Central Region Group Status and Positron Region

Similar documents
ILC. CFS update for Europe (CERN): Cross Sections 3d Layout and BDS tunnel diameters CERN Resources. LCWS10 and ILC10 - Beijing

Summary of Working Group C: Injection, Extraction, Accelerator Systems

Major Upgrade Activity of the PLS in PAL: PLS-II

Low Beta Cryomodule Development at Fermilab. Tom Nicol March 2, 2011

KAON Factory Alignment

Progress Towards Doubling the Beam Power at Fermilab s Accelerator Complex

Groove Mitigation and Plans

M. Modena - CERN. 18 th ATF2 Project Meeting, 26 Feb. 2015, LAPP, Annecy-F

SNS Operation and Upgrade Plans

Workshop on Accelerator Operations Roger Erickson Accelerator Operations and Safety Division

PETRA III Damping Sections

Experiences from First Top-Off Injection At The Stanford Synchrotron Radiation Lightsource

M. A. Green, and S. Yu Lawrence Berkeley National Laboratory, Berkeley CA 94720, USA

The CU Beam Test at CERN Status Report and highlights from workshop II

Electron Beam Alignment Strategy in the LCLS Undulators

Vacuum pumps for the ESRF EBS project Michael Hahn

Beam Energy Absorber and

Status of the Nuclotron-M project

Present and Future Cryogenics at Cornell

Carlo J. Bocchetta ESLS XIX Aarhus, Denmark November Status of Solaris

Magnet, Support and Infrastructure. Whit Seay November 7, 2014

Created: 4/23/2003 Page: 1 of 12. Abstract

Shifting Frontiers: Evolving the Fermilab Accelerator Complex

Owned and operated as a joint venture by a consortium of Canadian universities via a contribution through the National Research Council Canada

THE Gersh Budker Prize PRIZE FOR.THE SUCCESSFUL CONSTRUCTION AND COMMISSIONING OF THE SPALLATION NEUTRON SOURCE

The daily grind Cat fines and engine wear, Part 2

NLCTA Accelerator Safety Envelope

Activities of Hitachi Regarding Construction of the J-PARC Accelerator

Coreless Concept for High Gradient Induction Cell

Solenoid Magnets for the Front End of a Neutrino Factory

THE 12 GeV ENERGY UPGRADE AT JEFFERSON LABORATORY

The DRYSMES4GRID project: development of a cryogen free cooled 500 kj / 200 kw SMES demonstrator based on MgB 2

Zhiwen Zhao (UVa), Paul Reimer (ANL) SoLID Collboration Meeting 2013/03

Performance of Small-Gap Undulators at the SLS Intermediate Energy Storage Ring

The Generator-Electric Vehicle- A New Approach for Sustainable and Affordable Mobility

ALIGNMENT AND STABILITY OF THE TPS STORAGE RING AUTO- TUNING GIRDER SYSTEM

Estimation Approval Confirmation. Dear. Machine name : ACR- 2P. 20- Jul Author Review Confirm

SBS Update Mark Jones

The H1 Silicon Tracker. Benno List

KWS1, KWS2 housing including disk and dummy lower housing (left); view into lower housing (right)

Workshop on Automotive Stack Design Options, Platform Concept, and Cost Targets

The Status of SSRF Survey and Alignment System. ChenghaoYu, Hanwen Du Lixin Yin

Status of the DARHT 2 nd Axis Accelerator at Los Alamos National Laboratory

Task Cryomodule. Paolo Pierini INFN Sezione di Milano - LASA

Antiproton production horn operation and testing

Research on Transient Stability of Large Scale Onshore Wind Power Transmission via LCC HVDC

LiDAR Teach-In OSRAM Licht AG June 20, 2018 Munich Light is OSRAM

The ATLAS Detector at the Large Hadron Collider. Peter Krieger IPP/University of Toronto

Study of the impact of the remote alignment in the vacuum system

MOLLER Hybrid Toroid Engineering Design

The g-2 Project at FNAL. Horst Friedsam John Kyle IWAA 2014 at Beijing October 2014

