Interface-TailoredSecondary Excitation and UltrafastCharge/Energy Transfer in Ti<sub>3</sub>C<sub>2</sub>T<sub><i>x</i></sub>‑MoS<sub>2</sub> Heterostructure Films

Charge/energy separation across interfaces of plasmonic materials is vital for minimizing plasmonic losses and enhancing their performance in photochemical and optoelectronic applications. While heterostructures combining plasmonic two-dimensional transition metal carbides/nitrides (MXenes) and semiconducting transition metal dichalcogenides (TMDs) hold significant potential, the mechanisms governing plasmon-induced carrier dynamics at these interfaces remain elusive. Here, we uncover a distinctive secondary excitation phenomenon and an ultrafast charge/energy transfer process in heterostructure films composed of macro-scale Ti<sub>3</sub>C<sub>2</sub>T<sub><i>x</i></sub> and MoS<sub>2</sub> films. Using Rayleigh–Bénard convection and Marangoni effect-induced self-assembly, we fabricate large-scale (square centimeters) Ti<sub>3</sub>C<sub>2</sub>T<sub><i>x</i></sub> and MoS<sub>2</sub> films composed of edge-connected monolayer nanoflakes. These films are flexibly stacked in a controlled sequence to form macroscopic heterostructures, enabling the investigation and manipulation of excited-state dynamics using transient absorption and optical pump-terahertz probe spectroscopy. In the Ti<sub>3</sub>C<sub>2</sub>T<sub><i>x</i></sub>-MoS<sub>2</sub> heterostructure, we observe a secondary excitation in MoS<sub>2</sub> driven by the surface plasmon resonance of Ti<sub>3</sub>C<sub>2</sub>T<sub><i>x</i></sub>. This phenomenon, with a characteristic rise time constant of ∼70 ps, is likely facilitated by acoustic phonon recycling across the interface. Further interfacial thermal transport engineeringachieved by tailoring the sequence and combination of interfaces in trilayer heterostructuresallows extending the characteristic time to ∼175 ps. Furthermore, we identify a sub-150 fs ultrafast charge/energy transfer process from Ti<sub>3</sub>C<sub>2</sub>T<sub><i>x</i></sub> to MoS<sub>2</sub>. The transfer efficiency is strongly dependent on the excitation photon energy, resulting in amplified photoconductivity in MoS<sub>2</sub> by up to ∼180% under 3.10 eV excitation. These insights are crucial for developing plasmonic MXene-based heterostructures, paving the way for advancements in photochemical and optoelectronic applications.

Publication Details

Journal
Figshare
Published
2025-03-07
DOI
https://doi.org/10.1021/jacs.5c01826.s001
Primary Topic
MXene and MAX Phase Materials
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article
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article

Interface-TailoredSecondary Excitation and UltrafastCharge/Energy Transfer in Ti3C2Tx‑MoS2 Heterostructure Films

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MXene and MAX Phase Materials
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Interface-TailoredSecondary Excitation and UltrafastCharge/Energy Transfer in Ti3C2Tx‑MoS2 Heterostructure Films

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Abstract

Charge/energy separation across interfaces of plasmonic materials is vital for minimizing plasmonic losses and enhancing their performance in photochemical and optoelectronic applications. While heterostructures combining plasmonic two-dimensional transition metal carbides/nitrides (MXenes) and semiconducting transition metal dichalcogenides (TMDs) hold significant potential, the mechanisms governing plasmon-induced carrier dynamics at these interfaces remain elusive. Here, we uncover a distinctive secondary excitation phenomenon and an ultrafast charge/energy transfer process in heterostructure films composed of macro-scale Ti<sub>3</sub>C<sub>2</sub>T<sub><i>x</i></sub> and MoS<sub>2</sub> films. Using Rayleigh–Bénard convection and Marangoni effect-induced self-assembly, we fabricate large-scale (square centimeters) Ti<sub>3</sub>C<sub>2</sub>T<sub><i>x</i></sub> and MoS<sub>2</sub> films composed of edge-connected monolayer nanoflakes. These films are flexibly stacked in a controlled sequence to form macroscopic heterostructures, enabling the investigation and manipulation of excited-state dynamics using transient absorption and optical pump-terahertz probe spectroscopy. In the Ti<sub>3</sub>C<sub>2</sub>T<sub><i>x</i></sub>-MoS<sub>2</sub> heterostructure, we observe a secondary excitation in MoS<sub>2</sub> driven by the surface plasmon resonance of Ti<sub>3</sub>C<sub>2</sub>T<sub><i>x</i></sub>. This phenomenon, with a characteristic rise time constant of ∼70 ps, is likely facilitated by acoustic phonon recycling across the interface. Further interfacial thermal transport engineeringachieved by tailoring the sequence and combination of interfaces in trilayer heterostructuresallows extending the characteristic time to ∼175 ps. Furthermore, we identify a sub-150 fs ultrafast charge/energy transfer process from Ti<sub>3</sub>C<sub>2</sub>T<sub><i>x</i></sub> to MoS<sub>2</sub>. The transfer efficiency is strongly dependent on the excitation photon energy, resulting in amplified photoconductivity in MoS<sub>2</sub> by up to ∼180% under 3.10 eV excitation. These insights are crucial for developing plasmonic MXene-based heterostructures, paving the way for advancements in photochemical and optoelectronic applications.

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