Recognition: no theorem link
Parameter Estimation from Amplitude Collapse in Correlated Matter-Wave Interference
Pith reviewed 2026-05-16 02:16 UTC · model grok-4.3
The pith
Statistical inference on amplitude collapse in atom interferometers yields estimates with substantially reduced bias for correlated signals.
A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.
Core claim
The paper claims that applying statistical inference to the amplitude-collapse statistics of magnetically sensitive substates in an atom interferometer produces parameter estimates with higher trueness and substantially reduced bias compared with standard methods, provided the signals remain perfectly correlated, while maintaining competitive precision near vanishing amplitudes; this shows that zero-amplitude operation is not optimal for accuracy and supplies a general evaluation route for phase-unstable correlated interferometers.
What carries the argument
PEAC (Parameter Estimation from Amplitude Collapse), the statistical inference procedure that extracts parameters from the observed distribution of amplitude collapses across magnetically sensitive substates.
If this is right
- For perfectly correlated signals, PEAC delivers higher trueness and substantially lower bias than standard estimation methods.
- Precision stays competitive near vanishing amplitudes, showing that zero-signal points are not optimal for accuracy.
- The approach works for any correlated interferometer lacking phase stability and raises overall accuracy.
- Applications extend beyond atom-based interferometry to other correlated quantum sensors.
Where Pith is reading between the lines
- Choosing working points away from vanishing amplitude could improve sensitivity in quantum clock interferometry without sacrificing trueness.
- The method could be adapted to partially correlated signals by adding explicit noise terms to the inference model.
- Similar amplitude-collapse statistics might appear in other multi-state quantum systems, allowing the same inference technique in non-atomic platforms.
Load-bearing premise
The signals from the different magnetically sensitive substates remain perfectly correlated, with no residual differential noise or state-preparation errors that would change the amplitude-collapse statistics.
What would settle it
An experiment that measures significant residual differential noise between substates and finds that the amplitude statistics deviate from the predicted collapse behavior, eliminating the reported bias reduction, would falsify the central performance claim.
read the original abstract
Operating matter-wave interferometers as quantum detectors for fundamental physics or inertial sensors with unprecedented accuracies relies on noise rejection, often implemented by correlating multiple sensors. They can be spatially separated (gradiometry or gravitational-wave detection) or consist of different internal states (magnetometry or quantum clock interferometry), with a signal-amplitude modulation serving as a signature of a differential phase. In this work, we introduce Parameter Estimation from Amplitude Collapse (PEAC) by applying statistical inference techniques for different magnetically sensitive substates of an atom interferometer. We demonstrate that PEAC provides higher trueness, resulting in a substantially reduced bias compared to standard methods for perfectly correlated signals, while achieving competitive precision near, but not at, vanishing amplitudes. This indicates that vanishing signals do not constitute the most favourable working point for high-accuracy sensing, relevant to quantum clock interferometry. PEAC presents a generally applicable complementary evaluation method for correlated interferometers without phase stability, increasing the overall accuracy and enabling applications beyond atom-based interferometry.
Editorial analysis
A structured set of objections, weighed in public.
Referee Report
Summary. The paper introduces Parameter Estimation from Amplitude Collapse (PEAC), a statistical inference technique applied to amplitude-modulated signals from different magnetically sensitive substates in matter-wave interferometers. For signals that are perfectly correlated across substates, PEAC is claimed to deliver higher trueness with substantially reduced bias relative to standard methods while maintaining competitive precision near (but not at) vanishing amplitudes; this is positioned as a complementary evaluation approach for correlated interferometers lacking phase stability, with relevance to quantum clock interferometry.
Significance. If the bias-reduction result holds under the perfect-correlation regime, PEAC would offer a practical route to improved accuracy in atom-interferometric sensors and fundamental-physics measurements where differential-phase signatures are extracted from amplitude collapse. The method could be especially useful in setups with multiple internal states or spatially separated sensors, complementing existing correlation techniques without requiring phase stability.
major comments (2)
- [Methods / statistical model for amplitude collapse] The central claim of substantially reduced bias rests on the assumption of perfect inter-substate correlation (zero differential variance). The statistical model for amplitude collapse implicitly treats the joint distribution as having no residual uncorrelated component; once small differential noise from imperfect state preparation, magnetic gradients, or detection is present, the collapse statistics shift and the bias-reduction advantage is no longer guaranteed by the same derivation. No quantitative robustness analysis against such perturbations is reported.
