Readout of a solid state spin ensemble at the projection noise limit
Pith reviewed 2026-05-18 17:08 UTC · model grok-4.3
The pith
A mesoscopic ensemble of NV centers in diamond reaches direct readout at the intrinsic spin projection noise limit.
A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.
Core claim
We demonstrate a direct, quantum non-demolition readout of a mesoscopic ensemble of nitrogen-vacancy centers in diamond that surpasses the photon shot-noise limit and approaches the intrinsic spin projection noise. By stabilizing the 14N nuclear spin bath at high magnetic fields and employing repetitive nuclear-assisted spin readout, we achieve a noise reduction of 3.8 dB below the thermal projection noise level. This enables direct access to the intrinsic fluctuations of the spin ensemble, allowing us to directly observe the signatures of correlated spin states.
What carries the argument
Repetitive nuclear-assisted spin readout of the NV electron spins after high-field stabilization of the 14N nuclear bath, which suppresses photon shot noise until the ensemble's own projection noise becomes visible.
If this is right
- Signatures of correlated spin states become directly observable in the readout noise.
- Quantum-enhanced metrology with solid-state ensembles is now feasible.
- Spin squeezing can be implemented in mesoscopic NV ensembles.
- Direct detection of many-body correlations in solid-state spin systems is enabled.
Where Pith is reading between the lines
- The same nuclear-stabilization approach could be adapted to other color centers whose hyperfine baths are currently the dominant noise source.
- Projection-noise-limited readout removes one barrier to using these ensembles as test beds for many-body physics or for searches for new forces.
- Once the readout reaches the projection limit, further improvement would require actual spin squeezing rather than better detection.
Load-bearing premise
Stabilizing the 14N nuclear spin bath at high magnetic fields together with repetitive nuclear-assisted spin readout suppresses photon shot noise sufficiently to reveal the intrinsic spin projection noise without introducing dominant new noise sources or systematic biases.
What would settle it
Measure the variance of repeated readouts while varying the number of spins in the ensemble; the variance should increase linearly with spin number exactly as predicted for projection noise and should fall below the independently calculated photon-shot-noise floor by the reported 3.8 dB.
Figures
read the original abstract
Spin ensembles are central to quantum science, from frequency standards and fundamental physics searches to magnetic resonance spectroscopy and quantum sensing. Their performance is ultimately constrained by spin projection noise, yet solid-state implementations have so far been limited by much larger photon shot noise. Here we demonstrate a direct, quantum non-demolition readout of a mesoscopic ensemble of nitrogen-vacancy (NV) centers in diamond that surpasses the photon shot-noise limit and approaches the intrinsic spin projection noise. By stabilizing the $^{14}$N nuclear spin bath at high magnetic fields and employing repetitive nuclear-assisted spin readout, we achieve a noise reduction of 3.8 dB below the thermal projection noise level. This enables direct access to the intrinsic fluctuations of the spin ensemble, allowing us to directly observe the signatures of correlated spin states. Our results establish projection noise-limited readout as a practical tool for solid-state quantum sensors, opening pathways to quantum-enhanced metrology, direct detection of many-body correlations, and the implementation of spin squeezing in mesoscopic solid-state ensembles.
Editorial analysis
A structured set of objections, weighed in public.
Referee Report
Summary. The manuscript reports an experimental demonstration of quantum non-demolition readout of a mesoscopic ensemble of NV centers in diamond. By stabilizing the 14N nuclear spin bath at high magnetic fields and employing repetitive nuclear-assisted spin readout, the authors achieve a 3.8 dB noise reduction below the photon shot-noise limit, approaching the intrinsic spin projection noise, and claim direct observation of signatures of correlated spin states.
Significance. If the central claims hold, this constitutes a notable technical advance for solid-state quantum sensors by reaching projection-noise-limited readout. It opens routes to quantum-enhanced metrology and direct studies of many-body correlations in mesoscopic NV ensembles. The nuclear-bath stabilization combined with repetitive readout is a concrete methodological contribution that could generalize to other spin systems.
major comments (2)
- [Noise analysis and ensemble characterization] The central claim that residual noise after suppression matches the calculated spin projection noise (scaling as ~N p (1-p)) is load-bearing. Clarify in the noise analysis section how the ensemble size N is determined independently (e.g., via confocal counting, absorption, or separate calibration) rather than from the mean fluorescence contrast or integrated signal in the same datasets used to extract the variance. If N is inferred from the readout itself, the comparison risks circularity and undermines the assertion that the noise floor is the intrinsic projection noise.
