Structural Control of Photoconductivity in a Flexible Titanium‐Organic Framework

C Clara Chinchilla‐Garzón (Instituto de Ciencia Molecular (ICMol) Universitat de València Catedrático José Beltrán‐2 Paterna 46980 Spain) M Marta Galbiati (Instituto de Ciencia Molecular (ICMol) Universitat de València Catedrático José Beltrán 2 Paterna 46980 Spain) A Alechania Misturini (Functional Inorganic Materials Team, Instituto de Ciencia Molecular (ICMol)) P Pol Gimeno‐Fonquernie (Instituto de Ciencia Molecular (ICMol) Universitat de València Catedrático José Beltrán‐2 Paterna 46980 Spain) N Neyvis Almora‐Barrios (Instituto de Ciencia Molecular (ICMol) Universitat de València Catedrático José Beltrán‐2 Paterna 46980 Spain) N Natalia M. Padial (Functional Inorganic Materials Team, Instituto de Ciencia Molecular (ICMol)) C Carlos Martí‐Gastaldo (Instituto de Ciencia Molecular Universidad de Valencia Paterna 46980 Spain)

Abstract

Abstract The soft nature of Metal‐Organic Frameworks (MOFs) sets them apart from other non‐synthetic porous materials. Their flexibility allows the framework components to rearrange in response to environmental changes, leading to different states and properties. The work extends this concept to titanium frameworks, demonstrating control over charge transport in porous molecular crystals. MUV‐35 is a two‐fold catenated framework composed of heterometallic TiMn 2 trimers and electron donor 4,4′,4″‐(benzo[1,2‐ b :3,4‐ b ’:5,6‐ b ″]trithiophene‐2,5,8‐triyl)tribenzoic acid (H 3 BTTTB) linkers, forming a rare sit‐c net topology that can fold to reduce its volume by ≈40% through a single‐crystal transformation controlled by linker conformation in open, intermediate, and closed states. This process, driven by a free energy difference of ≈300 kJ mol −1 , originates from the formation of a continuous network of non‐covalent interactions that force the spontaneous loss of the solvent in the pores of the framework to establish charge transport pathways that afford photocurrents of 2.5 × 10 −3  S m −1 under visible light for an ON/OFF ratio (∆R) of four orders of magnitude. This photoconductivity rivals the best conductivity values described for though‐transport conductive MOFs while maintaining a porosity of ≈1.000 m 2  g −1 .

Article Details

Volume / Issue Vol. 37, Issue 52
Published December 01, 2025
ISSN 0935-9648
Publisher Unknown Publisher

Journal Info

Advanced Materials

Unknown Publisher

ISSN: 0935-9648 Physical Sciences

Authors (7)

C

Clara Chinchilla‐Garzón

Instituto de Ciencia Molecular (ICMol) Universitat de València Catedrático José Beltrán‐2 Paterna 46980 Spain

M

Marta Galbiati

Instituto de Ciencia Molecular (ICMol) Universitat de València Catedrático José Beltrán 2 Paterna 46980 Spain

A

Alechania Misturini

Functional Inorganic Materials Team, Instituto de Ciencia Molecular (ICMol)

P

Pol Gimeno‐Fonquernie

Instituto de Ciencia Molecular (ICMol) Universitat de València Catedrático José Beltrán‐2 Paterna 46980 Spain

N

Neyvis Almora‐Barrios

Instituto de Ciencia Molecular (ICMol) Universitat de València Catedrático José Beltrán‐2 Paterna 46980 Spain

N

Natalia M. Padial

Functional Inorganic Materials Team, Instituto de Ciencia Molecular (ICMol)

C

Carlos Martí‐Gastaldo

Instituto de Ciencia Molecular Universidad de Valencia Paterna 46980 Spain