- [Abstract and Results] Abstract and results: the claims of higher trueness and competitive precision are stated without accompanying derivation details, explicit error propagation, or tabulated bias/precision values for the PEAC estimator versus standard methods. This makes it impossible to verify the magnitude of the reported improvement or to assess whether the advantage persists away from the ideal correlation limit.
minor comments (1)
- [Notation] Notation for the substate amplitudes and the collapse parameter should be defined explicitly at first use, with a clear distinction between the observed fringe amplitude and the inferred differential phase.
Simulated Author's Rebuttal
We thank the referee for the careful reading and constructive feedback. We address the two major comments point by point below. The manuscript focuses on the ideal perfect-correlation regime, but we agree that additional clarity and discussion are warranted.
read point-by-point responses
-
Referee: The central claim of substantially reduced bias rests on the assumption of perfect inter-substate correlation (zero differential variance). The statistical model for amplitude collapse implicitly treats the joint distribution as having no residual uncorrelated component; once small differential noise from imperfect state preparation, magnetic gradients, or detection is present, the collapse statistics shift and the bias-reduction advantage is no longer guaranteed by the same derivation. No quantitative robustness analysis against such perturbations is reported.
Authors: We agree that the derivation of PEAC assumes perfect inter-substate correlation, as stated throughout the manuscript (e.g., in the abstract and Methods). The joint distribution is modeled without residual uncorrelated variance precisely because the paper targets this ideal regime for correlated matter-wave interferometers. We will add a new paragraph in the Discussion section providing an analytical approximation for how small differential noise perturbs the amplitude-collapse statistics and reduces the bias advantage. A full quantitative Monte-Carlo robustness study across multiple noise amplitudes is beyond the present scope and will be noted as future work. revision: partial
-
Referee: Abstract and results: the claims of higher trueness and competitive precision are stated without accompanying derivation details, explicit error propagation, or tabulated bias/precision values for the PEAC estimator versus standard methods. This makes it impossible to verify the magnitude of the reported improvement or to assess whether the advantage persists away from the ideal correlation limit.
Authors: The full derivations appear in the Methods and supplementary material, but we accept that the main text would benefit from greater transparency. In the revised version we will insert a compact table in the Results section listing bias and precision (standard deviation) for both PEAC and the conventional estimator at several representative amplitudes, together with a short inline derivation of the leading-order bias terms and the explicit error-propagation expressions used. These additions will allow direct verification of the reported improvement within the perfect-correlation limit. revision: yes
Circularity Check
No significant circularity in derivation chain
full rationale
The abstract introduces PEAC as a statistical inference method applied to amplitude collapse in perfectly correlated signals from magnetically sensitive substates. No equations, fitting procedures, or self-citations are shown that would reduce the claimed bias reduction or trueness improvement to a fitted parameter or input by construction. The central demonstration is conditioned on the explicit assumption of perfect inter-substate correlation, which is stated as a premise rather than derived from the method itself. The derivation chain remains self-contained against external benchmarks, with no load-bearing self-citation chains, ansatz smuggling, or renaming of known results visible. This matches the default expectation for non-circular papers.
Axiom & Free-Parameter Ledger
axioms (1)
- domain assumption Signals from different magnetically sensitive substates are perfectly correlated
Reference graph
Works this paper leans on
-
[1]
in one dimension, a benchmark application well-suited to typical vibration-prone environments and compact devices, even when state-selective interferometry is unavailable. Ultracold87Rb atoms from a Bose–Einstein condensate (BEC) provide a suitable point source (32) with sub-recoil momentum width, coherence, and access to efficient Bragg diffraction (56)....
