MOLLER Spectrometer Update Juliette M. Mammei. O UTLINE The Physics – Search for physics beyond the Standard Model – Interference of Z boson with single.

MOLLER Spectrometer Update Juliette M. Mammei

O UTLINE The Physics – Search for physics beyond the Standard Model – Interference of Z boson with single photon in Møller scattering – Measure the weak charge of the electron and sin 2 θ W – Sensitivity comparable to the two high energy collider measurements The Experiment – High rate, small backgrounds – 150 GHz, 8% backgrounds – Novel toroid design, with multiple current returns – Full azimuthal acceptance, scattering angles from 5.5-19 mrads, 2.5-8.5 GeV – 150cm (5 kW) target, detectors 28m downstream Magnet Advisory Group Meeting October 14, 2013 2

3 T HE P HYSICS e-

Erler, Kurylov, Ramsey-Musolf M EASUREMENT OF sin 2 θ W Magnet Advisory Group Meeting October 14, 2013 4 MOLLER Z-pole MOLLER Erler

T HE E XPERIMENT Magnet Advisory Group Meeting October 14, 2013 5 Detector Array Roman Pots (for tracking detectors) Scattering Chamber Target Hybrid Torus Upstream Torus Incoming Beam 28 m Collimators

e- Magnet Advisory Group Meeting October 14, 20136 Forward Backward ForwardBackward COM Frame e- Lab Frame e- Any odd number of coils will work 100% Azimuthal Acceptance

(Rate weighted 1x1cm 2 bins) Tracks in GEANT4 Magnet Advisory Group Meeting October 14, 2013 7 Mollers eps

Magnet Advisory Group Meeting October 14, 2013 8

I.Large phase space of possible changes A.Field (strength, coil position and profile) B.Collimator location, orientation, size C.Choice of Primary collimator D.Detector location, orientation, size II.Large phase space of relevant properties A.Moller rate and asymmetry B.Elastic ep rate and asymmetry C.Inelastic rate and asymmetry D.Transverse asymmetry E.Neutral/other background rates/asymmetries F.Ability to measure backgrounds (the uncertainty is what’s important) 1.Separation between Moller and ep peaks 2.Profile of inelastics in the various regions 3.Degree of cancellation of transverse (F/B rate, detector symmetry) 4.Time to measure asymmetry of backgrounds (not just rate) G.Beam Properties (location of primary collimator) Magnet Advisory Group Meeting October 14, 2013 9 Large Phase Space for Design

Conductor layout Magnet Advisory Group Meeting October 14, 2013 10 Spectrometer Design Optics tweaks Optimize collimators Ideal current distribution Add’l input from us Engineering design Fill azimuth at low radius, far downstream Half azimuth at upstream end No interferences Minimum bends 5x OD of wire Minimum 5x ms radius Double-pancake design Clearance for insulation, supports Fill azimuth at low radius, far downstream Half azimuth at upstream end No interferences Minimum bends 5x OD of wire Minimum 5x ms radius Double-pancake design Clearance for insulation, supports Return to proposal optics or better Optimize Moller peak Minimize ep backgrounds Symmetric front/back scattered mollers (transverse cancellation) Different W distributions in different sectors (inelastics, w/ simulation) Return to proposal optics or better Optimize Moller peak Minimize ep backgrounds Symmetric front/back scattered mollers (transverse cancellation) Different W distributions in different sectors (inelastics, w/ simulation) Force calculations Symmetric coils asymmetric placement of coils Sensitivity studies Materials Coils in vacuum or not Force calculations Symmetric coils asymmetric placement of coils Sensitivity studies Materials Coils in vacuum or not Water-cooling connections Support structure Electrical connections Power supplies Water-cooling connections Support structure Electrical connections Power supplies Optimize Moller peak Eliminate 1-bounce photons Minimize ep backgrounds Symmetric front/back scattered mollers (transverse cancellation) Different W distributions in different sectors (inelastics, w/ simulation) Optimize Moller peak Eliminate 1-bounce photons Minimize ep backgrounds Symmetric front/back scattered mollers (transverse cancellation) Different W distributions in different sectors (inelastics, w/ simulation)