Beam Test Results and ORCA validation for CMS EMU CSC front-end electronics N. Terentiev

Mineral Industry. Drive solutions for reclaimers, stackers, bulk conveyors applications

Electric Vehicles and the Environment (EVE IWG)

Ambient Magnetic Field Compensation for the ARIEL (Advanced Rare IsotopE Laboratory) Electron Beamline. Gabriela Arias April 2014, TRIUMF

Pedro Nunes. July 2016

Advant OCS controls cryogenic installations of CERN s particle accelerator

COMPARING SLOTTED vs. SLOTLESS BRUSHLESS DC MOTORS

RPCs for an atmospheric neutrino experiment

15 steel septum magnets MSD of three types MSDA, MSDB, and MSDC, located around IP6;

A Homopolar Inductor Motor/Generator and Six-step Drive Flywheel Energy Storage System

Electromagnetism - Invisible Forces

EKM Series Motors. For Aerospace & Defense Applications

Introduction. 1/2 Overview 1/3 Benefits 1/3 Application. 1/3 Order No. code. 1/4 Protection strategy

OMEGA and OMEGA EP Will Provide Key Physics Data for Laser IFE. J. M. Soures University of Rochester Laboratory for Laser Energetics

E / HYDAC KineSys Electric cylinders (HEZ)

Edgard Vangeel (Data on radars provided by EUMETNET) DFS Update: European Weather Radars Details & Overview

Featured Articles Utilization of AI in the Railway Sector Case Study of Energy Efficiency in Railway Operations

General Purpose Permanent Magnet Motor Drive without Speed and Position Sensor

System Integration of an Electronic Monitoring System in All-Terrain Vehicles

XFEL Bunch Compressor BC1 and BC2 Vacuum Issues

PLS Upgrade Project (PLS-II)Status

Toyota s European Exposure How did Toyota s European operations structure create operating exposure?

2006 MINI Cooper S GENINFO Starting - Overview - MINI

54 rd Meeting Informal Group on Child Restraint Systems Booster Seat Width Development. 27 th October2015

Cable Dragging Horizontal Takeoff Spacecraft Air Launch System

ADLATUS CR700. Fully autonomous cleaning robot system

PROJECT IDEA SUBMISSION STUDENT

Forward-Looking Statements

Strategy for Promoting Centers of Excellence (CoE) Activities

HVDC. TMT&D provides the best and most economical HVDC system.

HS-1000 Fast Low Noise High Voltage Switch

There s a new power in Solar 1500V ultra-high power string inverters for utility-scale PV applications

Cryogenic Improvements for the ATLAS Energy Upgrade

High Speed Rail Regional Impact

FRENIC-Mega Series of High-performance Multi-function Inverters

PowerTech converter family for industry and energy

PEAK DEMAND MANAGEMENT IN NEW ENGLAND A DYNAMIC SOLUTION TO MANAGING PEAK DEMAND CHARGES

Lunar Architecture and LRO

Recent Status of NEDO s EV Quick Charger related Projects

Integration issues in the tunnel and Impact on general LHC systems

Available online at ScienceDirect. Physics Procedia 67 (2015 )

General Atomics Urban Maglev: Moving Towards Demonstration

Mu2e Solenoids! Michael Lamm! L2 for the Mu2e Solenoid! July 27, 2015!

PowerGen Europe 2014 CIMAC circle

Calorimeter Subsystem. Status and Issues. W. Neil Johnson Naval Research Laboratory. Gamma-ray Large Area Space Telescope

Technical Presentation model

Carleton University ELEC DC Motor Project. Author: Adam Heffernan. Student Number: Project

Two Cell Battery. 6. Masking tape 7. Wire cutters 8. Vinegar 9. Salt 10. Lemon Juice DC ammeter

ZF posts record sales in 2017; announces increased research and development activities

Transcription:

Central Region Group Status and Positron Region K. Yokoya 2016.9.14. Posipol2016, LAL 2016/9/14 Posipol2016 1

