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Published on: May 28, 2016
Exploring the link between crystal defects and nonaffine displacement fluctuations
Pankaj Popli1, Sayantani Kayal1, Peter Sollich2,3
1Tata Institute for Fundamental Research, Centre for Interdisciplinary Sciences, 36/P Gopanapally, Hyderabad 500107, India.
This study analyzes atomic displacement fluctuations in crystals, distinguishing between affine (strain/rotation) and nonaffine (localized) modes. Compact crystals show dominant nonaffine modes linked to defects, while open crystals exhibit softer modes and greater instability. Keywords: atomic displacement, crystal fluctuations, lattice defects.
Area of Science:
- Solid-state physics
- Materials science
- Crystallography
Background:
- Thermal fluctuations cause atomic displacements in crystals.
- These displacements can be decomposed into affine (strain/rotation) and nonaffine (localized) components.
- Understanding these modes is crucial for predicting material properties and defect formation.
Purpose of the Study:
- To generalize and apply a formalism for studying thermal fluctuations of atomic displacements.
- To analyze both compact and open crystals with multiatom bases in various dimensions.
- To investigate the nature and behavior of affine and nonaffine displacement modes.
Main Methods:
- Generalization of a recently introduced formalism.
- Coarse-graining analysis of atomic displacement fluctuations.
- Computation of thermodynamic averages and correlation functions within harmonic theory.
Main Results:
- Compact crystals exhibit a dominant, gapped nonaffine mode linked to defect precursors.
- Open crystals lack a prominent gap, showing soft nonaffine modes associated with localized defects.
- Higher-order coupling between affine and nonaffine modes is significantly larger in open lattices.
Conclusions:
- The study provides a unified framework for understanding crystal deformation mechanisms like slips and stacking faults.
- Nonaffine modes play a critical role in lattice stability and defect formation.
- The findings are expected to be general, independent of specific atomic interactions.
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