High-Charged Magnetized Beams at FAST-IOTA [MagBeam] Northern - - PowerPoint PPT Presentation

high charged magnetized beams at fast iota magbeam
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High-Charged Magnetized Beams at FAST-IOTA [MagBeam] Northern - - PowerPoint PPT Presentation

NORTHERN ILLINOIS CENTER NORTHERN ILLINOIS CENTER FOR ACCELERATOR FOR ACCELERATOR AND DETECTOR AND DETECTOR DEVELOPMENT DEVELOPMENT High-Charged Magnetized Beams at FAST-IOTA [MagBeam] Northern Illinois University: A. Fetterman*, C.


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SLIDE 1

NORTHERN ILLINOIS CENTER FOR ACCELERATOR AND DETECTOR DEVELOPMENT NORTHERN ILLINOIS CENTER FOR ACCELERATOR AND DETECTOR DEVELOPMENT

High-Charged Magnetized Beams at FAST-IOTA [MagBeam]

Northern Illinois University: A. Fetterman*, C. Marshall*, P . Piot Fermilab: J. Ruan Collaborators at JLab: S. Benson, J. Gubeli,

  • F. Hannon, S. Wang

1

* Graduate students

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SLIDE 2

funded proposal to DOE NP

  • T1: High-charge magnetjzed beam:
  • Productjon of high-charge (1.6 and 3.2 nC) magnetjzed

beam

  • characterizatjon of magnetjzatjon
  • Transport + manipulatjon over long beamline including

use of locally non-symmetric optjcs

  • T2: Understanding halo
  • Explore halo formatjon in magnetjzed beam using a long-

dynamical range diagnostjcs (LDRD)

  • T3: New merger concept:
  • Tests of merger concept combining RF defmector and

magnetjc coil proposed by G. Kraffu and A. Hutuon -- augmentjng recent test at Cornell.

2

Some encouraging results produced during run I, but poor data quality for publication Initially planned for run II now moved to run III Initially planned for run III now moved to another facility (DOE approved)

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SLIDE 3

Relevance of FAST injector to EIC e- cooling

3

  • Similar beam parameters except

for a higher peak current

/1.6 (OLD)

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SLIDE 4

Outcomes and limitations of Run I

  • Signifjcantly improved bunch charge:
  • Emission was space-charge-limited
  • Increasing spot size resulted in bunch charge up to 6 nC
  • Produced and transported a magnetjzed beam up to the

low energy dump:

  • Characterized magnetjzatjon and other beam parameters
  • Produced a fmat beam:
  • Measured associated emituance (which corresponds to the

incoming magnetjzed beam eigen emituances)

  • Limitatjons:
  • Emituance measurement of eigenemituance could not be

performed precisely due to movable slit issues

  • We could not trust the ICT
  • Laser inhomogeneity

4

X118 X120 +X118H X120 +X118V

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SLIDE 5

Outcomes and Summer Improvements

  • Issue with single-slit scan was fjxed

(Daren, Jinhao) and analysis (Aaron) shows is could be used for emituance measurement

  • Improved analysis of data is encouraging

5

(analysis from Aaron Fetterman)

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SLIDE 6

Simulation using realistic experimental conditions reproduce some of the experimental feature (A. Fetterman et al. NAPAC19)

  • Optjmizatjon done for idealized laser distributjon
  • Impact of non-ideal distributjon is explored via simulatjon

04/02/2019

  • P. Piot | 2019 JLEIC collaboratjon meetjng, JLab

6

9 mm 9 mm E (MeV)

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SLIDE 7

Proposal (phase I: 4 shifts)

  • Shifu 1: essentjally reproduce settjngs of run 1 (FEB/

MAR):

– Vary solenoid and monitor vacuum

(processing)

– Test all diagnostjcs and especially all the

scanning single slits diagnostjcs

  • Shifus 2-4 (contjguous): 1.6 and 3.2-nC magnetjzed

beam characterizatjon

– Measure magnetjzatjon, eigen emituances, – Perform parametric studies for a few cases:

several laser-spot radii. Ratjo of Bmain and Bbuck

– Take data to compare the two eigen-emituance

measurement methods

7

Mapping through a round to flat beam transformer Direct measurement on mag. beam Beam termination in low-energy absorber

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SLIDE 8

Proposal (phase II: 2 shifts)

  • Shifu 5-6: beam transport to downstream

cryomodule (assuming all data of phase I have been collected)

– Transport through cryomodule (ideally

with cryomodule eventually ofg)

– Generatjon of a “skew” fmat beam with

Q441-3

– Measure beam magnetjzatjon

downstream of cryomodule and injector values.

– If tjmes allows study propagatjon

  • f magnetjzed beams in a non-locally

but globally symmetric beamline

8

Flat beam generated using Q441-3 quads and observed in the 450 area !!! Beam termination: not sure on its way to HE dump (is it acceptable with up to 10 bunches (total Q~50 nC over macropulse?)

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SLIDE 9

Personnel + TODO list

  • Shifu personnel:

– Shifu 1: local people (NIU

include A. Fetuerman and P. Piot)

– Shifu 2, 3, and 4: Jlab personnel

will join (list to be fjnalized

  • nce we have possible dates)

– Shifu 5, 6: locals only (TBC) will

likely include NIU’s C. Marshall,

  • A. Fetuerman and P. Piot.

9

  • Hardware:

– Check CCD focus at slit

locatjons [Aaron]

– Deploy/test RCDS algorithm for

fast on-line fmat beams

  • ptjmizatjon [Philippe]

– Ability to change the laser spot

size between 2 to 4 mm (full radius) if not what is possible?

– Are the ICTs OK?

  • Data acquisitjon/analysis

– Tools are mostly ready and will

enable some preliminary on-line analysis to guide experiment