-
[2]
L. Morel, Z. Yao, P. Clad ´e, S. Guellati-Kh ´elifa, Determination of the fine-structure constant with an accuracy of 81 parts per trillion.Nature588(7836), 61–65 (2020), doi:10.1038/ s41586-020-2964-7, https://doi.org/10.1038/s41586-020-2964-7
-
[4]
A. Arvanitaki, P. W. Graham, J. M. Hogan, S. Rajendran, K. Van Tilburg, Search for light scalar dark matter with atomic gravitational wave detectors.Phys. Rev. D97, 075020 (2018), doi:10.1103/PhysRevD.97.075020, https://link.aps.org/doi/10.1103/PhysRevD.97.075020
-
[5]
D. Derr, E. Giese, Clock transitions versus Bragg diffraction in atom-interferometric dark- matter detection.AVS Quantum Sci.5(4), 044404 (2023), doi:10.1116/5.0176666, https: //doi.org/10.1116/5.0176666
-
[6]
Abend,et al., Terrestrial very-long-baseline atom interferometry: Workshop summary
S. Abend,et al., Terrestrial very-long-baseline atom interferometry: Workshop summary. AVS Quantum Sci.6(2), 024701 (2024), doi:10.1116/5.0185291, https://doi.org/10.1116/5. 0185291
-
[7]
A. Abdalla,et al., Terrestrial Very-Long-Baseline Atom Interferometry: summary of the second workshop.EPJ Quantum Technol.12(1), 42 (2025), doi:10.1140/epjqt/s40507-025-00344-3, https://doi.org/10.1140/epjqt/s40507-025-00344-3
-
[8]
G. Rosi, F. Sorrentino, L. Cacciapuoti, M. Prevedelli, G. M. Tino, Precision measurement of the Newtonian gravitational constant using cold atoms.Nature510(7506), 518–521 (2014), doi:10.1038/nature13433, https://doi.org/10.1038/nature13433
-
[9]
G. Lamporesi, A. Bertoldi, L. Cacciapuoti, M. Prevedelli, G. M. Tino, Determination of the Newtonian Gravitational Constant Using Atom Interferometry.Phys. Rev. Lett.100, 050801 (2008), doi:10.1103/PhysRevLett.100.050801, https://link.aps.org/doi/10.1103/PhysRevLett. 100.050801. 29
-
[10]
J. B. Fixler, G. T. Foster, J. M. McGuirk, M. A. Kasevich, Atom Interferometer Measurement of the Newtonian Constant of Gravity.Science315(5808), 74–77 (2007), doi:10.1126/science. 1135459, https://www.science.org/doi/abs/10.1126/science.1135459
-
[11]
I. Pikovski, M. Zych, F. Costa, ˇC. Brukner, Universal decoherence due to gravitational time dilation.Nature Phys.11(8), 668–672 (2015), doi:10.1038/nphys3366, https://doi.org/10.1038/ nphys3366
-
[12]
Schlippert,et al., Quantum Test of the Universality of Free Fall.Phys
D. Schlippert,et al., Quantum Test of the Universality of Free Fall.Phys. Rev. Lett.112, 203002 (2014), doi:10.1103/PhysRevLett.112.203002, https://link.aps.org/doi/10.1103/PhysRevLett. 112.203002
-
[13]
P. Asenbaum, C. Overstreet, M. Kim, J. Curti, M. A. Kasevich, Atom-Interferometric Test of the Equivalence Principle at the 10 −12 Level.Phys. Rev. Lett.125, 191101 (2020), doi: 10.1103/PhysRevLett.125.191101, https://link.aps.org/doi/10.1103/PhysRevLett.125.191101
-
[14]
Barrett,et al., Dual matter-wave inertial sensors in weightlessness.Nat
B. Barrett,et al., Dual matter-wave inertial sensors in weightlessness.Nat. Commun.7(1), 13786 (2016), doi:10.1038/ncomms13786, https://doi.org/10.1038/ncomms13786
-
[15]
S. Schaffrath, D. St ¨ork, F. Di Pumpo, E. Giese, Unified laboratory-frame analysis of atomic gravitational-wave sensors.AVS Quantum Sci.7(4), 044402 (2025), doi:10.1116/5.0304468, https://doi.org/10.1116/5.0304468
