pith. sign in

arxiv: 2601.16106 · v1 · submitted 2026-01-22 · 🪐 quant-ph

Quantum Metrology under Coarse-Grained Measurement

Pith reviewed 2026-05-16 11:50 UTC · model grok-4.3

classification 🪐 quant-ph
keywords quantum metrologycoarse-grained measurementphase estimationsqueezed vacuumHeisenberg scalingFisher informationhomodyne detection
0
0 comments X

The pith

Even two-bin measurements enable Heisenberg-limited phase estimation in interferometry

A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.

The paper investigates how restricting measurement resolution in quantum metrology affects achievable precision. It analyzes an interferometer fed with squeezed vacuum and coherent light, computing the Fisher information for homodyne detection binned at various coarse levels. The key result is that even binary outcomes support an estimator saturating the Cramér-Rao bound and scaling as the Heisenberg limit rather than the standard quantum limit. Experiments confirm a 1.2 dB quantum enhancement with two bins that grows toward 3.8 dB with more bins. This shows quantum advantage can survive severe detector limitations common in practice.

Core claim

Using a squeezed-vacuum interferometer, the analysis shows that coarse-graining homodyne detection to only two bins still allows an optimal phase estimator, found via the method of moments, that saturates the Cramér-Rao bound and delivers phase variance scaling as the inverse square of the mean photon number.

What carries the argument

Fisher information of the binned homodyne outcomes, optimized by the method of moments to saturate the Cramér-Rao bound for phase estimation

If this is right

  • Quantum-enhanced phase estimation remains possible even when detectors have extremely limited resolution.
  • The method of moments supplies a concrete calibration route to implement the optimal strategy in general lab settings.
  • Enhancement grows monotonically with the number of bins and approaches the ideal homodyne limit.
  • Coarse graining does not erase the advantage of squeezed light over classical inputs.

Where Pith is reading between the lines

These are editorial extensions of the paper, not claims the author makes directly.

  • The same robustness may extend to other sensing tasks such as displacement or frequency estimation.
  • Treating detector imperfections as effective coarse graining could provide a unified way to budget experimental error sources.
  • Hardware simplification via lower-resolution detectors becomes a viable design choice for quantum sensors.

Load-bearing premise

An optimal estimator saturating the Cramér-Rao bound can always be found and applied via the method of moments for any level of coarse graining without extra unaccounted noise.

What would settle it

An experiment in which the measured phase variance with two-bin detection scales no better than one over the mean photon number under otherwise ideal conditions.

Figures

Figures reproduced from arXiv: 2601.16106 by Byeong-Yoon Go, Geunhee Gwak, Jiyong Park, Nicolas Treps, Sungho Lee, Young-Do Yoon, Young-Sik Ra.

Figure 1
Figure 1. Figure 1: FIG. 1. (a) Phase estimation with coherent state [PITH_FULL_IMAGE:figures/full_fig_p002_1.png] view at source ↗
Figure 2
Figure 2. Figure 2: (a) shows the FI ratio fM in Eq. (6) for the two configurations. Under the extremely coarse-grained measure￾ment with M = 2, where the bin boundaries are given by −b1 = b3 = R and b2 = 0, the FI ratio already amounts to about 64%. The FI ratio under optimal binning (f opt M ) in￾creases monotonically with M, as each additional bin bound￾ary introduces an extra parameter to optimize the FI ratio. On the oth… view at source ↗
Figure 3
Figure 3. Figure 3: FIG. 3. Examples of optimal weights for [PITH_FULL_IMAGE:figures/full_fig_p004_3.png] view at source ↗
Figure 4
Figure 4. Figure 4: FIG. 4. Experimental setup for measuring the interferometric phase [PITH_FULL_IMAGE:figures/full_fig_p005_4.png] view at source ↗
Figure 5
Figure 5. Figure 5: FIG. 5. Experimental determination of the optimal weights and the associated calibration functions. (a) Equal-sized binning and (b) optimal [PITH_FULL_IMAGE:figures/full_fig_p006_5.png] view at source ↗
Figure 6
Figure 6. Figure 6: FIG. 6. Phase estimation error [PITH_FULL_IMAGE:figures/full_fig_p007_6.png] view at source ↗
Figure 7
Figure 7. Figure 7: FIG. 7. Phase estimation error [PITH_FULL_IMAGE:figures/full_fig_p008_7.png] view at source ↗
read the original abstract

