Witte B B L, Röpke G, Neumayer P, French M, Sperling P, Recoules V, Glenzer S H, Redmer R
Institut für Physik, Universität Rostock, 18051 Rostock, Germany.
SLAC National Accelerator Laboratory, 2575 Sand Hill Road, MS 72 Menlo Park, California 94025, USA.
Phys Rev E. 2019 Apr;99(4-2):047201. doi: 10.1103/PhysRevE.99.047201.
Dharma-wardana et al. [M. W. C. Dharma-wardana et al., Phys. Rev. E 96, 053206 (2017)2470-004510.1103/PhysRevE.96.053206] recently calculated dynamic electrical conductivities for warm dense matter as well as for nonequilibrium two-temperature states termed "ultrafast matter" (UFM) [M. W. C. Dharma-wardana, Phys. Rev. E 93, 063205 (2016)2470-004510.1103/PhysRevE.93.063205]. In this Comment we present two evident reasons why these UFM calculations are neither suited to calculate dynamic conductivities nor x-ray Thomson scattering spectra in isochorically heated warm dense aluminum. First, the ion-ion structure factor, a major input into the conductivity and scattering spectra calculations, deviates strongly from that of isochorically heated aluminum. Second, the dynamic conductivity does not show a non-Drude behavior which is an essential prerequisite for a correct description of the absorption behavior in aluminum. Additionally, we clarify misinterpretations by Dharma-wardana et al. concerning the conductivity measurements of Gathers [G. R. Gathers, Int. J. Thermophys. 4, 209 (1983)IJTHDY0195-928X10.1007/BF00502353].
达摩瓦德纳等人[M. W. C. 达摩瓦德纳等人,《物理评论E》96, 053206 (2017)2470 - 004510.1103/PhysRevE.96.053206]最近计算了热密物质以及被称为“超快物质”(UFM)的非平衡双温状态[M. W. C. 达摩瓦德纳,《物理评论E》93, 063205 (2016)2470 - 004510.1103/PhysRevE.93.063205]的动态电导率。在本评论中,我们给出两个明显的理由,说明这些超快物质的计算既不适用于计算动态电导率,也不适用于计算等容加热的热密铝中的x射线汤姆逊散射光谱。第一,离子 - 离子结构因子是电导率和散射光谱计算的主要输入参数,它与等容加热铝的结构因子有很大偏差。第二,动态电导率没有显示出非德鲁德行为,而这是正确描述铝中吸收行为的一个基本前提条件。此外,我们澄清了达摩瓦德纳等人对加瑟斯[G. R. 加瑟斯,《国际热物理学杂志》4, 209 (1983)IJTHDY0195 - 928X10.1007/BF00502353]电导率测量的误解。