Spectrometer Meetings Director’s Review – January 2010 Advisory Group Meeting – August 2010 Collaboration Meeting – December 2010 Supergroup Meeting – June 2012 Collaboration Meeting – September 2012 Collaboration Meeting – June 2013 Advisory Group Meeting – October 2013 Magnet Advisory Group Meeting October 14, 2013 11

Suggestions of Advisory Group larger conductor and hole (→1550 A/cm 2 ) wanted a better representation of the fields, space constraints, etc., wanted Br, Bphi larger vacuum chamber instead of petals Wish list: – Get rid of negative bend – Use iron to reduce current density Magnet Advisory Group Meeting October 14, 2013 12 No showstoppers!

Work since original proposal First Engineering Review o Verified the proposal map in TOSCA o Created an actual conductor layout with acceptable optics Since the engineering review o New conductor layout, take into account keep-out zones o Water cooling more feasible o Preliminary look at the magnetic forces Interfacing with engineers o JLab engineers estimate that pressure head is not an issue o New conductor layout with larger water cooling hole o Coil carrier and support structure design o Working toward a “cost-able” design for DOE review soon Magnet Advisory Group Meeting October 14, 2013 13 Purchase of a new machine and TOSCA license for use at University of Manitoba Purchase of a new machine and TOSCA license for use at University of Manitoba

Proposal Model to TOSCA model Magnet Advisory Group Meeting October 14, 2013 Home built code using a Biot-Savart calculation Optimized the amount of current in various segments (final design had 4 current returns) Integrated along lines of current, without taking into account finite conductor size 14 “Coils-only” Biot-Savart calculation Verified proposal model Created a first version with actual coil layout Created second version with larger water cooling hole and nicer profile; obeyed keep-out zones

Concept 2 – Post-review Magnet Advisory Group Meeting October 14, 2013 15 Current density not an issue, but affects cooling  Larger conductor o Larger water-cooling hole o Fewer connections o Less chance of developing a plug  New layout o Use single power supply o Keep-out zones/tolerances o Need to think about supports o Study magnetic forces  Continued simulation effort o Consider sensitivities o Re-design collimation o Power of incident radiation

Layout 16 1AR1AL 1BL1BR 2L 3L 2R 3R 4C4R4L 1AR1AL 1BL1BR 2L 3L 2R 3R Magnet Advisory Group Meeting October 14, 2013 1AR1AL 1BL1BR 2L2R 1AR1AL 1BL1BR

Upstream Torus Magnet Advisory Group Meeting October 14, 2013 17

z coll =590cm z targ,up =-75cm z targ,center =0cm z targ,down =75cm θ low =5.5mrad θ high =17mrad R inner =3.658cm R outer =11.306cm From center:From downstream: θ low,cen =6.200mradsθ low,down =7.102mrads θ high,cen =19.161mradsθ high,down =21.950mrads Finite Target Effects R inner R outer z targ,down z targ,up z targ,center θ low,up θ low,down θ high,up θ high,down Assume 5.5 mrads at upstream end of target, instead of center

Looking downstream x y φ=-360°/14 φ=+360°/14 ͢ B r φ In this septant: B y ~ B φ B x ~ B r ByBy BxBx ByBy BxBx 19 Magnet Advisory Group Meeting October 14, 2013

up (z0 =-75 cm) 5.5 to 15 mrads middle (z0 =0 cm) 6.0 to 17 mrads down (z0 =75 cm) 6.5 to 19 mrads All phi values Tracks colored by theta from purple to red (low to high) Tracks in TOSCA Not using the mesh - “coils only” calculation fast enough on my machine - Actual layout much slower – use blocky version or improve mesh Magnet Advisory Group Meeting October 14, 2013 20

