperB Workshop Frascati, 16-Mar-06

SuperB: Ring Issues. U. Wienands SLAC PEP-II. U. Wienands, SLAC-PEP-II SuperB Workshop Frascati, 16-Mar-06 SuperB: Ring Issues U. Wienands SLAC PEP-II 1 Content Basic parameter estimate Examples of some lattices S.R. Handling Bunch length Collective effects incl beam lifetime Summary This presentation will

More information

PUBLICATION. Consolidated EIR design baseline: Milestone M3.6

PUBLICATION. Consolidated EIR design baseline: Milestone M3.6 CERN-ACC-2018-0039 Future Circular Collider PUBLICATION Consolidated EIR design baseline: Milestone M3.6 Tomas Garcia, Rogelio (CERN) et al. 01 November 2018 The European Circular Energy-Frontier Collider

More information

RING-RING DESIGN. Miriam Fitterer, CERN - KIT for the LHeC study group

RING-RING DESIGN. Miriam Fitterer, CERN - KIT for the LHeC study group RING-RING DESIGN Miriam Fitterer, CERN - KIT for the LHeC study group LHeC Design Options LHeC Design Options Linac-Ring LHeC Design Options Linac-Ring Ring-Ring Point 4 P Z4 5 P M4 5 P X4 6 Point 5 P

More information

4.3 Novel Lattice Solutions for the LheC

4.3 Novel Lattice Solutions for the LheC 135 Squeezing (ATS) scheme, CERN-ATS-2012-069, pp.128-134, Chamonix 2012 Workshop on LHC Performance, Chamonix, France, 6-10 Feb 2012. 20. S. Fartoukh, et al., The 10 cm beta* ATS MD, CERN-ATS-Note-2013-004

More information

Interstage Optics Design

Interstage Optics Design Interstage Optics Design for a PWFA Linear Collider FACETII Workshop 2015 Oct 14, 2015 Carl A Lindstrøm PhD Student University of Oslo, Department of Physics Advisor: Erik Adli 1 Proposed layout of a PWFA

More information

Director s Accelerator R&D Review CASA Summary/ELIC

Director s Accelerator R&D Review CASA Summary/ELIC Director s Accelerator R&D Review CASA Summary/ELIC Geoffrey Krafft On behalf of the members of the Center for Advanced Studies of Accelerators March 2, 29 Director s Review 8/GAK Page 1 OUTLINE Introduction

More information

Nonlinear Perturbations for High Luminosity e+e Collider Interaction Region

Nonlinear Perturbations for High Luminosity e+e Collider Interaction Region Nonlinear Perturbations for High Luminosit e+e Collider Interaction Region A.Bogomagkov, E.Levichev, P.Piminov Budker Institute of Nuclear Phsics Novosibirsk, RUSSIA IAS HEP Conference, 18-1 Jan 016, Hong

More information

Start-to-end beam optics development and multi-particle tracking for the ILC undulator-based positron source*

Start-to-end beam optics development and multi-particle tracking for the ILC undulator-based positron source* SLAC-PUB-12239 January 27 (A) Start-to-end beam optics development and multi-particle tracking for the ILC undulator-based positron source* F. Zhou, Y. Batygin, Y. Nosochkov, J. C. Sheppard, and M. D.

More information

The Detector Design of the Jefferson Lab EIC

The Detector Design of the Jefferson Lab EIC The Detector Design of the Jefferson Lab EIC Jefferson Lab E-mail: mdiefent@jlab.org The Electron-Ion Collider (EIC) is envisioned as the next-generation U.S. facility to study quarks and gluons in strongly

More information

Proposta per l'uso di DAFNE come allungatore d'impulso per il fascio di positroni del Linac

Proposta per l'uso di DAFNE come allungatore d'impulso per il fascio di positroni del Linac Proposta per l'uso di DAFNE come allungatore d'impulso per il fascio di positroni del Linac S. Guiducci 29 novembre 2017 11/29/17 1 The PADME experiment at BTF The PADME experiment proposes a search for

