Challenges in predicting positron annihilation lifetimes in lead halide perovskites: correlation functionals and polymorphism
Pith reviewed 2026-05-17 23:59 UTC · model grok-4.3
The pith
The choice of electron-positron correlation functional strongly affects predicted positron annihilation lifetimes in lead halide perovskites, especially for cation vacancies.
A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.
Core claim
In lead halide perovskites the positron annihilation lifetimes calculated for cation vacancies depend critically on the chosen electron-positron correlation functional, with differences far larger than those encountered in metals, alloys, or conventional semiconductors; the weighted density approximation and various semi-local forms are compared directly, and the results indicate that experimental lifetime assignments for these materials may need to be reconsidered.
What carries the argument
The electron-positron correlation functional (semi-local forms and the non-local weighted density approximation) that determines the positron's interaction with the spatially varying electron density inside the perovskite lattice.
Load-bearing premise
The differences among calculated lifetimes arise mainly from the choice of electron-positron correlation functional rather than from supercell size, k-point sampling, or the modeling of organic-cation motion.
What would settle it
Precise experimental positron lifetime spectra recorded on well-characterized lead halide perovskite crystals whose dominant vacancy type and concentration have been established by an independent method such as electron microscopy or Hall measurements.
Figures
read the original abstract
Halide perovskites have emerged in the last decade as a new important class of semiconductors for a variety of optoelectronic applications. A lot of previous studies were thus devoted to the characterisation of their point defects. Positron annihilation spectroscopy is a well recognized tool for probing vacancies in materials. Recent applications of this technique to APbX$_3$ halide perovskites are sparse, and the rare theoretical predictions of positron lifetimes in these materials, published in association with experiments, do not fully agree with each other. These works suggest that vacancies on the A site are not detected. In our theoretical study we focus on the role of the electron-positron correlation functional. We thoroughly revisit and compare several approximations when applied to methylammonium lead iodide (MAPbI$_3$) with or without vacancies, as well as inorganic perovskites CsPbI$_3$ and CsPbBr$_3$, in various phases. We show also the relationship between the size of the voids, through Voronoi volumes, and the calculated lifetimes. For the cubic phases we investigate in detail the role of polymorphism, including the distribution of vacancy formation energies and positron annihilation lifetimes. In our lifetimes calculations, apart from older and more recent semi-local approximations for the electron-positron correlation potential, we also consider the weighted density approximation (WDA), which is truly non-local and should better describe positron annihilation in regions with strong electronic density variations. We show that for this class of materials, and especially for cations vacancies, the influence of the chosen approximation is crucial, much stronger than in metals, alloys and conventional semiconductors. This influence may induce to reconsider the interpretation of experimentally determined lifetimes.
Editorial analysis
A structured set of objections, weighed in public.
Referee Report
Summary. The paper examines the sensitivity of positron annihilation lifetime calculations to the choice of electron-positron correlation functional in lead halide perovskites (MAPbI₃, CsPbI₃, CsPbBr₃). It compares semi-local approximations with the weighted density approximation (WDA) for systems with and without vacancies, across multiple phases, and relates computed lifetimes to Voronoi volumes of voids. The central claim is that functional choice exerts a much stronger influence on lifetimes—especially for A-site cation vacancies—than observed in metals, alloys, or conventional semiconductors, potentially requiring reinterpretation of experimental data. Polymorphism effects in cubic phases are also analyzed.
Significance. If the attribution of lifetime variations primarily to the correlation functional is substantiated, the work would demonstrate that non-local treatments such as WDA are essential for reliable positron lifetime predictions in hybrid perovskites with large voids and strong density gradients. This could refine defect identification via positron annihilation spectroscopy in optoelectronic materials and caution against over-reliance on semi-local functionals in systems with pronounced structural complexity.
major comments (2)
- [Computational Methods] Computational Methods section: The manuscript must demonstrate that supercell sizes, k-point meshes, ionic relaxation criteria, and basis-set parameters were converged to identical tolerances for every functional and every polymorph/phase. Without such uniform controls, the reported strong functional dependence on lifetimes (particularly for cation vacancies) cannot be unambiguously separated from possible artifacts arising from inconsistent technical settings in materials known to be sensitive to void volume and organic-cation dynamics.
