Facet‐Engineered Rubidium Lead Halide Nanocrystals for Pyro‐Phototronic Broadband Photodetection

D Diptam Nasipuri (School of Materials Sciences Indian Association for the Cultivation of Science Kolkata 700032 India) S Sougata Karmakar (School of Applied & Interdisciplinary Sciences Indian Association for the Cultivation of Science (IACS) Kolkata India) A Akram Hossain Sarkar (School of Physical Sciences Indian Association for the Cultivation of Science Kolkata 700032 India) N Naveen Goyal (Materials Research Centre) S Souvik Banerjee (School of Materials Sciences) R Rajdeep Das (School of Materials Sciences) N N. Ravishankar (Materials Research Centre) K K. D. M. Rao (School of Applied and Interdisciplinary Sciences Indian Association for the Cultivation of Science Kolkata 700032 India) N Narayan Pradhan (School of Materials Sciences)

Abstract

Abstract Cesium lead halide has been extensively studied as efficient materials for optoelectronic device applications. Beyond Cs(I), the exploration of other inorganic A‐site monovalent cations remains limited, though Rb(I) stands out as a potential alternative whose role in colloidal nanocrystals is largely unexplored. Here, Rb (I) is employed as an effective A‐site cation in forming monoclinic‐phase RbPb 2 Cl 5 , where Pb (II) heptahedrally coordinated. A template‐mediated cation exchange strategy is employed where 0D Rb 4 CdCl 6 used as host nanocrystals. Upon introduction of Pb (II), fast Cd to Pb ion exchange triggers and 2D RbPb 2 Cl 5 in rhombic prism, hexagonal prism or hexagonal platelet‐shaped nanocrystals are formed depending on the reaction conditions. Further to explore the optoelectronic properties, photo response measurements are carried out which exhibit significant pyro‐photocurrent response from these nanocrystals even under ultra‐low‐intensity light illumination (7 nW cm −2 ) across ultraviolet (UV) to near‐infrared (NIR) spectral range. Despite its centrosymmetric structure, RbPb 2 Cl 5 generates pyro‐photocurrent due to surface halide deficiencies, supported by DFT which shows surface polarization of |𝝙P| = 0.173 C m −2 . These findings highlight the pivotal role of Rb (I) in stabilizing these nanostructures and open a new avenue for their application in advanced optoelectronic devices.

Article Details

Volume / Issue Vol. 38, Issue 7
Published February 01, 2026
ISSN 0935-9648
Publisher Unknown Publisher

Journal Info

Advanced Materials

Unknown Publisher

ISSN: 0935-9648 Physical Sciences

Authors (9)

D

Diptam Nasipuri

School of Materials Sciences Indian Association for the Cultivation of Science Kolkata 700032 India

S

Sougata Karmakar

School of Applied & Interdisciplinary Sciences Indian Association for the Cultivation of Science (IACS) Kolkata India

A

Akram Hossain Sarkar

School of Physical Sciences Indian Association for the Cultivation of Science Kolkata 700032 India

N

Naveen Goyal

Materials Research Centre

S

Souvik Banerjee

School of Materials Sciences

R

Rajdeep Das

School of Materials Sciences

N

N. Ravishankar

Materials Research Centre

K

K. D. M. Rao

School of Applied and Interdisciplinary Sciences Indian Association for the Cultivation of Science Kolkata 700032 India

N

Narayan Pradhan

School of Materials Sciences