-
[16]
N. Yu, M. Tinto, Gravitational wave detection with single-laser atom interferometers.Gen. Relativ. Gravitation43(7), 1943–1952 (2011), doi:10.1007/s10714-010-1055-8, https://doi. org/10.1007/s10714-010-1055-8
-
[17]
W. Chaibi,et al., Low frequency gravitational wave detection with ground-based atom in- terferometer arrays.Phys. Rev. D93, 021101 (2016), doi:10.1103/PhysRevD.93.021101, https://link.aps.org/doi/10.1103/PhysRevD.93.021101
-
[18]
B. Barrett,et al., Correlative methods for dual-species quantum tests of the weak equivalence principle.New J. Phys.17(8), 085010 (2015), doi:10.1088/1367-2630/17/8/085010, https: //doi.org/10.1088/1367-2630/17/8/085010. 30
-
[19]
B. Barrett,et al., Testing the universality of free fall using correlated 39K–87Rb atom interferometers.AVS Quantum Sci.4(1), 014401 (2022), doi:10.1116/5.0076502, https: //doi.org/10.1116/5.0076502
-
[20]
K. Bongs,et al., Taking atom interferometric quantum sensors from the laboratory to real- world applications.Nat. Rev. Phys.1(12), 731–739 (2019), doi:10.1038/s42254-019-0117-4, https://doi.org/10.1038/s42254-019-0117-4
-
[21]
E. R. Elliott,et al., Quantum gas mixtures and dual-species atom interferometry in space. Nature623(7987), 502–508 (2023), doi:10.1038/s41586-023-06645-w, https://doi.org/10. 1038/s41586-023-06645-w
-
[22]
M. Meister,et al., Space magnetometry with a differential atom interferometer (2025), https: //arxiv.org/abs/2505.23532
-
[23]
K. S. Hardman,et al., Simultaneous Precision Gravimetry and Magnetic Gradiometry with a Bose-Einstein Condensate: A High Precision, Quantum Sensor.Phys. Rev. Lett.117, 138501 (2016), doi:10.1103/PhysRevLett.117.138501, https://link.aps.org/doi/10.1103/PhysRevLett. 117.138501
-
[24]
M.-K. Zhou,et al., Precisely mapping the magnetic field gradient in vacuum with an atom interferometer.Phys. Rev. A82, 061602 (2010), doi:10.1103/PhysRevA.82.061602, https: //link.aps.org/doi/10.1103/PhysRevA.82.061602
-
[25]
Z.-K. Hu,et al., Simultaneous differential measurement of a magnetic-field gradient by atom interferometry using double fountains.Phys. Rev. A84, 013620 (2011), doi:10.1103/PhysRevA. 84.013620, https://link.aps.org/doi/10.1103/PhysRevA.84.013620
-
[26]
T. L. Gustavson, A. Landragin, M. A. Kasevich, Rotation sensing with a dual atom- interferometer Sagnac gyroscope.Classical Quantum Gravity17(12), 2385 (2000), doi: 10.1088/0264-9381/17/12/311, https://doi.org/10.1088/0264-9381/17/12/311
-
[27]
Berg,et al., Composite-Light-Pulse Technique for High-Precision Atom Interferometry
P. Berg,et al., Composite-Light-Pulse Technique for High-Precision Atom Interferometry. Phys. Rev. Lett.114, 063002 (2015), doi:10.1103/PhysRevLett.114.063002, https://link.aps. org/doi/10.1103/PhysRevLett.114.063002. 31
-
[28]
Canuel,et al., Six-Axis Inertial Sensor Using Cold-Atom Interferometry.Phys
B. Canuel,et al., Six-Axis Inertial Sensor Using Cold-Atom Interferometry.Phys. Rev. Lett.97, 010402 (2006), doi:10.1103/PhysRevLett.97.010402, https://link.aps.org/doi/10. 1103/PhysRevLett.97.010402
-
[29]
