Abstract
Iron-based alloys are widely used as structural components in engineering applications. This calls for a fundamental understanding of their mechanical properties, including those of pure iron. Under operational temperatures the mechanical and magnetic properties will differ from those of ferromagnetic body-centered-cubic iron at 0 K. In this theoretical work we study the effect of disordered magnetism on the screw dislocation core structure and compare with results for the ordered ferromagnetic case. Dislocation cores control some local properties such as the choice of glide plane and the associated dislocation mobility. Changes in the magnetic state can lead to modifications in the structure of the core and affect dislocation mobility. In particular, we focus on the core properties of the $\frac{1}{2}\ensuremath{\langle}111\ensuremath{\rangle}$ screw dislocation in the paramagnetic state. Using the noncollinear disordered local moment approximation to address paramagnetism, we perform structural relaxations within density functional theory. We obtain the dislocation core structure for the easy and hard cores in the paramagnetic state, and compare them with their ferromagnetic counterparts. By averaging the energy of several disordered magnetic configurations, we obtain an energy difference between the easy- and hard-core configurations, with a lower, but statistically close, value than the one reported for the ferromagnetic case. The magnetic moment and atomic volume at the dislocation core differ between paramagnetic and ferromagnetic states, with possible consequences on the temperature dependence of defect-dislocation interactions.
Highlights
Iron and iron alloys, like steels, are the most technologically important metallic systems and have been so for millennia
The differential displacement (DD) maps show no substantial change between paramagnetic and ferromagnetic states, magnetic disorder does not affect the structure of the dislocation core
It should be noted that the hard core is stabilized in the paramagnetic state in our disordered local moment approach (DLM) calculations, while in the ferromagnetic state, the hard core can be stabilized only by fixing the coordinates of the core atoms along the Burgers vector direction
Summary
Like steels, are the most technologically important metallic systems and have been so for millennia. As such, they are currently being used as structural materials in nuclear energy applications and they are candidates for generation nuclear technology [1]. They are currently being used as structural materials in nuclear energy applications and they are candidates for generation nuclear technology [1] In many of these applications they are subjected to high operational temperatures. High temperature increases magnetic disorder, and when the critical temperature is reached, 1043 K in the case of bcc iron, the system no longer exhibits any long-range magnetic ordering, the local spin polarization of the atoms is still present.
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