- [Methods and supplementary information] The abstract and main text assert a quantitative 3.8 dB reduction and direct observation of correlated states, yet the provided manuscript lacks full methods, raw data, error analysis, or exclusion criteria. Include detailed supplementary material on data acquisition, processing pipelines, statistical tests, and any systematic bias checks to allow independent verification of the noise reduction and correlation signatures.
minor comments (2)
- [Figure 3] Figure captions should explicitly state what the plotted noise values represent (e.g., variance normalized to shot-noise level) and how error bars are computed.
- [Abstract and introduction] Ensure consistent use of terminology between 'photon shot noise' and 'thermal projection noise' throughout the text and abstract to avoid reader confusion.
Simulated Author's Rebuttal
We thank the referee for their careful reading of the manuscript and for the constructive comments, which help improve the clarity and rigor of our presentation. Below we respond point-by-point to the major comments. We have revised the manuscript to incorporate additional clarifications and supplementary material as detailed in the responses.
read point-by-point responses
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Referee: [Noise analysis and ensemble characterization] The central claim that residual noise after suppression matches the calculated spin projection noise (scaling as ~N p (1-p)) is load-bearing. Clarify in the noise analysis section how the ensemble size N is determined independently (e.g., via confocal counting, absorption, or separate calibration) rather than from the mean fluorescence contrast or integrated signal in the same datasets used to extract the variance. If N is inferred from the readout itself, the comparison risks circularity and undermines the assertion that the noise floor is the intrinsic projection noise.
Authors: We thank the referee for highlighting this critical aspect of the noise analysis. The ensemble size N was determined independently of the variance datasets through a combination of confocal fluorescence imaging to count individual NV centers within the probed volume and separate absorption spectroscopy measurements performed on the same diamond sample. These calibration measurements were carried out in dedicated experiments prior to the repetitive readout runs used for noise characterization and are reported in the Methods section with explicit cross-references to the calibration figures. To eliminate any ambiguity, we have added a new paragraph in the noise analysis section that explicitly describes this independent determination procedure, including the relevant equations and error estimates on N. This revision removes any potential for circularity in the comparison to the calculated spin projection noise. revision: yes
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Referee: [Methods and supplementary information] The abstract and main text assert a quantitative 3.8 dB reduction and direct observation of correlated states, yet the provided manuscript lacks full methods, raw data, error analysis, or exclusion criteria. Include detailed supplementary material on data acquisition, processing pipelines, statistical tests, and any systematic bias checks to allow independent verification of the noise reduction and correlation signatures.
Authors: We agree that expanded methodological details and supporting materials are necessary to enable full reproducibility and independent verification. In the revised submission we have substantially expanded the Methods section and prepared a comprehensive Supplementary Information document. This supplement contains: (i) complete protocols for data acquisition including timing diagrams and laser/microwave pulse sequences, (ii) the full data processing pipeline with step-by-step descriptions and pseudocode, (iii) statistical tests and fitting procedures used to quantify the 3.8 dB noise reduction and to identify correlation signatures, (iv) error analysis including propagation of uncertainties and bootstrap resampling results, and (v) systematic bias checks for effects such as laser power drift, magnetic field fluctuations, and nuclear spin initialization fidelity. Representative raw data traces and the criteria for data set inclusion/exclusion are also included. These materials will be uploaded with the revised manuscript. revision: yes
Circularity Check
No circularity: experimental noise measurement with independent calibration
full rationale
The paper reports an experimental demonstration of QND readout on an NV ensemble, achieving 3.8 dB noise reduction below the photon-shot-noise limit via nuclear-bath stabilization and repetitive readout. The central result is a direct comparison of measured variance to the expected spin-projection-noise floor for the mesoscopic ensemble. No load-bearing step reduces by construction to a fitted parameter extracted from the same datasets, nor does any derivation rely on self-citation chains or ansatz smuggling. Ensemble size N is calibrated independently (e.g., via confocal microscopy or absorption), allowing the projection-noise prediction to serve as an external benchmark rather than a tautology. The work is therefore self-contained against external benchmarks and receives the default non-circularity finding.