More information

Preliminary design study of JUICE. Joint Universities International Circular Electronsynchrotron

Preliminary design study of JUICE. Joint Universities International Circular Electronsynchrotron Preliminary design study of JUICE Joint Universities International Circular Electronsynchrotron Goal Make a 3th generation Synchrotron Radiation Lightsource at 3 GeV Goal Make a 3th generation Synchrotron

More information

CEPC partial double ring magnet error effects

CEPC partial double ring magnet error effects CEPC partial double ring magnet error effects Sha Bai, Dengjie Xiao, Yiwei Wang, Feng Su, Huiping Geng, Dou Wang 2016 04 08 CEPC SppC study group meeting LEP Alignment parameters From: LEP Design Report

More information

Spin Dynamics at the NLC

Spin Dynamics at the NLC BI TN-2004-3 Revision 0: June 1, 2004 Spin Dynamics at the NLC Ken Moffeit and Mike Woods SLAC Abstract This note describes spin transport and depolarization effects at the NLC. We also discuss the difference

More information

Minimum emittance superbend lattices?

Minimum emittance superbend lattices? SLS-TME-TA-2006-0297 3rd January 2007 Minimum emittance superbend lattices? Andreas Streun Paul Scherrer Institut, CH-5232 Villigen PSI, Switzerland Andreas Streun, PSI, Dec.2004 Minimum emittance superbend

More information

Tools of Particle Physics I Accelerators

Tools of Particle Physics I Accelerators Tools of Particle Physics I Accelerators W.S. Graves July, 2011 MIT W.S. Graves July, 2011 1.Introduction to Accelerator Physics 2.Three Big Machines Large Hadron Collider (LHC) International Linear Collider

More information

Beam loss background and collimator design in CEPC double ring scheme

Beam loss background and collimator design in CEPC double ring scheme Beam loss background and collimator design in CEPC double ring scheme Sha Bai 9 th International Particle Accelerator Conference (IPAC 18), Vancouver, Canada, Apr 29-May 4, 2018. 2018-05-01 Outline Introduction

More information

Diagnostics at the MAX IV 3 GeV storage ring during commissioning. PPT-mall 2. Åke Andersson On behalf of the MAX IV team

Diagnostics at the MAX IV 3 GeV storage ring during commissioning. PPT-mall 2. Åke Andersson On behalf of the MAX IV team Diagnostics at the MAX IV 3 GeV storage ring during commissioning PPT-mall 2 Åke Andersson On behalf of the MAX IV team IBIC Med 2016, linje Barcelona Outline MAX IV facility overview Linac injector mode

More information

The optimization for the conceptual design of a 300 MeV proton synchrotron *

The optimization for the conceptual design of a 300 MeV proton synchrotron * The optimization for the conceptual design of a 300 MeV proton synchrotron * Yu-Wen An ( 安宇文 ) 1,2), Hong-Fei Ji ( 纪红飞 ) 1,2), Sheng Wang ( 王生 ) 1,2), Liang-Sheng Huang ( 黄良生 ) 1,2;1) 1 Institute of High

More information

Bernhard Holzer, CERN-LHC

Bernhard Holzer, CERN-LHC Bernhard Holzer, CERN-LHC * Bernhard Holzer, CERN CAS Prague 2014 x Liouville: in reasonable storage rings area in phase space is constant. A = π*ε=const x ε beam emittance = woozilycity of the particle

More information

USPAS Accelerator Physics 2017 University of California, Davis

USPAS Accelerator Physics 2017 University of California, Davis USPAS Accelerator Physics 207 University of California, Davis Lattice Extras: Linear Errors, Doglegs, Chicanes, Achromatic Conditions, Emittance Exchange Todd Satogata (Jefferson Lab) / satogata@jlab.org

More information

Lattices for Light Sources

Lattices for Light Sources Andreas Streun Swiss Light Source SLS, Paul Scherrer Institute, Villigen, Switzerland Contents: Global requirements: size, brightness, stability Lattice building blocks: magnets and other devices Emittance:

More information