Issues Discussed in CRWG Positron-related 10Hz operation Auxiliary positron source (APS) Positron target region MPS,PPS Beam dumps Main dumps Tune-up dumps BDS-related Muon wall Tunnel of the Central Region 2016/9/14 Posipol2016 2

These are already accepted? Relocation of positron booster linac Yes Positron spin rotator 2 parallel line for up and down polarization (strong request from physics and positron groups) Superconducting or normal-conducting solenoid? Location of Global timing chicane 400MeV 5GeV Yes DR Location of 1.5km ML tunnel extention Not yet 2016/9/14 Posipol2016 3

10Hz Operation TDR mentions 10Hz operation for E CM < 250GeV Gives parameter sets for 200 and 230GeV Damping ring with stronger wigglers But detail of linac operation, additional beam line, beam dynamics are not given Is 10Hz operation really needed? 200-250GeV: sweep the region above LEP But most important is Z-pole (92GeV) and W-pair (160GeV) Conclusion in CRWG Prepare spaces for beamlines that guarantee down to E CM =200GeV Preliminary beamline optics to tune-up dump by Okugi This does not guarantee E CM <200GeV. Beam dynamics complex Will think of 92GeV and 160GeV later, if turn out to be necessary 2016/9/14 Posipol2016 4

Tune-up Dumps Change of the commissioning strategy Tuning by weak beam using local tune-up dumps Use main dumps for full current tuning Reduced power scale of all the tune-up dumps Maximum ~400kW Except main dumps (E-5,E+5) and photon dump E+7 Proposal of a new dump E+8 for spent electron after positron generation in 5+5 Hz operation Will soon come to a change request 2016/9/14 Posipol2016 5

New specification of Power Levels Not final yet TDR New spec (margin not added) kw MPD E-1 ** SC tune-up dump 311 60 MPD E-2 EDRX tune-up dump 220 60 MPD E-3 RTML tune-up dump 220 60 HPD E-4 BDS tune-up dump 1) 14000 400 HPD E-5 * Primary e- dump 14000 14000 MPD E-6 RTML tune-up dump 220 60 MPD E-7 Electron fast abort dump 250 60 E-8 Spent electron dump for 5+5Hz none 6300 MPD E+1 ** SC tune-up dump 311 60 MPD E+2 PDRX tune-up dump 220 60 MPD E+3 RTML tune-up dump 220 60 HPD E+4 BDS tune-up dump 14000 400 HPD E+5 * Primary e+ dump 14000 14000 MPD E+6 RTML tune-up dump 220 60 MPD E+7 * Target dump (mostly as photons) 200 300 ** 45kW always on * non-stop dump (always on) MPD High power dump HPD Medium power dump 1) Also as spent electron dump for 5+5Hz in TDR 2016/9/14 Posipol2016 6

XFEL Dump Solid dump being constructed as the main beam dump for XFEL Similar pulse structure and total power as ILC BDS tune-up dump and undulator photon dump Except (compared with photon dump) Electron dump vs. photon Max energy 25GeV vs. some 100MeV (Be careful: lower energy does not mean easier) XFEL Beam Parameters for the main beam dump Beam energy =< 25GeV Repetition rate 10Hz Bunch distance >= 200ns Average power <= 300kW Pulse length <= 800µs RMS spot (x,y) >= 2mm Bunch charge <= 1nC Slow sweep R=5cm Train charge <= 4000nC Fast (ibtratrain) sweep no Train energy <= 100kJ Life 20 years Description of the Beam Dump Systems for the European XFEL M. Schmitz, EDMS: D00000004303811 Feb.4.2014 2016/9/14 Posipol2016 7

2016/9/14 Posipol2016 8

2016/9/14 Posipol2016 9

Main Dumps Two 14 MW main dumps (plus 6.3MW spent electron dump) Detailed check of the dump system is not CRWG expertise Need specialist team Beam dump specialists CFS Issues Robot work Safety in particular window breakdown Required human access 2016/9/14 Posipol2016 10