M. M. Beydler, E. R. Moan, Z. Luo, Z. Chu, C. A. Sackett, Guided-wave Sagnac atom interferometer with large area and multiple orbits.AVS Quantum Sci.6(1), 014401 (2024), doi:10.1116/5.0173769, https://doi.org/10.1116/5.0173769
-
[30]
Sorrentino,et al., Sensitivity limits of a Raman atom interferometer as a gravity gradiometer
F. Sorrentino,et al., Sensitivity limits of a Raman atom interferometer as a gravity gradiometer. Phys. Rev. A89, 023607 (2014), doi:10.1103/PhysRevA.89.023607, https://link.aps.org/doi/ 10.1103/PhysRevA.89.023607
-
[31]
M. J. Snadden, J. M. McGuirk, P. Bouyer, K. G. Haritos, M. A. Kasevich, Measurement of the Earth’s Gravity Gradient with an Atom Interferometer-Based Gravity Gradiometer.Phys. Rev. Lett.81, 971–974 (1998), doi:10.1103/PhysRevLett.81.971, https://link.aps.org/doi/10.1103/ PhysRevLett.81.971
-
[32]
A. Bertoldi,et al., Atom interferometry gravity-gradiometer for the determination of the Newtonian gravitational constant G.Eur. Phys. J. D40(2), 271–279 (2006), doi:10.1140/epjd/ e2006-00212-2, https://doi.org/10.1140/epjd/e2006-00212-2
-
[33]
S. M. Dickerson, J. M. Hogan, A. Sugarbaker, D. M. S. Johnson, M. A. Kasevich, Mul- tiaxis Inertial Sensing with Long-Time Point Source Atom Interferometry.Phys. Rev. Lett. 111, 083001 (2013), doi:10.1103/PhysRevLett.111.083001, https://link.aps.org/doi/10.1103/ PhysRevLett.111.083001
-
[34]
G. T. Foster, J. B. Fixler, J. M. McGuirk, M. A. Kasevich, Method of phase extraction between coupled atom interferometers using ellipse-specific fitting.Opt. Lett.27(11), 951 (2002), doi:10.1364/ol.27.000951
-
[35]
X. Zhang,et al., Dependence of the ellipse fitting noise on the differential phase between interferometers in atom gravity gradiometers.Opt. Express31(26), 44102–44112 (2023), doi:10.1364/OE.507695, https://opg.optica.org/oe/abstract.cfm?URI=oe-31-26-44102. 32
-
[36]
A. Fitzgibbon, M. Pilu, R. Fisher, Direct least square fitting of ellipses.IEEE Transactions on Pattern Analysis and Machine Intelligence21(5), 476–480 (1999), doi:10.1109/34.765658
-
[37]
Z. L. Szpak, W. Chojnacki, A. van den Hengel, Guaranteed Ellipse Fitting with the Sampson Distance, inComputer Vision – ECCV 2012, A. Fitzgibbon, S. Lazebnik, P. Perona, Y. Sato, C. Schmid, Eds. (Springer Berlin Heidelberg, Berlin, Heidelberg) (2012), pp. 87–100
work page 2012
-
[38]
Joint Committee for Guides in Metrology, International Vocabulary of Metrology – Basic and general concepts and associated terms (VIM), 3rd edition, JCGM 200:2012 (2012), doi: 10.59161/JCGM200-2012, https://doi.org/10.59161/JCGM200-2012
-
[39]
Accuracy (trueness and precision) of measurement methods and results — Part 1: General principles and definitions (2023), https://www.iso.org/obp/ui/#iso:std:iso:5725:-1:ed-2:v1:en, 2nd edition, July 2023
work page 2023
-
[40]
Roura, Gravitational Redshift in Quantum-Clock Interferometry.Phys
A. Roura, Gravitational Redshift in Quantum-Clock Interferometry.Phys. Rev. X 10, 021014 (2020), doi:10.1103/PhysRevX.10.021014, https://link.aps.org/doi/10.1103/ PhysRevX.10.021014
-
[41]
Di Pumpo,et al., Gravitational Redshift Tests with Atomic Clocks and Atom Interferometers
