TY - JOUR
T1 - Quenching of Defect-Induced Photoluminescence in a Boron-Nitride and Carbon Hetero-nanotube
AU - Gulo, Desman Perdamaian
AU - Tuan Hung, Nguyen
AU - Chen, Wei Liang
AU - Wang, Shuhui
AU - Liu, Ming
AU - Kauppinen, Esko I.
AU - Takehara, Hikaru
AU - Taguchi, Atsushi
AU - Taniguchi, Takashi
AU - Maruyama, Shigeo
AU - Chang, Yu Ming
AU - Saito, Riichiro
AU - Liu, Hsiang Lin
N1 - Publisher Copyright:
© 2025 American Chemical Society.
PY - 2025/2/20
Y1 - 2025/2/20
N2 - Using a 266 nm laser, we simultaneously observe Raman and photoluminescence (PL) spectra of vertically aligned boron-nitride nanotubes (VA-BNNT) and single-walled carbon nanotubes (SWNT) encapsulated by boron nitride (VA-SWNT@BNNT). The larger PL intensity in VA-BNNT compared to that of the h-BN single crystal suggests that VA-BNNT contains more defect states. VA-SWNT@BNNT exhibits two multiphonon Raman peaks at 3033 and 3142 cm-1 and four PL peaks at 4639, 5859, 6905, and 8293 cm-1. Notably, the PL intensity of VA-SWNT@BNNT is 20 times smaller than that of VA-BNNT. In VA-SWNT, we observe an additional Raman peak at 4677 cm-1, which closely aligns with the 4639 cm-1 PL peak of VA-SWNT@BNNT, suggesting photoexcited electrons in VA-BNNT may transfer to the Raman process within VA-SWNT component of VA-SWNT@BNNT. The first-principles calculations identify possible donor and acceptor states in BN bilayers with substitutional defects (e.g., carbon replacing boron or nitrogen). These defect states are also relevant to understanding the origin of PL in BNNT.
AB - Using a 266 nm laser, we simultaneously observe Raman and photoluminescence (PL) spectra of vertically aligned boron-nitride nanotubes (VA-BNNT) and single-walled carbon nanotubes (SWNT) encapsulated by boron nitride (VA-SWNT@BNNT). The larger PL intensity in VA-BNNT compared to that of the h-BN single crystal suggests that VA-BNNT contains more defect states. VA-SWNT@BNNT exhibits two multiphonon Raman peaks at 3033 and 3142 cm-1 and four PL peaks at 4639, 5859, 6905, and 8293 cm-1. Notably, the PL intensity of VA-SWNT@BNNT is 20 times smaller than that of VA-BNNT. In VA-SWNT, we observe an additional Raman peak at 4677 cm-1, which closely aligns with the 4639 cm-1 PL peak of VA-SWNT@BNNT, suggesting photoexcited electrons in VA-BNNT may transfer to the Raman process within VA-SWNT component of VA-SWNT@BNNT. The first-principles calculations identify possible donor and acceptor states in BN bilayers with substitutional defects (e.g., carbon replacing boron or nitrogen). These defect states are also relevant to understanding the origin of PL in BNNT.
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U2 - 10.1021/acs.jpclett.4c03681
DO - 10.1021/acs.jpclett.4c03681
M3 - Article
C2 - 39928723
AN - SCOPUS:85217384844
SN - 1948-7185
VL - 16
SP - 1711
EP - 1719
JO - Journal of Physical Chemistry Letters
JF - Journal of Physical Chemistry Letters
IS - 7
ER -