Therefore, the manganites are intrinsically inhomogeneous at length scales of nanometers due to the strong electronic correlations. A SHP099 mouse phenomenological Ginzburg-Landau theory approach is also developed by using a Landau free-energy function and introducing the term of electronic softness to rationalize the possibility of phase coexistence and electronic inhomogeneities [93]. In this approach, magnetic and charge modulations are argued to coexist in new thermodynamic phases in contrast to Stem Cells inhibitor the previous models where the phase separation originates from disorder or as a strain-induced kinetic phenomenon. This approach leads to a rich diagram of equilibrium phases, qualitatively similar to those

seen experimentally. The success of this approach argues for a fundamental reinterpretation of the nature of charge modulation in manganite materials, from a localized to a more extended ‘charge-density wave’ picture. The same symmetry considerations that favor textured coexistence of charge and magnetic order may apply to many electronic systems with competing phases. The resulting ‘electronically soft’ phases of matter with incommensurate, inhomogeneous, and selleck products mixed order may be general phenomena in correlated systems. Figure 9 Phase diagram of two-orbital model in one-dimensional and T ~0 including Jahn-Teller phonons, obtained with Monte Carlo

techniques [[90]]. S-F labels a spin-ferromagnetic configuration. O-F, O-AF, and O-D denote a state where the orbital degrees of freedom are ordered uniformly, staggered or they are disordered, respectively; PS indicates a phase separated state, and AF

in an antiferromagnetic state. The Hund-coupling is J H = 8, the Heisenberg coupling between localized classical spins J AF = 0.05, both in units of the hopping amount the same orbitals. Since a number of competing energy scales are operative in manganite oxides giving rise to a large number of electronic orders such as spin, charge, and orbital (and associated lattice order), the emergence of these orders Phospholipase D1 and the associated couplings between them should be considered in a full Hamiltonian model for manganites, which makes the theoretical understanding of the EPS quite complex. Much work is further needed in this challenging area of research. Conclusions In recent years, a remarkable progress has been achieved in understanding the EPS phenomenon in low-dimensional perovskite manganite nanostructures such as manganite nanoparticles, nanowires, nanotubes, and nanostructured films/patterns. This progress is mainly made possible by building upon the experimental measurements and theoretical approaches, and clearly establishes the phase completion as the main source of the CMR effect in manganite oxides. The shape and scale of EPS are different for different systems with electronic domain sizes ranging from a few nanometers to several micrometers.