Solid Winston Cones Uni & ETH Zürich. 2 Basic Differences Primary refraction -> larger input angles...
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Transcript of Solid Winston Cones Uni & ETH Zürich. 2 Basic Differences Primary refraction -> larger input angles...
![Page 1: Solid Winston Cones Uni & ETH Zürich. 2 Basic Differences Primary refraction -> larger input angles accepted typical caveats: - false traces by muons.](https://reader030.fdocuments.us/reader030/viewer/2022032709/56649ec75503460f94bd4336/html5/thumbnails/1.jpg)
Solid Winston Cones
Uni & ETH Zürich
![Page 2: Solid Winston Cones Uni & ETH Zürich. 2 Basic Differences Primary refraction -> larger input angles accepted typical caveats: - false traces by muons.](https://reader030.fdocuments.us/reader030/viewer/2022032709/56649ec75503460f94bd4336/html5/thumbnails/2.jpg)
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Basic Differences
Primary refraction -> larger input angles accepted
typical caveats:- false traces by muons -> high line signal- UV transmittance -> select material- more NSB
Benefits:- larger collection efficiency- protection of light sensor- less Fresnel reflection
than at layer near detector- mass production
![Page 3: Solid Winston Cones Uni & ETH Zürich. 2 Basic Differences Primary refraction -> larger input angles accepted typical caveats: - false traces by muons.](https://reader030.fdocuments.us/reader030/viewer/2022032709/56649ec75503460f94bd4336/html5/thumbnails/3.jpg)
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Simulations
Home-made Ray Tracer includes:- reflection (usually assume 95%)- refraction- Fresnel Reflection- Absorption in medium ( dep.)- Detector properties (resin, I())
(Simple Output example)
![Page 4: Solid Winston Cones Uni & ETH Zürich. 2 Basic Differences Primary refraction -> larger input angles accepted typical caveats: - false traces by muons.](https://reader030.fdocuments.us/reader030/viewer/2022032709/56649ec75503460f94bd4336/html5/thumbnails/4.jpg)
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General Results
cone height: - changes shape of cutoff- little influence on position- optimum depends on reflectivity
![Page 5: Solid Winston Cones Uni & ETH Zürich. 2 Basic Differences Primary refraction -> larger input angles accepted typical caveats: - false traces by muons.](https://reader030.fdocuments.us/reader030/viewer/2022032709/56649ec75503460f94bd4336/html5/thumbnails/5.jpg)
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General Results
cone shape:- parabolic walls - hex-square possible without losses- same input area:solids gain signal, but loose S/N for same h
![Page 6: Solid Winston Cones Uni & ETH Zürich. 2 Basic Differences Primary refraction -> larger input angles accepted typical caveats: - false traces by muons.](https://reader030.fdocuments.us/reader030/viewer/2022032709/56649ec75503460f94bd4336/html5/thumbnails/6.jpg)
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Area concentration - empty cones
hex-squareR = 95%Do = 2.7 mmh = 20 m
Di/mm factor 4 1.9 82.3 6 4.3 86.4 8 7.6 78.6 10 11.9 57.1
![Page 7: Solid Winston Cones Uni & ETH Zürich. 2 Basic Differences Primary refraction -> larger input angles accepted typical caveats: - false traces by muons.](https://reader030.fdocuments.us/reader030/viewer/2022032709/56649ec75503460f94bd4336/html5/thumbnails/7.jpg)
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Area concentration - solid cones
R = 95%Do = 2.7 mmh = 20 m
Di/mm 4 86.7 6 88.3 8 87.2 10 75.2
![Page 8: Solid Winston Cones Uni & ETH Zürich. 2 Basic Differences Primary refraction -> larger input angles accepted typical caveats: - false traces by muons.](https://reader030.fdocuments.us/reader030/viewer/2022032709/56649ec75503460f94bd4336/html5/thumbnails/8.jpg)
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Comparison open-solid
R = 95%Di = 7.62 mmDo = 2.8 mmh = 20 m
open: 83.9% / 82.1% efficiencysolid: 89.1% / 88.0 % efficiency
![Page 9: Solid Winston Cones Uni & ETH Zürich. 2 Basic Differences Primary refraction -> larger input angles accepted typical caveats: - false traces by muons.](https://reader030.fdocuments.us/reader030/viewer/2022032709/56649ec75503460f94bd4336/html5/thumbnails/9.jpg)
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Additional Tests Implemented
Surface flatness
regions of different refractive index
simulations for non-flat angluar response of detector
![Page 10: Solid Winston Cones Uni & ETH Zürich. 2 Basic Differences Primary refraction -> larger input angles accepted typical caveats: - false traces by muons.](https://reader030.fdocuments.us/reader030/viewer/2022032709/56649ec75503460f94bd4336/html5/thumbnails/10.jpg)
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Prototpes
simple pyramid cone made from N-FK5 glass(cut & polished, ETH)
hex-square geometrymade from plexiglass(cut, UZH)
![Page 11: Solid Winston Cones Uni & ETH Zürich. 2 Basic Differences Primary refraction -> larger input angles accepted typical caveats: - false traces by muons.](https://reader030.fdocuments.us/reader030/viewer/2022032709/56649ec75503460f94bd4336/html5/thumbnails/11.jpg)
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Test “Camera“ (Uni ZH)
![Page 12: Solid Winston Cones Uni & ETH Zürich. 2 Basic Differences Primary refraction -> larger input angles accepted typical caveats: - false traces by muons.](https://reader030.fdocuments.us/reader030/viewer/2022032709/56649ec75503460f94bd4336/html5/thumbnails/12.jpg)
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Summary
use solid cones for large area concentration-> cheaper camera
good performance of hex-square geometrytransmission OK down to 300 nm (or lower)reduces Fresnel lossescan be combined with protective window