As both porous and amorphous semiconductors have different advantages the challenge becomes knowing how to select one over the other, and knowing how to anticipate the degree of crystallinity or the fraction of voids as a function of a controllable feature such as the density. These sorts of relationships can be modelled computationally but unambiguous characterisation of the porosity of complex and disordered structures requires specialist tools. In this paper we demonstrate the use of PorosityPlus to investigate porosity in the vacancy induced amorphisation of defective crystals of carbon, silicon and germanium. The PorosityPlus software allows for the identification of vacancies, twin vacancies and larger pores, along with their relative locations and their respective populations. Void migration and coalescence along with the associated density changes can also be calculated. We show that, with increasing initial vacancies (reduced density) carbon (diamond), silicon and germanium exhibit characteristic density-dependent porosity profiles, coupled with simultaneous amorphisation. This is an ideal tool for integration into advanced computational workflows, such as creating fingerprints for topological data analysis or machine learning, since the porosity profile for each configuration is unique.Although one often thinks of zeolites or metal organic frameworks when nanoporous materials are mentioned [1], pores in crystalline semiconductors can be produced in a wide range of geometries, giving rise to properties quite distinct from bulk materials and metamaterials. These materials have attracted considerable and increasing interest, lead by porous carbon materials that have been the topic of research for many decades [2]. Porous carbon can be obtained via mechanical rolling of thermally expanded graphite flakes, chemical vapour deposition and vacuum filtration of dispersions of graphene sheets or carbon nanotubes, or pyrolysis of thermosetting polymer precursors [3][4][5][6][7]. Such materials exhibit unique, tuneable physicochemical properties, and hold great promise in the fields of catalysis, water treatment, biofiltration, gas separation, fuel cells and optoelectronics due to their structural integrity, continuity and purity [8][9][10][11][12][13].Although it does not have the long history of porous carbon, porous silicon also exhibits unique properties suitable for a range of applications. Porous silicon can be obtained a variety of ways, including anodization [14], stain etching with acids [15, 16] and direct chemical synthesis from silicon tetrachloride using self-forming salt byproducts which are later removed [17]. Porous silicon has been used in sensing, tissue engineering, medical therapeutics and diagnostics, photovoltaics, rechargeable batteries, energetic materials, photonics, and micro electro mechanical systems [18]. Porous silicon was also found in 1995 to be either resorbable, bioactive or bioinert depending on the porosity, making it unique among the porous semiconductors [19].In contrast, porou...