Determination of weak values of quantum operators using only strong measurements
arXiv:1804.11298 · doi:10.1103/PhysRevA.98.042112
Abstract
Weak values have been shown to be helpful especially when considering them as the outcomes of weak measurements. In this paper we show that in principle, the real and imaginary parts of the weak value of any operator may be elucidated from expectation values of suitably defined density, flux and hermitian commutator operators. Expectation values are the outcomes of strong (projective) measurements implying that weak values are general properties of operators in association with pre- and post-selection and they need not be preferentially associated with weak measurements. They should be considered as an important measurable property which provides added information as compared with the "standard" diagonal expectation value of an operator. As a first specific example we consider the determination of the real and imaginary parts of the weak value of the momentum operator employing projective time of flight experiments. Then the results are analyzed from the point of view of Bohmian mechanics. Finally we consider recent neutron interferometry experiments used to determine the weak values of the neutron spin.
Accepted version
References in corpus (37)
- Ultrasensitive Beam Deflection Measurement via Interferometric Weak Value Amplification
- Direct Measurement of the Quantum Wavefunction
- Colloquium: Understanding Quantum Weak Values: Basics and Applications
- Quantum weak values
- Nonperturbative theory of weak pre- and post-selected measurements
- Direct measurement of general quantum states using weak measurement
- Technical advantages for weak value amplification: When less is more
- Violation of the Leggett-Garg inequality with weak measurements of photons
- Direct observation of Hardy's paradox by joint weak measurement with an entangled photon pair
- Precision frequency measurements with interferometric weak values
- Grounding Bohmian Mechanics in Weak Values and Bayesianism
- Measurement of Time-of-Arrival in Quantum Mechanics
- Direct measurement of the density matrix of a quantum system
- The significance of the imaginary part of the weak value
- Weak Values are Interference Phenomena
- Improving the precision of weak measurements by postselection measurement
- Strong measurements give a better direct measurement of the quantum wave function
- Measuring measurement--disturbance relationships with weak values
- Measuring incompatible observables of a single photon
- Weak value controversy
- Broadening the scope of weak quantum measurements I: A single particle accurately measured yet left superposed
- Broadening the scope of weak quantum measurements II: Past and future measurement effects within a double Mach-Zehnder-interferometer setting
- Weak value beyond conditional expectation value of the pointer readings
- Experimental demonstration of direct path state characterization by strongly measuring weak values in a matter-wave interferometer
- Imaging a single atom in a time-of-flight experiment
- Toward a thermo-hydrodynamic like description of Schrodinger equation via the Madelung formulation and Fisher information
- Classical Field Approach to Quantum Weak Measurements
- Observing trajectories with weak measurements in quantum systems in the semiclassical regime
- Coupling-Deformed Pointer Observables and Weak Values
- What is a quantum-mechanical 'weak value' the value of?
- Reconstructing weak values without weak measurements
- Probing finite coarse-grained virtual Feynman histories with sequential weak values
- Weak values are quantum: you can bet on it
- What weak measurements and weak values really mean - Reply to Kastner
- Are the 'weak measurements' really measurements?
- Time averaging of weak values - consequences for time-energy and coordinate-momentum uncertainty
- Process Tomography for Systems in a Thermal State
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- Quantum circuits for measuring weak values, Kirkwood--Dirac quasiprobability distributions, and state spectra
- Properties and Applications of the Kirkwood-Dirac Distribution
- Operational interpretation and estimation of quantum trace-norm asymmetry based on weak value measurement and some bounds
- Realism and causality I: Pilot wave and retrocausal models as possible facilitators
- Quantum coherence as asymmetry from complex weak values
- Geometric phases and the Sagnac effect: Foundational aspects and sensing applications
- A framework for measuring weak values without weak interactions and its diagrammatic representation
- Contextuality, Coherences, and Quantum Cheshire Cats
- Operational formulation of weak values without probe systems
- General quantum correlation from nonreal values of Kirkwood-Dirac quasiprobability over orthonormal product bases
- Dimension-independent weak value estimation via controlled SWAP operations
- Dependence of measurement outcomes on the dynamics of quantum coherent interactions between the system and the meter
- Toward practical weak measurement wavefront sensing: spatial resolution and achromatism
- Uncertainty relations for time averaged weak values
- A relational time-symmetric framework for analyzing the quantum computational speedup
- Systematic errors in direct state measurements with quantum controlled measurements
- Separation of measurement uncertainty into quantum and classical parts based on Kirkwood-Dirac quasiprobability and generalized entropy
- Quantum entanglement as an extremal Kirkwood-Dirac nonreality
- Quantum causality relations and the emergence of reality from coherent superpositions
- Kinetic energy equipartition: a tool to characterize quantum thermalization
- The real and imaginary parts of a weak value appearing as back-actions via a post-selection
- Quantum speed limit for observables from quantum asymmetry
- Interplay between strong and weak measurement: Comparison of three experimental approaches to weak value estimation
- Time Derivatives of Weak Values
- Estimation of multivariate traces of states given partial classical information
- Physics and mathematical reality: comments on Aharonov et al, arXiv:1902.08798