Institut für Angewandte Physik, Universität Bonn, Wegelerstrasse 8, 53115 Bonn, Germany.
Nature. 2010 Nov 25;468(7323):545-8. doi: 10.1038/nature09567.
Bose-Einstein condensation (BEC)-the macroscopic ground-state accumulation of particles with integer spin (bosons) at low temperature and high density-has been observed in several physical systems, including cold atomic gases and solid-state quasiparticles. However, the most omnipresent Bose gas, blackbody radiation (radiation in thermal equilibrium with the cavity walls) does not show this phase transition. In such systems photons have a vanishing chemical potential, meaning that their number is not conserved when the temperature of the photon gas is varied; at low temperatures, photons disappear in the cavity walls instead of occupying the cavity ground state. Theoretical works have considered thermalization processes that conserve photon number (a prerequisite for BEC), involving Compton scattering with a gas of thermal electrons or photon-photon scattering in a nonlinear resonator configuration. Number-conserving thermalization was experimentally observed for a two-dimensional photon gas in a dye-filled optical microcavity, which acts as a 'white-wall' box. Here we report the observation of a Bose-Einstein condensate of photons in this system. The cavity mirrors provide both a confining potential and a non-vanishing effective photon mass, making the system formally equivalent to a two-dimensional gas of trapped, massive bosons. The photons thermalize to the temperature of the dye solution (room temperature) by multiple scattering with the dye molecules. Upon increasing the photon density, we observe the following BEC signatures: the photon energies have a Bose-Einstein distribution with a massively populated ground-state mode on top of a broad thermal wing; the phase transition occurs at the expected photon density and exhibits the predicted dependence on cavity geometry; and the ground-state mode emerges even for a spatially displaced pump spot. The prospects of the observed effects include studies of extremely weakly interacting low-dimensional Bose gases and new coherent ultraviolet sources.
玻色-爱因斯坦凝聚(BEC)——低温高密下整数自旋粒子(玻色子)的宏观基态积累——已经在多个物理系统中被观察到,包括冷原子气体和固态准粒子。然而,最普遍的玻色气体,黑体辐射(与腔壁处于热平衡的辐射)并不显示这种相变。在这样的系统中,光子的化学势为零,这意味着当光子气体的温度变化时,它们的数量不守恒;在低温下,光子会消失在腔壁中,而不是占据腔的基态。理论工作已经考虑了守恒光子数的热化过程(BEC 的一个前提),涉及与热电子气体的康普顿散射或非线性谐振腔配置中的光子-光子散射。在填充有染料的光学微腔中的二维光子气体中,观察到了这种数守恒的热化,该微腔充当了“白墙”盒。在这里,我们报告了在该系统中观察到的光子玻色-爱因斯坦凝聚。腔镜提供了限制势和非零的有效光子质量,使系统在形式上等效于被捕获的二维重玻色子气体。光子通过与染料分子的多次散射,热化到染料溶液的温度(室温)。随着光子密度的增加,我们观察到以下 BEC 特征:光子能量具有玻色-爱因斯坦分布,在宽热翼上有大量占据的基态模式;相变发生在预期的光子密度处,并表现出与腔几何形状的预期依赖性;即使在空间上偏移的泵浦光斑下,基态模式也会出现。所观察到的效应的前景包括研究极弱相互作用的低维玻色气体和新的相干紫外光源。