A comparison is presented of the structural changes occurring in porous glass during laser-induced hot and cold compaction. The changes occurring in modified regions of different compaction processes when a porous-glass plate with a micro-region is sintered in a furnace are also compared.In recent years a great deal of attention has been devoted to the formation of modified regions (MR) of different sizes and shapes on the surface and in the interior of optically transparent materials as well as to the formation of 3D microstructures of arbitrary complexity, openings and channels, comprising the basis of photonic devices widely used in integrated optics and laser engineering. Laser microprocessing for the formation of such MR has undergone intensive development [1,2]. Such development was possible because of the relative simplicity and high workability of laser methods as compared with, for example, those based on photolithography. Work is now being done on the formation of MR using different materials, such as glass with complex composition, including doped with transition metals [3], fused quartz [4] and other high-silica compounds, such as porous glasses (PG), which are products of through chemical etching of two-phase alkali-borosilicate glass [5, Chap. 10], and quartzoid glasses (QG) [6], obtained when PG are sintered in a furnace [1].Near-IR and visible-range (l < 800 nm) femtosecond lasers are usually used as the radiation source for forming MR with all of the shapes mentioned [2]. As a rule, 10.6 mm cw CO 2 lasers [1, 7] and UV-range (l > 250 nm) lasers [8], whose radiation lies in the fundamental absorption range of glass, are used to form MR on a PG surface.Porous glasses possess a number of properties including the following: transparency in the visible range; optical strength combined with regulatable nano-range pore sizes; thermal, chemical and microbiological stability; stable properties during prolonged operation; and, unique adsorption properties [9]. All this makes PG promising materials for creating MR on a surface and in the interior.Local modifications of PG structure which are based on heating by laser radiation are presented in [1], where cw and pulsed CO 2 lasers (l = 10.6 mm) were used as sources of laser radiation. The heating of PG due to the absorption of laser radiation within the interaction region results in hot compaction, i.e., transformation into quartzoid and, correspondingly, the formation of a quartzoid MR. Such a MR surrounds a so-called transitional layer, whose porosity varies evenly from zero in the MR to that of the PG plate [10,11]. The dimensions and shape of the thermally compacted region can be set by changing the parameters of the laser radiation (intensity, focusing spot size, scan rate during ruling).Hot compaction by laser radiation is local and differs from furnace sintering [12] by the fact that the heating of PG is limited to approximately the cross section of the beam; it starts at the surface, and then the hot-compaction boundary advances into the interior of ...