Perovskites in the Light of X-Rays at the Home Laboratory
Davide Altamura a, Aurora Rizzo b, Rosanna Mastria b, Lucia Mercurio c, Giuseppe Conti b, Cinzia Giannini a
a Istituto di Cristallografia, Consiglio Nazionale delle Ricerche, via Amendola 122/O, 70126 Bari, Italy
b CNR NANOTEC–Istituto di Nanotecnologia, c/o Campus Ecotekne, Via Monteroni, Lecce, 73100 Italy
c Dipartimento di Matematica e Fisica “E. De Giorgi”, Università del Salento, Campus Ecotekne, via Arnesano, 73100 – Lecce, Italy
Proceedings of MATSUS Fall 2026 Conference (MATSUSFall26)
A6 Halide Perovskites Beyond the Ideal Crystal: Chemistry, Interfaces, and Functional Heterostructures
Palma, Spain, 2026 October 26th - 30th
Organizers: Ahmed Abdelhady and Anna Moliterni
Invited Speaker, Davide Altamura, presentation 266
Publication date: 22nd July 2026

Perovskites are highly versatile and promising materials for energy and sensing applications, and beyond. They are often referred to as “chameleon materials” as their properties can be tailored via compositional sub­stitution in the ABO₃ or ABX₃ structure [1]. Due to their potential in an extremely wide range of applications, from hydrogen or energy storage, in particular for lithium- and sodium-ion batteries, to catalysis, solar cells, sensors, thermochromic [2] and optoelectronic devices for displays, LEDs and radiation detection, perovskites are also synthesized in several forms, from single bulk crystals to polycrystalline films, dispersed and assembled nanocrystals, down to quantum dots, also with different structural dimensionality [3-7]. By scaling crystal size down to the nano-range, unique size-dependent properties and much larger surface-to-volume ratios arise, with consequently improved specific performances. Structure stability is a key point for perovskite design, also requiring careful optimization of microstructural and morphological parameters; low structural dimensionality e.g. can lead to improved stability as well, along with device flexibility. As a result, research on perovskite materials is a hot current topic and suitable characterization techniques and approaches are needed to assess structure-property relationships, particularly concerning nanostructures, taking into account the key constraint of rapid screening and short path from preparation to characterization laboratories before material degradation. Micro-diffraction, in particular for single crystal investigation, is typically available at synchrotron beamlines and is needful for structural studies whenever large crystals are not available; on the other hand, high intensity  X-rays with short-wavelength available at synchrotron beamlines can be necessary to study e.g. large perovskite crystals including heavy atoms, such as Pb, causing significant X-ray absorption. Advanced X-ray Scattering techniques in the small and wide angle ranges (SAXS and WAXS) are nowadays available in specialized laboratories thanks to high brilliance micro-sources and high-performance detectors (https://www.ic.cnr.it/laboratorio/xmi-lb/; https://www.itaca-sb.it/biosaxs/). Several experimental strategies are exploited, including Scanning Microscopy with scattering/absorption contrast, or Grazing Incidence geometry (GISAXS/GIWAXS), to address a large variety of studies requiring multiscale structural characterization. Representative case studies relevant to halide perovskite characterization will be shown, giving an insight into the effectiveness of state-of-the-art laboratory facilities combined with in-house developed software tools [8], as ready-to-use screening methods for self-consistent investigations as well as for preliminary tests to design further in-situ and operando experiments at large-scale facilities.

This work is supported by the Cooperation Program Italy (MUR) - Japan (MINISTRY OF EDUCATION, CULTURE, SPORTS, SCIENCE AND TECHNOLOGY) IN THE FIELDS OF SCIENTIFIC AND TECHNOLOGICAL RESEARCH (CUP B87G24000770001), MINISTRY DECREE N. 1096 of 25-07-2024 - FOE 2024, DFM.AD003.617.001, and by PRIN 2022 PNRR “Metal hAlide perovSkiTE single crystals for solaR cells (MASTER)” (CUP B53D23028740001).

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