Abstract

The KArlsruhe TRItium Neutrino (KATRIN) experiment, which aims to make a direct and model-independent determination of the absolute neutrino mass scale, is a complex experiment with many components.More than 15 years ago, we published a technical design report (TDR) [1] to describe the hardware design and requirements to achieve our sensitivity goal of 0.2 eV at 90% C.L. on the neutrino mass.Since then there has been considerable progress, culminating in the publication of first neutrino mass results with the entire beamline operating [2].In this paper, we document the current state of all completed beamline components (as of the first neutrino mass measurement campaign), demonstrate our ability to reliably and stably control them over long times, and present details on their respective commissioning campaigns.

Highlights

  • The determination of the neutrino mass plays an important role in cosmology, particle physics, and astroparticle physics

  • The results shown in figure 19 yield the specified homogeneity of ±10 % over the entire Rear Wall (RW) up to its maximal radius of 7 cm

  • The upgrade has been successfully used for the e-gun operating in pulse mode with varying multiplicities per pulse and varying spread in arrival times; this resulted in challenging peak pile-up situations at ∼10 kcps/pixel, but use of an algorithm, utilizing the bipolar shaper information, accurate counting with less than 0.1% correction errors was achieved

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Summary

Introduction

The determination of the neutrino mass plays an important role in cosmology, particle physics, and astroparticle physics. This paper, which builds on the original technical design report (TDR) [1], will focus on hardware implementation and commissioning results, and various systems for calibration and monitoring. It describes the status of all systems as they were during the first neutrino mass measurement campaign. The hardware implementation is described in the corresponding sections below, which include the source, transport, spectrometer, and detector sections. Each of these has undergone its respective commissioning phase. Additional systems for monitoring every operating parameter — from the source gas composition and activity to the adjustment of the spectrometer’s high voltage — have successfully demonstrated the KATRIN experiment’s ability to meet its design requirements for stability and control

Setup of the KATRIN experiment
Key parameters of the KATRIN experiment
Measurement modes
Windowless gaseous tritium source
WGTS principle and basic requirements
WGTS magnet cryostat system
Magnet system setup
80 K–103 K
Setup of the beam tube cooling system
Commissioning of the WGTS magnet cryostat system
Tritium loops
Tritium loops overview
KATRIN tritium loop system setup
Potential definition
Rear wall setup
Transport system
DPS principle and basic requirements The basic requirements for the DPS are:
Magnet system
Pumping system
Commissioning results
CPS principle and basic requirements
Magnet-cryostat setup
Argon cryo pump
Commissioning results with the magnet-cryostat system
Commissioning results with the argon frost pump
Spectrometer system
Spectrometer principle and basic requirements
Main spectrometer related background
Penning trap between the pre- and main spectrometers
F10 CF100 CF40
Detector system
Third-Shaped 0
Calibration and monitoring systems
Data management and control systems
Findings
Summary
Full Text
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