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Hiroshi Sakai (KEK)...Report of workshop of Operating SRF Systems reliably in a “Dirty” Machine...

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Report of workshop of Operating SRF Systems reliably in a “Dirty” Machine @ HZB (Berlin) Hiroshi Sakai (KEK) (Purpose of this workshop A workshop to explore the challenges of running SRF systems in an accelerator environment that may not meet the stringent requirements for high voltage SRF operation. The aim of the workshop is to gather together the expert community to compile experience with these operating conditions and develop recipes for the reliable operation of high- voltage SRF . (For ILC) As quick results of this workshop, Cavity performance during beam operation was mainly degradated by field emission which was produced by the small particle contamination. For ILC, How do we keep the high gradient in beam operation ? That is, what clean condition and care are needed ? We learned from this workshop. 23 pages LCWS2017 in Strasbourg, 2017.Oct.24 1
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Page 1: Hiroshi Sakai (KEK)...Report of workshop of Operating SRF Systems reliably in a “Dirty” Machine @ HZB (Berlin) Hiroshi Sakai (KEK) (Purpose of this workshop ) A workshop to explore

Report of workshop ofOperating SRF Systems reliably in a “Dirty” Machine @ HZB (Berlin)

Hiroshi Sakai (KEK)

(Purpose of this workshop )

A workshop to explore the challenges of running SRF systems in an accelerator environment that may not meet the stringent requirements for high voltage SRF operation.

The aim of the workshop is to gather together the expert community to compile experience with these operating conditions and develop recipes for the reliable operation of high-voltage SRF.

(For ILC)

As quick results of this workshop, Cavity performance during beam operation was mainly degradated by field emission which was produced by the small particle contamination. For ILC, How do we keep the high gradient in beam operation ?That is, what clean condition and care are needed ?

We learned from this workshop.

23 pages

LCWS2017 in Strasbourg, 2017.Oct.241

Page 2: Hiroshi Sakai (KEK)...Report of workshop of Operating SRF Systems reliably in a “Dirty” Machine @ HZB (Berlin) Hiroshi Sakai (KEK) (Purpose of this workshop ) A workshop to explore

Program of this workshop

Details about clean works

Introduction of E-XFEL clean work for assembly and vacuum .

Workshop was held on HZB on 14-15th

September organized by J.Knobloch. Participants are 62 peoples, who interested in operation SRF cavities at the existing accelerator (HZB, DESY, HZDR, GSI, ESS, SOLEIL, JLAB, SLAC, CLS, DIAMOND, PLS, IHEP, TPS, IFMIF, KEK, RIKEN) all over the world.

https://indico.helmholtz-berlin.de/conferenceTimeTable.py?confId=10#20170914

DESY

What kinds of problem about SRF operation were faced in the existing acceleratorsand how do we recover the problems.

CEBAF

CEBAF/KEK

2

Page 3: Hiroshi Sakai (KEK)...Report of workshop of Operating SRF Systems reliably in a “Dirty” Machine @ HZB (Berlin) Hiroshi Sakai (KEK) (Purpose of this workshop ) A workshop to explore

(Lesson 1) Learn from long-term beam operation and how to overcome ?

• SRF cavity performances for a long-beam operation are show as follows • CEBAF @JLAB

• KEKB @KEK

• How to overcome the performance degradation of SRF cavity in cryomodules.• Pulse processing

• He processing

• Plasma processing

• Horizontal HPR

3

Page 4: Hiroshi Sakai (KEK)...Report of workshop of Operating SRF Systems reliably in a “Dirty” Machine @ HZB (Berlin) Hiroshi Sakai (KEK) (Purpose of this workshop ) A workshop to explore

CEBAF introduction

Field emission is one of the main issue of gradient limiting and this was come from not only string assembly but also during beam operation

CH

L-2

Upgrade

magnets

and

power

supplies

Upgraded cavityCavity: 0.7 m, “Low loss”

cell shape, 1.497 GHz8 cavities/cryomodule

CEBAF

CEBAF field emission onset(C100 cryomodule)

4

C.Reece

Page 5: Hiroshi Sakai (KEK)...Report of workshop of Operating SRF Systems reliably in a “Dirty” Machine @ HZB (Berlin) Hiroshi Sakai (KEK) (Purpose of this workshop ) A workshop to explore

Example of dirty cavity inside during long operation and Degradation made radiation damage

Cleaning essential not only cavity but also beam line.

