pith. machine review for the scientific record. sign in

arxiv: 2603.27041 · v1 · submitted 2026-03-27 · 🪐 quant-ph · hep-ph· hep-th· physics.hist-ph

Recognition: 2 theorem links

· Lean Theorem

Derivation of the Schrodinger equation from fundamental principles

Authors on Pith no claims yet

Pith reviewed 2026-05-14 22:24 UTC · model grok-4.3

classification 🪐 quant-ph hep-phhep-thphysics.hist-ph
keywords Schrödinger equationprobability amplitudede Broglie relationswave functionquantum mechanics derivationenergy momentum relationsfundamental principles
0
0 comments X

The pith

The Schrödinger equation follows from assuming the wave function is a probability amplitude and applying de Broglie relations E=ħω, p=ħk.

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

The paper derives the Schrödinger equation by starting from the interpretation of the wave function as the probability amplitude for finding a particle at position r at time t. It combines this with the de Broglie relations that connect particle energy to the frequency of the associated wave and momentum to its wave vector. The derivation produces both the time-dependent and time-independent forms of the equation without relying on heuristic guesses. This approach matters to a reader because it reduces the foundational equation of quantum mechanics to a small set of explicit physical premises about probability and waves. If the steps hold, the equation becomes a logical consequence rather than an inspired postulate.

Core claim

Starting from the wave function ψ(r,t) as the probability amplitude and the relations E = ħω and p = ħk for the probability wave, the standard time-dependent Schrödinger equation i ħ ∂ψ/∂t = −(ħ²/2m) ∇² ψ + V ψ is obtained directly, along with its stationary-state version for definite energy.

What carries the argument

The probability-amplitude interpretation of the wave function combined with the de Broglie relations E=ħω and p=ħk that link particle energy and momentum to wave frequency and wave vector.

If this is right

  • The time-dependent Schrödinger equation i ħ ∂ψ/∂t = H ψ follows at once from the premises.
  • Energy eigenstates obey the time-independent equation H ψ = E ψ.
  • Superposition of amplitudes produces interference without extra assumptions.
  • The classical limit emerges when wave packets follow trajectories consistent with Newtonian mechanics.

Where Pith is reading between the lines

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

  • The same premises could be applied to derive wave equations for other particles by changing the dispersion relation.
  • The derivation isolates the probabilistic and wave-like inputs, so relaxing either premise would require a different dynamical law.
  • It raises the question whether linearity of the wave equation is forced by the amplitude-plus-de-Broglie starting point or added separately.
  • Similar logic might connect to path-integral formulations that also begin from probability amplitudes.

Load-bearing premise

The wave function must be a probability amplitude and the de Broglie relations must apply to that wave independently of the Schrödinger equation itself.

What would settle it

An experiment that measures a particle's position probability evolving in a manner inconsistent with the Schrödinger equation while its associated waves still satisfy E=ħω and p=ħk would disprove the derivation.

read the original abstract

Schrodinger path to the quantum mechanical wave equation was heuristic and guided more by physical intuition than formal deduction. Here we derive the Schrodinger equation for the particle wave function, assuming that it has a meaning of the probability amplitude to find the particle at time t at point r and the relations E=hw, p=hk expressing particle energy and momentum in terms of the frequency and wave vector of the associated probability wave.

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 / 0 minor

Summary. The manuscript claims to derive the time-dependent Schrödinger equation for a particle wave function ψ(r,t) by assuming that ψ represents the probability amplitude to find the particle at position r at time t and that the associated wave obeys the de Broglie relations E = ħω and p = ħk.

Significance. If the steps are shown to be non-circular and the assumptions are independently justified, the result could clarify the logical structure underlying the Schrödinger equation and address its original heuristic character. The absence of any derivation of the probability interpretation or dispersion relations from non-quantum starting points, however, limits the independence of the claimed derivation.

major comments (2)
  1. [Abstract] Abstract: The derivation is introduced by assuming both the probability-amplitude interpretation of ψ(r,t) and the relations E=ħω, p=ħk. These are the standard postulates that directly encode the replacements iħ∂/∂t → E and −iħ∇ → p; without an independent derivation of either premise from classical mechanics, relativity, or other non-quantum principles, the argument reduces to a restatement of the input relations rather than a deduction from more fundamental principles, as the title asserts.
  2. [Abstract] Abstract: No explicit algebraic steps are supplied in the abstract (and the manuscript provides no section deriving the assumptions). It is therefore impossible to verify whether the algebra reaches iħ∂ψ/∂t = −(ħ²/2m)∇²ψ + Vψ without inserting the operator identifications by hand or using post-hoc identifications that presuppose the target equation.

Simulated Author's Rebuttal

2 responses · 1 unresolved

We thank the referee for the detailed and constructive report. The comments highlight important points about the scope and presentation of our derivation. We address each major comment below and will revise the manuscript accordingly to improve clarity while preserving the intended logical structure.

read point-by-point responses
  1. Referee: [Abstract] Abstract: The derivation is introduced by assuming both the probability-amplitude interpretation of ψ(r,t) and the relations E=ħω, p=ħk. These are the standard postulates that directly encode the replacements iħ∂/∂t → E and −iħ∇ → p; without an independent derivation of either premise from classical mechanics, relativity, or other non-quantum principles, the argument reduces to a restatement of the input relations rather than a deduction from more fundamental principles, as the title asserts.

    Authors: We agree that the starting assumptions are the probability-amplitude interpretation and the de Broglie relations E=ħω, p=ħk. These are taken as the fundamental principles for this derivation, consistent with the standard formulation of quantum mechanics for a single particle. The manuscript's goal is to make the algebraic steps explicit: assume a wave form satisfying those relations, substitute the operator identifications that follow directly from them, and arrive at the differential equation. We do not claim an independent derivation of the postulates themselves from classical or relativistic mechanics. To avoid any implication that the title promises a derivation from non-quantum principles, we will revise the abstract and title to state clearly that the derivation proceeds from the stated quantum postulates. revision: yes

  2. Referee: [Abstract] Abstract: No explicit algebraic steps are supplied in the abstract (and the manuscript provides no section deriving the assumptions). It is therefore impossible to verify whether the algebra reaches iħ∂ψ/∂t = −(ħ²/2m)∇²ψ + Vψ without inserting the operator identifications by hand or using post-hoc identifications that presuppose the target equation.

    Authors: We accept that the abstract as written does not display the intermediate algebraic steps. In the revised manuscript we will expand the abstract to include a concise outline of the key steps: (i) posit a plane-wave solution ψ(r,t) ∝ exp[i(k·r − ωt)] consistent with the probability-amplitude interpretation, (ii) apply the de Broglie relations to obtain E = ħω and p = ħk, (iii) replace E and p by the corresponding differential operators acting on ψ, and (iv) insert the non-relativistic energy-momentum relation E = p²/2m + V to recover the Schrödinger equation. The body of the paper already contains the full derivation; the abstract revision will make the logic verifiable at a glance. revision: yes

standing simulated objections not resolved
  • Independent derivation of the probability-amplitude interpretation and the de Broglie dispersion relations from purely non-quantum starting points is not provided, as this lies outside the scope of the present work.

Circularity Check

1 steps flagged

Derivation assumes probability-amplitude interpretation and de Broglie relations E=ħω, p=ħk that already encode the Schrödinger equation

specific steps
  1. self definitional [Abstract]
    "Here we derive the Schrodinger equation for the particle wave function, assuming that it has a meaning of the probability amplitude to find the particle at time t at point r and the relations E=hw, p=hk expressing particle energy and momentum in terms of the frequency and wave vector of the associated probability wave."

    The target equation is the unique linear PDE whose plane-wave solutions satisfy precisely E=ħω and p=ħk with ψ as the amplitude. Assuming these relations therefore forces the differential form of the Schrödinger equation by direct substitution; the derivation is definitionally equivalent to its premises.

full rationale

The paper states it derives the Schrödinger equation by assuming the wave function is the probability amplitude and that the associated wave obeys E=ħω, p=ħk. These premises are the standard postulates that directly yield the operator replacements iħ∂/∂t → E and −iħ∇ → p. Substituting a plane-wave ansatz under exactly these relations recovers the Schrödinger equation by algebraic identity, so the claimed derivation reduces to restating its inputs. No independent derivation of the probability interpretation or dispersion relation from non-quantum principles is indicated.

Axiom & Free-Parameter Ledger

0 free parameters · 2 axioms · 0 invented entities

The central claim rests entirely on two domain assumptions that are standard in quantum mechanics and are not independently derived or tested in the abstract.

axioms (2)
  • domain assumption The wave function ψ(r,t) is the probability amplitude for finding the particle at position r at time t
    Explicitly stated as the starting assumption in the abstract.
  • domain assumption Particle energy and momentum are related to frequency and wave vector by E = ħω and p = ħk
    Explicitly stated as the second assumption in the abstract.

pith-pipeline@v0.9.0 · 5363 in / 1456 out tokens · 72398 ms · 2026-05-14T22:24:56.408906+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

75 extracted references · 75 canonical work pages

  1. [1]

    Kelvin, L. I. Nineteenth century clouds over the dynamical theory of heat and light. The London, Edinburgh, and Dublin Philosophical Magazine and Journal of Science 1901, 2, 1–40, doi:10.1080/14786440109462664

  2. [2]

    Über eine Verbesserung der Wienschen Spektralgleichung

    Planck, M. Über eine Verbesserung der Wienschen Spektralgleichung. In Von Kirchhoff bis Planck: Theorie der Wärmestrahlung in historisch-kritischer Darstellung, Schöpf, H.-G., Ed.; Vieweg+Teubner Verlag: Wiesbaden, 1978; pp. 175–178. https://link.springer.com/chapter/10.1007/978-3-663-13885-3_15

  3. [3]

    Ueber das Gesetz der Energieverteilung im Normalspectrum

    Planck, M. Ueber das Gesetz der Energieverteilung im Normalspectrum. Annalen der Physik 1901, 309, 553– 563, doi:https://doi.org/10.1002/andp.19013090310

  4. [4]

    Max Planck: the reluctant revolutionary

    Kragh, H. Max Planck: the reluctant revolutionary. Physics World 2000, 13, 31, doi:10.1088/2058- 7058/13/12/34

  5. [5]

    Ueber einen Einfluss des ultravioletten Lichtes auf die electrische Entladung

    Hertz, H. Ueber einen Einfluss des ultravioletten Lichtes auf die electrische Entladung. Annalen der Physik 1887, 267, 983–1000, doi:https://doi.org/10.1002/andp.18872670827

  6. [6]

    Über einen die Erzeugung und Verwandlung des Lichtes betreffenden heuristischen Gesichtspunkt

    Einstein, A. Über einen die Erzeugung und Verwandlung des Lichtes betreffenden heuristischen Gesichtspunkt. Annalen der Physik 1905, 322, 132–148, doi:https://doi.org/10.1002/andp.19053220607

  7. [7]

    A Direct Determination of "h."

    Millikan, R.A. A Direct Determination of "h.". Physical Review 1914, 4, 73–75, doi:10.1103/PhysRev.4.73.2

  8. [8]

    A Quantum Theory of the Scattering of X-rays by Light Elements

    Compton, A.H. A Quantum Theory of the Scattering of X-rays by Light Elements. Physical Review 1923, 21, 483–502, doi:10.1103/PhysRev.21.483

  9. [9]

    Bohr, N. I. On the constitution of atoms and molecules. The London, Edinburgh, and Dublin Philosophical Magazine and Journal of Science 1913, 26, 1–25, doi:10.1080/14786441308634955

  10. [10]

    The origin of the postulates in the Bohr model of the hydrogen atom

    Pinke, D.D.; Ősz, K.; Lente, G. The origin of the postulates in the Bohr model of the hydrogen atom. ChemTexts 2025, 11, 11, doi:10.1007/s40828-025-00208-4

  11. [11]

    Bohr, N. LXXIII. On the constitution of atoms and molecules. The London, Edinburgh, and Dublin Philosophical Magazine and Journal of Science 1913, 26, 857–875, doi:10.1080/14786441308635031

  12. [12]

    Recherches sur la théorie des Quanta

    de Broglie, L. Recherches sur la théorie des Quanta. Ann. Phys., vol. 2, pp. 22–128, 1925

  13. [13]

    Schrödinger's route to wave mechanics

    Wessels, L. Schrödinger's route to wave mechanics. Studies in History and Philosophy of Science Part A 1979, 10, 311–340, doi:https://doi.org/10.1016/0039-3681(79)90018-9

  14. [14]

    Why Was It Schrödinger Who Developed de Broglie's Ideas? Historical Studies in the Physical Sciences 1969, 1, 291–314, doi:10.2307/27757299

    Raman, V.V.; Forman, P. Why Was It Schrödinger Who Developed de Broglie's Ideas? Historical Studies in the Physical Sciences 1969, 1, 291–314, doi:10.2307/27757299

  15. [15]

    Three Millennia of Atoms and Molecules

    Ruedenberg, K.; Schwarz, W.H.E. Three Millennia of Atoms and Molecules. In Pioneers of Quantum Chemistry; ACS Symposium Series; American Chemical Society: 2013; Volume 1122, pp. 1–45

  16. [16]

    Square root of minus one, complex phases and Erwin Schrödinger

    Yang, C.N. Square root of minus one, complex phases and Erwin Schrödinger. In Schrödinger: Centenary Celebration of a Polymath, Kilmister, C.W., Ed.; Cambridge University Press: Cambridge, 1987; pp. 53–64

  17. [17]

    Plancks Gesetz und Lichtquantenhypothese.Zeitschrift für Physik, 26(1): 178–181, 1924

    Bose. Plancks Gesetz und Lichtquantenhypothese. Zeitschrift für Physik 1924, 26, 178–181, doi:10.1007/BF01327326

  18. [18]

    Heisenberg and the early days of quantum mechanics

    Bloch, F. Heisenberg and the early days of quantum mechanics. Physics Today 1976, 29, 23–27, doi:10.1063/1.3024633

  19. [19]

    Quantisierung als Eigenwertproblem

    Schrödinger, E. Quantisierung als Eigenwertproblem. Annalen der Physik 1926, 384, 361–376, doi:https://doi.org/10.1002/andp.19263840404

  20. [20]

    Quantisierung als Eigenwertproblem

    Schrödinger, E. Quantisierung als Eigenwertproblem. Annalen der Physik 1926, 384, 489–527, doi:https://doi.org/10.1002/andp.19263840602

  21. [21]

    Quantisierung als Eigenwertproblem

    Schrödinger, E. Quantisierung als Eigenwertproblem. Annalen der Physik 1926, 386, 109–139, doi:https://doi.org/10.1002/andp.19263861802

  22. [22]

    Über das Verhältnis der Heisenberg-Born-Jordanschen Quantenmechanik zu der meinen

    Schrödinger, E. Über das Verhältnis der Heisenberg-Born-Jordanschen Quantenmechanik zu der meinen. Annalen der Physik 1926, 384, 734–756, doi:https://doi.org/10.1002/andp.19263840804

  23. [23]

    Zur Quantenmechanik der Stoßvorgänge

    Born, M. Zur Quantenmechanik der Stoßvorgänge. Zeitschrift für Physik 1926, 37, 863–867, doi:10.1007/BF01397477

  24. [24]

    The quantum theory of the electron

    Dirac, P.A.M. The quantum theory of the electron. Proceedings of the Royal Society of London. Series A, Containing Papers of a Mathematical and Physical Character 1928, 117, 610–624, doi:10.1098/rspa.1928.0023

  25. [25]

    The quantum theory of the emission and absorption of radiation

    Dirac, P.A.M. The quantum theory of the emission and absorption of radiation. Proceedings of the Royal Society of London. Series A, Containing Papers of a Mathematical and Physical Character 1927, 114, 243–265, doi:10.1098/rspa.1927.0039. 13

  26. [26]

    One Hundred Years of Quantum Physics

    Kleppner, D.; Jackiw, R. One Hundred Years of Quantum Physics. Science 2000, 289, 893–898, doi:10.1126/science.289.5481.893

  27. [27]

    Quantentheorie in hydrodynamischer Form

    Madelung, E. Quantentheorie in hydrodynamischer Form. Zeitschrift für Physik 1927, 40, 322–326, doi:10.1007/BF01400372

  28. [28]

    Densities, density-functionals and electron fluids

    Ghosh, S.K.; Deb, B.M. Densities, density-functionals and electron fluids. Physics Reports 1982, 92, 1–44, doi:https://doi.org/10.1016/0370-1573(82)90134-X

  29. [29]

    The physical interpretation of wave mechanics

    Jánossy, L. The physical interpretation of wave mechanics. I. Foundations of Physics 1973, 3, 185–202, doi:10.1007/BF00708438

  30. [30]

    The hydrodynamical model of wave mechanics I

    Jánossy, L.; Ziegler, M. The hydrodynamical model of wave mechanics I. Acta Physica Academiae Scientiarum Hungaricae 1963, 16, 37–48, doi:10.1007/BF03157004

  31. [31]

    Single-particle Schrödinger fluid

    Kan, K.-K.; Griffin, J.J. Single-particle Schrödinger fluid. I. Formulation. Physical Review C 1977, 15, 1126– 1151, doi:10.1103/PhysRevC.15.1126

  32. [32]

    Interpretation of the hydrodynamical formalism of quantum mechanics

    Sonego, S. Interpretation of the hydrodynamical formalism of quantum mechanics. Foundations of Physics 1991, 21, 1135–1181, doi:10.1007/BF00734264

  33. [33]

    On the Formulation of Quantum Mechanics associated with Classical Pictures

    Takabayasi, T. On the Formulation of Quantum Mechanics associated with Classical Pictures. Progress of Theoretical Physics 1952, 8, 143–182, doi:10.1143/ptp/8.2.143

  34. [34]

    Remarks on the Formulation of Quantum Mechanics with Classical Pictures and on Relations between Linear Scalar Fields and Hydrodynamical Fields

    Takabayasi, T. Remarks on the Formulation of Quantum Mechanics with Classical Pictures and on Relations between Linear Scalar Fields and Hydrodynamical Fields. Progress of Theoretical Physics 1953, 9, 187–222, doi:10.1143/ptp/9.3.187

  35. [35]

    Hydrodynamic Model of Quantum Mechanics

    Wilhelm, H.E. Hydrodynamic Model of Quantum Mechanics. Physical Review D 1970, 1, 2278–2285, doi:10.1103/PhysRevD.1.2278

  36. [36]

    On the Schrödinger equation in fluid-dynamical form

    Wong, C.Y. On the Schrödinger equation in fluid-dynamical form. Journal of Mathematical Physics 1976, 17, 1008–1010, doi:10.1063/1.523008

  37. [37]

    The lagrangian approach to stochastic variational principles on curved manifolds

    Aldrovandi, E.; Dohrn, D.; Guerra, F. The lagrangian approach to stochastic variational principles on curved manifolds. Acta Applicandae Mathematica 1992, 26, 219–236, doi:10.1007/BF00047204

  38. [38]

    Derivation of the Schrödinger Equation from a Stochastic Theory

    Baublitz, M., Jr. Derivation of the Schrödinger Equation from a Stochastic Theory. Progress of Theoretical Physics 1988, 80, 232–244, doi:10.1143/ptp.80.232

  39. [39]

    Mathematical and physical aspects of stochastic mechanics; Springer: 1987

    Blanchard, P.; Combe, P.; Zheng, W. Mathematical and physical aspects of stochastic mechanics; Springer: 1987

  40. [40]

    A generalization of the Fényes — Nelson stochastic model of quantum mechanics

    Davidson, M. A generalization of the Fényes — Nelson stochastic model of quantum mechanics. Letters in Mathematical Physics 1979, 3, 271–277, doi:10.1007/BF01821846

  41. [41]

    On the stochastic Lagrangian and a new derivation of the Schrodinger equation

    Davies, I.M. On the stochastic Lagrangian and a new derivation of the Schrodinger equation. Journal of Physics A: Mathematical and General 1989, 22, 3199, doi:10.1088/0305-4470/22/16/010

  42. [42]

    A new formulation of stochastic theory and quantum mechanics

    De la Pena Auerbach, L. A new formulation of stochastic theory and quantum mechanics. Phys. Lett. A. 1968, 27, 594-595, https://doi.org/10.1016/0375-9601(68)90068-6

  43. [43]

    New Formulation of Stochastic Theory and Quantum Mechanics

    De La Peña-Auerbach, L. New Formulation of Stochastic Theory and Quantum Mechanics. J. Math. Phys. 1969, 10, 1620–1630, https://doi.org/10.1063/1.1665009

  44. [44]

    Eine wahrscheinlichkeitstheoretische Begründung und Interpretation der Quantenmechanik

    Fényes, I. Eine wahrscheinlichkeitstheoretische Begründung und Interpretation der Quantenmechanik. Zeitschrift für Physik 1952, 132, 81–106, doi:10.1007/BF01338578

  45. [45]

    Derivation of the quantum potential from realistic Brownian particle motions

    Garbaczewski, P. Derivation of the quantum potential from realistic Brownian particle motions. Physics Letters A 1992, 162, 129–136, doi:https://doi.org/10.1016/0375-9601(92)90988-X

  46. [46]

    Quantum dynamics from the Brownian recoil principle

    Garbaczewski, P.; Vigier, J.-P. Quantum dynamics from the Brownian recoil principle. Physical Review A 1992, 46, 4634–4638, doi:10.1103/PhysRevA.46.4634

  47. [47]

    Stochastic mechanics and quantum theory

    Goldstein, S. Stochastic mechanics and quantum theory. Journal of Statistical Physics 1987, 47, 645–667, doi:10.1007/BF01206150

  48. [48]

    Quantization of dynamical systems and stochastic control theory

    Guerra, F.; Morato, L.M. Quantization of dynamical systems and stochastic control theory. Physical Review D 1983, 27, 1774–1786, doi:10.1103/PhysRevD.27.1774

  49. [49]

    Stochastic quantization of a dissipative dynamical system and its hydrodynamical interpretation

    Hajra, K. Stochastic quantization of a dissipative dynamical system and its hydrodynamical interpretation. Journal of Mathematical Physics 1991, 32, 1505–1509, doi:10.1063/1.529257

  50. [50]

    Theory of Hidden Variables

    Kershaw, D. Theory of Hidden Variables. Physical Review 1964, 136, B1850–B1856, doi:10.1103/PhysRev.136.B1850

  51. [51]

    The density manifold and configuration space quantization

    Lafferty, J.D. The density manifold and configuration space quantization. Trans. Am. Math. Soc. 1988, 305, 699, ams.org/journals/tran/1988-305-02/S0002-9947-1988-0924776-9/S0002-9947-1988-0924776-9.pdf 14

  52. [52]

    Variational principles for conservative and dissipative diffusions

    Marra, R. Variational principles for conservative and dissipative diffusions. Physical Review D 1987, 36, 1724– 1730, doi:10.1103/PhysRevD.36.1724

  53. [53]

    Path-wise stochastic calculus of variations with the classical action and quantum systems

    Morato, L.M. Path-wise stochastic calculus of variations with the classical action and quantum systems. Phys. Rev. D 1985, 31, 1982–1987, DOI: https://doi.org/10.1103/PhysRevD.31.1982

  54. [54]

    Nonlocal Quantum Field Theory and Stochastic Quantum Mechanics

    Namsrai, K. Nonlocal Quantum Field Theory and Stochastic Quantum Mechanics. Emergence 2017

  55. [55]

    An Overview of the application of the Langevin equation to the description of Brownian and quantum motions of a particle

    Namsrai, K.; Hulree, Y.; Njamtseren, N. An Overview of the application of the Langevin equation to the description of Brownian and quantum motions of a particle. Int. J. Mod. Phys. A 1992, 07, 2661–2677, https://doi.org/10.1142/s0217751x92001198

  56. [56]

    Derivation of the Schrödinger Equation from Newtonian Mechanics

    Nelson, E. Derivation of the Schrödinger Equation from Newtonian Mechanics. Physical Review 1966, 150, 1079–1085, doi:10.1103/PhysRev.150.1079

  57. [57]

    Dynamical Theories of Brownian Motion; Princeton University Press: 1967

    Nelson, E. Dynamical Theories of Brownian Motion; Princeton University Press: 1967

  58. [58]

    Quantum Fluctuations; Princeton University Press: 1985

    Nelson, E. Quantum Fluctuations; Princeton University Press: 1985

  59. [59]

    Derivation of Feynman's path integral theory based on stochastic mechanics

    Wang, M.S. Derivation of Feynman's path integral theory based on stochastic mechanics. Physics Letters A 1989, 137, 437–439, doi:https://doi.org/10.1016/0375-9601(89)90220-X

  60. [60]

    Stochastic calculus of variations

    Yasue, K. Stochastic calculus of variations. Journal of Functional Analysis 1981, 41, 327–340, doi:https://doi.org/10.1016/0022-1236(81)90079-3

  61. [61]

    A Suggested Interpretation of the Quantum Theory in Terms of "Hidden" Variables

    Bohm, D. A Suggested Interpretation of the Quantum Theory in Terms of "Hidden" Variables. I. Physical Review 1952, 85, 166–179, doi:10.1103/PhysRev.85.166

  62. [62]

    A Suggested Interpretation of the Quantum Theory in Terms of "Hidden" Variables

    Bohm, D. A Suggested Interpretation of the Quantum Theory in Terms of "Hidden" Variables. II. Physical Review 1952, 85, 180–193, doi:10.1103/PhysRev.85.180

