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Optical Track Imaging in KamLAND: Enhancing Track Reconstruction and Vertex Localization

This paper discusses the use of optics to image tracks in the KamLAND scintillator "bubble chamber" and the potential benefits it could provide in terms of track reconstruction and precise vertex localization. The study was conducted by John Learned at the Gatlinburg KamLAND Collaboration meeting, with assistance from Byron Dieterle.

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Optical Track Imaging in KamLAND: Enhancing Track Reconstruction and Vertex Localization

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  1. Tracking in KamLAND?CAN WE USE OPTICS TO IMAGE TRACKS AND WHAT WOULD IT GET US? John Learned at Gatlinburg 4/05 John Learned University of Hawaii At KamLAND Collaboration meeting Gatlinburg, Tennessee, 4/05 Byron Dieterle has done optical studies, thought about problem, and been a great help in developing this idea.

  2. Basic Idea: a Scintillator “Bubble Chamber” • If we can design the optics with enough light collection adequate depth of field • and not much rescattering of light • Reconstruct tracks and precise vertices. John Learned at Gatlinburg 4/05

  3. KamLAND Physics Applications • Accelerator neutrinos: superior recognition of electron events and rejection of πos. • PDK: excellent K mode resolution. • SN: resolution of direction. • Reactors: better e+-n direction resolution. • Solar Nu’s: Some directionality. • Muons: very accurate track reconstruction, increased rejection of backgrounds. • Nuclearites, Q-Balls, etc. : not presently recorded in SK or KL (?)… opportunity. John Learned at Gatlinburg 4/05

  4. Sensitivity & Implications • Aperture: assume 8 x 17”PMTs (~1.2m pupil) • Similar QE, efficiency • Assume 8 wide field cameras • ~2.4 PE/cm track in each camera • 40 MeV track yields ~200 pixels • 1 MeV yields ~10 pixels • Aim for resolution ~4 mm • Implies camera with ~4M pixels => commerically available CCDs John Learned at Gatlinburg 4/05

  5. 4,500x3,000 (14M) pix. Commercial CMOS Camera PMT-array Camera CMOS Sensor Chip Starting point: ASHRA Imaging Particle Detector Ideas and leader: Makoto Sasaki, ICRR Key Technology 9M-pix. CMOS Sensor Covering 50deg-FoV John Learned at Gatlinburg 4/05 Pixel Cost Reduction by O(104)

  6. Design of Ashra Optics Modified Baker-Nunn • Schmidt-type optics • Spherical segment mirror • Spherical focal surface • 3-element corrector lens John Learned at Gatlinburg 4/05 • Advantage: a large degree of freedom for optimization of lens surface shape to cancel • spherical aberration • chromatic aberration. pupil : 1m F/0.74 Details can be found in M.Sasaki et al, NIM A492 (2002) 49

  7. incident angle Performance of Ashra Optics Spot diagram after optimization wavelength 4 largest peaks in air-fluorescence spectra John Learned at Gatlinburg 4/05 incident angle

  8. incident angle performance of Ashra Optics Ashra Optics has capability to achieve 1 arcmin resolution within the whole FOV of ± 25° Spot size = 0.0167°(1 arcmin) John Learned at Gatlinburg 4/05 from weighted sum of several wavelength using ZEMAX by A.Okumura

  9. 3mφmirror 1 deg/Pix 3mφmirror 1 deg/Pix 3mφmirror 1 deg/Pix 3mφmirror 1 deg/Pix 3mφmirror 1 arcmin/Pix ASHRA 3mφmirror 1 arcmin/Pix Angular Resolution 1arcmin • < 1 arcmin at E > 1018.5eV • 0.3 arcmin at E ~ 1020eV What this does for ASHRA EAS air fluorescence angular resolution John Learned at Gatlinburg 4/05

  10. 2/3 scale prototype R&D 状況ー2/3モデル望遠鏡 • I.I. • 補正レンズ • ミラー John Learned at Gatlinburg 4/05

  11. Proximity focused I.I. Lens I.I. photocathode Incident photons photon phosphor screen gate pulse >5ns commercial ASHRA I.I. Minimum modification of focal surface Focal sphere => => CMOS Sensor Image Intensifier Pipeline John Learned at Gatlinburg 4/05 • 4.6 Lp/mm =>σ~70μm @ input surface • de-magnification factor ~ 10 • 46 Lp/mm => σ~7μm ~ CCD pix. size • magnification factor = 1

  12. Large Diameter Image Intensifier Existing 16” (400mm)φphotocathode John Learned at Gatlinburg 4/05 • photocathode resolution 3.4 line pair/mm (largest and finest resolution in world) • 24“ under development (but maybe 20” limit)

  13. Prototype Image Pipeline Not needed for KL application John Learned at Gatlinburg 4/05

  14. Add Cameras to KamLAND? Would require draining the detector: stopper? Present idea based on ASHRA size camera. Maybe smaller camera which replaces 1 PMT and requires no cutting steel, but then need More cameras. John Learned at Gatlinburg 4/05

  15. Beam4 Calculations Simple setup, easy to get started Start with Sasaki design Can do simple optimization Example of card file below: • 9 surfaces sas16.opt Diameter dia index Zvx Curv A4 A6 A8 shape Mir/Lens --------------:--------:----------:---------:----------------:------------------:---------------:--------------:---------:------------: • 2.400 : : : -.22 : -0.0 : 0. : 0. : 0. : 1. : lens : L1 • 2.400 : : 1.414 : -.195 : -0.0013394: 0.07467649 : 0.0011911: 0. : 1. : lens : L1 • 2.000 : : : -.05 : 0.0130258:-0.06570667 :-0.0011347:-0.000453 : 1. : lens : L2 • 2.000 : : 1.414 : 0.0 : -0.0 : 0. : 0. : 0. : : iris : L2 2.000 : : 1.414 : .05 : -0.0130258: 0.06570667 : 0.0011347: 0.000453 : 1. : lens : L2 2.400 : : : .195 : 0.0013394:-0.07467649 :-0.0011911: 0. : 1. : lens : L3 • 2.400 : : 1.414 : .22 : -0.0 : 0. : 0. : 0. : 1. : lens : L3 • 2.400 : : :1.50 :-.667 : : : : 1. : mirror : M • 0.400 : : :0.694 :-1.441 : : : : 1. : other : D John Learned at Gatlinburg 4/05 Calculations by Byron Dieterle

  16. Byron has done some Beam4 Sims for KL-like Geometry John Learned at Gatlinburg 4/05 Conclude: resolutions of order of mm are achieved at IIT.

  17. Image of a Track John Learned at Gatlinburg 4/05 Use tomographic methods to reconstruct out of focus image.

  18. Conclusion • Idea to add imaging to KamLAND needs study…. optics, design practicality, sensitivity, reconstruction. • How about small camera in place of a neck 6” PMT? Could do muon tracks, nuclearites? • Biggest question: does it buy us something really important? • Should we pursue it? Anyone interested? John Learned at Gatlinburg 4/05

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