“…High resolution at the nanoscale is achieved by focusing SR to a secondary source and then exploiting the cone-beam geometry (Mokso et al, 2007;Bartels et al, 2015) and the Fresnel scaling theorem (Paganin, 2006). A wide range of dedicated beamlines are now available for parallel-beam PBI (see, for example, Weitkamp et al, 2010;Longo et al, 2019;Wang et al, 2001;Schell et al, 2013) as well as -at a somewhat smaller scale and numberfor cone-beam PBI based on nano-focused undulator radiation (da Silva et al, 2017;Wilde et al, 2016;Lovric et al, 2016;Salditt et al, 2015). In addition, a new generation of microfocus X-ray sources, with increased flux and improved spatial coherence (Hemberg et al, 2003), has enabled the implementation of PBI and computed tomography at the micrometre scale (microCT) in the laboratory (Bartels et al, 2013;Vå gberg et al, 2015;Larsson et al, 2016).…”