Yvan Velenik
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 Jun 10 answered Can temperature be a complex number? Jun 10 awarded Organizer Jun 10 revised Transition from one state to another in Quantum Mechanics Removed irrelevant tag Jun 10 suggested approved edit on Transition from one state to another in Quantum Mechanics Jun 4 comment Local and global detailed balance Well, I am not sure about the physicists's terminology, but I guess that they refer to local detailed balance for the condition you wrote (it should be $k(x,y)\rho(x)=k(y,x)\rho(y)$ (for all $x$ and $y$), by the way), and to global detailed balance for the weaker condition $\sum_x \rho(x) k(x,y) = \rho(y)$ (for all $y$). In Markov chain theory, the latter characterizes the stationary distribution, while the former implies in addition that the Markov chain is reversible w.r.t. this distribution. May 31 comment Is 'Boltzon' an accepted name for particles following Maxwell-Boltzmann (MB) statistics? Some people also use Boltzmannons. There is no final consensus on this terminology. May 28 comment What is normal fluctuation? He probably means that the fluctuations of the relevant quantity (here the energy) follow a normal distribution. Actually, here he seems happy with the weaker claim that the scale of these fluctuations are of the right order (the variance is of order $N$). May 13 comment Statistical Mechanics vs Statistics First of all, the terminology statistical mechanics is rather unfortunate, and it would have been much better to call this theory probabilistic mechanics, for example. Indeed, the concepts and techniques of probability theory play an essential role in statistical mechanics (even if they are, quite wrongly, somewhat hidden in many books and courses). Statistics, however, is mostly irrelevant to statistical mechanics. May 11 comment 1 dimensional Ising model @Math_overview: Well, the way the Hamiltonian and free energy are defined here, the $\log 2$ term is fine. What makes you think this is incorrect if you agree with the computations? May 3 comment Percolation and number of phases in the 2D Ising model @Math_overview: Thanks for your positive feedback on the book. I am happy you find it useful. There will be a chapter on the variational approach to (translation invariant) Gibbs states at some point, but for the moment, we're working on one chapter on reflection positivity and one on the Pirogov-Sinai theory. May 3 comment Percolation and number of phases in the 2D Ising model @Math_overview: yes, this is correct ($\nu$-almost surely, of course). See Chapter 6 of our book, in particular Section 6.3.1. Apr 26 awarded Yearling Apr 15 comment Legendre transformation: non-convex/non-convave functions One deals with such situations by using the more general Legendre-Fenchel transformation (see the article "Convex conjugate" on wikipedia). Morally, this amounts to taking the Legendre tranformation of the convex envelope of your function (so you lose information in this way). This turns out to be the relevant conept in particular in statistical physics. In the latter, nonconvex thermodynamic potentials appear naturally in mean-field theories and, when this occurs, equivalence of ensembles is violated. Mar 26 comment How to understand singularities in physics? Not sure about your second part. Phase transitions are defined as singularities of thermodynamic potentials, because this is what one seems to observe experimentally. Statistical mechanics then tells you that these singularities are in fact only approximate (they only exist in the ideal limit of infinite systems). The "real" functions remain smooth, although they mimic very closely singular behaviour. Mar 7 comment Phase Transition at Zero Temperature (Not QPT) I still don't see what you mean. In the 1d Ising model, the thermal fluctuations restore the symmetry which is broken at $T=0$ (the model is symmetric whenever $T\neq 0$, but is not symmetric when $T=0$). This is the opposite of what you seem to say. Mar 6 comment Phase Transition at Zero Temperature (Not QPT) I am not sure I understand your analogy: in the 1d Ising model, $T=0$ is the only temperature at which the symmetry is broken. In any case, this is of course extremely general: the same will be true (at the classical level) for any one-dimensional model with compact spins, and periodic interactions. This, of course, includes models with continuous symmetry (the one-dimensional $O(N)$-models, for example). Jan 15 answered Correlation length in d>1 Ising model, at zero temperature Jan 2 comment Why are large scale structures isotropic in the Ising model? Note that the latter result has been only proved in dimension $2$, and there it results from the fact that surface tension becomes isotropic in this limit, for very much the same reason the 2d random walk converges to Brownian motion. Jan 2 comment Why are large scale structures isotropic in the Ising model? What do you mean by "the phase separated 'blob' pattern that forms when the Ising model is quenched"? Do you mean the shape of the droplet of one phase immersed inside the other, when the magnetization is fixed at a value between $m^*$ and $-m^*$? If yes, then this shape is not rotation invariant, since the surface tension is not and the shape is obtained by the Wulff construction. It is true, however, that (properly rescaled) this shape converges to a disk as $\beta\downarrow\beta_c$. Dec 29 comment What is the central charge of the disordered $q$-state Potts model, for large $q$? The phase transition of the Potts model is first-order for $q\geq 5$ (in two dimensions), there is no critical point.