TiN coating of the CSNS ceramic vacuum chambers.ppt · magnetic fields and the large ohmic losses....

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TiN coating of the CSNS ceramic vacuum chambers Haiyi Dong Institute of High Energy Physics, CAS 9/28/2015

Transcript of TiN coating of the CSNS ceramic vacuum chambers.ppt · magnetic fields and the large ohmic losses....

TiN coating of the CSNS ceramic vacuum chambers

Haiyi DongInstitute of High Energy Physics, CAS

9/28/2015

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Outline

• CSNS Project

• Ceramic chambers

• Setup of TiN coating

• Analysis of the samples

• Summary

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Schematic layout of CSNS facilities

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China Spallation Neutron Source (CSNS) is designed to accelerate proton beam pulses to 1.6GeV kinetic energy with a beam power of 100kW at 25Hz repetition rate, striking a solid metal target to produce spallation neutrons. H- are firstly generated from a Penning ion source. RFQ forms beam bunches and accelerates the beam to 3 MeV. DTL tanks further increase the beam energy to 80 MeV. A long beam transport line is followed with the DTL to send the beam to a rapid cycling synchrotron (RCS) accelerator. The H- beam is stripped to become proton beam and injected into the RCS ring. In the ring the proton beam is accumulated to a high current pulse and then accelerated to 1.6 GeV. The high-energy proton beam extracted from the RCS bombards on the target to generate neutrons through spallation reaction.

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Linear Accelerator (Ion Source+LEBT+RFQ+MEBT+DTL)

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LRBT vacuum system

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Rapid Cycling Synchrotron (RCS)

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2. Ceramic chambers

• The ceramic chambers were chosen in the dipole and quadrupole magnets to reduce the eddy-current effect which will produce the perturbation of magnetic fields and the large ohmic losses.

• The quadrupole ceramic chambers have been fabricated by metallizing and brazing.

• The glass joint has been adopted for the CSNS dipole ceramic chambers since this method is considerably less expensive and relatively simple than that of metallizing the ceramic pipe ends and brazing them together.

• Metal seal of Helicoflex Delta type and demountable chain clamp are used for the quick disconnect flanges.

• A new RF shielding method for the ceramic chambers has been developed.

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Quadrupole Ceramic Vacuum Chamber

Glass jointLaser welding

Cu-Ag brazing

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Dipole Ceramic Vacuum Chamber

• A 2.8m-long dipole ceramic chamber consists of 8 ceramic tubes with 15 bending .

• Each end of the ceramic tube is ground flat and glazed with a thin layer of suitable glass.

• The ceramic flange is also joined to the ceramic tubes by glass brazing in the air furnace of 1200C.

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Types of Ceramic Chambers

MB QA QB QC QD INB1 INB2 QKA QKB

Drawings No. ACVA-****-0000

1101 1102 1103 1104 1105 1106 1107 1108 1109

Flange Sizes KF250 KF250 KF250 KF250 KF250 KF200KF200 CF150

KF250 KF250

Numbers of Installation 24 15 15 8 8 3 1 1 1Numbers of Spares 2 1 1 1 1 1 1 1 1

Numbers of manufacture 26 16 16 9 9 4 2 2 2

Length (mm) 2775 780 1535 1540 1205 1070 1415 740 1520

Outer Diameter (mm) 152×248 198 264 214 245 178 165 198 264

Inner Diameter (mm) 135×218 183 249 199 230 163 150 183 249

Wall Thickness (mm) 8.5×15 7.5 7.5 7.5 7.5 7.5 7.5 7.5 7.5

Numbers and Types of the CSNS Ceramic Vacuum Chambers

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• The total leak rate of the dipole ceramic chamber is less than 2×10-11 Pam3/s

• The ultimate pressure of the ceramic chamber reached 5×10-8 Pa after 48h bakeout at 160C.

• The outgassing rate of the inner surface of the ceramic chamber is less than 5×10-13 Pam3/scm2.

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RF shielding prototype of a dipole ceramic chamber

• RF copper strips with a length of 3m were cut with water according to the shape of a dipole ceramic chamber. • 8 sheets of RF copper strips with 3 types were fixed on the surface of ceramic chamber by kapton film knitting.• Advantage: no soldering points, cost-efficient.

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3. Setup of TiN coating for the ceramic chambers

• A thin TiN layer of about 100 nm in thickness was coated in order to minimize the secondary electron yield (SEY) and prevent the charges from building-up in the inner surface.

• DC magnetron sputtering has been adopted to coat TiN inside the ceramic chambers.

• The equipment of TiN coating consists of Ti cathodes with magnets and copper anodes outside the ceramic chambers.

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Ti Cathode and vacuum seal assembly

• The magnets inserted inside Ti cathode are stacked with opposing poles, resulting in a looping magnetic field of sufficient strength on the cathode surface.

• Ti cathode is insulated with vacuum chamber by teflon and sealed by viton ring.

• A cooling water tube is needed to cool down Ti cathode during DC magnetron sputtering.

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TiN coating for the quadrapole ceramic chamber

An anode screen made of thin copper sheet of 1 mm in thickness is wrapped outside the ceramic chamber in order to produce an electric field with the Ti cathode. This will result in a uniform thickness of TiN along the ceramic chamber. The uniformity of TiN thickness is better than 10, and the ratio of Ti and N is about 0.93.

SNS

J-PARC

CSNS

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The electric field simulation for TiN coating of the quadrapole ceramic chamber(CST)

An anode grid inside chamber(2100V/m) An Anode screen outside chamber(1956V/m) No anode(1561V/m)

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Ar+ discharge plasma distribution on the surface of a cathode(COMSOL Multiphysics)

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Setup of TiN coating for the quadrupole ceramic chamber

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Left cathode(7.5)

Right cathode(7.5)

N2/Ar inlet

Cathode supports

TiN coating setup for a full-scale dipole ceramic chamber

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TiN coating for the CSNS dipole ceramic chamber

• Two bending magnetron sputtering cathodes with a curve of 7.5 were inserted inside the dipole ceramic chamber symmetrically. • An anode screen made of thin copper sheet of 1 mm in thickness is wrapped outside the ceramic chamber in order to produce

an electric field with the Ti cathode. • The uniformity of TiN thickness is better than 50, and the ratio of Ti and N is about 0.92.

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5.00E‐03

5.00E‐02

5.00E‐01

5.00E+00

5.00E+01

5.00E+0214:38:02

14:39:34

14:41:06

14:42:38

14:44:10

14:45:42

14:47:14

14:48:46

14:50:18

14:51:50

14:53:22

14:54:54

14:56:26

14:57:58

14:59:30

15:01:02

15:02:34

15:04:06

15:05:38

15:07:10

15:08:42

15:10:14

15:11:46

15:13:18

15:14:50

15:16:22

15:17:54

15:19:26

15:20:58

15:22:30

15:24:02

15:25:34

15:27:06

15:28:38

15:30:10

15:31:42

15:33:14

15:34:46

15:36:18

15:37:50

15:39:22

15:40:54

Voltage(V)

Current(A)

Pressure(mbar)

Ar(sccm)

N2(sccm)

TiN coating parameters for the dipole ceramic chamber

Coating Ti and TiN with cathode 1 Coating Ti and TiN with cathode 2

390V

4.4sccm

2.3sccm

7E-3 mbar

7A

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4. Analysis of the TiN-coating samples

• TiN film thickness

• XPS measurements for TiN film Composition

• Secondary Electron yields

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TiN coating samples for the dipole ceramic chamber

TiN film thickness (44nm~135nm)

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Observation of digital metallurgical microscope for the ceramic samples with and w/o TiN film

Ceramic sample Ceramic sample coated with TiN

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0.00E+00

2.00E+04

4.00E+04

6.00E+04

8.00E+04

1.00E+05

1.20E+05

1.40E+05

010020030040050060070080090010001100

Cou

nts

/ s

Binding Energy (eV)

Survey1 Scan, 55.5 s, 500µm, CAE 100.0, 1.00 eV

92.028.19

78.17

N

Ti

XPS spectrum for TiN film composition measurement

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SEY measurements for the ceramic samples with and w/o TiN coating

Ceramic sample

5.821.92~2.06

Ceramic sample coated by TiN

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TiN coating for the CSNS Extraction kicker Ferrites

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5. Summary

• Most of the CSNS equipment have been produced and begun to install. The normal operation for user is foreseen in 2018.

• Both the dipole and quadrupole ceramic chambers have been coated with TiN by magnetron sputtering. Especially for the dipole ceramic chambers, two curved Ti cathodes of 7.5 were used.

• The thickness, composition and SEY for the samples coated with TiN have been measured. The results meet the requirements.

• Making use of the Ti cathode for coating the quadrupole ceramic chambers, the CSNS Extraction kicker Ferrites were coated with TiN to reduce SEY.

• The TiN coating of 86 ceramic chambers has almost been completed.

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