diff toolboxes/FullBNT-1.0.7/bnt/CPDs/@discrete_CPD/Old/convert_to_pot.m @ 0:e9a9cd732c1e tip

first hg version after svn

--- /dev/null	Thu Jan 01 00:00:00 1970 +0000
+++ b/toolboxes/FullBNT-1.0.7/bnt/CPDs/@discrete_CPD/Old/convert_to_pot.m	Tue Feb 10 15:05:51 2015 +0000
@@ -0,0 +1,44 @@
+function pot = convert_to_pot(CPD, pot_type, domain, evidence)
+% CONVERT_TO_POT Convert a tabular CPD to one or more potentials
+% pots = convert_to_pot(CPD, pot_type, domain, evidence)
+%
+% pots{i} = CPD evaluated using evidence(domain(:,i))
+% If 'domains' is a single row vector, pots will be an object, not a cell array.
+
+ncases = size(domain,2);
+assert(ncases==1); % not yet vectorized
+
+sz = dom_sizes(CPD);
+ns = zeros(1, max(domain));
+ns(domain) = sz;
+
+local_ev = evidence(domain);
+obs_bitv = ~isemptycell(local_ev);
+odom = domain(obs_bitv);
+T = convert_to_table(CPD, domain, local_ev, obs_bitv);
+
+switch pot_type
+ case 'u',
+  pot = upot(domain, sz, T, 0*myones(sz));  
+ case 'd',
+  ns(odom) = 1;
+  pot = dpot(domain, ns(domain), T);          
+ case {'c','g'},
+  % Since we want the output to be a Gaussian, the whole family must be observed.
+  % In other words, the potential is really just a constant.
+  p = T;
+  %p = prob_node(CPD, evidence(domain(end)), evidence(domain(1:end-1)));
+  ns(domain) = 0;
+  pot = cpot(domain, ns(domain), log(p));       
+ case 'cg',
+  T = T(:);
+  ns(odom) = 1;
+  can = cell(1, length(T));
+  for i=1:length(T)
+    can{i} = cpot([], [], log(T(i)));
+  end
+  pot = cgpot(domain, [], ns, can);   
+ otherwise,
+  error(['unrecognized pot type ' pot_type])
+end
+