Fakultät für Physik, Universität Duisburg-Essen, Lotharstr. 1, D-47048 Duisburg, Germany.
J Phys Condens Matter. 2013 Mar 6;25(9):094003. doi: 10.1088/0953-8984/25/9/094003. Epub 2013 Feb 12.
We employed femtosecond time- and angle-resolved photoelectron spectroscopy to analyze the response of the electronic structure of the 122 Fe-pnictide parent compounds Ba/EuFe(2)As(2) and optimally doped BaFe(1.85)Co(0.15)As(2) near the Γ point to optical excitation by an infrared femtosecond laser pulse. We identify pronounced changes of the electron population within several 100 meV above and below the Fermi level, which we explain as a combination of (i) coherent lattice vibrations, (ii) a hot electron and hole distribution, and (iii) transient modifications of the chemical potential. The responses of the three different materials are very similar. In the coherent response we identify three modes at 5.6, 3.3, and 2.6 THz. While the highest frequency mode is safely assigned to the A(1g) mode, the other two modes require a discussion in comparison to the literature. Employing a transient three temperature model we deduce from the transient evolution of the electron distribution a rather weak, momentum-averaged electron-phonon coupling quantified by values for λ<ω(2)> between 30 and 70 meV(2). The chemical potential is found to present pronounced transient changes reaching a maximum of 15 meV about 0.6 ps after optical excitation and is modulated by the coherent phonons. This change in the chemical potential is particularly strong in a multiband system like the 122 Fe-pnictide compounds investigated here due to the pronounced variation of the electron density of states close to the equilibrium chemical potential.
我们采用飞秒时间分辨和角度分辨光电子能谱,分析了 122 铁磷母体化合物 Ba/EuFe(2)As(2)和最佳掺杂 BaFe(1.85)Co(0.15)As(2)在Γ点附近对红外飞秒激光脉冲光激发的电子结构响应。我们发现费米能级上下几百毫电子伏特范围内电子占据数发生了显著变化,我们将其解释为(i)相干晶格振动、(ii)热电子和空穴分布、(iii)化学势的瞬态变化的组合。三种不同材料的响应非常相似。在相干响应中,我们在 5.6、3.3 和 2.6 THz 处识别出三个模式。虽然最高频率模式可安全地分配到 A(1g)模式,但其他两个模式需要与文献进行比较讨论。通过瞬态三温度模型,我们从电子分布的瞬态演化中推断出,电子-声子耦合相当弱,动量平均的电子-声子耦合通过 λ<ω(2)>值来量化,范围在 30 到 70 meV(2)之间。化学势呈现出明显的瞬态变化,在光激发后约 0.6 ps 时达到最大值 15 meV,并且被相干声子调制。由于接近平衡化学势的电子态密度的显著变化,在像我们这里研究的 122 铁磷化合物这样的多带系统中,这种化学势的变化尤为强烈。