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Page 1: SRF Cavity Preparation and Limitations - CERN · – Process of connecting subcomponents to cavity openings – Slow and careful steps, high level of attention to detail – Ionized

1 Managed by UT-Battellefor the U.S. Department of Energy Presentation_name

SRF Cavity Preparation and Limitations

J. Mammosser (ORNL)

Page 2: SRF Cavity Preparation and Limitations - CERN · – Process of connecting subcomponents to cavity openings – Slow and careful steps, high level of attention to detail – Ionized

2 Managed by UT-Battellefor the U.S. Department of Energy Presentation_name

Outline:• Cavity Qualifying Test Limitations (Vertical Test)

– Vertical Test Results– Main Limitations (Field emission, Thermal breakdown,

Multipacting)– Not Covered - (Q-disease, Trapped Magnetic Field, High Field Q-

Drop)– Performance History

• Today's Standard Processing Procedures– Standard Processing Sequence (30-40 MV/m)– Surface cleaning, Chemistry, HPR, Heat treatment, Baking, Helium

Processing• Future Process Improvements

– Vertical EP, Plasma Cleaning, Integrated Process Automation

Page 3: SRF Cavity Preparation and Limitations - CERN · – Process of connecting subcomponents to cavity openings – Slow and careful steps, high level of attention to detail – Ionized

3 Managed by UT-Battellefor the U.S. Department of Energy Presentation_name

When Proper Procedure and Attention to Detail Occur –

Rongli Geng 3

• 4 out of 5 reached > 35 MV/m after 1st light EP• A15 quench limited by one defect in one cell

• A15 quench source identified by T-mapping and optical inspection• A12 data after 1st light EP is not shown• A12 data shown are after 2nd light EP

Crawford et al

Page 4: SRF Cavity Preparation and Limitations - CERN · – Process of connecting subcomponents to cavity openings – Slow and careful steps, high level of attention to detail – Ionized

4 Managed by UT-Battellefor the U.S. Department of Energy Presentation_name

However performances are not always ideal

11

10

9

80 25 50 MV/m

Accelerating Field

Residual losses

Multipacting

Field emission

Thermal breakdown

Quench

Ideal

RF Processing

10

10

10

10

Q

Page 5: SRF Cavity Preparation and Limitations - CERN · – Process of connecting subcomponents to cavity openings – Slow and careful steps, high level of attention to detail – Ionized

5 Managed by UT-Battellefor the U.S. Department of Energy Presentation_name

Field Emission

Characterized by an exponential drop of the Q-value

Associated with production of x-rays and emission of dark current

Today good processes and procedures can minimize or eliminate this issue but its always there at some level

Page 6: SRF Cavity Preparation and Limitations - CERN · – Process of connecting subcomponents to cavity openings – Slow and careful steps, high level of attention to detail – Ionized

6 Managed by UT-Battellefor the U.S. Department of Energy Presentation_name

Field Emission

1,E+09

1,E+10

1,E+11

0 2 4 6 8 10 12 14 16 18 20

Qo

E (MV/m)

SNS HB54 Qo versus EaccMultipacting limited at 16MV/m 5/16/08 cg

Page 7: SRF Cavity Preparation and Limitations - CERN · – Process of connecting subcomponents to cavity openings – Slow and careful steps, high level of attention to detail – Ionized

7 Managed by UT-Battellefor the U.S. Department of Energy Presentation_name

Field Emission

0

0

0

0

1

10

100

1000

0 5 10 15 20 25

mR

em/h

r)

E (MV/m)

SNS HTB 54 Radiation at top plate versus Eacc 5/16/08 cg

Page 8: SRF Cavity Preparation and Limitations - CERN · – Process of connecting subcomponents to cavity openings – Slow and careful steps, high level of attention to detail – Ionized

8 Managed by UT-Battellefor the U.S. Department of Energy Presentation_name

Field Emission from Ideal SurfaceFowler-Nordheim model

( )

⎥⎥⎥

⎢⎢⎢

⎡×

−×

=E

EAeEIFN

FN

βφ

φβ 2

3326 1083.6exp1054.1)(

FactortEnhancemenFieldFieldElectricE

AreaSurfaceEmitterEffectiveAfunctionwork

FN

e

==

==

β

φ

Page 9: SRF Cavity Preparation and Limitations - CERN · – Process of connecting subcomponents to cavity openings – Slow and careful steps, high level of attention to detail – Ionized

9 Managed by UT-Battellefor the U.S. Department of Energy Presentation_name

Geometrical Origin of Field Enhancement

Smooth particles show little field emission

Simple protrusions are not sufficient to explain the measured enhancement factors

Possible explanation: tip on tip (compounded enhancement)

Page 10: SRF Cavity Preparation and Limitations - CERN · – Process of connecting subcomponents to cavity openings – Slow and careful steps, high level of attention to detail – Ionized

10 Managed by UT-Battellefor the U.S. Department of Energy Presentation_name

Localized Defects

mμ20≈

mμ20≈

Page 11: SRF Cavity Preparation and Limitations - CERN · – Process of connecting subcomponents to cavity openings – Slow and careful steps, high level of attention to detail – Ionized

11 Managed by UT-Battellefor the U.S. Department of Energy Presentation_name

Field Emission

mμ1015×≈

Page 12: SRF Cavity Preparation and Limitations - CERN · – Process of connecting subcomponents to cavity openings – Slow and careful steps, high level of attention to detail – Ionized

12 Managed by UT-Battellefor the U.S. Department of Energy Presentation_name

Example of Field Emittors

V

Ni Ni

Page 13: SRF Cavity Preparation and Limitations - CERN · – Process of connecting subcomponents to cavity openings – Slow and careful steps, high level of attention to detail – Ionized

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C, O, Na, In Al, Si

Stainless steel

Melted

Melted

Melted

Example of Field Emitters

Page 14: SRF Cavity Preparation and Limitations - CERN · – Process of connecting subcomponents to cavity openings – Slow and careful steps, high level of attention to detail – Ionized

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Looking Inside the Cavity During Testing

• Before onset of Radiation outside dewar

• Radiation present on detector and in CCD image

Page 15: SRF Cavity Preparation and Limitations - CERN · – Process of connecting subcomponents to cavity openings – Slow and careful steps, high level of attention to detail – Ionized

15 Managed by UT-Battellefor the U.S. Department of Energy Presentation_name

Enhancement by Absorbates

Adsorbed atoms on the surface can enhance the tunneling of electrons from the metal and increase field emission

Beta Enhancement Factors1 - tip on tip2 - absorbed gas3 – insulator enhancement (field distortion)

Page 16: SRF Cavity Preparation and Limitations - CERN · – Process of connecting subcomponents to cavity openings – Slow and careful steps, high level of attention to detail – Ionized

16 Managed by UT-Battellefor the U.S. Department of Energy Presentation_name

Qo vs. Eacc Radiation vs. Eacc

If this cavity is limited at this condition, what is the limiting factor?Field emission?

MP

FE

Field Emission ?MP! And then later on Field Emission !VTA

Page 17: SRF Cavity Preparation and Limitations - CERN · – Process of connecting subcomponents to cavity openings – Slow and careful steps, high level of attention to detail – Ionized

17 Managed by UT-Battellefor the U.S. Department of Energy Presentation_name

17b in open loop

Radiation Increase(in log scale)

Eacc

CCG5

10

15

20Eacc=16.5

Time (us) Time (us)

[MV/m]Eacc=17.5

Pulsed operationWaveform tells us

what is happening inside

17bRadiation at Eacc=16.5 (Elim=17.5 MV/m due to FE!)

Radiation waveform

Field emissionEx. 17b individual

Page 18: SRF Cavity Preparation and Limitations - CERN · – Process of connecting subcomponents to cavity openings – Slow and careful steps, high level of attention to detail – Ionized

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Thermal Breakdown

1 4log(ΔT [mK])

Localized heating

Hot area increases with field

At a certain field there is a thermal runaway, the field collapses

sometimes displays a oscillator behavior

sometimes settles at a lower value

sometimes displays a hysteretic behavior

Page 19: SRF Cavity Preparation and Limitations - CERN · – Process of connecting subcomponents to cavity openings – Slow and careful steps, high level of attention to detail – Ionized

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Thermal Breakdown

Thermal breakdown occurs when the heat generated at the hot spot is larger than that can be evacuated to the helium bath

Both the thermal conductivity and the surface resistance of Nb are highly temperature dependent between 2 and 9K

Page 20: SRF Cavity Preparation and Limitations - CERN · – Process of connecting subcomponents to cavity openings – Slow and careful steps, high level of attention to detail – Ionized

20 Managed by UT-Battellefor the U.S. Department of Energy Presentation_name

Thermal Breakdown

Page 21: SRF Cavity Preparation and Limitations - CERN · – Process of connecting subcomponents to cavity openings – Slow and careful steps, high level of attention to detail – Ionized

21 Managed by UT-Battellefor the U.S. Department of Energy Presentation_name

Pd

T

T

T

Ts-Tb

q

T

Rs

Page 22: SRF Cavity Preparation and Limitations - CERN · – Process of connecting subcomponents to cavity openings – Slow and careful steps, high level of attention to detail – Ionized

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Surface Resistance vs Temperature

Page 23: SRF Cavity Preparation and Limitations - CERN · – Process of connecting subcomponents to cavity openings – Slow and careful steps, high level of attention to detail – Ionized

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Power Dissipation vs Temperature

Page 24: SRF Cavity Preparation and Limitations - CERN · – Process of connecting subcomponents to cavity openings – Slow and careful steps, high level of attention to detail – Ionized

24 Managed by UT-Battellefor the U.S. Department of Energy Presentation_name

Niobium Specific Heat vs Temperature

Page 25: SRF Cavity Preparation and Limitations - CERN · – Process of connecting subcomponents to cavity openings – Slow and careful steps, high level of attention to detail – Ionized

25 Managed by UT-Battellefor the U.S. Department of Energy Presentation_name

Heat Transfer Density (Bath-Niobium)

• Tb –Helium Bath• Ts – Niobium

Surface Helium side

• q- heat density

Page 26: SRF Cavity Preparation and Limitations - CERN · – Process of connecting subcomponents to cavity openings – Slow and careful steps, high level of attention to detail – Ionized

26 Managed by UT-Battellefor the U.S. Department of Energy Presentation_name

Niobium Thermal Conductivity vs Temperature

Page 27: SRF Cavity Preparation and Limitations - CERN · – Process of connecting subcomponents to cavity openings – Slow and careful steps, high level of attention to detail – Ionized

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Thermal Breakdown

Page 28: SRF Cavity Preparation and Limitations - CERN · – Process of connecting subcomponents to cavity openings – Slow and careful steps, high level of attention to detail – Ionized

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Thermal Conductivity of Nb

Page 29: SRF Cavity Preparation and Limitations - CERN · – Process of connecting subcomponents to cavity openings – Slow and careful steps, high level of attention to detail – Ionized

29 Managed by UT-Battellefor the U.S. Department of Energy Presentation_name

Residual Resistance Ratio

RRR is the ratio of the resistivity at 300K and 4.2K

(300 )(4.2 )

KRRRK

rr

=

RRR is related to the mean free path.

For Nb: ( 4.2 ) 27 (Å)l T K RRR= »

RRR is related to the thermal conductivity

For Nb: ( 4.2 ) / 4 ( )-1 -1W. m . KT K RRRl = »

At normal conducting and cryogenic state

Page 30: SRF Cavity Preparation and Limitations - CERN · – Process of connecting subcomponents to cavity openings – Slow and careful steps, high level of attention to detail – Ionized

30 Managed by UT-Battellefor the U.S. Department of Energy Presentation_name

Thermal Breakdown

Breakdown field given by(very approximately):

4 ( )T c btb

d d

T THr R

k -=

κT: Thermal conductivity of NbRd: Defect surface resistanceTc: Critical temperature of NbTb: Bath temperature

Page 31: SRF Cavity Preparation and Limitations - CERN · – Process of connecting subcomponents to cavity openings – Slow and careful steps, high level of attention to detail – Ionized

31 Managed by UT-Battellefor the U.S. Department of Energy Presentation_name

Kim ORNL

Quenching pattern examples in the end group

during pulse

during gape-loadings around HOM antenna

e-loading at OC

Low RRR & long path to the thermal sinkThermal margin is relatively small,Intermediate stage at the end-group Results in thermal quench/gas burst

Page 32: SRF Cavity Preparation and Limitations - CERN · – Process of connecting subcomponents to cavity openings – Slow and careful steps, high level of attention to detail – Ionized

32 Managed by UT-Battellefor the U.S. Department of Energy Presentation_name

Thermal Breakdown

Page 33: SRF Cavity Preparation and Limitations - CERN · – Process of connecting subcomponents to cavity openings – Slow and careful steps, high level of attention to detail – Ionized

33 Managed by UT-Battellefor the U.S. Department of Energy Presentation_name

Rongli Geng

33

700 μm dia. defect in AES5

300 μm dia. defect in A15

JLab T-mapping and High-Resolution Optical Inspection

hot spot near equator EBW

Precursor T-jumpat quench location

Ciovati et al

Page 34: SRF Cavity Preparation and Limitations - CERN · – Process of connecting subcomponents to cavity openings – Slow and careful steps, high level of attention to detail – Ionized

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Multipacting

Page 35: SRF Cavity Preparation and Limitations - CERN · – Process of connecting subcomponents to cavity openings – Slow and careful steps, high level of attention to detail – Ionized

35 Managed by UT-Battellefor the U.S. Department of Energy Presentation_name

Multipacting

1,E+09

1,E+10

1,E+11

0 2 4 6 8 10 12 14 16 18 20

Qo

E (MV/m)

SNS HB54 Qo versus EaccMultipacting limited at 16MV/m 5/16/08 cg

Page 36: SRF Cavity Preparation and Limitations - CERN · – Process of connecting subcomponents to cavity openings – Slow and careful steps, high level of attention to detail – Ionized

36 Managed by UT-Battellefor the U.S. Department of Energy Presentation_name

Multipacting

Multipacting is characterized by an exponential growth in the number of electrons in a cavity

Multipacting requires 2 conditions:

Electron motion is periodic (resonance condition)

Impact energy is such that secondary emission coefficient is >1

Page 37: SRF Cavity Preparation and Limitations - CERN · – Process of connecting subcomponents to cavity openings – Slow and careful steps, high level of attention to detail – Ionized

37 Managed by UT-Battellefor the U.S. Department of Energy Presentation_name

Multipacting

Page 38: SRF Cavity Preparation and Limitations - CERN · – Process of connecting subcomponents to cavity openings – Slow and careful steps, high level of attention to detail – Ionized

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Secondary Emission in Niobium

Page 39: SRF Cavity Preparation and Limitations - CERN · – Process of connecting subcomponents to cavity openings – Slow and careful steps, high level of attention to detail – Ionized

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Page 40: SRF Cavity Preparation and Limitations - CERN · – Process of connecting subcomponents to cavity openings – Slow and careful steps, high level of attention to detail – Ionized

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More Then Just Cell Mulitpacting4 MP Locations in the SNS Cavity Observed:

Cell Equator

Input coupler

Beam pipe Transitions

HOM Hooks

Page 41: SRF Cavity Preparation and Limitations - CERN · – Process of connecting subcomponents to cavity openings – Slow and careful steps, high level of attention to detail – Ionized

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Separating MP and Field Emission Contributions to X-rays Observed

Page 42: SRF Cavity Preparation and Limitations - CERN · – Process of connecting subcomponents to cavity openings – Slow and careful steps, high level of attention to detail – Ionized

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Performance History DESY cavity experience

L. Lijie’s summary of DESY cavity databank, DESY, 2006

Page 43: SRF Cavity Preparation and Limitations - CERN · – Process of connecting subcomponents to cavity openings – Slow and careful steps, high level of attention to detail – Ionized

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Performance from my experience• In the early 1990’s gradients were mainly limited around15MV/m

vertical test and 10MV/m in machines– Field emission dominated the performance– Preparation procedure

• Bulk removal BCP, RF tuning, Degreasing, Final light BCP, DI water rinsing, Assembly

• By the mid 1990’s high pressure rinse was established as a new cleaning method to reduce field emission

• Early 2000 – Gradients had reached 20-25 MV/m vertical test which correlated to

machine performance as well– Electropolish chemistry was reintroduced and showed gradients could be

pushed to 30-35MV/m

• Today the focus is on reproducibility with occasional 40MV/m performances

Page 44: SRF Cavity Preparation and Limitations - CERN · – Process of connecting subcomponents to cavity openings – Slow and careful steps, high level of attention to detail – Ionized

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Standard Process Generalized• Heavy chemical etch (EP or BCP)

– Removal of damaged surface layer (100-150um) caused by fabrication and handling

• Removal of surface contamination– Ultrasonic cleaning of surface with detergent and DI water, heated and or– Alcohol rinse of surface to remove chemical residues

• Heat treatment (600-800C in vacuum furnace)– Removes hydrogen from the bulk niobium to reduce the risk of Q-disease

• RF tuning and mechanical inspection– Last chance to prepare cavity for operational use– Field profile, calibration of test probes, check mechanical structure

Page 45: SRF Cavity Preparation and Limitations - CERN · – Process of connecting subcomponents to cavity openings – Slow and careful steps, high level of attention to detail – Ionized

45 Managed by UT-Battellefor the U.S. Department of Energy Presentation_name

Standard Process Generalized cont.• Removal of surface contamination

– Ultrasonic cleaning of surface with detergent and DI water, heated

• Light chemical etch (EP)– Remove any risk from damage during handling and furnace contamination

• Removal of surface contamination (chemical residues)– Ultrasonic cleaning– Alcohol rinse

• High pressure rinse (UPW) + Class 10 drying of cavity– Reduction of field emission sources, surface particulates– At least two passes over entire surface

Page 46: SRF Cavity Preparation and Limitations - CERN · – Process of connecting subcomponents to cavity openings – Slow and careful steps, high level of attention to detail – Ionized

46 Managed by UT-Battellefor the U.S. Department of Energy Presentation_name

Standard Process Generalized cont.

• Assembly of subcomponents (most hardware at this step)– Process of connecting subcomponents to cavity openings– Slow and careful steps, high level of attention to detail– Ionized nitrogen gas blow off (cleaning) of subcomponents and hardware – Assembly optimized to reduce particulate contamination into cavity

surface

• High pressure rinse (UPW) + Class 10 drying of cavity– Last chance to clean surface and remove particulates from first assembly– Most critical cleaning step against field emission– At least two passes over entire surface

• Assembly of subcomponents (final evacuation flange)– Most critical assembly step no follow-up cleaning

Page 47: SRF Cavity Preparation and Limitations - CERN · – Process of connecting subcomponents to cavity openings – Slow and careful steps, high level of attention to detail – Ionized

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Heat treatment (600-800C)Details

Temperatureof hot zone

Low end 600C Typical 800C

Vacuum Start 1e-7 Torr End 1e-5 Torr

Cavity cleaning

Typically -degreasing

Sometimes-Chemistry and HPR

Support structure

Moly rails or rods

Automated controls

RGA, PLC

Process time 6-12 hrs or more

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Small Part Ultrasonic Cleaning Stations• Rinse tank out• Fill with DI water• Add Liquid Detergent

– Liquinox– Micro-90– Few percent by

volume• Ultrasonic agitation

– 15-60 minutes• Remove and rinse

parts with DI water• Blow dry

– ionized nitrogen gas– Laminar flow hepa air

Page 49: SRF Cavity Preparation and Limitations - CERN · – Process of connecting subcomponents to cavity openings – Slow and careful steps, high level of attention to detail – Ionized

49 Managed by UT-Battellefor the U.S. Department of Energy Presentation_name

Ultrasonic cleaning

• Immersion of components in DI water and detergent medium

• Wave energy forms microscopic bubbles on component surfaces. Bubbles collapse (cavitation) on surface loosening particulate matter.

• Transducer provides high intensity ultrasonic fields that set up standing waves. Higher frequencies lowers the distance between nodes which produce less dead zones with no cavitation.

• Ultrasonic transducers are available in many different wave frequencies from 18 KHz to 120 KHz, the higher the frequency the lower the wave intensity.

Page 50: SRF Cavity Preparation and Limitations - CERN · – Process of connecting subcomponents to cavity openings – Slow and careful steps, high level of attention to detail – Ionized

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The Need For Material Removal

• • • • •

• 0

10

20

30

40

0 50 100 150 200 250

Rre

s [nΩ

]

Material Removal [µm]

• •

• • •

• •

010203040506070

0 50 100 150 200 250

Epe

ak [M

V/m

]

Material Removal [µm]

K. SaitoP. Kneisel

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Niobium Material Removal by Chemistry

Niobium surface after BCP Niobium surface after EP

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Hydrofluoric Acid Safety• Hydrofluoric acid is an anomaly

– It does not react like all other acids once absorbed into the skin

– It absorbs deeply into skin, destroys everything in the path, then slowly releases into blood stream bonding all calcium

– Calcium is needed to control the hart cardiac arrest can result in 8 hours after the exposure

– Time to proper first aid (removal of and bonding of fluorine) is the most important detail and will determine the outcome

– Large exposures always lead to death even with first aid and medical treatment

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HF Safety cont.

• Before using HF– Ensure the lab has a functioning safety shower– Calcium gluconate cream or equivalent– Proper PPE to cover all exposed skin– Additional personnel trained in providing first aid and available

• Before using a System– Review and understand the hazards– Know what to do when an accident happens

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Buffered Chemical Polish (BCP)Acid = HF (49%), HNO3 (65%), H3PO4 (85%)Mixture 1:1:1 , or 1:1:2 by volume typical

Reaction:

Oxidation 2Nb + 5HNO3 Nb205 + 5NO2

Reduction Nb2O5 + 6HF H2NbOF5 + NbO2F 0.5H2O + 1.5H2O

NbO2F 0.5H2O + 4HF H2NbOF5 + 1.5H2OReaction exothermic!

Brown gas

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Use of BCP:

• 1:1:1 still used for etching of subcomponents (etch rates of 8um/min)

• 1:1:2 used for most cavity treatments– Mixing necessary reaction products at surface– Acid is usually cooled to 10-15C (1-3um/min) to control

the reaction rate and Nb surface temperatures (reduce hydrogen absorption)

Dissolved Niobium in Acid (g/L)

Etch rate (um/min)

Acid Wasted After 15g/L Nb

Page 56: SRF Cavity Preparation and Limitations - CERN · – Process of connecting subcomponents to cavity openings – Slow and careful steps, high level of attention to detail – Ionized

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Effects of BCP on The Niobium Surface

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(BCP) Systems for Cavity Etching:

• Bulk & Final chemistry– Bulk removal of (100-200um)– Final removal of (5-20um) to

remove any additional damage from QA steps and produce a fresh surface

Implementation:

• Cavity held vertically

• Closed loop flow through style process, some gravity fed system designs

• Etch rate 2X on iris then equator

• Temperature gradient causes increased etching from one end to the other

• Manually connected to the cavity but process usually automated

BCP Cabinet JLab

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Electropolish (EP)

Electrolyte = 1 part HF(49%), 9 parts H2SO4 (96%)

Reaction:Oxidation

2Nb +5SO42- + 5H2O Nb2O5 +10H+ +5SO4

2- +10e-

ReductionNb2O5 + 6HF H2NbOF5 + NbO2F 0.5H2O + 1.5H2O

NbO2F 0.5H2O + 4HF H2NbOF5 + 1.5H2O

Hydrogen Gas

These are not the only reactions that take place!

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Nb Surface Effects After EP

Page 60: SRF Cavity Preparation and Limitations - CERN · – Process of connecting subcomponents to cavity openings – Slow and careful steps, high level of attention to detail – Ionized

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50 μm 50 μm

BCP EP

Surface Roughness of Niobium

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Basic Concepts of EP

+--

PotentialV1 V2 V3

Curr

ent

Den

sity

• 0-V1- Concentration Polarization occurs, active dilution of niobium, electrolyte resistance

• V2-V3 – Limiting Current Density, viscous layer on niobium surface

• >V3 Additional Cathodic Processes Occur, oxygen gas generated

Al

Nb

I-V Curve

DC Power Supply

Page 62: SRF Cavity Preparation and Limitations - CERN · – Process of connecting subcomponents to cavity openings – Slow and careful steps, high level of attention to detail – Ionized

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Cavity IV Curve not easy to interpret

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63 Managed by UT-Battellefor the U.S. Department of Energy Presentation_name3/27/06 OPS-

T lk

Hydrogen Gas Shielding Experiment

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Electropolishing of 9-cell Resonators (Nomura Plating & KEK)

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Electropolishing Systems JLAB

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Electropolishing Systems DESY

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T lk

High Pressure Rinsing:

• The need for HPR surface cleaning:– Entire surface contaminated after

chemistry, early field emission will result if not performed

– Effective at removing particulates on the surface after assembly steps

ISSUES:

• HPR systems are still not optimized for the best surface cleaning performance • Surface left in a vulnerable state, wet

• This is still the best cleaning method against field emission!

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T lk

HPR spray heads needs to be optimized for a particular geometry!

Very effective on irises Equator fill with water too high flow rate

For a given pump displacement the nozzle opening diameter and number of nozzles sets the system pressure and flow rate

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Helium Processing

• Variation of RF processing• Keep pressure below discharge condition• Run cavity in the field emission regime• Push the gradient as high as the system allows• The process in details is unknown

– Electron spraying from FE bombard surface ionization of helium at around surface destroy field emitter???

– Controlled processing is difficult• Relying on field emitter locations and responses

– Uniformity??

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71 Managed by UT-Battellefor the U.S. Department of Energy Presentation_nameRongli Geng

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Preliminary experimental setup in RFTF

805 MHz500W CW amplifier

HB cavity

Gas feedingmanifold

Pump

First plasma in the SNSHB cavity

300W forward200W reflected1e-4 torr

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Plasma cleaning

• Ablation– Soft– Etching

• Activation• Crosslinking• Deposition

Base material

contaminants

Ion, molecule (radical), electron

before

afterwettability

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AP Talk Feb 19 2009

Radiation (before and after processing)Radiation reduced by factor of 5 to 100Showed promising results for in-situ processing

before after

Eacc=10 Eacc=10

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Integrated Process Automation

The Need!• Cryomodules are expensive ($M)

– Amount of hands-on labor– Failure rates (sensitivity of performance to errors)– Material costs (increasing with time, complexity of design)

• Machine energies are increasing– Cryomodule numbers are increasing (100,s 1000’s)

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Integrated Process Automation

• There is hope however for reduction of failure rates and labor– In my opinion “Vertical EP” may be the breakthrough we

needed

– Now one can imagine combining many of the processes into a single process station or two• Example

• Degreasing Assembly• Electropolish Evacuation• HPR Leak test• Drying Baking