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Whether solid, liquid, or gas, a substance's state depends on the order and arrangement of its particles (atoms, molecules, or ions). Particles in the solid pack closely together, generally in a pattern. The particles vibrate about their fixed positions but do not move or squeeze past their neighbors. In liquids, although the particles are closely spaced, they are randomly arranged. The position of the particles are not fixed—that is, they are free to move past their neighbors to...
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Prediction of First-Order Phase Transition with Electron-Phonon Interaction.

Mario Graml1,2, Kurt Hingerl1

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This study reveals electron-phonon interactions drive first-order phase transitions in solids by altering free energies. Incorporating nuclear kinetic energy explains these transitions and their critical temperatures.

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Area of Science:

  • Condensed Matter Physics
  • Materials Science
  • Quantum Mechanics

Background:

  • Phase transitions in solids are traditionally explained by the balance between binding energies and entropy.
  • Existing models often do not fully account for quantum mechanical effects on nuclear behavior during transitions.

Purpose of the Study:

  • To investigate the role of electron-phonon interactions in driving first-order phase transitions in solids.
  • To incorporate the quantum mechanical kinetic energy of nuclei into theoretical models of phase transitions.
  • To derive methods for determining critical transition temperatures, latent heat, and nuclear displacement.

Main Methods:

  • Incorporation of electron-phonon interactions into the system's Hamiltonian.
  • Application of Bogoliubov's inequality to account for the quantum mechanical kinetic energy operator of the nucleus.
  • Derivation of an implicit equation for critical temperature and estimation of thermodynamic properties.

Main Results:

  • Electron-phonon interactions lead to distinct free energies at different temperatures, resulting in first-order phase transitions.
  • The inclusion of nuclear quantum effects via Bogoliubov's inequality confirms first-order phase transitions.
  • An equation for critical temperature is implicitly derived, alongside estimations for latent heat and nuclear positional displacement.

Conclusions:

  • Electron-phonon interactions are crucial for understanding first-order phase transitions, particularly when nuclear quantum effects are considered.
  • The derived theoretical framework allows for the prediction of transition temperatures and associated physical properties.
  • This work establishes parameter boundaries for distinguishing between first- and second-order phase transitions.