Electrostatic Septa for Mu2e Design V. Nagaslaev ESS Engineering - - PowerPoint PPT Presentation

electrostatic septa for mu2e design
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Electrostatic Septa for Mu2e Design V. Nagaslaev ESS Engineering - - PowerPoint PPT Presentation

Introduction for the Electrostatic Septa for Mu2e Design V. Nagaslaev ESS Engineering Review, January 18, 2017 Content for the discussions About the review process Introduction Mu2e Experiment Beam Delivery for Mu2e Slow


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SLIDE 1
  • V. Nagaslaev

ESS Engineering Review, January 18, 2017

Introduction for the Electrostatic Septa for Mu2e Design

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SLIDE 2
  • About the review process
  • Introduction
  • Mu2e Experiment
  • Beam Delivery for Mu2e
  • Slow Extraction

Slow Extraction for Mu2e 2

Content for the discussions

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SLIDE 3

Slow Extraction for Mu2e 3

The Mu2e Experiment

4.6T 2.5T 2.0T 1.0T 1.0T

  • Improved sensitivity by ~4 orders of magnitude
  • Great potential to discover new physics
  • Expect to start taking data in 2021-2022
  • CD3c in June 2016
  • Transitioning to the fabrication phase

Direct conversion of muons into electrons in the field of nucleus

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SLIDE 4

Slow Extraction for Mu2e 4

Pulsed beam time structure

This beam structure can be realized with slow extraction from a machine with circulating narrow bunches, separated by ~1700nsec.

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SLIDE 5

Slow Extraction for Mu2e 5

Mu2e Proton Delivery

Main Injector & Recycler

Mu2e

  • Two Booster “batches” are injected

into the Recycler (8 GeV storage ring). Each is:

  • 4x1012 protons
  • 1.7 msec long
  • These are divided into 8 bunches
  • f 1012 each
  • The bunches are extracted one at a

time to the Delivery Ring

  • Period = 1.7 msec
  • As the bunch circulates, it is

resonantly extracted to produce the desired beam structure.

  • Bunches of ~3x107 protons each
  • Separated by 1.7 msec

Booster Delivery Ring (aka Debuncher)

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SLIDE 6

Slow Extraction for Mu2e 6

Machine cycles

Full cycle in the Main Injector (1.33sec) is used to serve the neutrino experiments 12/20 of the cycle Booster and RR supply protons for the Main Injector 8/20 of the cycle can be used for muon physics Beam intensity in the Recycler during 8/20 of the cycle Beam intensity in the Delivery Ring during 8/20 of the cycle

0 1 2 3 4 4 6 7 8 9 10 11 12 13 14 15 16 17 18 19

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SLIDE 7

Slow Extraction for Mu2e 7

Slow (Resonant) Extraction Design

  • 3rd Order Resonance Extraction
  • DR to be augmented for 3rd order resonance:
  • Operation point moved to 2/3
  • 2 circuits of sextupole magnets
  • Squeeze by ramped quads circuit
  • Dynamic orbit control in extraction region
  • Spill Monitoring
  • Spill regulation by RF Knock-Out system
  • Electrostatic septa based on thin foils
  • Cost effective:
  • Minimal changes to the legacy Debuncher lattice
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SLIDE 8

Slow Extraction for Mu2e 8

Beam parameters

Parameter Value Units Beam kinetic energy 8.0 GeV MI Cycle time 1.333 sec Number of spills per MI cycle 8 Number of protons per micro-pulse 3.9×107 protons Maximum DR Beam Intensity 1.0×1012 protons Average spill rate 6.0×1012 protons/sec Duty Factor (Total Spill Time ÷ MI Cycle Length) 29 % Duration of one spill 43 msec Time Gap between spills 5 msec Extraction efficiency >98 % Max variation of pulse intensity ±50 %

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SLIDE 9

Slow Extraction for Mu2e 9

Remodeling the Debuncher  Delivery Ring

  • Old Injection  Abort line
  • New Injection (new beam line)
  • New Extraction in SS30
  • ESS
  • Sextupoles:
  • 2 families in Low Disp.
  • Suppress Octupole

harmonic

  • Tune Quads
  • Magnetic septa (LAM+C-mag)
  • Dynamic bump
  • RFKO for spill regulation
  • Spill monitoring
  • Spill regulation

SS10-60 SS40-50 SS20-30

RFKO kicker

ESS

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SLIDE 10

Slow Extraction for Mu2e 10

Electrostatic Septum Specifications

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SLIDE 11

Slow Extraction for Mu2e 11

Main design constraints

  • Physics, beam parameters
  • Beam losses
  • Space available
  • Available technologies
  • Cost
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SLIDE 12

Slow Extraction for Mu2e 12

Specifics of the ESS design

  • 2 septa @ max beta
  • Foil septum plane
  • Diffuser
  • 2 vessels identical
  • Heavy shielding
  • No remotely controlled

motion inside vessels:

  • Movable vessel support
  • Bellows for decoupling
  • Adjustable field gap
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SLIDE 13

Slow Extraction for Mu2e 13

ESS length specifications

ESS1 ESS2

ESS:

  • Deflects beam horizontally INWARD
  • Need >2mrad kick
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SLIDE 14

Slow Extraction for Mu2e 14

Diffusor

No diffuser Diffuser Modeling:

X1 X2 X1 X2

Simulations made with sparse Mo foils Titanium foils seem to be available Carbon foils would be ideal!

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SLIDE 15

Slow Extraction for Mu2e 15

Critical performance

  • 1. Foil plane quality (mechanical tolerance)
  • 2. Foil plane and cathode alignment (motion)
  • 3. High Voltage
  • 4. High Vacuum
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SLIDE 16

Slow Extraction for Mu2e 16

ESS Specifications document

Printouts provided

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SLIDE 17

Slow Extraction for Mu2e 17

Summary

This is a friendly review, hope this will be fun for you!