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@PHDTHESIS{Ulrich:684349,
      author       = {Ulrich, Jascha},
      othercontributors = {Hassler, Fabian and Schoeller, Herbert},
      title        = {{L}arge impedances and {M}ajorana bound states in
                      superconducting circuits},
      school       = {RWTH Aachen University},
      type         = {Dissertation},
      address      = {Aachen},
      reportid     = {RWTH-2017-01921},
      pages        = {1 Online-Ressource (xiv, 173 Seiten) : Diagramme},
      year         = {2017},
      note         = {Auch veröffentlicht auf dem Publikationsserver der RWTH
                      Aachen University; Dissertation, RWTH Aachen University,
                      2017},
      abstract     = {Superconducting circuits offer the opportunity to study
                      quantum mechanics on mesoscopic scales unimpeded by
                      dissipation. This fact and the nonlinearity of the Josephson
                      inductance make it possible to use superconducting circuits
                      as artificial atoms whose long-lived states can be
                      selectively addressed and studied. A pronounced nonlinearity
                      of the energy spectrum, however, requires quantum
                      fluctuations of the flux across the Josephson junction which
                      are large on the scale of the superconducting flux quantum
                      $\Phi_Q = h/2e$. This implies charge fluctuations below the
                      single Cooper-pair limit via flux-charge duality. The
                      localization of charge leads to a strong susceptibility to
                      interactions with charges in the environment which has
                      motivated the search for schemes to decouple charges from
                      their environment. This thesis is concerned with theoretical
                      challenges arising from two complementary approaches to this
                      problem: the realization of large impedances and the
                      fractionalization of electrons by means of Majorana bound
                      states.In recent years, the decoupling of charges from the
                      environment through reactive large impedances, so-called
                      "superinductances" $L$, has attracted much interest. These
                      inductances feature small parasitic capacitance $C$ such
                      that the characteristic impedance $\sqrt{L/C}$ is much
                      larger than the superconducting resistance quantum $R_Q =
                      h/4e^2$. Superinductances have various applications ranging
                      from qubit designs such as the $0$-$\pi$ qubit or the
                      fluxonium to impedance matching, Bloch oscillations and the
                      stabilization of phase slips in superconducting nanowires.
                      Although there exists a well-established formalism for the
                      quantization of superconducting circuits in terms of node
                      fluxes, this formalism is ill-suited for the description of
                      fast flux transport with localized charges in
                      large-impedance environments. In particular, the nonlinear
                      capacitive behavior of phase slip junctions cannot be
                      modeled in a straightforward way using node fluxes. In view
                      of the ever growing interest in superinductances, in the
                      first part of the thesis, we present a recipe for
                      quantization of planar circuits in terms of loop charges. As
                      we will show, the loop charge approach is dual to the usual
                      node flux formalism and well-adapted to a large impedance
                      setting.In the second part of the thesis, we turn to a
                      complementary approach of charge decoupling by means of
                      Majorana bound states (MBS). MBS solve the decoupling
                      problem by encoding a fermionic mode nonlocally into two
                      bound states with large spatial separation such that a local
                      coupling to the stored charge is no longer possible. It has
                      been shown that despite the apparent nonlocality of the
                      fermionic mode, transport through the mode remains local
                      unless the MBS are coupled by a global perturbation like a
                      finite charging energy. Here we show that, even in absence
                      of charging energy, decoupling the superconductor from the
                      ground plane achieves subtle coupling of the MBS that leads
                      to nonlocal transport.Finally, in the last part of the
                      thesis, we turn to two mesoscopic applications related to
                      supersymmetric quantum mechanics. The simultaneous presence
                      of a fermionic mode due to the MBS and a bosonic mode due to
                      the Cooper-pair condensate makes systems involving MBS
                      appealing candidates for the realization of supersymmetric
                      quantum mechanics. For a Majorana Cooper-pair box, we
                      discuss an unusual "bosonic" supersymmetry and its
                      experimental signatures. Since MBS remain challenging to
                      realize experimentally, we show that a similar supersymmetry
                      can even be realized in a setup using standard
                      superconducting circuitry without MBS.},
      cin          = {137230 / 130000},
      ddc          = {530},
      cid          = {$I:(DE-82)137230_20140620$ / $I:(DE-82)130000_20140620$},
      typ          = {PUB:(DE-HGF)11},
      urn          = {urn:nbn:de:hbz:82-rwth-2017-019212},
      doi          = {10.18154/RWTH-2017-01921},
      url          = {https://publications.rwth-aachen.de/record/684349},
}