R&D status of the Scintillator- strip based ECAL for the ILD Oct LCWS14 Belgrade Satoru Uozumi (KNU) For the CALICE collaboration Scintillator strips.

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Presentation transcript:

R&D status of the Scintillator- strip based ECAL for the ILD Oct LCWS14 Belgrade Satoru Uozumi (KNU) For the CALICE collaboration Scintillator strips For active & fine granular sensor

Contents Introduction of the Scintillator-strip ECAL (ScECAL) – Principle & structure – Physical & Technological prototypes Improvements ongoing – Hardware … optimization of scintillator shape and optical signal readout – Software … hit strip →cluster reconstruction Evaluation of Jet Energy Resolution (JER)

Introduction : Why ScECAL? First requirement : high granularity to improve jet energy resolution Second requirement : chop the calorimeters as small as possible ☆ Need 5 mm x 5 mm effective segmentation → Strip idea Orthogonally aligned strips with Pixelated Photo Detector (PPD) make “virtual cells”. ~ 10 7 strips ☆ Low cost. ☆ many established technologies ☆ Challenge with new Si-photo sensor ☆ Timing resolution < 1 ns 5 x 45 mm Plastic scintillator

Two scintillator layers in an alveolar make a sandwich structure with a tungsten absorber. Strip directions are orthogonal to each other. base board Scintillator layer (x) W absorber base board Cu radiator Scintillator layer (z) Mechanical design of the barrel and the endcaps is developed by CALICE ECAL group. “Alveolar” frame structure is made with tungsten absorber. Strip ScECAL in the ILD

5 Physics & technological prototypes

6 180x 180mm 2 x30 layers 2160 ch Physics prototype (BT will be published to NIM) (unit mm) An array of strips in a layer LED light is distributed to each channel by those fibers 9 MPPCs on a cable Scintillator strip with MPPC and WLS fiber

Two layers of Technological prototype 3 GeV e - Tungsten plate in front of ECAL Ecal behind AHCAL :-) two-layers ECAL two-layers HCAL one HCAL channel corresponds 6x6 ECAL segmentations 2013

8 Improvements of scintillator & photo-sensor components

Granularity 10mm → 5mm … hard step 90 Sr Baseline design: -Photon yield (~10p.e.) is OK -Uniformity is almost OK except very close side of the photo-sensor Beta-ray scanning system Any idea to uniformize scitillator-strip response?? → next

New ideas 10 dead area,0.9mm MPPC base board Scintillator Baseline design has Tokyo Group 45 mm 1-2 mm MPPC sensor 4 mm 0.5mm MC 0.25 mm 1x1mm x4mm 2 Bottom readout with wedge

Wedge-type readout strip (Otani Many wedge types are tested Current best solution (by horizontal beta-ray scan) Better response uniformity than baseline design High light yield

Wedge-type readout : implementation Oct 8th 2014 ~

New idea : readout by ｒ ectangular PPD & tapered scintillator Scintillator strip Sensitive area PPD max – min ~ 7% Light strength Tapered scintillator and PPD with ｒ ectangu ｌ ar PPD is a new idea to absorb response non- uniformity Simple MC simulation result shows ~7% of non-uniformity Asking Hamamatsu to provide the ｒ ectangular PPD MC simulation result

14 PPD (MPPC) development We were (are) requiring : lower noise rate, cross-talk, afterpulse : high Photon Detection Efficiency : large number of pixels to Hamamatsu K.K. Saturation effect is drastically improved!

15 Development of Reconstruction software

Jet energy GeV 16 cos(θ_Thrust) < 0.7 (Barrel) RMS90: RMS of 90% of center events SSA makes JER of strip ECAL close to 5 x 5 mm 2 tile ECAL 45 x 5 mm 2 ScECAL w SSA DBD result (SiW ECAL) 5 x 5 mm 2 tile ScECAL 15 x 15 mm 2 tile ScECAL 45 x 5 mm 2 ScECAL w/o SSA Difference is only %. PFA algorithm = PandoraPFA alternate(45 x 5+10 x 10) mm 2 ScECAL w 2 step SSA Study with more realistic MC simulation is currently underway. Shinshu)

Summary & Plans The ScECAL is being established through physics & technological prototypes Further improvement of scintillator components & PPDs are actively underway At this moment, test beam of the wedge-type scintillator is ongoing! Cluster reconstruction study shows reasonable performance with Strip Splitting Algorithim. Next Goal : determine the detector design in couple of years.

Backup

1600 pix 2500 pix PPD(MPPC) measured linearity

20 Physics prototype GeV electron (at Fermilab) Maximum deviation : 1.6±0.7% dataMC stochastic term 12.8±0.1± ±0.08 constant term 1.0± ± Linearity and Resolution difference < 1 σ

21 Strip Split Algorithm Left: position accuracy and precision Error bar (RMS) < 1 mm w/ SSA. Middle: Energy is recovered correctly w/ SSA. Right: Jet energy resolution is kept w/ SSA. Position of 10 GeV photonEnergy sum of 2 x 100 GeV jet Energy resln. 100 GeV Jet 5mm W, 1 mm T Sc. strip Sc strip Energy deposits are redistributed into 5x5 mm 2 virtual cells referring hits in the nearest layers. strips in the nearest layers have orthogonal direction.