MOLLER Spectrometer Update Juliette M Mammei Future Priorities

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MOLLER Spectrometer Update Juliette M. Mammei

MOLLER Spectrometer Update Juliette M. Mammei

Future Priorities (from last meeting) • Physicist input to engineering (highest priority) o Magnetic

Future Priorities (from last meeting) • Physicist input to engineering (highest priority) o Magnetic force studies o Sensitivity studies o Design of the water-cooling and electrical services o Radiation doses (brought up by companies) • Optimization of the optics o He bag/central beam pipe o Multiple magnets o No negative bend o Iron in coils • Engineering work (MIT/Bates) o Design of support structure o Vacuum vessel design Lower priority MOLLER Collaboration Meeting May 8, 9 2014 2

 • • • Forces with asymmetric coils – http: //ace. phys. virginia. edu/Moller.

• • • Forces with asymmetric coils – http: //ace. phys. virginia. edu/Moller. Spectrometer/297 – http: //ace. phys. virginia. edu/Moller. Spectrometer/298 – http: //ace. phys. virginia. edu/Moller. Spectrometer/299 – http: //ace. phys. virginia. edu/Moller. Spectrometer/300 (Jason) (Juliette) Radiation dose on coils – http: //ace. phys. virginia. edu/Moller. Spectrometer/305 – http: //ace. phys. virginia. edu/Moller. Spectrometer/306 (Tyler) (Seamus) Coil sensitivities – http: //ace. phys. virginia. edu/Moller. Spectrometer/287 – http: //ace. phys. virginia. edu/Moller. Spectrometer/308 – See slides Support Structure – See slides Vacuum vessel – See slides (Sakib, Juliette preliminary) (Tyler) Bids MOLLER Collaboration Meeting May 8, 9 2014 3

Forces Old New Coil off Forces on coil to beam left with adjacent coil

Forces Old New Coil off Forces on coil to beam left with adjacent coil off MOLLER Collaboration Meeting May 8, 9 2014 4

Coil off New Old Forces MOLLER Collaboration Meeting May 8, 9 2014 5

Coil off New Old Forces MOLLER Collaboration Meeting May 8, 9 2014 5

Sensitivity Studies • Need to consider the effects of asymmetric coils, misalignments etc. on

Sensitivity Studies • Need to consider the effects of asymmetric coils, misalignments etc. on acceptance • This could affect our manufacturing tolerances and support structure • Have created field maps for a single coil misplaced by five steps in: – -1° < pitch < 1° – -4° < roll < 4° – -1° < yaw < 1° – -2 < r < 2 cm – -10 < z < 10 cm – -5° < φ < 5° MOLLER Collaboration Meeting May 8, 9 2014 Axes in frame of single coil 6

Sensitivity Studies We’ll measure a certain rate R and asymmetry A in each septant.

Sensitivity Studies We’ll measure a certain rate R and asymmetry A in each septant. We assume the allowable uncertainty on A to be 0. 1 ppb MOLLER Collaboration Meeting May 8, 9 2014 7

MOLLER Collaboration Meeting May 8, 9 2014 8

MOLLER Collaboration Meeting May 8, 9 2014 8

Asymmetry vs. position offset

Asymmetry vs. position offset

Asymmetry vs. rotation offset

Asymmetry vs. rotation offset

Preliminary Results Z R T Roll Yaw Pitch Mean Asymmetry a (ppb) b 31.

Preliminary Results Z R T Roll Yaw Pitch Mean Asymmetry a (ppb) b 31. 75 -0. 01 ppb/cm 31. 75 0. 34 ppb/cm 31. 74 -0. 01 ppb/degree 31. 72 0. 04 ppb/degree 31. 75 0. 06 ppb/degree 31. 77 -0. 13 ppb/degree -9. 24 cm 2. 94 mm -17. 86° 2. 28° 1. 59° -0. 75° (>10 cm over magnet length) MOLLER Collaboration Meeting May 8, 9 2014 What about physical 11 constraints?

