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High current SRF gun Erdong Wang High current SRF gun Erdong Wang

High current SRF gun Erdong Wang - PowerPoint Presentation

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High current SRF gun Erdong Wang - PPT Presentation

Brookhaven National Laboratory 6152015 1 IEB Workshop 2015 Outline Overview SRF gun technology Overview high current SRF gun projects SRF guns Photocathodes Recent progress of BNL 704MHz SRF gun ID: 760685

gun 2015 srf high 2015 gun high srf ieb workshop current bunch charge beam cathode operation gradient long emittance

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Slide1

High current SRF gun

Erdong WangBrookhaven National Laboratory

6/15/2015

1

IEB Workshop 2015

Slide2

Outline

Overview SRF gun technologyOverview high current SRF gun projectsSRF gunsPhotocathodesRecent progress of BNL 704MHz SRF gunChallenges and considerationsSummary

6/15/2015

IEB Workshop 2015

2

Slide3

Why SRF photocathode gun?

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IEB Workshop 2015

3

To get high average current , the gun must operate in CW mode.Candidate: DC gun, VHF NCRF gun, VHF~L band SCRF gun

DC gun:

Mature

Cathode

gradient<7MV/mGun voltage:550kVCornell, Jlab, KEK, JAEA,IHEP

NCRF gun:

Commissioning

Cathode Gradient:

20MV/mGun voltage:1MVLBNL, SLAC,SHLS

SCRF gun:

Commissioning

CW at high frequencyCathode gradient:20~35MV/mGun voltage:2~9.4MVBNL, HZD,HZB, NPS, WiFEL

High gradient :High bunch charge Small emittanceLarge gap voltage:Small emittance

Slide4

Overview : SRF gun technology

Advantages:CW mode of operation: High rate of acceleration; high average beam current; Very stable(phase, amplitude) system reduce time jitter.High gradient on cathode: high bunch charge ; small emittance.SRF cavity and operation have matured.Elliptic cavity(low-β cell + 0~3 cell high-β) geometries based SRF gun has demonstrated and under developing for high current operation.Quarter wave resonator SRF gun is under development and got beam on NPS gun.The integration of a high QE semiconductor photocathode and the SRF gun is still a challenging topic.

6/16/2015

IEB Workshop 2015

4

Slide5

Overview SRF gun :Elliptic cavity+NC_cathode

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IEB Workshop 2015

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BNL /AES 704MHzHZD 3.5 CellHZB Berlin ProGun structureBunch charge(nC)5/1.4/0.71/0.0770.077Ave. Current(mA)50/3000.5/14Gun freq.(MHz)703.7513001300Peak gradient(MV/m)2030/22<10photocathodeCsK2SbCs3Te,MgCsK2SbN_Emittance(mm-mrad)5/2.3/1.42.5/11Kinetic energy(MeV)29.4/43.5Current statusBeam commissioningBeam commissioning ,upgradeVertical tested

Mature cavity shape; high kinetic

energy; high average current

Slide6

Overview SRF gun :QWR cavity+NC_cathode

6/15/2015

IEB Workshop 2015

6

BNL 112MHz(CeC)NPS (FEL)Wi FEL (FEL)Gun structureBunch charge(nC)510.2Ave. Current(mA)5011Gun freq.(MHz)112500200Peak gradient(MV/m)19.72545photocathodeCsK2SbCsK2SbCs3Te, CuN_Emittance(mm-mrad)340.9Kinetic energy(MeV)21.24.58Current statusRF conditioningBeam commissioningBeam commissioning

4K operation; high gradient; long bunch; constant field(small energy spread)

Slide7

Overview SRF gun :Other type

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IEB Workshop 2015

7

PKU DC-SC 3.5 cellHZB HoBiCatGun structureBunch charge(nC)0.10.015Ave. Current(mA)1~50.0045Gun freq.(MHz)13001300Peak gradient(MV/m)4.510photocathodeCs3TePb/NbN_Emittance(mm-mrad)1.21Kinetic energy(MeV)53.5Current statusCommissioning finished, upgradeupgrade

Prevent cathode contamination;

Full superconducting

Slide8

Photocathode

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IEB Workshop 2015

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To generate high average current beam, high QE(>1%) photocathode is required.

Wavelength(nm)

QE

Thermal

emittance

(mm-

mrad

/mm)

Lifetime

K

2

Cs(Na)Sb

532

10%~1%

0.4

Long

GaAs

532/780

~10%/1%

0.44

Short

Cs

3

Te

266

16%~1%

0.5

Long

Diamond amplifier

Electron

beam

Gain >200 times

?/ Energy spread

σ

=0.12eV

Long

Diamond

/Si field

emitter

Field emitter

NA

?

Very

long

Plasmonic

800

nonlinear

1.4

Very

long

Pb

250

0.0001%

?

Very

long

Slide9

704MHz gun and beamline

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IEB Workshop 2015

9

SRF gun: Pulse to CW 2MV

Laser: LUMERA: Nd: YVO4, single pulse to 9.38 MHz, up to 6 W at the cathode surface.

RF: adjustable pulse length

Raw signal

Integrated signal

ICT window

7

μ

S

Laser pulse

(controlled by

pockels

cell)

Slide10

Choke joint cathode stalk upgrade

6/15/2015

IEB Workshop 2015

10

Re-designed choke

structure to eliminate

multipacting

. Allow CW operation

up to

2MV.

Change the cathode substrate to

Ta to have better QE for high current, high bunch charge operation.Better cooling design to dump the heat dissipation on the stalk.

Double choke with groove

Slide11

Photocathode for BNL SRF gun

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IEB Workshop 2015

11

CsK

2

Sb @

532nm ,10%

Slide12

Photocathode preparation and transferring

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IEB Workshop 2015

12

Slide13

Conditioning result and beam commission

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IEB Workshop 2015

13

550pC bunch charge

Dark current

Photo current

Courtesy by Wencan Xu

The

QE of CsK

2

Sb was 4.1% at initial prepared and 3.8% before inserting into the gun.

The

gun was then conditioned and

sent beam to

a Faraday

cup. Pulsed

operations yielded bunches with up to 0.55nC

per-bunch

.

The gun was operated in pulsed mode at 0.85MV

kinetic

energy. The

ICT and Faraday cup measurements

confirmed

QE=1% at low

current.

A

fter

running for a couple of

days including condition and high bunch charge test,

there was no observed degradation of the QE

.

Slide14

Challenges and considerations

SRF gun merging high QE photocathode, superconducting RF, high repetition rate laser, beam diagnostic. All complex.Semiconductor cathode material contamination the gun/stalk induce the multipacting.Bias the cathodeShielding the RF fieldProtect the multipacting zone in cathode preparationHigh bunch charge and high average current operation with long lifetime cathodeGood vacuum in gun operationHigh input power couplerBeam halo controlGood beam qualityHigh peak gradient on the cathodeUniform ,smooth and low thermal emittance photocathodeLaser shaping on both transverse and longitudinalLaser and gun synchronization precisely. CW mode Dark current eliminatingKick the dark currentReduce the field emitter areaStable SRF operationCryogenic operationCoupler kick and HOM damping

6/15/2015

IEB Workshop 2015

14

Slide15

Summary

SRF photoinjectors are promising to provide high bunch charge, high average current and small emittance beam.Significant progress on SRF gun researches in last a few years. For example: BNL 704MHz gun generated 550pC per bunch and no observed degradation of the QE in two days gun condition and operation.ELBE SRF gun I generated beam for FEL operation and PKU DC-SC gun delivered beam for THz and UED test.Demonstration of high average current operation and high bunch charge operation are under going.Beginning of a new adventure, look forward to having more exciting results soon.

6/15/2015

IEB Workshop 2015

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Slide16

Acknowledgements

Thanks to BNL ERL and CeC project team.I. Ben-Zvi; T. Rao; S. Belomestnykh; D. Kayran; B. Sheehy; H. Xie; T. Xin; W. Xu; L. Hammons; R. Kellerman; C. Liaw; V. Litvinenko; G. McIntyre; T. Miller; T. Seda; R. Than; D. Weiss; B. Xiao; J. Skaritka; I. Pinayev and many others.

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Slide17

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IEB Workshop 2015

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Thanks for you attention!

Slide18

Backup

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IEB Workshop 2015

18

Slide19

6/15/2015

IEB Workshop 2015

19

From J. Teichert IPAC 2014 slides