harold g. kirk brookhaven national laboratory progress in quad ring coolers ring cooler workshop...

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Harold G. Kirk Brookhaven National Laboratory Progress in Quad Ring Coolers Ring Cooler Workshop UCLA March 7-8, 2002

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Page 1: Harold G. Kirk Brookhaven National Laboratory Progress in Quad Ring Coolers Ring Cooler Workshop UCLA March 7-8, 2002

Harold G. KirkBrookhaven National Laboratory

Progress in Quad Ring Coolers

Ring Cooler Workshop

UCLA

March 7-8, 2002

Page 2: Harold G. Kirk Brookhaven National Laboratory Progress in Quad Ring Coolers Ring Cooler Workshop UCLA March 7-8, 2002

Harold G. Kirk

Snowmass 01

Explore Ring Cooling Designs Use only Quads & Dipoles Obtain Longitudinal Cooling Maintain/Reduce Transverse Emittance Linear Lattice Design (SYNCH) Cooling Simulation (ICOOL)

Strategy

Page 3: Harold G. Kirk Brookhaven National Laboratory Progress in Quad Ring Coolers Ring Cooler Workshop UCLA March 7-8, 2002

Harold G. Kirk

The Snowmass Lattice

4 m drift available for rf Low (25 cm) at absorber Pseudo-combined function

dipole Allows for matching straight

sections 450 bending cell x max > y max

Cell tune is ~ 3/4

x

y

Page 4: Harold G. Kirk Brookhaven National Laboratory Progress in Quad Ring Coolers Ring Cooler Workshop UCLA March 7-8, 2002

Harold G. Kirk

Single Particle DynamicNo Stochastic Processes

10 ns

Longitudinal phase space damping increases with degree of wedge angle

Horizontal phase space reduces for wedge angles < 150 and increases for angles > 150

Vertical phase space reducesat a rate independent of wedge angles

V

R

Page 5: Harold G. Kirk Brookhaven National Laboratory Progress in Quad Ring Coolers Ring Cooler Workshop UCLA March 7-8, 2002

Harold G. Kirk

Snowmass Lattice Performance

10 ns

• initial y > initial x

• y and z decreases• x increases•Transmission 40%

Total Merit = Transmission x(x y z )initial/ (x y z )final

V

R

Beam momentum 500 MeV/c25 cm LH2 wedgesWedge angle 100

Rf frequency 201.25 MHzEmax = 10 MV/m

Page 6: Harold G. Kirk Brookhaven National Laboratory Progress in Quad Ring Coolers Ring Cooler Workshop UCLA March 7-8, 2002

Harold G. Kirk

Equilibrium Emittances

Problem is noted with the equilibrium horizontal emittance, which is much

higher than expected

Horizontal equilibrium emittance persists even for 00 wedges. Higher order dispersion effects?

Page 7: Harold G. Kirk Brookhaven National Laboratory Progress in Quad Ring Coolers Ring Cooler Workshop UCLA March 7-8, 2002

Harold G. Kirk

The Berkeley Lattice

4 m drift available for rf Low (25 cm) at absorber Pseudo-combined function dipole Allows for matching straight

sections 22.50 bending cell y max > x max

Cell tune is ~ 3/4

x

y

Page 8: Harold G. Kirk Brookhaven National Laboratory Progress in Quad Ring Coolers Ring Cooler Workshop UCLA March 7-8, 2002

Harold G. Kirk

Berkeley Lattice Equilibrium Emittances

Horizontal equilibrium emittance increases with wedge angle but 00 wedge angle behaves as expected

Longitudinal equilibrium emittance declines with increasing wedge angle

Page 9: Harold G. Kirk Brookhaven National Laboratory Progress in Quad Ring Coolers Ring Cooler Workshop UCLA March 7-8, 2002

Harold G. Kirk

Berkeley Lattice Performance

10 ns

• y and z decreases• x nearly constant•Transmission 60%

Total Merit = Transmission x(x y z )initial/ (x y z )final

V

R

Beam momentum 500 MeV/c25 cm LH2 wedgesWedge angle 200

Rf frequency 201.25 MHzEmax = 8 MV/m

Page 10: Harold G. Kirk Brookhaven National Laboratory Progress in Quad Ring Coolers Ring Cooler Workshop UCLA March 7-8, 2002

Harold G. Kirk

Consider Decay Losses

Ratio ( initial

Initial After 8

Turns

After 16

Turns

x, mm 2.5 0.93 0.87

y, mm2.6 2.33 2.65

z, mm29.2 2.83 4.02

Transmission 1.0 0.67 0.55

Decay survival

1.0 0.65 0.43Total merit peaks near 8full turns. 200 to 300

wedges are best.

final )

Page 11: Harold G. Kirk Brookhaven National Laboratory Progress in Quad Ring Coolers Ring Cooler Workshop UCLA March 7-8, 2002

Harold G. Kirk

What has been accomplished

The SYNCH + ICOOL approach works well Emittance exchange has been demonstrated This quad ring design does not replace Study II front

end but can follow it Transmission losses are still high Need to consider realistic quads (L = 20cm ; R = 20 cm) Horizontal - vertical coupling should be considered

Skew quads Solenoids

Need to incorporate soft edges