Damaged by radiation produced by F.E

Particle sampling inside the cavity and vacuum chamberIn one cryomodule in CEBAF (FRANKLIN)

Many particles come from assembly work and ceramic ?

5

C.Reece

Page 6: Hiroshi Sakai (KEK)...Report of workshop of Operating SRF Systems reliably in a “Dirty” Machine @ HZB (Berlin) Hiroshi Sakai (KEK) (Purpose of this workshop ) A workshop to explore

He processing

Increase by He processing

Procedure : Add He to 2KProcess by RF under He pressure around 0.05-0.1 mTorrFor about 1 hour.Warm up again to 40 K.

See the radiation onset before and after He processing.

total

1MV gain per cavity with 100 cavities by He processing. One solution is to recover the cavity performance !But this mainly effectively work for lower cavity and sometimes degrade the cavity during processing .

One example

6

C.Reece

Page 7: Hiroshi Sakai (KEK)...Report of workshop of Operating SRF Systems reliably in a “Dirty” Machine @ HZB (Berlin) Hiroshi Sakai (KEK) (Purpose of this workshop ) A workshop to explore

Reference of CEBAF (see ref. in detail)

7

Page 8: Hiroshi Sakai (KEK)...Report of workshop of Operating SRF Systems reliably in a “Dirty” Machine @ HZB (Berlin) Hiroshi Sakai (KEK) (Purpose of this workshop ) A workshop to explore

509 MHz 8 Nb Single-cell Cavities, 4.4 K Operation

RF-Voltage : 1.5MV/cav, unloaded-Q > 1e9@2MV

Re-use of existing SRF system in SuperKEKB

Issues in SuperKEKB for SCCLarge HOM power is expected due to twice highbeam current and shorter bunch length.Degradation of RF performance of Qo for many years.

Degradation might be due to particle contamination during

*repair of vacuum leak.*replacement of coupler gaskets to change Qext.

Experience of KEKB and recovery to Super KEKB Michiru Nishiwaki (KEK)

SC-Cavity(HER)

HER(e-): 7 GeV, 2.6ALER(e+) : 4 GeV, 1.6A

NC-cavity(LER)

Super KEKB Highest luminosity machineUnder commissioning from 2016

Q0 at 1.5 MV > 1e+09 => Acceptable for SupeKEKBFurther degradation make the operation difficult. Need to recover the cavity performance8

Page 9: Hiroshi Sakai (KEK)...Report of workshop of Operating SRF Systems reliably in a “Dirty” Machine @ HZB (Berlin) Hiroshi Sakai (KEK) (Purpose of this workshop ) A workshop to explore

Both cavity performances were successfully recovered in Super-KEKBIt suggests, the causes of FE are not only gas absorption but also dust particles on the surface.This HHPR worked well because we could remove all particles inside the cavity. It is also effective wayto recovery performance in principle. But is it applicable to ILC cavity (9-cell, long string assembly) ?

Horizontal HPR applied to Degraded Cavity

9

Rotating Water Jets

• New horizontal HPR with ultrapure water system was developed.

• Input coupler and both end groups, including ferrite HOM damper,taper chamber, bellows chamber, ion pump, vacuum gauges andGV, are removed before HHPR in a clean booth.

• Water in the cell is pumped up by aspiration system during rinsing.

• Only cell and iris area are rinsed.

