Martin Jérôme, Avalos-Ovando Oscar, Simon Thomas, Arditi Gabriel, Lamaze Florian, Proust Julien, Tizei Luiz, Wang Zhiming, Kociak Mathieu, Govorov Alexander O, Stéphan Odile, Gérard Davy
Lumière, nanomatériaux, nanotechnologies (L2n), UMR CNRS 7076, Université de Technologie de Troyes, Troyes 10004, France.
Department of Physics and Astronomy and Nanoscale and Quantum Phenomena Institute, Ohio University, Athens, Ohio 45701, United States.
ACS Nano. 2025 Jun 24;19(24):22343-22356. doi: 10.1021/acsnano.5c05690. Epub 2025 Jun 11.
Strong coupling typically occurs between two separate objects or between an object and its environment (such as an atom and a cavity). However, it can also occur between two different excitations within the same object, a situation that has been much less studied. In this study, we observe strong coupling between localized surface plasmon resonances and the interband transition in aluminum nanorods, as evidenced by optical spectroscopy and electron energy loss spectroscopy, and corroborated with numerical simulations. Strong coupling is observed between the interband transition and multiple orders of the surface plasmon mode, including dark ones. We also obtain experimental maps of the hybrid modes at the nanoscale. In each case, the associated Rabi energy, which corresponds to the energy splitting between the two polaritonic branches, is obtained. Moreover, a dedicated numerical model was employed to calculate the hot electron generation rate in the nanorods. The calculations demonstrate that efficient generation of hot electrons can be achieved in the near-infrared region when the interband transition is strongly coupled with a plasmon resonance. This high generation rate stems from the hybrid nature of the mode, as its plasmonic component provides a high absorption cross-section, while the interband transition part ensures efficient conversion to hot electrons. Consequently, aluminum nanorods represent an efficient source of hot electrons in the visible and near-infrared regions, with potential applications in local photochemistry, photodetection, and solar energy harvesting.
强耦合通常发生在两个独立的物体之间,或者一个物体与其环境之间(例如一个原子和一个腔)。然而,它也可能发生在同一物体内的两种不同激发之间,而这种情况的研究要少得多。在本研究中,我们观察到了铝纳米棒中局域表面等离子体共振与带间跃迁之间的强耦合,这通过光谱学和电子能量损失光谱学得到了证实,并通过数值模拟得到了进一步验证。在带间跃迁与表面等离子体模式的多个阶次(包括暗阶次)之间观察到了强耦合。我们还获得了纳米尺度下混合模式的实验图谱。在每种情况下,都得到了与两个极化子分支之间的能量分裂相对应的拉比能量。此外,采用了一个专门的数值模型来计算纳米棒中的热电子产生率。计算结果表明,当带间跃迁与等离子体共振强耦合时,在近红外区域可以实现热电子的高效产生。这种高产生率源于模式的混合性质,因为其等离子体成分提供了高吸收截面,而带间跃迁部分则确保了向热电子的高效转化。因此,铝纳米棒是可见光和近红外区域中高效的热电子源,在局部光化学、光探测和太阳能收集方面具有潜在应用。