Abstract
Suppose we have a simple bar magnet. We know it is a ferromagnet because it is capable of picking up thumbtacks, the number of which is called the order parameter M. As we heat this system, M decreases and eventually, at a certain critical temperature T c , it reaches zero: no more thumbtacks remain! In fact, the transition is remarkably sharp, since M approaches zero at T c with infinite slope. Such singular behavior is an example of a “critical phenomenon.”
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Stanley, H.E. (1999). Scaling, Universality, and Renormalization: Three Pillars of Modern Critical Phenomena. In: Bederson, B. (eds) More Things in Heaven and Earth. Springer, New York, NY. https://doi.org/10.1007/978-1-4612-1512-7_39
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