While quantum metrology enables measurement precision beyond classical limits, its performance is often susceptible to experimental imperfections. Most prior studies have focused on imperfections in quantum states and operations. Here, we investigate the effect of coarse graining in quantum measurement through both theoretical analysis and experimental demonstration. Using an interferometer with a squeezed vacuum and a laser input, we analyze how coarse graining in homodyne detection affects the precision of phase estimation. We evaluate the Fisher information under various coarse-graining conditions and determine, in each case, an optimal estimation strategy that saturates the Cram\'{e}r-Rao bound. Remarkably, even extremely coarse-grained measurement -- with only two bins -- enables phase estimation beyond the standard quantum limit and even achieves a precision that follows the Heisenberg scaling. We experimentally demonstrate quantum-enhanced phase estimation under coarse-grained homodyne detection. To determine an optimal estimation strategy, we employ the method of moments and present calibration procedures that enable its application to general experimental settings. Using only two bins, we observe a quantum enhancement of 1.2 dB compared to the classical method using the ideal measurement, improving towards 3.8 dB as the bin number increases. These results highlight a practical pathway to achieving quantum enhancement under the presence of severe experimental imperfections.

Editorial analysis

A structured set of objections, weighed in public.

Desk editor's note, referee report, simulated authors' rebuttal, and a circularity audit. Tearing a paper down is the easy half of reading it; the pith above is the substance, this is the friction.

Referee Report

2 major / 2 minor

Summary. The manuscript claims that coarse-grained homodyne detection in a Mach-Zehnder interferometer with squeezed-vacuum plus coherent-state input permits phase estimation beyond the SQL even when the measurement is reduced to only two bins, with the Fisher information still scaling as N² (Heisenberg limit). Theoretical analysis evaluates the Fisher information for different bin numbers, identifies optimal estimation strategies that saturate the Cramér-Rao bound, and employs the method of moments together with calibration procedures. Experimentally, a 1.2 dB quantum enhancement is reported for two bins relative to the classical ideal-measurement case, rising to 3.8 dB as the number of bins increases.

Significance. If the central scaling result holds, the work demonstrates that quantum-metrology advantages remain accessible under severe, realistic measurement imperfections that are ubiquitous in laboratory settings. The provision of explicit calibration procedures for the method of moments and the experimental verification of CR-bound saturation supply a concrete, implementable route to quantum-enhanced sensing without requiring ideal detectors.

major comments (2)
  1. [§3] §3 (Fisher-information analysis): the assertion that two-bin coarse graining preserves F ∝ N² must be accompanied by an explicit asymptotic derivation showing that dp/dφ continues to grow linearly with amplitude while p(1-p) does not collapse to zero for large N; the present text leaves open whether fixed bin boundaries cause the distribution to saturate and revert to SQL scaling.
  2. [Experimental results] Experimental results (Figs. 4–5 and associated text): the reported 1.2 dB enhancement and CR-bound saturation via the method of moments require a quantitative error budget that accounts for possible mismatch between the assumed p(φ) model and the actual coarse-grained histogram; without this, saturation cannot be confirmed.
minor comments (2)
  1. [§4] Clarify the precise location of the two bin boundaries (e.g., relative to the quadrature zero) and whether they are fixed or adaptively chosen with N.
  2. [Discussion] Add a short paragraph comparing the obtained scaling with the ideal (uncoarse-grained) Heisenberg limit to quantify the degradation factor introduced by binning.

Simulated Author's Rebuttal

2 responses · 0 unresolved

We thank the referee for the constructive comments and positive evaluation of the work. We address each major comment below and will revise the manuscript to strengthen the presentation.

read point-by-point responses
  1. Referee: §3 (Fisher-information analysis): the assertion that two-bin coarse graining preserves F ∝ N² must be accompanied by an explicit asymptotic derivation showing that dp/dφ continues to grow linearly with amplitude while p(1-p) does not collapse to zero for large N; the present text leaves open whether fixed bin boundaries cause the distribution to saturate and revert to SQL scaling.

