domenicodigangi / ScoreDrivenExponentialRandomGraphs

Score Driven Exponential Random Graphs Models
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Compare Psudo-SDERGM and SDERGM for toy model dirBin0Rec0 #27

Open domenicodigangi opened 3 years ago

domenicodigangi commented 3 years ago

Altought the physical bounds are always satisfied there are issues when the natural paramters get close to them. One possible way to define the time evol for eta and theta is the following :

  • choose a scaling for alpha

    • alpha~const dense scaling
    • alpha~1/(N-1) sparse scaling
  • choose a scaling for beta, s.t. it remains well within the bounds : 0 + c3<beta<alpha/2 - c4 . Where we assumed alpha<1/2, and choose c3 and c4 to guarantee that beta stays well within the bounds. E.g. we would like to have at least a few rec pair on average, i.e. beta = min_n_pairs/(N^2-N)
  • define a dynamics for alpha and beta, that remains well within the bounds. Then transform the obtained paths for alpha and beta in paths for theta and eta and use the latters for the dgp
domenicodigangi commented 3 years ago

written tested and compared on SIN and AR

domenicodigangi commented 3 years ago

Tried some scalings that return weird results for SIN filter of large N

domenicodigangi commented 3 years ago

Notes on the model and the relation between parameters in the mean value (alpha and beta) and natural parametrizations (eta theta)

dirBin0Rec0_exp_var_par_maps

dirBin0Rec0_exp_var_par_maps 2

domenicodigangi commented 3 years ago

Altought the physical bounds are always satisfied there are issues when the natural paramters get close to them. One possible way to define the time evol for eta and theta is the following :

domenicodigangi commented 3 years ago

The approach of defining the dynamics in the space of mean values, i.e. alpha and beta (mean density and reciprocity), transform to natural par space and use the latter as dgp, seems to work. Indeed the mapping induces some highly nonlinear transformation effectively forcing theta and eta to be counterciclycal, and non precisely sin shaped (sin with random phase was the original dgp as shown in the attached figure)

dgp_non_linear_map

domenicodigangi commented 3 years ago

Attached recap email mail_toy_model_ML_vs_PML_filter.pdf

domenicodigangi commented 3 years ago

Update da call 4/12/2020:

domenicodigangi commented 3 years ago

Ho aggiunto le formule delle note al pdf in overleaf

domenicodigangi commented 3 years ago

Riguardo i problemi riscontrati dai filtri (both mle e pmle) in caso di dgp definito in modo naive: example_filter_issue_naive_dgp, penso che l'intuizione sulla regione di osservabilitá a N (numero di nodi) finito sia confermata da alcune simulazioni fatte. Ricapitolando: