Fisher information and multiparticle entanglement
Open accessAbstract
The Fisher information $F$ gives a limit to the ultimate precision achievable in a phase estimation protocol. It has been shown recently that the Fisher information for a linear two-mode interferometer cannot exceed the number of particles if the input state is separable. As a direct consequence, with such input states the shot-noise limit is the ultimate limit of precision. In this work, we go a step further by deducing bounds on $F$ for several multiparticle entanglement classes. These bounds imply that genuine multiparticle entanglement is needed for reaching the highest sensitivities in quantum interferometry. We further compute similar bounds on the average Fisher information $\overline{F}$ for collective spin operators, where the average is performed over all possible spin directions. We show that these criteria detect different sets of states and illustrate their strengths by considering several examples, also using experimental data. In particular, the criterion based on $\overline{F}$ is able to detect certain bound entangled states.
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The bound could be valid for non-Markovian dynamics as long as they admit a representation in terms of a CP map.
“As a result, the bound could be valid for non Markovian dynamics as long as they admit a representation in terms of a CP map [38].”
From Quantum Speed Limits in Open System Dynamics (2013) · cites this paper as [38]
The QFI connects to other aspects of quantum physics, such as quantum phase transition and entanglement witness.
“Apart from quantum metrology, the QFI also connects to other aspects of quantum physics, such as quantum phase transition [18][19][20] and entanglement witness [21,22].”
From Quantum Fisher information matrix and multiparameter estimation (2020) · cites this paper as [21]
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“The rotation scenario serves also as a powerful entanglement detector [23,24] that can detect a vanishing fraction of entanglement [25] or even bound entanglement [26] with scaling close to the Heisenberg limit.”
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Evaluating Convex Roof Entanglement Measures
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Quantum-enhanced multiparameter estimation in multiarm interferometers
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“The right-hand side inequality in Eqs (4) and (5) is saturated if and only if the FIM is diagonal.”
BackgroundBridging entanglement dynamics and chaos in semiclassical systems
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Random Bosonic States for Robust Quantum Metrology
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“Quantum-enhanced parameter sensitivity can only be observed with systems exhibiting interparticle entanglement [19]; thus, such enhanced sensitivity can be used to detect multipartite entanglement [20–23] and lower bound the number of particles being entangled [24,25].”
BackgroundMetrological Nonlinear Squeezing Parameter
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“[75] In fact a sharper bound for N-qubit states with up to k entangled qubits [74] is given as ξ−2 opt[ρ̂, Ĥ, Ĥ] ≤ sk2 + r2 where s = bN/kc and r = N − sk.”
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Entanglement between Identical Particles Is a Useful and Consistent Resource
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“Then, for any particle-separable state, we have F (ρ, n · S) ≤ 1 [52, 53].”
BackgroundKind of entanglement that speeds up quantum evolution
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Witnessing entanglement in quantum magnets using neutron scattering
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InfluentialGraph States as a Resource for Quantum Metrology
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Family of Bell-like Inequalities as Device-Independent Witnesses for Entanglement Depth
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Origin of the slow growth of entanglement entropy in long-range interacting spin systems
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Metrological Detection of Multipartite Entanglement from Young Diagrams
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“In this context, metrological entanglement criteria are powerful tools that establish a quantitative link between the number of detected entangled parties and the quantum gain in interferometric measurements [8–12].”
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Experimental Comparison of Efficient Tomography Schemes for a Six-Qubit State
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Self-citationQuantifying and Controlling Entanglement in the Quantum Magnet Cs2CoCl4
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Enhancement of parameter-estimation precision in noisy systems by dynamical decoupling pulses
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Critical behavior of dissipative two-dimensional spin lattices
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Witnessing entanglement without entanglement witness operators
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“In this case, the above method can be extended as a witness of multiparticle entanglement (22, 23): The inequality”
MethodSelf-citationEfficient entanglement criteria for discrete, continuous, and hybrid variables
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“[48] to the case of unequal, arbitrary subsystems.”
