Upgrade of CEBAF to 12 GeV

Similar documents
THE JLAB 12 GEV ENERGY UPGRADE OF CEBAF *

RF Upgrades & Experience At JLab. Rick Nelson

Experience with the Cornell ERL Injector SRF Cryomodule during High Beam Current Operation

3 cerl. 3-1 cerl Overview. 3-2 High-brightness DC Photocathode Gun and Gun Test Beamline

Introduction: CW SRF linac types, requirements and challenges High power RF system architecture

2 Work Package and Work Unit descriptions. 2.8 WP8: RF Systems (R. Ruber, Uppsala)

RF considerations for SwissFEL

PoS(EPS-HEP2015)525. The RF system for FCC-ee. A. Butterworth CERN 1211 Geneva 23, Switzerland

PEP II Design Outline

The ESS Accelerator. For Norwegian Industry and Research. Oslo, 24 Sept Håkan Danared Deputy Head Accelerator Division Group Leader Beam Physics

SUMMARY OF THE ILC R&D AND DESIGN

Operating Experience and Reliability Improvements on the 5 kw CW Klystron at Jefferson Lab

LLRF at SSRF. Yubin Zhao

RF Power Upgrade at Jefferson Lab

High Brightness Injector Development and ERL Planning at Cornell. Charlie Sinclair Cornell University Laboratory for Elementary-Particle Physics

!"!3

The LEP Superconducting RF System

5 Project Costs and Schedule

ILC-LNF TECHNICAL NOTE

A Cathode Development Cornell Cultera This scope includes all labor and purchases required produce photocathodes required by CBETA.

AREAL- Phase 1. B. Grigoryan on behalf of AREAL team

DESIGN OF 1.2-GEV SCL AS NEW INJECTOR FOR THE BNL AGS*

LSD Review December 2012 Schedule, Re-Baseline, & Resource Analysis

Diamond RF Status (RF Activities at Daresbury) Mike Dykes

Oak Ridge Spallation Neutron Source Proton Power Upgrade Project and Second Target Station Project

SRS and ERLP developments. Andrew moss

Extraction/Separator Setup. Michael Spata Operations Stay Treat July 16, 2015

Welcome and FRIB Project Status. FRIB Highlights and Plan Ahead

Detailed Design Report

Low Level RF for PIP-II. Jonathan Edelen LLRF 2017 Workshop (Barcelona) 16 Oct 2017

BBU threshold current study for 6 GeV beam in 12 GeV beamline setup

Workshop on Accelerator Operations August 6-10, 2012 Glen D. Johns Accelerator Operations Manager

INFN School on Electron Accelerators. RF Power Sources and Distribution

NSLS-II RF Systems James Rose, Radio Frequency Group Leader PAC 2011

CEBAF Accelerator Update. Michael Tiefenback CASA Accelerator Physics Experimental Liaison June 14, 2017

IOT OPERATIONAL EXPERIENCE ON ALICE AND EMMA AT DARESBURY LABORATORY

The PEFP 20-MeV Proton Linear Accelerator

LCLS RF Reference and Control R. Akre Last Update Sector 0 RF and Timing Systems

TITLE PAGE. Title of paper: PUSH-PULL FEL, A NEW ERL CONCEPT Author: Andrew Hutton. Author Affiliation: Jefferson Lab. Requested Proceedings:

Status of SOLARIS. Paweł Borowiec On behalf of Solaris Team

Bunch-by-bunch feedback and LLRF at ELSA

Synchrotron Light Facility. Operation of ALBA RF. Angela Salom on behalf of RF team: Francis Perez, Bea Bravo and Jesus Ocampo

ANKA RF System - Upgrade Strategies

CLIC Feasibility Demonstration at CTF3

JEFFERSON LAB, A STATUS REPORT*

High Rep Rate Guns: FZD Superconducting RF Photogun

North Damping Ring RF

9th ESLS RF Meeting September ALBA RF System. F. Perez. RF System 1/20

Empirical Model For ESS Klystron Cathode Voltage

XFEL High Power RF System Recent Developments

Jefferson Lab Experience with Beam Halo, Beam Loss, etc.

