29 June 2018 to 4 July 2018
IBS HQ, Daejeon, Korea
Asia/Seoul timezone
There will be Welcome Reception at 18:00 on June 28, 2018

Session

Parallel Session 1-8

3 Jul 2018, 16:30
IBS HQ, Daejeon, Korea

IBS HQ, Daejeon, Korea

Conveners

Parallel Session 1-8: BD

  • Loredana Gastaldo (Heidelberg University, Kirchhoff Institute for Physics)

Presentation materials

There are no materials yet.

  1. Prof. Gray Rybka (University of Washington)
    03/07/2018, 16:30
    Oral
    Project 8 has demonstrated Cyclotron Radiation Emission Spectroscopy (CRES) as a novel technique for performing electron spectroscopy. Applying this method to highest energy electrons from tritium beta decay will lead to a direct neutrino mass measurement. A proof of this concept was performed with a waveguide detector utilizing monoenergetic 83mKr conversion electrons. The demonstrator has...
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  2. Prof. Angelo Nucciotti (Dip. di Fisica, U. Milano-Bicocca / INFN Sez. Milano-Bicocca, Italy)
    03/07/2018, 17:00
    Oral
    The assessment of the neutrino absolute mass scale remains one of the most crucial challenges in today particle physics and cosmology. Nuclear beta decay spectrum end-point study is currently the only experimental method to provide a model independent measurement of the lowest neutrino mass. HOLMES is an experiment to directly measure the electron neutrino mass by performing a calorimetric...
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  3. Dr Wonqook Choi (Karlsruher Institut für Technologie (KIT))
    03/07/2018, 17:30
    Oral
    The goal of the \textbf{KA}rlsruhe \textbf{TRI}tium \textbf{N}eutrino (KATRIN) experiment is the determination of the electron neutrino mass $m(\nu_\mathrm{e})$ with a sensitivity of $0.2$\,eV/c$^2$ (90$\%$ C.L.) by measuring an integrated energy spectrum of electrons from tritium $\beta$-decay. The measurement of the tritium $\beta$-spectrum close to its endpoint at $E_0 =...
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  4. Mr Joel Kostensalo (University of Jyväskylä)
    03/07/2018, 18:00
    Oral
    Highly-forbidden non-unique beta-decays are known to have electron-spectrum shapes which depend on the effective value of the axial vector coupling constant $g_{\rm A}$ [1, 2]. Resent calculations show that this is also the case for many first-forbidden non-unique decays. Moreover, the spectral shapes of first-forbidden $J^{+}\leftrightarrow \, J^{-}$ decays with $J\neq 0$ are found to depend...
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