High Field Q-Slope in Superconducting RF Cavities

Similar documents
Nb 3 Sn Present Status and Potential as an Alternative SRF Material. S. Posen and M. Liepe, Cornell University

COMPARISON OF BUFFERED CHEMICAL POLISHED AND ELECTROPOLISHED 3.9 GHz CAVITIES*

Processing and Testing of PKU 3-1/2 Cell Cavity at JLab

Recent Results of High Gradient Superconducting Cavities at Cornell

Vertical Tests of ILC Cavities and Detection of X-Rays from Field Emission

RECORD QUALITY FACTOR PERFORMANCE OF THE PROTOTYPE CORNELL ERL MAIN LINAC CAVITY IN THE HORIZONTAL TEST CRYOMODULE

INTRODUCTION. METHODS Cavity Preparation and Cryomodule Assembly

EXPLORING THE MAXIMUM SUPERHEATING MAGNETIC FIELDS OF NIOBIUM

CHALLENGES IN ILC SCRF TECHNOLOGY *

Nb 3 Sn Fabrication and Sample Characterization at Cornell

HIGH POWER INPUT COUPLERS FOR THE STF BASELINE CAVITY SYSTEM AT KEK

SRF Cavities A HIGHLY PRIZED TECHNOLOGY FOR ACCELERATORS. An Energetic Kick. Having a Worldwide Impact

CAVITY DIAGNOSTIC SYSTEM FOR THE VERTICAL TEST OF THE BASELINE SC CAVITY IN KEK-STF

Cavity development for TESLA

Cornell ERL s Main Linac Cavities

Frequency Tuning and RF Systems for the ATLAS Energy Upgrade. Gary P. Zinkann

HIGH Q CAVITIES FOR THE CORNELL ERL MAIN LINAC

REVIEW OF NEW SHAPES FOR HIGHER GRADIENTS

Examination of Microphonic Effects in SRF Cavities

TEMPERATURE WAVES IN SRF RESEARCH*

DEVELOPMENTS OF HORIZONTAL HIGH PRESSURE RINSING FOR SUPERKEKB SRF CAVITIES

TEMPERATURE MAPPING SOFTWARE FOR SINGLE-CELL CAVITIES*

LCLS-II SRF Linac Multi-lab partnership to build CW FEL based on SRF at SLAC. Marc Ross 13 January 2014

SRF Advances for ATLAS and Other β<1 Applications

Superconducting 1.3 GHz Cavities for European XFEL

RECENT DEVELOPMENTS IN ELECTROPOLISHING AND TUMBLING R&D AT FERMILAB

Current Industrial SRF Capabilities and Future Plans

To produce more powerful and high-efficiency particle accelerator, efforts have

UPDATE ON THE R&D OF VERTICAL BUFFERED ELECTROPOLISHING ON NIOBIUM SAMPLES AND SRF SINGLE CELL CAVITIES*

Completion of the first SSR1 cavity for PXIE

Liquid Helium Heat Load Within the Cornell Mark II Cryostat

Structures for RIA and FNAL Proton Driver

ASSEMBLY PREPARATIONS FOR THE INTERNATIONAL ERL CRYOMODULE AT DARESBURY LABORATORY

MULTIPACTING IN THE CRAB CAVITY

The Low-Noise, Integrated Transformer Helium-4 Dipstick Insert

LARGE SCALE TESTING OF SRF CAVITIES AND MODULES

SINAP surface preparation processing for superconducting cavities

Review of New Shapes for Higher Gradients

discovery in 1993 [1]. These molecules are interesting due to their superparamagneticlike

3.9 GHz work at Fermilab

NIOBIUM IMPURITY-DOPING STUDIES AT CORNELL AND CM COOL-DOWN DYNAMIC EFFECT ONQ 0

THE MULTIPACTING STUDY OF NIOBIUM SPUTTERED HIGH-BETA QUARTER-WAVE RESONATORS FOR HIE-ISOLDE

Report of working group 5

DEVELOPMENT OF A BETA 0.12, 88 MHZ, QUARTER WAVE RESONATOR AND ITS CRYOMODULE FOR THE SPIRAL2 PROJECT

Tests of the Spoke Cavity RF Source and Cryomodules in Uppsala

A 3 GHz SRF reduced-β Cavity for the S-DALINAC

Summary of the cryogenic rf tests of a seamless Nb-Cu 2-cell cavity

REVIEW OF HIGH POWER CW COUPLERS FOR SC CAVITIES. S. Belomestnykh

Sample Testing with the Quadrupole Resonator A way to obtain RF results over a wide parameter range

SRF Surface Preparation Technique

INFN- LASA MEDIUM BETA CAVITY PROTOTYPES FOR ESS LINAC

TESLA RF POWER COUPLERS DEVELOPMENT AT DESY.

