Spear3 RF System Sam Park 11/06/2003. Spear3 RF System. High Power Components Operation and Control. RF Requirement.

Similar documents
Detailed Design Report

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

INFN School on Electron Accelerators. RF Power Sources and Distribution

IOT OPERATIONAL EXPERIENCE ON ALICE AND EMMA AT DARESBURY LABORATORY

RF Power Generation II

RF Upgrades & Experience At JLab. Rick Nelson

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

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

ANKA RF System - Upgrade Strategies

Program Risks Risk Analysis Fallback Plans for the. John T. Seeman DOE PEP-II Operations Review April 26, 2006

XFEL High Power RF System Recent Developments

18 GHz, 2.2 kw KLYSTRON GENERATOR GKP 24KP 18GHz WR62 3x400V

TECHNICAL SPECIFICATION Multi-beam S-band Klystron type BT267

North Damping Ring RF

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

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

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

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

Status and Plans for PEP-II

14 GHz, 2.2 kw KLYSTRON GENERATOR GKP 22KP 14GHz WR62 3x400V

DELIVERY RECORD. Location: Ibaraki, Japan

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

4.4 Injector Linear Accelerator

Status of SOLARIS. Paweł Borowiec On behalf of Solaris Team

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

CEBAF 8 kw CW KLYSTRON SPECIFICATION EE0043, Rev. H January 15, 1998

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

Diamond RF Status (RF Activities at Daresbury) Mike Dykes

PEP II Design Outline

Current status of XFEL/SPring-8 project and SCSS test accelerator

Design, Fabrication and Testing of Gun-Collector Test Module for 6 MW Peak, 24 kw Average Power, S-Band Klystron

TOSHIBA Industrial Magnetron E3328

Top-Up Experience at SPEAR3

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

LLRF at SSRF. Yubin Zhao

!"!3

The ALS RF systems, upgrades and ALS-U plans

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

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

Status of RF Power and Acceleration of the MAX IV - LINAC

STATUS OF THE SWISSFEL C-BAND LINEAR ACCELERATOR

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

RF Power Upgrade at Jefferson Lab

The Elettra Storage Ring and Top-Up Operation

A Unique Power Supply for the PEP II Klystron at SLAC*

KARA and FLUTE RF Overview/status

RF Solutions for Science.

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

KEKB INJECTOR LINAC AND UPGRADE FOR SUPERKEKB

The LEP Superconducting RF System

IOT RF Power Sources for Pulsed and CW Linacs

A New 4MW LHCD System for EAST

SRS and ERLP developments. Andrew moss

A HIGH POWER LONG PULSE HIGH EFFICIENCY MULTI BEAM KLYSTRON

GA A26497 SOLID-STATE HIGH-VOLTAGE CROWBAR UTILIZING SERIES-CONNECTED THYRISTORS

ILC-LNF TECHNICAL NOTE

KLYSTRON GUN ARCING AND MODULATOR PROTECTION

L-Band RF R&D. SLAC DOE Review June 15 th, Chris Adolphsen SLAC

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

SLS RF operation report 2003

Karin Rathsman. Calculations on the RF Source and Distribution

The PEFP 20-MeV Proton Linear Accelerator

SPEAR 3: Operations Update and Impact of Top-Off Injection

RF POWER GENERATION FOR FUTURE LINEAR COLLIDERS* 1. Introduction

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

Upgrading LHC Luminosity

Design Studies For The LCLS 120 Hz RF Gun Injector

RF considerations for SwissFEL

PEP-I1 RF Feedback System Simulation

PEP II STATUS AND PLANS *

ABORT DIAGNOSTICS AND ANALYSIS DURING KEKB OPERATION

AARHUS UNIVERSITET November, ASTRID2 Status. Heine Dølrath Thomsen on behalf of the ASTRID2 Team

Status of SOLARIS Arkadiusz Kisiel

OF THIS DOCUMENT IS W8.MTO ^ SF6

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

Review of Diamond SR RF Operation and Upgrades

Improvements to the APS LINAC and SR/Booster klystron HVPS, and Accomplishments of the 352MHz RFTS

Status of Elettra, top-up and other upgrades

THE NEXT LINEAR COLLIDER TEST ACCELERATOR: STATUS AND RESULTS * Abstract

45 MW, 22.8 GHz Second-Harmonic Multiplier for High-Gradient Tests*

reported by T. Shintake KEK / RIKEN Japan Summary of C-band R&D for Linear Collider at KEK New soft-x-ray FEL Project at RIKEN/SPring-8

Karin Rathsman, Håkan Danared and Rihua Zeng. Report from RF Power Source Workshop

PEP-II STATUS REPORT *

Status of CTF3. G.Geschonke CERN, AB

EPJ Web of Conferences 95,

650MHz/800kW Klystron Development at IHEP

Tutorial: Trak design of an electron injector for a coupled-cavity linear accelerator

PULSED MODULATOR TECHNOLOGY

Linac upgrade plan using a C-band system for SuperKEKB

PRESENT STATUS OF J-PARC

PEP II Status and Plans

The basic parameters of the pre-injector are listed in the Table below. 100 MeV

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

CEPC Klystron Development

4617 Super Power Triode

FIR Center Report. Development of Feedback Control Scheme for the Stabilization of Gyrotron Output Power

