Beenakker C W J, Schomerus H
Instituut-Lorentz, Universiteit Leiden, P.O. Box 9506, 2300 RA Leiden, The Netherlands.
Phys Rev Lett. 2004 Aug 27;93(9):096801. doi: 10.1103/PhysRevLett.93.096801. Epub 2004 Aug 23.
Motivated by the experimental search for "GHz nonclassical light," we identify the conditions under which current fluctuations in a narrow constriction generate sub-Poissonian radiation. Antibunched electrons generically produce bunched photons, because the same photon mode can be populated by electrons decaying independently from a range of initial energies. Photon antibunching becomes possible at frequencies close to the applied voltage V x e/variant Planck's over 2pi, when the initial energy range of a decaying electron is restricted. The condition for photon antibunching in a narrow frequency interval below eV/variant Planck's over 2pi reads [SigmanTn(1-Tn)]2<2Sigman[Tn(1-Tn)]2, with Tn an eigenvalue of the transmission matrix. This condition is satisfied in a quantum point contact, where only a single Tn differs from 0 or 1. The photon statistics is then a superposition of binomial distributions.
受“吉赫兹非经典光”实验探索的推动,我们确定了窄缩区域中电流涨落产生亚泊松辐射的条件。反聚束电子通常会产生聚束光子,因为同一光子模式可由从一系列初始能量独立衰变的电子填充。当衰变电子的初始能量范围受到限制时,在接近施加电压V×e/(2πħ)的频率处,光子反聚束变得可能。在低于eV/(2πħ)的窄频率区间内光子反聚束的条件为[SigmanTn(1 - Tn)]² < 2Sigman[Tn(1 - Tn)]²,其中Tn是传输矩阵的一个本征值。在量子点接触中满足此条件,其中只有一个Tn不同于0或1。此时光子统计是二项分布的叠加。