HIGH POWER COUPLER FOR THE TESLA TEST FACILITY

SRF in Storage Rings. Michael Pekeler ACCEL Instruments GmbH Bergisch Gladbach Germany

DC FIELD EMISSION SCANNING MEASUREMENTS ON ELECTROPOLISHED NIOBIUM SAMPLES

Amit Roy Director, IUAC

OVERVIEW OF REGIONAL INFRASTRUCTURES FOR SCRF DEVELOPMENT

Characterization of Common Electron Multipliers in Harsh Environments

Current Industrial SRF Capabilities and Future Plans

Status and Plans for the 805 MHz Box Cavity MuCool RF Workshop III 07/07/09 Al Moretti

NONDISTRUCTIVE TESTING INSTRUMENT OF DISHED Nb SHEETS FOR SRF CAVITIES BASED ON SQUID TECHNOLOGY

Status of the superconducting cavity development at RISP. Gunn Tae Park Accelerator division, RISP May 9th. 2014

High Power Couplers for TTF - FEL

1.3 GHz CAVITY TEST PROGRAM FOR ARIEL

Cavity fabrication and characterization

Latest Developments in Superconducting RF Structures for beta=1 Particle Acceleration

Upper limit of the electron beam energy at the CEBAF 2D injector spectrometer and its functionality

SEVEN-CELL CAVITY OPTIMIZATION FOR CORNELL S ENERGY RECOVERY LINAC

Effects of Temperature Changes on a Vibrating Wire in Superfluid Helium

Mircea Stirbet. RF Conditioning: Systems and Procedures. Jefferson Laboratory

PROGRESS IN IFMIF HALF WAVE RESONATORS MANUFACTURING AND TEST PREPARATION

INSTRUMENTATION AND CONTROL SYSTEM FOR THE INTERNATIONAL ERL CRYOMODULE

Design of a High-Speed, High-Resolution Thermometry System for 1.5-GHz Superconducting Radio-Frequency Cavities

Overview of ERL Projects: SRF Issues and Challenges. Matthias Liepe Cornell University

THE PROTOTYPE FUNDAMENTAL POWER COUPLER FOR THE SPALLATION NEUTRON SOURCE SUPERCONDUCTING CAVITIES: DESIGN AND INITIAL TEST RESULTS*

Commissioning of the ALICE SRF Systems at Daresbury Laboratory Alan Wheelhouse, ASTeC, STFC Daresbury Laboratory ESLS RF 1 st 2 nd October 2008

CURRENT INDUSTRIAL SRF CAPABILITIES AND FUTURE PLANS

Performance of Superconducting Cavities for the European XFEL. Detlef Reschke DESY for the EU-XFEL Accelerator Consortium

Packaging of Cryogenic Components

New apparatus for precise synchronous phase shift measurements in storage rings 1

PIP-II Superconducting RF Linac Status and Challenges" Leonardo Ristori! ICEC-ICMC Conference, New Delhi! 9 March 2016!!

TESTS AND DESIGNS OF HIGH-POWER WAVEGUIDE VACUUM WINDOWS AT CORNELL

THE CRYOGENIC SYSTEM OF TESLA

THE HIGH LUMINOSITY PERFORMANCE OF CESR WITH THE NEW GENERATION SUPERCONDUCTING CAVITY

Schematic diagram of the DAP

5.5 SNS Superconducting Linac

SUPERCONDUCTING PROTOTYPE CAVITIES FOR THE SPALLATION NEUTRON SOURCE (SNS) PROJECT *

RF power tests of LEP2 main couplers on a single cell superconducting cavity

Residual Gas Analyzers XT Series

GA MICROWAVE WINDOW DEVELOPMENT

2. Accelerating Structures for Future Linear Colliders

LOW BETA CAVITY DEVELOPMENT FOR AN ATLAS INTENSITY UPGRADE

Superconducting RF cavity R&D for future accelerators

Snowmass WG5: Superconducting Cavities and Couplers (Draft August 12, 2005 Rong-Li Geng) Topic 1: Cavity Shape

R.Bachimanchi, IPAC, May 2015, Richmond, VA

DEVELOPMENT OF SUPERCONDUCTING RF SAMPLE HOST CAVITIES AND STUDY OF PIT-INDUCED CAVITY QUENCH

QWR Nb sputtering. Anna Maria Porcellato. MoP04. S. Stark, F. Stivanello, V. Palmieri INFN Laboratori Nazionali di Legnaro

Project X Cavity RF and mechanical design. T. Khabiboulline, FNAL/TD/SRF

Superconducting RF for Energy-Recovery Linacs

Mechanical study of the «Saclay piezo tuner» PTS (Piezo Tuning System) P. Bosland, Bo Wu DAPNIA - CEA Saclay. Abstract

Transcription:

High Field Q-Slope in Superconducting RF Cavities Jordan Webster Advisor: Matthias Liepe August 7, 2008

High Field Q-Slope in Superconducting RF Cavities A Tragic Experimental Tale Jordan Webster Advisor: Matthias Liepe August 7, 2008

Background SRF Cavities 1 Used to accelerate bunches through EM waves normal conducting superconducting (1965) constructed from niobium Collection of SRF cavities, taken at Cornell ILC

