Ultra-compact graphene plasmonic filter integrated in a waveguide<xref rid="cpb_27_9_094101fn1" ref-type="fn">*</xref><fn id="cpb_27_9_094101fn1"><label>*</label><p>Project supported by the National Basic Key Research Program of China (Grant No. 2015CB932400), the National Key Research and Development Program of China (Grant No. 2016YFA0201600), the National Natural Science Foundation of China (Grant Nos. 51372045, 11504063, and 11674073), the Key Program of the Bureau of Frontier Sciences and Education, Chinese Academy of Sciences (Grant No. QYZDBSSW- SLH021), and the Science and Technology Projects of Beijing City, China (Grant No. Z161100002116016).</p></fn>

Ultra-compact graphene plasmonic filter integrated in a waveguide**

Project supported by the National Basic Key Research Program of China (Grant No. 2015CB932400), the National Key Research and Development Program of China (Grant No. 2016YFA0201600), the National Natural Science Foundation of China (Grant Nos. 51372045, 11504063, and 11674073), the Key Program of the Bureau of Frontier Sciences and Education, Chinese Academy of Sciences (Grant No. QYZDBSSW- SLH021), and the Science and Technology Projects of Beijing City, China (Grant No. Z161100002116016).

Liao Baoxin^{1, 2}, Guo Xiangdong^{1, 2}, Hu Hai^{1, 2}, Liu Ning^{1, 2}, Chen Ke^{1, 2}, Yang Xiaoxia^{1, 2, ‡}, Dai Qing^{1, 2, †}

(color online) (a) Transmission spectra of GPs waveguide filter with different scattering rates (Γ) of graphene. (b) Height difference (orange), cavity quality factor (blue), and coupling quality factor (green) as a function of scattering rate for peak 1 in panel (a). (c)–(e) Height difference as a function of Fermi level, length of cavity, and width of cavity, respectively, for peak 1. The values are extracted from Figs. 4(a), 3(a), and 3(c), respectively.