TY - JOUR
T1 - Strong electron–phonon coupling in magic-angle twisted bilayer graphene
AU - Chen, Cheng
AU - Nuckolls, Kevin P.
AU - Ding, Shuhan
AU - Miao, Wangqian
AU - Wong, Dillon
AU - Oh, Myungchul
AU - Lee, Ryan L.
AU - He, Shanmei
AU - Peng, Cheng
AU - Pei, Ding
AU - Li, Yiwei
AU - Hao, Chenyue
AU - Yan, Haoran
AU - Xiao, Hanbo
AU - Gao, Han
AU - Li, Qiao
AU - Zhang, Shihao
AU - Liu, Jianpeng
AU - He, Lin
AU - Watanabe, Kenji
AU - Taniguchi, Takashi
AU - Jozwiak, Chris
AU - Bostwick, Aaron
AU - Rotenberg, Eli
AU - Li, Chu
AU - Han, Xu
AU - Pan, Ding
AU - Liu, Zhongkai
AU - Dai, Xi
AU - Liu, Chaoxing
AU - Bernevig, B. Andrei
AU - Wang, Yao
AU - Yazdani, Ali
AU - Chen, Yulin
N1 - Publisher Copyright:
© The Author(s) 2024.
PY - 2024/12/12
Y1 - 2024/12/12
N2 - The unusual properties of superconductivity in magic-angle twisted bilayer graphene (MATBG) have sparked considerable research interest1, 2, 3, 4, 5, 6, 7, 8, 9, 10, 11, 12–13. However, despite the dedication of intensive experimental efforts and the proposal of several possible pairing mechanisms14, 15, 16, 17, 18, 19, 20, 21, 22, 23–24, the origin of its superconductivity remains elusive. Here, by utilizing angle-resolved photoemission spectroscopy with micrometre spatial resolution, we reveal flat-band replicas in superconducting MATBG, where MATBG is unaligned with its hexagonal boron nitride substrate11. These replicas show uniform energy spacing, approximately 150 ± 15 meV apart, indicative of strong electron–boson coupling. Strikingly, these replicas are absent in non-superconducting twisted bilayer graphene (TBG) systems, either when MATBG is aligned to hexagonal boron nitride or when TBG deviates from the magic angle. Calculations suggest that the formation of these flat-band replicas in superconducting MATBG are attributed to the strong coupling between flat-band electrons and an optical phonon mode at the graphene K point, facilitated by intervalley scattering. These findings, although they do not necessarily put electron–phonon coupling as the main driving force for the superconductivity in MATBG, unravel the electronic structure inherent in superconducting MATBG, thereby providing crucial information for understanding the unusual electronic landscape from which its superconductivity is derived.
AB - The unusual properties of superconductivity in magic-angle twisted bilayer graphene (MATBG) have sparked considerable research interest1, 2, 3, 4, 5, 6, 7, 8, 9, 10, 11, 12–13. However, despite the dedication of intensive experimental efforts and the proposal of several possible pairing mechanisms14, 15, 16, 17, 18, 19, 20, 21, 22, 23–24, the origin of its superconductivity remains elusive. Here, by utilizing angle-resolved photoemission spectroscopy with micrometre spatial resolution, we reveal flat-band replicas in superconducting MATBG, where MATBG is unaligned with its hexagonal boron nitride substrate11. These replicas show uniform energy spacing, approximately 150 ± 15 meV apart, indicative of strong electron–boson coupling. Strikingly, these replicas are absent in non-superconducting twisted bilayer graphene (TBG) systems, either when MATBG is aligned to hexagonal boron nitride or when TBG deviates from the magic angle. Calculations suggest that the formation of these flat-band replicas in superconducting MATBG are attributed to the strong coupling between flat-band electrons and an optical phonon mode at the graphene K point, facilitated by intervalley scattering. These findings, although they do not necessarily put electron–phonon coupling as the main driving force for the superconductivity in MATBG, unravel the electronic structure inherent in superconducting MATBG, thereby providing crucial information for understanding the unusual electronic landscape from which its superconductivity is derived.
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U2 - 10.1038/s41586-024-08227-w
DO - 10.1038/s41586-024-08227-w
M3 - Article
C2 - 39663492
AN - SCOPUS:85211621887
SN - 0028-0836
VL - 636
SP - 342
EP - 347
JO - Nature
JF - Nature
IS - 8042
M1 - 087001
ER -