[b1_ana] draft proposal v02

Oscar Rondon-Aramayo or at cms.mail.virginia.edu
Sat May 4 13:37:49 EDT 2013


Hi,

So, we're back to the difference of counts, eq. (19) or eq. (20) of my 
method.

In terms of eq. (20), the combined charge calibration and efficiency 
"drifts" over ~20 hours will have to be less than ~ 0.8%, just like I 
discuss around eq. (14) of my draft, in order to match the HERMES error.

 From JP's comments cited by Dustin, it looks like the efficiency component 
could be 0.1% or less. I leave it to the experts to say what the charge 
calibration drift could be. It needs to be < 0.3% to have a systematic 1/2 
that of HERMES.

I am posting the LaTex source of my method on my b1 page, if it can be of 
any help
http://twist.phys.virginia.edu/~or/b1/

Just to make everything clear, in my eq. (20), f is not the usual dil. fac. 
It is defined at the top of p. 3, before eq. (11).

Cheers,

Oscar



On Sat, 4 May 2013 11:25:59 -0400 (EDT)
  Dustin Keller <dustin at jlab.org> wrote:
> Hi,
> As I mentioned these relative errors you seem to be pointing too have
> already been considered at least to a small degree.  What I am concerned
> with is when steve says:
> 
> "With a rate of switching polarization states of hours or days,
> there will be drifts in things, drifts that get magnified
> because this measurement is a subtraction of large numbers.  I
> don't know what the target (f * Pzz * delta-Azz) is, but it is
> 10^-something where something is certainly >= 4.  If, for
> example, the detector efficiency were to drift by 1% between
> the two polarization states, and this drift was unknown, it
> would be a complete killer.
> 
> I think the main systematic drift effects will be
> 1.  Drifts in beam current measurement calibration
> 2.  Drifts in detector efficiency
> 3.  Drifts in luminosity"
> 
> This statement (to me) seems to request a demonstration that
> the drifts do not lead to a deltaAzz much larger than 1*10^-4.
> 
> The key point here is that if J.P. what right about the drifts
> 1% is seen in about 90 days for 2.)  But its 1.) that may still
> need some explanation.
> 
> dustin
> 
> 
> 
> On Sat, 4 May 2013, Oscar Rondon-Aramayo wrote:
> 
>> Hi,
>>
>> Actually, since Q and epsilon are only factors of Np, Nu, they aren't 
>>scales
>> of Azz. Steve is right. We still have a difference: Np/Nu - 1, with Np/Nu 
>>~
>> 1.
>>
>> So, we need to keep track of Q and e even in the statistical error. The 
>>only
>> way of doing this right is to propagate the errors for both Q's and e's in
>> detail.
>>
>> Oscar
>>
>>
>> On Fri, 03 May 2013 21:38:37 -0400
>>  "Oscar  Rondon-Aramayo" <or at cms.mail.virginia.edu> wrote:
>>> Hi,
>>>
>>> To further remove any confusion about our method and its errors, I suggest
>>> that instead of writing eq. (19) in terms of charge normalized, efficiency
>>> corrected counts, we display the charges and efficiencies explicitly, and
>>> use raw counts. Although we stated the kind of counts we are using in that
>>> eq. just above it, it seems Steve missed it.
>>>
>>> Per eqs. (32) and (33) in the appendix 2.2.3, this means just moving Q's
>>> and epsilons to the l.h.sides, since N1 and N are indeed raw counts there,
>>> and don't make any approximations, like Q1 ~ Q, etc.
>>>
>>> Then, the l.h.s. of eq. (34) would be
>>>
>>> (Q/Q1)*(e/e1)*(N1/N) and
>>>
>>> eq. (19) becomes
>>>
>>>  Azz =  2/(f*Pzz)*[(Q/Q1)*(e/e1)*(N1/N) - 1]
>>>
>>> where it's evident that Q's and e's are normalizations or scale factors,
>>> just like f and Pzz, and change the text above the equation to say raw
>>> counts, not normalized and corrected ones.
>>>
>>> I don't see any other way to make it any clearer.
>>>
>>> And, of course, we need to emphasize somewhere that the statistical error
>>> is
>>> always based on the RAW counts.
>>>
>>> Cheers,
>>>
>>> Oscar
>>>
>>>
>>>
>>> On Fri, 3 May 2013 17:43:55 -0400
>>>  Karl Slifer <karl.slifer at unh.edu> wrote:
>>>> Hi all,
>>>>
>>>> I got a ton of comments, and I think I've implemented them all.  I think
>>>> the most substantial pertain to the following: (equation numbers refer to
>>>> the attached draft)
>>>>
>>>> Eq 17 and 19: Azz expressed as ratio - 1 as suggested by Oscar
>>>>
>>>> Eq 22 : Total time expressed in terms of R_T as noted by Patricia and
>>>> concurred by Ellie and Oscar.
>>>>
>>>> Page 23 Charge determination systematic : modified to reflect Oscar and
>>>> JP's suggestions
>>>>
>>>> There were a lot more, so please double check that your suggestions have
>>>> been satisfactorily included.
>>>>
>>>> The overhead and target sections are still in progress.  Anyone have time
>>>> to help with that?
>>>>
>>>> thanks,
>>>>
>>>> Karl
>>>>
>>>>
>>>> ---
>>>> Karl J. Slifer
>>>> Assistant Professor
>>>> University of New Hampshire
>>>> Telephone : 603-722-0695
>>>
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