Electronic structure and optical properties of quantum crystals from first principles calculations in the Born–Oppenheimer approximation
At a Glance
Section titled “At a Glance”| Metadata | Details |
|---|---|
| Publication Date | 2020-12-21 |
| Journal | The Journal of Chemical Physics |
| Authors | Vitaly Gorelov, David M. Ceperley, Markus Holzmann, Carlo Pierleoni |
| Institutions | University of Illinois Urbana-Champaign, Centre National de la Recherche Scientifique |
| Citations | 10 |
| Analysis | Full AI Review Included |
Executive Summary
Section titled “Executive Summary”This research develops and validates a highly accurate, non-perturbative computational framework for determining the electronic structure and optical properties of quantum crystals, focusing on systems where nuclear quantum and thermal motion significantly impact electronic behavior.
- Methodological Breakthrough: A new formalism is established using Quantum Monte Carlo (QMC) methods to accurately account for the renormalization of electronic structure due to nuclear motion, moving beyond the limitations of the harmonic approximation and perturbative treatments.
- Quantum Averaging (QA): The paper introduces a “Quantum Averaging” procedure for calculating optical conductivity (via Kubo-Greenwood formalism), which is essential for light nuclei (like hydrogen) at low temperatures where phonon quantization invalidates the traditional semi-classical (William-Lax, WL) approach.
- Band Structure Restoration: A procedure is defined to meaningfully extend the concept of electronic crystal momentum (quasi-momentum) to quantum crystals by averaging the electron-ion wave function over the nuclear equilibrium distribution.
- Hydrogen Gap Closure: Applied to C2/c-24 solid hydrogen (200 K, 250 GPa), the method confirms a large electronic gap reduction (on the order of 2 eV) primarily due to zero-point nuclear motion.
- Optical Accuracy: QA successfully predicts the onset of optical absorption (Tauc gap) for hydrogen, yielding results consistent with the fundamental band gap, unlike the semi-classical WL method which significantly underestimates the gap near metallization pressures.
- Validation: The methodology was also applied to carbon diamond (297 K), confirming that the differences between QA and WL methods are minimal for heavier elements, validating the necessity of QA specifically for light quantum systems.
Technical Specifications
Section titled “Technical Specifications”| Parameter | Value | Unit | Context |
|---|---|---|---|
| Hydrogen Crystal Structure | C2/c-24 | N/A | High-pressure solid phase studied |
| Hydrogen Simulation Temperature | 200 | K | CEIMC/RQMC calculations |
| Hydrogen Simulation Pressure Range | 248 to 290 | GPa | Range of pressures studied for H2 |
| Hydrogen Gap Reduction (ZPM) | ~2 | eV | Reduction in electronic gap due to nuclear motion |
| Hydrogen Tauc Gap (248 GPa, QA) | 1.3 | eV | Gap extracted via Quantum Averaging |
| Hydrogen Tauc Gap (248 GPa, WL) | 0.8 | eV | Gap extracted via Semi-classical Averaging |
| Carbon Diamond Temperature | 297 | K | Simulation temperature for C |
| Carbon Diamond Supercell Size | 64 | Atoms | Cubic supercell used for PIMD |
| Carbon Tauc Gap (297 K, QA) | 3.55 | eV | Gap extracted via Quantum Averaging (PBE) |
| RQMC Imaginary Time Projection (t) | 2.00 | Ha-1 | Used for electron addition/removal energy convergence |
| RQMC Time Step (τ) | 0.01 | Ha-1 | Used for electron addition/removal energy calculation |
| QMC Twist Grid Size | 6x6x6 or 8x8x8 | N/A | Monkhorst-Pack grid used for twist averaging |
Key Methodologies
Section titled “Key Methodologies”The methodology combines advanced many-body QMC techniques with path integral methods to handle both electronic correlation and nuclear quantum dynamics non-perturbatively under the Born-Oppenheimer (BO) approximation.