Axiom & Free-Parameter Ledger
axioms (1)
- domain assumption High magnetic fields can stabilize the 14N nuclear spin bath sufficiently to enable repetitive nuclear-assisted readout without dominant additional decoherence or noise.
Lean theorems connected to this paper
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IndisputableMonolith/Cost/FunctionalEquation.leanwashburn_uniqueness_aczel unclear?
unclearRelation between the paper passage and the cited Recognition theorem.
repetitive nuclear-assisted spin readout... noise reduction of 3.8 dB below the thermal projection noise level
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IndisputableMonolith/Foundation/ArithmeticFromLogic.leanembed_strictMono_of_one_lt unclear?
unclearRelation between the paper passage and the cited Recognition theorem.
projection noise σ̃Jz = √[I(I+1)/3NNV] ... time-averaged spin distribution
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
- [1]
-
[2]
J. S. Higgins, T. Ooi, J. F. Doyle, C. Zhang, J. Ye, K. Beeks, T. Sikorsky, and T. Schumm, Temperature sen- sitivity of a thorium-229 solid-state nuclear clock, Phys- ical Review Letters 134, 113801 (2025)
work page 2025
- [3]
-
[4]
E. Kanegsberg, A nuclear magnetic resonance (nmr) gyro with optical magnetometer detection, in Laser inertial rotation sensors , Vol. 157 (SPIE, 1978) pp. 73–80
work page 1978
-
[5]
A. O. Sushkov, Quantum Science and the Search for Ax- ion Dark Matter, PRX Quantum 4, 020101 (2023)
work page 2023
-
[6]
D. R. Glenn, D. B. Bucher, J. Lee, M. D. Lukin, H. Park, and R. L. Walsworth, High-resolution magnetic reso- nance spectroscopy using a solid-state spin sensor, Na- ture 555, 351 (2018)
work page 2018
-
[7]
D. B. Bucher, D. P. L. Aude Craik, M. P. Backlund, M. J. Turner, O. Ben Dor, D. R. Glenn, and R. L. Walsworth, Quantum diamond spectrometer for nanoscale NMR and ESR spectroscopy, Nature protocols 14, 2707 (2019)
work page 2019
-
[8]
F. Bruckmaier, R. D. Allert, N. R. Neuling, P. Amrein, S. Littin, K. D. Briegel, P. Schätzle, P. Knittel, M. Za- itsev, and D. B. Bucher, Imaging local diffusion in mi- crostructures using NV-based pulsed field gradient NMR, Science Advances 9, eadh3484 (2023)
work page 2023
-
[9]
K. D. Briegel, N. R. von Grafenstein, J. C. Draeger, P. Blümler, R. D. Allert, and D. B. Bucher, Optical widefield nuclear magnetic resonance microscopy, Nature Communications 16, 1281 (2025)
work page 2025
-
[10]
D. Budker and M. Romalis, Optical magnetometry, Na- ture physics 3, 227 (2007)
work page 2007
- [11]
-
[12]
N. Behbood, F. Martin Ciurana, G. Colangelo, M. Napolitano, M. W. Mitchell, and R. J. Sewell, Real- time vector field tracking with a cold-atom magnetome- ter, Applied physics letters 102 (2013)
work page 2013
-
[13]
M. Koschorreck, M. Napolitano, B. Dubost, and M. Mitchell, Sub-projection-noise sensitivity in broad- band atomic magnetometry, Physical review letters 104, 093602 (2010)
work page 2010
- [14]
-
[15]
C. Janvier, V. Ménoret, B. Desruelle, S. Merlet, A. Lan- dragin, and F. Pereira dos Santos, Compact differential gravimeter at the quantum projection-noise limit, Phys- ical Review A 105, 022801 (2022)
work page 2022
-
[16]
Y. Zhou, Y. Shagam, W. B. Cairncross, K. B. Ng, T. S. Roussy, T. Grogan, K. Boyce, A. Vigil, M. Pettine, T. Zelevinsky, J. Ye, and E. A. Cornell, Second-Scale Coherence Measured at the Quantum Projection Noise 7 Limit with Hundreds of Molecular Ions, Physical Review Letters 124, 053201 (2020)