- [Results] Results on vacancy lifetimes (likely §4 or equivalent): Direct numerical tables comparing lifetimes across functionals for the same supercell and k-point settings should be presented, together with estimated uncertainties from convergence tests. The claim that the functional influence is “much stronger than in metals, alloys and conventional semiconductors” requires explicit side-by-side benchmarks against at least one reference material computed with the identical protocol.
minor comments (2)
- [Figures] Figure captions and text should explicitly state the supercell size and k-point sampling used for each reported lifetime value to allow immediate assessment of consistency.
- [Discussion] The relationship between Voronoi volumes and lifetimes is interesting but would benefit from a quantitative correlation plot or fit parameter in the main text rather than only qualitative discussion.
Simulated Author's Rebuttal
We thank the referee for the careful and constructive review of our manuscript. We address each major comment below and describe the revisions that will be incorporated to strengthen the presentation and support for our claims.
read point-by-point responses
-
Referee: [Computational Methods] Computational Methods section: The manuscript must demonstrate that supercell sizes, k-point meshes, ionic relaxation criteria, and basis-set parameters were converged to identical tolerances for every functional and every polymorph/phase. Without such uniform controls, the reported strong functional dependence on lifetimes (particularly for cation vacancies) cannot be unambiguously separated from possible artifacts arising from inconsistent technical settings in materials known to be sensitive to void volume and organic-cation dynamics.
Authors: We agree that uniform convergence settings across all calculations are essential to isolate the influence of the electron-positron correlation functional. Our original calculations employed identical supercell sizes, k-point meshes, ionic relaxation criteria, and basis-set parameters for every functional and every phase/polymorph. In the revised manuscript we will expand the Computational Methods section with an explicit statement of these shared parameters and add a summary table listing the settings used for each system and functional, together with representative convergence tests confirming that the chosen tolerances were met uniformly. revision: yes
-
Referee: [Results] Results on vacancy lifetimes (likely §4 or equivalent): Direct numerical tables comparing lifetimes across functionals for the same supercell and k-point settings should be presented, together with estimated uncertainties from convergence tests. The claim that the functional influence is “much stronger than in metals, alloys and conventional semiconductors” requires explicit side-by-side benchmarks against at least one reference material computed with the identical protocol.
Authors: We accept that a consolidated table would improve clarity and verifiability. We will add a new table in the Results section that compiles all computed positron lifetimes for the different functionals, vacancy types, and phases, all obtained with the same supercell and k-point settings, and will include estimated uncertainties based on our convergence tests. For the comparative claim, our statement is grounded in published lifetime differences reported for metals, alloys, and conventional semiconductors; however, to address the request for an identical-protocol benchmark we will either (i) perform a limited test calculation on a simple reference system such as bulk silicon using our current setup or (ii) qualify the claim more precisely by direct reference to the literature values while noting the protocol differences. We therefore mark this revision as partial pending feasibility of new calculations within the revision period. revision: partial
Circularity Check
No significant circularity: direct first-principles comparison of functionals
full rationale
The paper reports explicit DFT-based computations of positron lifetimes in MAPbI3, CsPbI3 and CsPbBr3 using multiple electron-positron correlation approximations (semi-local and WDA) together with Voronoi-volume analysis. No parameters are fitted to experimental lifetimes and then re-predicted; no equations reduce to self-definition; no load-bearing self-citation chain is invoked to justify the central claim. The reported functional dependence is therefore an output of the calculations rather than an input by construction, rendering the derivation self-contained.
