Co-reporter:Jinfeng Jia
Science Bulletin 2015 Volume 60( Issue 15) pp:1368-1369
Publication Date(Web):2015 August
DOI:10.1007/s11434-015-0853-5
Co-reporter:Lin Miao;Wenmei Ming;Fang Yang;Z. F. Wang;Y. R. Song;Alexei V. Fedorov;Qi-Kun Xue;Chao-Xing Liu;Feng Liu;Canhua Liu;Dong Qian;C. L. Gao;Fengfeng Zhu;Meixiao Wang;Z. Sun;Meng-Yu Yao
PNAS 2013 Volume 110 (Issue 8 ) pp:2758-2762
Publication Date(Web):2013-02-19
DOI:10.1073/pnas.1218104110
Topological insulators and graphene present two unique classes of materials, which are characterized by spin-polarized (helical)
and nonpolarized Dirac cone band structures, respectively. The importance of many-body interactions that renormalize the linear
bands near Dirac point in graphene has been well recognized and attracted much recent attention. However, renormalization
of the helical Dirac point has not been observed in topological insulators. Here, we report the experimental observation of
the renormalized quasiparticle spectrum with a skewed Dirac cone in a single Bi bilayer grown on Bi2Te3 substrate from angle-resolved photoemission spectroscopy. First-principles band calculations indicate that the quasiparticle
spectra are likely associated with the hybridization between the extrinsic substrate-induced Dirac states of Bi bilayer and
the intrinsic surface Dirac states of Bi2Te3 film at close energy proximity. Without such hybridization, only single-particle Dirac spectra are observed in a single Bi
bilayer grown on Bi2Se3, where the extrinsic Dirac states Bi bilayer and the intrinsic Dirac states of Bi2Se3 are well separated in energy. The possible origins of many-body interactions are discussed. Our findings provide a means
to manipulate topological surface states.
Co-reporter:Mei-Xiao Wang;Canhua Liu;Jin-Peng Xu;Fang Yang;Lin Miao;Meng-Yu Yao;C. L. Gao;Chenyi Shen;Xucun Ma;X. Chen;Zhu-An Xu;Ying Liu;Shou-Cheng Zhang;Dong Qian;Qi-Kun Xue
Science 2012 Vol 336(6077) pp:52-55
Publication Date(Web):06 Apr 2012
DOI:10.1126/science.1216466
Co-reporter:Qing Zhang, Xin-Yan Shan, Xiao Feng, Chun-Xiao Wang, Qu-Quan Wang, Jin-Feng Jia, and Qi-Kun Xue
Nano Letters 2011 Volume 11(Issue 10) pp:4270-4274
Publication Date(Web):September 6, 2011
DOI:10.1021/nl2022674
Semiconductor nanowire (NW) cavities with tailorable optical modes have been used to develop nanoscale oscillators and amplifiers in microlasers, sensors, and single photon emitters. The resonance modes of NW could be tuned by different boundary conditions. However, continuously and reversibly adjusting resonance modes and improving Q-factor of the cavity remain a great challenge. We report a method to modulate resonance modes continuously and reversibly and improve Q-factor based on surface plasmon-exciton interaction. By placing single Ag nanoparticle (NP) nearby a CdS NW, we show that the wavelength and relative intensity of the resonance modes in the NW cavity can systematically be tuned by adjusting the relative position of the Ag NP. We further demonstrate that a 56% enhancement of Q-factor and an equivalent π-phase shift of the resonance modes can be achieved when the Ag NP is located near the NW end. This hybrid cavity has potential applications in active plasmonic and photonic nanodevices.
Co-reporter:Guang Wang;Xiegang Zhu;Jing Wen;Xi Chen;Ke He;Lili Wang;Xucun Ma
Nano Research 2010 Volume 3( Issue 12) pp:874-880
Publication Date(Web):2010 December
DOI:10.1007/s12274-010-0060-2
The growth and characterization of single-crystalline thin films of topological insulators (TIs) is an important step towards their possible applications. Using in situ scanning tunneling microscopy (STM) and angle-resolved photoemission spectroscopy (ARPES), we show that moderately thick Sb2Te3 films grown layer-by-layer by molecular beam epitaxy (MBE) on Si(111) are atomically smooth, single-crystalline, and intrinsically insulating. Furthermore, these films were found to exhibit a robust TI electronic structure with their Fermi energy lying within the energy gap of the bulk that intersects only the Dirac cone of the surface states. Depositing Cs in situ moves the Fermi energy of the Sb2Te3 films without changing the electronic band structure, as predicted by theory. We found that the TI behavior is preserved in Sb2Te3 films down to five quintuple layers (QLs).