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arxiv: 2504.20218 · v2 · submitted 2025-04-28 · 🪐 quant-ph · math-ph· math.MP

Fractional Angular Momentum and Quasi-Probability Densities for Angular Degrees of Freedom

Pith reviewed 2026-05-22 17:18 UTC · model grok-4.3

classification 🪐 quant-ph math-phmath.MP
keywords fractional angular momentumquasi-probability densitiesangular positionangular momentum operatorBorn's rulequantum witnessesuncertainties
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The pith

Properly defined two-parameter quasi-probability densities serve as witnesses for quantum behaviour in pure states involving angular position and angular momentum L, where negatives flag fractional mean L superpositions ambiguously.

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

The paper examines two-parameter quasi-probability densities for systems described by a self-adjoint angular position observable and the angular momentum operator L. It demonstrates that these densities can exhibit negative values for superpositions of angular momentum eigenstates possessing a fractional mean value of L, potentially revealing their quantum nature though in an ambiguous manner. For certain choices of parameters, the densities remain positive and align with the probabilities given by Born's rule in quantum mechanics. Additionally, measurements of the uncertainties in the angular position and L observables can be enough to uncover distinctive quantum-mechanical aspects of these states, without requiring the quasi-probability densities.

Core claim

In the present update work we consider properly defined two-parameter quasi-probability densities that, e.g., can be used as witness for quantum behaviour for a class of pure states as expressed in terms of a self-adjoint observable angular position and the corresponding angular momentum operator L. It is shown that negative values of the corresponding quasi-probability densities may reveal the quantum nature of superpositions of angular momentum eigenstates with a fractional mean value of L but in an ambiguous manner. For a suitable choice of parameters these quasi-probability densities are positive and are in accordance with Borns rule in quantum mechanics. It is also shown that experiment

What carries the argument

The two-parameter quasi-probability densities for angular position and angular momentum observables that can take negative values for certain superpositions or stay positive for suitable parameters.

If this is right

  • Negative values of the quasi-probability densities may reveal the quantum nature of superpositions with fractional mean angular momentum, but only in an ambiguous manner.
  • A suitable choice of parameters makes the quasi-probability densities positive and consistent with Born's rule.
  • Experimental data on the uncertainties for angular position and L observables can reveal unique quantum-mechanical features without using quasi-probability densities.

Where Pith is reading between the lines

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

  • The ambiguity in using negative values as a quantum witness suggests that uncertainties provide a more direct experimental route for angular systems.
  • These densities could be compared against other quasi-probability constructions like the Wigner function to test consistency across different parameter regimes.
  • If uncertainties alone suffice, then similar uncertainty-based tests might apply to other pairs of conjugate observables with periodic boundary conditions.

Load-bearing premise

The two-parameter quasi-probability densities are properly defined such that they can serve as witnesses for quantum behaviour in the class of pure states considered.

What would settle it

Preparing a superposition state with fractional mean angular momentum, computing or measuring the two-parameter quasi-probability density, and checking whether it shows negative values or stays positive under chosen parameters while matching Born rule probabilities.

Figures

Figures reproduced from arXiv: 2504.20218 by Bo-Sture K. Skagerstam, Per K. Rekdal.

Figure 1
Figure 1. Figure 1: The Wigner distribution W[θ, p] according to Eq.(15) with −π ≤ θ ≤ π and ¯θ = 0 for the state ψ(θ) as given in Eq.(3). In general W[θ, p] is bounded by |W[θ, p]| ≤ 1/2π . Here q = exp(−1/2λ) = 0.5 and integer-valued ¯l = l as a function of the parameter m = p−l in the range −2 ≤ m ≤ 2. With this choice of parameters W[θ, p] is then symmetric with respect to a line with m = 0. For half-integer values of m t… view at source ↗
Figure 2
Figure 2. Figure 2: The Wigner distribution W[θ, p] according to Eq.(15) for −π ≤ θ ≤ π as in Fig.1 now with q = exp(−1/2λ) = 0.001, ϵ = 1/2, and ¯l = l + 1/2 in the range −2 ≤ m ≤ 2 with m = p−l for the state ψ(θ) as in Eq.(3). The symmetry with respect to the line with m = 0 as in Fig.1 is now not present. For half-integer values of m the Wigner function W[θ, p] can be negative at |θ| = O(π) and the parameter p must then be… view at source ↗
Figure 3
Figure 3. Figure 3: The Wigner distribution W1/2[θ, p] according to Eq.(34) for −π ≤ θ ≤ π for −π ≤ θ ≤ π with q = 0.001, ¯l = l + ϵ, and ϵ = 1/2 for the state ψ(θ) according to Eq.(3) as a function of the parameter m = p − l in the range −2 ≤ m ≤ 2. As in Fig.2 the symmetry with respect to the line with m = 0 is absent. Regions of negativity for W1/2[θ, p] are in general not the same as in Fig.2 for the same quantum state co… view at source ↗
Figure 4
Figure 4. Figure 4: The upper solid curve corresponds to the uncertainty ∆ [PITH_FULL_IMAGE:figures/full_fig_p013_4.png] view at source ↗
read the original abstract

In the present update work we consider properly defined two-parameter quasi-probability densities that, e.g., can be used as witness for quantum behaviour for a class of pure states as expressed in terms of a self-adjoint observable angular position and the corresponding angular momentum operator L. It is shown that negative values of the corresponding quasi-probability densities may reveal the quantum nature of superpositions of angular momentum eigenstates with a fractional mean value of L but in an ambiguous manner. For a suitable choice of parameters these quasi-probability densities are positive and are in accordance with Borns rule in quantum mechanics. It is also shown that experimental data of the uncertainties for the angular position and L observables can be sufficient to reveal some unique quantum-mechanical features of such states without necessarily making use of quasi-probability densities.

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 / 1 minor

Summary. The manuscript presents an update on two-parameter quasi-probability densities for angular degrees of freedom, specifically for a self-adjoint angular position observable and the angular momentum operator L. It claims that negative values of these densities can indicate the quantum nature of superpositions of angular momentum eigenstates with fractional mean L, albeit ambiguously. For appropriate parameter choices, the densities are positive and consistent with Born's rule. Additionally, it suggests that experimental uncertainties in angular position and L can suffice to reveal unique quantum features without relying on quasi-probability densities.

Significance. If the claims hold, this work could advance the understanding of quasi-probability representations in systems with angular degrees of freedom, particularly highlighting the role of fractional angular momentum and providing uncertainty-based methods to detect quantum features. However, the abstract-only availability limits a full assessment of the novelty and impact.

major comments (2)
  1. [Abstract] The central claims depend on the proper definition of the two-parameter quasi-probability densities, but without access to the full manuscript, including mathematical definitions, derivations, and any supporting evidence or examples, it is not possible to evaluate whether these densities are rigorously defined or if the negativity indeed serves as an ambiguous witness for quantum behavior in the described states.
  2. [Abstract] The statement that 'experimental data of the uncertainties for the angular position and L observables can be sufficient to reveal some unique quantum-mechanical features' lacks any indication of the specific features or how the data suffices, making it difficult to assess the strength of this claim without further details.
minor comments (1)
  1. [Abstract] The abstract mentions 'Borns rule' which should be 'Born's rule' for grammatical correctness.

Simulated Author's Rebuttal

2 responses · 0 unresolved

We thank the referee for their comments on our manuscript. We address the major comments point by point below. The full manuscript on arXiv:2504.20218 contains the detailed mathematical definitions, derivations, and examples referenced in the abstract; we regret that only the abstract appears to have been available for review and are happy to expand the abstract or add clarifications as needed.

read point-by-point responses
  1. Referee: [Abstract] The central claims depend on the proper definition of the two-parameter quasi-probability densities, but without access to the full manuscript, including mathematical definitions, derivations, and any supporting evidence or examples, it is not possible to evaluate whether these densities are rigorously defined or if the negativity indeed serves as an ambiguous witness for quantum behavior in the described states.

    Authors: The full manuscript defines the two-parameter quasi-probability densities rigorously for the self-adjoint angular position observable and the angular momentum operator L, with explicit constructions, derivations of their properties, and concrete examples for superpositions of angular momentum eigenstates having fractional mean L. These examples illustrate how negativity can serve as an (ambiguous) witness for quantum behavior. We can revise the abstract to include a concise statement of the key definition if that addresses the concern. revision: partial

  2. Referee: [Abstract] The statement that 'experimental data of the uncertainties for the angular position and L observables can be sufficient to reveal some unique quantum-mechanical features' lacks any indication of the specific features or how the data suffices, making it difficult to assess the strength of this claim without further details.

    Authors: The full manuscript shows that measured uncertainties in angular position and L for the indicated states can violate classical bounds or exhibit signatures tied to the fractional mean angular momentum that are impossible for classical mixtures, thereby revealing quantum features directly from uncertainty data. We will revise the abstract to specify these features and the manner in which the data suffices. revision: yes

Circularity Check

0 steps flagged

No significant circularity detectable from abstract

full rationale

Only the abstract is provided, which states results on two-parameter quasi-probability densities for angular position and L without any equations, derivation steps, self-citations, or fitted parameters. No load-bearing claim reduces by construction to its inputs, as no specific mathematical chain or ansatz is exhibited. The assertions that negativity may reveal quantum features (ambiguously) and that suitable parameters yield positivity consistent with Born's rule are presented as demonstrated outcomes, but the absence of the underlying definitions or proofs means no circularity of any enumerated kind can be identified or quoted. The paper's claims appear self-contained within the given text.

Axiom & Free-Parameter Ledger

0 free parameters · 0 axioms · 0 invented entities

Abstract-only review provides no details on free parameters, axioms, or invented entities; full text required to identify any fitted values, background assumptions, or new postulated constructs.

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Reference graph

Works this paper leans on

60 extracted references · 60 canonical work pages

  1. [1]

    Wigner, ” On the Quantum Correction for Thermodynamic Equilibrium ”, Phys

    E. Wigner, ” On the Quantum Correction for Thermodynamic Equilibrium ”, Phys. Rev. 40 (1932) 749–759

  2. [2]

    Hudson, ” When is the Wigner Quasi-Probability Density Non-Negative? ”, Rep

    R.L. Hudson, ” When is the Wigner Quasi-Probability Density Non-Negative? ”, Rep. Math. Phys. 6 (1974) 249-252

  3. [3]

    O’Connell, ” The Wigner Distribution Function—50th Birthday ”, Found

    R.F. O’Connell, ” The Wigner Distribution Function—50th Birthday ”, Found. Phys. 13 (1983) 83–92

  4. [4]

    Hillery, R.F

    M. Hillery, R.F. O’Connell, M.O. Scully, and E.P. Wigner, ” Distribution functions in physics: Fundamentals ”, Phys. Rep. 106 (1984) 121–167. 15

  5. [5]

    Risken, ” Determination of Quasiprobability Distributions in Terms of Probability Distributions for the Rotated Quadrature Phase ”, Phys

    K.Vogel and H. Risken, ” Determination of Quasiprobability Distributions in Terms of Probability Distributions for the Rotated Quadrature Phase ”, Phys. Rev. A 40 (1989) 2847-2849

  6. [6]

    Buˇ zek and P.L

    V. Buˇ zek and P.L. Knight , ”I: Quantum Interference, Superposition States of Light, and Nonclassical Effects ”, in Prog. in Optics 34 (1995) 1-158

  7. [7]

    Lee, ” Theory and Application of the Quantum-Phase Distribution Functions ”, Phys

    H.W. Lee, ” Theory and Application of the Quantum-Phase Distribution Functions ”, Phys. Rep. 259 (1995) 147–211

  8. [8]

    Leonhardt, ” Measuring the Quantum State of Light ”, Cambridge University Press, Cambridge (1997)

    U. Leonhardt, ” Measuring the Quantum State of Light ”, Cambridge University Press, Cambridge (1997)

  9. [9]

    L¨ utkenhaus and S.M

    N. L¨ utkenhaus and S.M. Barnett, ”Nonclassical Effects in Phase Space ”, Phys. Rev. A 51 (1995) 3340-3342

  10. [10]

    Quantum Optics in Phase Space

    W.P. Schleich, “ Quantum Optics in Phase Space ”, Wiley-VCH, Berlin (2001)

  11. [11]

    Kenfack and K

    A. Kenfack and K. ˙Zyczkowski, ”Negativity of the Wigner function as an Indicator of Non-Classicality ”, J. Opt. B: Quantum Semiclass. Opt. 6 (2004) 396-404

  12. [12]

    Quantum State Estimation

    “ Quantum State Estimation ”, Eds. M. Paris and J. ˇReh´ aˇ cek, Lecture Notes in Physics 649, Springer, Science & Business Media, Berlin Heidelberg (2004)

  13. [13]

    Exploring the Quantum - Atoms, Cavities, and Photons

    S. Haroche and J.M. Raimond, “Exploring the Quantum - Atoms, Cavities, and Photons” (Oxford University Press, Oxford, 2006)

  14. [14]

    Gross, ” Hudson’s Theorem for Finite-Dimensional Quantum Systems ”, J

    D. Gross, ” Hudson’s Theorem for Finite-Dimensional Quantum Systems ”, J. Math. Phys. 47 (2006) 122107-1-25

  15. [15]

    ˇReh´ aˇ cek, Z

    J. ˇReh´ aˇ cek, Z. Bouchal, R.ˇCelechovsk´ y, Z. Hradil, and L.L. S´ anchez-Soto, ”Experimental Test of Uncertainty Relations for Quantum Mechanics on a Circle ”, Phys. Rev. A 77 (2008) 032110-1-13

  16. [16]

    Orbital Angular Momentum in Phase Space

    I. Rigas, L.L. S´ anchez-Soto, A.B. Klimov, J. ˇReh´ aˇ cek, and Z. Hradil , “Orbital Angular Momentum in Phase Space ”, Ann. Phys. 326 (2011) 426-439

  17. [17]

    Kastrup, ” Wigner Functions for the Pair Angle and Orbital Angular Momentum ”, Phys

    H.A. Kastrup, ” Wigner Functions for the Pair Angle and Orbital Angular Momentum ”, Phys. Rev. A 94 (2016) 062113-1-14 and ” Wigner Functions for the Pair Angle and Orbital Angular Momentum:Operators and Dynamics ”, ibid. 95 (2017) 052111-1-13

  18. [18]

    Tilma, M.J

    T. Tilma, M.J. Everitt, J.H. Samson, W.J. Munro, and K. Nemoto, ” Wigner Functions for Arbitrary Quantum Systems ”, Phys. Rev. Lett. 117 (2016) 180401-1-5

  19. [19]

    From Cavity to Circuit Quantum Electro- 16 dynamics

    S. Haroche, M. Brune, and J.M. Raimond, “ From Cavity to Circuit Quantum Electro- 16 dynamics ” , Nature Physics 16 (2020) 243-246

  20. [20]

    Wigner Functions and Coherent States for the Quantum Mechanics on a Circle

    K. Kowalski and K. Lawniczak, “Wigner Functions and Coherent States for the Quantum Mechanics on a Circle ”, J. Phys. A: Math. Theor. 54 (2021) 275302-1-23

  21. [21]

    Feynman, ” Simulating Physics With Computers ”, Int

    R.P. Feynman, ” Simulating Physics With Computers ”, Int. J. Theor. Phys. 21 (1982) 467-488

  22. [22]

    Yuen and J.H

    H.P. Yuen and J.H. Shapiro, ”Optical Communication with Two-Photon Coherent States - Part Ill: Quantum Measurements Realizable with Photoemissive Detectors ”, IEEE Trans. Inform. Theory IT 26 (1980) 78-92

  23. [23]

    Welsch, W

    D.-G. Welsch, W. Vogel, and T. Opatrn´ y, ” Homodyne Detection and Quantum State Reconstruction ”, in ” Progress in Optics ”, Vol. XXXIX, (1999) 63-211, Ed. E. Wolf, Elsevier Science & Technology, Amsterdam (1999)

  24. [24]

    Gottesman, A

    D. Gottesman, A. Kitaev, and J. Preskill, ” Encoding a Qubit in an Oscillator ”, Phys. Rev. A 64 (2001) 012310-1-21

  25. [25]

    On Quantum States for Angular Position and An- gular Momentum of Light

    B.-S. Skagerstam and P.K. Rekdal, “ On Quantum States for Angular Position and An- gular Momentum of Light ” , (arXiv:2312.16535v1 [quant-ph] 27 Dec 2023) and in J. Opt. 26 (2024) 095201-1-6

  26. [26]

    Uncer- tainty Principle for Angular Position and Angular Momentum

    S. Franke-Arnold, S.M. Barnett, E. Yao, J. Leach, J. Courtial, and M. Padgett, “ Uncer- tainty Principle for Angular Position and Angular Momentum ”, New J. Phys. 6 (2004) 103-1-8

  27. [27]

    Minimum Uncertainty States of Angular Momentum and Angular Position

    D.T. Pegg, S.M. Barnett, R. Zambrini, S. Franke-Arnold and M.J. Padgett, “ Minimum Uncertainty States of Angular Momentum and Angular Position”, New J. Phys. 7 (2005) 62-1-21

  28. [28]

    Orbital Angular Momentum of Light

    S.M. Barnett and R. Zambrini, “ Orbital Angular Momentum of Light ”, in “ Quantum Imaging ”, Ed. M.I. Kolobov, pp. 277-311, Springer, New York (2007)

  29. [29]

    Efficient Sorting of Orbital Angular Momentum States of Light

    G.C.G. Berkhout, M.P.J. Lavery, J. Courtial, M.W. Beijersbergen, and M.J. Padgett, “Efficient Sorting of Orbital Angular Momentum States of Light ”, Phys. Rev. Lett. 105 (2010) 153601-1-4

  30. [30]

    Measuring the Orbital Angular Momentum of a Single Photon

    J. Leach, M.J. Padgett, S.M. Barnett, S. Franke-Arnold, and J. Courtial, “ Measuring the Orbital Angular Momentum of a Single Photon ”, Phys. Rev. Lett. 88 (2002) 257901-1–4

  31. [31]

    Observation of the Vortex Structure of a Non-Integer Vortex Beam

    J. Leach, E. Yao and M.J. Padgett, “Observation of the Vortex Structure of a Non-Integer Vortex Beam ”, New J. Phys. 6 (2004) 71-1-8. 17

  32. [32]

    Optical Vortices Evolving From Helicoidal Integer and Fractional Phase Steps

    M.V. Berry, “ Optical Vortices Evolving From Helicoidal Integer and Fractional Phase Steps ”, J. Opt. A: Pure Appl. Opt. 6 (2004) 259-268

  33. [33]

    Experimental Demonstration of Fractional Orbital Angular Momentum En- tanglement of Two Photons

    S.S.R. Oemrawsingh, X. Ma, D. Voigt, A. Aiello, E.R. Eliel, G.W. ’t Hooft, and J.P. Woerdman, “Experimental Demonstration of Fractional Orbital Angular Momentum En- tanglement of Two Photons ”, Phys. Rev. Lett. 95 (2005) 240501-1–4

  34. [34]

    Fractional Optical Vortex Beam Induced Rotation of Particles

    S.H. Tao, X-C. Yuan, J. Lin, X. Peng, and H.B. Niu, “ Fractional Optical Vortex Beam Induced Rotation of Particles ”, Optics Express 13 (2005) 7726-7731

  35. [35]

    Observation of Quantum Entanglement Using Spatial Light Modulators

    E. Yao, S. Franke-Arnold, J. Courtial and M.J. Padgett, and S.M. Barnett, “Observation of Quantum Entanglement Using Spatial Light Modulators ”, Optics Express 14 (2006) 13089-13094

  36. [36]

    Uncertainty Relation Between Angle and Orbital Angular Momentum: Interference Effect in Electron Vortex Beams

    S. Tanimura, “ Uncertainty Relation Between Angle and Orbital Angular Momentum: Interference Effect in Electron Vortex Beams ”, Nanosystems: Phys. Chem. Math. 6 (2015) 205-212

  37. [37]

    Gradual Edge Enhancement in Spiral Phase Contrast Imaging With Fractional Vortex Filters

    J. Wang, W. Zhang, Q. Qi, S. Zheng, and L. Chen, “Gradual Edge Enhancement in Spiral Phase Contrast Imaging With Fractional Vortex Filters ”, Nature Scientific Reports 5 (2015) 1-6

  38. [38]

    There are Many Ways to Spin a Photon: Half-Quantization of a Total Optical Angular Momentum

    K.E. Ballantine, J.F. Donegan, and P.R. Eastham, “ There are Many Ways to Spin a Photon: Half-Quantization of a Total Optical Angular Momentum ”, Sci. Adv. 2 (2016) 1-7

  39. [39]

    Negative Optical Spin Torque Wrench of a Non-Diffracting Non-Paraxial Fractional Bessel Vortex Beam

    F.G. Mitri, “ Negative Optical Spin Torque Wrench of a Non-Diffracting Non-Paraxial Fractional Bessel Vortex Beam ”, J. Quantitative Spectroscopy and Radiative Transfer 182 (2016) 172-179

  40. [40]

    Arbitrarily Tunable Orbital Angular Momentum of Photons

    Y. Pan, X.Z. Gao, Z.C. Ren, X.L. Wang, C. Tu, Y. Li, and H.T. Wang, “ Arbitrarily Tunable Orbital Angular Momentum of Photons ”, Nature Scientific Reports 6 (2016) 1-8

  41. [41]

    Precision Measurement of Fractional Orbital Angular Momentum

    D. Deng, M. Lin, Y. Li, and H. Zhao, “ Precision Measurement of Fractional Orbital Angular Momentum ”, Phys. Rev. Applied 12 (2019) 014048–1–7

  42. [42]

    Quantifiable Example of Complementarity Relation Between Optical Or- bital Angular Momentum and Angular Position

    H.-C. Huang, “ Quantifiable Example of Complementarity Relation Between Optical Or- bital Angular Momentum and Angular Position ”, Opt. Commun. 446 (2019) 23-32

  43. [43]

    Bright Solid-State Sources for Single Photons with Orbital Angular Momentum

    B. Chen, Y. Wei, T. Zhao, S. Liu, R. Su, B. Yao, Y. Yu, J. Liu, and X. Wang ,“ Bright Solid-State Sources for Single Photons with Orbital Angular Momentum ”, Nature Nan- otech. 16 (2021) 302-307. 18

  44. [44]

    Production of Orbital Angular Momentum States of Optical Vortex Beams Using a Vortex Half-Wave Retarder With Double-Pass Configuration

    S. Deachapunya, S. Srisuphaphon, and S. Buathong ,“ Production of Orbital Angular Momentum States of Optical Vortex Beams Using a Vortex Half-Wave Retarder With Double-Pass Configuration ”, Nature Scientific Reports 12 (2022) 6061-1–7

  45. [45]

    Fractional Optical Angular Momentum and Multi-Defect-Mediated Mode Renormaliza- tion and Orientation Control in Photonic Crystal Microring Resonators

    M. Wang, F. Zhou, X. Lu, A. McClung, M. Davanco, V.A. Aksyuk, and K. Srinivasan ,“Fractional Optical Angular Momentum and Multi-Defect-Mediated Mode Renormaliza- tion and Orientation Control in Photonic Crystal Microring Resonators ”, Phys. Rev. Lett. 129 (2022) 186101-1–6

  46. [46]

    Fractional Topological Numbers at Photonic Edges and Corners

    C.P. Liang, Y. Liu, F.F. Li, S.W. Leung, Y. Poo, and J.H. Jiang, “ Fractional Topological Numbers at Photonic Edges and Corners ”, Phys. Rev. Appl. 20 (2023) 034028-1–10

  47. [47]

    The Convolution Transform

    D.V. Widder, “ The Convolution Transform ”, Bull. Amer. Math. Soc. 60 (1954) 444-456 and I.I. Hirschman and D.V. Widder, “ The Convolution Transform ”, Princeton University Press, Princeton (1955)

  48. [48]

    Density Operators and Quasiprobability Distributions

    K.E. Cahill and R.J. Glauber,“ Density Operators and Quasiprobability Distributions ”, Phys. Rev. 177 (1969) 1882-1902

  49. [49]

    Generalized Phase-Space Representation of Opera- tors

    J.R. Klauder and B.-S. Skagerstam,“ Generalized Phase-Space Representation of Opera- tors ”, J. Phys. A: Math. Theor. 40 (2007) 2093–2105

  50. [50]

    Fluctuating Magnetic Fields

    C. Itzykson, “ Fluctuating Magnetic Fields ”, Ref.TH.1703.CERN, 1973 and in Commun. Math. Phys. 36 (1974) 19-36

  51. [51]

    On Convergence and Growth of Partial Sums of Fourier Series

    L. Carleson, “ On Convergence and Growth of Partial Sums of Fourier Series ”, Acta Math. 116 (1966) 135-157 and reviewed by C. Demeter, in “ A Guide to Carleson’s Theorem ”, Rocky Mountain J. of Math. 45 (2015) 169-212

  52. [52]

    Introduction to the Theory of Fourier’s Series and Integrals

    H.S. Carslaw, “ Introduction to the Theory of Fourier’s Series and Integrals ”, Third Edition , Dover Publ. Inc. (N.Y., 1930) and Chapter 5 in N. Young, “ An Introduction to Hilbert Space ”, Cambridge University Press, Cambridge (1988)

  53. [53]

    From “Dirac Combs

    B.G. Giraud and R. Peschanski, “ From “Dirac Combs” to Fourier-Positivity ”, Acta Phys. Pol. B 47 (2016) 1075-1100

  54. [54]

    On the Functions Which are Represented by the Expansions of the Interpolation Theory

    E.T. Whittaker, “ On the Functions Which are Represented by the Expansions of the Interpolation Theory ”, Proc. Roy. Soc. Edinburgh 35 (1915) 181-194

  55. [55]

    Certain Topics in Telegraph Transmission Theory

    H. Nyquist, “ Certain Topics in Telegraph Transmission Theory ”, Trans. Amer. Inst. Elec. Eng. 47 (1928) 617-644

  56. [56]

    A Mathematical Theory of Communication

    C.E. Shannon, “ A Mathematical Theory of Communication ”, Bell System Tech. J. 27 (1948) 379-423, 623-656; C.E. Shannon and W. Weaver, “ The Mathematical Theory of 19 Communication ”, The University of Illinois Press, Urbana (1964)

  57. [57]

    Whittaker’s Cardinal Function in Retro- spect

    J. McNamee, F. Stenger and E. L. Whitney, “ Whittaker’s Cardinal Function in Retro- spect ”, Mathematics of Computation 25 (1971) 141-154

  58. [58]

    Numerical Methods Based on Whittaker Cardinal, or Sinc Functions

    F. Stenger, “ Numerical Methods Based on Whittaker Cardinal, or Sinc Functions ”, SIAM Review 23 (1981) 165-224

  59. [59]

    The Function sin x x

    W.B. Gearhart and H.S. Shultz, “The Function sin x x ”, The College Mathematics Journal 21 (1990) 90-99

  60. [60]

    Quantum Versus Classical Phase in Optical Systems

    G.S. Agarwal, “ Quantum Versus Classical Phase in Optical Systems ”, in Proceedings of the International Symposium, “Coherent States - Past, Present, and Future ”, Eds. D.H. Feng, J.R. Klauder, and M.R. Strayer, World Scientific, Singapore (1994). 20