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石墨中的光致 π-π* 带隙重整化。

Photoinduced π-π* band gap renormalization in graphite.

机构信息

Dipartimento di Matematica e Fisica, Università Cattolica del Sacro Cuore, I-25121 Brescia, Italy.

出版信息

J Am Chem Soc. 2011 Apr 27;133(16):6318-22. doi: 10.1021/ja1110738. Epub 2011 Mar 31.

Abstract

As is well-known, the character of the π orbitals is of paramount importance for the chemical properties of the carbon allotropes and their derived compounds. While at equilibrium the nature of these orbitals is well understood, their photoinduced nonequilibrium behavior is under investigation. Here, we demonstrate that when a UV-laser pulse excites a carrier density larger than 10% of the π* density of state in graphite, a renormalization of the π-π* band gap takes place. This result has been achieved by detecting the transient reflectivity and the associated decay time of an infrared probe following the excitation of a UV pump pulse tuned across the π-π* absorption resonance. The pump photon energy at which both the transient reflectivity and the decay time are maximum is downshifted by 500 meV with respect to the relative absorption maximum at equilibrium. This finding is interpreted as a transient π-π* band gap shrinking of similar magnitude, near the M point of the Brillouin zone.

摘要

众所周知,π 轨道的性质对于碳同素异形体及其衍生化合物的化学性质至关重要。虽然这些轨道在平衡态时的性质已经得到很好的理解,但它们的光诱导非平衡行为仍在研究中。在这里,我们证明了当紫外激光脉冲激发的载流子密度超过石墨中π态密度的 10%时,π-π带隙会发生重整化。这一结果是通过探测在激发紫外泵浦脉冲后,在π-π吸收共振调谐范围内,红外探针的瞬态反射率和相关衰减时间来实现的。瞬态反射率和衰减时间达到最大值的泵浦光子能量相对于平衡时的相对吸收最大值下移了 500 meV。这一发现被解释为在布里渊区的 M 点附近,瞬态π-π带隙的类似程度的收缩。

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