Yvan Velenik
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 2d answered Why do we work in thermodynamic limit in statistical physics? Feb 1 comment Relation between the $N$ particle partition function and probability? I agree with the answer, but disagree with the characterization of the partition function as the most important quantity in statistical physics (even though it is often presented as such in textbooks). This central role should be reserved to the probability measure itself. Indeed, the latter gives you access to much more information (even about macroscopic quantities) than the partition function, which only gives you access to the statistical properties of the macroscopic quantities appearing in the Boltzmann weight: energy, magnetization, etc.). Jan 28 awarded Custodian Jan 28 reviewed Approve What exactly “triggers” a matter/antimatter detonation? Jan 22 comment Reference request: 2D conformal field theory and functions on the triangular lattice You should google "discrete complex analysis". There are many papers introducing these ideas, for example those by Chelkak, Smirnov, etc. Jan 22 comment Cluster Expansion Done. I tried to make a readable answer out of the comments, but had only limited time, so there might be typos. Jan 22 answered Cluster Expansion Jan 22 comment Cluster Expansion Yes you sum over all possible values of $n_\ell$ for each possible values of $\ell$ (so $\{n_\ell\}$ specifies the values of $n_1, n_2, n_3, \ldots$). Then, once these are fixed, you take the product of all the functions $f_\ell(n_\ell)$ (for these specific values of $n_1,n_2,n_3,\ldots$). Jan 22 comment Cluster Expansion Sure. Imagine that the only allowed cluster sizes are $\ell=1$ and $\ell=2$ (so that I can write things down explicitely). Let us use the notation $f_\ell(n_\ell) = \frac{1}{n_\ell!}\bigl( \frac{e^{\ell\beta\mu}b_\ell}{\lambda^{3\ell}\ell!} \bigr)^{n_\ell}$. Then your identity becomes $\sum_{\{n_1,n_2\} \in\{0,1,2,\ldots\}^2} \prod_{\ell=1}^2 f_\ell(n_\ell) = \sum_{n_1\geq 0} \sum_{n_2\geq 0} f_1(n_1) f_2(n_2)= \sum_{n_1\geq 0} f_1(n_1) \sum_{n_2\geq 0} f_2(n_2)= \prod_{\ell=1}^2 \sum_{n_\ell\geq 0} f_\ell(n_\ell)$ Jan 21 comment Cluster Expansion This is just linearity of the sum. Maybe it will become obvious if you look at the following particular case: $\sum_{i,j} a_i b_j = \sum_i \sum_j a_i b_j = \Bigl(\sum_i a_i\Bigr)\Bigl(\sum_j b_j\Bigr)$, which follows by pulling out $a_i$ from the inner sum and then pulling out $\sum_j b_j$ from the outer sum. Now, in your formula $\{n_\ell\}$ denotes the number of clusters of each possible length (so $\sum_{\{n_\ell\}} = \sum_{n_1\geq 0}\sum_{n_2\geq 0}\cdots = \prod_{\ell\geq 1} \sum_{n_\ell\geq 0}$). Jan 19 comment What are alternative ways to think about transfer matrix as used in Ising model? @Nathaniel : yes, that's exactly the point. If you denote by $\varphi^{*,1}$ the left Perron-Frobenius eigenvector (associated, of course, to the same eigenvalue $\lambda_1$), then the only thing that changes is the expression for the invariant measure, which becomes $\mu( \sigma) = \varphi^{*,1}_\sigma \varphi^1_\sigma$. (Note also that you could define another Markov chain with transition probabilities $\pi^*(\sigma,\sigma') = \frac{\varphi^{*,1}_{\sigma'}}{\lambda_1\varphi^{*,1}_\sigma} T_{\sigma',\sigma}$; this corresponds to the time-reversed chain (which has the same invariant measure). Jan 19 comment What are alternative ways to think about transfer matrix as used in Ising model? @Nathaniel : thanks for your appreciation (and the unexpected bounty). Concerning the nonsymmetric case, I might either add a (short) second part to the answer, in which I point out the relevant changes, or simply point them out in the comments. What would be the best solution? Jan 19 awarded Mortarboard Dec 29 comment annealed randomness vs quenched randomness Quenched randomness means that the disorder is sampled first and then equilibrium statistical mechanics is applied to the system's other degrees of freedom with this particular frozen disorder. Annealed means that you average on the disorder at the same time as you take the thermal average over the other degrees of freedom. Dec 7 comment What is the difference between toy models and normal models? @Ooker : yes, it is a caricature, keeping enough relevant features to make it useful for the discussion of a particular aspect of the phenomenon, while keeping the model tractable enough to make a detailed analysis possible. Dec 5 comment What is the difference between toy models and normal models? @Ooker: the point of the Ising model is certainly not to provide quantitative information (even in a limit), but rather to provide a rather simple, yet very rich model in which a great variety of fundamental issues can be investigated. As a matter of fact, it does model adequatly a number of systems, but that's far from its main purpose. Universality also guarantees that it does provide a good description of the critical behavior of a wide class of (real) systems. Dec 4 comment Extending the ergodic theorem to non-equilibrium systems I am not at all an expert in these topics, but you might have a look at the book Mathematical Theory of Nonequilibrium Steady States, Lecture Notes in Mathematics, Volume 1833, 2004, and references therein. If you want something shorter, maybe look at this review by Ruelle. Dec 4 comment Extending the ergodic theorem to non-equilibrium systems @JánLalinský : I think that he's interested in "open" Hamiltonian systems, for which Liouville's theorem indeed does not hold. Nov 28 comment Minimization of energy for non-equilibrium systems at steady state (NESS)? No, it's not "a matter of definition", except if you wish for every physicist to use its own set of definitions for everything... There is a very clear definition of equilibrium systems, to which NESS do not belong: equilibrium systems are systems with time-invariant statistical properties and no macroscopic flow of matter or energy. The distinction is not gratuitous: the formalism of equilibrium statistical physics does not apply to NESS (and the same is true of equilibrium thermodynamics). Nov 27 comment Minimization of energy for non-equilibrium systems at steady state (NESS)? Yes, and @David, note that a lot of work has been done specifically for the type of stochastic dynamics that you seem to have in mind; see, e.g., this paper and papers citing the latter.