F. Di Pumpo,et al., Gravitational Redshift Tests with Atomic Clocks and Atom Interferometers. PRX Quantum2, 040333 (2021), doi:10.1103/PRXQuantum.2.040333, https://link.aps.org/ doi/10.1103/PRXQuantum.2.040333
-
[42]
G. Rosi,et al., Quantum test of the equivalence principle for atoms in coherent superposition of internal energy states.Nat. Commun.8(1), 15529 (2017), doi:10.1038/ncomms15529, https://doi.org/10.1038/ncomms15529
-
[43]
J. Borregaard, I. Pikovski, Testing quantum theory on curved spacetime with quantum networks. Phys. Rev. Res.7, 023192 (2025), doi:10.1103/PhysRevResearch.7.023192, https://link.aps. org/doi/10.1103/PhysRevResearch.7.023192
-
[44]
C. Fromonteil,et al., Non-local mass superpositions and optical clock interferometry in atomic ensemble quantum networks (2025), https://arxiv.org/abs/2509.19501. 33
-
[45]
M. G¨ undo˘gan, R. Barzel, D. R¨atzel, Gravitational time dilation in quantum clock interferometry with entangled multi-photon states and quantum memories.arXiv(2026), https://doi.org/10. 48550/arXiv.2601.02470
-
[46]
M. Zych, F. Costa, I. Pikovski, ˇC. Brukner, Quantum interferometric visibility as a witness of general relativistic proper time.Nat. Commun.2(1), 505 (2011), doi:10.1038/ncomms1498, https://doi.org/10.1038/ncomms1498
-
[47]
J. P. Covey, I. Pikovski, J. Borregaard, Probing Curved Spacetime with a Distributed Atomic Processor Clock.PRX Quantum6, 030310 (2025), doi:10.1103/q188-b1cr, https://link.aps. org/doi/10.1103/q188-b1cr
-
[48]
Loriani,et al., Interference of clocks: A quantum twin paradox.Sci
S. Loriani,et al., Interference of clocks: A quantum twin paradox.Sci. Adv.5(10), eaax8966 (2019), doi:10.1126/sciadv.aax8966, https://www.science.org/doi/abs/10.1126/ sciadv.aax8966
-
[49]
Y. Margalit,et al., A self-interfering clock as a “which path” witness.Science349(6253), 1205– 1208 (2015), doi:10.1126/science.aac6498, https://www.science.org/doi/abs/10.1126/science. aac6498
-
[50]
Geiger,et al., Detecting inertial effects with airborne matter-wave interferometry.Nat
R. Geiger,et al., Detecting inertial effects with airborne matter-wave interferometry.Nat. Commun.2(1), 474 (2011), doi:10.1038/ncomms1479, https://doi.org/10.1038/ncomms1479
-
[51]
Abend,et al., Atom-Chip Fountain Gravimeter.Phys
S. Abend,et al., Atom-Chip Fountain Gravimeter.Phys. Rev. Lett.117, 203003 (2016), doi: 10.1103/PhysRevLett.117.203003, https://link.aps.org/doi/10.1103/PhysRevLett.117.203003
-
[52]
Pelluet,et al., Atom interferometry in an Einstein Elevator.Nat
C. Pelluet,et al., Atom interferometry in an Einstein Elevator.Nat. Commun.16(1), 4812 (2025), doi:10.1038/s41467-025-60042-7, https://doi.org/10.1038/s41467-025-60042-7
-
[53]
Z. Zhou, S. C. Carrasco, C. Sanner, V. S. Malinovsky, R. Folman, Geometric phase amplification in a clock interferometer for enhanced metrology.Sci. Adv.11(18), eadr6893 (2025), doi: 10.1126/sciadv.adr6893, https://www.science.org/doi/abs/10.1126/sciadv.adr6893
-
[54]
X. Zheng, J. Dolde, M. C. Cambria, H. M. Lim, S. Kolkowitz, A lab-based test of the grav- itational redshift with a miniature clock network.Nat. Commun.14(1), 4886 (2023), doi: 10.1038/s41467-023-40629-8, https://doi.org/10.1038/s41467-023-40629-8. 34
-
[55]