BMOD z=1375 cm Magnet Advisory Group Meeting October 14, 2013 21 Field representations

Radial plot, middle of open sector BMOD Magnet Advisory Group Meeting October 14, 2013 22 Z=1375, φ = 0

Radial plot, edge of open sector BMOD Magnet Advisory Group Meeting October 14, 2013 23

Around Azimuth Center of open sector Z=1375, r = 13.5 cm BMOD Magnet Advisory Group Meeting October 14, 2013 24

up (z0 =-75 cm) 5.5 to 15 mrads middle (z0 =0 cm) 6.0 to 17 mrads down (z0 =75 cm) 6.5 to 19 mrads phi=0 only Tracks colored by theta from purple to red (low to high) Magnet Advisory Group Meeting October 14, 2013 25

up (z0 =-75 cm) 5.5 to 15 mrads middle (z0 =0 cm) 6.0 to 17 mrads down (z0 =75 cm) 6.5 to 19 mrads phi=0 only, near magnet Tracks colored by theta from purple to red (low to high) Magnet Advisory Group Meeting October 14, 2013 26

up (z0 =-75 cm) 5.5 to 15 mrads middle (z0 =0 cm) 6.0 to 17 mrads down (z0 =75 cm) 6.5 to 19 mrads phi = 0, Mollers only 3.0 Tracks colored by theta from purple to red (low to high) Magnet Advisory Group Meeting October 14, 2013 27

up (z0 =-75 cm) 5.5 to 15 mrads middle (z0 =0 cm) 6.0 to 17 mrads down (z0 =75 cm) 6.5 to 19 mrads phi=0 only, near magnet, mollers only 3.0 Tracks colored by theta from purple to red (low to high) Magnet Advisory Group Meeting October 14, 2013 28

up (z0 =-75 cm) 5.5 and 15 mrads middle (z0 =0 cm) 6.0 and 17 mrads down (z0 =75 cm) 6.5 and 19 mrads phi=0 only green – eps blue - mollers

up (z0 =-75 cm) 5.5 and 15 mrads middle (z0 =0 cm) 6.0 and 17 mrads down (z0 =75 cm) 6.5 and 19 mrads phi=0 only, near magnet 3.0 green – eps blue - mollers Magnet Advisory Group Meeting October 14, 2013 30

Magnet Advisory Group Meeting October 14, 2013 Tweaking the Optics 31 0 (1.0)8 (2.11)

2.8 (blue) ee 3.0 (red) 2.0 (green) Tracks from middle of target (z=0), phi =0 only 6.0 and 17 mrads ep Magnet Advisory Group Meeting October 14, 2013 32

2.8 (blue) ee 3.0 (red) 2.0 (green) ep Tracks from center of target, phi =0 only 6.0 and 17 mrads Magnet Advisory Group Meeting October 14, 2013 33

3.0 (default) 2.8 up (z0 =-75 cm) 5.5 to 15 mrads middle (z0 =0 cm) 6.0 to 17 mrads down (z0 =75 cm) 6.5 to 19 mrads ep ee ep ee Tracks colored by theta from purple to red (low to high) Magnet Advisory Group Meeting October 14, 2013 34

GEANT4 Magnet Advisory Group Meeting October 14, 2013 35 Moved to GDML geometry description Defined hybrid and upstream toroids Parameterized in same way as the TOSCA models

GEANT4 - Collimators Magnet Advisory Group Meeting October 14, 2013 36

GEANT4 – Acceptance definition Magnet Advisory Group Meeting October 14, 2013 37

Collimator Optimization Magnet Advisory Group Meeting October 14, 2013 38

Comparison of GEANT4 Simulations Proposal

Comparison of GEANT4 Simulations TOSCA version Magnet Advisory Group Meeting October 14, 2013 41

