Coexistence of electron whispering-gallery modes and atomic collapse states in graphene/WSe2 heterostructure quantum dots
The relativistic massless charge carriers with a Fermi velocity of about c /300 in graphene enable us to realize two distinct types of resonances (here, c is the speed of light in vacuum). One is the electron whispering-gallery mode in graphene quantum dots arising from the Klein tunneling of the ma...
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| Published in | Nature communications Vol. 13; no. 1; p. 1597 |
|---|---|
| Main Authors | , , , |
| Format | Journal Article |
| Language | English |
| Published |
London
Nature Publishing Group UK
24.03.2022
Nature Publishing Group Nature Portfolio |
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| Abstract | The relativistic massless charge carriers with a Fermi velocity of about
c
/300 in graphene enable us to realize two distinct types of resonances (here,
c
is the speed of light in vacuum). One is the electron whispering-gallery mode in graphene quantum dots arising from the Klein tunneling of the massless Dirac fermions. The other is the atomic collapse state, which has never been observed in experiment with real atoms due to the difficulty of producing heavy nuclei with charge Z > 170; however, they can be realized near a Coulomb impurity in graphene with a charge Z ≥ 1 because of the “small” velocity of the Dirac excitations. Here we demonstrate that both the electron whispering-gallery modes and atomic collapse states coexist in graphene/WSe
2
heterostructure quantum dots due to the Coulomb-like potential near their edges. By applying a perpendicular magnetic field, we explore the evolution from the atomic collapse states to unusual Landau levels in the collapse regime.
The whispering-gallery mode and the atomic collapse state are two distinct resonances in condensed matter associated with relativistic massless charge carriers. Now, it is shown that these states can coexist in graphene/WSe
2
heterostructure quantum dots. |
|---|---|
| AbstractList | The whispering-gallery mode and the atomic collapse state are two distinct resonances in condensed matter associated with relativistic massless charge carriers. Now, it is shown that these states can coexist in graphene/WSe2 heterostructure quantum dots. The relativistic massless charge carriers with a Fermi velocity of about c/300 in graphene enable us to realize two distinct types of resonances (here, c is the speed of light in vacuum). One is the electron whispering-gallery mode in graphene quantum dots arising from the Klein tunneling of the massless Dirac fermions. The other is the atomic collapse state, which has never been observed in experiment with real atoms due to the difficulty of producing heavy nuclei with charge Z > 170; however, they can be realized near a Coulomb impurity in graphene with a charge Z ≥ 1 because of the “small” velocity of the Dirac excitations. Here we demonstrate that both the electron whispering-gallery modes and atomic collapse states coexist in graphene/WSe2 heterostructure quantum dots due to the Coulomb-like potential near their edges. By applying a perpendicular magnetic field, we explore the evolution from the atomic collapse states to unusual Landau levels in the collapse regime.The whispering-gallery mode and the atomic collapse state are two distinct resonances in condensed matter associated with relativistic massless charge carriers. Now, it is shown that these states can coexist in graphene/WSe2 heterostructure quantum dots. The relativistic massless charge carriers with a Fermi velocity of about c /300 in graphene enable us to realize two distinct types of resonances (here, c is the speed of light in vacuum). One is the electron whispering-gallery mode in graphene quantum dots arising from the Klein tunneling of the massless Dirac fermions. The other is the atomic collapse state, which has never been observed in experiment with real atoms due to the difficulty of producing heavy nuclei with charge Z > 170; however, they can be realized near a Coulomb impurity in graphene with a charge Z ≥ 1 because of the “small” velocity of the Dirac excitations. Here we demonstrate that both the electron whispering-gallery modes and atomic collapse states coexist in graphene/WSe 2 heterostructure quantum dots due to the Coulomb-like potential near their edges. By applying a perpendicular magnetic field, we explore the evolution from the atomic collapse states to unusual Landau levels in the collapse regime. The whispering-gallery mode and the atomic collapse state are two distinct resonances in condensed matter associated with relativistic massless charge carriers. Now, it is shown that these states can coexist in graphene/WSe 2 heterostructure quantum dots. The relativistic massless charge carriers with a Fermi velocity of about c /300 in graphene enable us to realize two distinct types of resonances (here, c is the speed of light in vacuum). One is the electron whispering-gallery mode in graphene quantum dots arising from the Klein tunneling of the massless Dirac fermions. The other is the atomic collapse state, which has never been observed in experiment with real atoms due to the difficulty of producing heavy nuclei with charge Z > 170; however, they can be realized near a Coulomb impurity in graphene with a charge Z ≥ 1 because of the “small” velocity of the Dirac excitations. Here we demonstrate that both the electron whispering-gallery modes and atomic collapse states coexist in graphene/WSe 2 heterostructure quantum dots due to the Coulomb-like potential near their edges. By applying a perpendicular magnetic field, we explore the evolution from the atomic collapse states to unusual Landau levels in the collapse regime. |
| ArticleNumber | 1597 |
| Author | Zhuang, Yu-Chen He, Lin Sun, Qing-Feng Zheng, Qi |
| Author_xml | – sequence: 1 givenname: Qi orcidid: 0000-0003-3484-5418 surname: Zheng fullname: Zheng, Qi – sequence: 2 givenname: Yu-Chen surname: Zhuang fullname: Zhuang, Yu-Chen – sequence: 3 givenname: Qing-Feng orcidid: 0000-0002-5512-9608 surname: Sun fullname: Sun, Qing-Feng email: sunqf@pku.edu.cn – sequence: 4 givenname: Lin orcidid: 0000-0001-5251-1687 surname: He fullname: He, Lin email: helin@bnu.edu.cn |
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| CitedBy_id | crossref_primary_10_1103_PhysRevLett_129_076803 crossref_primary_10_1103_PhysRevLett_129_076802 crossref_primary_10_1209_0295_5075_ad129f crossref_primary_10_3390_molecules28114334 crossref_primary_10_1021_acs_nanolett_2c04957 crossref_primary_10_1103_PhysRevLett_130_076202 crossref_primary_10_1002_aisy_202200128 crossref_primary_10_1103_PhysRevB_109_045430 crossref_primary_10_1007_s11433_022_2094_3 crossref_primary_10_1021_acs_nanolett_3c02286 crossref_primary_10_1007_s44214_023_00027_z crossref_primary_10_1103_PhysRevB_108_L081408 |
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| Snippet | The relativistic massless charge carriers with a Fermi velocity of about
c
/300 in graphene enable us to realize two distinct types of resonances (here,
c
is... The relativistic massless charge carriers with a Fermi velocity of about c/300 in graphene enable us to realize two distinct types of resonances (here, c is... The whispering-gallery mode and the atomic collapse state are two distinct resonances in condensed matter associated with relativistic massless charge... |
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| SubjectTerms | 147/138 639/301/357/1017 639/925/918/1052 Coexistence Collapse Current carriers Electrons Fermions Graphene Heavy nuclei Heterostructures Humanities and Social Sciences Light speed Magnetic fields multidisciplinary Quantum dots Relativistic effects Science Science (multidisciplinary) Velocity |
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| Title | Coexistence of electron whispering-gallery modes and atomic collapse states in graphene/WSe2 heterostructure quantum dots |
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