The theoretical study of instabilities, thermal fluctuations, and topological defects in the crystal-rotator-I-rotator-II () phase transitions of n-alkanes has been conducted. First, we examine the nature of the phase transition in nanoconfined alkanes. We propose that under confined conditions, the presence of quenched random orientational disorder makes the phase unstable. This disorder-mediated transition falls within the Imry-Ma universality class. Next, we discuss the role of thermal fluctuations in certain rotator phases, as well as the influence of dislocations on the phase transition. Our findings indicate that the Herringbone order in the -phase and the Hexatic order in the -phase exhibit quasi-long-range characteristics. Furthermore, we find that in two dimensions, the unbinding of dislocations does not result in a disordered liquid state.

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