BackgroundSelf-citationQuantum States with a Positive Partial Transpose are Useful for Metrology
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“There have been results concerning entanglement criteria with several quantum Fisher information terms detecting PPT entangled states as well as concerning the metrological usefulness of multipartite states that are not PPT with respect to all bipartions [6,13,14].”
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Self-citationCharacterization of Topological States via Dual Multipartite Entanglement
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Phase damping destroys quantum Fisher information of W states
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Frequentist and Bayesian Quantum Phase Estimation
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Self-citationImproving cold-atom sensors with quantum entanglement: Prospects and challenges
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Multipartite Entanglement at Finite Temperature
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Geometric perspective on quantum parameter estimation
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Quantum dynamics of disordered spin chains with power-law interactions
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Many-Body Nonlocality as a Resource for Quantum-Enhanced Metrology
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Phase-sensitivity bounds for two-mode interferometers
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Self-citationEfficiently solving the dynamics of many-body localized systems at strong disorder
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Experimental estimation of the quantum Fisher information from randomized measurements
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“[18] Philipp Hyllus, Wiesław Laskowski, Roland Krischek, Christian Schwemmer, Witlef Wieczorek, Harald Weinfurter, Luca Pezzé, and Augusto Smerzi, “Fisher information and multiparticle entanglement,” Phys.”
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Genuine multipartite entanglement of quantum states in the multiple-copy scenario
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Extensive Multipartite Entanglement from su(2) Quantum Many-Body Scars
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Multipartite entanglement in the measurement-induced phase transition of the quantum Ising chain
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“[45] and [46], this quantity can be used to witness multipartite entanglement when Ô = Ô[{nj}] = 12 ∑ j nj · σ̂j , where nj are unit vectors.”
BackgroundEntanglement and extreme spin squeezing for a fluctuating number of indistinguishable particles
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“Assuming an initial state with no interparticle entanglement (ie, a coherent spin state (CSS) [28]), the maximum possible value is f0 = N , or FQ = NT 2 [17, 18], which we define as the shot-noise limit.”
BackgroundDetection of genuine tripartite entanglement by multiple sequential observers
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“[4] P.”
Background
- Authors
- Hyllus, P., Laskowski, W., Krischek, R., Schwemmer, C., Wieczorek, W., Weinfurter, H., Pezzé, L., & Smerzi, A.
- Affiliations
- University of the Basque Country (ES)
- University of Gdańsk (PL)
- Max Planck Institute of Quantum Optics (DE)
- University of Trento (IT)
- Venue
- Physical Review A
- Publisher
- American Physical Society (APS)
- Published
- 2012-02-16
- Volume
- 85
- Issue
- 2
- ISSN
- 0556-2791 (ISSN-L)
- 1050-2947
- 1094-1622
- OpenAlex
- W2041209858
- Cited by
- 593
- References
- 80
- Citations by year
- 2026: 44 · 2025: 80 · 2024: 74 · 2023: 52 · 2022: 38 · 2021: 57 · 2020: 43 · 2019: 46 · 2018: 32 · 2017: 33 · 2016: 32 · 2015: 31 · 2014: 16 · 2013: 9 · 2012: 6
- FWCI
- 19.48
- Type
- journal article
- Language
- en
- Open access
- green
- arxiv.org
- Locations
- Physical Review A (publishedVersion)
- arXiv (Cornell University) (publishedVersion)
- INO Open Portal (submittedVersion)
- MPG.PuRe (Max Planck Society) (submittedVersion)
- arXiv (Cornell University)
- Topics
- Physical Sciences › Computer Science › Artificial Intelligence › Quantum Information and Cryptography
- Physical Sciences › Physics and Astronomy › Atomic and Molecular Physics, and Optics › Quantum Mechanics and Applications
- Physical Sciences › Computer Science › Artificial Intelligence › Quantum Computing Algorithms and Architecture
- Keywords
- Fisher information, multipartite entanglement, quantum phase estimation, quantum interferometry, shot-noise limit, entanglement detection, bound entangled states, quantum metrology
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