[b1_ana] Fwd: Uncertainties in measuring b1/Azz
Dustin Keller
dustin at jlab.org
Fri May 3 17:55:09 EDT 2013
this is a very very small effect, but it is the reason to
keep the temperature the same in each case.
On Fri, 3 May 2013, J. P. Chen wrote:
> Dustin,
>
> I guess Steve also worried the change/drift in target
> thickness/density. Due to beam heating and He4 cooling,
> target can be slightly different at different time period.
>
> Cheers.
>
> Jian-ping
>
> On 5/3/2013 5:42 PM, Dustin Keller wrote:
>> I not sure why he lists luminosity as an additional issue. We have a good
>> handle on acceptance differences so its really just beam current
>> calibration differences and drift in detector efficiency.
>>
>> dustin
>>
>>
>>
>>
>> On Fri, 3 May 2013, Patricia SOLVIGNON wrote:
>>
>>>
>>> Begin forwarded message:
>>>
>>>> From: "Stephen A. Wood" <saw at jlab.org>
>>>> Subject: Uncertainties in measuring b1/Azz
>>>> Date: May 3, 2013 4:40:27 PM EDT
>>>> To: Patricia Solvignon-Slifer <solvigno at jlab.org>
>>>>
>>>> Patricia:
>>>>
>>>> Thank you for showing me the document describing estimates of errors in
>>>> measuring b1.
>>>>
>>>> The formula for estimating statistical errors (or rather time needed to
>>>> achieve a given statistical precision) looks correct to me.
>>>>
>>>> In the discussion of systematic errors, the uncertainties discussed
>>>> appear to mostly relate to the scale of b1 or Azz. While important,
>>>> these scale systematics are not the dominant systematics. The main
>>>> systematic will be unknown differences in the calibrations, efficiencies,
>>>> luminosities etc between the two polarization states.
>>>>
>>>> This is similar to experiments with polarized beam, particularly parity
>>>> experiments, where one worries that about unknown differences in rate
>>>> between the two helicities that are not due to the physics of interest.
>>>> These differences could be due to fluctuations in target density,
>>>> fluctuations in beam current measurement calibration etc. In such
>>>> experiments, these systematics are mitigated by reversing the beam
>>>> polarization quickly so that efficiencies, target densities etc don't
>>>> have time to drift.
>>>>
>>>> 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
>>>>
>>>> I am sure there are others.
>>>>
>>>> There can be many subtle effects in any of these. BCM efficiency could
>>>> depend on ambient temperature which will have daily variations as well as
>>>> several hour variations due to AC cycling. The BCM calibration at
>>>> different currents could be different, making
>>>>
>>>> Detector efficiency can drift for a variety of reasons, for example
>>>> including fluctuations in gas quality, HV drift or drifts in spectrometer
>>>> magnetic field.
>>>>
>>>> There can be difficult to know changes in luminosity. As I understand
>>>> it, the target is a set of discrete beads. So, when the beam moves, the
>>>> thickness of the target seen by the beam changes. Or if the amount of
>>>> helium seen by the beam changes, the rate changes.
>>>>
>>>> It may be that all of these systematics can be addressed, but it may not
>>>> be possible to make a completely convincing case by the the of the PAC.
>>>> But I think it is important to acknowledge all the systematics you can
>>>> think of and acknowledge the difficulty of beating them down. (Otherwise
>>>> PAC members or the technical review will point them out.) There are
>>>> things that can be pointed to such as the big effort that went into
>>>> modernizing BCMs for g2p and Qweak. Some of that effort may be useful in
>>>> this case. It would be good to sketch out a plan for studying the
>>>> systematic effects. There will be plenty of time to do parasitic
>>>> systematic effects studies during the experimental program that will
>>>> precede an eventual b1 run.
>>>>
>>>> It would be helpful if you could remind me of the expected numerical
>>>> values of f and Pzz, and the desired deltaAzz.
>>>>
>>>> Steve
>>>
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