Abstract

We consider a feedback control loop rectifying particle transport through a single quantum dot that is coupled to two electronic leads. While monitoring the occupation of the dot, we apply conditional control operations by changing the tunneling rates between the dots and its reservoirs, which can be interpreted as the action of a Maxwell demon opening or closing a shutter. This can generate a current at equilibrium or even against a potential bias, producing electric power from information. While this interpretation is well-explored in the weak-coupling limit, we can address the strong-coupling regime with a fermionic reaction-coordinate mapping, which maps the system into a serial triple quantum dot coupled to two leads. There, we find that a continuous projective measurement of the central dot would lead to a complete suppression of electronic transport due to the quantum Zeno effect. In contrast, a microscopic model for the quantum point contact detector implements a weak measurement, which allows for closure of the control loop without inducing transport blockade. In the weak-coupling regime between the central dot and its leads, the energy flows associated with the feedback loop are negligible, and the information gained in the measurement induces a bound for the generated electric power. In contrast, in the strong coupling limit, the protocol may require more energy for opening and closing the shutter than electric power produced, such that the device is no longer information-dominated and can thus not be interpreted as a Maxwell demon.

Highlights

  • In the famous thought experiment, Maxwell’s demon is an intelligent being that measures the direction and speed of particles in a box with two compartments

  • The weak measurement is described by a positive operator-valued measures (POVMs), which depends on two dimensionless parameters x and y and can be written as a minimally disturbing measurement [29], which after observing n tunneled quantum point contact (QPC) electrons during measurement interval τ acts on the triple quantum dot system (TQD) system density matrix ρ as

  • We have considered the performance of an externally controlled feedback loop implementing an electronic Maxwell demon

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Summary

INTRODUCTION

In the famous thought experiment, Maxwell’s demon is an intelligent being that measures the direction and speed of particles in a box with two compartments. In contrast to classical systems, which ideally remain unaltered by the measurement alone, the dynamics of quantum systems is modified already by a measurement, which can have drastic consequences such as the quantum Zeno effect While this second approach appears closer to the original setup and may be more flexible, it has the disadvantages that its theoretical discussion and experimental implementation are demanding regarding the inclusion of the quantum measurement process and the fidelity of measurement and control steps, respectively. We will see that projective measurements will imply Zeno-related modifications [28] to the Maxwell demon dynamics, which requires a generalized discussion of the control loop including weak measurements [29].

SQD with projective measurements
TQD without measurements
TQD with projective measurements and Zeno blockade
TQD with weak measurements
TQD with feedback
THERMODYNAMICS
Heat flow during conditional evolution
Heat during measurement
Switching work
First law
Second law
NUMERICAL RESULTS
Weak-coupling regime
Towards strong coupling
Coarse-graining effects
SUMMARY
Measurement dissipator without counting fields
Measurement dissipator in the presence of QPC electron counting
Example
Spectrum
Correlation functions
Born-Markov master equation in the absence of feedback
Full Text
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