Scanning Tunneling Spectroscopy Observation of Electronic Resonances Originating from 1 ×1 Potential on the Dense Pb Overlayer on Si(111)
We use scanning tunneling spectroscopy (STS) to investigate the electronic structures of dense Pb overlayers of three phases grown on the Si(111) surface: the 1 ×1, √7 ×√3, and stripe incommensurate (SIC) phases. Although their atomic structures are all very different, the STS spectra of all three p...
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Published in | Japanese Journal of Applied Physics Vol. 51; no. 1R; p. 15702 |
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Main Authors | , , , , , , , , , |
Format | Journal Article |
Language | English |
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01.01.2012
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Abstract | We use scanning tunneling spectroscopy (STS) to investigate the electronic structures of dense Pb overlayers of three phases grown on the Si(111) surface: the 1 ×1, √7 ×√3, and stripe incommensurate (SIC) phases. Although their atomic structures are all very different, the STS spectra of all three phases show nearly identical oscillatory features with two resonance peaks. These resonances are not common quantum-well states; they are energy bands originating from the dominant 1 ×1 potential in these phases. However, the local electronic states found by STS show that the resonance peaks are modulated with the superstructure of the √7 ×√3 phase, and that the resonance energy varies with the domains and the domain walls in the SIC phase. |
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AbstractList | We use scanning tunneling spectroscopy (STS) to investigate the electronic structures of dense Pb overlayers of three phases grown on the Si(111) surface: the 1 ×1, √7 ×√3, and stripe incommensurate (SIC) phases. Although their atomic structures are all very different, the STS spectra of all three phases show nearly identical oscillatory features with two resonance peaks. These resonances are not common quantum-well states; they are energy bands originating from the dominant 1 ×1 potential in these phases. However, the local electronic states found by STS show that the resonance peaks are modulated with the superstructure of the √7 ×√3 phase, and that the resonance energy varies with the domains and the domain walls in the SIC phase. |
Author | Chan, Wen-Yuan Tsong, Tien Tzou Hsiao, Hsi-Lien Lu, Shin-Ming Jiang, Chi-Lun Chang, Chia-Seng Chu, Pei-Hong Su, Wei-Bin Chou, Hsing-Yi Chiu, Ya-Ping |
Author_xml | – sequence: 1 givenname: Shin-Ming surname: Lu fullname: Lu, Shin-Ming – sequence: 2 givenname: Wen-Yuan surname: Chan fullname: Chan, Wen-Yuan – sequence: 3 givenname: Hsing-Yi surname: Chou fullname: Chou, Hsing-Yi – sequence: 4 givenname: Ya-Ping surname: Chiu fullname: Chiu, Ya-Ping – sequence: 5 givenname: Wei-Bin surname: Su fullname: Su, Wei-Bin – sequence: 6 givenname: Pei-Hong surname: Chu fullname: Chu, Pei-Hong – sequence: 7 givenname: Chi-Lun surname: Jiang fullname: Jiang, Chi-Lun – sequence: 8 givenname: Chia-Seng surname: Chang fullname: Chang, Chia-Seng – sequence: 9 givenname: Hsi-Lien surname: Hsiao fullname: Hsiao, Hsi-Lien – sequence: 10 givenname: Tien Tzou surname: Tsong fullname: Tsong, Tien Tzou |
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CitedBy_id | crossref_primary_10_1116_1_4832336 crossref_primary_10_1073_pnas_1611967113 |
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