共 7 条
Investigating the effect of H+-ion irradiation on layered α-MoO3 flakes by defect engineering
被引:3
|作者:
Kumar, Ravindra
[1
,2
,3
]
Mishra, Vikash
[1
,2
]
Dixit, Tejendra
[4
]
Sarangi, S. N.
[5
]
Samal, D.
[5
]
Miryala, Muralidhar
[6
]
Nayak, Pramoda K.
[3
,7
]
Rao, M. S. Ramachandra
[1
,2
]
机构:
[1] Indian Inst Technol Madras, Quantum Ctr Excellence Diamond & Emergent Mat QuC, Nano Funct Mat Technol Ctr, Dept Phys, Chennai 600036, India
[2] Indian Inst Technol Madras, Mat Sci Res Ctr, Chennai 600036, India
[3] Indian Inst Technol Madras, Dept Phys, Mat Res & Innovat Grp 2D, Chennai 600036, India
[4] Indian Inst Informat Technol Design & Mfg, Dept Elect & Commun Engn, Optoelect & Quantum Devices Grp, Chennai 600127, India
[5] Inst Phys, Sachivalaya Marg, Bhubaneswar 751005, India
[6] Shibaura Inst Technol, Grad Sch Sci & Engn, Superconducting Mat Lab, 3-7-5 Toyosu,Koto Ku, Tokyo 1358546, Japan
[7] Jain Deemed Univ, Ctr Nano & Mat Sci, Jain Global Campus, Bangalore 562112, Karnataka, India
关键词:
RAMAN-SPECTROSCOPY;
MOLYBDENUM OXIDES;
THIN-FILMS;
MOO3;
ELECTRONICS;
STATES;
D O I:
10.1063/5.0166452
中图分类号:
O59 [应用物理学];
学科分类号:
摘要:
Ion irradiation is a versatile and convenient tool for modifying the optical, electrical, and catalytic properties of two-dimensional (2D) materials through controlled induction of impurities and defects. The behavior of 2D materials under ion irradiation is interesting, which needs to be explored in the contest of their optoelectronic applications. In the present work, we have reported the effect of H & thorn;-ion irradiation on layered a-MoO3 flakes by defect engineering. Initially, the a-MoO3 crystals were synthesized using the physical vapor deposition technique followed by mechanical exfoliation of an as-grown crystal to obtain a-MoO3 flakes of different thicknesses. Then, the exfoliated flakes were exposed to H & thorn;-ion/proton irradiation with a fluence of 1 10(16) ions/cm(2) using a 30 keV source. After irradiation, new photoluminescence (PL) emission peaks were observed at different positions in the range of 2.4-1.9 eV, which was found to be absent in pristine flakes. Raman studies revealed non-uniform oxygen vacancy distribution in H & thorn;-ion irradiated a-MoO3 flakes, which affected the PL peak positions. Additionally, first-principle calculations and Bader charge analysis were performed to identify the origin of the new PL peaks. Our findings indicate that oxygen vacancies positioning at different locations of the a-MoO3 lead to the emergence of new absorption peaks within the range of 2.2-1.25 eV, which is consistent with our experimental findings. The present study gives insight into exploring the use of ionirradiated a-MoO3 in optoelectronics applications with tunable properties.
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