Phonovoltaic. III. Electron-phonon coupling and figure of merit of graphene:BN
Abstract
The phonovoltaic cell harvests optical phonons like a photovoltaic harvests photons, that is, a nonequilibrium (hot) population of optical phonons (at temperature $$T$$ p,O ) more energetic than the band gap produces electron-hole pairs in a $$p$$-$$n$$ junction, which separates these pairs to produce power. A phonovoltaic material requires an optical phonon mode more energetic than its band gap and much more energetic than the thermal energy ($$E$$p,O $ΔE$e,g≫ $$k$$B$$T$$ ) , which relaxes by generating electrons and power (at rate $$\dot{γ}$$ e-p) rather than acoustic phonons and heat (at rate $$\dot{γ}$$ p-p ). Graphene (h-C) is the most promising material candidate: when its band gap is tuned to its optical phonon energy without greatly reducing the electron-phonon (e-p) coupling, it reaches a substantial figure of merit [ $$Z$$pV= $ΔE$e,g $$\dot{γ}$$ e-p/ $$E$$p,O($$\dot{γ}$$ e-p + $$\dot{γ}$$ p-p) ≈ 0.8 ] . A simple tight-binding (TB) model presented here predicts that lifting the sublattice symmetry of graphene in order to open a band gap proscribes the e-p interaction at the band edge, such that $$\dot{γ}$$ e-p→ 0 as $ΔE$e,g → $$E$$p,O. However, ab initio (DFT-LDA) simulations of layered h-C/BN and substitutional h-C:BN reveal that the e-p coupling remains substantial in these asymmetric crystals. Indeed, h-C:BN achieves a high figure of merit ( $$Z$$pV ≈ 0.6 ) . At 300 K and for a Carnot limit of 0.5 ( $$T$$ p,O = 600 K ) , a h-C:BN phonovoltaic can reach an efficiency of ηpV ≈ 0.2 , double the thermoelectric efficiency ( $ZT$ ≈ 1) under similar conditions.
- Authors:
-
- Univ. of Michigan, Ann Arbor, MI (United States). Dept. of Mechanical Engineering
- Publication Date:
- Research Org.:
- Lawrence Berkeley National Laboratory (LBNL), Berkeley, CA (United States). National Energy Research Scientific Computing Center (NERSC)
- Sponsoring Org.:
- USDOE Office of Science (SC); National Science Foundation (NSF)
- OSTI Identifier:
- 1544415
- Alternate Identifier(s):
- OSTI ID: 1335056
- Grant/Contract Number:
- AC02-05CH11231; CBET1332807
- Resource Type:
- Accepted Manuscript
- Journal Name:
- Physical Review B
- Additional Journal Information:
- Journal Volume: 94; Journal Issue: 24; Journal ID: ISSN 2469-9950
- Publisher:
- American Physical Society (APS)
- Country of Publication:
- United States
- Language:
- English
- Subject:
- 75 CONDENSED MATTER PHYSICS, SUPERCONDUCTIVITY AND SUPERFLUIDITY
Citation Formats
Melnick, Corey, and Kaviany, Massoud. Phonovoltaic. III. Electron-phonon coupling and figure of merit of graphene:BN. United States: N. p., 2016.
Web. doi:10.1103/PhysRevB.94.245412.
Melnick, Corey, & Kaviany, Massoud. Phonovoltaic. III. Electron-phonon coupling and figure of merit of graphene:BN. United States. https://doi.org/10.1103/PhysRevB.94.245412
Melnick, Corey, and Kaviany, Massoud. Fri .
"Phonovoltaic. III. Electron-phonon coupling and figure of merit of graphene:BN". United States. https://doi.org/10.1103/PhysRevB.94.245412. https://www.osti.gov/servlets/purl/1544415.
@article{osti_1544415,
title = {Phonovoltaic. III. Electron-phonon coupling and figure of merit of graphene:BN},
author = {Melnick, Corey and Kaviany, Massoud},
abstractNote = {The phonovoltaic cell harvests optical phonons like a photovoltaic harvests photons, that is, a nonequilibrium (hot) population of optical phonons (at temperature $T$ p,O ) more energetic than the band gap produces electron-hole pairs in a $p$-$n$ junction, which separates these pairs to produce power. A phonovoltaic material requires an optical phonon mode more energetic than its band gap and much more energetic than the thermal energy ($E$p,O $ΔE$e,g≫ $k$B$T$ ) , which relaxes by generating electrons and power (at rate $\dot{γ}$ e-p) rather than acoustic phonons and heat (at rate $\dot{γ}$ p-p ). Graphene (h-C) is the most promising material candidate: when its band gap is tuned to its optical phonon energy without greatly reducing the electron-phonon (e-p) coupling, it reaches a substantial figure of merit [ $Z$pV= $ΔE$e,g $\dot{γ}$ e-p/ $E$p,O($\dot{γ}$ e-p + $\dot{γ}$ p-p) ≈ 0.8 ] . A simple tight-binding (TB) model presented here predicts that lifting the sublattice symmetry of graphene in order to open a band gap proscribes the e-p interaction at the band edge, such that $\dot{γ}$ e-p→ 0 as $ΔE$e,g → $E$p,O. However, ab initio (DFT-LDA) simulations of layered h-C/BN and substitutional h-C:BN reveal that the e-p coupling remains substantial in these asymmetric crystals. Indeed, h-C:BN achieves a high figure of merit ( $Z$pV ≈ 0.6 ) . At 300 K and for a Carnot limit of 0.5 ( $T$ p,O = 600 K ) , a h-C:BN phonovoltaic can reach an efficiency of ηpV ≈ 0.2 , double the thermoelectric efficiency ( $ZT$ ≈ 1) under similar conditions.},
doi = {10.1103/PhysRevB.94.245412},
journal = {Physical Review B},
number = 24,
volume = 94,
place = {United States},
year = {Fri Dec 09 00:00:00 EST 2016},
month = {Fri Dec 09 00:00:00 EST 2016}
}
Web of Science
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