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金纳米天线中四光子光致发光的动力学。

Dynamics of four-photon photoluminescence in gold nanoantennas.

机构信息

CNISM, Piazza Leonardo da Vinci 32, 20133 Milano, Italy.

出版信息

Nano Lett. 2012 Jun 13;12(6):2941-7. doi: 10.1021/nl300616s. Epub 2012 May 14.

Abstract

Two-pulse correlation is employed to investigate the temporal dynamics of both two-photon photoluminescence (2PPL) and four-photon photoluminescence (4PPL) in resonant and nonresonant nanoantennas excited at a wavelength of 800 nm. Both 2PPL and 4PPL data are consistent with the same two-step model already established for 2PPL, implying that the first excitation step in 4PPL is a three-photon sp → sp direct interband transition. Considering energy and parity conservation, we also explain why 4PPL behavior is favored over, for example, three- and five-photon photoluminescence in the power range below the damage threshold of our antennas. Since sizable 4PPL requires larger peak intensities of the local field, we are able to select either 2PPL or 4PPL in the same gold nanoantennas by choosing a suitable laser pulse duration. We thus provide a first consistent model for the understanding of multiphoton photoluminescence generation in gold nanoantennas, opening new perspectives for applications ranging from the characterization of plasmonic resonances to biomedical imaging.

摘要

采用双脉冲相关法研究了在 800nm 波长激发下共振和非共振纳米天线中双光子光致发光(2PPL)和四光子光致发光(4PPL)的时间动力学。2PPL 和 4PPL 数据都与已经为 2PPL 建立的相同两步模型一致,这意味着 4PPL 中的第一个激发步骤是一个三光子 sp→sp 直接带间跃迁。考虑到能量和宇称守恒,我们还解释了为什么在低于我们天线破坏阈值的功率范围内,4PPL 行为优于例如三光子和五光子光致发光。由于较大的 4PPL 需要更大的局域场峰值强度,因此我们可以通过选择合适的激光脉冲持续时间在相同的金纳米天线中选择 2PPL 或 4PPL。因此,我们为理解金纳米天线中的多光子光致发光产生提供了第一个一致的模型,为从等离子体共振的表征到生物医学成像的应用开辟了新的视角。

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