% IMPORTANT: The following is UTF-8 encoded. This means that in the presence
% of non-ASCII characters, it will not work with BibTeX 0.99 or older.
% Instead, you should use an up-to-date BibTeX implementation like “bibtex8” or
% “biber”.
@ARTICLE{Hell:824045,
author = {Hell, Michael and Wegewijs, Maarten Rolf and DiVincenzo,
David},
title = {{Q}ubit quantum-dot sensors: {N}oise cancellation by
coherent backaction, initial slips, and elliptical
precession},
journal = {Physical review / B},
volume = {93},
number = {4},
issn = {2469-9950},
address = {Woodbury, NY},
publisher = {Inst.},
reportid = {FZJ-2016-06669},
pages = {045418},
year = {2016},
abstract = {We theoretically investigate the backaction of a sensor
quantum dot with strong local Coulomb repulsion on the
transient dynamics of a qubit that is probed capacitively.
We show that the measurement backaction induced by the noise
of electron cotunneling through the sensor is surprisingly
mitigated by the recently identified coherent backaction [M.
Hell, M. R. Wegewijs, and D. P. DiVincenzo, Phys. Rev. B 89,
195405 (2014)] arising from quantum fluctuations. This
indicates that a sensor with quantized states may be
switched off better than naively expected. This
renormalization effect is missing in semiclassical
stochastic fluctuator models and typically also in
Born-Markov approaches, which try to avoid the calculation
of the nonstationary, nonequilibrium state of the qubit plus
sensor. Technically, we integrate out the current-carrying
electrodes to obtain kinetic equations for the joint,
nonequilibrium detector-qubit dynamics. We show that the
sensor current response, level renormalization, cotunneling
broadening, and leading non-Markovian corrections always
appear together and cannot be turned off individually in an
experiment or ignored theoretically. We analyze the
backaction on the reduced qubit state—capturing the full
non-Markovian effects imposed by the sensor quantum dot on
the qubit—by applying a Liouville-space decomposition into
quasistationary and rapidly decaying modes. Importantly, the
sensor cannot be eliminated completely even in the simplest
high-temperature, weak-measurement limit since the qubit
state experiences an initial slip depending on the initial
preparation of qubit plus sensor quantum dot. The slip
persists over many qubit cycles, i.e., also on the time
scale of the qubit decoherence induced by the backaction. A
quantum-dot sensor can thus not be modeled as usual as a
“black box” without accounting for its dynamical
variables; it is part of the quantum circuit. We furthermore
find that the Bloch vector relaxes (rate 1/T1) along an axis
that is not orthogonal to the plane in which the Bloch
vector dephases (rate 1/T2), blurring the notions of
relaxation and dephasing times. Moreover, the precessional
motion of the Bloch vector is distorted into an ellipse in
the tilted dephasing plane.},
cin = {IAS-3 / PGI-2 / JARA-FIT},
ddc = {530},
cid = {I:(DE-Juel1)IAS-3-20090406 / I:(DE-Juel1)PGI-2-20110106 /
$I:(DE-82)080009_20140620$},
pnm = {144 - Controlling Collective States (POF3-144)},
pid = {G:(DE-HGF)POF3-144},
typ = {PUB:(DE-HGF)16},
UT = {WOS:000368486600010},
doi = {10.1103/PhysRevB.93.045418},
url = {https://juser.fz-juelich.de/record/824045},
}