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Springer eBooks

Quantum Mechanics: The Unavoidable Path

Bernard Fernandez

Published Jul 23, 2012• 0 citations
Publisher
DOI
10.1007/978-1-4614-4181-6_3

Related papers

Quantum Mechanics at the Crossroads

James W. Evans, Alan S. Thorndike

Springer eBooks•Nov 1, 2006•13 citations

Mesoscopic Corridors Are Dynamically Unavoidable in a One-Dimensional Block-Spin Chain

S. Pan

We study single-spin-flip switching paths in a one-dimensional interacting block-spin chain. Previous static work shows that the minimal phase-crossing energy scales as K*sqrt(J) and that any optimal crossing layer has width of order sqrt(J). The missing step toward metastable slowdown is dynamical: one must show that near-optimal switching paths cannot avoid such an extended layer. In this paper we isolate that bridge. We prove that any minus-to-plus path whose maximal energy remains on the near-optimal K*sqrt(J) scale must contain an intermediate configuration with a transition corridor of width at least c*sqrt(J). Thus the static mesoscopic layer is not merely an optimizer of a boundary-value problem: it is dynamically unavoidable along low-barrier switching paths. The present result is a mechanism theorem rather than a full mixing-time theorem, and it prepares the corridor-shell bottleneck analysis needed for later conductance and spectral-gap estimates. Related earlier works by S. Pan are available at DOI: 10.5281/zenodo.19673404 and DOI: 10.5281/zenodo.19689210.

•Apr 22, 2026•0 citations

Lord Kelvin's Second Cloud

Gilles Montambaux

On April 27, 1900, William Thomson, better known as Lord Kelvin, delivered a visionary speech before the Royal Institution of Great Britain. In it, he presented two unresolved problems which, to him, appeared fundamental and unavoidable at the turn of the 20th century. He compared them to two clouds obscuring our understanding of physics. Dissipating these two clouds would eventually require the development of special relativity and quantum mechanics. This article revisits the second cloud which, contrary to what is often claimed in the literature, did not concern black-body radiation, but rather the specific heat of polyatomic molecules. To clarify this, the article aims to place Kelvin's speech within the historical context of the time and to situate it within the sequence of developments, from Kirchhoff to the first Solvay Conference in 1911, that marked the path of the extraordinary intellectual adventure that led to the birth of quantum mechanics. It will also be shown that Max Planck's initial motivation was not to solve the problem of the so-called "ultraviolet catastrophe."

physics.hist-phCross-listedarXiv:2603.16902•Mar 5, 2026

QUANTUM MECHANICS: THE REAL AND THE POSSIBLE

Giuseppe Boscarino

Conference on the Foundations of Quantum Mechanics: Historical Analysis and Open Questions•May 1, 2000•1 citation

The Uncertainty Principle as a Structural Admissibility Constraint

Lisa Michelle Doumbouya

The uncertainty principle is among the most widely cited results of quantum mechanics, yet it is also one of the most persistently misunderstood. It is frequently explained as a limitation of measurement, experimental disturbance, or technological precision, despite being fundamentally independent of observation. This paper reframes the uncertainty principle as a structural constraint arising from the geometry of admissible physical paths under finite temporal resolution. We argue that tradeoffs between localization and momentum coherence do not reflect epistemic ignorance or measurement back-action, but instead express an unavoidable incompatibility between competing structural requirements. Within a structure-first framework, uncertainty emerges naturally from the need to maintain global coherence while restricting admissible continuation. This interpretation preserves the standard formalism of quantum mechanics while clarifying the conceptual origin of uncertainty and preparing a foundation for later discussions of quantum fields as pre-nodal harmonic structure.

•Dec 18, 2025•0 citations

Quantum Mechanics: Perspectives

WORLD SCIENTIFIC eBooks•Aug 1, 2009•0 citations
We study single-spin-flip switching paths in a one-dimensional interacting block-spin chain. Previous static work shows that the minimal phase-crossing energy scales as K*sqrt(J) and that any optimal crossing layer has width of order sqrt(J). The missing step toward metastable slowdown is dynamical: one must show that near-optimal switching paths cannot avoid such an extended layer. In this paper we isolate that bridge. We prove that any minus-to-plus path whose maximal energy remains on the near-optimal K*sqrt(J) scale must contain an intermediate configuration with a transition corridor of width at least c*sqrt(J). Thus the static mesoscopic layer is not merely an optimizer of a boundary-value problem: it is dynamically unavoidable along low-barrier switching paths. The present result is a mechanism theorem rather than a full mixing-time theorem, and it prepares the corridor-shell bottleneck analysis needed for later conductance and spectral-gap estimates. Related earlier works by S. Pan are available at DOI: 10.5281/zenodo.19673404 and DOI: 10.5281/zenodo.19689210.
On April 27, 1900, William Thomson, better known as Lord Kelvin, delivered a visionary speech before the Royal Institution of Great Britain. In it, he presented two unresolved problems which, to him, appeared fundamental and unavoidable at the turn of the 20th century. He compared them to two clouds obscuring our understanding of physics. Dissipating these two clouds would eventually require the development of special relativity and quantum mechanics. This article revisits the second cloud which, contrary to what is often claimed in the literature, did not concern black-body radiation, but rather the specific heat of polyatomic molecules. To clarify this, the article aims to place Kelvin's speech within the historical context of the time and to situate it within the sequence of developments, from Kirchhoff to the first Solvay Conference in 1911, that marked the path of the extraordinary intellectual adventure that led to the birth of quantum mechanics. It will also be shown that Max Planck's initial motivation was not to solve the problem of the so-called "ultraviolet catastrophe."
The uncertainty principle is among the most widely cited results of quantum mechanics, yet it is also one of the most persistently misunderstood. It is frequently explained as a limitation of measurement, experimental disturbance, or technological precision, despite being fundamentally independent of observation. This paper reframes the uncertainty principle as a structural constraint arising from the geometry of admissible physical paths under finite temporal resolution. We argue that tradeoffs between localization and momentum coherence do not reflect epistemic ignorance or measurement back-action, but instead express an unavoidable incompatibility between competing structural requirements. Within a structure-first framework, uncertainty emerges naturally from the need to maintain global coherence while restricting admissible continuation. This interpretation preserves the standard formalism of quantum mechanics while clarifying the conceptual origin of uncertainty and preparing a foundation for later discussions of quantum fields as pre-nodal harmonic structure.