2013
DOI: 10.1209/0295-5075/103/17003
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Anomalous transmission of disordered photonic graphenes at the Dirac point

Abstract: The transmission properties of disordered photonic graphenes are investigated in microwave experiments. In the weak-localization regime, we found that, in the passbands the transmission decreases as the random degree increases, owing to the enhanced coherent backscattering effect. However, at the Dirac point, with the increase of the random degree, the transmission increases rather than decreasing. This observed anomalous transportation, also called weak antilocalization, provides the important experimental cl… Show more

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Cited by 12 publications
(11 citation statements)
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“…[216], references therein). Due to the wave nature of the electron motion in the honeycomb graphene lattice, the relativistic pseudo-particles can also be created using microwave photonic crystals [217][218][219][220][221][222][223][224][225][226][227][228][229][230] or mechanical vibrations and phononic crystals [231][232][233][234][235][236], where the propagation of the electromagnetic or acoustic wave follows the same honeycomb lattice structure, as shown in the left panel of Fig. 2.…”
Section: B Microwave Billiards With a Triangular Photonic Structurementioning
confidence: 99%
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“…[216], references therein). Due to the wave nature of the electron motion in the honeycomb graphene lattice, the relativistic pseudo-particles can also be created using microwave photonic crystals [217][218][219][220][221][222][223][224][225][226][227][228][229][230] or mechanical vibrations and phononic crystals [231][232][233][234][235][236], where the propagation of the electromagnetic or acoustic wave follows the same honeycomb lattice structure, as shown in the left panel of Fig. 2.…”
Section: B Microwave Billiards With a Triangular Photonic Structurementioning
confidence: 99%
“…The effective boundary displacement can be determined as δ 1 = ∆l − ∆ l − and δ 2 = ∆ l + − ∆l. (220,222,223)]. The parameters are u 0 = 2.045/a, ∆l = 2a, m 0 = 0.2/a, and the resulting boundary shift is δ = 0.032a.…”
Section: Tunneling Rate and Tunneling Probability Of Spin-polarized Statesmentioning
confidence: 99%
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“…Using photons, one can selectively excite states, and observe both the spectral and spatial responses throughout the material, which are challenging tasks in electronic systems. Experimental efforts studying gauge fields with photons have been limited to the microwave domain [3][4][5][6][7], while investigations in the optical domain have remained elusive. This is due to the fact that magneto-optic effectsthe simplest source of coupling between gauge fields and photons-are extremely weak at optical frequencies.…”
mentioning
confidence: 99%
“…In optics, it was predicted that in photonic graphene lattices, the pseudospin of the backscattered wave is anti-parallel to the input pseudospin direction, resulting in a CBS dip due to a Berry phase of π 26 . Consequently, enhanced transmission in photonic graphene lattices was observed in the microwave regime 27 . Here, we directly measured the destructive interference between the counter-propagating paths inside the fiber.…”
Section: Discussionmentioning
confidence: 99%