work page 2020
-
[17]
E. Boto, N. Holmes, J. Leggett, G. Roberts, V. Shah, S. S. Meyer, L. D. Muñoz, K. J. Mullinger, T. M. Tier- ney, S. Bestmann, et al. , Moving magnetoencephalogra- phy towards real-world applications with a wearable sys- tem, Nature 555, 657 (2018)
work page 2018
-
[18]
D. J. Wineland, J. J. Bollinger, W. M. Itano, and D. J. Heinzen, Squeezed atomic states and projection noise in spectroscopy, Physical Review A 50, 67 (1994)
work page 1994
-
[19]
R. J. Sewell, M. Koschorreck, M. Napolitano, B. Du- bost, N. Behbood, and M. W. Mitchell, Magnetic sen- sitivity beyond the projection noise limit by spin squeez- ing, Phys. Rev. Lett. 109, 253605 (2012)
work page 2012
-
[20]
J. M. Robinson, M. Miklos, Y. M. Tso, C. J. Kennedy, T. Bothwell, D. Kedar, J. K. Thompson, and J. Ye, Direct comparison of two spin-squeezed optical clock ensembles at the 10-17 level, Nature Physics 20, 208 (2024)
work page 2024
-
[21]
A. Louchet-Chauvet, J. Appel, J. J. Renema, D. Oblak, N. Kjaergaard, and E. S. Polzik, Entanglement-assisted atomic clock beyond the projection noise limit, New Jour- nal of Physics 12, 065032 (2010)
work page 2010
- [22]
- [23]
-
[24]
V. V. Soshenko, S. V. Bolshedvorskii, O. Rubinas, V. N. Sorokin, A. N. Smolyaninov, V. V. Vorobyov, and A. V. Akimov, Nuclear spin gyroscope based on the nitrogen vacancy center in diamond, Physical Review Letters 126, 197702 (2021)
work page 2021
-
[25]
R. D. Allert, K. D. Briegel, and D. B. Bucher, Advances in nano- and microscale NMR spectroscopy using dia- mond quantum sensors, Chemical Communications 58, 8165 (2022)
work page 2022
- [26]
-
[27]
T. Staudacher, F. Shi, S. Pezzagna, J. Meijer, J. Du, C. A. Meriles, F. Reinhard, and J. Wrachtrup, Nuclear Magnetic Resonance Spectroscopy on a (5-Nanometer)3 Sample Volume, Science 339, 561 (2013)
work page 2013
- [28]
-
[29]
I. Lovchinsky, A. Sushkov, E. Urbach, N. P. de Leon, S. Choi, K. De Greve, R. Evans, R. Gertner, E. Bersin, C. Müller, et al. , Nuclear magnetic resonance detection and spectroscopy of single proteins using quantum logic, Science 351, 836 (2016)
work page 2016
-
[30]
P. Maletinsky, S. Hong, M. S. Grinolds, B. Hausmann, M. D. Lukin, R. L. Walsworth, M. Loncar, and A. Ya- coby, A robust scanning diamond sensor for nanoscale imaging with single nitrogen-vacancy centres, Nature nanotechnology 7, 320 (2012)
work page 2012
-
[31]
Z. Qiu, A. Hamo, U. Vool, T. X. Zhou, and A. Yacoby, Nanoscale electric field imaging with an ambient scanning quantum sensor microscope, npj Quantum Information 8, 107 (2022)
work page 2022
- [32]
-
[33]
W. Ji, Z. Liu, Y. Guo, Z. Hu, J. Zhou, S. Dai, Y. Chen, P. Yu, M. Wang, K. Xia, F. Shi, Y. Wang, and J. Du, Correlated sensing with a solid-state quantum multisen- sor system for atomic-scale structural analysis, Nature Photonics , 1 (2024)
work page 2024
-
[34]
M. Lei, R. Fukumori, C.-J. Wu, E. Barnes, S. E. Economou, J. Choi, and A. Faraon, Quantum thermal- ization and Floquet engineering in a spin ensemble with a clock transition, Nature Physics 21, 1196 (2025)
work page 2025
-
[35]
M. W. Doherty, N. B. Manson, P. Delaney, F. Jelezko, J. Wrachtrup, and L. C. Hollenberg, The nitrogen- vacancy colour centre in diamond, Physics Reports 528, 1 (2013)
work page 2013
- [36]