10atm water beam dump layout B. Smith, CCLRC: 0-TB-0067-404-00-A D00000000945405 2016/9/14 Posipol2016 11

Water beam dump surface site scheme B. Smith, CCLRC: 0-TB-0067-410-00-A D00000000945465 Shows surface facilities that service the dump, including cooling and exhaust for gases (tritium!) 2016/9/14 Posipol2016 12

Positron (target region) Main issues needed as inputs to CRWG Design of photon dump A problem (radiation damage of the window by photon beam) of TDR design pointed out at Santander Required shielding of the target region including the thoughts on Target replacement Where/how waste targets to be stored Path to take waste target to the surface Will be discussed in POSIPOL@LAL next week This would take some more time 2016/9/14 Posipol2016 13

Consensus among ILC positron team No human access to the accelerator and service tunnels needed during high-energy beam on (normal operation and commissioning) as in main linac region Special shield wall needed for target+fc+solenoid+a few cavities Photon/electron dumps must also be shielded This figure is for illustration only. To be discussed in the WS 2016/9/14 Posipol2016 14

BDS Tunnel (electron) Okugi s proposal Single (kamaboko) tunnel from ML end to e+ ECS Twin tunnel to muon wall Penetration for cables only (no waveguides) Small tunnel cross-section possible after collimators Must come to final conclusion Info from positron team needed e-linac end IP 2016/9/14 Posipol2016 15

BDS Tunnel (positron) Okugi s proposal Move electron source upstream Must come to final conclusion Required size of the components Then, send to CFS team for tunnel layout TDR Okugi 2016/9/14 Posipol2016 16

Muon Wall TDR: 5m long magnetized spoiler, filling the tunnel crosssection. Background to the detector was re-estimated with different conditions #/200 bunches R=6.5m detector No spoilers 138 9648 2x 5m mag.spoilers 25 1008 5x 5m toroid 3.3 273 both 0.5 17 #/200 bunches R=2.5m TPC Can we remove 5m magnetized iron? 2016/9/14 Posipol2016 17

Auxiliary Positron Source Our conclusion has been to retain it for DR and BDS commissioning Weak intensity but can still useful for DR emittance tuning if stacking possible Does it require a wider tunnel? Now, under new commissioning strategy, is it still useful? 2016/9/14 Posipol2016 18

New Members to CRWG Members Since Dec.2015) K.Yokoya (KEK,chair), E.Paterson (SLAC), G.White (SLAC), B.List (DESY), T.Okugi (KEK), M.Kuriki (Hiroshima U.), M.Miyahara (KEK), T.Sanuki (Tohoku U.) Reorganization of CFS team in Japan Lead by Hayano & Terunuma New members (all KEK) Shinichiro Michizono Hitoshi Hayano Nobuhiro Terunuma 2016/9/14 Posipol2016 19

Future Plan Expect change of organization in December Some items may come to conclusion by that time Positron BDS tunnel Auxiliary positron source Some items require more inputs Electron BDS tunnel including positron target region Main dump-related issues Whole system must be reviewed Installation Commissioning Accidents Problem Expand the expertise? 2016/9/14 Posipol2016 20

Recent Decision by the Technical Board after a meeting with CRWG The CRWG will submit a CR to specify the dump layout and power levels. We will try to do this before the Sept 20th CMB meeting. Glen White will work with the experimentalists to ascertain whether the muon spoiler is necessary. If not then a CR will be generated. The CFS team will create a basic central region concept based on Okugi-san s 2-tunnel scheme. It is recognized that no design exists at present for the high power (multi-mw dumps) so these areas will be shown generically. Likewise the positron target area and photon dump is also not defined and again will be represented generically for the present time. We will endeavor to obtain assistance (from CERN) to develop the design of the high power dumps and associated remote handling scheme. The low power dumps will be based on the existing designs such as he solid dump for XFEL and aluminum ball dump of JLAB. There will be no action on the positron system until after the upcoming POSIPOL meeting 2016/9/14 Posipol2016 21