By Manfred Opper, David Saad

ISBN-10: 0262150549

ISBN-13: 9780262150545

An immense challenge in smooth probabilistic modeling is the large computational complexity considering common calculations with multivariate chance distributions whilst the variety of random variables is big. simply because precise computations are infeasible in such circumstances and Monte Carlo sampling ideas may possibly succeed in their limits, there's a want for ways that let for effective approximate computations. one of many least difficult approximations relies at the suggest box approach, which has a protracted background in statistical physics. the strategy is familiar, really within the growing to be box of graphical models.Researchers from disciplines corresponding to statistical physics, laptop technological know-how, and mathematical records are learning how you can increase this and similar tools and are exploring novel program parts. prime ways comprise the variational procedure, which matches past factorizable distributions to accomplish systematic advancements; the faucet (Thouless-Anderson-Palmer) procedure, which includes correlations by means of together with potent response phrases within the suggest box thought; and the extra common tools of graphical models.Bringing jointly principles and strategies from those various disciplines, this ebook covers the theoretical foundations of complex suggest box tools, explores the relation among the several methods, examines the standard of the approximation received, and demonstrates their program to varied components of probabilistic modeling.

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**Extra resources for Advanced Mean Field Methods: Theory and Practice**

**Example text**

For instance, for the Ising model on a square lattice, it is known as the Bragg-Williams approximation [3] and it is generalized to other models in the Landau theory [10]. One can show that the above lower bound corresponds to the first term in a Taylor series expansion of the free energy around a factorized model. This Taylor series can be continued and the second order term is known as the Thouless Anderson Palmer ( TAP ) correction [16; 13; 6; 7]. The second order term significantly improves the quality 38 Hilbert J.

We first consider the first order mean field equation. Setting the lhs of Eq. ¢o:) e 0: = L (¢o:) si,e - log qi(si) + constant 0: (16) The constant term collects all contributions that are independent of Si. These terms do not have to be considered, because they are absorbed in the normalisation of qi. Eq. (16 ) can be reformulated as (17 ) 2 For instance, when Q contains three binary variables, cp",(x"') is an 8-dimensional vector. Mean Field Theory for Graphical Models 43 in which the constants Zi follow from normalisation.

45 Mean Field Theory for Graphical Models 5 Sigmoid belief networks In this section, we illustrate the geometric mean field approach for sigmoid belief networks on binary variables, defined as (21) a( x) (1 + exp( _2 x) )-1, Xi ±1 and hi is the local field: hi( x) L7=1 Wij Xj + (h Since nodes can have a large number of parents, computation of where = = = the marginal distributions for the sigmoid belief network is intractable in general. This is also the case in the presence of evidence. When evidence is present, we separate the total set of variables in evidence variables e and the remaining hidden variables s: x (s, e).

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