Updates and Status of the Noble Element Simulation Technique Jon - - PowerPoint PPT Presentation

updates and status of the noble element simulation
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Updates and Status of the Noble Element Simulation Technique Jon - - PowerPoint PPT Presentation

Updates and Status of the Noble Element Simulation Technique Jon Balajthy CPAD Workshop December 10, 2019 1 2 Noble Element Simulation Technique (NEST) Simulation package for modelling response of noble element detectors Interpolates


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Updates and Status of the Noble Element Simulation Technique

Jon Balajthy

CPAD Workshop December 10, 2019

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Noble Element Simulation Technique (NEST)

Simulation package for modelling response of noble element detectors

  • Interpolates between existing calibration datasets to provide predictions

for arbitrary energies and fields

  • LXe is most fully developed model, LAr is currently in development
  • Collaborators from wide range of experiments and institutions

○ LUX/LZ, XENON, (n)EXO, DUNE Main webpage: http://nest.physics.ucdavis.edu/ Github page: https://github.com/NESTCollaboration/nest Several implementation platforms:

  • C++ based executable
  • Geant4 integration
  • Python wrapper
  • Online calculator

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The NEST Physics model

NEST is a set of mostly empirical models that simulates S1 and S2 size, timing, and location The inputs required:

  • Event energy and/or interaction type

○ Beta/Compton (spectra for H-3 and C-14 included) ○ NR (AmBe, B-8, WIMP, neutrons) ○ Kr-83m ○ Heavy Ions ○ Alphas ○ Photoabsorption

  • Drift field profile (can be a constant or a detailed map)
  • Detector parameters (g1, g1_gas, density, extraction efficiency, etc.)

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Current Status

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Very brief overview- more detailed information available at NEST website (http://nest.physics.ucdavis.edu/) Also see Greg Rischbieter’s talk from DANCE conference (https://indico.cern.ch/event/824917/contributions/3571627/att achments/1934381/3205056/NEST_DANCE_GR.pdf)

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Nuclear Recoil Yields

Same yields model used for WIMPs, D-D, B-8, Cf, AmBe Recent data from LLNL improves model at low energy

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  • M. Szydagis. (NEST Collaboration) A Comprehensive,

Exhaustive, Complete Analysis of World LXe NR Data With a Final Model. 2019. Need Ly data in <1keV region

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Electron Recoil Yields

Currently divided into two(ish) parts:

  • Compton/beta yields
  • Photo-absorption
  • Also includes special case of Kr-83m

Ly and Qy are complementary, (Ly = 1/W - Qy)

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photoabsorption

beta/Compton

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Ions and alphas and krypton, oh my!

alpha-NR Heavy Ions Kr-83m

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Resolution Model

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Improved Modeling of β Electronic Recoils in Liquid Xenon Using LUX Calibration Data LUX Collaboration (D.S. Akerib et al.). Oct 9, 2019. 17 pp. e-Print: arXiv:1910.04211 [physics.ins-det]

LUX C-14 LUX D-D NEST doesn’t just do mean yields! Fluctuations from recombination + detector resolution, tuned to match band means+widths

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Recent/Ongoing Updates

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  • 1. LArNEST
  • 2. Low energy NR model
  • 3. ER model overhaul
  • a. Inner shell interactions (nu-e, EC)
  • b. Compton vs beta
  • 4. Work Function
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LAr ER Model

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Coming soon! Models based on LXe equations and fit to LAr calibration data

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LAr NR Model

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NR, too! Low energy behavior modeled after LXe measurements

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Low Energy NR Model

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New data from Livermore improves sub-keV Qy, but Ty and Ly are still unknown

Need total yields measurements in sub-keV region

  • Low energy behavior could trend high or

low

  • Difficult measurement to make due to

small LY at low E NR

Lenardo, Brian, et al. "Measurement of the ionization yield from nuclear recoils in liquid xenon between 0.3--6 keV with single-ionization-electron sensitivity." arXiv preprint arXiv:1908.00518 (2019).