108

109

1010

0 0.5 1 1.5 2 2.5Vc [MV]

108

109

1010

0 0.5 1 1.5 2 2.5Vc [MV]

CA-B03 CA-B04

BeforeLeak

Degradedat Repairing work

after HHPR

Degradedby Vacuum Trouble

after HHPRafter Aging in Tunnel Results of HHPR

Page 10: Hiroshi Sakai (KEK)...Report of workshop of Operating SRF Systems reliably in a “Dirty” Machine @ HZB (Berlin) Hiroshi Sakai (KEK) (Purpose of this workshop ) A workshop to explore

(Lesson 2) Controlling Particulates and Dust in Vacuum Systems

Lutz LiljeDESY, 14.9.2017

(Lesson 2) Learn from the experience of EURO-XFEL construction (Lutz@DESY)

10

Page 11: Hiroshi Sakai (KEK)...Report of workshop of Operating SRF Systems reliably in a “Dirty” Machine @ HZB (Berlin) Hiroshi Sakai (KEK) (Purpose of this workshop ) A workshop to explore

Before we start: Introduction and definition of the Problem

• Dust is composed of particulates. • A particle accelerator accelerates particles: electrons, protons, ions

• Particulates make field emission even though this was very small (~ 0.1 um).

• When people aim for „particle-free“ vacuum systems, they mean a vacuum system with the lowest possible count of particulates• A truly particulate-free accelerator is difficult – if not impossible –

to achieve.• Need to much reduce introducing the particulates to the cavity

during assembly work, especially vacuum work.

• From previous slides of long-term operation, dusts might come from outside of the dirty components during beam operation. • Keep clean not only inside the cavity but also other components

near the cavity.• It is desirable to clean all vacuum components, especially for ILC

accelerators.

Some information is available in the recent 2017 CERN Accelerator School on vacuum

Lutz

11

Page 12: Hiroshi Sakai (KEK)...Report of workshop of Operating SRF Systems reliably in a “Dirty” Machine @ HZB (Berlin) Hiroshi Sakai (KEK) (Purpose of this workshop ) A workshop to explore

Mass of Particulates

• They have mass• 6,2 mg per m2 per day …

• In vacuum they fall down• A particle needs a few ten

milliseconds to traverse a typical beam pipe (if only accelerated by gravity)

• BUT: They have only a small mass

• They will be transported in gaseous media at pressures above 1 mbar.• Opening an angle valve at

10 mbar while pumping a system

By Original uploader was Sullivan.t.j at English Wikipedia. - The description as originally from Wikipedia., CC BY-SA 3.0, https://commons.wikimedia.org/w/index.php?curid=2249027

12

Lutz

Page 13: Hiroshi Sakai (KEK)...Report of workshop of Operating SRF Systems reliably in a “Dirty” Machine @ HZB (Berlin) Hiroshi Sakai (KEK) (Purpose of this workshop ) A workshop to explore

Avoiding Particulate Transport during Pumpdown and Vent

• Particle transport will be avoided by careful operation of the vacuum system

• Avoiding vibrations is mandatory in general• When there is no vacuum, this is

even more important

• Use laminar gas flow while venting and pumping vacuum systems• Avoid turbulences• Even with laminar gas flow

mechanical vibrations can lead to long distance particle transport

K. Zapfe, J. Wojtkiewicz

SRF2007, WEP74

Slow vent

13

Lutz

Page 14: Hiroshi Sakai (KEK)...Report of workshop of Operating SRF Systems reliably in a “Dirty” Machine @ HZB (Berlin) Hiroshi Sakai (KEK) (Purpose of this workshop ) A workshop to explore

Venting and Pump Down of “Particle Free” Sections

• There are and always will be particles in the vacuum system!

• Developments of slow pumping / venting procedures by means on in-vacuum particle counter. No particles are transported if either:

• Flow ≤ 3 ln/min, or

• Pressure < 1 mbar

• Automatic pumping / venting units developed

• Constant flow of 3 ln/min of nitrogen or argon, by means of mass flow controllers.

• Units have been widely used for XFEL.

