1. NON-INTERCEPTING DIAGNOSTIC FOR HIGH BRIGHTNESS ELECTRON BEAMS USING OPTICAL DIFFRACTION RADIATION INTERFERENCE (ODRI) A. Cianchi #1,2, M. Castellano 3, L. Catani 2, E. Chiadroni 3, G. Gatti 3, K. Honkavaara 4, G. Kube 4 1 University of Rome “Tor Vergata” v. della Ricerca Scientifica 1, 00133 Rome, Italy 2 INFN- Roma Tor Vergata, v. della Ricerca Scientifica 1, 00133 Rome, Italy 3 INFN –LNF, v. E. Fermi 40, 00040 Frascati (RM), Italy 4 DESY, Notkestrasse 85, 22607 Hamburg, Germany IX International Symposium RREPS - 11

2. Outlook  Importance of not intercepting diagnostic  Optical Diffraction Radiation vs Optical Diffraction Radiation Interference  Non collinear apertures  Experimental setup  Results  Horizontal polarization

3. High Brightness Machines [A/(m-rad) 2 ] V. Balandin, N. Golubeva High density power beam can substantially damage or destroy a foil or a wire scanner Possible alternatives are multishots devices ― Wire scanner (intercepting) ― Laser wire

4. Optical Diffraction Radiation (ODR)  The charge goes into the hole without touching the screen  The electromagnetic field of the moving charge interacts with the metallic screen  No power is deposited on the screen  The angular distribution of the emerging radiation is affected by the beam transverse size, the angular spread and the position inside the slit  Rectangular slit P. Karataev et al., “Beam-Size Measurement with Optical Diffraction Radiation at KEK Accelerator Test Facility”, Phys. Rev. Lett. 93, 244802 (2004)

5. Background noise E. Chiadroni et al., Non-intercepting electron beam transverse diagnostics with optical diffraction radiation at the DESY FLASH facility NIM B 266 (2008) 3789–3796 Mainly Synchrotron radiation, both directly coming for bending magnets and reflected from the vacuum chamber walls

6. Two slits geometry (ODRI) Optical Diffraction Radiation Interference (ODRI)

7. Collinear slits Point like beams with different angular spread Possible confusion between the contribution of the angular spread and the beam dimension

8. Non collinear slits The 50  m offset between the slits is enough to avoid mixing between the contributions of angular spread and beam size

9. Approximations and formulas  Perfect metal  Filter bandwidth negligible  Beam energy spread negligible  Beam Gaussian both in y and y’  Slit parallelism correction (M. Castellano, E. Chiadroni, A. Cianchi, “Phase control effects in optical diffraction radiation from a slit”, Nuclear Instruments and Methods in Physics Research A 614 (2010) 163–168)  Numerical code

10. Experiment @ FLASH FLASH is an excellent linac for this experiment:  High energy up to 1 GeV  Large number of bunches (up to 30) with high charge (up to 1 nC)  Frequency repetition 5 Hz  Long collaboration history

11. Optical System (1) High Sensitivity Hamamatsu Camera  High quantum efficiency  Air Cooling -55˚C  Long exposure time up to 2 hours Interferential filter at 800 nm Interferential filter at 450 nm Glenn-Thompson polarizer Achromat Lens with f=500 mm for DR angular distribution Lens with f=250 mm for beam imaging Hamamatsu CCD camera

12. Experimental Setup (1) Mirror Lenses Actuator Interferential filters Polarizer Camera holder

13. center -25 um -50 um -75 um -100 um -125 um -150 um Angular distribution

14. center +25 um +50 um +75 um +100 um +125 um +175 um Angular distribution (2)

15. Two different spots OTR beam 78±4 μ m 90±4 μ m ODRI beam 82 μ m 94 μ m,

16. A divergence of about 320 μ rad can be estimated from a quadrupole-scan emittance measurement carried out under the same experimental conditions RMS Beam Size (  m) 8278 RMS angular spread (  rad) 260310 Displacement in respect to the second slit (  m) -6-55 Misalignment between two slits (  m) 110113

17. Hardware evolution  New design in the mover Old screen holderNew screen holder

18. Experimental Setup (2) Mirror Lenses with one apochromatic lens Interferential filter 2 polarizers

19. Different wavelength 800 nm550 nm

20. Horizontal polarization Vertical Horizontal

21. X polarization 550 nm800 nm

22. Scan with the 1 mm slit 0.5  m slit out off center about -70  m 1 mm slit move range from -66  m to +200  m

23. To improve  Horizontal polarization features not fully understood  A control of the all known parameters is mandatory in order to make precise measurements  An analytic formula would be better than a MonteCarlo code

24. Conclusion  ODRI is in developing  ODRI dramatically reduce or eliminate the problem of background  Asymmetric configuration resolves parameters ambiguities  New measurements are foreseen to make a totally non intercepting emittance measurement

25. Thank you for your attention

26. Formulas

27. Multiple fit

28. Importance of side peaks

29. All data