Photoluminescence (PL) in the near infrared (NIR) region is applicable to bioimaging and telecommunication devices. Single-walled carbon nanotubes (SWNTs) with semiconducting features show NIR PL whose properties are governed by photogenerated excitons in the one-dimensional nanostructures. Defect doping to SWNTs is gathering great attentions due to enhance the contribution of the excitons to PL. The doped sites work as emissive sites with narrower bandgaps and exciton trapping features. As a result, additional PL (E 11*) with red-shifted wavelengths and enhanced quantum yields newly appears compared to original PL (E 11) of pristine SWNTs.[1-9]Local chemical modification for the defect creation achieves molecular functionalization of the defect-doped sites of the tubes, providing locally functionalized SWNTs (lf-SWNTs). They are found to show PL modulation based on the functionalized molecules. Here, we report bis-aryl functionalization for proximal defect doping of lf-SWNTs, in which molecular structure effects of bis-aryl diazonium modifiers and microenvironmental effects of the doped sites are discussed.Bis-arydiazonium salts (bAs) that had two reactive aryldiazonium groups connected with a methylene linker were synthesized and reacted with solubilized SWNTs for local functionalization. For PL wavelength modulation, the linker effects were examined by changing the connected positions on the aryl groups (pbAs for para and mbAs for meta) and the length of methylene chains.[5,8] In PL spectra of the synthesized lf-SWNTs (lf-SWNTs-pbA and lf-SWNTs-mbA), peaks appearing over 1200 nm (E 11 2*) changed sensitively depending on the chemical structures of bAs. In addition, the E 11 2* PL showed unique wavelength shifting behaviors by microenvironment changes using various organic solvents, which was different from those of E 11 PL and E 11* PL.[9]Thus, bis-aryl functionalization in lf-SWNTs creates the doped sites whose properties are different from typical doped sites showing E 11* PL and would be useful for fundamental understanding of this material and developing modulation techniques of the longer wavelength NIR PL.[1] B. Weisman et al. Science, 330, 1656 (2010). [2] Y. Miyauchi et al. Nat. Photon., 7, 715 (2013). [3] Y. Wang et al. J. Am. Chem. Soc., 138, 6878 (2016). [4] S. Doorn et al. Nat. Photon., 11, 577 (2017). [5] T. Shiraki et al. Sci. Rep., 6, 28393 (2016). [6] Y. Maeda et al. Nanoscale, 8, 16916 (2016) [7] T. Shiraki et al. Chem. Commun., 53, 12544 (2017). [8] T. Shiraki et al. Chem. Lett., 48, 791 (2019). [9] T. Shiraki et al. Chem. Commun., 55, 3662 (2019). Figure 1