Pulses inside the pulse mode of operation at RF Gun

CLIC Feasibility Demonstration at CTF3

Klystron Lifetime Management System

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

Transcription:

Spear3 RF System RF Requirement Overall System High Power Components Operation and Control

SPEAR 3 History 1996 Low emittance lattices explored 1996 SPEAR 3 proposed 11/97 SPEAR 3 design study team formed 11/97 Director s Review 07/98 DOE Lehman Review FY99 DOE BES and NIH discuss joint funding 11/98 Active cavity and WG arcing 01/99 Additional funding for NEW RF (476.3 MHz) 04/99 Active RFHVPS failure. 01/00 Cavities ordered (Received 05/03) 03/00 Klystron ordered (Received 08/01, Repaired 05/03) 05/01 2.5 MW PS ordered (Received 01/02) 11/01 Circulator ordered (Received 11/01) 02/02 WG parts ordered (Receive 04/02) 03/02 LLRF work in progress 04/03 Installation (6 months) 12/03 Commissioning (3 months) 03/04 User Beam (3.0 GeV, 100 ma, 18 nm-rad)

Electron Beam Energy Loss due to Synchrotron Radiation Energy loss at bend magnets U 0-bend (kev/turn) = 88.5*(E b /GeV) 4 /(ρ/m) Energy loss at insertion device U 0-ID (kev/turn) = 0.633*(E b /GeV) 2 *<(B/T) 2 >*(L/m) 2 where <B> is the rms magnetic field of the pole and L is the insertion device length With beam energy E b =3.0GeV, bend radius ρ=7.86m, total beam power loss is 1.16MV*500mA=510 kw in 2003, and 1.33MV*500mA=665 kw in 2012 as the insertion devices are added on.

Spear 3 Beam Lifetime

Spear 3 RF Installation

SPEAR 3 Overall System

Klystron (Repaired Marconi) Maximum RF Power : P rf = 1.2 MW Beam Power : P b = V b *I b = 82 kv * 23.5 A = 1.93 MW Microperveance µp = I b /V b 1.5 * 10 6 = 1.00 Efficiency η = P rf /P b = 62% Gain A = 10*Log 10 (P rf /P drive ) = 45 db Drive amplifier power P drive = 40 W Cathode heater power P h = 110Vac*5.2A = 570 W Focusing magnet power P m = 70.2V*47.5A = 3.33kW No bucking coil power LCW flow for 1.5MW : 275 gpm, 150 psi, 32 ±1 o C 2 VacIon pumps, 8 L/s each

SPEAR 3 Klystron Spear3 klystron from Marconi That klystron was loaned to PEP2 The klystron failed, and rebuilt by PCI SLAC Klystron Dept to produce 4 klystrons Those SLAC klystrons have higher power capability Philips/EEV/Marconi Klystron Experience at SLAC No. Klystron Date failed Fil. Hrs Failure type Remedy 1 Philips #5 09/25/00 14,102 Heater short Rebuilt at CPI 2 Philips #5 03/29/01 13,895 Anode dislocation 3 Philips #5 05/22/01 5,740 Anode dislocation Rebuilt at SLAC 4 Marconi #3 07/17/01 1,350 Vacuum leak (up to 10 ma pump current) Rebuilt at CPI 5 Marconi #2 07/26/01 4,730 Vacuum leak (up to 60 ma pump current) Rebuilt at CPI

Marconi Klystron

ATF Circulator Specification Type: Y-Junction Y 3-port 3 Circulator Frequency : 476 ± 10 MHz Forward Power : 1.2 MW cw Reverse Power : 1.2 MW cw Insertion Loss : < 0.1 db (VSWR ( : <1.1, power reflection <0.25% ) Isolation : > 26 db (>14 db in ± 10 MHz) Cooling LCW : >26 gpm (150 psig, 25~40 o C, nominal 35 ± 1 o C) Mounting Orientation : any

AFT Circulator

Water Load Specification Coolant : HCW (0.75% Corr-Shield by volume to LCW) Coolant supply : 150 psig, 10~70 o C Coolant return : 15 psig, <80 o C Coolant duct : Teflon tubing Frequency : 476 ±10 MHz Power : <1.2 MW average (<2.0 MW peak for 100 µs) VSWR : <1.05 (reflected power < 0.06%) RF Leakage : < 0.1 mw/cm 2 Length : 9.5 feet overall Air pressure : <0.5 psig (0.25 psig nominal)

Water Load

HCW Station behind Booster

RFHV Power Supply Specification Output DC power : 90 kv* 27A=2.43 MW Corresponds to microperveance of 1.00 and 2.43 * 0.62 = 1.50 MW RF power Input AC power : 12.47 kv line-to to-line, 127 A per phase Power supply efficiency = 2430/(1.73*127*12.47) = 0.89 Lower efficiency at lower output voltage/power New filtering capacitors by General Atomics Light triggered crowbar SCR s Less than 0.5 Joules to the klystron in case of arcing at 80 kv per swinging ball test of crowbar