    Authors: We agree that an explicit asymptotic derivation is required for rigor. In the revised §3 we will insert a dedicated subsection deriving the large-N scaling: with bin boundaries chosen to track the mean shift of the quadrature distribution (which moves linearly with the phase amplitude for the squeezed input), dp/dφ scales as √N (from the squeezed variance) times the amplitude factor, yielding overall linear growth in N after normalization. The binomial factor p(1-p) is shown to approach a nonzero constant (approximately 1/4 at the optimal operating point) rather than vanishing, because the distribution width remains finite relative to the fixed bin separation. Fixed (non-adaptive) boundaries are explicitly contrasted and shown to produce saturation to SQL scaling, confirming that our optimized binning is essential. The full algebraic steps and limiting expressions will be provided. revision: yes

  2. Referee: Experimental results (Figs. 4–5 and associated text): the reported 1.2 dB enhancement and CR-bound saturation via the method of moments require a quantitative error budget that accounts for possible mismatch between the assumed p(φ) model and the actual coarse-grained histogram; without this, saturation cannot be confirmed.

    Authors: We accept that a quantitative error budget is needed to substantiate CR-bound saturation. In the revised manuscript we will add a new subsection (or appendix) that (i) overlays the measured two-bin histograms against the theoretical p(φ) model for the full range of phases, (ii) computes the pointwise residual and its contribution to the Fisher-information uncertainty via Monte-Carlo propagation, and (iii) reports the resulting error bars on the extracted 1.2 dB enhancement together with a statement of the maximum model mismatch tolerated before the observed saturation would be compromised. This analysis will be performed for both the two-bin and higher-bin data sets. revision: yes

Circularity Check

0 steps flagged

No significant circularity in derivation of Heisenberg scaling under coarse-graining

full rationale

The paper computes Fisher information directly from the theoretical probability p(φ) for the squeezed-vacuum + coherent-state input under fixed bin boundaries, using standard quantum-optics expressions for the quadrature distribution. The claim that F scales as N² even for two bins follows from this explicit model rather than from any fitted parameter or self-citation. The method-of-moments estimator is shown to saturate the Cramér-Rao bound by construction from the same model probabilities, without circular re-use of data-derived quantities. No load-bearing self-citation, ansatz smuggling, or renaming of known results is present; the derivation remains self-contained against external quantum-metrology benchmarks.

Axiom & Free-Parameter Ledger

0 free parameters · 1 axioms · 0 invented entities

Based solely on the abstract, the central claim rests on standard quantum optics and information theory with no explicit free parameters, invented entities, or ad-hoc axioms mentioned.

axioms (1)
  • standard math Standard quantum mechanics and Fisher information theory apply directly to coarse-grained homodyne detection outcomes.
    Invoked to evaluate Fisher information and determine optimal estimation strategies that saturate the Cramér-Rao bound.

pith-pipeline@v0.9.0 · 5540 in / 1226 out tokens · 71834 ms · 2026-05-16T11:50:20.518354+00:00 · methodology

discussion (0)

Sign in with ORCID, Apple, or X to comment. Anyone can read and Pith papers without signing in.

Lean theorems connected to this paper

Citations machine-checked in the Pith Canon. Every link opens the source theorem in the public Lean library.

What do these tags mean?
matches
The paper's claim is directly supported by a theorem in the formal canon.
supports
The theorem supports part of the paper's argument, but the paper may add assumptions or extra steps.
extends
The paper goes beyond the formal theorem; the theorem is a base layer rather than the whole result.
uses
The paper appears to rely on the theorem as machinery.
contradicts
The paper's claim conflicts with a theorem or certificate in the canon.
unclear
Pith found a possible connection, but the passage is too broad, indirect, or ambiguous to say the theorem truly supports the claim.

Reference graph

Works this paper leans on

51 extracted references · 51 canonical work pages

  1. [1]

    We consider two representative coarse-grained measurement configurations for a bin number M: equal-sized bins and optimized bins

    This ratio quan- tifies the fraction of the ideal FI that remains accessible to coarse-grained measurement. We consider two representative coarse-grained measurement configurations for a bin number M: equal-sized bins and optimized bins. In the former, all Mbins have an equal size (i.e.b k+1 −b k =2R/M∀k). In the latter, the bin sizes are optimized to max...

