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NO A at Caltech Leon Mualem DOE Review July 25, 2007
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The NO A Detector ~80 m 15.7 m ~16 kT total mass “Totally Active” granular design Outstanding e pattern recognition & measurement Alternating X and Y views 12 Extruded PVC Modules per plane 32 Individual cells per Module, so 384 Cells per plane Working to fit 260M AY$ TPC cap
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NO A Tasks Caltech Initiated or Responsible for many aspects of NO A Hardware DAQ/Electronics Management APD Testing PVC Testing Fiber Testing Vertical Slice Tests Software Framework Development Subshower Package Photon Transport simulation Supernova Sensitivity
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Overview of Detector R&D NO A Perform light output tests to understand the components of the scintillator system [Ongoing] PVC extrusions, liquid scintillator, WLS fiber Verification of scintillator system performance using a NO A APD [Ongoing] Photon production and transport Monte Carlo [Ongoing] Personnel – Jason Trevor, Leon Mualem + undergraduate
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NO A Scintillator System Each cell an extruded TiO 2 loaded PVC tube with ID 60mm x 39mm x 15.7m long Cells are filled with mineral oil scintillator which is read out at one end with a U-loop WLS fiber running to a multi-pixel APD Kuraray 0.7 mm WLS Fiber Light output requirement determined by achievable noise on the APD amplifier. The current estimate of minimum required Light Output is ~20-25 photoelectrons One Cell 0.7mm WLS Fiber R&D at Caltech Composition of the PVC cell walls Liquid scintillator composition Fiber diameter and dye concentration Fiber position Integration testing
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Interface and Readout Electronics Box
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32 Pixel APD Photodetector Array Manufacturer Pixel Active Area1.95 mm × 1.0 mm Pixel Pitch2.65 mm Array Size32 pixels Die Size15.34mm × 13.64mm Quantum Efficiency (>525 nm)85% Pixel Capacitance10 pF Bulk Dark Current (I B ) at 25 C12.5 pA Bulk Dark Current (I B ) at -15 C0.25 pA Peak Sensitivity600 nm Operating Voltage375 ± 50 volts Gain at Operating Voltage100 Operating Temperature (with Thermo-Electric Cooler) -15 º C Expected Signal-to-Noise Ratio (Muon at Far End of Cell) 10:1 APD channels per plane384 APD arrays per plane12
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APD Photodetector Si Avalanche Photodiode Custom design to match two-fiber aspect ratio Bare die mounted to PCB via gold bump thermo- compression
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Scintillator System R&D Liquid Scintillator Two competing mineral oil vendors (Parol, Ren) Competing vendors for additives Concentration of additives (pseudocumene, PPO, Bis-MSB) PVC Extrusions Three competing PVC formulations (Prime, Aurora, NOvA collaboration) Two types of TiO 2 (Anatase, Rutile) Competing factors (extrudability, reflectivity, structural issues)
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Test Setup PMT M16 PMT Box “ Cell” Lead Scintillating Disc 1.2mm Clear Fiber We are currently using a “NO A Cell” with internal dimensions 38.5mm x 60mm x 85cm. Each end of the fiber “U” is connected to an individual pixel on an M16 phototube by 3.5m of 1.2mm clear fiber. Fibers are held in a fixed position inside the cell by a pair of acrylic “spiders.” (More on this later) For testing purposes I am using vertical muons from cosmic rays. The cosmic ray muon telescope consists of two circular discs (~4 cm diam) separated by 14 cm and 1 inch of lead.
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The “NO A Cell” PVC 60mm “NO A Cell” 38.5mm The “NO A Cell” is actually a rectangular aluminum tube which is lined on the inside with the PVC we are testing.
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More “NOvA Cell” Pictures
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Data Data from each fiber end is collected and plotted separately Because the rate is low (one event every 150 seconds), data is acquired over a long period of time (>72 hours) in order to obtain a statistically significant sample
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Results: Scintillator Samples Three scintillator samples, RenDix 517p, ParDix 517p, and RenAld517p. Results show a 20% difference in light output between scintillators made with oil from Ren Oil and those made with oil from Parol. Pseudocumene from different suppliers appear to perform similarly. Measurements are highly repeatable.
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Results: Extrusions We have tested several extrusion samples. Shown here are our baseline extrusion, our best extrusion made with rutile Ti0 2, and our best Anatase extrusion. We have also included two other samples for reference: A MINOS Strip The duplicate “NO A Cell” painted on the inside with BC-620, an acrylic based paint loaded with TiO2(Anatase). All measurements were performed with RenDix 517P Initial results show we can do better that the minimum light output specification. Minimum Spec.