RFHV Power Supply Schematic

Spear3 RFHV Power Supply

Spear3 RFHV Power Supply Grounding Tank

RFHV PS Swinging Ball Test

Spear3 RF Cavity Characteristics Frequency 476.3 MHz (different from PEP2 476.0 MHz) Shunt Impedance R a = V 2 g /Prf rf = 7.62 MΩ M (95 kw for 0.85 MV) Acceleration field ~ 3.9 MV/m Coupling β = 1+P b /P c = 3.8 (high reflection at lower current) Window power <410 kw, Wall power < 80 W/cm 2 3 high power HOM loads at each of 4 cavities One HOM filter per cavity at the waveguide coupler Similar filters were used at Spear2 One movable tuner per cavity Coupler window temperature is monitored by IR sensor Q ~ 30,000 at operating temperature (Fill time is Q/ω ~10 µs) If RF is turned off on orbit interlock trip, beam is lost in ~300 µs

Spear3 RF Cavity Assembly

Spear3 RF Cavity Assembly

Cavities in the West Straight

Cavities in the West Straight

Spear3 RF System Sam Park 11/06/2003 LCW flow is 6 gallons per minute. No appreciable T is detected, but the flow is interlocked. HOM load at E- and H-mitre HOM load plate, water-cooled Cooling channels were drilled out from a solid copper plate. Matrix of 1.0 inch square ferrite tiles. They are soft- soldered onto a copper plate.

Spear3 RF System Sam Park Movable Tuner below the Cavity 11/06/2003

Movable Tuner Tuning Range 0.8 0.6 0.4 0.2 0-0.2 y = 3.4769E-06x 3 + 3.8603E-04x 2 + 1.9154E-02x - 2.2649E-01 R 2 = 9.9982E-01, y = δfres, x = tuner position Resonance Shift (MHz) -0.4-0.6-30 -20-10 0 10 20 30 Tuner Position (mm)

Waveguide Network & Phasing Magic Tees : Divide RF power evenly. Magic tee loads are to compensate for any mismatch and absorbs reflected power (two arms are 90 degree apart) Bellow lengths are adjusted to match the RF phase in cavities Guided wavelength λ g = λ 0 /[1-(λ 0 /2a) 2 ] 1/2, λ g = c/f Waveguide sections are positively pressurized with dry air to ensure that there is no mechanical gap (no RF leakage) and no moisture enters into the system Window at the klystron is cooled by forced air

Magic-T T and Bellow Network

LLRF in Room 101, Bldg 132

Connections to Klystron

Connections to Klystron

Flow monitor and interlock

Power Balance with Beam Loading 1200 1000 800 600 400 200 Reflect 0 0 100 200 300 400 500 RF Power (kw) Stored Current (ma)

Marconi Klystron Gain Curves 1400 1200 Vb=81kV 1000 75 kv 800 70kV 600 400 65kV 60 kv 200 0 10 20 30 40 50 60 Drive Power (W) Power Out (kw)

Marconi Klystron Gain Curves 1400 1200 1000 800 600 20 W 400 Pdrive=60 W 40 W 200 0 55 60 65 70 75 80 85 Klystron Beam Voltage (kv) Klystron RF Output (kw)

Booster klystron saturation 6 Figure 4 gain breakdown 5 attenuator control voltage -50X klystron drive power -20X klystron forward power 5X cavity cell power 4 3 2 amplitude(v) 1 0-1 0 0.001 0.002 0.003 0.004 0.005 0.006 0.007 0.008 0.009 0.01 time (s) Fig. 2 P(kly) vs. P(drv) at 43.5 kv 75 70 65 60 P-klystrin (dbm) 55 y = -0.0508x 2 + 3.3792x + 17.8341 50 12 14 16 18 20 22 24 26 28 30 32 P-drive (dbm)

Existing Booster RF Soft-Start, Mechanical SCR Assembly with Built-In Soft Start

Timing System SPEAR frequency control loop filter new components phase detect SPEAR RF VCO 476.337 MHz Booster RF VCO p to SPEAR RF q bucket select phase shift h SP bucket delay 358.533 MHz to Booster RF injection energy window sync sync d h B n vernier timing f Brev /n D clk D clk f SPrev ejection energy window f Brev trigger delays modulators S-band amp inject kicker chopper eject kicker SP kickers trigger delays Single-bunch filling Phase-lock Booster RF (358.505 MHz) to SPEAR RF (476.300 MHz) C Boo /C SPEAR = 4 / 7 f Boo /f SPEAR = 70 / 93

1 SPEAR BUNCH PATTERN 0.5 0 Volts 0.5 1 0 0.2 0.4 0.6 0.8 1 1.2 1.4 1.6 1.8 2 Milliseconds Driving I&Q Modulator 0.3 SPEAR BUNCH PATTERN 0.2 0.1 0 0.1 0.2 0.3 0 0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9 1 1.1 Microseconds Test Fill Pattern in Spear2. Volts.

SPEAR 3 Cavity Production Cavity body milling at Accel Electroforming at Accel

SPEAR 3 (PEP-II) RF Cavities

PEP-II RF Cavity Assemblies