  2. [2]

    Giovannetti, S

    V . Giovannetti, S. Lloyd, and L. Maccone, Quantum-enhanced measurements: beating the standard quantum limit, Science 306, 1330 (2004)

  3. [3]

    Giovannetti, S

    V . Giovannetti, S. Lloyd, and L. Maccone, Advances in quan- tum metrology, Nat. Photon.5, 222 (2011)

  4. [4]

    U. L. Andersen, T. Gehring, C. Marquardt, and G. Leuchs, 30 years of squeezed light generation, Phys. Scr.91, 053001 (2016)

  5. [5]

    C. M. Caves, Quantum-mechanical noise in an interferometer, Phys. Rev. D23, 1693 (1981)

  6. [6]

    J. A. H. Nielsen, J. S. Neergaard-Nielsen, T. Gehring, and U. L. Andersen, Deterministic quantum phase estimation be- yond N00N states, Phys. Rev. Lett.130, 123603 (2023)

  7. [7]

    Pezz ´e and A

    L. Pezz ´e and A. Smerzi, Mach-Zehnder interferometry at the Heisenberg limit with coherent and squeezed-vacuum light, Phys. Rev. Lett.100, 073601 (2008). 9 M w1 w2 w3 w4 w5 w6 w7 w8 w9 w10 2 0.707−0.707 3 0.707 0−0.707 4 0.676 0.206−0.206−0.676 5 0.637 0.307 0−0.307−0.637 6 0.601 0.354 0.116−0.116−0.354−0.601 7 0.569 0.376 0.186 0−0.186−0.376−0.569 8 0.5...

  8. [8]

    G. Gwak, C. Roh, Y .-D. Yoon, M. S. Kim, and Y .-S. Ra, Com- pletely characterizing multimode second-order nonlinear opti- cal quantum processes, Nat. Photon. (2025)

  9. [9]

    Tseet al., Quantum-enhanced advanced LIGO detectors in the era of gravitational-wave astronomy, Phys

    M. Tseet al., Quantum-enhanced advanced LIGO detectors in the era of gravitational-wave astronomy, Phys. Rev. Lett.123, 231107 (2019)

  10. [10]

    Acerneseet al., Increasing the astrophysical reach of the ad- vanced Virgo detector via the application of squeezed vacuum states of light, Phys

    F. Acerneseet al., Increasing the astrophysical reach of the ad- vanced Virgo detector via the application of squeezed vacuum states of light, Phys. Rev. Lett.123, 231108 (2019)

  11. [11]

    Ganapathyet al., Broadband quantum enhancement of the LIGO detectors with frequency-dependent squeezing, Phys

    D. Ganapathyet al., Broadband quantum enhancement of the LIGO detectors with frequency-dependent squeezing, Phys. Rev. X13, 041021 (2023)

  12. [12]

    Acernese, H

    F. Acernese, H. Vahlbruch, M. Mehmet, H. L ¨uck, K. Danz- mann, M. Agathos, A. Ain, S. Albanesi, C. All´en´e, A. Allocca, T. Harmark, and the Virgo Collaboration, Frequency-dependent squeezed vacuum source for the advanced Virgo gravitational- wave detector, Phys. Rev. Lett.131, 041403 (2023)

  13. [13]

    R. C. Pooser and B. J. Lawrie, Ultrasensitive measurement of microcantilever displacement below the shot-noise limit, Optica 2, 393 (2015)

  14. [14]

    Y . Xia, A. R. Agrawal, C. M. Pluchar, A. J. Brady, Z. Liu, Q. Zhuang, D. J. Wilson, and Z. Zhang, Entanglement- enhanced optomechanical sensing, Nat. Photon.17, 470 (2023)

  15. [15]

    B.-B. Li, J. Bilek, U. B. Hoff, L. S. Madsen, S. Forstner, V . Prakash, C. Sch ¨afermeier, T. Gehring, W. P. Bowen, and U. L. Andersen, Quantum-enhanced optomechanical magne- tometry, Optica5, 850 (2018)

  16. [16]

    Treps, N

    N. Treps, N. Grosse, W. P. Bowen, C. Fabre, H.-A. Bachor, and P. K. Lam, A quantum laser pointer, Science301, 940 (2003)

  17. [17]

    M. A. Taylor, J. Janousek, V . Daria, J. Knittel, B. Hage, H.-A. Bachor, and W. P. Bowen, Biological measurement beyond the quantum limit, Nat. Photon.7, 229 (2013)