This is important not to move the particle under pumping and venting during all cavity & vacuum works14

Lutz

Page 15: Hiroshi Sakai (KEK)...Report of workshop of Operating SRF Systems reliably in a “Dirty” Machine @ HZB (Berlin) Hiroshi Sakai (KEK) (Purpose of this workshop ) A workshop to explore

Example XFEL: Overview of “Particle-Free” sections

CL Collimation T1, T3, U1, T5, U2, T5D

Electron transfer lines of the southern branch up the XSDU1 dump

TL, TLD Switch-Yard, electron transfer line to XS1 dump

S2 SASE section of the southern branch

T2,T4, T4D Electron transfer lines of the northern branch up the XSDU2 dump

T6, T7, T8 Photon transfer lines of the southern branch *

S1, S3 SASE sections of the northern branch

T9, T10 Photon transfer lines of the northern branch *

I1, I1D Injector, Injector dump

BC0, BC1, BC2 Bunch compressor 0, 1, and 2

BC1D, BC2D Bunch compressor 1 and 2 dumps

L1, L2, L3 Superconducting linacs (4, 12, and 80 accelerator modules)

And the X-ray optics areas, too.

(not covered here)

Around 1.5 km need to be set “particle-free” section from injector to main-linac (cryomodule section)At least ISO 5 level cleaness are needed on these area. How to make in acclelerator tunnel ?

15

Lutz

Page 16: Hiroshi Sakai (KEK)...Report of workshop of Operating SRF Systems reliably in a “Dirty” Machine @ HZB (Berlin) Hiroshi Sakai (KEK) (Purpose of this workshop ) A workshop to explore

Particle Cleanliness: Segmentation• Segmentation is important

• Pumpdown time needs to be acceptable• Efficient leak searches• Cleaning of subsections in an optimised environment i.e. normal clean room• Steel flanges , plastic caps

• Reduction of types and number of flange connections to be made in the tunnel• Better reproducibility • Time saving

Reduce open parts and time in accelerator tunnel.16

Lutz

Page 17: Hiroshi Sakai (KEK)...Report of workshop of Operating SRF Systems reliably in a “Dirty” Machine @ HZB (Berlin) Hiroshi Sakai (KEK) (Purpose of this workshop ) A workshop to explore

Particle Cleanliness: Segmentation of Accelerator Modules

Dust stick to the surface: (by Van der Vaals) Cleaned by Ionized nitrogen blowing.

Make local clean booseWith laminer flow

Before opening the flanges, particulates must be blowedto keep 0 particle by particle counters.

17

Lutz

Page 18: Hiroshi Sakai (KEK)...Report of workshop of Operating SRF Systems reliably in a “Dirty” Machine @ HZB (Berlin) Hiroshi Sakai (KEK) (Purpose of this workshop ) A workshop to explore

Mobile Clean Rooms: Example XFEL HOM-Absorber

• Air flow from below

• Access from both sides

• Handling system for the component (No need access by human, who produce particulates.)

> Stairs can be removed fortransports

18

Lutz

Page 19: Hiroshi Sakai (KEK)...Report of workshop of Operating SRF Systems reliably in a “Dirty” Machine @ HZB (Berlin) Hiroshi Sakai (KEK) (Purpose of this workshop ) A workshop to explore

Mobile Clean Rooms: Injector Version

• Filter system attached to blower unit and can be tilted

• Access with two people possible

Injector is a complex area. It is difficult to smart clean boose19

Lutz

Page 20: Hiroshi Sakai (KEK)...Report of workshop of Operating SRF Systems reliably in a “Dirty” Machine @ HZB (Berlin) Hiroshi Sakai (KEK) (Purpose of this workshop ) A workshop to explore

XFEL „Particle-free“ Highlights in Numbers (include)

• 1 RF Gun including cathode handling system• Very delicate components, very little space, very demanding requirements

• 38 girders with 5 m each• More than 500 different pieces • Tubes, pumps, compensators, diagnostics incl. transverse deflecting structure,

• Laser heater chicane

• 3 Bunch Compressor Chicanes• Long chambers• Large flanges

• 6 pressure stages at warm cold transition

• 3 dump lines

• 60 m warm beam line at the end of the cold linac as a buffer zone

• For the 100 accelerator modules• 200 all metal date valves• 800 cavity and 800 coupler bellows• 200 coupler pump lines with TSP, sputter ion pump• 100 HOM Absorbers• Plus testing, installation etc.