Axiom & Free-Parameter Ledger
axioms (1)
- domain assumption Electron-positron correlation can be approximated by semi-local or weighted-density functionals within a DFT framework
Lean theorems connected to this paper
-
IndisputableMonolith/Cost/FunctionalEquation.leanwashburn_uniqueness_aczel unclear?
unclearRelation between the paper passage and the cited Recognition theorem.
We explored several approximations: two LDA based ones, by Boronski and Nieminen (BN-LDA [27]) and Drummond et al. (D-LDA [38]), three GGA based (B95-GGA ... K14-GGA ... B15-GGA ...), and the non-local weighted density approximation (WDA)
-
IndisputableMonolith/Foundation/AlexanderDuality.leanalexander_duality_circle_linking unclear?
unclearRelation between the paper passage and the cited Recognition theorem.
We show also the relationship between the size of the voids, through Voronoi volumes, and the calculated lifetimes.
What do these tags mean?
- matches
- The paper's claim is directly supported by a theorem in the formal canon.
- supports
- The theorem supports part of the paper's argument, but the paper may add assumptions or extra steps.
- extends
- The paper goes beyond the formal theorem; the theorem is a base layer rather than the whole result.
- uses
- The paper appears to rely on the theorem as machinery.
- contradicts
- The paper's claim conflicts with a theorem or certificate in the canon.
- unclear
- Pith found a possible connection, but the passage is too broad, indirect, or ambiguous to say the theorem truly supports the claim.
Reference graph
Works this paper leans on
-
[1]
Positron lifetimes in positrons traps in MAPbI 3: vacancies in the tetragonal phase We calculated the positron lifetime at 0K for tetragonal supercells of various sizes containing a vacancy. As seen in Table II the lifetime of the lead vacancy seems to be relatively well converged already with a supercell containing 16 fu, while the lifetime of the methyl...
-
[2]
Positron lifetimes in positrons traps in MAPbI 3: vacancies in the polymorphous cubic phase Polymorphism in the cubic phase of MAPbI 3 manifests itself in a variety of local environments for point defects and, thus, also for the positrons trapped in them. To the best of our knowledge, the distribution of formation energies of defects induced by polymorphi...
work page 2025
-
[3]
https://www.perovskite-info.com/, accessed January 2025
work page 2025
-
[4]
He Dong and Chenxin Ran and Weiyin Gaoand Mingjie Li and Yingdong Xia and Wei Huang, eLight 3, 3 (2023)
work page 2023
-
[5]
Nalwa, Communications Materials4, 52 (2023)
Saurabh Srivastava and Sudhir Ranjan and Lokesh Yadav and Tejasvini Sharma and Shivani Choudhary and Daksh Agarwal and Anand Singh and Soumitra Satapathi and Raju Kumar Gupta and Ashish Garg and Kanwar S. Nalwa, Communications Materials4, 52 (2023)
work page 2023
-
[6]
M. Eldrup and B. N. Singh, Journal of Nuclear Materials323, 346 (2003), proceedings of the Second IEA Fusion Materials Agreement Workshop on Modeling and Experimental Validation
work page 2003
-
[7]
F. A. Selim, Materials Characterization174, 110952 (2021)
work page 2021
-
[8]
