Residual Gases in CEBAF Warm Beam Line Sources and Evacuation

Slides:



Advertisements
Similar presentations
Vacuum at CEBAF Seminar for Accelerator Operators 17 January, 2006 Marcy Stutzman and Philip Adderley.
Advertisements

Basics of Vacuum Technology Unit: Pa = N/m 2 = J/m 3 UnitPa or N/m 2 bar10 5 mbar100 atm= 760 torr x 10 5.
High Gradient and High Q R&D Topics 1- Explore Q > for TESLA parameter flexibility –higher luminosity through higher rep rate, longer rf pulse… 2-
Stimulating a discussion on cavity performance metrics.
Vacuum, Surfaces & Coatings Group Technology Department Vacuum tests for CLIC module prototypes 6 November 2013 C. Garion2 Outline: Reminder: specification.
E-CLOUD VACUUM OBSERVATIONS AND FORECAST IN THE LHC Vacuum Surfaces Coatings Group 03/07/2011 G. Bregliozzi On behalf of VSC Group with the contributions.
Vacuum system in the main Linacs C. Garion CERN/TE/VSC CLIC09 workshop, October.
Dark Current Measurements and Simulations Chris Adolphsen 2/4/15.
23 Jan 2007 LASA Cryogenics Global Group 1 ILC Cryomodule piping L. Tavian for the cryogenics global group.
13/09/2005Vacuum Systems for Synchrotron Light Sources Workshop, Barcelona, Spain 1 Gas Flow Modelling in Design of the Vacuum System for of the Synchrotron.
Vacuum tests of the accelerating structure mock-up The main outputs of the tests would be the following: Feasibility of the assembly of the vacuum manifold.
1.3GHz Input Coupler for ILC
Preliminary calculations for the vacuum system of ELENA R. Kersevan TE/VSC-IVM – 21/6/2012 The vacuum sectors, the position of vacuum pumps, flanges, and.
56 MHz SRF Cavity Thermal Analysis and Vacuum Chamber Strength C. Pai
Eric Montesinos - CERN - First SPL collaboration meeting - CERN December 11th 2008 First SPL collaboration meeting Experience with the LHC Main power Coupler.
Thomas Jefferson National Accelerator Facility Operated by the Southeastern Universities Research Association for the U.S. Department of Energy Kirk Davis.
September 17-21, 2007Workshop on ILC Interaction Region Engineering Design, SLAC IR Vacuum Systems first thoughts Oleg Malyshev ASTeC, STFC Daresbury Laboratory.
704 MHz warm cavity November 4, 2015 A.Zaltsman: SRF & warm RF components for LEReC1  A single cell 704 MHz warm cavity is used to correct the beam energy.
2007/09/17-21 SLAC IRENG07 1 A Basic Design of IR Vacuum system Y. Suetsugu, KEK Possibility of a pumping system without in-situ baking at z < L*
Outgassing Test and the Getter Specification
THIN FILMS FOR CLIC ELEMENTS Outline Motivation The role of MME-CCS DB and MB transfer lines Main beam Main beam quadrupoles Other issues conclusions CLIC.
MAIN LINAC CRYOMODULE DESIGN REVIEW INPUT COUPLER September 5, 2012V. Veshcherevich.
Date 2007/Sept./12-14 EDR kick-off-meeting Global Design Effort 1 Cryomodule Interface definition N. Ohuchi.
Estimates of residual gas pressure in the LHC Adriana Rossi AT-VAC Workshop on Experimental Conditions and Beam Induced Detector Backgrounds April.
Power couplers Timergali Khabiboulline (FNAL) FNAL-LBNL meeting on NGLS April 13, 2012.
State of ECR Plasma Test & Measurement of Ferrite Materials Permittivity Summer student meeting August 27, 2007 Ivan Pechenezhskiy, MIPT. Supervisor: Genfa.
Warm Girder UHV Components John Heckman Anthony DiPette Vacuum Group 2/29/2016.
Workshop on cryogenic & vacuum sectorisation of the SPL Vacuum Sectorisation Paul Cruikshank, CERN Technology Department (TE) Vacuum Surfaces & Coatings.
Techniques of Vacuum and Basics of High Voltage (3/3) Pauli Heikkinen Jyväskylä University.
Plasma Cleaning of SRF Cavities Program Status J. Mammosser, S. Ahmed, L. Phillips Jlab S. Popovic, J. Upadhyay, L. Vuskovic, M. Nikolic ODU.
Task 4.3: Mitigate beam-induced vacuum effects (STFC, CERN) O.B. Malyshev and R. Valizadeh, ASTeC Vacuum Science Group, STFC Daresbury Laboratory, UK EuroCirCol.
325 MHz Superconducting Spoke Cavity Coupler status. T. Khabiboulline Power Coupler design for Superconducting Spoke cavities. Originally.
Task 4.3: Mitigate beam-induced vacuum effects (STFC, CERN) O.B. Malyshev and R. Valizadeh, ASTeC Vacuum Science Group, STFC Daresbury Laboratory, UK EuroCirCol.
2007/09/17 SLAC IRENG07 1 Comment on IR Vacuum system Y. Suetsugu Pumping System without in-situ baking at z < L*
NEG pumps Used at CEBAF, FEL electron guns for >15 years Three varieties – Laminated strips: used inserted in CEBAF gun – Sintered disks – Beampipe coating.
Time-Resolved IR and Mass Spectroscopy of Laser-Ablated Magnesium
SRF Operating Experience at JLab
Introduction Six-Month Follow-Up on Action Items of Feb 2016 CEBAF Field Emitter Workshop Rongli Geng September 12, 2016.
Field Emission Minimization for LCLS-II
Degradation and Recovery of Cavity Performance
Vacuum Problems in the ILC Damping Ring
NL C100 Vacuum Spikes and Valve Trips
Cornell ERL Prototype Injector DC Photocathode Gun Design Review Vacuum Systems Yulin Li, January 5th– 6th, /5-6/2011 Cornell Gun Review.
Leak Detection Tutorial Work
Update on HW commissioning
Electron cloud & vacuum pressure observations: 2011 proton run
SNS Operational History
R&D Activity for Field Emission and Vertical EP
Operational Experience - Field Emission
Operating SRF in a "dirty" machine
SNS Fundamental Power Coupler History
Summary, workshop for “Operating SRF reliably in a dirty machine”
V. Veshcherevich Cornell University
Regular cryomodule maintenance plans (radiation damage, seals, etc)
Space Charge Effect Simulation Using DA Based FMM and Electron Cooling Simulation for JLab’s MEIC Project.
Thermal Outgassing Rate for Various Beam Line Materials
Cryomodule (C20, C50, C100) Field Emission Performance to Date
Greg Marble, Rongli Geng
Discussion on the TDI impedance specifications
TTC Hot Topic Common Questions
Cryomodule design modifications for C75
INTC September 2002 ISOLDE Mats Lindroos Mats Lindroos.
Strategy for operation and recovery of performance at SNS -Background -History of performance -What is our operational strategy -Performance recovery.
Performance Recovery at CEBAF
Cryomodule Assembly Plan
Pressure distribution calculations for the PETS
V. Veshcherevich Cornell University
Workshop Aim Rongli Geng February 29, 2016
8-T Solenoid Package and Local Magnetic Shielding in FRIB Cryomodules
Field Emission and Mitigation in the CEBAF Linacs R Legg, R Geng Jlab SRF Ops Dept. TTC,
Presentation transcript:

Residual Gases in CEBAF Warm Beam Line Sources and Evacuation Rongli Geng October 12, 2015 CEBAF Performance Improvement Team Meeting

What is the vacuum level in warm beam line between cryomodules? Questions What is the vacuum level in warm beam line between cryomodules? a. 10-11 Torr b. 10-9 Torr c. 10-6 Torr d. 10-3 Torr

What is the residual gas species in CEBAF beam line vacuum? Questions What is the residual gas species in CEBAF beam line vacuum? a. H2 b. H2O c. CO d. CO2 e. He f. O2

Residual Gas Species – an Example Thanks Anthony Dipette and John Heckman for assistance in accessing the data.

What is the effective pumping speed of the beam line vacuum pumps? Questions What is the effective pumping speed of the beam line vacuum pumps? a. 35 l/s b. 22 l/s c. 2 l/s d. All of the above

35 l/s specification 22 l/s @ 10-9 torr best pumping speed Typically @ 10-6 torr 22 l/s @ 10-9 torr

Case I: Gases Due to Field Emission via ESD This surface intercepts lots FE electrons F. Marhauser et al., SRF2013, TUP095

Thanks Jim Henry for creating and exporting the 3D model of the vacuum space between cavities, needed for pumping speed computation

Case I: Effective Pumping Speed ~ 2 l/s ~ 0.3 l/s

Case I continued: Launch Gas at Varied Locations

twice likely cryosorbed by cold cavity than evacuated by ion pump 100 mm away from step transition (close to slotted beam tube)

Summary Initial data mining reveals that the warm beam line vacuum can be as high as 10-6 torr. Is this typical in the whole machine? Is not this too high? Are the cavities constantly under gas loading? First result on effective pumping speed Beam line ion pumps provide feeble evacuation compared to the strong cryosoption by cold cavities Beam line ion pumps shut off once the cavities are cold? Not much pumping benefit Possible risk of shedding particulate field emitters

Gas Sources Outgassing from ceramic RF window Inevitable RF heating Outgassing from warm beam line surface First/last cavity more vulnerable Desorption stimulated by surface bombardment from field emission electrons Accidental air leaks at warm beamline components Gas release from cold cavity surface by thermal quenching, multipacting

FE Electron Bombardment Sites (Simulation) F. Marhauser et al., SRF2013, TUP095