Status of high intensity polarized electron gun project

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Status of high intensity polarized electron gun project at MIT-Bates 09/13/2011 Evgeni Tsentalovich MIT

Status of high intensity polarized electron gun project at MIT-Bates 09/13/2011 Evgeni Tsentalovich MIT 1

e. RHIC (Linac-ring version) Requires a polarized electron source with an extremely high current

e. RHIC (Linac-ring version) Requires a polarized electron source with an extremely high current ( at least 50 m. A). • Average current of tens or even hundreds of m. A is required • Modern state-of-the-art guns produce ~100 -200 A • Average current of ~ 1 m. A achieved in tests at JLab and Mainz; lifetime ~ 20 h • Average current of up to 10 m. A achieved at Mainz with very short lifetime (needs active cathode cooling) Main problem – ion backbombardment 2

Ion damage mostly the center of cathode (Bates results) Damage pattern Laser beam profile

Ion damage mostly the center of cathode (Bates results) Damage pattern Laser beam profile 05/20/2008 3

High Intensity Polarized Electron Gun The principal points to achieve high average current: •

High Intensity Polarized Electron Gun The principal points to achieve high average current: • Large area cathode. • Ions tend to damage the central area of the cathode – ring-shaped emission pattern. • Active cathode cooling. • Very small beam losses could be allowed near the gun ( ).

Phase I results: beam simulations. Three different initial emitting pattern were used: Ring-shaped Gaussian

Phase I results: beam simulations. Three different initial emitting pattern were used: Ring-shaped Gaussian Flat The pictures represent the beam shape 400 mm from the cathode.

Beam line. Pipe aperture ~± 34 mm. Beam dump Dipoles Solenoidal lenses Gun

Beam line. Pipe aperture ~± 34 mm. Beam dump Dipoles Solenoidal lenses Gun

Losses estimates It is difficult to get a correct shape of the tails in

Losses estimates It is difficult to get a correct shape of the tails in regular simulations. Special simulations with electrons emitted only from the edge of the cathode (r>11. 8 mm) have been performed. The resulting tail can be approximated by Gaussian distribution: R, mm 10 11 Losses . 037 . 012 12 13 14 15 16 17 Results for the ring-shaped beam at the entrance into the first dipole. r 0=4. 9 mm, σ=1. 9 mm. Aperture is about 30 mm. Similar calculations have been performed in several different locations in the beam line with all three initial emitting pattern. No substantial beam losses have been discovered.

Ion distribution Simplification: the cross section ionization was independent of electron energy. Electron current

Ion distribution Simplification: the cross section ionization was independent of electron energy. Electron current profile Ion energy profile

Interesting problem - beam dump Water cooling Beam Current monitor PUMPS I~50 m. A

Interesting problem - beam dump Water cooling Beam Current monitor PUMPS I~50 m. A → P~6 k. W !!! Outgasing in the dump could be serious problem.

Biased beam dump (energy recovery) -120 k. V Gun power supply Isolated 1 k.

Biased beam dump (energy recovery) -120 k. V Gun power supply Isolated 1 k. V power supply Gun Electron energy in the dump drops from 120 k. V to 1 k. V. Heating power in the dump drops from 10 k. W to 100 W Beam line -119 k. V Beam dump 100 W in the dump still needs to be removed, and now dump is at 120 k. V ! Needs fluorinert chiller.

Cathode Cooling Test Chamber HV Coolant in Coolant out Manipulator Crystal Cathode Laser 11

Cathode Cooling Test Chamber HV Coolant in Coolant out Manipulator Crystal Cathode Laser 11

Cathode – anode assembly Fluorinert (cooling agent)

Cathode – anode assembly Fluorinert (cooling agent)

Cathode – anode assembly Fluorinert (cooling agent)

Cathode – anode assembly Fluorinert (cooling agent)

Cathode – anode assembly

Cathode – anode assembly

Pack with a crystal

Pack with a crystal

Heat exchanger

Heat exchanger

Preparation chamber

Preparation chamber

General assembly – top view MANIPULATORS PREP. CHAMBER LENSES LOAD LOCK SECOND DIPOLE GUN

General assembly – top view MANIPULATORS PREP. CHAMBER LENSES LOAD LOCK SECOND DIPOLE GUN

General assembly – top view GUN PREP. CHAMBER LOAD LOCK FIRST DIPOLE

General assembly – top view GUN PREP. CHAMBER LOAD LOCK FIRST DIPOLE

Tests results in the cathode cooling chamber T(crystal), C -Vacuum manipulations works very well:

Tests results in the cathode cooling chamber T(crystal), C -Vacuum manipulations works very well: excellent illumination with internal halogen bulbs, good visibility, reliable pack transfer. -High Voltage: processed the chamber to 125 k. V, but electrical discharges happened. The ceramic pipes need better protection from the electrons produced by cold emission. -Temperature control: the pack temperature could be held at below 25°C even at the maximum laser power available (about 34 W on the crystal) 70 60 50 40 30 20 10 0 Chiller off Tch=20 C Tch=15 C Tch=10 C Tch=5 C 0 5 10 15 P. W 20 25 30 35

Vacuum features of the gun chamber • 100 l/s Ion pump with 400 l/s

Vacuum features of the gun chamber • 100 l/s Ion pump with 400 l/s NEG. • 4 additional 400 l/s NEGs (only two are currently installed). • The chamber walls are thin (~ 3 mm) to reduce outgasing. • The chamber and most of the parts have been prebaked to 400°C before the final assembly. • Bake-out at 250°C after the final assembly. • RGA readings after bake-out: m P, mbar 2 16 18 28 44

HV processing • The operating voltage is 120 k. V • The gun was

HV processing • The operating voltage is 120 k. V • The gun was processed to 150 k. V • After the processing no activity (measurable dark current, vacuum increase) could be detected at 120 k. V • The Fluorinert produces virtually zero conductivity (unable to measure).

Current status The gun chamber: built and tested. It was vented 3 weeks ago

Current status The gun chamber: built and tested. It was vented 3 weeks ago to install the first dipole followed the gate valve and 2 additional NEGs. Rebaked and HV reprocessed. • • The preparation chamber: design is completed, the main chamber has been manufactured, many parts are already ordered. • Load lock – the design is in progress. • Beam line – conceptual design is completed, some parts are designed, the dipole vacuum chambers have been manufactured.