I. Makkonen and F. Tuomisto, Journal of Applied Physics135, 040901 (2024), https://pubs.aip.org/aip/jap/article-pdf/doi/10.1063/5.0180024/19977875/040901 1 5.0180024.pdf
-
[9]
Z. Guo, M. Yuan, G. Chen, F. Liu, R. Lu, and W.-J. Yin, Advanced Science11, 2305799 (2024), https://advanced.onlinelibrary.wiley.com/doi/pdf/10.1002/advs.202305799
-
[10]
J. Dryzek and D. Singleton, Nuclear Instruments and Methods in Physics Research Section B: Beam Interactions with Materials and Atoms252, 197 (2006)
work page 2006
-
[11]
R. Krause-Rehberg and H. S. Leipner,Positron Annihilation in Semiconductors: Defect Studies, Springer Series in Solid-State Sciences (Springer, 1999)
work page 1999
-
[12]
J. Dhar, S. Sil, A. Dey, D. Sanyal, and P. P. Ray, The Journal of Physical Chemistry C121, 5515 (2017), https://doi.org/10.1021/acs.jpcc.7b01047
-
[13]
Joydeep Dhar and Sayantan Sil and Arka Dey and Partha Pratim Ray and Dirtha Sanyal, J. Phys. Chem. Lett. (1745)
-
[14]
J. Dhar, S. Sil, N. A. Hoque, A. Dey, S. Das, P. P. Ray, and D. Sanyal, ChemistrySelect3, 5304 (2018), https://chemistry-europe.onlinelibrary.wiley.com/doi/pdf/10.1002/slct.201801034
-
[15]
D. J. Keeble, J. Wiktor, S. K. Pathak, L. J. Phillips, M. Dickmann, K. Durose, H. J. Snaith, and W. Egger, Nature Communications12, 5566 (2021)
work page 2021
-
[16]
Y. Cai, D. Begin, C. Lefevre, C. Sidhoum, E. Elkaim, P. Boulet, P. Desgardin, M.-F. Barthe, R. Helm, W. Egger, M. Butterling, A. Wagner, V. Papaefthimiou, S. Zafeiratos, D. Cianferani, L. Mager, O. Ersen, C. Corbel, C. Sanchez, and S. Begin-Colin, Small Structuresn/a, 2500066 (2025), https://onlinelibrary.wiley.com/doi/pdf/10.1002/sstr.202500066
-
[17]
P. Aversa, R. Helm, H. Jun, Y. Cai, H. Nahdi, P. Desgardin, D. Tondelier, J. Bour´ ee, S. Begin, F. Oswald, Y. Bonnassieux, T. Fischer, J. Mitteneder, M. Liedke, K. Madaan, G. Roma, P. Pochet, J. Liszkay, M. Butterling, M. Dickmann, A. Wagner, M. Barthe, W. Egger, B. Geffroy, and C. Cor- bel, “Evidence of Different Positron Annihilation Quantum Statesin M...
- [18]
-
[19]
A. Musiienko, J. ˇC´ ıˇ zek, H. Elhadidy, P. Praus, K. Higgins, B. Dryzhakov, A. Kanak, F. Sureau, J. Pipek, E. Belas, M. Betuˇ siak, M. Brynza, E. Lukosi, B. Hu, and M. Ahmadi, Chemistry of Materials34, 297 (2022), https://doi.org/10.1021/acs.chemmater.1c03540
-
[20]
J. A. Schmidt, S. Tinte, S. Dalosto, D. Chrastina, D. R. Ceratti, and R. Ferragut, The Journal of Physical Chemistry C129, 7207 (2025), https://doi.org/10.1021/acs.jpcc.5c01174
-
[21]
Liedke and Andreas Wagner and Yifan Dong and Matthew C
Zhenyi Ni and Liang Zhao and Zhifang Shi and Aryaveer Singh and Julia Wiktor and Maciej O. Liedke and Andreas Wagner and Yifan Dong and Matthew C. Beard and David J. Keeble and Jinsong Huang, Adv. Mater.36, 2406193 (2024)
work page 2024
-
[22]
H. Nahdi, R. Helm, J. Ihrenberger, T. Lemercier, N. Heshmati, P. Desgardin, D. Tondelier, J. Bour´ ee, E. G. d’Aillon, F. Zaccaro, D. Ceratti, F. Oswald, Y. Bonnassieux, T. Fischer, S. Mathur, J. Mitteneder, M. Liedke, K. Madaan, G. Roma, P. Pochet, J. Liszkay, M. Butterling, M. Dickmann, A. Wagner, M. Barthe, W. Egger, and C. Corbel, “Positron Lifetime i...