• More than 1,5 km of vacuum chambers have been cleaned (without the cavities)

20

Lutz

Page 21: Hiroshi Sakai (KEK)...Report of workshop of Operating SRF Systems reliably in a “Dirty” Machine @ HZB (Berlin) Hiroshi Sakai (KEK) (Purpose of this workshop ) A workshop to explore

XFEL Module Gradient Performance

Module performance well

above XFEL specs.

and visible

improvement with time

Tunnel installation used

sorting of modules

based on AMTF

performance

vertical test (clipped at 31 MV/m)module performance

Remarks:Clipping at 31 MV/m is done due to max. available RF power; limit given by waveguide distribution.XM98 is a scavenger module.

Ncavs Average RMS

VT 815 28.3 MV/m 3.5

CM 815 27.5 MV/m 4.8

XFEL Spec23.6 MV/m

see talk by D. Kostin “European-XFEL summary: Cavities/Modules performance” in SRF session, Tue 24th AM

15

We have ~10 % degradation from VT to CM. But we could keep the cavity requirements of E-XFEL of 23.6 MV/m. Elaborate clean assembly works for E-XFEL at string-assembly kept the cavity performance.

By Nick Walker(Presented by Denis Kostin)on this workshop.

Page 22: Hiroshi Sakai (KEK)...Report of workshop of Operating SRF Systems reliably in a “Dirty” Machine @ HZB (Berlin) Hiroshi Sakai (KEK) (Purpose of this workshop ) A workshop to explore

Now . First Lasing at European XFEL – 2nd of May 2017

6.3 GeV electron beam energy500 pC buch charge, 1 Hz, single bunch→ 0.8 nm SASE wave length

SASE intensity vs. compression(lower Pyro signal = higher compression)

SASE image on OTR station

No beam

Compression OFF

Compression ON

Now:

14 GeV, 30 Bunches,

1.3 Angström, 9.3 keV, upto 1mJ

22We did not see the significant degradation in E-XFEL. need to continue measuring SRF performance

Lutz

Page 23: Hiroshi Sakai (KEK)...Report of workshop of Operating SRF Systems reliably in a “Dirty” Machine @ HZB (Berlin) Hiroshi Sakai (KEK) (Purpose of this workshop ) A workshop to explore

Summary from E-XFEL experience about clean work

• Remember the basic rules as follows• Avoid particulates at every stage and include it in the mechanical design• Remove particulates at every stage possible• Do not produce particulates especially during installation and operation• Never transport particulates

• Layout and mechanical design need to take into account cleaning and installation

• Transport of particulates must be avoided• Methods to avoid turbulent flows during pump-down and venting are available

• Large-scale infrastructures can be built “particle-free”• A large part of the European XFEL accelerator vacuum system is „particle-free“• … and it works!

• ILC needs higher gradient of more than 10 times larger SRF scale than E-XFEL. These clean work of E-XFEL must be learned more and brushed up.

23

For ILC up to now, keep clean clean clean clean as much as possible.

