  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 [PRB 89, 195405] arising from
quantum fluctuations. 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, 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: The
qubit state experiences an initial slip that persists over many qubit cycles
and depends on the initial preparation of qubit plus sensor quantum dot. A
quantum-dot sensor can thus not be modeled as a 'black box' without accounting
for its dynamical variables. We furthermore find that the Bloch vector relaxes
(T1) along an axis that is not orthogonal to the plane in which the Bloch
vector dephases (T2), blurring the notions of T1 and T2 times. Finally, the
precessional motion of the Bloch vector is distorted into an ellipse in the
tilted dephasing plane.
