[d2n-analysis-talk] Dilution Factors
Matthew R. Posik
tua88437 at temple.edu
Thu Apr 21 12:15:36 EDT 2011
Hi Greg,
On Wed, Apr 20, 2011 at 8:56 PM, Gregg B. Franklin <gbfranklin at cmu.edu>wrote:
> Matt,
> The plots you have are very interesting. The dilution factor at low
> x is a much bigger effect than we were anticipating. I think we should
> first try to make sure we agree on the dilution factor determined by the
> reverse polarity run at 4.7 GeV. It would be useful to plot 1-D instead
> of D since D gets close to 1.0 through much of our range. Lets make
> sure we agree on the runs, the cuts, etc.
>
I plotted 1-D. Again D is defined as:
D = 1-(Q-/Q+)*(N+/N-),
Q-, N- is the accumulated charge and total counts from the negative
polarity runs 2024-2195
Q+, N+ is the accumulated charge and total counts from the positive
polarity runs 2199-2212
The plot pos_outrun_1mdilution.eps shows 1-D. Since the higher x bins are
near 0 here I also plotted it on log scale (pos_outrun_1mdilution_log.eps)
I also plotted 1-D' for the negative polarity runs 2024-2195 using
BB.optics.charge==-1 for electrons and BB.optics.charge==1 for positrons
Again here D' is defined as
D' = 1 - N-/N+
where N- are the total counts with charge==-1
N+ are the total counts with charge==1
You can see a plot of 1-D' pos_inrun_1mdilution.eps
>
> We also want to check the asymmetry, also. If it is large, this is a
> big problem in addition to just "dilution factor". We need to at least
> put a bound on the asymmetry.
>
I Computed the raw positron asymmetry from the positive polarity runs. I
will send that result out in a separate email.
>
> For the 5-pass data, the following strategy might work if we have
> enough statistics.
>
> 1) Start with the 4.7 GeV data and determine the positrons (from reverse
> polarity running) normalize by charge as a 2-D function of momentum and
> scattering angle. Call this 2D histogram 1. It will have to be course
> binned.
>
> 2) Do the same for positrons determined from the negative (normal
> polarity) running at 4.7G. In both cases, we should have mostly just
> positrons. Call this histogram 2.
>
I will get started on getting these histograms.
>
> 3) Determine the ratio of Hisogram 2) over Histogram 1) bin by bin
> should give use the relative acceptance for positrons as a function of
> scattering angle and momentum. (Our statistics will be poor at high x,
> but hopefully the positrons aren't a problem there.)
>
> I don't think positrons will be an issue here, looking at the dilution
factors that I got using the two different methods, they seem to both agree
pretty well at large x and both say very few positrons at large x.
> 3) For the 5-pass data, make hisogram 3 with similar bins for positrons.
> This will be for the normal polarity, which means the acceptance will
> be very different than for the real data. However, you can use the
> ratios (bin by bin) determined in step 3 to correct for this. The
> problem might be that the "4-pass" data may have low statistics in
> kinematics bins that become important at 5-pass.
>
> In the longer run, we can try to understand this ratio with Monte Carlo.
> If there is a large asymmetry and therefore can depend on the target
> polarization direction, it will be harder.
>
> Regards,
> Gregg
>
>
>
> --
> Prof. Gregg B Franklin
> Head, Department of Physics
> Carnegie Mellon University
> phone: (412) 268-2743 fax: (412) 681-0648
> _______________________________________________
> d2n-analysis-talk mailing list
> d2n-analysis-talk at jlab.org
> https://mailman.jlab.org/mailman/listinfo/d2n-analysis-talk
>
--
Matthew Posik
Email: posik at temple.edu
Temple University Physics Dept.
Office: BA-319
Office #: 215-204-1331
WebSites:
Temple:
http://quarks.temple.edu/
d2n:
http://hallaweb.jlab.org/experiment/E06-014/
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