[Loops] EM loci
Klimchuk, James A. (GSFC-6710)
james.a.klimchuk at nasa.gov
Tue Sep 28 06:39:07 MDT 2010
Thanks, Giulio. You make many excellent points. I have two quick comments. First, the DEM distributions for dynamic and static loops can be vastly different (theoretically). Second, I agree completely that we need to pay more attention to the diffuse emission, which is much stronger than the emission contained in discrete loop features. I hope people realize that the Loops Workshops are not restricted to discrete loops. Every closed magnetic flux tube can be thought of as a loop, even those that make up the diffuse corona.
Thanks again,
Jim
> -----Original Message-----
> From: loops-bounces at solar.physics.montana.edu [mailto:loops-
> bounces at solar.physics.montana.edu] On Behalf Of Giulio Del Zanna
> Sent: Tuesday, September 28, 2010 5:10 AM
> To: A mailing list for scientists involved in the observation and modeling of
> solar loop structures
> Subject: Re: [Loops] EM loci
>
>
> Dear Jim et al.,
>
> there seems to be a bit of confusion and some elephants in the room,
> so I list a few clarifications below.
>
> - I believe it was my 'fault' to re-introduce in 2003 the old EM loci method to
> study AR loops for the first time, and to show that *most* 'warm' loops
> are nearly isothermal at each location.
> I have to agree that, despite the limitations of the method, this is an useful
> SOHO/CDS result, that so far has been confirmed by Hinode/EIS (in general,
> iso-thermality appears to be the norm in AR structures, rather than
> multi-thermality).
>
> - I did not and would not 'trust' too much any EM method, however forward
> modelling the line intensities in the loops (see Del Zanna & Mason 2003)
> gave consistent results (though still static).
>
> - Of course, it has been known for a very long time that any dynamics in the
> loops will change the shape of any DEM/EM distributions, but by not too
> much I believe.
> I've shown in 2007 how clear patterns of dopplershifts are present in
> coronal
> loops from Hinode/EIS, so we now have some extra observational
> constraints.
>
> - One elehpant in the room is the problem that large (up to a factor of 10)
> discrepancies are present in any EM modelling, when the lines from the
> 'anomalous' ions are considered. This was obvious even in the Pottasch
> (1963)
> results but went un-noticed until 1971 and has since been considered by
> very
> few people (Phil Judge is one of them). There are a lot of erroneous
> statements
> in the literature by the way (interested readers should look at some of my
> papers).
>
> - Even when considering lines from ions 'well behaved', the largest variations
> in results are coming from the use of different ion abundances.
> The latest ionization and recombination rates we have in CHIANTI are giving
> results for some ions that are quite different, for example.
>
> - The EM loci plots were first introduced by K. Strong in 1978 I believe, and
> not by Pottasch who did something very different. The method is often not
> explained (I am afraid to say understood) properly.
>
> - As any EM method, the EM loci will not give you an unique solution.
>
> - To measure the electron temperature, there are better methods.
> In the last couple of years I showed that some diagnostics (athough very
> limited)
> for coronal loops are available from Fe VII, Fe VIII, Fe IX and Fe XI lines
> observed by Hinode/EIS. It is a start.
> When proposing for new instruments I always suggest that some
> temperature
> diagnostics should be included..
>
> - Another elphant in the room is the unresolved AR emission. It was ignored
> until the first loop meeting when I and Peter Young showed how dominant it
> is.
> I am glad to see that it is now a comonly-accepted issue.
> All EUV imagers are inherently multi-thermal, so it is more
> difficult to use them to measure the unresolved AR emission, compared to a
> spectrometer.
> Ideally, we would need two spectrometers with high spatial resolution and
> very different viewing angles.
>
>
>
> Giulio
> --
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