超强耦合区极化模的非均匀展宽

S. Rajabali, G. Scalari, J. Keller, M. Beck, J. Faist
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摘要

由于超强耦合(USC)能够改变耦合系统的基态和激发态,因此在腔量子电动力学(QED)实验中一直是一个有趣的研究课题[1-3]。我们利用太赫兹时域光谱研究了二维电子气体中朗道能级(LL)跃迁到太赫兹(THz)超表面的USC。互补太赫兹分裂环谐振器(cSRR)阵列被用作超表面。由于真空场波动的增加,可以通过减小谐振器的容性间隙来实现更高的耦合率。然而,我们的研究结果表明,这种减少在阈值间隙宽度以下引入了上极化子分支的不均匀展宽。
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Inhomogeneous Broadening of a Polaritonic Mode in the Ultrastrong Coupling Regime
Ultrastrong coupling (USC) regime has been an intriguing research topic in cavity quantum electrodynamics (QED) experiments due to its capability to modify the ground and the excited states of a coupled system[1–3]. We investigate the USC of Landau level (LL) transitions in a two dimensional electron gas to teraherz (THz) metasurfaces using THz time domain spectroscopy. Complementary THz split ring resonator (cSRR) arrays are used as metasurfaces]. A higher coupling rate can be achieved by reducing the capacitive gap of the resonator due to the increased vacuum field fluctuations. However, our results indicate that this reduction introduces an inhomogenous broadening of the upper polariton branch below a threshold gap width.
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