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Accurate Calibration of Raman Systems

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Abstract

The work in hand is focused thematically on the accurate calibration of a Raman system at the Karlsruhe Tritium Neutrino Experiment (KATRIN).

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Notes

  1. 1.

    \(Z\) and \(A\) are atomic number (number of protons) and mass number (number of nucleons), respectively.

  2. 2.

    The “standard” neutrinos are dubbed Dirac neutrinos.

  3. 3.

    Note that this matrix is similar to the unitarian Cabbibo-Kobayashi-Maskawa (CKM) matrix in the quark sector [60].

  4. 4.

    LNGS is the Gran Sasso Underground Laboratory in Italy.

  5. 5.

    There are also no left-handed \(\bar{\nu }_{L}\) single states for anti-neutrino.

  6. 6.

    The Hermitian conjugate is abbreviated by \(h.c.\)

  7. 7.

    Originally proposed by M. Goeppert-Mayer in 1935 [45].

  8. 8.

    Originally suggested by H. W Furry in 1939 [37].

  9. 9.

    The helicity is defined as the projection of the spin \(\varvec{s}\) onto the momentum direction \(\mathbf{{p}}\): \(H=(\mathbf{{s}}\cdot \mathbf{{p}})/(|\mathbf{{s}}|\cdot |\mathbf{{p}}|)\).

  10. 10.

    This term denotes in principle that a massive neutrino has two helicity components.

  11. 11.

    In specific cases even a black hole is formed.

  12. 12.

    MARE \(=\) Microcalorimeter Arrays for a Rhenium Experiment.

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  1. Tritium Laboratory Karlsruhe, Karlsruhe Institute of Technology, Institute for Technical Physics, Eggenstein-Leopoldshafen, Germany

    Magnus Schlösser

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Schlösser, M. (2014). Introduction. In: Accurate Calibration of Raman Systems. Springer Theses. Springer, Cham. https://doi.org/10.1007/978-3-319-06221-1_1

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