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Sack, Rudolf: Measurement of the energy loss of 18.6 keV electrons on deuterium gas and determination of the tritium Q-value at the KATRIN experiment. 2020
Inhalt
Abstract
Abstract (deutsch)
Summary
Zusammenfassung
Neutrino physics
Postulation and discovery
Neutrinos in the Standard Model
Neutrino oscillation
Search for δCP:
Hint at mass ordering:
Neutrino mass theory
Seesaw mechanism
Neutrino mass determination
Observational cosmology
Neutrinoless double beta decay 0νββ
Direct neutrino mass measurements from the kinematics of weak decays
KATRIN experiment
Measurement principle
Tritium beta spectrum
MAC-E-Filter
Electric filtering
Magnetic adiabatic collimation
Energy resolution
Magnetic mirror
Magnetic flux tube
Transmission of the main spectrometer
Background of the main spectrometer
Source and transport section (STS)
Stability of the source
Temperature stability
Tritium circulation
Transport section
Differential pumping section
Cryogenic pumping section
Spectrometer and detector section (SDS)
Pre spectrometer (PS)
Main spectrometer (MS)
Focal plane detector - FPD
Monitor spectrometer - MoS
High voltage at KATRIN
Calibration and monitoring tools
Rear wall and instrumentation
Activity monitoring
Composition monitoring
Precision electron sources
Precision photoelectron source
Working principle and concept
Description of the e-gun flange
Optical components
Optics box and light sources
Laser driven light source
Pulsed UV-laser
HV concept of the electron gun
Measurements with the electron gun at a test stand
Photoelectron gun in KATRIN:
Vacuum system
Electromagnetic design of the rear section
Rate and rate stability
Beam diameter
Transmission function
Zero angle
Transmission function measurements with higher B-field and non-zero angles
Energy loss due to scattering with D2 molecules
General idea of electron scattering in KATRIN
Response function
Details on scattering in KATRIN
Energy loss measurement on deuterium in STS3a
Integral measurement
Time of flight method
Measurement and data handling
Novel parametrization for energy loss model with BED ionization tail
Fit of the Eloss data
Mean energy loss comparison with stopping power
Comparison with other energy loss models
Discussion and outlook
Q-value of tritium
Motivation to measure the Q-value
Q-value from other experiments
Endpoint and recoil
Determination of Q(T2) in KATRIN
Overview over the potentials in KATRIN
Fowler method
Corrections to the measured data
Work function of the e-gun
Determination of the spectrometer work function
Stability of the work functions
Work function of the rear wall
Work function investigations in STS3a
Summary of RW work function investigations
Starting potential in the WGTS
Q-value of tritium in the first tritium campaign
Q-value of tritium in the first science run of KATRIN
Possible plasma instabilities in KATRIN
General introduction to plasma instabilities
General Introduction
Current driven instability in partially ionised media
Plasma instability in the Whistler mode caused by a gyrating electron stream
Two stream instability
Appendix
Eloss results
Contact potential difference with Kelvin probe on rear wall
Plasma