Termodinâmica de um gelo de spin artificial regravável

• Ano de defesa: 2018
• Autor(a) principal: Rodrigo Alves Stancioli
• Tipo de documento: Dissertação
• Tipo de acesso: Acesso aberto
• Idioma: por
• Instituição de defesa: Universidade Federal de Minas Gerais; UFMG
• Palavras-chave em Português: Gelo de spin artificial; transições de fase; simulação; Carlo; método de Monte; Método de Monte Carlo; Modelos de spins; Transição de fase; Simulação
• Link de acesso: http://hdl.handle.net/1843/SMRA-BBKFXG

Artificial spin ices (ASI) are geometrically frustrated, two-dimensional arrays of magnetic nanoislands, originally designed to mimic the behavior of pyrochlore spin ice materials. Different types of ASI have been developed lately, giving rise to interesting phenomena such as magnetic monopole-like excitations, as well as suggesting the possibility of newapplications. A novel geometry of ASI recently proposed in the literature has been termed "rewritable" artificial spin ice, for it allows total control over the microstates of the system at room temperature. Although the reported experimental realization of this particular system is essentially athermal, recent techniques permit the fabrication of nanoislandssusceptible to thermal fluctuations, which makes it important to investigate the thermal behavior of ASI. We have performed Monte Carlo simulations of a model of the rewritable ASI, with nanoislands being treated as Ising macrospins with dipolar interactions, in orderto study its phase transitions in the absence of a magnetic field. Both periodic and open boundary conditions have been considered. The ground state has been determined to be maximally magnetized, and an ordered phase has been observed at low temperatures.In the thermodynamic limit, a continuous transition between this ordered phase and a paramagnetic one is evidenced by the divergence of the specific heat curve at the critical temperature. In finite systems, however, a low temperature pseudo-phase transition takes place, introducing an intermediary phase between the paramagnetic and fully magnetizedphases which has few local excitations and shows low net magnetization values. The critical temperature has been determined by means of a new method based upon the energy probability distribution zeros. In future works, we intend to further investigate the nature of this pseudo-transition, as well as the behavior of excitations in the lattice.