STATUS AND COMMISSIONING RESULTS OF THE R&D ERL AT BNL*

Effects of the cryogenics operational conditions on the mechanical stability of the FLASH linac modules

ESS: The Machine. Bucharest, 24 April Håkan Danared Deputy Head Accelerator Division. H. Danared Industry & Partner Days Bucharest Page 1

A New High Intensity Proton Source. The SCRF Proton Driver. (and more!) at Fermilab. July 15, Bill Foster SRF2005

RF Power Generation II

ANKA Status Report. N.Smale, on behalf of all ANKA colleagues, Directors : A.-S. Müller, C Heske, T Baumbach.

Evaluation of Performance, Reliability, and Risk for High Peak Power RF Sources from S-band through X-band for Advanced Accelerator Applications

PRESENT STATUS OF J-PARC

The Construction Status of CSNS Linac

PEP-II Overview & Ramp Down Plan. J. Seeman DOE PEP-II Ramp Down-D&D Review August 6-7, 2007

A HIGH-POWER SUPERCONDUCTING H - LINAC (SPL) AT CERN

Status of BESSY II and berlinpro. Wolfgang Anders. Helmholtz-Zentrum Berlin for Materials and Energy (HZB) 20th ESLS-RF Meeting

Concept and R&D Plans for Project X

RF Power Klystrons & 20 Year Look. R. Nelson 7/15/15

A Fifteen Year Perspective on the Design and Performance of the SNS Accelerator

The TESLA RF System. S. Choroba. for the TESLA Collaboration. DESY Notkestr. 85, D Hamburg, Germany

CEBAF 12GeV Commissioning: Status and Plans

WG2 Group Summary. Chris Adolphsen Terry Garvey Hitoshi Hayano

Status of CTF3. G.Geschonke CERN, AB

RF plans for ESS. Morten Jensen. ESLS-RF 2013 Berlin

Next Linear Collider. The 8-Pack Project. 8-Pack Project. Four 50 MW XL4 X-band klystrons installed on the 8-Pack

An Operational Diagnostic Complement for Positrons at CEBAF/JLab

Dark current and multipacting trajectories simulations for the RF Photo Gun at PITZ

LEP OPERATION AND PERFORMANCE WITH ELECTRON-POSITRON COLLISIONS AT 209 GEV

CONSTRUCTION AND COMMISSIONING OF BEPCII

TTF / VUV-FEL. Schedule 2005 and Project Management Issues. Schedule 2005 Project Organisation Budget & Controlling

Proton Engineering Frontier Project

The Elettra Storage Ring and Top-Up Operation

PEP II STATUS AND PLANS *

STATUS OF THE INTERNATIONAL LINEAR COLLIDER

ESS Linac WP8 Radio Frequency Systems and Test Facilities

COMMISSIONING SCENARIOS FOR THE J-PARC ACCELERATOR COMPLEX

Electron linac photo-fission driver for rare isotope program at TRIUMF

The FAIR plinac RF Systems

A HIGH POWER LONG PULSE HIGH EFFICIENCY MULTI BEAM KLYSTRON

4.4 Injector Linear Accelerator

PHIN. Report on the Development of a Radio-Frequency Photo Electron Source with Superconducting Niobium Cavity (SRF Gun Realization)

Beam Loss Detection for MPS at FRIB

Suggested ILC Beam Parameter Range Rev. 2/28/05 Tor Raubenheimer

Commissioning of Accelerators. Dr. Marc Munoz (with the help of R. Miyamoto, C. Plostinar and M. Eshraqi)

Jae-Young Choi On behalf of PLS-II Linac team

Accelerator Instrumentation RD. Monday, July 14, 2003 Marc Ross

The FLASH objective: SASE between 60 and 13 nm

News from HZB / BESSY Wolfgang Anders at ESLS-RF Meeting September 2010 Trieste

Pulsed Klystrons for Next Generation Neutron Sources Edward L. Eisen - CPI, Inc. Palo Alto, CA, USA

Production of accelerators and accelerator components in industry

The Beam Test Facility at the SNS

STATUS OF THE EUROPEAN XFEL CONSTRUCTING THE 17.5 GEV SUPERCONDUCTING LINEAR ACCELERATOR

RUNNING EXPERIENCE OF FZD SRF PHOTOINJECTOR

Transcription:

Upgrade of CEBAF to 12 GeV Leigh Harwood (for 12 GeV Accelerator team) Page 1

Outline Background High-level description Schedule Sub-system descriptions and status Summary Page 2

CEBAF Science Mission CEBAF was originally built to establish a deep understanding of the quark/gluon structure of nuclei. (non-perturbative QCD) The program to date has been highly successful. Theoretical initiatives identified critical areas with new opportunities for understanding. Explanation for quark confinement (exotic meson spectroscopy) Tomography of the nucleus with Generalized Parton Distributions Valence quark behavior Investigating these open questions required doubling the CEBAF beam energy Page 3

12 GeV Upgrade Project Scope of the project includes: Doubling the accelerator beam energy New experimental Hall and beamline Upgrades to existing Experimental Halls The completion of the 12 GeV Upgrade of CEBAF was ranked the highest priority in the 2007 NSAC Long Range Plan. This priority was re-iterated in an 2013 NSAC report to DOE/NP The Upgrade is built on an existing facility: The vast majority of accelerator and experimental equipment have continued use Page 4

6 GeV CEBAF 550m 42 cryomodules (1497 MHz, 9m long) 8 cavities/cryomodule with individual power and control (343 klystrons+controls) Helium plant: 4.6 kw @ 2K >2200 magnets with >1800 power supplies Page 5

12 6 GeV CEBAF Add 5 100MV cryomodules Add beamline Upgrade magnets and power supplies CHL-2 CHL-2 has same capability as CHL-1 Add arc Add 5 100MV cryomodules Two 1.1 0.6 GeV linacs New cryomodules get new rf zones (80 individually controlled klystrons) Page 6

Schedule: Long View Page 7

Sub-system Descriptions and Status Page 8

Cryomodules: Scope & Key Technical Parameters Scope: Develop, Design, Fabricate, Install and Check-out 10 Cryomodules (5 new cryomodules per linac) (The following parameters are for each Cryomodule) Voltage (Includes 10% reserve): 98MV (108 MV) (ensemble average in each linac) Heat budget: (Interface with Cryogenics) 2 K 300 W 50 K 300 W Slot Length: 9.8 m Tuner resolution: 2 Hz (stepper + PZT) Fundamental Power Coupler: 7.5/13 kw (Avg/Pk) Higher Order Mode (HOM) damping: Transverse (R/Q)Qk < 2.4 x 10 10 Ω/m Longitudinal (R/Q)Q < 6.5 x 10 11 Ω Cryomodule Length (Physical) ~8.5m Page 9

Cryomodules: Status Checked out in tunnel #1 104 MV #2 110 MV #3 118 MV #4 106 MV #5 110 MV #6 108 MV #7 108 MV #8 #9 114 MV #10 110 MV Avg 109 MV Avg Q 0 @ 19.2MV = 8.1x10 9 Final C100 installed in linac Hogan: WEZAA2 Page 10

RF: Key Technical Parameters Ten new zones of RF power for new accelerating structures: Operating Freq: 1497 MHz Eight cavities per zone Individual low-level controls Cavity Q L : 2x10 7 Operating Gradients: >17.5 MV/m One cavity per klystron 1.0 EPICS IOC Phase Stability (rms) Amplitude (rms) Ethernet Fast ( <1sec) Slow (>1sec) 0.5º 3.0º 4.5x10-4 NA High Voltage Power Supply PwrSupply 0.9 Energy Content (Norm.) Cavity de-tuning curve 0.8 0.7 0.6 0.5 0.4 0.3 0.2 MO Master Oscillator Ethernet LL LLRF Controls Klystron 8 0.1 0.0-600 -500-400 -300-200 -100 0 Detuning (Hz) SRF cavity Superconducting Cavity Page 11

RF details Low Level RF Ground-breaking digital solution for cw controls Double-moded Self-Excited Loop (SEL): If phase/amplitude control is not needed Permits cavities to be energized and quickly brought onto resonance. Mitigates the doublevalued detuning curve. Generator-Driven Resonator: When phase/amplitude control is needed for beam Hovater: TUZBA1 Hoffler: THTB1 High power RF New 13kW klystron Only 2 cavities/klystrons per high-power amplifier Improved up time Installation is complete Page 12

