An Electronic Quantum Eraser

TL;DR

This paper reports the first implementation of a quantum eraser in an electronic system using entangled Mach-Zehnder interferometers, demonstrating control over which-path information and interference visibility through measurement basis adjustments.

Contribution

It introduces a novel electronic quantum eraser setup with entangled MZIs, enabling continuous control of which-path information and interference via measurement basis and post-selection.

Findings

Controlled the visibility of Aharonov-Bohm oscillations by adjusting measurement basis.

Achieved a smooth transition between which-path information preservation and erasure.

Demonstrated the feasibility of quantum eraser experiments in electronic systems.

Abstract

Complementarity, the incomplete nature of a quantum measurement - a core concept in quantum mechanics - stems from the choice of the measurement apparatus. The notion of complementarity is closely related to Heisenberg's uncertainty principle, but the exact relation between the two remains a source of debate. For example, knowledge of a particle's position in a double slit interference experiment will quench its wave-like nature and, vice versa, observing the wave property via interference implies lack of knowledge of the particle's path. A canonical system for exploring complementarity is the quantum eraser (QE), predominantly studied thus far in photonic systems. A QE is an interference experiment consisting of two stages. First, one of the interfering paths is coupled to a 'which path' (WP) detector - demonstrating loss of interference due to acquisition of WP information. Second, the WP information is being 'erased' by projecting the detector's wavefunction on a particular basis; this renders the WP information inaccessible, thus allowing reconstruction of the interference pattern. In this work, we present a first implementation of a QE in an electronic system. Our system consists of two identical electronic Mach-Zehnder interferometers (MZIs) entangled via Coulomb interactions. Such novel setup has already attracted a considerable theoretical attention. With one MZI serving as a path detector and the other as the system interferometer, the visibility of the Aharonov-Bohm oscillation in the System can be controlled by the Detector. We demonstrate how a continuous change of the measurement basis, followed by post selection (via cross correlation of current fluctuations), allows a smooth transition between keeping and erasing the WP information.