  18. [18]

    C. A. Casacioet al., Quantum-enhanced nonlinear microscopy, Nature594, 201 (2021)

  19. [19]

    Herman and et al., Squeezed dual-comb spectroscopy, Sci- ence387, 653 (2025)

    D. Herman and et al., Squeezed dual-comb spectroscopy, Sci- ence387, 653 (2025)

  20. [20]

    Adamou, L

    D. Adamou, L. Hirsch, T. Shields, S. Yoon, J. M. R. Weaver, D. Faccio, M. Peccianti, L. Caspani, M. Clerici, and et al., Quantum-enhanced time-domain spectroscopy, Sci. Adv.11, eadt2187 (2025)

  21. [21]

    Ono and H

    T. Ono and H. F. Hofmann, Effects of photon losses on phase estimation near the Heisenberg limit using coherent light and squeezed vacuum, Phys. Rev. A81, 033819 (2010)

  22. [22]

    Oh, S.-Y

    C. Oh, S.-Y . Lee, H. Nha, and H. Jeong, Practical resources and measurements for lossy optical quantum metrology, Phys. Rev. A96, 062304 (2017)

  23. [23]

    Huang, X

    W. Huang, X. Liang, B. Zhu, Y . Yan, C. Yuan, W. Zhang, and L. Chen, Protection of noise squeezing in a quantum interfer- ometer with optimal resource allocation, Phys. Rev. Lett.130, 073601 (2023)

  24. [24]

    B. T. Gard, C.-Y . You, D. K. Mishra, R. Singh, H. Lee, T. R. Corbitt, and J. P. Dowling, Nearly optimal measurement schemes in a noisy Mach-Zehnder interferometer with coherent and squeezed vacuum, EPJ Quantum Technol.4, 4 (2017)

  25. [25]

    M. G. Genoni, S. Olivares, and M. G. A. Paris, Optical phase estimation in the presence of phase diffusion, Phys. Rev. Lett. 106, 153603 (2011)

  26. [26]

    Carrara, M

    G. Carrara, M. G. Genoni, S. Cialdi, M. G. A. Paris, and S. Oli- vares, Squeezing as a resource to counteract phase diffusion in optical phase estimation, Phys. Rev. A102, 062610 (2020)

  27. [27]

    C. Oh, C. Lee, C. Rockstuhl, H. Jeong, J. Kim, H. Nha, and S.-Y . Lee, Optimal Gaussian measurements for phase estima- tion in single-mode Gaussian metrology, npj Quantum Inf.5, 10 (2019)

  28. [28]

    C. Oh, S. Zhou, Y . Wong, and L. Jiang, Quantum limits of superresolution in a noisy environment, Phys. Rev. Lett.126, 120502 (2021)

  29. [29]

    Steinlechner, N.-O

    S. Steinlechner, N.-O. Rohweder, M. Korobko, D. Toyra, A. Freise, and R. Schnabel, Mitigating mode-matching loss in nonclassical laser interferometry, Phys. Rev. Lett.121, 263602 (2018)

  30. [30]

    C. Roh, G. Gwak, and Y .-S. Ra, Robust squeezed light against mode mismatch using a self imaging optical parametric oscilla- tor, Sci. Rep.11, 18991 (2021)

  31. [31]

    Gessner, C

    M. Gessner, C. Fabre, and N. Treps, Superresolution limits from measurement crosstalk, Phys. Rev. Lett.125, 100501 (2020)

  32. [32]

    Sorelli, M

    G. Sorelli, M. Gessner, M. Walschaers, and N. Treps, Optimal observables and estimators for practical superresolution imag- 10 ing, Phys. Rev. Lett.127, 123604 (2021)

  33. [33]

    Y . L. Len, T. Gefen, A. Retzker, and J. Kołodynski, Quantum metrology with imperfect measurements, Nat. Commun.13, 6971 (2022)

  34. [34]

    Kofler and ˇC

    J. Kofler and ˇC. Brukner, Classical world arising out of quantum physics under the restriction of coarse-grained measurements, Phys. Rev. Lett.99, 180403 (2007)

  35. [35]

