[Halld-physics] correlations in neutral shower parameters
Mark M. Ito
marki at jlab.org
Fri Aug 19 09:52:21 EDT 2011
Richard et al.,
A general comment: it seems some of these correlations are weak and in
fact we may never have sensible values for them. If we are going for a
compact format, we might think about initially dropping the off-diagonal
elements that are only non-zero in principle.
I'm worried about keeping a significant amount of zero-valued data as a
place-holder for future use and having that future never arrive.
As an extreme version of this, you can imagine a near-diagonal
representation where none of the off-diagonal elements are kept. Don't
know if this is actually possible. It likely would mean a
parametrization aligned with detector geometry rather than an abstract
global coordinate system.
For tracking, the off-diagonal elements arise naturally in the process
of fitting and some of the correlations are certainly significant. So
the values are both non-zero and meaningful; they should be kept.
-- Mark
On 08/18/2011 06:19 PM, Richard Jones wrote:
> In laying out the dst format for MC studies, I claimed in an earlier
> message that the error matrix used to store the errors on neutral hit
> parameters only needs to contain 3 (bcal) or 2 (fcal) off-diagonal
> elements. Our argument follows below. The starting point for this is
> a single cluster reconstructed in the bcal or fcal. No vertex
> hypothesis has yet been applied to this hit, nor has a momentum vector
> been assigned to it. It is just a neutral cluster in a calorimeter.
>
> 1. *bcal* - the set of measured hit parameters which are most
> loosely coupled in terms of the raw measurements are
> (r,phi,z,E,t). A transformation can be used to convert into any
> other preferred set of hit parameters. Correlations are (r,z) ,
> (r,E) , and (z,E).
> * phi is decoupled from all of the others.
> * r is directly measured through the radial profile, but
> couples to z and E implicitly.
> * z is independently measured using timing, but is
> implicitly correlated with r through fluctuations in the
> energy deposition for oblique showers, and with E through
> the position of the shower maximum, and explicitly with E
> through the attenuation correction.
> * E correlates implicitly to r,z through shower depth
> variations, and explicitly to z through the attenuation
> correction.
> * the t of the shower maximum correlates with r,z (and
> through them with E). However this correlation is
> trivial, and will be taken out when the time is projected
> back from the shower maximum to a reference vertex. Since
> the speed of light is independent of E, this correlation
> of t with r,z is trivial and need not be carried along
> with the shower.
> 2. *fcal* - the set of measured hit parameters which are most
> loosely coupled in terms of the raw measurements are (x,y,E,t).
> Note that the depth z of the shower maximum is not measured in
> the fcal, so it does not belong in the list, being a pure
> function of E. Correlations are (x,y) , (x,E) , and (y,E).
> 1. x,y are implicitly correlated with each other by the shape
> of shower deposition in the fcal, and with E through
> shower depth.
> 2. as for the fcal, the t of the shower maximum is trivially
> correlated with E,x,y. I argue that this correlation is
> trivial and need not be carried along with the shower
> object for the same reasons as given above under the bcal
> heading.
>
> Thus, for the bcal we must keep 3 off-diagonal error matrix elements
> per shower. For the fcal there are also 3 non-trivial off-diagonal
> elements, but two of them are related to each other in a simple way:
>
> x * sigma(y,E) = y * sigma(x,E)
>
> So strictly speaking there are only 2 off-diagonal error matrix
> elements per shower that must be kept in the fcal.
>
> -Richard J.
>
>
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