T. Bothwell,et al., Resolving the gravitational redshift across a millimetre-scale atomic sam- ple.Nature602(7897), 420–424 (2022), doi:10.1038/s41586-021-04349-7, https://doi.org/10. 1038/s41586-021-04349-7
-
[56]
C. Struckmann,et al., Platform and environment requirements of a satellite quantum test of the weak equivalence principle at the 10 −17 level.Phys. Rev. D109, 064010 (2024), doi: 10.1103/PhysRevD.109.064010, https://link.aps.org/doi/10.1103/PhysRevD.109.064010
-
[57]
S. Hartmann,et al., Regimes of atomic diffraction: Raman versus Bragg diffraction in retrore- flective geometries.Phys. Rev. A101, 053610 (2020), doi:10.1103/PhysRevA.101.053610, https://link.aps.org/doi/10.1103/PhysRevA.101.053610
-
[58]
T. Lauber, J. K¨ uber, O. Wille, G. Birkl, Optimized Bose-Einstein-condensate production in a dipole trap based on a 1070-nm multifrequency laser: Influence of enhanced two-body loss on the evaporation process.Phys. Rev. A84(4), 043641 (2011), doi:10.1103/PhysRevA.84. 043641, https://link.aps.org/doi/10.1103/PhysRevA.84.043641
-
[59]
D. Pfeiffer, M. Dietrich, P. Schach, G. Birkl, E. Giese, Dichroic mirror pulses for opti- mized higher-order atomic Bragg diffraction.Phys. Rev. Res.7, L012028 (2025), doi:10.1103/ PhysRevResearch.7.L012028, https://link.aps.org/doi/10.1103/PhysRevResearch.7.L012028
-
[60]
R. B. Blackman, J. W. Tukey, The Measurement of Power Spectra from the Point of View of Communications Engineering — Part I.Bell System Technical Journal37(1), 185–282 (1958), doi:https://doi.org/10.1002/j.1538-7305.1958.tb03874.x, https://onlinelibrary.wiley.com/doi/ abs/10.1002/j.1538-7305.1958.tb03874.x
-
[61]
Weisstein, Blackman Function,MathWorld–A Wolfram Resource, https://mathworld
E. Weisstein, Blackman Function,MathWorld–A Wolfram Resource, https://mathworld. wolfram.com/BlackmanFunction.html
-
[62]
S.-w. Chiow, T. Kovachy, H.-C. Chien, M. A. Kasevich, 102ℏ𝑘Large Area Atom In- terferometers.Phys. Rev. Lett.107, 130403 (2011), doi:10.1103/PhysRevLett.107.130403, https://link.aps.org/doi/10.1103/PhysRevLett.107.130403. 35
-
[63]
Berrada,et al., Integrated Mach–Zehnder interferometer for Bose–Einstein conden- sates.Nat
T. Berrada,et al., Integrated Mach–Zehnder interferometer for Bose–Einstein conden- sates.Nat. Commun.4(1), 2077 (2013), doi:10.1038/ncomms3077, https://doi.org/10.1038/ ncomms3077
-
[64]
A. Bertoldi, F. Minardi, M. Prevedelli, Phase shift in atom interferometers: Corrections for nonquadratic potentials and finite-duration laser pulses.Phys. Rev. A99, 033619 (2019), doi: 10.1103/PhysRevA.99.033619, https://link.aps.org/doi/10.1103/PhysRevA.99.033619
-
[65]
W. Gerlach, O. Stern,Der experimentelle Nachweis der Richtungsquantelung im Mag- netfeld(Springer Berlin Heidelberg, Berlin, Heidelberg), pp. 26–29 (1989), doi:10.1007/ 978-3-642-74813-4 4, https://doi.org/10.1007/978-3-642-74813-4 4
-
[66]
Der experimentelle Nachweis der Richtungsquantelung im Magnetfeld
M. Bauer, The Stern-Gerlach Experiment, Translation of: “Der experimentelle Nachweis der Richtungsquantelung im Magnetfeld” (2023), https://arxiv.org/abs/2301.11343
- [67]
-
[68]
Efron, The Bootstrap and Modern Statistics.J
