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Direct measurement of general quantum states using weak measurement (1112.5471v1)

Published 22 Dec 2011 in quant-ph

Abstract: Recent work [J.S. Lundeen et al. Nature, 474, 188 (2011)] directly measured the wavefunction by weakly measuring a variable followed by a normal (i.e. strong') measurement of the complementary variable. We generalize this method to mixed states by considering the weak measurement of various products of these observables, thereby providing the density matrix an operational definition in terms of a procedure for its direct measurement. The method only requires measurements in two bases and can be performedin situ', determining the quantum state without destroying it.

Citations (229)

Summary

  • The paper introduces a weak measurement technique that directly captures the elements of the density matrix in mixed quantum states.
  • The method measures products of projectors from mutually unbiased bases to yield the complete Dirac distribution of quantum states.
  • These findings pave the way for non-invasive, in situ quantum state analysis with potential applications in quantum computing and chemical monitoring.

Direct Measurement of General Quantum States Using Weak Measurement

In this paper, the authors address a significant problem in quantum mechanics—the direct measurement of the quantum state. Traditional methods, such as Quantum State Tomography, require extensive data and complex reconstruction processes. This work extends previous findings on the direct measurement of the wavefunction to more general quantum states, i.e., mixed states, through weak measurement techniques.

Key Concepts and Methodology

The central focus of this paper is the weak measurement method, which was notably employed by Lundeen and colleagues for measuring the wavefunction directly. A weak measurement interacts minimally with the system, thereby preserving its state. The measurement is followed by a strong measurement of a complementary variable. This paper extends the method to describe mixed quantum states represented by the density operator ρ, which accounts for both classical randomness and quantum entanglement.

Two innovative approaches are proposed:

  1. Direct Measurement of Quantum States: The authors demonstrate that it is possible to directly measure the elements of the density matrix by utilizing weak measurements of various operators. Weak measurements of a product space formed by projectors on two mutually unbiased bases provide a direct view of the density operator elements, suggesting a new operational definition for measuring quantum states.
  2. Measurement of the Dirac Distribution: By weakly measuring the product of projectors from mutually unbiased bases, the Dirac distribution, an alternative representation of quantum states in a phase-space-like formulation, can be directly obtained. Notably, the Dirac distribution contains complete information about the density matrix, resonating with classical probability theories yet compatible with the quantum framework.

Results and Implications

The principal result is that general quantum states (mixed states) can be characterized by direct measurement methods without requiring state reconstruction. This is critical since it bypasses the need for complex procedures commonly associated with Quantum State Tomography. The authors speculate that these techniques could become foundational in scenarios where in situ measurements are crucial, such as real-time quantum computing or chemical reaction monitoring.

The operational definition provided for the density matrix through weak measurements holds theoretical and practical significance. It enables point-by-point local measurements with reduced disturbance to the quantum system compared to traditional methods, potentially allowing non-invasive examination of quantum processes.

Limitations and Future Directions

While the direct measurement method holds promise, its practical implementation requires careful consideration of factors such as signal-to-noise ratios and resolution compared to existing techniques like tomography. Moreover, the complexity involved in weakly measuring non-Hermitian operators suggests further exploration into measurement schemes and apparatus enhancements.

Looking ahead, extending these direct measurement methodologies to other quantum systems and high-dimensional spaces could provide new insights. Additionally, investigating error quantification in weak measurements could help bridge the gap between theory and implementation, enhancing the robustness and applicability of the approach in various scientific and technological domains.

In conclusion, this paper contributes substantially to the experimental and theoretical understanding of quantum state measurement, proposing novel methods based on weak measurement techniques. The potential applications of these findings are vast, with promising implications for quantum information science, quantum computing, and other areas involving complex quantum systems.

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