MOLLER Spectrometer Update

65
MOLLER Spectrometer Update Juliette M. Mammei

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MOLLER Spectrometer Update. Juliette M. Mammei. Large Phase Space for Design. Large phase space of possible changes Field (strength, coil position and profile) Collimator location, orientation, size Choice of Primary collimator Detector location, orientation, size - PowerPoint PPT Presentation

Transcript of MOLLER Spectrometer Update

Page 1: MOLLER Spectrometer Update

MOLLER Spectrometer Update

Juliette M. Mammei

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I. Large phase space of possible changesA. Field (strength, coil position and profile)B. Collimator location, orientation, sizeC. Choice of Primary collimatorD. Detector location, orientation, size

II. Large phase space of relevant propertiesA. Moller rate and asymmetryB. Elastic ep rate and asymmetryC. Inelastic rate and asymmetryD. Transverse asymmetryE. Neutral/other background rates/asymmetriesF. Ability to measure backgrounds (the uncertainty is what’s important)

1. Separation between Moller and ep peaks2. Profile of inelastics in the various regions3. 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)

Large Phase Space for Design

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Conductor layout

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

• 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

• 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)

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Work since the proposal• First Engineering Review

o Verified the proposal map in TOSCAo Created an actual conductor layout with acceptable optics

• Since the engineering reviewo New conductor layout, take into account keep-out zoneso Water cooling more feasibleo Preliminary look at the magnetic forces

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Work since the collaboration meeting• Interfacing with engineers

o JLab engineers estimate that pressure head is not an issueo New conductor layout with larger water cooling hole “approved”o MIT engineers recalculate Robin’s initial water cooling calculationso Determine what more work is needed on our side

• Ongoing/Future worko Optimization of the opticso Magnetic force studieso Sensitivity studieso Collimator optimizationo Design of the water-cooling and supportso Design of electrical connectionso Look at optics for 3 coils

Purchase of a new machine and TOSCA license for use at University of Manitoba

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Not using the mesh - “coils only” calculation fast enough on my machine

- Actual layout much slower – use blocky version or improve mesh

Mollers (blue)eps (green)

Mollers, no collimation(red)Mollers, accepted (blue)eps, accepted (green)

Tracks in TOSCA

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Proposal Model to TOSCA modelHome 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

“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

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Concept 2 – Post-review4C 4R4L

1AR1AL

1BL 1BR

2L

3L

2R

3R

Current density not an issue, but affects cooling

Larger conductoro Larger water-cooling hole o Fewer connectionso Less chance of developing a plug

New layouto Use single power supplyo Keep-out zones/toleranceso Need to think about supportso Study magnetic forces

Continued simulation efforto Consider sensitivitieso Re-design collimationo Power of incident radiation

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Layout

1AR1AL

1BL 1BR

2L

3L

2R

3R4C 4R4L

1AR1AL

1BL 1BR

2L

3L

2R

3R4C 4R4L

1AR1AL

1BL 1BR

2L

3L

2R

3R

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Upstream Torus

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Sector Orientation

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1 (2.0)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

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Tweaking the Optics

0 1 2 3 4 5 6 7 8 90

5

10

15

20

25Width of radial focus

"Good" angles"All" angles

Version

Wid

th (c

m)

0 1 2 3 4 5 6 7 8 90

5

10

15

20

25Separation of ends

"Good" angles"All" angles

Version

Sepa

ratio

n (c

m)

0 (1.0) 8 (2.11)

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Comparison of GEANT4 Simulations

Proposal

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Comparison of GEANT4 Simulations

TOSCA version

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2.6

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Current Version of the Hybrid and Upstream

17

Default svn

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Tweaking the OpticsAssume: 6.0-15.4 mrads from upstream end of target

Finite target effects: We’ll accept some high angles from further downstream for which we won’t have full azimuthal acceptance

Primary concern: focus the “good” high angles

Blue: AllRed: “Good”Green: “Extreme”

Blue: low anglesGreen: mid anglesRed: high angles

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Collimator Study

see elog 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

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Rate Comparison*

Field Map Moller(GHz)

Elastic ep (GHz)

Inelastic ep (GHz)

Bkgd. Fraction (%)

Proposal 133 12 0.4 9

Actual 0 (1.0) 162 18 0.6 10

Actual 3 (2.6) 140 13 0.6 10

svn 147 16 0.6 11

*Assuming 75µA

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Photons

see elog 199

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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

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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

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GEANT4• Moved to GDML geometry description• Defined hybrid and upstream toroids• Parameterized in same way as the TOSCA models

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GEANT4 – Upstream Torus

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GEANT4 – Hybrid Torus

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GEANT4

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Magnet StatsProperty Moller

Concept 1 Upstream MollerConcept 2 Qweak

Field Integral (Tm) 1.4 0.15 1.1 0.89

Total Power (kW) 820 40 765 1340

Current per wire (A) 243 298 384 9500

Voltage per coil (V) 480 19 285 18

Current Density (A/cm2) 1600 1200 1550 500Wire cross section

(ID: water hole) (in) 0.182x0.182

(0.101)0.229x0.229

(0.128)0.229x0.229

(0.128)2.3x1.5 (0.8)

Weight of a coil (lbs) 556 44 555 7600

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Extra Slides

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Water-cooling and supportsVerified by MIT engineers – cooling could be accomplished in concept 2 with 4 turns per loop Still 38 connections per coil!

