Fitting Supernova Spectral Parameters with DUNE Erin Conley On - - PowerPoint PPT Presentation

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Fitting Supernova Spectral Parameters with DUNE Erin Conley On - - PowerPoint PPT Presentation

Fitting Supernova Spectral Parameters with DUNE Erin Conley On behalf of the DUNE Collaboration April 14, 2019 Outline Introduction The Deep Underground Neutrino Experiment (DUNE) Supernova neutrinos Modeling supernova neutrinos


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Fitting Supernova Spectral Parameters with DUNE

Erin Conley On behalf of the DUNE Collaboration April 14, 2019

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Outline

  • Introduction

– The Deep Underground Neutrino Experiment (DUNE) – Supernova neutrinos

  • Modeling supernova neutrinos in DUNE

– SNOwGLoBES – MARLEY – Pinched-thermal flux model

  • Parameter fitting algorithm

– Studying incorrect detector performance assumptions

  • Summary
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  • International experiment for neutrino science (1100+ collaborators!)

– Neutrino oscillation physics, supernova physics, nucleon decay

  • Two detectors:

– Near detector on-site at Fermilab – Far detector at Sanford Underground Research Facility (SURF) in South Dakota

  • Far detector: world’s largest liquid argon time-projection chamber

(40 kton fiducial mass)

– Ionization electrons drift due to high-voltage electric field – Parallel wire planes create 3D images of particle tracks

www.dunescience.org

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Supernova Neutrinos in DUNE

  • Expect ~3000 neutrino

interaction events in DUNE detector for a 10 kpc SN

– Neutrinos of all flavors carry 99% of core collapse energy – LAr is sensitive to !" (versus water/scintillator which are sensitive to ̅ !")

  • DUNE devotes much time

into studying theory, event simulation, reconstruction algorithms, etc. related to supernova physics

Number of SN interactions expected to be seen in DUNE detector

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Simulating Supernova Neutrino Signals

  • SNOwGLoBES:

SuperNova Observatories with GLoBES

– GLoBES: General Long Baseline Experiment Simulator

  • Open source event

rate calculation tool

http://phy.duke.edu/~schol/snowglobes/

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Supernova Flux Model

  • Supernova neutrino spectrum AKA

“pinched-thermal form”: ! "# = % "# "#

&

exp − + + 1 "# "#

– "#: Neutrino energy – %: Normalization constant (related to luminosity, .) – "# : Mean neutrino energy – +: Pinching parameter; large + corresponds to more pinched spectrum

  • Parameters of interest: ., "# , +

Pinched-thermal for a 10kpc supernova (K. Scholberg) Note: Fluence refers to a time-integrated flux.

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MARLEY: Model of Argon Reaction Low-Energy Yields

  • MARLEY models low-energy

!"CC neutrino interactions

  • More sophisticated modeling
  • f final state particles
  • S. Gardiner (http://www.marleygen.org/)

$% = 16.3 MeV

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Measuring the Flux Parameters

  • Use pinched-thermal flux +

MARLEY modeling to simulate event rates in DUNE detector

  • Flux parameters play

significant role in !" event rates

  • Develop algorithm to

measure, constrain flux parameters based on SNOwGLoBES event rates

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( )

1) Test Spectrum !", $% ", &"

2) Grid with many different combinations of (!, ⟨$%⟩, &)

Parameter Fitting Algorithm

  • Algorithm uses the

following tools:

– “Test spectrum” with given set of pinching parameters !", $% ", &" – Grid of energy spectra containing combinations of (!, $% , &)

  • Compute '( value between

test spectrum and all grid spectra; determine best-fit grid element, “sensitivity regions” that constrain parameters

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Studying Biases due to Incorrect Detector Assumptions

  • Test spectrum: data from

supernova as observed by DUNE

  • Grids: different DUNE detector

performance assumptions

  • Change assumptions for test

spectrum, and for grids, to study effect of mismatched assumptions about detector performance

– Study parameter biases introduced by incorrect assumptions using fractional difference from truth:

  • Frac. Diff. = * − *,

*,

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Studying Effect of Detector Performance Knowledge on Bias:

  • Each box corresponds to a unique combination of test

spectrum and grid; diagonal boxes correspond to correct assumptions

  • Color scale indicates best-fit parameter fractional

difference from truth

  • As assumptions get farther from truth, biases

increase; +30% shift in assumed energy resolution yields ±20% bias on '

Test Spectrum Resolution (Percent) Grid Spectra Resolution (Percent)

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Summary

  • DUNE is preparing to observe supernova neutrinos and

extract as much information as possible

  • Parameter fitting algorithm used to understand DUNE’s

ability to constrain supernova flux parameters

– 2D fractional difference plots show bias results from imperfect knowledge of detector parameters; helps quantify how well we need to know these parameters

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Backup Slides

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  • Neutrino-argon interaction: argon is

ionized by charged secondary particles

– Scintillation light detected by photon detectors provides timing information

  • Charged particles drift toward induction

planes, deposit charge on collection plane wires

  • Charge deposited on wire planes

– Reconstructed wire objects (signals for specific particles) – Reconstructed 2D hits (single ionized particles) – Reconstructed 2D clusters (ionization of multiple particles) – Reconstructed 3D objects like tracks, showers, space points

LArTPC Schematic

Liquid Argon Time Projection Chamber

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Forward Fitting: “Sensitivity”

  • Use SNOwGLoBES to generate

binned energy spectra for a given set of pinched-thermal parameters !", $%

", &" → “test spectrum”

  • Determine () values for all elements

in grid with many combinations of (!, $% , &)

  • Minimize () while profiling over 1 or

2 model parameters

  • Form sensitivity regions using cut
  • n () values

Example () Map

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Energy Resolution: Introduction

  • Determine how smearing

affects parameter measurements – what if

  • ur resolution

assumptions are incorrect?

  • Smearing matrices: true

deposited energy from MARLEY + LArSoft; smeared with Gaussian resolution from 0 − 30%

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Examples of Sensitivity Regions

Notes:

  • Here we see

superimposed sensitivity regions + best-fit parameters for one test spectrum input into different grids

  • We can see how

the areas change and also how the bias in our best-fit measurements change!

! " (10&' ergs)

  • . (MeV)

!