Lutz

Page 24: Hiroshi Sakai (KEK)...Report of workshop of Operating SRF Systems reliably in a “Dirty” Machine @ HZB (Berlin) Hiroshi Sakai (KEK) (Purpose of this workshop ) A workshop to explore

Thank you

Participants of the workshop 24

Page 25: Hiroshi Sakai (KEK)...Report of workshop of Operating SRF Systems reliably in a “Dirty” Machine @ HZB (Berlin) Hiroshi Sakai (KEK) (Purpose of this workshop ) A workshop to explore

backup

25

Page 26: Hiroshi Sakai (KEK)...Report of workshop of Operating SRF Systems reliably in a “Dirty” Machine @ HZB (Berlin) Hiroshi Sakai (KEK) (Purpose of this workshop ) A workshop to explore

Particulate-related Degradations:LHC Beam Losses• 2010 and 2011 beam losses

leading to 35 protection beam dumps were observed

• With improved diagnostics information of about 7800 suspicious events detected

• UFOs !• Unidentified Falling Objects

• 6% of these events could be attributed to the injection kickers which are only 0,06% of the LHC length

• Other kickers were not showing is anomaly

• Clear correlation to kickers being pulsed

TRANSIENT BEAM LOSSES IN THE LHC INJECTION KICKERS FROM MICRON

SCALE DUST PARTICLES

B. Goddard et al., IPAC2012, TUPPR092

26

Page 27: Hiroshi Sakai (KEK)...Report of workshop of Operating SRF Systems reliably in a “Dirty” Machine @ HZB (Berlin) Hiroshi Sakai (KEK) (Purpose of this workshop ) A workshop to explore

Particulate-related Degradations:LHC Injection Kicker

• Added beam loss monitors confirm location

• Kicker vibrates when pulsed

• Aluminum oxide particles were found in abundance after one item removed from the accelerator• Other kickers have metallic coating

27

Page 28: Hiroshi Sakai (KEK)...Report of workshop of Operating SRF Systems reliably in a “Dirty” Machine @ HZB (Berlin) Hiroshi Sakai (KEK) (Purpose of this workshop ) A workshop to explore

Vacuum systems of the XFEL acceleratorWarm beam line vacuum

Material properties alignment RF shielding Vacuum (**)

conductivity rel. magneticpermeabilityμr

R + 50*O max. step at flanges

max. longitudinalgap

Flanges, bellows, pumps, valves

Particlefree

Average pressure

mWcm nm mm mm mbar

RF-gun (up to L0) 75 <1.01 --- --- --- --- ISO 5 < 10-10

I1, BC0, BC1-, BC2-chicane

3 1.01 1250 0.2 0.5 YES ISO 5 < 2 10-8 *

I1, BC1, BC2 dump 3 1.05 2000 0.2 0.5 NO ISO 5 < 2 10-8

BC1,2 3 1.05 1250 0.2 0.5 YES ISO 5 < 2 10-8 *

CL, TL, T1, T2, T3. T4, T4D, T5, T5D, U1, U2

3 1.05 1250 0.2 0.5 YES NO < 2 10-8 *

S1, S2, S3 3 1.01 550 0.1 0.5 YES NO < 2 10-7

Right in front of main dumps

3 1.05 2000 0.2 0.5 NO NO < 2 10-8

(*) close to SRF modules 10-10 mbar(**) In addition all components have to be in accordance to the DESY vacuum specification

Requirements from beam dynamicsExcept μr and RF-shielding absolutely new

requirements on an accelerator vacuum system

28

Page 29: Hiroshi Sakai (KEK)...Report of workshop of Operating SRF Systems reliably in a “Dirty” Machine @ HZB (Berlin) Hiroshi Sakai (KEK) (Purpose of this workshop ) A workshop to explore

E-XFEL Cavities : from VT to (current) operation

Single Cavity Vertical Test (VT)Single cavity CW

<E> ~ 30 MV/m<E> ~ 28 MV/m clipped at 31 MV/m

Cryomodule Test (CM)Single Cavity (pulsed)

<E> ~ 27 MV/m

Current XFEL operation (approximate)

<E> ~ 22 MV/m

Work in progress – expect to do better

ILC 35 MV/m ILC 31.5 MV/m ILC 31.5 MV/m

24

31.5MV/m is limited by RF power source in CM test

By Nick Walker(Presented by Denis Kostin)on this workshop.


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