1. High Intensity Polarized Electron Gun Studies at MIT-Bates 10/01/2008 PESP2008 1 Evgeni Tsentalovich MIT

2. Introduction, motivation Major challenges Developments at MIT-Bates Conclusion 10/01/2008 PESP2008 2 OUTLINE

3. eRHIC (Linac-ring version) 3 Requires a polarized electron source with an extremely high current Luminosity ~  I(average) ~ 250 mA I(peak) ~ 100 A High polarization → strained GaAs → QE ~ 0.5% Average laser power ~ 80 W (fresh crystal) Hundreds Watts might be needed as crystal loses QE 200 µA 10 A 1 W Currently achieved 10/01/2008 PESP2008

4. 4 Main challenges High average current – cathode damage by ion bombardment High heat load on the cathode – tens of Watts of laser power Solution: Cathode with very large area High peak current – surface charge saturation (QE drops at high light intensity); space charge saturation

5. 10/01/2008 PESP2008 5 Ion Damage Ion damage is inversely proportional to emitting area residual gas cathode Ionized residual gas strikes photocathode anode Ion damage distributed over larger area

6. 10/01/2008 PESP2008 6 Damage location Electrons and ions follow different trajectories. Usually, ions tend to damage central area of the cathode. JLAB data Ring-like cathodes ?

7. 10/01/2008 PESP2008 7 Ion Trapping in CW Beam Cathode Anode Beam line Ions produced below the anode are trapped in the electron beam. Half of them will drift toward the gun and get accelerated in the cathode-anode gap toward the crystal.

8. 10/01/2008 PESP2008 8 JLAB results for anode biasing Anode = 0 V Support = 0 V Charge = 172 C  QE Anode = 2 kV Support = 300 V Charge 175 C  QE

9. 10/01/2008 PESP2008 9 High Intensity Gun Studies at MIT/Bates The project investigates the feasibility of extracting very high (tens, perhaps hundreds of mA) current from the gun. The project addresses issues of high average current and high heat load on the cathode. Phase I – studies of ion damage, design and construction of the cathode cooler, gun simulations. Phase II – design and construction of the gun and the beam line, beam tests.

10. 10/01/2008 PESP2008 10 Ion Damage Studies - Apparatus Existing gun. New diode array laser ( ~808 nm, P up to 45 W). Existing test beam line. This beam line was not designed for high current and beam losses of 5-10% are typical. These losses produce out-gassing, and reduce the lifetime by both poisoning the cathode and ion bombardment. Relatively low lifetime and significant ion damage allowed to conduct the measurements fast. CW current – one can expect ion trapping.

11. Ring-shaped Laser Beam 10/01/2008 PESP2008 11 Fiber Cathode L1AxiconL2 Axicon (conical lens) in combination with a converging lens (L2) produces ring-shaped beam in the focal plane of L2. Lens L1 reduces the laser beam divergence (25  from the fiber). Without axicon, a very small beam spot will be produced. QE could be mapped by moving the L2

12. 10/01/2008 PESP2008 12 Axicon-based System Simulations L1L2Axicon

13. 10/01/2008 PESP2008 13 Axicon-based System Simulations

14. 10/01/2008 PESP2008 14 Beam Profile (no axicon) FWHM<.5 mm Measured using razor blade technique and inverse Abel transformation

15. 10/01/2008 PESP2008 15 Axicon Beam Profile

16. 10/01/2008 PESP2008 16 Axicon Beam Profile

17. 10/01/2008 PESP2008 17 Axicon Beam Profile

18. 10/01/2008 PESP2008 18 QE map of the Fresh Crystal QE, %

19. 10/01/2008 PESP2008 19 QE change (small spot in the center) Run 12.32 C

20. 10/01/2008 PESP2008 20 QE change (run with axicon) Run 17.35 C

21. 10/01/2008 PESP2008 21 QE change (axicon, anode biased 1 kV) Run 17.62 C

22. 10/01/2008 PESP2008 22 QE change (large spot in the center) Run 17.46 C

23. 10/01/2008 PESP2008 23 QE change (small spot in the corner) Run 16.84 C

24. 10/01/2008 PESP2008 24 Radial distribution

25. 10/01/2008 PESP2008 25 Lifetime

26. 10/01/2008 PESP2008 26 High Intensity Run (1 mA) Achieved.5 mA with laser power of.25 W (QE=.34 %) Achieved 1 mA with laser power of 1.16 W (QE=.15%) Gun vacuum pressure rise (factor of 10) Current dropped to 132  A in 1 hour At laser power of 1.16 W, QE degrades even without HV ! – Overheating. Thermal estimate (thermal conductivity through the stalk only ~.01-.025 W/degree

27. 10/01/2008 PESP2008 27 Conclusion Ion damage is concentrated near the center of the cathode in every configuration. Ring-shaped beam allows to improve the lifetime significantly. Biasing the anode improves the lifetime of the CW beam. Active cooling is a “must” for laser powers exceeding 1 W.

28. 10/01/2008 PESP2008 28 New optics Old optics: Small spot Axicon New optics

29. 10/01/2008 PESP2008 29 Gun Simulation Large emitting area produces large emittance Although emittance is less important for eRHIC, large beam could result in beam losses near the gun. The main purpose of the simulations is to minimize the beam losses in the gun and beam line. The second goal – ion distribution optimization

30. 10/01/2008 PESP2008 30 Gun Simulation

31. 10/01/2008 PESP2008 31 Gun Simulations - Ions

32. 10/01/2008 PESP2008 32 Gun Simulations - Ions

33. 10/01/2008 PESP2008 33 Gun Simulations - Ions

34. 10/01/2008 PESP2008 34 Cathode Cooling The conceptual design of the test chamber is completed. The test chamber will validate the adequacy of the cooling power, HV and high vacuum compatibility and vacuum cathode handling with manipulators.

35. 10/01/2008 PESP2008 35 Cathode Cooling Water in Water out HV Laser Manipulator Cathode Crystal

36. 10/01/2008 PESP2008 36 DBR – Equipped Crystal “Normal” cathode Cathode with Distributed Bragg Reflector (DBR) In “normal” cathode, only 30% of light is reflected. In DBR- equipped cathode 99% of light is reflected. For instance, talk by L. Gerchikov, St. Petersburg, at PESP 2007