The arrangement of low-angle boundaries and the subgrain structure of crystals with high ( 2 106 crn-$) dislocation density are considered. Relations to estimate cross dimensions and misorientations of nucleating subgrains are derived. Production conditions for single crystals without nucleating low-angle boundaries are described and relations to estimate the critical dislocation density, below which subgrain nucleation is highly improbable, are supplied. Macrosubgrain formation mechanisms are described. Growing conditions for crystals free of macrosubgrains are formulated. Equations to estimate their cross dimensions and misorientations are proposed. These are compared with the available experimental data for a variety of materials.PaccMoTpeHa cxeMa pacnonomemm Manoymosbix rpamu, II 6~10q~ofi CTPJ'KTJ'PH KPHC-oqeHKH nonepewbix p a 3~e p o~ II p a a o p~e~~a s~f i 3apom~amlq11xc~ BJIOHOB. Y K~~~H H TaJIJIOB C B61COKOfi ( 2 lo5 CM-') IIJIOTHOCTbH) HHCJIOKaUHfi. QaHbI COOTHOUIeHHR AJIR