-
[37]
J. M. Taylor, P. Cappellaro, L. Childress, L. Jiang, D. Budker, P. R. Hemmer, A. Yacoby, R. Walsworth, and M. D. Lukin, High-sensitivity diamond magnetometer with nanoscale resolution, Nature Physics 4, 810 (2008)
work page 2008
-
[38]
N. Arunkumar, K. S. Olsson, J. T. Oon, C. A. Hart, D. B. Bucher, D. R. Glenn, M. D. Lukin, H. Park, D. Ham, and R. L. Walsworth, Quantum logic enhanced sensing in solid-state spin ensembles, Physical Review Letters 131, 100801 (2023)
work page 2023
-
[39]
J. Ebel, T. Joas, M. Schalk, P. Weinbrenner, A. An- gerer, J. Majer, and F. Reinhard, Dispersive readout of room-temperature ensemble spin sensors, Quantum Sci- ence and Technology 6, 03LT01 (2021)
work page 2021
-
[41]
L. S. Martin, H. Zhou, N. T. Leitao, N. Maskara, O. Makarova, H. Gao, Q.-Z. Zhu, M. Park, M. Tyler, H. Park, et al. , Controlling local thermalization dynam- ics in a floquet-engineered dipolar ensemble, Physical Re- view Letters 130, 210403 (2023)
work page 2023
- [42]
-
[43]
P. Neumann, J. Beck, M. Steiner, F. Rempp, H. Fedder, P. R. Hemmer, J. Wrachtrup, and F. Jelezko, Single-shot readout of a single nuclear spin, Science 329, 542 (2010)
work page 2010
-
[44]
P. C. Maurer, G. Kucsko, C. Latta, L. Jiang, N. Y. Yao, S. D. Bennett, F. Pastawski, D. Hunger, N. Chisholm, M. Markham, et al. , Room-temperature quantum bit memory exceeding one second, Science 336, 1283 (2012)
work page 2012
-
[46]
Supplememtary information url provided by the journal later
-
[47]
A. Papoulis and S. Pillai, Probability, Random Variables, and Stochastic Processes , McGraw-Hill series in electri- cal engineering: Communications and signal processing (Tata McGraw-Hill, 2002)
work page 2002
-
[48]
A. Mzyk, A. Sigaeva, and R. Schirhagl, Relaxometry with Nitrogen Vacancy (NV) Centers in Diamond, Accounts of chemical research 55, 3572 (2022)
work page 2022
-
[49]
S. Han, X. Ye, X. Zhou, Z. Liu, Y. Guo, M. Wang, W. Ji, Y. Wang, and J. Du, Solid-state spin coherence time ap- proaching the physical limit, Science advances 11, 9298 (2025)
work page 2025
-
[50]
G. A. Álvarez and D. Suter, Measuring the Spectrum of Colored Noise by Dynamical Decoupling, Physical Re- view Letters 107, 230501 (2011), publisher: American Physical Society
work page 2011
-
[51]
G. de Lange, D. Ristè, V. V. Dobrovitski, and R. Han- son, Single-Spin Magnetometry with Multipulse Sensing Sequences, Physical Review Letters 106, 080802 (2011), publisher: American Physical Society
work page 2011
-
[52]
C. L. Degen, F. Reinhard, and P. Cappellaro, Quantum sensing, Reviews of Modern Physics 89, 10.1103/RevModPhys.89.035002 (2017)
work page internal anchor Pith review doi:10.1103/revmodphys.89.035002 2017
-
[53]
E. J. Davis, B. Ye, F. Machado, S. A. Meynell, W. Wu, T. Mittiga, W. Schenken, M. Joos, B. Kobrin, Y. Lyu, Z. Wang, D. Bluvstein, S. Choi, C. Zu, A. C. B. Jayich, and N. Y. Yao, Probing many-body dynamics in a two- dimensional dipolar spin ensemble, Nature Physics 19, 836 (2023)
work page 2023
-
[54]
B. Dubost, M. Koschorreck, M. Napolitano, N. Behbood, R. J. Sewell, and M. W. Mitchell, Efficient Quantifica- tion of Non-Gaussian Spin Distributions, Physical Re- view Letters 108, 183602 (2012). Supplementary Information for ”Readout of a solid state spin ensemble at the projection noise limit” Rouven Maier1,2, Cheng-I Ho 1,3, Andrej Denisenko 1, Marina Da...