  63. [63]

    Une Tentative d'Interpretation Causale et Non Linéaire de la Mécanique Ondulatoire (la Théorie de la Double Solution); Gauthier Villars: Paris, 1956

    de Broglie, L. Une Tentative d'Interpretation Causale et Non Linéaire de la Mécanique Ondulatoire (la Théorie de la Double Solution); Gauthier Villars: Paris, 1956. https://fondationlouisdebroglie.org/LDB-oeuvres/LDB- oeuvres-b/LdB56_Ch1.pdf

  64. [64]

    Étude critique des bases de l'interprétation actuelle de la mécanique ondulatoire; Gauthier-Villars: Paris, 1963

    de Broglie, L. Étude critique des bases de l'interprétation actuelle de la mécanique ondulatoire; Gauthier-Villars: Paris, 1963

  65. [65]

    Schrödinger equation revisited

    Schleich, W.P.; Greenberger, D.M.; Kobe, D.H.; Scully, M.O. Schrödinger equation revisited. Proceedings of the National Academy of Sciences 2013, 110, 5374–5379, doi:10.1073/pnas.1302475110

  66. [66]

    A simple derivation of the Schroedinger equation from the theory of Markoff processes

    De La Peña-Auerbach, L. A simple derivation of the Schroedinger equation from the theory of Markoff processes. Phys. Lett. A 1967, 24, 603, https://doi.org/10.1016/0375-9601(67)90639-1

  67. [67]

    Foundations of quantum mechanics (II): equilibrium, Bohr–Sommerfeld rules and duality

    Olavo, L.S.F. Foundations of quantum mechanics (II): equilibrium, Bohr–Sommerfeld rules and duality. Physica A: Statistical Mechanics and its Applications 1999, 271, 260, https://doi.org/10.1016/S0378-4371(99)00216- 2

  68. [68]

    Derivation of Schriidinger's Equation from Stochastic Electrodynamics

    Surdin, M. Derivation of Schriidinger's Equation from Stochastic Electrodynamics. International Journal of Theoretical Physics 1971, 4, 117-123, https://link.springer.com/article/10.1007/BF00670387

  69. [69]

    The time dependent Schrödinger equation revisited I: Quantum field and classical Hamilton- Jacobi routes to Schrödinger's wave equation

    Scully, M.O. The time dependent Schrödinger equation revisited I: Quantum field and classical Hamilton- Jacobi routes to Schrödinger's wave equation. Journal of Physics: Conference Series 2008, 99, 012019

  70. [70]

    The time-dependent Schrödinger equation revisited: quantum optical and classical Maxwell routes to Schrödinger’s wave equation

    Scully, M.O. The time-dependent Schrödinger equation revisited: quantum optical and classical Maxwell routes to Schrödinger’s wave equation. Lect. Notes Phys. 2009, 789, 15–24

  71. [71]

    Spacetime approach to nonrelativistic quantum mechanics

    Feynmann, R.P. Spacetime approach to nonrelativistic quantum mechanics. Rev. Mod. Phys. 1948, 20, 367, https://doi.org/10.1103/revmodphys.20.367

  72. [72]

    Feynman's derivation of Schrödinger equation

    Derbes, D. Feynman's derivation of Schrödinger equation. Am. J. Phys. 1996, 64, 881, https://doi.org/10.1119/1.18114

  73. [73]

    Vector theory of gravity: Universe without black holes and solution of dark energy problem

    Svidzinsky, A.A. Vector theory of gravity: Universe without black holes and solution of dark energy problem. Physica Scripta 2017, 92, 125001, https://iopscience.iop.org/article/10.1088/1402-4896/aa93a8

  74. [74]

    Inner structure of leptons, nature of dark matter, and non-Higgs origin of elementary particle masses

    Svidzinsky, A.A. Inner structure of leptons, nature of dark matter, and non-Higgs origin of elementary particle masses. Quantum Stud.: Math. Found. 2026, 13, 17, https://doi.org/10.1007/s40509-026-00387-w

  75. [75]

    GW170817 event rules out general relativity in favor of vector gravity

    Svidzinsky, A.A.; Hilborn, R.C. GW170817 event rules out general relativity in favor of vector gravity. Eur. Phys. J. Spec. Top. 2021, 230, 1149–1166, https://doi.org/10.1140/epjs/s11734-021-00080-6