Shot noise measurements were recently exploited to measure the charge of thequasiparticles in the Fractional Quantum Hall (FQH) regime. For fractionalfilling factors nu=1/3 and 2/5 of the first Landau level, fractional chargesq=e/3 and e/5, respectively, were measured. We investigate here the interactionof e/3 quasiparticles with a strong backscatterer and find unexpected results.When a weak backscatterer is introduced in the path of an otherwise noiselesscurrent of quasiparticles, stochastic partitioning of the quasiparticles takesplace and shot noise proportional to their charge appears. Specifically, atnu=1/3, noise corresponding to q=e/3 appears. However, the measured chargeincreases monotonically as backscattering becomes stronger, approachingasymptotically q=e. In other words, only electrons, or alternatively, threebunched quasiparticles, tunnel through high potential barriers when impinged bya noiseless current of quasiparticles. Here we show that such bunching ofquasiparticles by a strong backscatterer depends on the average occupation(dilution) of the impinging quasiparticle current. For a very dilute impingingcurrent, bunching ceases altogether and the transferred charge approachesq=e/3. These surprising results prove that a sparse beam of quasiparticles,each with charge e/3, tunnel through high potential barriers, originallythought to be opaque for them.
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机译:最近利用散粒噪声测量来测量分数量子霍尔(FQH)方案中的准粒子的电荷。对于第一朗道能级的分数填充因子nu = 1/3和2/5,分别测量了分数电荷q = e / 3和e / 5。我们在这里研究e / 3准粒子与强后向散射体的相互作用并发现意外的结果。当将弱后向散射体引入到原本无噪声的准粒子流的路径中时,准粒子发生随机分配,并且散粒噪声与电荷成正比。具体地,atnu = 1/3,出现对应于q = e / 3的噪声。但是,随着反向散射变强,测得的电荷单调增加,渐近地接近q = e。换句话说,当受到准粒子的无噪声电流撞击时,只有电子或三束准粒子会隧穿高势垒。在这里,我们证明了强反向散射体对准粒子的这种聚集取决于撞击的准粒子电流的平均占有(稀释)。对于非常稀薄的冲击电流,束聚完全停止,转移的电荷接近q = e / 3。这些令人惊讶的结果证明,稀疏的准粒子束(每个电荷为e / 3)通过高势垒形成隧道,这些势垒本来是不透明的。
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