The aim of this article is to review the literature dealing with the deformation step in the phenomenon of film formation from a latex. It will be shown that the situation of this problem in the literature is quite confusing. The article will be divided in two parts. The first will recall the classical theories proposed in the past to account for the deformation of latex particles in the film formation process, namely the dry sintering theory by Dillon et al., Brown's capillary theory, the wet sintering theory by Vanderhoff et al., and the surface layer theory by Sheetz. The second part will deal with following works which were all attempts to experimentally verify and/or improve the main theories.One can distinguish three steps in the process of film formation from a latex (/, 2). i) In the first step, water evaporates at a constant rate until a stage is reached where particles form a dense packing of spheres. The solid volume fraction, for a latex monodispersed in size, is then close to 0.74. An additional condition for high packing fraction is sufficient colloidal stability. Otherwise, a less ordered structure with lower polymer volume fraction will result. ii) At the beginning of the second step, particles show at the surface of the latex, and the rate of water evaporation decreases. Forces start to act which ensure the deformation of the particles in such a way that polymeric material fills all the space. Acting forces have to surmount the mechanical resistance of the particles against deformation. The spheres are transformed into rhombic dodecahedra. A rhombic dodecahedron has 12 rhombic faces, and 14 vertices of two types. Six vertices correspond to 4-fold axes, and 8 to 3-fold axes. It is not easy to draw this polyhedron. A schematic representation can be found in reference 3. They can also be observed in beautiful freeze fracture micrographs of poly(butyl methacrylate) latex films (4). At this stage, interfaces between particles still exist (5). For latexes, the compaction/deformation step is favorable from a thermodynamical point of view