453nm光激发下porphyrin-ruthenium二聚体的超快速能级转移观测

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本文主要探讨了通过时间分辨荧光光谱技术对一种由polypyridyl ruthenium II [Ru(phen)2(ip)]2+ 和5,10,15,20-四苯基卟啉(H2TPP)组成的分子复合物——卟啉-钌二元体系的光致发光动态特性进行直接观测。这项研究的焦点在于超快的能量转移过程。 在实验中,当[Ru(phen)2(ip)]2+ 分子在453纳米的光激发下,观察到一个显著的现象:在300皮秒(ps)的时间尺度上,发生了高效的能量转移。这种现象表明,两个分子之间存在一种快速的非辐射能量传递机制,可能是通过 Förster共振能量转移(FRET)或者其他高效能传递途径,使得初始激发的能量迅速转移到了H2TPP分子上,从而影响了后续的发光行为。 然而,当激发波长调整至400纳米,对应于H2TPP的吸收峰时,却没有观察到类似的能量转移。这暗示了能量转移的发生并非是简单的线性关系,而是依赖于激发光的波长和分子间的距离,以及它们之间的相互作用强度。400纳米的光没有激发到[Ru(phen)2(ip)]2+ 的能量吸收特征,因此能量转移过程被抑制,显示出能量传递的敏感性。 这项研究对于理解光致反应动力学、设计新型光致变色材料以及探索生物光化学过程中的能量传递机制具有重要意义。它展示了如何利用时间分辨荧光技术来揭示分子复合物中的复杂能量流动,并为未来的光能转化和控制提供了新的见解。通过深入研究这类卟啉-金属配合物,科学家们可以开发出更高效、响应更快的光驱动设备,如太阳能电池、光催化剂和生物传感器。

翻译Agent 𝑐 𝑖 . In this paper, we regard each charging station 𝑐 𝑖 ∈ 𝐶 as an individual agent. Each agent will make timely recommendation decisions for a sequence of charging requests 𝑄 that keep coming throughout a day with multiple long-term optimization goals. Observation 𝑜 𝑖 𝑡 . Given a charging request 𝑞𝑡 , we define the observation 𝑜 𝑖 𝑡 of agent 𝑐 𝑖 as a combination of the index of 𝑐 𝑖 , the real-world time 𝑇𝑡 , the number of current avail able charging spots of 𝑐 𝑖 (supply), the number of charging requests around 𝑐 𝑖 in the near future (future demand), the charging power of 𝑐 𝑖 , the estimated time of arrival (ETA) from location 𝑙𝑡 to 𝑐 𝑖 , and the CP of 𝑐 𝑖 at the next ETA. We further define 𝑠𝑡 = {𝑜 1 𝑡 , 𝑜2 𝑡 , . . . , 𝑜𝑁 𝑡 } as the state of all agents at step 𝑡. Action 𝑎 𝑖 𝑡 . Given an observation 𝑜 𝑖 𝑡 , an intuitional design for the action of agent𝑐 𝑖 is a binary decision, i.e., recommending 𝑞𝑡 to itself for charging or not. However, because one 𝑞𝑡 can only choose one station for charging, multiple agents’ actions may be tied together and are difficult to coordinate. Inspired by the bidding mechanism, we design each agent 𝑐 𝑖 offers a scalar value to "bid" for 𝑞𝑡 as its action 𝑎 𝑖 𝑡 . By defining 𝑢𝑡 = {𝑎 1 𝑡 , 𝑎2 𝑡 , . . . , 𝑎𝑁 𝑡 } as the joint action, 𝑞𝑡 will be recommended to the agent with the highest "bid" value, i.e., 𝑟𝑐𝑡 = 𝑐 𝑖 , where 𝑖 = arg max(𝑢𝑡)

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