DUNE FD Calibration workshop: Summary, additional thoughts & Next steps
Sowjanya Gollapinni (UTK) Kendall Mahn (MSU) DUNE Calibration Workshop March 16, 2018
DUNE FD Calibration workshop: Summary, additional thoughts & - - PowerPoint PPT Presentation
DUNE FD Calibration workshop: Summary, additional thoughts & Next steps Sowjanya Gollapinni (UTK) Kendall Mahn (MSU) DUNE Calibration Workshop March 16, 2018 Calibration Strategy: Collaboration Process Timeline 2 Workshop Goals/Format
Sowjanya Gollapinni (UTK) Kendall Mahn (MSU) DUNE Calibration Workshop March 16, 2018
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(https://indico.fnal.gov/event/16087/other-view?view=standard)
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Attendance: 20 in-person and 5-10 remote (productive discussions!)
used to test models
strong argument for redundancy
timescales for measurements, need to take it into account
and also how we can use it to test things for DUNE (e.g. DUNE electronics test)
All consortia need to thinking about
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External Calibration Systems (currently considered)
System (e.g. T2K)
devices — not discussed
considered/discussed
attached to cathode; injecting sources into argon
feasibility study planned
emitter? — bench tests and protoDUNE for feasibility
the cathode, a nice wake-up system to know things are alive
to understand
penetrate ground plane
require updating with new simulation-based cosmic numbers from
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9 MeV
Muon decay (Michels) endpoint ~50MeV
6 MeV (captures)
9 MeV
Muon decay (Michels) endpoint ~50MeV
6 MeV (captures)
9 MeV
Muon decay (Michels) endpoint ~50MeV
6 MeV total photon signal
EM shower outliers
can span the detector
understand needs
test bench
Calibration Source in the DUNE FD
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fibers safely
electrons off the mirror? much simpler system
studies
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(Josh Klein, Richard Diurba)
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(Matt Graham, Josh Klein, Kurt Biery)
will be >10 MeV for normal running
builder cannot keep up
suppression (~10 Tb/s/10 kt)
suppressed)
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in TP (see backup)
coming weeks
from underground location to surface discussed; zero suppression schemes
maybe challenges on that front that needs to be considered
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Clara Cuesta based on ProtoDUNE-DP design
Clara Cuesta
detected in the gaseous phase above liquid level
provide enormous number of APA-CPA crossers
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cm (dQ/dx 2 – 3%) — without taking into account ion accumulation
APA flatness etc.) — more of an issue for SP than DP
complicated for DP: +ve ions may collect above the liquid and create surface interface
drift field
variations b/n gas and liquid phase can be an issue; flow pattern can also impact
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A&3D&model&of&a&small§ion&
CRP®ion.
Extraction&grid (10mm&below& LEM) Liquid&gas& interface LEM&(0.5mm& holes&@&0.8mm& pitch,&1mm&thick) CRP
DUNE&Calibration&Workshop,&14O16&March& 2018 10
2kV/cm 30kV/cm 3kV/cm 2kV/cm 0.5kV/cm
A&2D&cut&plane&near&the&front& face&of&the&model&is&plotted&in& the&following&slides.
DP&cross§ion&view
From&S.&Murphy
Bo Yu
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Bo Yu
DUNE&Calibration&Workshop,&14?16&March& 2018 12
Due&to&the&unfavorable&collection&to&extraction& field&ratio&(2:3),&a&fraction&(1/3?)&of&the&electrons& lands&on&the&upper&surface&of&the&LEM,&therefore& not&contributing& to&the&CRP&signal. Electron&multiplication&occurs&mostly&in&the&blue& region.&&The&positive&ions&created&drift&down& following&the&same&paths&as&the&incoming& electrons. Diffusion& of&electrons&and&ions&will&alter&their& actual&drift&paths&from&these&ideal&lines&(much& less&effective&for&ions).&& Assuming& the&gain&of&the&LEM&is&defined&by&the& collected&electrons&on&the&CRP,&the&ions&created& by&these&electrons&are¬&near&the&outer&layer&
most&likely&drift&back&to&the&cathode.&&&&
(also need to consider liquid flow effects into this)
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0.01 0.1 1 10 100 1000 0.1 1 10 100 1000 10000 1 10
Maximum'Longitudinal'Delay'[µs] Maximum'Transverse'Deflection''[mm]
Drift'Length'[m]
Ar39'Positive'Ion'Space'Charge'Distortion'vs.'Drift'Length''
DUNE(SP DUNE(DP(w/o(ion( feedback Solid(lines:(TPC(with(a(square(cross(section DUNE(DP(with(10%( ion(feedback
DUNE(Calibration(Workshop,(14F16(March( 2018 16
The maximum E (transverse) is 14% of drift field
The maximum E(longitudinal) is 15% of drift field
Bo Yu
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Bo Yu
DUNE&Calibration&Workshop,&14A16&March& 2018 18
I&have¬&seen&a&CFD&of&the&DP&FD&cryostat.&&The&closest&study&I&can&find&is&this& plot&from&Erik&Voirin on&a&LBNE&33kt&design,& in&which&the&cathodes&are&wire&mesh& with&little&impact&on&the&liquid&flow.&&The&red&bands&represents®ions&where& the&liquid&flow&velocity&is&close&to&8mm/s,&the&ion&drift&velocity&@&500V/cm&field.&& The&two&blue&circles&indicate&the®ion&with&possible&stalled&ion&movement.&&On& the&other&hand,&the¢er&of&the&cryostat&should&have&reduced&space&charge& build&up&due&to&the&downward&flow&of&the&liquid.
Need to understand this more
phase by the 3kV/cm extraction field? Or can the electron be striped off the ion and pulled into the gas by the extraction field?
the gain drifts with time, periodic re-mapping of the gain may be needed.
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discussions/considerations into the summary document with responses to key questions/concerns
Proposal (2 to 3 page long?)
will be included in individual consortium chapters?
main editors — we will follow up
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