Contents:

Method for data scoring:

This assessment is provided as a (very rough) guide to the quality of the experimental data. The lower a score, the better.The score is computed by: Score = aveDev + sqrt(varDev) + (2004-pubYear)/5 + pubTypeFactor.

The pubTypeFactor is a cheezy measure of the amount of peer review a data set has received. It is given by:

The aveDev is computed by first creating an average evaluation from all the evaluations for the specific reaction. With that, we loop over the data and compute the average deviation from the average evaluation and the data. The uncertainty on the data are not taken into account (this is done in the evaluation scoring). Similarly, the varDev is the variation in the deviation of the data and the average evaluation. Together, these two quantities tell us whether the data has the right magnitude (low aveDev) and the right shape (low varDev).

In addition to the raw score, some comments are generated. They come in two flavors: a raw assessment of the shape of the data and an assessment of the score itself. The assessment of the shape is straightforward and relies on aveDev and varDev:

The assessment of the score itself is just a straightforward comment regarding the Score:

Method for fit quality assesment:

This assessment is provided as a guide to determine whether it is possible to perform a reasonable fit to the data. If so, then we recommend either finding a recent evaluation in which the evaluators actually performed a fit to the data or performing a fit yourself.

We now list the column labels and their meaning:


Method for evaluation scoring:

To determine whether an evaluation is suitable, we first compute the evaluation's chi^2/nData:

chi^2/nData = (1/nData) sum_{i=1}^{nData} (sigma_i^{exp} - sigma^{eval}(E_i))^2}/(delta sigma_i^{exp})^2

Eventually we will compare each evaluation's chi^2/nData to a predetermined parameter eta_cut for each energy range and choose the evaluation with the lowest chi^2 from all of the suitable evaluations. These calculations come with the following caveats: Once we have computed the chi^2/nData for each of the evaluations in an energy region, we can loop through them and make a guess as to which evaluation is the "best" one. Only evaluations that have a chi^2/nData < 1010 are considered (This sounds like a lot, but one big dataset in the resonance region with small uncertainties and bad normalization can do it!).

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UCRL-WEB-210095
David Brown 2005-01-31