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Ab initio variational approach for evaluating lattice thermal conductivity (1212.0470v2)

Published 3 Dec 2012 in cond-mat.mtrl-sci

Abstract: We present a first-principles theoretical approach for evaluating the lattice thermal conductivity based on the exact solution of the Boltzmann transport equation. We use the variational principle and the conjugate gradient scheme, which provide us with an algorithm faster than the one previously used in literature and able to always converge to the exact solution. Three-phonon normal and umklapp collision, isotope scattering and border effects are rigorously treated in the calculation. Good agreement with experimental data for diamond is found. Moreover we show that by growing more enriched diamond samples it is possible to achieve values of thermal conductivity up to three times larger than the commonly observed in isotopically enriched diamond samples with 99.93% C12 and 0.07 C13.

Citations (206)

Summary

  • The paper presents a novel ab initio variational method using a conjugate gradient scheme to directly solve the Boltzmann transport equation without relying on traditional approximations.
  • It accurately models key phonon interactions including three-phonon normal and umklapp processes, isotope scattering, and boundary effects to improve thermal conductivity predictions.
  • The method achieves up to three times higher thermal conductivity in isotopically enriched diamond, offering promising insights for optimizing thermal management in advanced materials.

Ab initio Variational Approach for Evaluating Lattice Thermal Conductivity

The paper presents an innovative theoretical framework for accurately calculating the lattice thermal conductivity of materials, employing a first-principles approach based on the Boltzmann transport equation (BTE). The authors introduce a refined method combining the variational principle with a conjugate gradient scheme, resulting in an algorithm that converges more reliably and expeditiously than existing solutions. This approach specifically handles three-phonon normal (N) and umklapp (U) interactions, isotope scattering, and boundary effects with precision.

Theoretical Contributions

The primary advancement of this study lies in its proposed solution to the linearized BTE, achieved without the approximations traditionally relied upon, such as the single-mode relaxation time approximation (SMA). Instead of approximating the repopulation of phonon states, the authors solve the BTE using a variational method that ensures mathematical stability and fast convergence. This method utilizes preconditioned conjugate gradient minimization, a notable improvement over the Omini-Sparavigna (OS) iterative scheme known for its susceptibility to numerical instabilities in certain regimes.

A salient feature of this work is the robust treatment of phonon scattering processes, crucial for accurately modeling thermal transport in semiconductors and insulators. The lattice thermal conductivity is expressed via phonon frequencies, group velocities, and phonon populations, calculated from second and third order interatomic force constants (IFCs). These constants are derived using Density Functional Perturbation Theory (DFPT) and the Quantum ESPRESSO package, sidestepping the limitations of semi-empirical treatments.

Numerical Results and Practical Implications

A significant result of this work is the capability to compute thermal conductivity values up to three times larger than those observed in typical isotopically enriched diamond, showcasing the potential to optimize thermal transport properties through isotopic enrichment. The paper underscores the sensitivity of thermal conductivity to isotopic composition at low temperatures—a domain where traditional approximations often fail due to weak U processes and dominant N scattering.

The study explores the evaluation of diamond, a material with remarkably high thermal conductivity. Noteworthy numerical convergence is demonstrated with the proposed approach, particularly evident in scenarios where standard iterative methods falter due to the dominance of momentum-conserving N processes. The work further explores how lattice thermal conductivity varies with isotopic presence, demonstrating substantial differences that ground experimental expectations with theoretical predictions, especially in high crystalline purity contexts.

Theoretical and Future Implications

The implications of this research resonate both theoretically and practically. Theoretically, it provides a paradigm for exact solutions in phonon-driven thermal conductivity analyses, extending beyond the specific case of diamond to more complex atomic structures. Practically, the insights on isotopic variation and thermal conduction optimization hold promise for material engineering, especially for applications necessitating efficient heat dissipation, such as microelectronics and thermoelectric devices.

Looking forward, this ab initio method could be expanded to accommodate metallic systems and broader phonon interactions, potentially integrating more nuanced quantum mechanical effects. Its adoption could spur advancements in material design and characterization, facilitating the development of novel materials with tailored thermal properties.

In summary, this paper presents a significant technical advancement in the calculation of lattice thermal conductivity, providing both a methodological foundation and empirical insights for future materials research and application.

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