I don't think you need this: Raul> match_dataset_grids(data_vec1); Raul> match_dataset_grids(data_vec2); since it looks like the vec1 is MEG and the vec2 is HEG - the +1 and -1 orders are already on the same grid. This isn't necessary, but could be nice if you want to look at the fluxed arrays: Raul> flux_corr(data_vec1); Raul> flux_corr(data_vec2); I think your fit might be spurious because you left it totally unconstrained. Try setting some reasonable limits on the parameters: Raul> set_par("xaped(1).norm",1,0); Raul> set_par("xaped(1).temperature",1e+7,0); set_par("xaped(1).temperature",1e+7,0, 1.e6, 1.e8); Since AtomDB is low-density only, this has no effect, so leave it frozen at 1.0: Raul> set_par("xaped(1).density",1,0); The norm is % this is 1.e-14 * VEM / (4*PI*d^2), which will require an estimat, or better, we'll renorm_counts when ready: set_par("xaped(1).norm", 1.e-3, 0, 0.0, 0.1 ); Raul> list_par; Raul> exclude( all_data ); Raul> include(data_vec1); Raul> group_data( data_vec1, 4 ); Raul> xnotice( data_vec1, 1.7, 25 ); Delta Ori probably has low nH. If you have an estimate, set it and freeze it.. NH will be degenerate with temperatures and abundances. To get and estimate using a isothermal plasma, you might do: set_par( "phabs(1).nH", 0.1, 0, 0, 0.5); Delta Ori also has slightly broadened lines, I think, so try the following: use_thermal_profile; % to turn on thermal + turbulent broadening set_par( "xaped(1).vturb", 300, 0, 0.0, 1000); Check the params to see if they have reasonable ranges, or are left at some reasonable frozen value: list_par; Now get a better guess for the norm: renorm_counts; list_par; popt.res = 4; % for combined residuals plot_counts( -data_vec1, popt ); And adjust the norm limits, if needed. Now try the fit, and see if it converges on something reasonable, within the limits of a low-density, isothermal model. The emission measure should at least be well constrained. You might need to allow the ovarall metal abundances to be free (you might give individual abundances can be specified in the plasma state variable in a future refinement, once the basics are working). You will get a bad fit for some lines --- the forbidden lines are photexcited away, and there is no density- or photoexcitation-dependence in AtomDB. You might ignore the intercombination and resonance lines in the triplets until you get a reasonable fit (which also might not be possible with an isothermal plasma). Then you could try the photoexcitation models from <http://space.mit.edu/cxc/analysis/he_modifier/>. -- Dave ---- You received this message because you are subscribed to the isis-users list. To unsubscribe, send a message to isis-users-request_at_email.domain.hiddenwith the first line of the message as: unsubscribeReceived on Thu May 23 2013 - 15:43:33 EDT
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