Commissioning and First Results from the Photo Injector Test - - PowerPoint PPT Presentation

commissioning and first results from the photo injector
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Commissioning and First Results from the Photo Injector Test - - PowerPoint PPT Presentation

Commissioning and First Results from the Photo Injector Test Facility at DESY Zeuthen (PITZ) introduction rf measurements dark current measurements with beam F. Stephan (DESY Zeuthen) for the PITZ Collaboration, ICFA Workshop


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SLIDE 1

Commissioning and First Results from the Photo Injector Test Facility at DESY Zeuthen (PITZ)

  • introduction
  • rf measurements
  • dark current
  • measurements with beam
  • F. Stephan (DESY Zeuthen) for the PITZ Collaboration,

ICFA Workshop @ Sardinia, Italy, July 1st – 5th, 2002

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SLIDE 2

The Photo Injector Test Facility at DESY Zeuthen (PITZ)

Goals:

  • test facility for FELs and future LCs:

⇒ very small transverse emittance (1 mm mrad @ 1 nC)

⇒ stable production of short bunches with small energy spread

  • extensive R&D on photo injectors in parallel to TTF operation
  • compare detailed experimental results with simulations:

⇒ benchmark theoretical understanding of photo injectors

  • test rf guns for subsequent operation at TTF-FEL
  • test new developments (laser, cathodes, beam diagnostics)
  • for TESLA: flat beams, polarized electrons
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SLIDE 3

BESSY, Berlin CAEP Mian Yang DESY, Hamburg and Zeuthen HEPI Tbilisi INFN Milano INR Troitsk INRNE Sofia Max-Born-Institute, Berlin TU Darmstadt, department TEMF YERPHI Yerevan

Current Layout

ICT

Collaboration:

  • diagn. cross
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SLIDE 4
  • January 13th, 2002: first photo electrons

rf pulse length: 300µs laser pulse length: 222µs

signal from Faraday cup

∆rf (laser- rf) = 5 kHz ⇒ automatic phase scan

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SLIDE 5

RF Conditioning in March 2002

  • rf pulse length: stable operation up to 400 µs

(more needs adjustment of gun water cooling system, ongoing)

  • rf pulse repetition rate: 5 Hz operation
  • gradient at cathode: up to 34 MV/m, limit of old PS

(new PS is installed, now under commissioning)

duty cycle: 0.2%

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SLIDE 6

DC measurements (preliminary results)

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SLIDE 7
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SLIDE 8

Laser Parameters and Bunch Charge

UV light at virtual cathode:

  • long. profile

by streak camera:

mm RMS y

x

65 .

, =

ps FWHMz 10 ≈

Laser:

(still gaussian shape)

Bunch Charges:

( ) pC

Qbunch 30 5− ≈ (MBI, Berlin)

  • during first run:
  • after cathode exchange:

up to 0.8 nC

  • serveral nC with

better cathode handling

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SLIDE 9

Momentum Measurements

(preliminary results)

80 70 / 35 180 = − = = = pulses laser

  • f

Number SP m MV SP A I

  • Phase

Voltage main

parameters: ← picture in dispersive arm

⇒up to 4.0 MeV/c

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SLIDE 10

1 70 arg / 27 200 = = = = pulses laser

  • f

Number pC e Ch m MV SP A I

Voltage main

parameters:

Mean Momentum vs. RF Phase

(preliminary) good agreement

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SLIDE 11

Calibration of Set Point voltage

maximum electron momentum vs. SP voltage: measurement with dark current maximum electric field vs. SP voltage: conclusions: Eacc

max ≈ 34 MV/m

klystron is operated close to saturation

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SLIDE 12
  • Phase

Voltage main

SP pC e Ch m MV SP A I 42 100 arg / 30 200 − = = = =

parameters: for 1: 1 2

Momentum spread vs. # of bunches

(prelininary results) for 2: possible explanation: RF amplitude changes during rf pulse conclusions: need to run with RF feedback (in preparation), measure momentum spread with low # of bunches

  • Phase

Voltage main

SP pC e Ch m MV SP A I 50 180 arg / 27 190 − = = = =

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SLIDE 13
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SLIDE 14

Commissioning the emittance measurement system

(very preliminary results) parameters:

SP = 32 MV/m I(main) = 166 A charge = 20 pC phase at optimum

  • method 1: measure all parameters with beamlets
  • method 2: measure beam size separately at position of slit mask
  • method 3: beam size from M2, divergence as weighted av. from

beamlets, correlation set zero

r m s v a lu e s m e th o d 1 m e th o d 2 m e th o d 3 b e a m s iz e [ m m ] 1 .0 5 1 .7 3 1 .7 3 d iv e r g e n c e [ m r a d ]

0 . 3 6 7 6

0 .3 6 7 6 0 .1 4 c o v a r ia n c e [ m m .m r a d ]

  • 0 . 3 4 3
  • 0 . 3 4 3
  • n o r m .e m itta n c e

[ m m .m r a d ] 1 .5 4 .3 1 .9

simulation result: 0.76 π mm mrad

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SLIDE 15

Future plans @ PITZ

  • upgrade rf system: better stability + higher
  • utput power (in autumn: 10 MW klystron)
  • commission diagnostics (p&∆p, Q, BPM,

EMSY, bunch length, long. phase space)

  • until end of April 2003: gun should be fully

characterized → use at TTF-FEL 2

  • then: upgrade PITZ with a booster cavity
  • 2004: measurements with higher beam energy

(~ 40 MeV)

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SLIDE 16

Simulations with booster cavity (Ph. Piot)

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SLIDE 17

Acknowledgements

for the current status of PITZ:

  • strong support from technical groups, physics groups

and administration at DESY (Hamburg and Zeuthen)

  • people from cooperation partners: BESSY, CAEP

Mian Yang, HEPI Tbilisi, INFN Milano, INR Troitsk, INRNE Sofia, Max-Born-Institute, TEMF@TUD, YERPHI Yerevan

  • colleagues from DESY Hamburg: J.P. Carneiro, K.

Flöttmann, Ph. Piot, J. Roßbach, S. Schreiber

  • members of the Zeuthen PITZ group: J. Bähr, I.

Bohnet, D. Lipka, A. Oppelt, T. Thon

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SLIDE 18

Summary

  • photo injector test facility at DESY Zeuthen

(PITZ) has taken first measurements with and without beam

  • commissioning and upgrade is ongoing
  • characterization of FEL gun is foreseen until

spring 2003

  • then upgrade facility with booster cavity