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000599299 037__ $$aPUBDB-2023-07306
000599299 041__ $$aEnglish
000599299 1001_ $$0P:(DE-H253)PIP1103471$$aAthanassiadis, Antonios$$b0$$eCorresponding author
000599299 1112_ $$a9. Annual Matter and Technologies Meeting$$cKIT Karlsruhe$$d2023-10-09 - 2023-10-10$$wGermany
000599299 245__ $$aA Cherenkov detector for high-rate electron detection in the LUXE experiment
000599299 260__ $$c2023
000599299 3367_ $$033$$2EndNote$$aConference Paper
000599299 3367_ $$2BibTeX$$aINPROCEEDINGS
000599299 3367_ $$2DRIVER$$aconferenceObject
000599299 3367_ $$2ORCID$$aCONFERENCE_POSTER
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000599299 3367_ $$0PUB:(DE-HGF)24$$2PUB:(DE-HGF)$$aPoster$$bposter$$mposter$$s1703076352_3513259
000599299 502__ $$cUniversität Hamburg
000599299 520__ $$aThe Laser Und XFEL Experiment (short LUXE) based at DESY, Hamburg is aplanned experiment to study nonlinearity effects in the strong-field QED regimewith high precision.In order to create electric fields stronger than the so-called Schwinger limit, it isplanned to collide a high-intensity laser pulse with either high-energy electronsup to 16.5 GeV or high-energy photons.As a result, non-linear Compton scattering or Breit-Wheeler interactions willtake place, leading to a laser-intensity-dependent shift of the Compton edge andthe appearance of higher-order harmonics in the energy spectrum. One of thechallenges of measuring the Compton energy spectrum in laser-electron-beamcollisions is the expected flux of outgoing Compton-scattered electrons andphotons, ranging from $10^3$ to $10^9$ particles per collision.This contribution will present the simulation-based design of an electronflux-resistant Cherenkov detector prototype, first testbeam results as well asoptical simulation studies. Further optimisation of the various components aswell as reconstruction algorithms will be discussed.
000599299 536__ $$0G:(DE-HGF)POF4-622$$a622 - Detector Technologies and Systems (POF4-622)$$cPOF4-622$$fPOF IV$$x0
000599299 693__ $$0EXP:(DE-H253)LUXE-20220501$$5EXP:(DE-H253)LUXE-20220501$$eLaser Und XFEL Experiment$$x0
000599299 7001_ $$0P:(DE-H253)PIP1028638$$aJacobs, Ruth Magdalena$$b1$$udesy
000599299 7001_ $$0P:(DE-H253)PIP1005630$$aList, Jenny$$b2$$udesy
000599299 7001_ $$0P:(DE-H253)PIP1011115$$aMoortgat-Pick, Gudrid$$b3$$udesy
000599299 7001_ $$0P:(DE-H253)PIP1101170$$aRanken, Evan$$b4$$udesy
000599299 7001_ $$0P:(DE-H253)PIP1001586$$aSchmitt, Stefan$$b5$$udesy
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000599299 9101_ $$0I:(DE-588b)2008985-5$$6P:(DE-H253)PIP1103471$$aDeutsches Elektronen-Synchrotron$$b0$$kDESY
000599299 9101_ $$0I:(DE-588b)2008985-5$$6P:(DE-H253)PIP1028638$$aDeutsches Elektronen-Synchrotron$$b1$$kDESY
000599299 9101_ $$0I:(DE-588b)2008985-5$$6P:(DE-H253)PIP1005630$$aDeutsches Elektronen-Synchrotron$$b2$$kDESY
000599299 9101_ $$0I:(DE-588b)2008985-5$$6P:(DE-H253)PIP1011115$$aDeutsches Elektronen-Synchrotron$$b3$$kDESY
000599299 9101_ $$0I:(DE-588b)2008985-5$$6P:(DE-H253)PIP1101170$$aDeutsches Elektronen-Synchrotron$$b4$$kDESY
000599299 9101_ $$0I:(DE-588b)2008985-5$$6P:(DE-H253)PIP1001586$$aDeutsches Elektronen-Synchrotron$$b5$$kDESY
000599299 9131_ $$0G:(DE-HGF)POF4-622$$1G:(DE-HGF)POF4-620$$2G:(DE-HGF)POF4-600$$3G:(DE-HGF)POF4$$4G:(DE-HGF)POF$$aDE-HGF$$bForschungsbereich Materie$$lMaterie und Technologie$$vDetector Technologies and Systems$$x0
000599299 9141_ $$y2023
000599299 9201_ $$0I:(DE-H253)FTX-20210408$$kFTX$$lTechnol. zukünft. Teilchenph. Experim.$$x0
000599299 980__ $$aposter
000599299 980__ $$aVDB
000599299 980__ $$aI:(DE-H253)FTX-20210408
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