Magnet Advisory Group Meeting October 14, 2013 42 2.6

Magnet Advisory Group Meeting October 14, 2013 43 Current Version of the Hybrid and Upstream 43 Default svn

Magnetic Forces Use TOSCA to calculate magnetic forces on coils Have calculated the centering force on coil: ~3000lbs (compare to Qweak: 28000 lbs) Need to look at effects of asymmetric placement of coils Could affect the manufacturing tolerances Magnet Advisory Group Meeting October 14, 2013 44

Magnet Advisory Group Meeting October 14, 2013 45 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° Simulations need to be run and analyzed

Ongoing/Future Work Ongoing/Future work o Optimization of the optics o Magnetic force studies o Sensitivity studies o Collimator optimization o Design of the water-cooling and supports o Design of electrical connections o Look at optics for 3 coils Magnet Advisory Group Meeting October 14, 2013 46

Extra Slides Magnet Advisory Group Meeting October 14, 2013 47

Sector Orientation Magnet Advisory Group Meeting October 14, 2013 48

Collimator Study Magnet Advisory Group Meeting October 14, 2013 49 see elog 200elog 200 Look at focus for different Sectors Parts of target Useful for optics tweaks and collimator optimization Ideally the strips would be vertical in these (actually theta vs. radius) plots

Water-cooling and supports Magnet Advisory Group Meeting October 14, 2013 Verified by MIT engineers – cooling could be accomplished in concept 2 with 4 turns per loop Still 38 connections per coil! 50 Suggestion from engineering review: Put the magnets inside the vacuum volume

GEANT4 – Upstream Torus Magnet Advisory Group Meeting October 14, 2013 54

GEANT4 – Hybrid Torus Magnet Advisory Group Meeting October 14, 2013 55

GEANT4 Magnet Advisory Group Meeting October 14, 2013 56

Direct Comparison of Fields Magnet Advisory Group Meeting October 14, 2013 Complicated field because of multiple current returns The average total field in a sector in bins of R vs. z The difference of the total field in a sector in bins of R vs. z for the TOSCA version of the proposal and the original proposal model 57

Magnet Advisory Group Meeting October 14, 2013 Comparison of field values Red – proposal model Black – TOSCA model By (left) or Bx (right) vs. z in 5° bins in phi -20°— -15° -25°— -20° -5°— 0° -20°— -15° -5°— 0° -15°— -10° -10°— -5° -15°— -10° -10°— -5° 58

Proposal Model Magnet Advisory Group Meeting October 14, 2013 OD (cm) A cond (cm 2 ) Total # Wires Current (A) Current per wire J (A/cm 2 ) XYZAXYZA Proposal--- 7748106271685929160---1100 0.41150.124840548614679891078517176291602001600 0.46200.156832447012077761069217010291602431550 0.51890.19782636569480661116817372291603101568 0.58270.24762028407676801075215360291843841551 59

Actual Conductor Layout Magnet Advisory Group Meeting October 14, 2013 60

Choose constraints Choose (standard) conductor size/layout minimizes current density Try to use “double pancakes”; as flat as possible Minimum bend radius 5x conductor OD Fit within radial, angular acceptances (360°/7 and <360°/14 at larger radius) Total current in each inner “cylinder” same as proposal model Take into account water cooling hole, insulation Need to consider epoxy backfill and aluminum plates/ other supports?  Radial extent depends on upstream torus and upstream parts of hybrid!! Magnet Advisory Group Meeting October 14, 2013 61

Conductor Size Trade-off between more insulation for smaller conductor and losing space at the “edges” with larger conductor Also need to fit all the conductor in a particular radius at a given z location  Much bigger conductors have even higher current densities because of “edge” effects Need to “fill” the available space at low radius

Actual conductor layout Magnet Advisory Group Meeting October 14, 2013 65

Magnet Advisory Group Meeting October 14, 2013 Actual conductor layout 66

Blocky Model superimposed Magnet Advisory Group Meeting October 14, 2013 67

Keep Out Zones Magnet Advisory Group Meeting October 14, 2013 ±360°/28 68 cones are defined using:  nothing w/in 5σ of the multiple scattering radius  + 1/4" each for Al support and W shielding ±360°/14

