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Uberuaga, and Hannes Jónsson

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16 Pith papers citing it
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  • method increase the combinations of binding sites, defect states, surface disorder, adsorbate orientations/coverages, and interactions with the gas/liquid phase. PredictingE a via transition state searches is particularly challenging, as it requires accurate knowledge of the PES near both local minima and saddle points. The nudged elastic band (NEB) method[4] has been widely used to identify transition states, but has an cost that scales with number of intermediate images and can converge slowly for po
  • background annihilation of Frenkel defects in organo- lead halide perovskites.Energy Environ. Sci. 2016,9, 3180-3187. (21) deQuilettes, D. W.; Zhang, W.; Burlakov, V. M.; Graham, D. J.; Lei- jtens, T.; Osherov, A.; Bulovi' c, V.; Snaith, H. J.; Ginger, D. S.; Stranks, S. D. Photo-induced halide redistribution in organic-inorganic perovskite films.Nat. Commun.2016,7, 11683. (22) Xing, J.; Wang, Q.; Dong, Q.; Yuan, Y.; Fang, Y.; Huang, J. Ultrafast ion migration in hybrid perovskite polycrystalline thin film
  • background The calculated diffusion barrier ofCu+ i is 0.15 eV, whereas that ofCu0 i is 0.46 eV. Our result forCu+ i is consistent with intrinsic diffusion barrier of0.18 ± 0 .02 eV obtained by transient ion drifting (TID) experiment [2]. For comparison, our calculated diffusion barrier with PBE-GGA functional for Cu+ i is 0.13 eV, which is close to a previous LDA result of 0.11 eV [46]. It should be noted that both LDA and GGA functionals tend to underestimate reaction barriers due to the intrinsic approx
  • background The minimum energy path for the migration of the polaron from one Fe ion to an adjacent one within the basal plane was calculated using the NEB method. The results are shown in Figure 3. The rise in the energy along the minimum energy path gives an activation energy of 0.12 eV. This is in excellent agreement with the experimental estimate of 0.118 eV [23]. Figure 3. Minimum energy path found using NEB calculations for polaron migration between two adjacent Fe ions, Fe0 and Fe1, within the same b
  • background 3] 3916.8 [217.8]3.2 [0.8] 56.0 [11.0] NTK 261.3 [22.3] 3945.3 [393.3]2.8 [1.2] 54.3 [11.3] NTK-F 329.7 [41.3] 4395.5 [467.5] 3.5 [0.5] 59.5 [13.5] NTK-EF 343.2 [71.2] 4287.7 [352.3] 3.3 [1.3] 59.7 [13.7] Intra (Frame) Random 528.3 [164.8] 7117.8 [1018.3] 6.5 [2.5] 112.0 [19.0] Committee-E 671.0 [210.0] 7690.5 [722.5] 5.0 [2.0] 90.5 [12.5] Tanimoto 492.0 [139.0] 6255.0 [623.0] 7.0 [3.0] 112.5 [26.5] SOAP 362.8 [14.8] 5541.3 [388.8] 3.5 [1.5] 67.5 [6.5] Activation274.5 [30.5] 4086.5 [318.5]3.5 [0

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2026 16

representative citing papers

A Unified microscopic picture of cation and anion migration in MAPbI$_3$

cond-mat.mtrl-sci · 2026-05-04 · unverdicted · novelty 6.0

Molecular dynamics simulations find that both I and MA defects in MAPbI3 diffuse rapidly at room temperature with barriers of 0.15-0.20 eV, with MA interstitials moving via concerted mechanisms and no MA vacancy migration observed.

Systematic Fine-Tuning of MACE Interatomic Potentials for Catalysis

physics.chem-ph · 2026-05-10 · conditional · novelty 5.0

Fine-tuned MACE MLIPs achieve lower mean absolute errors on catalytic reaction energies and barriers than from-scratch models, with a large fine-tuned model performing best on both metallic and oxide systems including out-of-distribution cases.

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