-
[23]
M. J. Puska and R. M. Nieminen, Rev. Mod. Phys.66, 841 (1994)
work page 1994
-
[24]
Gonze andet al., Computer Physics Communications248, 107042 (2020)
X. Gonze andet al., Computer Physics Communications248, 107042 (2020)
work page 2020
- [25]
-
[26]
R. P. Gupta and R. W. Siegel, Phys. Rev. B22, 4572 (1980)
work page 1980
-
[27]
M. J. Puska and R. M. Nieminen, Journal of Physics F: Metal Physics13, 333 (1983)
work page 1983
-
[28]
M. J. Puska and C. Corbel, Phys. Rev. B38, 9874 (1988)
work page 1988
- [29]
-
[30]
B. Barbiellini, M. J. Puska, T. Torsti, and R. M. Nieminen, Phys. Rev. B51, 7341 (1995)
work page 1995
-
[31]
B. Barbiellini and J. Kuriplach, Phys. Rev. Lett.114, 147401 (2015)
work page 2015
-
[32]
K. A. Simula, J. E. Muff, I. Makkonen, and N. D. Drummond, Phys. Rev. Lett.129, 166403 (2022)
work page 2022
-
[33]
W. Shi, V. Callewaert, B. Barbiellini, R. Saniz, M. Butterling, W. Egger, M. Dickmann, C. Hugen- schmidt, B. Shakeri, R. W. Meulenberg, E. Br¨ uck, B. Partoens, A. Bansil, and S. W. H. Eijt, Phys. Rev. Lett.121, 057401 (2018)
work page 2018
-
[34]
V. Callewaert, R. Saniz, B. Barbiellini, A. Bansil, and B. Partoens, Phys. Rev. B96, 085135 (2017)
work page 2017
-
[35]
P. S. Whitfield, N. Herron, W. E. Guise, K. Page, Y. Q. Cheng, I. Milas, and M. K. Crawford, Scientific Reports6, 35685 (2016)
work page 2016
-
[36]
Giannozzi andet al., Journal of Physics: Condensed Matter21, 395502 (2009)
P. Giannozzi andet al., Journal of Physics: Condensed Matter21, 395502 (2009)
work page 2009
-
[37]
Giannozzi andet al., Journal of Physics: Condensed Matter29, 465901 (2017)
P. Giannozzi andet al., Journal of Physics: Condensed Matter29, 465901 (2017). 27
work page 2017
-
[38]
Giannozzi Paolo and Baseggio Oscar and Bonf` a Pietro and Brunato Davide and Car Roberto and Carnimeo Ivan and Cavazzoni Carlo and de Gironcoli Stefano and Delugas Pietro and Ferrari Ruffino Fabrizio and Ferretti Andrea and Marzari Nicola and Timrov Iurii and Urru Andrea and Baroni Stefano, The Journal of Chemical Physics152, 154105 (2020), https://doi.or...
-
[39]
T. Torsti and T. Eirola and J. Enkovaara and T. Hakala and P. Havu and V. Havu and T. H¨ oyn¨ al¨ anmaa and J. Ignatius and M. Lyly and I. Makkonen and T. T. Rantala and J. Ruokolainen and K. Ruot- salainen and E. R¨ as¨ anen and H. Saarikoski and M. J. Puska, physica status solidi (b)243, 1016 (2006), https://onlinelibrary.wiley.com/doi/pdf/10.1002/pssb....
-
[40]
N. D. Drummond and P. L´ opez R´ ıos and R. J. Needs and C. J. Pickard, Phys. Rev. Lett.107, 207402 (2011)
work page 2011
- [41]
-
[42]
Klimeˇ s, D. R. Bowler, and A. Michaelides, Phys. Rev. B83, 195131 (2011)
work page 2011
-
[43]
A. Marronnier, H. Lee, B. Geffroy, J. Even, Y. Bonnassieux, and G. Roma, The Journal of Physical Chemistry Letters8, 2659 (2017), http://dx.doi.org/10.1021/acs.jpclett.7b00807
-
[44]
A. Marronnier, G. Roma, S. Boyer-Richard, L. Pedesseau, J.-M. Jancu, Y. Bonnassieux, C. Katan, C. C. Stoumpos, M. G. Kanatzidis, and J. Even, ACS Nano12, 3477 (2018), https://doi.org/10.1021/acsnano.8b00267
- [45]
- [46]
-
[47]
K. Madaan,Phases and vacancy defects in methylammonium lead iodide perovskite : an ab initio study, Ph.D. thesis, Universit´ e Paris-Saclay (2023)
work page 2023
-
[48]
X.-G. Zhao, G. M. Dalpian, Z. Wang, and A. Zunger, Phys. Rev. B101, 155137 (2020)
work page 2020
- [49]
-
[50]
M. Zacharias, G. Volonakis, F. Giustino, and J. Even, Phys. Rev. B108, 035155 (2023)
work page 2023
-
[51]
M. Zacharias, G. Volonakis, F. Giustino, and J. Even, npj Computational Materials9, 153 (2023), https://www.nature.com/articles/s41524-023-01089-2.pdf
work page 2023
-
[52]
Wan-Jian Yin and Tingting Shi and Yanfa Yan, Appl. Phys. Lett. (2014)
work page 2014
-
[53]
D. Meggiolaro and S. G. Motti and E. Mosconi and A. J. Barker and J. Ball and A. A. R. Perini and F. Deschler and A. Petrozza and F. De Angelis, Energy Environ . Sci.11, 702 (2018)
work page 2018
-
[54]
A. Baldereschi, S. Baroni, and R. Resta, Phys. Rev. Lett.61, 734 (1988)
work page 1988
-
[55]
See Supplemental Material
-
[56]
V. Ramasubramani, B. D. Dice, E. S. Harper, M. P. Spellings, J. A. Anderson, and S. C. Glotzer, Computer Physics Communications254, 107275 (2020)
work page 2020
-
[57]
A. N. Beecher, O. E. Semonin, J. M. Skelton, J. M. Frost, M. W. Terban, H. Zhai, A. Alatas, J. S. Owen, A. Walsh, and S. J. L. Billinge, ACS Energy Letters1, 880 (2016), https://doi.org/10.1021/acsenergylett.6b00381. 28
-
[58]
L. Qiao, A. S. Vasenko, E. V. Chulkov, and R. Long, The Journal of Physical Chemistry Letters16, 215 (2025), pMID: 39714949, https://doi.org/10.1021/acs.jpclett.4c03313
-
[59]
S. J. Tao, The Journal of Chemical Physics56, 5499 (1972), https://pubs.aip.org/aip/jcp/article- pdf/56/11/5499/18879615/5499 1 online.pdf
work page 1972
- [60]
-
[61]
A. M. Frolov, Phys. Rev. A60, 2834 (1999)
work page 1999
-
[62]
S. M. Fleischer, K. Degreif, G. Gwinner, M. Lestinsky, V. Liechtenstein, F. Plenge, and D. Schwalm, Phys. rev. Lett.96, 063401 (2006)
work page 2006
-
[63]
H. Ceeh, C. Hugenschmidt, K. Schreckenbach, S. A. G¨ artner, P. G. Thirolf, S. M. Fleischer, and D. Schwalm, Phys. Rev. A84, 062508 (2011)
work page 2011
- [64]
-
[65]
Gilgien, Lise and Galli, Giulia and Gygi, Fran¸ cois and Car, Roberto, Phys. Rev. Lett.72, 3214 (1994)
work page 1994
-
[66]
M. J. Puska and A. P. Seitsonen and R. M. Nieminen, Phys. Rev. B (1995)
work page 1995
- [67]
discussion (0)
Sign in with ORCID, Apple, or X to comment. Anyone can read and Pith papers without signing in.