In the last few years research activities have been focused on the modification of fiber properties with nano-scaled additives. One of the most important fields of research is the alteration of mechanical properties such as the tenacity and the specific breaking load. In this study, we determined the influence of nano-phyllosilicates on the drawability of polyamide 6 multifilament yarns. It was first demonstrated that the drawability of the fibers drastically increased in an industrially relevant high-speed melt spinning process. Structural properties of the material are identified by wide-angle X-ray diffraction (WAXD) and differential scanning calorimetry (DSC). Changes in the crystalline properties as well as in the alignment of the silicates are compared with the stress-strain curves of the fibers, and a molecular mechanism for the drawing process is derived from these experiments. In a first step, a significant phase transition in the crystalline structure unaffected by the silicates occurs for low draw ratios (DRs). Beyond this point, where unmodified fibers start to break, a gliding between the silicate layers takes place, which is responsible for an extended drawability of the fibers. This mechanism leads to new possibilities for fiber processing, which can be used to research ultra-fine filaments in future studies.Polyamide 6 (PA6), also called Polycaprolactam or Perlon as a trademark, is a polymer of the group of polyamides. It was first synthesized by means of ringopening polymerization reactions from "-aminocaprolactam in 1938. 1 The '6' in the name denotes the number of carbon atoms in the repeating base molecule. The resulting sequence in the polymer chain is À½HN À ðCH 2 Þ 5 À CO n À. 2 The polymer is a polymorphic, semi-crystalline material. Three different thermodynamic, metastable phases can coexist in the glassy or rubbery solid state. 3,4 The so-called g phase is crystalline with a monoclinic unit cell. The lattice parameters are known as a ¼ 9.33 Å and c ¼ 4.78 Å perpendicular to the polymer chains as well as b ¼ 16.88 Å in the polymer chain direction from wide-angle X-ray diffraction (WAXD) experiments. The value of the angle between a and c axis is 121 . 5 Since g is around 120 , a pseudohexagonal version of this unit cell can be calculated and is often used in theory for the structural description. 4 The second crystalline phase denoted as the a phase also has a monoclinic cell with lattice parameters a ¼ 9.56 Å , b ¼ 17.24 Å , and c ¼ 8.01 Å with an angle ¼ 67.5 . 6 As distinguished from the a and g phase, the phase as the third stable phase is characterized by a mesomorphic structure. The short-range order exceeds the typical values for an amorphous material. Since no long-range order exists