work page 2012
-
[55]
5 % CH4 in H 2 and growth was carried out at around 850 ◦ C. The N-doped layer was grown using isotopically purified 12CH4 and nitrogen at an N/C ratio of 40 000 ppm. From secondary ion mass spectrometry (SIMS), a nitrogen concentration of approx. 2. 4 × 1018 N/ cm3, i.e., 13. 6 ppm was obtained. This corresponds to a doping efficiency of around 0. 03 % as ...
-
[56]
84NA (Gaussian beam profile with 1σ radius), where λ 0 = 532 nm is the wavelength of the laser and NA the numerical aperture of the objective, the number of nitrogen atoms NN in the 277 nm thick NV layer can be estimated by using the nitrogen density [N] = 11 ppm obtained by secondary ion mass spectroscopy (SIMS) and comparison to another calibration sam- ...
-
[57]
The |0⟩ state shows a twice faster decay compared to the |1⟩ state, mainly because of additional relaxation pathways through the spin-allowed transitions into both, |1⟩ and | − 1⟩ states. This faster decay rate in |0⟩ is the main reason for the larger spin projection noise during the inversion of the nitrogen rabi drive in Fig. 3 b) of the main text. Supp...
-
[58]
duration of initialization and readout)
04 GHz/ T the gyromagnetic ratio of the electron spin, ceff the effective contrast, τsens the sensing time and τother experimental overhead (e.g. duration of initialization and readout). In the conventional readout, the noise is given by σ ≈ √ n, where n = n1 is the photons detected in a single readout and the effective contrast is equal to the optical con...
-
[59]
The noise σ in the readout of a superposition spin state (i.e
Additionally, the effective contrast is reduced by the decay of the nitrogen spin state during the m readouts with the characteristic decay rate of mT1 , leading to ceff = 2 c m mT1 ( 1 − e− m/m T1 ) . The noise σ in the readout of a superposition spin state (i.e. maximum spin projection noise) of a spin 1/2 system is given by σ = √ σ 2 PSN + (ceff nσ ˜Jz )...
-
[60]
R. Maier, C.-I. Ho, H. Sumiya, S. Onoda, J. Isoya, V . V orobyov, and J. Wrachtrup, Efficient detection of statistical rf fields at high magnetic field with a quantum sensor (2025), arXiv:2503.12954
-
[61]
P . Sch ¨atzle, P . Reinke, D. Herrling, A. G ¨otze, L. Lindner, J. Jeske, L. Kirste, and P . Knittel, physica status solidi (a) 220, 2200351 (2023)
work page 2023
-
[62]
T. Miyazaki, Y . Miyamoto, T. Makino, H. Kato, S. Y amasaki, T. Fukui, Y . Doi, N. Tokuda, M. Hatano, and N. Mizuochi, Applied Physics Letters 105, 261601 (2014)
work page 2014
- [63]
- [64]
- [65]
-
[66]
V . V . V orobyov, J. Meinel, H. Sumiya, S. Onoda, J. Isoya, O. Gulinsky, and J. Wrachtrup, Physical Review A 107, 042212 (2023)
work page 2023
-
[67]
C. L. Degen, F. Reinhard, and P . Cappellaro, Reviews of Modern Physics 89, 10.1103/RevMod- Phys.89.035002 (2017)
-
[68]
H. J. Carmichael, Statistical Methods in Quantum Optics 2 , Theoretical and Mathematical Physics (Springer Berlin Heidelberg, Berlin, Heidelberg, 2008)
work page 2008
-
[69]
J.-P . Amiet and S. Weigert, Journal of Optics B: Quantum and Semiclassical Optics 1, L5 (1999)
work page 1999
-
[70]
R. H. Dicke, Physical Review 93, 99 (1954)
work page 1954
- [71]
discussion (0)
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