MOLLER Collaboration Meeting May 8, 9 2014 12

MOLLER Collaboration Meeting May 8, 9 2014 12

Closest approach MOLLER Collaboration Meeting May 8, 9 2014 13

Closest approach MOLLER Collaboration Meeting May 8, 9 2014 13

Summary • These results have some simulations with same random seed (statistical uncertainty is

Summary • These results have some simulations with same random seed (statistical uncertainty is not as good as it seems) – Need to re-run those simulations and redo the results – All plots vs. offset treated as linear, though some clearly are not • Very preliminary results show order ~3 mm sensitivities (not sub-mm) • Need to look at the effect of tracking algorithm with incorrect maps • What is the most important parameter – what is it that will determine the sensitivity – A background correction done incorrectly? – The mean asymmetry, as I’ve assumed here? – The mean θlab, which will go into the extraction of sin 2θW? MOLLER Collaboration Meeting May 8, 9 2014 14

Neutron shielding MOLLER Collaboration Meeting May 8, 9 2014 15

Neutron shielding MOLLER Collaboration Meeting May 8, 9 2014 15

Radiation dose MOLLER Collaboration Meeting May 8, 9 2014 16

Radiation dose MOLLER Collaboration Meeting May 8, 9 2014 16

Support Structure MOLLER Collaboration Meeting May 8, 9 2014 17

Support Structure MOLLER Collaboration Meeting May 8, 9 2014 17

Frame Design MOLLER Collaboration Meeting May 8, 9 2014 18

Frame Design MOLLER Collaboration Meeting May 8, 9 2014 18

Vacuum Chamber design MOLLER Collaboration Meeting May 8, 9 2014 19

Vacuum Chamber design MOLLER Collaboration Meeting May 8, 9 2014 19

Cut away views MOLLER Collaboration Meeting May 8, 9 2014 20

Cut away views MOLLER Collaboration Meeting May 8, 9 2014 20

Stress and deformation analysis MOLLER Collaboration Meeting May 8, 9 2014 21

Stress and deformation analysis MOLLER Collaboration Meeting May 8, 9 2014 21

Bids? MOLLER Collaboration Meeting May 8, 9 2014 22

Bids? MOLLER Collaboration Meeting May 8, 9 2014 22

Extra Slides MOLLER Collaboration Meeting May 8, 9 2014 23

Extra Slides MOLLER Collaboration Meeting May 8, 9 2014 23

Tracks in GEANT 4 for nominal field Mollers eps (Rate weighted 1 x 1

Tracks in GEANT 4 for nominal field Mollers eps (Rate weighted 1 x 1 cm 2 bins) MOLLER Collaboration Meeting May 8, 9 2014 24

MOLLER Collaboration Meeting May 8, 9 2014 25

MOLLER Collaboration Meeting May 8, 9 2014 25

MOLLER Collaboration Meeting May 8, 9 2014 26

MOLLER Collaboration Meeting May 8, 9 2014 26

MOLLER Collaboration Meeting May 8, 9 2014 27

MOLLER Collaboration Meeting May 8, 9 2014 27

Finite Target Effects θhigh, down θlow, down θhigh, up Router θlow, up Assume 5.

Finite Target Effects θhigh, down θlow, down θhigh, up Router θlow, up Assume 5. 5 mrads at upstream end of target, instead of center Rinner ztarg, up ztarg, center zcoll = 590 cm ztarg, up = ztarg, center = ztarg, down = -75 cm 0 cm 75 cm θlow = θhigh = 5. 5 mrad 17 mrad ztarg, down Rinner = 3. 658 cm Router = 11. 306 cm From center: θlow, cen = 6. 200 mrads θhigh, cen = 19. 161 mrads From downstream: θlow, down = 7. 102 mrads θhigh, down = 21. 950 mrads

Looking downstream φ= 14 0°/ +3 60 -36 °/1 4 φ= B Bx By

Looking downstream φ= 14 0°/ +3 60 -36 °/1 4 φ= B Bx By x r In this septant: φ By ~ Bφ y Bx ~ Br MOLLER Collaboration Meeting May 8, 9 2014 29

GEANT 4 • Moved to GDML geometry description • Defined hybrid and upstream toroids

GEANT 4 • Moved to GDML geometry description • Defined hybrid and upstream toroids • Parameterized in same way as the TOSCA models MOLLER Collaboration Meeting May 8, 9 2014 30

GEANT 4 - Collimators MOLLER Collaboration Meeting May 8, 9 2014 31

GEANT 4 - Collimators MOLLER Collaboration Meeting May 8, 9 2014 31

GEANT 4 – Acceptance definition MOLLER Collaboration Meeting May 8, 9 2014 32

GEANT 4 – Acceptance definition MOLLER Collaboration Meeting May 8, 9 2014 32