Suggestion from engineering review: Put the magnets inside the vacuum volume

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GEANT4 - Collimators

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GEANT4 – Acceptance definition

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zcoll = 590cm

ztarg,up = -75cmztarg,center = 0cmztarg,down = 75cm

θlow = 5.5mradθhigh = 17mrad

Rinner = 3.658cmRouter = 11.306cm

From center: From downstream:

θlow,cen = 6.200mrads θlow,down = 7.102mradsθhigh,cen = 19.161mrads θhigh,down = 21.950mrads

Finite Target Effects

Rinner

Router

ztarg,downztarg,up ztarg,center

θlow,up

θlow,down

θhigh,up

θhigh,down

Assume 5.5 mrads at upstream end of target, instead of center

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Direct Comparison of FieldsComplicated 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

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Field Components

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Field Components

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Comparison of field valuesRed – proposal modelBlack – TOSCA model By (left) or Bx (right) vs. z in 5° bins in phi

-20°— -15°

-25°— -20° -25°— -20°

-5°— 0°

-20°— -15°

-5°— 0°

-15°— -10°

-10°— -5°

-15°— -10°

-10°— -5°

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Proposal Model

OD (cm)

Acond (cm2)

Total # Wires Current (A) Current per wire J (A/cm2)

X Y Z A X Y Z A

Proposal --- --- --- --- 7748 10627 16859 29160 --- 1100

0.4115 0.1248 40 54 86 146 7989 10785 17176 29160 200 1600

0.4620 0.1568 32 44 70 120 7776 10692 17010 29160 243 1550

0.5189 0.1978 26 36 56 94 8066 11168 17372 29160 310 1568

0.5827 0.2476 20 28 40 76 7680 10752 15360 29184 384 1551

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Actual Conductor Layout

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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!!

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Conductor SizeTrade-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 particularradius 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

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Conductor SizeTrade-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 particularradius at a given z location

Much bigger conductors have even higher current densities because of “edge” effects

1LA 1C 1RA

1RB1LB

2LA

3LA

2RA

3RA

2RB2LB

3LB 3RB 1RC1LC

2C

3C

Need to “fill” the available space at low radius

Page 44: MOLLER Spectrometer Update

Conductor SizeTrade-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 particularradius at a given z location

Much bigger conductors have even higher current densities because of “edge” effects

1LA 1C 1RA

1RB1LB

2LA

3LA

2RA

3RA

2RB2LB

3LB 3RB 1RC1LC

2C

3C

Need to “fill” the available space at low radius

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Actual conductor layout

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Actual conductor layout

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Blocky Model superimposed

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Keep Out Zones±360°/28

cones are defined using:

nothing w/in 5σ of the multiple scattering radius + 1/4" each for Al support and W shielding

±360°/14

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Keep Out Zones±360°/28

cones are defined using:

nothing w/in 5σ of the multiple scattering radius + 1/4" each for Al support and W shielding

±360°/14

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Keep Out Zones±360°/28

cones are defined using:

nothing w/in 5σ of the multiple scattering radius + 1/4" each for Al support and W shielding

±360°/14

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Keep Out Zones/Concept 2±360°/28

±360°/14

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Interferences

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Interferences

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1 (2.0)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

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1 (2.0)8 (2.11)7 (2.10)6 (2.9)5 (2.8)4 (2.7)3 (2.6)2 (2.5)

Tweaking the Optics

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1 (2.0)8 (2.11)7 (2.10)6 (2.9)5 (2.8)4 (2.7)3 (2.6)

Tweaking the Optics

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1 (2.0)8 (2.11)7 (2.10)6 (2.9)5 (2.8)4 (2.7)

Tweaking the Optics

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1 (2.0)8 (2.11)7 (2.10)6 (2.9)5 (2.8)

Tweaking the Optics

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1 (2.0)8 (2.11)7 (2.10)6 (2.9)

Tweaking the Optics

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1 (2.0)8 (2.11)7 (2.10)

Tweaking the Optics

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1 (2.0)8 (2.11)

Tweaking the Optics

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1 (2.0)

Tweaking the Optics

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Comparison of GEANT4 Simulations

TOSCA version

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2.11

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3.0