Tracking in KamLAND? CAN WE USE OPTICS TO IMAGE TRACKS AND WHAT WOULD IT GET US? - PowerPoint PPT Presentation

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Tracking in KamLAND? CAN WE USE OPTICS TO IMAGE TRACKS AND WHAT WOULD IT GET US?

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The advantage of this optics is a large degree of freedom for optimization of lens surface shape to cancel spherical aberration and chromatic aberration. – PowerPoint PPT presentation

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Title: Tracking in KamLAND? CAN WE USE OPTICS TO IMAGE TRACKS AND WHAT WOULD IT GET US?


1
Tracking in KamLAND?CAN WE USE OPTICS TO IMAGE
TRACKS AND WHAT WOULD IT GET US?
  • 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.

3
KamLAND Physics Applications
  • Accelerator neutrinos superior recognition of
    electron events and rejection of pos.
  • PDK excellent K mode resolution.
  • SN resolution of direction.
  • Reactors better e-n direction resolution.
  • Solar Nus Some directionality.
  • Muons very accurate track reconstruction,
    increased rejection of backgrounds.
  • Nuclearites, Q-Balls, etc. not presently
    recorded in SK or KL (?) opportunity.

4
Sensitivity Implications
  • Aperture assume 8 x 17PMTs (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
  • gt commerically available CCDs

5
Starting point ASHRA Imaging Particle Detector
Ideas and leader Makoto Sasaki, ICRR
Key Technology 9M-pix. CMOS Sensor Covering
50deg-FoV
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
  • Advantage a large degree of freedom for
    optimization of lens surface shape to cancel
  • spherical aberration
  • chromatic aberration.

F/0.74
pupil 1m
Details can be found in M.Sasaki et al, NIM A492
(2002) 49
7
Performance of Ashra Optics
Spot diagram after optimization
wavelength
4 largest peaks in air-fluorescence spectra
incident angle
8
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)
from weighted sum of several wavelength
using ZEMAX by A.Okumura
9
What this does for ASHRA EAS air fluorescence
angular resolution
10
RD ???2/3??????
  • I.I.
  • ?????
  • ???

11
Image Intensifier Pipeline
Focal sphere gt
gt CMOS Sensor
  • 46 Lp/mm gt s7µm CCD pix. size
  • magnification factor 1
  • 4.6 Lp/mm gts70µm _at_ input surface
  • de-magnification factor 10

12
Large Diameter Image Intensifier
Existing 16 (400mm)fphotocathode
  • 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
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.
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

Calculations by Byron Dieterle
16
Byron has done some Beam4 Sims for KL-like
Geometry
Conclude resolutions of order of mm are achieved
at IIT.
17
Image of a Track
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?
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