It appears you don't have support to open PDFs in this web browser. To view this file, Open with your PDF reader
Abstract
The Kirkwood-Dirac quasiprobability distribution, intimately connected with the quantum correlation function of two observables measured at distinct times, is becoming increasingly relevant for fundamental physics and quantum technologies. This quasiprobability distribution can take non-positive values, and its experimental reconstruction becomes challenging when expectation values of incompatible observables are involved. Here, we use an interferometric scheme aided by an auxiliary system to reconstruct the Kirkwood-Dirac quasiprobability distribution. We experimentally demonstrate this scheme in an electron-nuclear spin system associated with a nitrogen-vacancy center in diamond. By measuring the characteristic function, we reconstruct the quasiprobability distribution of work and analyze the behavior of its first and second moments. Our results clarify the physical meaning of the work quasiprobability distribution in the context of quantum thermodynamics. Finally, we study the uncertainty of measuring the Hamiltonian of the system at two times, via the Robertson-Schrödinger uncertainty relation, for different initial states.
You have requested "on-the-fly" machine translation of selected content from our databases. This functionality is provided solely for your convenience and is in no way intended to replace human translation. Show full disclaimer
Neither ProQuest nor its licensors make any representations or warranties with respect to the translations. The translations are automatically generated "AS IS" and "AS AVAILABLE" and are not retained in our systems. PROQUEST AND ITS LICENSORS SPECIFICALLY DISCLAIM ANY AND ALL EXPRESS OR IMPLIED WARRANTIES, INCLUDING WITHOUT LIMITATION, ANY WARRANTIES FOR AVAILABILITY, ACCURACY, TIMELINESS, COMPLETENESS, NON-INFRINGMENT, MERCHANTABILITY OR FITNESS FOR A PARTICULAR PURPOSE. Your use of the translations is subject to all use restrictions contained in your Electronic Products License Agreement and by using the translation functionality you agree to forgo any and all claims against ProQuest or its licensors for your use of the translation functionality and any output derived there from. Hide full disclaimer
Details




1 Massachusetts Institute of Technology, Research Laboratory of Electronics, Cambridge, USA (GRID:grid.116068.8) (ISNI:0000 0001 2341 2786)
2 Massachusetts Institute of Technology, Research Laboratory of Electronics, Cambridge, USA (GRID:grid.116068.8) (ISNI:0000 0001 2341 2786); Massachusetts Institute of Technology, Department of Nuclear Science and Engineering, Cambridge, USA (GRID:grid.116068.8) (ISNI:0000 0001 2341 2786)
3 German Aerospace Center (DLR), Institute of Quantum Technologies, Ulm, Germany (GRID:grid.7551.6) (ISNI:0000 0000 8983 7915)
4 Bar-Ilan University, Department of Chemistry, Institute of Nanotechnology and Advanced Materials and the Center for Quantum Entanglement Science and Technology, Ramat-Gan, Israel (GRID:grid.22098.31) (ISNI:0000 0004 1937 0503)
5 Istituto Nazionale di Ottica del Consiglio Nazionale delle Ricerche (CNR-INO), Sesto Fiorentino, Italy (GRID:grid.425378.f) (ISNI:0000 0001 2097 1574); Università di Firenze, European Laboratory for Non-linear Spectroscopy (LENS), Sesto Fiorentino, Italy (GRID:grid.425378.f) (ISNI:0000 0000 9458 0261)
6 Università di Firenze, European Laboratory for Non-linear Spectroscopy (LENS), Sesto Fiorentino, Italy (GRID:grid.425378.f) (ISNI:0000 0000 9458 0261); Istituto Nazionale di Ottica del Consiglio Nazionale delle Ricerche (CNR-INO), Firenze, Italy (GRID:grid.425378.f) (ISNI:0000 0001 2097 1574); SISSA, Trieste, Italy (GRID:grid.5970.b) (ISNI:0000 0004 1762 9868)