Porous materials have attracted tremendous scientific and industrial interest due to their broad commercial applicability. However, some applications require that these materials are deposited on surfaces to create thin films. Here, the recent progress of new porous thin-film material classes is described: porous organic molecular materials, porous organic polymers, covalent organic frameworks, and nanoporous carbon. In each case, the state of the art and current barriers in their thin-film fabrication, as well as intrinsic material advantages that are suited for different applications are presented. By highlighting the unique structural characteristics and properties of these materials, it is hoped that increased research development and industrial interest will be fostered, which will lead to new methods of thin-film synthesis and consequently to new applications. Figure 2. 1) Structure, crystal packing and BET surface area of triptycene trisbenzimidazolone (TTBI), 2) structure and BET surface area of OMIM-10-14, 3) structure of Doonan cage C1 and BET surface area of the two different crystalline polymorphs obtained by slow and fast precipitation, 4) structure and BET surface area of a triptycene-based cage, 5) structure of Cooper Cage CC3 (cyclohexyl vertices). A) Schematic low-energy crystal packings for CC1 (hydrogens on vertices; formally nonporous), CC2 (methyl vertices; 1D external pore channels), and CC13 (dimethyl vertices; 2D layered pore structure with formally disconnected voids). As such, small structural changes to the vertex groups lead to three quite different crystal packings and pore topologies for the α polymorphs shown here (orange = disconnected voids; yellow = interconnected pores). Crystallization in the presence of 1,4-dioxane causes pseudoisostructural window-to-window packing for all three cage modules, causing the materials to mimic the 3D diamondoid pore structure of CC3 shown in D. B) N 2 sorption isotherms (77 K) for homochiral CC3 produced by freeze-drying (green diamonds, 6 repetitions), vacuum evaporation (blue triangles), standard reaction (black squares), and slow crystallization (red circles, 6 repetitions). C,D) Molecular simulation of amorphous packing (top) and crystalline structure (bottom) of CC3, with the Connolly surface probed by N 2 molecules (kinetic diameter of 3.64 Å) shown in blue, and average BET surface area extracted from the isotherms shown in (B). 1) Reproduced with permission. [58] Figure 12. A) CDC thin-film synthesis and EDLC test cell preparation. Titanium is extracted from titanium carbide as TiCl 4 , forming a porous carbon film. Two carbide plates with the same CDC coating thickness are placed face to face and separated by a polymer fabric soaked with electrolyte. The SEM image (left) shows a representative image of a CDC/TiC interface with a good film adhesion. Reproduced with permission. [187]