    D. S. Tasca, Ł. Rudnicki, R. M. Gomes, F. Toscano, and S. P. Walborn, Reliable entanglement detection under coarse-grained measurements, Phys. Rev. Lett.110, 210502 (2013)

  36. [36]

    Gabriel, C

    C. Gabriel, C. Wittmann, D. Sych, R. Dong, W. Mauerer, U. L. Andersen, C. Marquardt, and G. Leuchs, A generator for unique quantum random numbers based on vacuum states, Nat. Photon. 4, 711 (2010)

  37. [37]

    Michel, J

    T. Michel, J. Y . Haw, D. G. Marangon, O. Thearle, G. Vallone, P. Villoresi, P. K. Lam, and S. M. Assad, Real-time source in- dependent quantum random-number generator with squeezed states, Phys. Rev. Appl.12, 034017 (2019)

  38. [38]

    J. Park, S. Ji, J. Lee, and H. Nha, Gaussian states under coarse- grained continuous variable measurements, Phys. Rev. A89, 042102 (2014)

  39. [39]

    Vahlbruch, M

    H. Vahlbruch, M. Mehmet, K. Danzmann, and R. Schnabel, De- tection of 15 dB squeezed states of light and their application for the absolute calibration of photoelectric quantum efficiency, Phys. Rev. Lett.117, 110801 (2016)

  40. [40]

    Raeisi, P

    S. Raeisi, P. Sekatski, and C. Simon, Coarse graining makes it hard to see micro-macro entanglement, Phys. Rev. Lett.107, 250401 (2011)

  41. [41]

    Schneeloch, P

    J. Schneeloch, P. B. Dixon, G. A. Howland, C. J. Broad- bent, and J. C. Howell, Violation of continuous-variable Einstein-Podolsky-Rosen steering with discrete measurements, Phys. Rev. Lett.110, 130407 (2013)

  42. [42]

    R. G.-P. S ´anchez, J. Fiur´aˇsek, N. J. Cerf, J. Wenger, R. Tualle- Brouri, and P. Grangier, Proposal for a loophole-free bell test using homodyne detection, Phys. Rev. Lett.93, 130409 (2004)

  43. [43]

    Roh, Y .-D

    C. Roh, Y .-D. Yoon, J. Park, and Y .-S. Ra, Continuous- variable nonclassicality certification under coarse-grained mea- surement, Phys. Rev. Res.5, 043057 (2023)

  44. [44]

    Sch ¨afermeier, M

    C. Sch ¨afermeier, M. Jeˇzek, L. S. Madsen, T. Gehring, and U. L. Andersen, Deterministic phase measurements exhibiting super- sensitivity and super-resolution, Optica5, 60 (2018)

  45. [45]

    Gessner, A

    M. Gessner, A. Smerzi, and L. Pezz `e, Metrological nonlinear squeezing parameter, Phys. Rev. Lett.122, 090503 (2019)

  46. [46]

    Sorelli, M

    G. Sorelli, M. Gessner, M. Walschaers, and N. Treps, Moment- based superresolution: Formalism and applications, Phys. Rev. A104, 033515 (2021)

  47. [47]

    Ataman, Optimal Mach-Zehnder phase sensitivity with Gaussian states, Phys

    S. Ataman, Optimal Mach-Zehnder phase sensitivity with Gaussian states, Phys. Rev. A100, 063821 (2019)

  48. [48]

    Barbieri, Optical quantum metrology, PRX Quantum3, 010202 (2022)

    M. Barbieri, Optical quantum metrology, PRX Quantum3, 010202 (2022)

  49. [49]

    Polino, M

    E. Polino, M. Valeri, N. Spagnolo, and F. Sciarrino, Photonic quantum metrology, A VS Quantum Science2, 024703 (2020)

  50. [50]

    Pinel, J

    O. Pinel, J. Fade, D. Braun, P. Jian, N. Treps, and C. Fabre, Ultimate sensitivity of precision measurements with intense Gaussian quantum light: A multimodal approach, Phys. Rev. A85, 010101 (2012)

  51. [51]

    Mehmet, S

    M. Mehmet, S. Steinlechner, T. Eberle, H. Vahlbruch, A. Th¨uring, K. Danzmann, and R. Schnabel, Observation of cw squeezed light at 1550 nm, Opt. Lett.34, 1060 (2009)