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首页> 外文期刊>Physical Review, A. Atomic, molecular, and optical physics >Sub-shot-noise phase sensitivity with a Bose-Einstein condensate Mach-Zehnder interferometer
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Sub-shot-noise phase sensitivity with a Bose-Einstein condensate Mach-Zehnder interferometer

机译:Bose-Einstein凝结Mach-Zehnder干涉仪的亚散相噪声灵敏度

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摘要

Bose-Einstein condensates (BEC), with their coherence properties, have attracted wide interest for their possible application to ultraprecise interferometry and ultraweak force sensors. Since condensates, unlike photons, are interacting, they may permit the realization of specific quantum states needed as input of an interferometer to approach the Heisenberg limit, the supposed lower bound to precision phase measurements. To this end, we study the sensitivity to external weak perturbations of a representative matter-wave Mach-Zehnder interferometer whose input are two Bose-Einstein condensates created by splitting a single condensate in two parts. The interferometric phase sensitivity depends on the specific quantum state created with the two condensates, and, therefore, on the time scale of the splitting process. We identify three different regimes, characterized by a phase sensitivity Delta theta scaling with the total number of condensate particles N as (i) the standard quantum limit Delta theta similar to 1/N-1/2, (ii) the sub shot-noise Delta theta similar to 1/N-3/4, and the (iii) the Heisenberg limit Delta theta similar to 1/N. However, in a realistic dynamical BEC splitting, the 1/N limit requires a long adiabaticity time scale, which is hardly reachable experimentally. On the other hand, the sub-shot-noise sensitivity Delta theta similar to 1/N-3/4 can be reached in a realistic experimental setting. We also show that the 1/N-3/4 scaling is a rigorous upper bound in the limit N ->infinity, while keeping constant all different parameters of the bosonic Mach-Zehnder interferometer.
机译:玻色-爱因斯坦凝聚物(BEC)具有相干特性,因其可能应用于超精密干涉测量和超弱力传感器而引起了广泛的关注。由于与光子不同,凝聚物相互作用,因此它们可以允许实现特定的量子态,作为干涉仪的输入以接近海森堡极限(假定为精确相位测量的下限)。为此,我们研究了代表性物质波马赫曾德尔干涉仪对外部弱摄动的灵敏度,该干涉仪的输入是通过将单个冷凝物分成两部分而产生的两个玻色-爱因斯坦冷凝物。干涉相灵敏度取决于两种冷凝物产生的特定量子态,因此取决于拆分过程的时间尺度。我们确定了三种不同的状态,其特征在于相敏度Delta theta缩放,冷凝液颗粒N的总数为(i)类似于1 / N-1 / 2的标准量子极限Delta theta,(ii)子散粒噪声Delta theta类似于1 / N-3 / 4,并且(iii)Heisenberg极限Delta theta类似于1 / N。但是,在实际的动态BEC分割中,1 / N限制要求较长的绝热时间尺度,这在实验上几乎是无法达到的。另一方面,在实际的实验设置中,可以达到类似于1 / N-3 / 4的子散粒噪声灵敏度Delta theta。我们还表明,1 / N-3 / 4缩放比例在极限N->无限范围内是一个严格的上限,同时使Bosonic Mach-Zehnder干涉仪的所有不同参数保持不变。

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