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ER-Model Overhaul

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  • Re-fit beta model using C-14 from LUX and H-3 data from

XENON and XeLDA

  • (?)Separate beta and Compton models
  • Develop new electron capture/ nu-e scattering model
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Beta vs EC

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XeLDA detector at FNAL observed offset of H-3 vs Xe-127 L-shell capture Primary decay mode: 5.1keV is divided ~evenly between 6 electrons

  • > Higher dE/dx means more recombination

Slide from Dylan Temple’s TAUP talk

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Beta vs EC

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This effect was also observed in LUX, but was within systematic error. Is not observed in K, M, or N shells ER->NR leakage fraction for L-shell captures increases from ~0.5% to ~3% Leads to ~20% increase in neutrino burden in LZ G3 experiments will have O(10,000) 𝜉-e scatters (~7% are 𝜉-L, or ~1,000 events) XeLDA result predicts ~30 leaked events vs. ~5 for current NEST

Preliminary plot from Dylan Temples Identical

  • ffset in LUX

and XeLDA

Need to develop L-shell NEST model

  • Measurements limited to < 300 V/cm
  • Direct 𝜉-e measurements could be

informative

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Beta vs Compton

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Possibly a similar effect in Compton scattering vs beta decay Tritium data is very consistent, but NEST tends to overshoot at high field

  • > Comes from previous lack of beta data above 180 V/cm

~100 V/cm 150-180 V/cm ~275 V/cm 330-366 V/cm

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Beta vs Compton

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Compton data is also consistent, but disagrees with all available beta data No strong physical explanation for disparity

~180 V/cm ~410 V/cm ~500 V/cm ~2000 V/cm

Need to investigate possible split of CS/beta models

  • Compton/beta measurements from the same detector would cancel any

possible systematic effects (possibly forthcoming from XeLDA?)

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W-value: New EXO result

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Density (g/cc) W (eV/quantum)

The new EXO yields calibration includes a measurement of the average work function (W) Disagrees with accepted results by ~15% Existing measurements of W agree with 13.7 +/-~0.2 eV

arXiv:1908.04128v1

Note: mass density shown, but # density is important. EXO effective density is 2.9 g/cc. Most commonly cited: Absolute measurement from E. Dahl Not listed: 13.4 +/-0.4 eV from neriX. W floated in MC fit.

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W-value: Excess light yield?

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Need more measurements

  • Want to verify our explanation
  • If confirmed, IR scintillation will need to be measured

and modeled. A structured 35% effect might change the field/energy dependence, or even break the combined energy model (no more 1:1 recombination?)

Points include CS and photoabsorption, so expect to fall between beta and gamma Qy seems ~correct, while Ly is high

  • > Additional IR photons detected by APDs?
  • > Add 35% to Ly for silicon PDs
  • > Adding ~15% to both Ly & Qy doesn’t work

(Green is modified NEST model )

Least kludgy method- assumes everyone is right IR scintillation is expected (but not this much)

arXiv:1908.04128v1

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Conclusions

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  • NEST is a robust set of empirical models that currently

matches all world data to ~10% (most places much better)

  • There are still several open questions caused by lack of

data/ contradictory data

  • a. Total yield of low energy NR- Data does not exist
  • b. L-shell interactions- Known to differ, but only measured

at 2 fields in Xe-127 EC

  • c. Beta v. Compton- All available data shows ~10-20%

discrepancy.

  • d. W value- Few absolute measurements available.

Those that exist disagree by ~15%. Might be explained by detector effects

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Extra Slides

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IR Scintillation in LXe

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SD 630-70-75-500 APDs PMT cutoff DOI:10.1016/S0168-9002(00)01249-3

Significant IR scintillation is observed in GXe (~= VUV) Few direct measurements in LXe (none at wavelengths <1um ) Only measurements show LXe << GXe for IR scintillation

Need ~17 ph/keV NIR to explain EXO result

  • GAr NIR yield is 17.5 ph/keV (Xe is higher)
  • LAr yield is ~0.5 ph/keV (times ~30% QE)
  • LXe NIR yield needs to be ~50x yield in LAr

( A Bondar et al 2012 JINST 7 P06014 )

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The NEST Physics model

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  • a. Draws number of quanta given

event type/energy/field

  • b. Divides into Ne, Nγ according to

mean yields model + recombination fluctuations 2. Propagate photons and calculate S1 size/timing ○ Pulse shape model is included ○ Detailed hit-mapping is in development 3. Propagate electrons calculate drift time and S2 size

+ + + -

  • *

*

EExtraction Liquid Gas EDrif

t

e- e- e- e- e-

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Recombination Model

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Recombination is integral to the observed

  • f charge and light yield

Note that recombination does not affect the total number of quanta.