2019
DOI: 10.1103/physrevmaterials.3.104604
|View full text |Cite
|
Sign up to set email alerts
|

Stability and electronic properties of GaN phases with inversion symmetry to inherently inhibit polarization

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
4
1

Citation Types

2
12
0

Year Published

2020
2020
2022
2022

Publication Types

Select...
6

Relationship

2
4

Authors

Journals

citations
Cited by 11 publications
(14 citation statements)
references
References 48 publications
2
12
0
Order By: Relevance
“…The atomic structures of pristine w -GaN and 4|8-GaN were optimized with the GGA-PBE functional, and the band structures are calculated with both GGA-PBE and HSE functionals. w -GaN exhibits a strong piezoelectric effect along the c axis together with strong polarity of the [0001̅] surface, while 4|8-GaN has rigorous zero polarization in the z axis, which significantly stabilizes the 4|8-GaN phase compared to w -GaN for few-atom-thick films, i.e., for films of from 2 to 18 monolayers, 4|8-GaN is the most stable phase. ,, The band gap of w -GaN obtained with the HSE functional is in good agreement with the experimental value (3.4 eV), while PBE-GGA gravely underestimates the band gap. The HSE functional predicts a direct band gap of 3.36 eV at the Γ point for 4|8-GaN, which ensures a high hole–electron recombination rate of 4|8-GaN similar to w -GaN. , Apart from the band gap underestimation by GGA-PBE for w -GaN and 4|8-GaN, their band dispersion properties are very similar to those obtained by the HSE functional.…”
Section: Results and Discussionsupporting
confidence: 76%
“…The atomic structures of pristine w -GaN and 4|8-GaN were optimized with the GGA-PBE functional, and the band structures are calculated with both GGA-PBE and HSE functionals. w -GaN exhibits a strong piezoelectric effect along the c axis together with strong polarity of the [0001̅] surface, while 4|8-GaN has rigorous zero polarization in the z axis, which significantly stabilizes the 4|8-GaN phase compared to w -GaN for few-atom-thick films, i.e., for films of from 2 to 18 monolayers, 4|8-GaN is the most stable phase. ,, The band gap of w -GaN obtained with the HSE functional is in good agreement with the experimental value (3.4 eV), while PBE-GGA gravely underestimates the band gap. The HSE functional predicts a direct band gap of 3.36 eV at the Γ point for 4|8-GaN, which ensures a high hole–electron recombination rate of 4|8-GaN similar to w -GaN. , Apart from the band gap underestimation by GGA-PBE for w -GaN and 4|8-GaN, their band dispersion properties are very similar to those obtained by the HSE functional.…”
Section: Results and Discussionsupporting
confidence: 76%
“…[27][28][29] Exhibiting differing physical properties, 6 polymorphs of a compound are desired for different applications. [30][31][32] While fourfold coordinated zinc blende and wurtzite phases as well as numerous stacking variations are used in current technologies, the search for novel polymorphs is a lasting endeavor. 14,32,33 Compared with the wurtzite phase, the vefold coordinated structure possesses higher symmetry that results in technologically favorable physical properties (e.g., absence of spontaneous polarization) for certain applications.…”
Section: Introductionmentioning
confidence: 99%
“…For example, it was predicted that the haeckelite bulk of C [44] and GaN could be semiconducting. [45,46] Experimentally, only the haeckelite crystal of β-BeO has been synthesized, [47] which is a semiconducting compound. Fascinated by interesting electronic properties of 2D T-lattice structures and to fill the gap in scientific knowledge on haeckelite crystal, here, by performing a set of first-principles calculations we have studied the electronic structures of twenty haeckelite XY compounds (X = B, Al, Ga, In, Tl; Y = N, P, As, Sb) belonging to the bigger family of III-V element compounds.…”
Section: Introductionmentioning
confidence: 99%