Acoustic Landau quantization and quantum-Hall-like edge states
Many intriguing phenomena occur for electrons under strong magnetic fields 1 , 2 . Recently, it was shown that an appropriate strain texture in graphene could induce a synthetic gauge field 3 – 6 , in which electrons behave as they do in a real magnetic field 7 – 11 . This enabled the control of qua...
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Veröffentlicht in: | Nature physics 2019-04, Vol.15 (4), p.352-356 |
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Sprache: | eng |
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Zusammenfassung: | Many intriguing phenomena occur for electrons under strong magnetic fields
1
,
2
. Recently, it was shown that an appropriate strain texture in graphene could induce a synthetic gauge field
3
–
6
, in which electrons behave as they do in a real magnetic field
7
–
11
. This enabled the control of quantum transport by mechanical means and allowed the unreached high-field regime to be explored. Such synthetic gauge fields have been achieved in molecular
12
and photonic
13
lattices. Here we report an experimental realization of a giant uniform pseudomagnetic field in acoustics by introducing a simple uniaxial deformation to the acoustic graphene. The controllability of our macroscopic platform enables us to observe the acoustic Landau levels in frequency-resolved spectroscopy and their spatial localization in pressure-field distributions. We further visualize the quantum-Hall-like edge states (connected to the zeroth Landau level), which have been elusive owing to the difficulty in creating large-area uniform pseudomagnetic fields
5
,
6
. These results, consistent with our full-wave simulations, establish a complete framework for artificial structures under constant pseudomagnetic fields. Our findings may also offer opportunities to manipulate sound in conceptually novel ways.
A graphene-like two-dimensional sonic crystal, under uniaxial deformation, experiences a giant uniform pseudomagnetic field. This leads to the quantization of the cyclotron orbits—a kind of acoustic Landau level—that is observed here. |
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ISSN: | 1745-2473 1745-2481 |
DOI: | 10.1038/s41567-019-0446-3 |