FNAL Optimization Update Laura Fields 11 February 2015 1 Outline - - PowerPoint PPT Presentation

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FNAL Optimization Update Laura Fields 11 February 2015 1 Outline - - PowerPoint PPT Presentation

FNAL Optimization Update Laura Fields 11 February 2015 1 Outline Results of three optimizations Cylindrical Target Parabolic Horns Reduced engineering constraints Further study of 3-horn optimized design w/ NuMI target


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11 February 2015

FNAL Optimization Update

Laura Fields

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Outline

✤ Results of three optimizations ✤ Cylindrical Target ✤ Parabolic Horns ✤ Reduced engineering constraints ✤ Further study of 3-horn optimized design w/ NuMI target ✤ Effect of endcap material ✤ Beam simulation news

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✤ Last time I showed early results of a cylindrical target optimization:

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Best fitness: 1.98 Compared to 1.47 reference and 1.97 (NuMI-style target, optimized)

Cylindrical Target Optimization

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✤ After running a bit more (and having a lot of grid failures):

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Best fitness: 2.01 Compared to 1.47 reference and 1.97 (NuMI-style target, optimized)

Cylindrical Target Optimization

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✤ NuMI-style target optimization, for comparison:

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Best fitness: 1.97 Compared to 1.47 reference

NuMI-style Target Optimization

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Cylindrical Target Optimization Results

Parameter Lower Limit Upper Limit Unit Horn A: LA 1000 4500 mm 3717 Horn A: F1A 1 99 % 51 Horn A: r1A 20 50 mm 33 Horn A: r2A 20 200 mm 147 Horn A rOCA 200 650 mm 630 Horn B: LB 2000 4500 mm 2551 Horn B: F1B 100 % 37 Horn B: F2B 100 % 12 Horn B: F3B 100 % 2 Horn B: F4B 100 % 16 Horn B: R1B 50 200 mm 186 Horn B: R2B 20 50 mm 47 Horn B: R3B 50 200 mm 179 Horn B: ROCB 200 650 mm 633 HornB: Z position 2000 17000 mm 5453 Horn C: LC 2000 4500 mm 2694 Horn C: F1C 100 % 30 Horn C: F2C 100 % 21 Horn C: F3C 100 % 2 Horn C: F4C 100 % 9 Horn C: R1C 50 550 mm 388 Horn C: R2C 20 50 mm 26 Horn C: R3C 50 550 mm 306 Horn C: ROCC 550 650 mm 620 Horn C: Z Position 4000 19000 mm 17836 Target Length 0.5 2.0 m 1.98 Beam spot size 1.6 2.5 mm 2.1 Target Radius 9 15 mm 7.8 Proton Energy 60 120 GeV 108 Horn Current 150 300 kA 270

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Parameter Lower Lim Upper Lim Unit Final Optimum Horn A: LA 1000 4500 mm 2815 Horn A: F1A 1 99 % 65 Horn A: r1A 20 50 mm 34 Horn A: r2A 20 200 mm 145 Horn A rOCA 200 650 mm 630 Horn B: LB 2000 4500 mm 3229 Horn B: F1B 100 % 20 Horn B: F2B 100 % 21 Horn B: F3B 100 % 1 Horn B: F4B 100 % 22 Horn B: R1B 50 200 mm 191 Horn B: R2B 20 50 mm 47 Horn B: R3B 50 200 mm 204 Horn B: ROCB 200 650 mm 630 HornB: Z position 2000 17000 mm 3637 Horn C: LC 2000 4500 mm 2816 Horn C: F1C 100 % 36 Horn C: F2C 100 % 16 Horn C: F3C 100 % 3 Horn C: F4C 100 % 5 Horn C: R1C 50 550 mm 398 Horn C: R2C 20 50 mm 45 Horn C: R3C 50 550 mm 310 Horn C: ROCC 550 650 mm 643 Horn C: Z Position 4000 19000 mm 17478 Target Length 0.5 2.0 m 2.00 Beam spot size 1.6 2.5 mm 1.62 Target Fin Width 9 15 mm 13.4 Proton Energy 60 120 GeV 62 Horn Current 150 300 kA 296

Final Optimum Horn A Horn B Horn C

NuMI-Style Target Optimization Results

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✤ Some conclusions ✤ Optimization run with cylindrical target gives slightly better results than

NuMI-style

✤ Difference in flux is small, and consistent with what I’ve seen before when

I place cylindrical and fin-style target in the same focusing system

✤ One substantial difference between the two optimizations ✤ NuMI-style target is limited by size of target can; cylindrical target is not

constrained and can grow larger

✤ Optimized focusing system is very similar for two options. Primary

differences (other than target):

