1 Meson Production Simulations X. Ding, D. B. Cline UCLA H. Kirk, J. S. Berg BNL N u F a c t 0 9 11th International Workshop on Neutrino Factories, Superbeams.

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1 Meson Production Simulations X. Ding, D. B. Cline UCLA H. Kirk, J. S. Berg BNL N u F a c t th International Workshop on Neutrino Factories, Superbeams and Beta Beams July 20-25, 2009 — IlT — Chicago

2 Outline Mercury Target Geometry and Optimized Target Parameters (Beam below Mercury Jet) Beam Initial Position, Beam/Jet Crossing Angle and Beam Path Length inside the Hg Jet (Beam below Mercury Jet) Multiple Proton Beam Entry Directions (Beam around Mercury Jet) Meson Production Summary

3 Neutrino Factory Target Concept

4 Mercury Target Geometry 1. The proton beam is below the Hg jet at z=-75cm. 2. Count all the pions and muons of positives and negatives that cross the transverse plane at z=50m. 3. For this analysis we select all pions and muons with 40MeV<KE<180MeV.

5 Optimized Target Parameters at z=-75cm 1. Beam and Jet cross only at z=-37.5cm. Beam angles also vary at different z. So the crossing angle at z=-75cm actually means the angle between beam moving direction and jet. 2. Previous Baseline: radius of 0.5cm,beam angle of 67mrad and beam/jet crossing angle of 33mrad.

6 Meson Production w/wt Optimization

7 Required Beam Initial Position at z=- 75cm to Achieve x=y=0 at z=-37.5cm)

8 Effect of Different Beam Initial Position 0.319

9 Beam/Jet Crossing Angle at z=-75cm and z=-37.5cm 8GeV, 18.55mrad at z=-75cm and 27.05mrad at z=-37.5cm

10 Beam Path Length inside the Mercury Jet Nuclear interaction length for Hg is 14.58cm

11 Multiple Proton Beam Entry Directions  8GeV,  Roll angle(Φ): Telling us what side of the jet the beam is on. (below: Φ=π, up: Φ=0, left: Φ= π/2, right: Φ=3π/2)  Clearance: Telling us the extent of proton beam away from the Hg jet at z=-75cm. x j =0, y j =3.64cm. (x 0, y 0 ) is beam initial position.

12 Multiple Proton Beam Entry Directions The Required Beam Position at z=-75cm to Keep Same Crossing Angle and 24 0 Roll Angle Apart at z=-37.5cm p0 p4 p8 p12 jet (0, 3.64) y x Previous Incident Beam at z=-75cm for optimization p1 p2 p3 p5 p6 p7 p9 p10 p11 p13 p14 4.3% higher in meson production at p11 than at p6  =0 0  =96 0  =264 0  =192 0

13 Multiple Proton Beam Entry Directions x-y plot of proton relative to jet at different z

14 Multiple Proton Beam Entry Directions

15 Multiple Proton Beam Entry Directions Clearance at z=-75cm for Same Crossing Angle and 24 0 Roll Angle apart at z=-37.5cm p0 p4 p6 p11

16 Multiple Proton Beam Entry Directions Meson 40MeV<KE<180 MeV at 50m for Same Crossing Angle and 24 0 Roll Angle apart at z=-37.5cm p11 p6 p4

17 Increasing Clearance of p4

18 Normalized Meson Production (beam below jet)

19 Normalized Mesons at 50m (beam below jet)

20 Summary Target parameters of incident beam below Hg target and KE from 2 to 100GeV are optimized. Beam angles and beam/jet crossing angles vary at low KE due to magnet field. The beam path length inside the jet is less than 2 times of the Hg interaction length at low KE. Layouts of multiple proton beam entry directions relative to the Hg jet at z=-75cm are determined to achieve the same crossing angle at z=-37.5cm. There is about 4% increase in meson production at p11 compared to p6.