High-pressure gaseous argon in the DUNE near detector Andy - - PowerPoint PPT Presentation

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High-pressure gaseous argon in the DUNE near detector Andy - - PowerPoint PPT Presentation

High-pressure gaseous argon in the DUNE near detector Andy Furmanski, on behalf of the DUNE collaboration CPAD 2019 Madison, Wisconsin DUNE D eep U nderground N eutrino E xperiment: Next-gen long-baseline neutrino oscillation experiment


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High-pressure gaseous argon

in the DUNE near detector

Andy Furmanski, on behalf of the DUNE collaboration CPAD 2019 Madison, Wisconsin

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Andrew Furmanski University of Minnesota 2

DUNE

Deep Underground Neutrino Experiment: Next-gen long-baseline neutrino oscillation experiment running from Fermilab (Illinois) to SURF (South Dakota)

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Andrew Furmanski University of Minnesota 3

The DUNE far detector

  • 40 kt of liquid argon (fiducial)
  • 1 mile underground
  • 1300 km from beam source
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Andrew Furmanski University of Minnesota 4

The DUNE near detector

ArgonCube: Liquid argon (LAr) Multi-Purpose Detector (MPD): Gaseous argon (GAr) 3D scintillator tracker (SAND): Hydrocarbon LAr+GAr move off- axis: PRISM A highly capable near detector complex is critical for reducing flux and cross section uncertainties for DUNE’s physics goals!

Neutrinos coming from the right

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Andrew Furmanski University of Minnesota 5

Why use a gas detector?

  • Gas detector provides:

– Lower thresholds – Fewer showers

  • Better hadron and electron energy measurements
  • Photons, neutrons need an ECAL
  • Complementary measurements to the liquid
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Andrew Furmanski University of Minnesota 6

More reasons to use gas!

  • Even angular acceptance

– Magnet provides good momentum measurement for all particles – Liquid near detector is too small to contain many events

  • Cross-check acceptance/efficiency and model

dependence

Far detector acceptance LAr near detector acceptance GAr near detector acceptance

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Andrew Furmanski University of Minnesota 7

MPD - requirements

  • As a muon spectrometer:

– Reasonable momentum resolution → magnet for curvature – Particle ID – Cross-sectional area matched to LAr

  • As a neutrino target:

– 1000 kg fiducial mass of argon → high pressure – Measure photons, neutrons → ECAL – Excellent PID – Low thresholds (few-MeV for protons) → spatial resolution

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Andrew Furmanski University of Minnesota 8

MPD baseline design

  • Re-use the ALICE TPC readout

chambers (already in-hand)

  • New central readout chambers

– New field cage, support structure, etc

  • Pressure vessel at 10atm
  • Surrounding ECAL (from new)
  • Magnet (multiple designs being

considered)

– Will be instrumented as a muon

catcher

5m 5m

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Andrew Furmanski University of Minnesota 9

Gas readout

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Andrew Furmanski University of Minnesota 10

Gas TPC expected performance

  • Few-percent momentum resolution (~3%

below 1 GeV)

– ALICE achieved < 1%

  • Few-percent dE/dx measurements

(8.5 atm) ECAL/muID used to ID particles where these lines crossed DUNE baseline design uses the same 90:10 Ar:CH4 mixture as PEP-4

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Andrew Furmanski University of Minnesota 11

ECAL design

  • Based on CALICE design
  • Combination of scintillator tiles (inner) and strips (outer)

– High-granularity inner provides photon direction and good energy

resolution

  • Fast timing for t0 for TPC

– Maybe neutron TOF too → leads to O(ns) timing resolution requirement

  • Optimisation in progress
  • ~50% of pions won’t interact in the ECAL
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Andrew Furmanski University of Minnesota 12

Magnet design

  • Exploring various options
  • Considerations:

– Field uniformity – Stray field – Total space needed – Material between liquid and gas

  • Instrument magnet as a muon

catcher

– Solves the mu/pi problem in the ECAL

Superconducting 3-coil Helmholtz with 2 bucking coils Solenoid with partial return yoke (no front face)

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Andrew Furmanski University of Minnesota 13

R&D – FNAL test-stand

  • Test at FNAL:

– Using one of the ALICE inner chambers – Small field cage and cathode to form drift region – Pressure vessel rated to 10 atm

  • Planned measurements:

– Gas gain for different gas mixtures at various

pressures

– Demonstrate successful drift and readout at 10

atmospheres!

  • Currently operated up to 5 atm

– Test of readout electronics planned for use (as

much overlap with liquid as possible)

  • LArPix, Qpix?
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Andrew Furmanski University of Minnesota 14

First pulses

Cosmic, 1atm Fast signal – electron avalanche near anode wires produces lots of positive ions Ions moving away from the pad plane Long positive pulse as ions move in the field cage

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Andrew Furmanski University of Minnesota 15

Iron-55 source pulses

  • Fe-55 source (X-rays)
  • Frequently observe

multiple pulses close together

Fe-55, 1atm

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Andrew Furmanski University of Minnesota 16

Preliminary gain measurement

  • Pulse height used to infer gain
  • Gain measured at various anode voltages

– Results agree with our expectations

1 atm Fe-55 source

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Andrew Furmanski University of Minnesota 17

High-pressure testing

  • Successfully run at 5 atmospheres

– Gas gain drops as expected – Next stop – 10 atmospheres!

Fe-55, 5atm Cosmic, 5atm

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Andrew Furmanski University of Minnesota 18

RHUL test-stand

  • Royal Hollaway University of London are testing an ALICE outer

chamber

– Still in the gas-tight transport box

  • Currently testing at 1atm
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Andrew Furmanski University of Minnesota 19

RHUL: coming up

  • Transfer to a pressure

vessel rated to 5 atmospheres

  • A tight fit!
  • Make the same

measurements as GOAT

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Andrew Furmanski University of Minnesota 20

Simulations

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Andrew Furmanski University of Minnesota 21

Conclusions

  • DUNE has designed a capable near detector complex
  • High-pressure gas TPC as a spectrometer and an

independent neutrino target is a crucial part of the design

  • High-pressure gas TPC design based on ALICE is

maturing

  • R&D in the US and the UK is making good progress
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Andrew Furmanski University of Minnesota 22

Thank you for listening

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Andrew Furmanski University of Minnesota 23

Backups

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Andrew Furmanski University of Minnesota 24

DUNE physics goals

  • Long-baseline (accelerator):

– Determination of neutrino mass hierarchy – Observation of CP-violation in the lepton sector (if the

universe is kind)

  • Other:

– Supernova detection and measurement – Baryon number violation (nucleon decay) – BSM searches, both accelerator and non-accelerator

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Andrew Furmanski University of Minnesota 25

DUNE sensitivity

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Andrew Furmanski University of Minnesota 26

DUNE long-baseline analysis

  • Measure event rate vs

(reconstructed) neutrino energy at far-detector

  • Compare to predictions with

various oscillation parameters

– Infer best-fit parameters!

  • Uncertainties in flux, cross

sections lead to uncertainties on

  • scillation measurement

– Solution - measure the flux and

cross sections at a near detector!

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Andrew Furmanski University of Minnesota 27

More HpgTPC images

In liquid argon, this is all in one voxel

Inner and Outer readout chambers

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Andrew Furmanski University of Minnesota 28

Detecting light in gaseous Ar

  • Studying the ability to read out

scintillation signals too

– For a t0 tag if entire interaction is contained – Not critical for primary DUNE physics

program

– Not being pursued for DUNE

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Andrew Furmanski University of Minnesota 29

GOAT details

  • 1ADC = 0.48mV
  • 1 tick = 128ns