Open AccessOptical performance of materials for X‐ray refractive optics in the energy range 8–100 keV
Author(s) -
Serebrennikov Dmitry,
Clementyev Evgeny,
Semenov Alexander,
Snigirev Anatoly
Publication year - 2016
Publication title -
journal of synchrotron radiation
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 1.172
H-Index - 99
ISSN - 1600-5775
DOI - 10.1107/s1600577516014508
Subject(s) - materials science , beryllium , synchrotron radiation , optics , amorphous solid , boron nitride , range (aeronautics) , x ray optics , laser , diamond , crystal (programming language) , synchrotron , x ray , optoelectronics , crystallography , chemistry , nanotechnology , physics , programming language , computer science , composite material , organic chemistry
A quantitative analysis of the crucial characteristics of currently used and promising materials for X‐ray refractive optics is performed in the extended energy range 8–100 keV. According to the examined parameters, beryllium is the material of choice for X‐ray compound refractive lenses (CRLs) in the energy range 8–25 keV. At higher energies the use of CRLs made of diamond and the cubic phase of boron nitride (c‐BN) is beneficial. It was demonstrated that the presence of the elements of the fourth (or higher) period has a fatal effect on the functional X‐ray properties even if low‐ Z elements dominate in the compound, like in YB 66 . Macroscopic properties are discussed: much higher melting points and thermal conductivities of C and c‐BN enable them to be used at the new generation of synchrotron radiation sources and X‐ray free‐electron lasers. The role of crystal and internal structure is discussed: materials with high density are preferable for refractive applications while less dense phases are suitable for X‐ray windows. Single‐crystal or amorphous glass‐like materials based on Li, Be, B or C that are free of diffuse scattering from grain boundaries, voids and inclusions are the best candidates for applications of highly coherent X‐ray beams.