✤ Cylindrical target prefers lower horn current and higher proton energy

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Cylindrical Target Optimization Conclusions

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✤ Last time I also showed early results from a parabolic horn

  • ptimization

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Best fitness: 1.85 Compared to 1.47 reference and 1.97 (NuMI-style target, conical horns)

Numi-Style Target w/ Parabolic Horns

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✤ More recent results:

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Best fitness: 1.89 Compared to 1.47 reference and 1.97 (NuMI-style target, conical horns)

Numi-Style Target w/ Parabolic Horns

It doesn’t look like this is going to do better than the conical horn option

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✤ I’m also running an optimization with relaxed engineering

constraints — seems to be converging very slowly

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Best fitness: 1.90 Compared to 1.47 reference and 1.97 (NuMI-style target w/ engineering constraints, final optimum)

Numi-Style Target w/ Relaxed Engineering Constraints

Allows longer target, longer target chase, larger conductor radii

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Optimization Next Steps

✤ To do ✤ Debug grid failures which may be affecting speed

  • f optimization

✤ Run an optimization with more realistic IC

thicknesses

✤ Tighter constraint on OD radius (due to nickel-

plating limitations)

✤ Study optimized fluxes with updated sensitivity

calculations

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✤ In past talks, when I’ve described the 3-horn optimized system

(NuMI-style target), people have been curious about the importance

  • f the “pinch” in Horn C

Further Study of 3 Horn Option w/ NuMI Target

✤ The neck radius was constrained to be small < 50 mm, primarily to

help the optimization converge a few months ago when separate problems were causing it not to converge

✤ In future runs, I can relax this constraint. But to understand it’s

impact, I did a scan of this parameter with a wider range than was used in the optimization

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Further Study of 3 Horn Option w/ NuMI Target

CP sensitivity is fairly flat vs. horn C neck radius Some small loss in sensitivity above r = ~120 mm

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Effect of Endcap Material

✤ For Horns A and B, I use 2 mm inner conductor and

endcap thicknesses

✤ We know this is underestimating material ✤ Last November, I presented results of a study that

attempted to quantify the effect of more realistic material…

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Reminder of Material Study

✤ Effect of increasing upstream neck of Horn 1 (in 2-

horn optimized design) to 3 mm:

This made sense…

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✤ Effect of 6 mm downstream endcap:

This was surprising. And indeed, when Paul and I poked further, there was a bug in this simulation…

Reminder of Material Study

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✤ Effect of 45 mm downstream endcap:

~3% flux loss in peak with 4.5 cm endcap (note that this is much thicker than we expect any single endcap to be)

Updated Material Study

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✤ Effect of 6 mm downstream endcap:

<1% flux loss in peak with 4.5 cm endcap (note that this is much thicker than we expect any single endcap to be)

Updated Material Study

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✤ Still to-do: ✤ Study effect of gradually thickening endcap material

as radius increases

✤ For technical reasons, I have to remove the water

layer to do this, but I think that is okay

✤ Study endcap effect in 3-horn optimized system

Updated Material Study

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✤ As you may have heard, our experiment is called DUNE ✤ A lot of computing stuff still refers to LBNE ✤ The machines known as lbnegpvm0X that many of us use for building and running gl4bnf

are being converted to dunegpvm0X

✤ /lbne/data/ and /lbne/app/ mounts have been renamed /dune/data/ and /dune

app/

✤ /pnfs/lbne appears to be available on the dungpvm’s, but you should probably start

using /pnfs/dune

✤ Our group name is ‘dune’ instead of ‘lbne’, which means that you can possibly not

modify/delete files created on the lbnegpvm’s

✤ I’ve updated the files in g4lbnf/ProductionScripts to deal with all of this ✤ You scan do a git pull to get the new scripts ✤ Let me know if you have problems (test on dunegpvm06-10)

Beam Simulation News

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✤ I think we are pretty close to being able to submit

g4lbnf jobs to the Open Science Grid

✤ Will give us a lot more grid slots ✤ I’ve installed g4lbnf v3r4p2 in cvmfs (a

prerequisite to running on the OSG)

✤ Let me know if you are interested in helping push

this forward

Beam Simulation News

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The End

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3 Horn Optimization Results

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Horn Parameters

LA F1A r1A rOCA r2A r1B r2B r3B F1B F2B F3B F4B r1C rOCB rOCC r2C r3C F1C F2C F3C F5C LB LC

✤ Last time I showed preliminary results of a three horn

  • ptimization