RF: Layout Control racks, PSU s Manifolds Klystrons Waveguide components Cathode power supply Page 13

RF: LLRF/HPA Control Systems Field Control Chassis Page 14 Cryomodule Interlocks Chassis High Power Amplifier Control Chassis Stepper Tuner Control Chassis Piezo Tuner Amplifier Chassis Klystron Solenoid Power Supplies

Cryogenics Double the capacity of 2K plant: 4.6kW 9kW New 4.5K helium refrigerator: 4.6kW @ 2.1K, 12kW@35K plus 15 g/s of 4.5K liquefaction Modified the cryogenic distribution system for the interconnection of 10 new C100 cryomodules Note: Leveraged an existing 2K coldbox Status 4.5K coldbox has been accepted Distribution system is complete Commissioning on integrated system is underway Page 15

Cryogenics (cont d) Lower coldbox Upper coldbox Page 16

Beamlines Overall length (excluding linacs) Original: 4.3 km Upgrade: 4.9 km New 10 th recirculation arc and beamline to new Hall D Original layout retained (including dipole & quad locations) Almost all magnets were reused Dipoles Beam energy at any location has increased by ~2x, so BdL of dipoles much increase by same ratio Solution: Increase the current in the dipoles by 2x Saturation was beaten by adding more return iron» Changed C dipoles to H Quads Most reused w/o change ~100 were shifted to higher-current power supplies Page 17

Beamlines (cont d) Magnets Major ( 1m) dipoles Quads Steering dipoles Original 452 705 750 Upgrade Unchanged 27 635 750 Reworked* 425 0 0 New 43 114 64 *Reworked: disassembled, insulation replaced, iron modified and/or added, coils reconfigured on some magnets, reassembled, QA ed and field mapped Power supplies 35-260kW 40-1080kW 10A/20V 20A/70V Original 22 1455 Upgrade Reused 9 1322 New 15 240 Page 18

Beamlines (cont d) Original Removed original East Recombiner East Arcs 12GeV Page 19

Extraction: Beam to 3 Halls at Once New Relocated Modified Elevation View Pass 1 Pass 2 Pass 3 Pass 4 Pass 5 Horizontally deflecting RF cavities (499MHz, copper) Horizontally deflecting septa Recirculation ARCS Horizontally deflecting dipoles Horizontally deflecting Lambertson Plan View 1497 MHz Page 20

I&C/Safety Added diagnostics and machine protection systems for new beamlines New design for beam position monitor electronics was needed because of obsolescence of components for original Expanded network and modify control software for new cryomodule/rf zones, magnet power supplies, and CHL expansion Modified control software to incorporate new magnet power supplies and new cryomodule/rf zones Expanded personnel safety system to cover new Hall D Status Ready for beam commissioning Additions for Hall D will complete in FY14 Page 21

Schedule: 2009-now FY11 shutdown: Reworked 7 arcs and installed 2 zones of cryomodules & RF FY12-13 shutdown: Completed accelerator installation for commissioning Page 22

Cryomodule voltage 2012: Full Performance of C100 + RF was Demonstrated C100 Cryomodule Energy Gain May 18 th, 2012 Total current in linacs: 465 A 98 MeV 108 MeV 200 ENERGY GAIN (MeV) 150 100 50 Beam Current/pass ( A) TIME (in 20 minute increments) This is with beam going to the NP experiments Page 23

Costs Extraction Extraction 0.5% I&C/Safety Instrumentation & Control Systems 6.6% Construction Accelerator Breakout by Sub-system Cryogenics Cryomodules 26.1% Beam Transport 22.1% Beam Transport Total: $119M Cryogenics 26.0% Cryogenics Power Systems 18.7% Systems Page 24

Future What s after 12 GeV? The NP community is looking towards an Electron-Ion Collider. Zhang: TUZAA1 Page 25

Summary An exciting research program in the study of the quark structure of nuclei as well as the fundamental question of quark confinement is possible with a 12GeV cw electron beam. The CEBAF accelerator has been upgraded to deliver 12 GeV beam. The core of that upgrade was increasing the total linac voltage by 1.0 GV to a total of 2.2 GV. All systems have met their defined goals Beam commissioning is about to start! Page 26