B. Efron, The Bootstrap and Modern Statistics.J. Am. Stat. Assoc.95(452), 1293– 1296 (2000), doi:10.1080/01621459.2000.10474333, https://www.tandfonline.com/doi/abs/ 10.1080/01621459.2000.10474333
-
[69]
A. Zoubir, B. Boashash, The bootstrap and its application in signal processing.IEEE Signal Processing Magazine15(1), 56–76 (1998), doi:10.1109/79.647043
-
[70]
Rosi,et al., Measurement of the Gravity-Field Curvature by Atom Interferometry.Phys
G. Rosi,et al., Measurement of the Gravity-Field Curvature by Atom Interferometry.Phys. Rev. Lett.114, 013001 (2015), doi:10.1103/PhysRevLett.114.013001, https://link.aps.org/doi/ 10.1103/PhysRevLett.114.013001
-
[71]
X. Jiang, D.-C. Cheng, Fitting of 3D circles and ellipses using a parameter decomposition approach, inFifth International Conference on 3-D Digital Imaging and Modeling (3DIM’05) (2005), pp. 103–109, doi:10.1109/3DIM.2005.46
-
[72]
Signature of grav ity waves in the polarization of the mi- crowave background
S.-w. Chiow, S. Herrmann, S. Chu, H. M¨ uller, Noise-Immune Conjugate Large-Area Atom Interferometers.Physical Review Letters103(5), 050402 (2009), doi:10.1103/PhysRevLett. 103.050402, https://link.aps.org/doi/10.1103/PhysRevLett.103.050402. 36
- [73]
-
[74]
C. Hill, Ellipse Fitting Algorithm, scipython.com, https://scipython.com/blog/ direct-linear-least-squares-fitting-of-an-ellipse/
-
[75]
K. Ridley, A. Rodgers, An investigation of errors in ellipse-fitting for cold-atom interferometers. EPJ Quantum Technol.11(1), 79 (2024), doi:10.1140/epjqt/s40507-024-00292-4, https://doi. org/10.1140/epjqt/s40507-024-00292-4
-
[76]
W. Gander, G. H. Golub, R. Strebel, Least-squares fitting of circles and ellipses.BIT34(4), 558–578 (1994), doi:10.1007/bf01934268, https://doi.org/10.1007/BF01934268
-
[77]
S. J. Ahn, W. Rauh, H.-J. Warnecke, Least-squares orthogonal distances fitting of cir- cle, sphere, ellipse, hyperbola, and parabola.Pattern Recognit.34(12), 2283–2303 (2001), doi:10.1016/S0031-3203(00)00152-7, https://www.sciencedirect.com/science/article/ pii/S0031320300001527
-
[78]
X. Chen,et al., Proportional-scanning-phase method to suppress the vibrational noise in non- isotope dual-atom-interferometer-based weak-equivalence-principle-test experiments.Phys. Rev. A90, 023609 (2014), doi:10.1103/PhysRevA.90.023609, https://link.aps.org/doi/10.1103/ PhysRevA.90.023609
-
[79]
H. M¨ uller, S.-w. Chiow, Q. Long, S. Herrmann, S. Chu, Atom Interferometry with up to 24-Photon-Momentum-Transfer Beam Splitters.Phys. Rev. Lett.100, 180405 (2008), doi: 10.1103/PhysRevLett.100.180405, https://link.aps.org/doi/10.1103/PhysRevLett.100.180405
-
[80]
T. Kovachy,et al., Quantum superposition at the half-metre scale.Nature528(7583), 530–533 (2015), doi:10.1038/nature16155, https://doi.org/10.1038/nature16155
-
[81]
d’ Armagnac de Castanet,et al., Atom interferometry at arbitrary orientations and rotation rates.Nat
Q. d’ Armagnac de Castanet,et al., Atom interferometry at arbitrary orientations and rotation rates.Nat. Commun.15(1), 6406 (2024), doi:10.1038/s41467-024-50804-0, https://doi.org/ 10.1038/s41467-024-50804-0. 37
discussion (0)
Sign in with ORCID, Apple, or X to comment. Anyone can read and Pith papers without signing in.