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Nuclear Dynamics Sampling:
- Coupled Electron-Ion Monte Carlo (CEIMC) and Path Integral Molecular Dynamics (PIMD) were used to sample nuclear configurations (R) at finite temperature (T) and constant volume (V).
- This sampling inherently includes nuclear zero-point motion and thermal fluctuations without relying on the harmonic approximation.
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Electronic Energy Calculation (Gap):
- The fundamental electronic gap (Δ = µ+ - µ-) was determined from electron addition and removal energies using high-accuracy Reptation Quantum Monte Carlo (RQMC).
- The Grand-Canonical Twist Averaging Boundary Conditions (GCTABC) approach was employed to minimize finite-size effects and calculate the electronic density of states (DOS) and energy density ε(µ).
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Band Structure Extension:
- The electronic quasi-momentum (Bloch vector) for excitations in the quantum crystal was restored by marginalizing the total electron-ion wave function with respect to the nuclear equilibrium distribution.
- This involved analyzing the overlap matrix elements T(q, m; q, m’) averaged over nuclear configurations, confirming that excitations retain a well-defined crystal momentum.
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Optical Conductivity Calculation:
- Optical conductivity σ(ω, T) was computed using the Kubo-Greenwood (KG) formalism.
- Quantum Averaging (QA): For light nuclei (H2), the standard semi-classical William-Lax (WL) procedure was replaced by QA, where the electronic eigenvalues and transition matrix elements are averaged over the nuclear states (Eq. 28), ensuring consistency with the thermodynamic gap definition at low temperatures.
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DFT Support:
- Density Functional Theory (DFT) calculations (PBE, vdW-DF, HSE) were used for initial structural relaxation, generating trial wave functions for QMC, and performing comparative Tauc analysis on the absorption profiles.
Commercial Applications
Section titled “Commercial Applications”This advanced computational framework provides critical predictive capabilities for materials operating under extreme conditions or where quantum effects dominate, enabling reliable design and engineering of next-generation materials.
- High-Pressure Materials Discovery: Essential for accurately modeling materials (like hydrogen) under extreme pressures, guiding the search for high-temperature superconductors or novel metallic phases.
- Advanced Semiconductor and Insulator Design: Provides highly accurate electronic band gaps and excitation spectra for wide-bandgap materials (e.g., diamond), crucial for high-power electronics and UV optics.
- Predictive Optical Engineering: Enables precise prediction of optical absorption profiles and conductivity in quantum crystals, necessary for designing transparent materials or optimizing light-harvesting systems operating at cryogenic temperatures.
- Quantum Materials Modeling: Offers a robust, non-perturbative tool for investigating strongly correlated systems and molecular crystals where electron-phonon coupling and nuclear quantum motion are significant, improving the reliability of ab initio simulations.
View Original Abstract
We develop a formalism to accurately account for the renormalization of the electronic structure due to quantum and thermal nuclear motions within the Born-Oppenheimer approximation. We focus on the fundamental energy gap obtained from electronic addition and removal energies from quantum Monte Carlo calculations in either the canonical or grand-canonical ensembles. The formalism applies as well to effective single electron theories such as those based on density functional theory. We show that the electronic (Bloch) crystal momentum can be restored by marginalizing the total electron-ion wave function with respect to the nuclear equilibrium distribution, and we describe an explicit procedure to establish the band structure of electronic excitations for quantum crystals within the Born-Oppenheimer approximation. Based on the Kubo-Greenwood equation, we discuss the effects of nuclear motion on optical conductivity. Our methodology applies to the low temperature regime where nuclear motion is quantized and, in general, differs from the semi-classical approximation. We apply our method to study the electronic structure of C2/c-24 crystalline hydrogen at 200 K and 250 GPa and discuss the optical absorption profile of hydrogen crystals at 200 K and carbon diamond at 297 K.
Tech Support
Section titled “Tech Support”Original Source
Section titled “Original Source”References
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- 2020 - Quantum Monte Carlo Compton profiles of solid and liquid lithium [Crossref]
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