Keep Out Zones/Concept 2 Magnet Advisory Group Meeting October 14, 2013 71 ±360°/28 ±360°/14

Interferences Magnet Advisory Group Meeting October 14, 2013 72

Interferences Magnet Advisory Group Meeting October 14, 2013 73

1 (2.0) Magnet Advisory Group Meeting October 14, 2013 74 8 (2.11) 7 (2.10) 6 (2.9)5 (2.8) 4 (2.7) 3 (2.6) 2 (2.5)1 (2.0) Tweaking the Optics

1 (2.0) Magnet Advisory Group Meeting October 14, 2013 75 8 (2.11) 7 (2.10) 6 (2.9)5 (2.8) 4 (2.7) 3 (2.6) 2 (2.5)1 (2.0) Tweaking the Optics

1 (2.0) Magnet Advisory Group Meeting October 14, 2013 76 8 (2.11) 7 (2.10) 6 (2.9)5 (2.8) 4 (2.7) 3 (2.6) 2 (2.5) Tweaking the Optics

1 (2.0) Magnet Advisory Group Meeting October 14, 2013 77 8 (2.11) 7 (2.10) 6 (2.9)5 (2.8) 4 (2.7) 3 (2.6) Tweaking the Optics

1 (2.0) Magnet Advisory Group Meeting October 14, 2013 78 8 (2.11) 7 (2.10) 6 (2.9)5 (2.8) 4 (2.7) Tweaking the Optics

1 (2.0) Magnet Advisory Group Meeting October 14, 2013 79 8 (2.11) 7 (2.10) 6 (2.9)5 (2.8) Tweaking the Optics

1 (2.0) Magnet Advisory Group Meeting October 14, 2013 80 8 (2.11) 7 (2.10) 6 (2.9) Tweaking the Optics

1 (2.0) Magnet Advisory Group Meeting October 14, 2013 81 8 (2.11) 7 (2.10) Tweaking the Optics

1 (2.0) Magnet Advisory Group Meeting October 14, 2013 82 8 (2.11) Tweaking the Optics

1 (2.0) Magnet Advisory Group Meeting October 14, 2013 83 Tweaking the Optics

4.1 middle only (z0 =0 cm), 6.0, 11.5 and 17, phi=0 only blue – eps red - mollers Magnet Advisory Group Meeting October 14, 2013 84

4.2 middle only (z0 =0 cm), 6.0, 11.5 and 17, phi=0 only blue – eps green - mollers Magnet Advisory Group Meeting October 14, 2013 85

4.2 4.1 middle (z0 =0 cm) 6.0 to 17 mrads Tracks colored by theta from purple to red (low to high) Magnet Advisory Group Meeting October 14, 2013 86

4.2 4.1 3.0 4.2 middle (z0 =0 cm) 6.0 to 17 mrads Tracks colored by theta from purple to red (low to high) Magnet Advisory Group Meeting October 14, 2013 87

4.3b middle only (z0 =0 cm), 6.0, 11.5 and 17, phi=0 only blue – eps green - mollers Magnet Advisory Group Meeting October 14, 2013 88

4.3b 3.0 Magnet Advisory Group Meeting October 14, 2013 89

Meshed with no iron for comparison Used Willy’s conceptual design for iron pieces Not optimized in any way Used thin and thick pieces Compared fields (BMOD and BR) Compared tracks for no iron and thick iron Note: op3 file names are: no_iron_in_coils_test_ver2.op3 (smaller mesh size) iron_in_coils_ver3.op3 (thin) iron_in_coils_ver4.op3 (thick) Outline

No iron, coils only BMOD z=1375 cm Magnet Advisory Group Meeting October 14, 2013 91

