Challenges
Datasets
Workspaces
Papers
Discussions
Leaderboard
Log inSign up
Challenges
Datasets
Workspaces
Papers
Discussions
Leaderboard
Blog
Job Board
Q3AS

© 2026 Aqora Quantum S.A.S.

TermsPrivacyLegal Notice

Lettere al nuovo cimento della societa italiana di fisica/Lettere al nuovo cimento

Schrödinger’s equation as a consequence of zitterbewegung

G. Cavalleri

Published Jul 1, 1985• 31 citations
Publisher
DOI
10.1007/bf02751922

Related papers

The Schrödinger Equations and Their Consequences

Salvatore Capozzıello, Wladimir-Georges Boskoff

UNITEXT for physics•Jan 1, 2021•0 citations

The Schrödinger Equation and Negative Energies

Stanley A. Bruce

Abstract It is known that there is no room for anti-particles within the Schrödinger regime in quantum mechanics. In this article, we derive a (non-relativistic) Schrödinger-like wave equation for a spin- 1 / 2 $1/2$ free particle in 3 + 1 space-time dimensions, which includes both positive- and negative-energy eigenstates. We show that, under minimal interactions, this equation is invariant under 𝒫 𝒯 $\mathcal{P}\mathcal{T}$ and 𝒞 discrete symmetries. An immediate consequence of this is that the particle exhibits Zitterbewegung (‘trembling motion’), which arises from the interference of positive- and negative-energy wave function components.

Zeitschrift für Naturforschung A•Sep 19, 2018•2 citations

More on the Schrödinger Equation

Jochen Pade

Undergraduate lecture notes in physics•Jan 1, 2018•0 citations

Schrodinger Equation for Nanoscience

Janina Marciak-kozlowska B, Mirosław Kozłowski

The second order (in time) Schrodinger equation is proposed. The additional term (in comparison to Schrodinger equation) describes the interaction of particles with vacuum filled with virtual particle-antiparticle pairs (zitterbewegung). Key words: Schrodinger equation; Nanoscience; Zitterbewegung.

arXiv:cond-mat/0306699•Jun 27, 2003•3 citations

More on the Schrödinger Equation

Jochen Pade

Undergraduate lecture notes in physics•Nov 7, 2013•0 citations

2X2 Matrix Model And The Schrodinger Equation

Francesco R. Ruggeri

In a series of notes it was shown that a 2x2 matrix energy eigenvalue equation is naturally contained in Einstein´s 1905 energy momentum equation E2 = p2 + m2 . This equation, which appears to be related to the Dirac equation, but contains no spatial features, is linear in energy and describes bouncing of a particle back and forth with an overall average motion of v to the right. It appears to be quantum mechanical in nature as the energy matrix acts as an evolution operator, expectation values of operators are taken and one has an energy eigenvector representing the square roots of probability. Knuth [18 ] has used a model which yields directly probabilities for a particle bouncing back and forth with an average v to the right. It was shown that these probabilities, the squares of the terms of the energy eigenvector, can be obtained by maximizing Shannon´s entropy subject to the constraint the f1-f2= v, where f1 is the probability to move forward and f2, that to move backward. In this note, we try to find a link between the 2x2 matrix equation and the Schrodinger (or Dirac) equation in a region with a potential V(r). The Schrodinger equation, unlike the matrix equation, is spatial. Next, we try to see if there are any features of zitterbewegung that might apply in this case. In the 2x2 matrix model, Schrodinger´s zitterbewegung can be derived, so it seems reasonable to ask whether there might be zitterbewegung in the more complicated case of a bound state in a potential. Finally, we raise the issue of a possible link between the Schrodinger equation and statistical mechanics. In the 2x2 model, the forward and backward postulated motion of a particle was connected to maximum entropy. It would be interesting if a similar idea could be applied to bound states. We do not present any calculations related to such entropy maximization, but mention work in the literature in which Tsallis entropy is maximized subject to constraints to obtain the ground state wavefunction without solving the single particle temperature=0 Schrodinger equation.

•Aug 10, 2018•0 citations
Abstract It is known that there is no room for anti-particles within the Schrödinger regime in quantum mechanics. In this article, we derive a (non-relativistic) Schrödinger-like wave equation for a spin- 1 / 2 1/21/21/2 free particle in 3 + 1 space-time dimensions, which includes both positive- and negative-energy eigenstates. We show that, under minimal interactions, this equation is invariant under 𝒫 𝒯 PT\mathcal{P}\mathcal{T}PT and 𝒞 discrete symmetries. An immediate consequence of this is that the particle exhibits Zitterbewegung (‘trembling motion’), which arises from the interference of positive- and negative-energy wave function components.
In a series of notes it was shown that a 2x2 matrix energy eigenvalue equation is naturally contained in Einstein´s 1905 energy momentum equation E2 = p2 + m2 . This equation, which appears to be related to the Dirac equation, but contains no spatial features, is linear in energy and describes bouncing of a particle back and forth with an overall average motion of v to the right. It appears to be quantum mechanical in nature as the energy matrix acts as an evolution operator, expectation values of operators are taken and one has an energy eigenvector representing the square roots of probability. Knuth [18 ] has used a model which yields directly probabilities for a particle bouncing back and forth with an average v to the right. It was shown that these probabilities, the squares of the terms of the energy eigenvector, can be obtained by maximizing Shannon´s entropy subject to the constraint the f1-f2= v, where f1 is the probability to move forward and f2, that to move backward. In this note, we try to find a link between the 2x2 matrix equation and the Schrodinger (or Dirac) equation in a region with a potential V(r). The Schrodinger equation, unlike the matrix equation, is spatial. Next, we try to see if there are any features of zitterbewegung that might apply in this case. In the 2x2 matrix model, Schrodinger´s zitterbewegung can be derived, so it seems reasonable to ask whether there might be zitterbewegung in the more complicated case of a bound state in a potential. Finally, we raise the issue of a possible link between the Schrodinger equation and statistical mechanics. In the 2x2 model, the forward and backward postulated motion of a particle was connected to maximum entropy. It would be interesting if a similar idea could be applied to bound states. We do not present any calculations related to such entropy maximization, but mention work in the literature in which Tsallis entropy is maximized subject to constraints to obtain the ground state wavefunction without solving the single particle temperature=0 Schrodinger equation.