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Derivation of the Schrodinger equation from fundamental principles

Published 27 Mar 2026 in quant-ph, hep-ph, and physics.hist-ph | (2603.27041v1)

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.

Summary

  • The paper demonstrates that the Schrödinger equation can be rigorously derived from foundational probabilistic and symmetry principles rather than postulated heuristically.
  • It employs a Fourier basis and the continuity equation to connect classical kinetic energy with quantum corrections via the quantum potential.
  • Implications extend to hydrodynamic formulations, quantum information theory, and unified models in particle physics and cosmology.

Formal Derivation of the Schrödinger Equation from Fundamental Principles

Historical and Conceptual Foundations

The paper meticulously traces the development of quantum mechanics, emphasizing its transition from heuristic models to formal theoretical structure. Early quantum theory, originating with Planck’s quantization of energy and Einstein’s introduction of photons, established the discrete nature of energy and the duality of light. Bohr’s model addressed atomic stability and spectral lines by postulating stationary states, but its lack of rigorous justification and failure to predict additional properties (such as ground-state angular momentum in hydrogen) revealed the necessity for deeper principles.

The wave-particle duality was further codified through de Broglie’s hypothesis associating matter waves with particles, constituting a pivotal conceptual bridge. Schrödinger’s formulation of wave mechanics, inspired directly by de Broglie and Einstein, relied heavily on mathematical analogy and variational principles but was initially lacking rigorous derivational justification of its wave equation from first principles.

Born’s probabilistic interpretation and the equivalence with matrix mechanics, provided by Schrödinger and contemporaries, solidified the foundations of quantum mechanics. Subsequent developments by Dirac, including the relativistic wave equation and quantum field theory, integrated quantum concepts into broader physical frameworks.

Stepwise Derivation of the Schrödinger Equation

The authors present a derivation that begins with the probabilistic postulate: the wave function Y(t,r)Y(t, r) serves as the probability amplitude for detecting the particle at position rr and time tt. They adopt the Planck–de Broglie relations, E=hωE = h\omega and p=hkp = h k, relating particle energy and momentum to the frequency and wave vector of the associated wave.

The formalism proceeds by expressing the wave function in a Fourier basis, which enables calculation of expectation values for momentum and kinetic energy. These quantities are shown to depend on the phase of the wave function, with the kinetic energy expression containing an additional term—a quantum potential—absent in the classical formulation. This quantum potential, also known as the Bohm term, is nonlocal and can be negative, accounting for phenomena such as tunneling.

The derivation employs the continuity equation to ensure conservation of probability and identifies the corresponding probability current. Using these relationships, the authors establish a quantum analog of the Hamilton–Jacobi equation. Specifically, the kinetic and potential energies are expressed in terms of the wave function and its derivatives, reproducing the classical energy relationship but incorporating quantum corrections.

Under the constraint that the governing equation obeys linear superposition—an axiom of quantum mechanics—the derivation reduces to a unique form for the potential which must coincide with the classical potential energy in the limit of fast-moving particles. The resulting equation is the familiar time-dependent Schrödinger equation:

ihYt=h22M2Y+V(t,r)Yi h \frac{\partial Y}{\partial t} = -\frac{h^2}{2M} \nabla^2 Y + V(t, r) Y

where YY is a complex-valued function, MM is the mass, and V(t,r)V(t, r) is the external potential. The Hamiltonian operator is shown to be Hermitian, guaranteeing unitary evolution and real energy eigenvalues.

Implications: Hydrodynamics, Quantum Information, and Interpretations

The hydrodynamic formulation, introduced by Madelung, is highlighted: writing Y=YeiSY = |Y| e^{iS} recovers a quantum Hamilton–Jacobi equation for the action rr0 and a continuity equation for rr1. This connects quantum mechanics to fluid dynamics, stochastic mechanics, and hidden-variable theories, and underpins various classical interpretations.

The quantum potential’s connection to Fisher information elucidates the informational content of quantum states and its role in quantum coherence and localization phenomena. The authors note that for macroscopic systems or high-energy regimes, the quantum corrections are negligible and the classical Hamilton–Jacobi equation is recovered, emphasizing the robustness of the quantum-classical correspondence.

Alternative Derivations and Symmetry Protocol

The paper surveys alternative derivations rooted in stochastic mechanics, statistical theory, Markov processes, Liouville equation, and path integrals, further establishing the Schrödinger equation as a consequence of deeper mathematical structure. The “symmetry protocol” is discussed as a guiding principle, analogous to gauge and Lorentz invariance in electromagnetism and relativity, yielding field equations uniquely from underlying symmetries—an approach which extends to modern particle physics (Standard Model) and vector gravity.

The authors argue that such symmetry-based derivations are instrumental in constructing self-consistent theories and evaluating their empirical predictions. Notably, while the Standard Model relies on experimentally-motivated symmetry selection, aspects such as family multiplicity and charge origin remain unexplained within its current framework. Vector gravity is posited as a promising avenue for integrating gravitational phenomena with quantum theory and particle physics.

Critique of Derivational Practice and Consequential Claims

A strong claim is made: the Schrödinger equation need not be adopted as a postulate, but can be rigorously derived from fundamental principles—chiefly the probabilistic nature of microphysics, the energy-momentum–frequency relations, continuity, and linearity. This perspective challenges the prevailing pedagogical tradition and urges a shift toward principle-based theoretical construction, paralleling historical developments in electromagnetism and relativity.

Furthermore, the discussion explores how modifications in foundational principles—such as the symmetry protocol—yield alternative physical theories with testable consequences for cosmology, elementary particle masses, dark energy, and gravitational waves. The vector gravity model’s predictions are cited as congruent with recent astrophysical observations.

Conclusion

This paper provides a comprehensive and formal derivation of the Schrödinger equation from foundational probabilistic and symmetry principles, situating it as a necessary structure within quantum mechanics rather than a heuristic postulate. The derivational methodology not only clarifies quantum-classical correspondence and informational aspects but also demonstrates the power of symmetry-driven theoretical construction. The argumentation advocates for principle-based approaches to physical theory, with broad implications for future research in quantum foundations, quantum information, and unified models of fundamental interactions (2603.27041).

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