4.6 Article

Asymptotic role of entanglement in quantum metrology

期刊

PHYSICAL REVIEW A
卷 94, 期 1, 页码 -

出版社

AMER PHYSICAL SOC
DOI: 10.1103/PhysRevA.94.012339

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资金

  1. ERC AdG OSYRIS
  2. ERC CoG QITBOX
  3. Axa Chair in Quantum Information Science
  4. John Templeton Foundation
  5. EU IP SIQS
  6. EU STREP QUIC
  7. EU EQuaM
  8. Spanish Ministry National Plan FOQUS [FIS2013-46768]
  9. Spanish Ministry National Plan MINECO [SEV-2015-0522]
  10. Fundacio Privada Cellex
  11. Generalitat de Catalunya [SGR 874, SGR 875]
  12. Foundation for Polish Science (START scholarship)
  13. Alexander von Humboldt Foundation
  14. European Union's Horizon research and innovation programme under the Marie Sklodowska-Curie Q-METAPP Grant [655161, 705109]
  15. European Union's Horizon research and innovation programme under the Marie Sklodowska-Curie N-MuQuaS Grant [655161, 705109]
  16. ICREA Funding Source: Custom
  17. Marie Curie Actions (MSCA) [655161, 705109] Funding Source: Marie Curie Actions (MSCA)

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Quantum systems allow one to sense physical parameters beyond the reach of classical statistics-with resolutions greater than 1/N, where N is the number of constituent particles independently probing a parameter. In the canonical phase-sensing scenario the Heisenberg limit 1/N-2 may be reached, which requires, as we show, both the relative size of the largest entangled block and the geometric measure of entanglement to be nonvanishing as N -> infinity. Yet, we also demonstrate that in the asymptotic N limit any precision scaling arbitrarily close to the Heisenberg limit (1/N2-epsilon with any epsilon > 0) may be attained, even though the system gradually becomes noisier and separable, so that both the above entanglement quantifiers asymptotically vanish. Ourwork shows that sufficiently large quantum systems achieve nearly optimal resolutions despite their relative amount of entanglement being arbitrarily small. In deriving our results, we establish the continuity relation of the quantum Fisher information evaluated for a phaselike parameter, which lets us link it directly to the geometry of quantum states, and hence naturally to the geometric measure of entanglement.

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