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Upgraded Test Setup PMT M16 PMT Box Actual Cell Lead Scintillating strip 1.2mm Clear Fiber Increased trigger sizes. More than triple the rate, no effect on precision. Testing apparatus is otherwise unchanged Increased throughput of system; limited by sample preparation time, instead of trigger rate.
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Extrusion tests
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More Extrusion Results Tests of recent extrusions show high and consistent light output compared to previous recipes. Recent extrusions have also extruded well mechanically. This is CRITICAL to integrity of the detector: — the PVC is the structure
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Caltech Mini Mini Tracker Minos Scintillator Trigger Minos Scintillator Trigger FRONT VIEW SIDE VIEW 16.4 cm 30 cm 60cm 40cm 150ppm 1 2 3 4 300ppm 250ppm N N 1” Lead “N” = Near length fibers
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Actual Device Not as photogenic, but: Uses prototype APD 33.4m fiber (Actual length) It works
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300 ppm results
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Far Light Output vs. Concentration
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Measurement Summary 150 ppm 24 pe ’ s Significant spread, 20-35 250 ppm 22 pe ’ s Very small spread (only 2 samples) 300 ppm 35 pe ’ s Range: 30-40 3 with ~10% spread
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NO A Software at Caltech We developed a set of light weight libraries (“SoCal”) to allow people to access NO A data and information in C++/ROOT. SoCal consists of: Data format for NOνA NOvA geometry and electronics connection map Event display package Detector & Electronics response simulation tools Full (and up to date) documentation. Tools to help people write further packages. Used by the collaboration to develop reconstruction and analysis used for TDR SoCal Caius Howcroft
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Decay chain Branding Event Source Reco'ed event True Hits e/μ π p Colour = energy deposited Event Display
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Caltech Reconstruction: “Subshower” Code [HZ, CH] 3D shower & Track- like feature reco. Now the standard in MINOS Has been applied to NO A Preliminary use by Bob Bernstein at Fermilab shows significant signal/background separation Needs to be carried through to a complete analysis [e.g. Patterson] “Raw Data” Sub Showers Caius Howcroft
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Detector Simulation Detector simulation code that models the light output of the scintillator, the collection of WLS fiber and the propagation to the APD, “PhotonTransporter” Tracks individual photons and correctly deals with wavelength dependent absorption, reflection and emission coefficients. Has been used to understand results from the Caltech test-stand and in production MC. Accurately reproduces features of measured light collection in a cell Caius Howcroft Charged Particle Simulated Cell WLS Fibers Photon
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Simulations of Light Output vs. Position
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Fiber Position Results Light Yield Simulation suggests light output decreases as fibers approach walls Effect seen in test stand data, but magnitude smaller than predicted Tune simulations with data to reproduce changes quantitatively
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Background Studies NO A is a search for a small signal Understanding and correctly modeling the background is important Work at Minnesota demonstrated the need for an overburden This work also showed potential for Supernova detection with the overburden Additional effort needed to determine sensitivity, and computing requirements to search for small signal events
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Find the SuperNOvA 31 Leon MualemNOvA Electronics ~15min of data With typical ~10s supernova signal 1s time bins NO OVERBURDEN
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Find the SuperNOvA ~15min of data With typical ~10s supernova signal 100ms time bins 1m OVERBURDEN
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Software / Analysis Created the Framework used for NOvA software development and TDR analysis This base now being expanded to add features Created the Subshower analysis package for MINOS, ported to NOvA framework Showing promising results by Bernstein@FNAL Needs to be carried through to a complete analysis Created Photon propagation code Generally useful for understanding light collection and detector performance Validation with actual test data continues
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Caltech Work on NO A WLS Fiber R&D Examined the effect of fiber diameter on light collection in the NO A geometry (The reduction to 0.7mm WLS Fiber saved $3 million+) Measured light output for fibers with varying fluor concentration, ongoing optimization Examine the effect of fiber position inside the NO A cell on light collection, ongoing input to simulation Optical Readout System Verify scintillator system performance using the NO A APD, original and prototype versions Quantify results of production variability using different plastic samples, many cells and fibers Gain experience using the new NO A APD in small scale prototype modules
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Summary NO A Caltech has taken a leading role in NO A detector hardware R&D Measurements done thus far at Caltech have been, and continue to be instrumental in the detector design process We will continue to make contributions central to the detector development effort throughout the next year We will continue to define the detector performance and identify unique capabilities, such as supernova detection The arrival of Ryan Patterson will add considerable strength, allowing us to build on our founding roles in NO A software and analysis
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