No iron w/ mesh BMOD z=1375 cm Magnet Advisory Group Meeting October 14, 2013 92

Field on a line, middle of open sector BMOD z=1375 cm, y= 0 cm, 0 < x < -40 cm With coils only With mesh BMOD Magnet Advisory Group Meeting October 14, 2013 93

Model body in mesh Magnet Advisory Group Meeting October 14, 2013 94

thin iron thick iron Iron design Magnet Advisory Group Meeting October 14, 2013 95

thick iron 1 m long, section of tube from 0.5 to 5.5 cm radius Opening angle, thin: 5 degrees Opening angle, thick: 20 degrees Placed radially from 5 – 20 cm between 1325 and 1425 cm in z Iron design Magnet Advisory Group Meeting October 14, 2013 96

Thin Iron w/ mesh BMOD z=1375 cm Magnet Advisory Group Meeting October 14, 2013 97

Thick Iron w/ mesh BMOD z=1375 cm Magnet Advisory Group Meeting October 14, 2013 98

Giant blocks of iron BMOD z=1375 cm Magnet Advisory Group Meeting October 14, 2013 99

No iron w/ mesh BMOD z=1375 cm Magnet Advisory Group Meeting October 14, 2013 100

Thin Iron w/ mesh BMOD z=1375 cm Magnet Advisory Group Meeting October 14, 2013 101

Thick Iron w/ mesh BMOD z=1375 cm Magnet Advisory Group Meeting October 14, 2013 102

Giant blocks of iron BMOD z=1375 cm Magnet Advisory Group Meeting October 14, 2013 103

Vector plots BMOD Magnet Advisory Group Meeting October 14, 2013 104

Middle of open sector With thin iron With no iron BMOD Magnet Advisory Group Meeting October 14, 2013 105

Middle of open sector With thin iron With thick iron With no iron BMOD Magnet Advisory Group Meeting October 14, 2013 106

Edge of open sector With thin iron With no iron BMOD Magnet Advisory Group Meeting October 14, 2013 107

Edge of open sector With thin iron With thick iron With no iron BMOD Magnet Advisory Group Meeting October 14, 2013 108

With thin iron With no iron Center of open sector Z=1375, r = 13.5 cm BMOD Magnet Advisory Group Meeting October 14, 2013 109

With thin iron With no iron Z=1375, r = 13.5 cm BR Magnet Advisory Group Meeting October 14, 2013 110

With thick iron With thin iron Z=1375, r = 13.5 cm BMOD Magnet Advisory Group Meeting October 14, 2013 111

With thick iron With thin iron Z=1375, r = 13.5 cm BR Magnet Advisory Group Meeting October 14, 2013 112

With no iron With thick iron Z=1375, r = 16.0 cm BMOD Magnet Advisory Group Meeting October 14, 2013 113

With “giant” iron With thick iron Z=1375, r = 16.0 cm BMOD Magnet Advisory Group Meeting October 14, 2013 114

With thick iron With no iron Magnet Advisory Group Meeting October 14, 2013 115

With no iron With giant iron Magnet Advisory Group Meeting October 14, 2013 116

With no iron With giant iron, BFIL 90% Magnet Advisory Group Meeting October 14, 2013 117

With no iron With giant iron, BFIL 80% Magnet Advisory Group Meeting October 14, 2013 118

Summary Magnet Advisory Group Meeting October 14, 2013 120

MOLLER Spectrometer Update Juliette M. Mammei. O UTLINE The Physics – Search for physics beyond the Standard Model – Interference of Z boson with single.

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MOLLER Spectrometer Update Juliette M. Mammei. O UTLINE The Physics – Search for physics beyond the Standard Model – Interference of Z boson with single.

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Presentation on theme: "MOLLER Spectrometer Update Juliette M. Mammei. O UTLINE The Physics – Search for physics beyond the Standard Model – Interference of Z boson with single."— Presentation transcript:

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