April 22 - 26, 2024
Seattle, Washington
May 7 - 9, 2024 (Virtual)
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2024 MRS Spring Meeting & Exhibit
SF03.04.09

Tailoring The Optical and Electrical Properties of MoTe2 via Electrochemical Intercalation of Lithium Ions

When and Where

Apr 24, 2024
11:00am - 11:15am
Room 339, Level 3, Summit

Presenter(s)

Co-Author(s)

Alyssa Shiyu Xu1

Cornell University1

Abstract

Alyssa Shiyu Xu1

Cornell University1
Intercalation of lithium (Li) ions is one of the most effective methods to realize structural transformation and to tune the optical and electrical properties of two-dimensional transition metal dichalcogenides (2D TMDCs). Numerous studies have focused on the phase transition from semiconducting 2H phase to metallic 1T (or 1T’) phase in MoS<sub>2</sub> and WS<sub>2</sub> induced by the intercalation of Li ions. However, few reports explore the effects of Li intercalation in other TMDCs, such as Mo- or W- ditellurides. In particular, novel electronic and energy devices can be achieved using the Li-intercalated MoTe<sub>2</sub> with its intriguing electrical, topological and catalytic properties.<br/>Here, we report electrochemical Li intercalation into 1T’- MoTe<sub>2</sub> flakes. The 1T’ phase is stable down to 0.9 V of the applied electrochemical voltage, and two new phases are observed at 0.7 V (phase I) and 0.4 V (phase II), respectively. The lightly Li-intercalated phase I is evidenced by the disappearance of the A<sub>g</sub> peak at ~77.7 cm<sup>-1</sup> and the appearance of a peak at ~86.9 cm<sup>-1</sup> in Raman spectroscopy and a 10% increase of electrical resistance in two-terminal measurements. For the heavily Li-intercalated phase II, we observe a lattice expansion of ~7% in (001) direction in single-crystal X-ray diffraction, the emergence of new Raman peaks at 16.8 cm<sup>-1</sup>, 109.0 cm<sup>-1</sup> and 132.8 cm<sup>-1</sup> in Raman spectroscopy and increase of electrical resistance for over 8 folds<i>. In situ</i> Hall effect measurements confirm the decrease in conductivity, which also decreases with decreasing temperature for the phase II, suggesting a semiconducting phase. The Hall carrier density falls from 10<sup>15</sup> cm<sup>-2</sup> in pristine 1T’-MoTe<sub>2</sub> to 10<sup>14</sup> cm<sup>-2</sup> in phase I and to 10<sup>12</sup> cm<sup>-2</sup> in phase II. Our results highlight the importance of electrochemical intercalation of Li ions as a powerful tool to manipulate phase stability and electron density of 2D TMDCs.

Keywords

2D materials | in situ | Raman spectroscopy

Symposium Organizers

Iwnetim Abate, Stanford University
Judy Cha, Cornell University
Yiyang Li, University of Michigan
Jennifer Rupp, TU Munich

Symposium Support

Bronze
Journal of Materials Chemistry A

Session Chairs

Iwnetim Abate
Judy Cha

In this Session