Single-Cell Cavity Coupler sites 2

3

Yayyyyy! Simple!! 4

Multi-Cell Cavity 5

Yayyyyy! Cheap!!$! 6

Boring Math Stuff & the Q 0 curve 7 V c = d E el dz 0 (voltage seen by a passing electron bunch) E acc = V c d (average accelerating field seen by a passing electron bunch) Q 0 = ω 0 U P C low field Q-slope **high field Q-slope** mid field Q-slope

Quality & Loss Mechanisms 8 Quality vs. Accelerating Field (Example) My Tragic Experiment Detlef Reschke (of DESY), tutorial on Limits in Cavity Performance, 2007 (2)

Cavity Testing finding the Q 0 curve, in 3 easy steps!!! 9 1. Prepare test stand 2. Place test stand into 3. Wire up, cool down, test pit and power up!! Cavity is pumped down below 10-7 torr, given a leak check, and wired up Crane Top plate Transmitted power is measured Cavity Test pit A known amount of RF power is supplied Reflected power is measured

Thermometry 10 Example Temperature Map Another testing technique J. Knobloch, Advanced Thermometry Studies of Superconducting RF Cavities, 1997, 67 Different loss mechanisms cause cavity walls to heat up in unique ways. The cavity wall can be monitored and mapped out using lots and lots and lots of thermometers

Thermometry Exposed 11 Thermometer board 756 Allen Bradley copper resisters are used to obtain temperature map (~1 resister per square cm) T -1 vs. R J. Knobloch, Advanced Thermometry Studies of Superconducting RF Cavities, 1997, 65

Thermometry More Exposed 12 top plate of test stand schematic of thermometry setup J. Knobloch, Advanced Thermometry Studies of Superconducting RF Cavities, 1997, 63 Computer (w/ Labview) cavity (in pit) SCXI multiplexing system

My Goals: Improve our understanding of high field Q-drop 13 Initial Setup: cavity was chemically etched by a BCP, and placed in a class 10 clean room Here s the plan high pressure rinse mount cavity and thermometry system test cavity, look for Q-drop HF rinse (removes oxide on surface) high pressure rinse test, look for Q-drop effects of oxide layer 400 C bake test, look for Q-drop vent cavity with N 2 gas test effects of N 2 impurities more venting

High Pressure Rinse 14

Pumping 15 Mounting & Leak Check

Thermometry System Mounted 16 Progress Check List: high pressure rinse mount cavity and thermometry system test cavity, look for Q-drop HF rinse (removes oxide on surface) high pressure rinse test, look for Q-drop 400 C bake test, look for Q-drop vent cavity with N 2 gas test more venting

Thermometry Trouble! 17 At room temperature, each thermometer should have a resistance of ~120Ω 250 200 Resistance of Thermometers at Room Temperature All thermometers with resistances outside of the threshold from 50Ω-200Ω were reset to 25Ω on this plot Resistance (Ω) 150 100 50 Broken thermometers 0 0 64 128 192 256 320 384 448 512 576 640 704 768 Thermometer #

The Culprits 18 1. Terminal boxes were not plugged in tightly enough to SCXI system (~100 thermometers) 2. Cross-talk caused by broken thermometers with excessively high resistances 3. Some thermometers lacked a thin layer of varnish, shorted to cavity surface 4. Lots of thermometers that were simply broken & needed replacement

3 Weeks Later 19 Progress Check List: high pressure rinse mount cavity and thermometry system test cavity, look for Q-drop HF rinse (removes oxide on surface) high pressure rinse test, look for Q-drop 400 C bake test, look for Q-drop vent cavity with N 2 gas test more venting It s ok though, just test and move on

But then 20 Progress Check List: high pressure rinse Before data can be taken, leaks open in vacuum system!@#! mount cavity and thermometry system test cavity, look for Q-drop HF rinse (removes oxide on surface) high pressure rinse test, look for Q-drop 400 C bake test, look for Q-drop vent cavity with N 2 gas test more venting

So, Leak Checking 21 Residual Gas Analyzer (RGA): detects amount of helium gas being pumped out of cavity Helium gas is sprayed around seals while RGA output is monitored to check for leaks Vacuum pump used for pumping cavity pressure down to 10-7 torr

Fun New Leak Checking Techniques: 22 in-pit leak checking can be used to search for leaks anywhere beneath the top plate of the test stand. bagging nitrogen purging

Several more weeks pass 23 Progress Check List: high pressure rinse mount cavity and thermometry system test cavity, look for Q-drop HF rinse (removes oxide on surface) high pressure rinse test, look for Q-drop 400 C bake test, look for Q-drop vent cavity with N 2 gas test more venting Current Status: Leaks presumably still exist. Test stand will be moved to clean room, cavity will be removed, given a HPR, and then reattached to test stand with fresh indium seals. Some work will have to be done in order to catch up to where we were at the start of the summer But much was learned, so all is not lossed!

The End 24 Thanks to those involved Matthias Liepe Dave Meidlinger SRF group members Rich Galik