The 77th JSAP Autumn Meeting, 2016

Presentation information

Oral presentation

4 JSAP-OSA Joint Symposia 2016 » 4.6 Nanocarbon and 2D Materials

[13p-A37-1~13] 4.6 Nanocarbon and 2D Materials

Tue. Sep 13, 2016 1:15 PM - 5:45 PM A37 (306-307)

Kazunari Matsuda(Kyoto Univ.), Yuhei Miyauchi(Kyoto Univ.)

3:15 PM - 3:30 PM

[13p-A37-7] Photoluminescence Quantum Yield and Effective Exciton Radiative Lifetime in Monolayer Transition Metal Dichalcogenides

〇(D)Nur Baizura Mohamed1, Feijiu Wang1, Sandhaya Koirala1, Hong En Lim1, Shinichiro Mouri1, Yuhei Miyauchi1, Kazunari Matsuda1 (1.Inst. of Advanced Energy, Kyoto Univ.)

Keywords:photoluminescence quantum yield, radiative lifetime, transition metal dichalcogenides

The discovery of graphene and its fascinating properties [1] motivates new research fields in two-dimensional (2D) atomically thin-layered materials. The semiconductor transition metal dichalcogenides (TMDs) with chemical formula of MX2, (M = Mo, W; X = S, Se, Te) have attracted great research interest due to its intriguing properties [2,3]. It is very crucial to know the photoluminescence (PL) quantum yield and exciton radiative lifetime of this material in both viewpoint of research and opto-electronic device applications [4].

In this study, monolayer tungsten diselenides (1L-WSe2) from mechanically exfoliation technique was experimentally evaluated its PL quantum yield, FPL and effective radiative lifetime, trad at room temperature. Figure 1(a) show that PL spectrum of 1L-WSe2 at power density of 1 kW/cm2 is mainly dominates by exciton, while the inset figure shows the integrated PL with varying power density in the linear region. In addition, PL quantum yield of 0.2 % was estimated using relative quantum yield method using highly fluorescent standard dye [5] as reference. We also conducted time-resolved PL spectroscopy measurement to measure the PL decay time of 1L-WSe2 at room temperature. The exciton effective radiative lifetime of 280 ns was determined using the PL quantum yield and PL decay time, tPL of ~ 560 ps (Figure 1(b)). This experimental result with considerably long exciton effective radiative lifetime compared to 5 ns of theoretical predicted value at room temperature [6], is suggested due to existence of the dark states. Our finding will provide some information for future development of TMDs application.