[b1_ana] Axx
Narbe Kalantarians
narbe at jlab.org
Fri Apr 26 13:14:36 EDT 2013
Hi Karl,
I agree that this is what we concluded with at the end of the meeting
yesterday.
1 thing that I just wanted to mention;
The time dependence between +/- P_zz could be handled, possibly in the
sense of systematics, provided that they're both in the same orientation
(i.e. either para. or perp.) If it were to be a difference of para. and
perp., then it becomes a major challenge.
Also, Steve Wood has offered to take an early look at our numbers before
we submit. This might be a good idea.
Narbe
On 04/26/2013 12:22 PM, Karl Slifer wrote:
>
> Hi,
>
> While it would be easier to run with only positive Pzz, there is no
> technical or theoretical reason that I know of that prevents us from
> using negative pol. This will require target development to achieve
> large negative as well as positive tensor polarizations, along with
> careful study of the systematics in extracting these values. I
> thought we all agreed on this yesterday....And I also see no technical
> or theoretical reason (other than it is difficult and will require
> R&D) which limits the enhanced tensor polarization to 10%. I believe
> Don, Chris, Josh would all agree with this, atleast they all did when
> I talked to them within the last 6 months.
>
> So to be clear, I believe we can propose an experiment where we
> enhance the m=0 population (via rf saturation or by using two
> independent microwave sources) and measure N_0 unpolarized electrons
> inclusively scattered while in this state, and then we deplete the m=0
> state to obtain a positive polarization and measure N_1 unpolarized
> electrons scattered while in this state. Then we form the asymmetry
> (with appropriate numerical factors). The Pzz will not be the maximal
> positive or negative value in either state, but we can correct for
> this by the relative Pzz in each state. One significant concern is
> that this introduces time dependent systematics since it will likely
> require some time to switch between the two states. This has to be
> studied, but I do not see it as a fundamental limitation.
>
> After careful study of the systematics, its possible that the cross
> section difference method may well turn out to be the best way to do
> the experiment, but I suspect we will struggle mightily to convince a
> very skeptical PAC in 30 mins that we really can control all the
> systematic effects to the level needed for a cross section measurement.
>
> With this in mind, I think it is reasonable to aim for conditional
> approval based on demonstration of the target performance to the level
> needed (+-20% tensor pol with about 5% relative uncertainty). I
> believe we can defend these as reasonable goals, although we should
> get something in the way of a support statement from Don or Chris.
> And I believe conditional approval is a highly desirable state, since
> the target groups will not be able to commit serious R&D to this
> without an approved experiment for motivation. In addition, it opens
> the door to attract more theory support and start consideration of
> several other possible experiments.
>
> my few further cents,
>
> Karl
>
>
>
>
>
>
>
>
>
>
> ---
> Karl J. Slifer
> Assistant Professor
> University of New Hampshire
> Telephone : 603-722-0695
>
>
> On Fri, Apr 26, 2013 at 11:04 AM, Dustin Keller <dustin at jlab.org
> <mailto:dustin at jlab.org>> wrote:
>
> As I mentioned in the meeting using the notation Axx can be
> mis-leading especially in the case of DIS where azimuthal
> control is not obvious. However the relationship for
> sigma^{+/-} for m=+1,-1 is sigma^{+/-}=sigma^u(1+(1/2)AzzPzz).
> If you believe that then Axx=Azz, and the conclusion is the same.
> If you call it Axx or Azz in either case you just measure the
> ratio of polarized and unpolarized cross sections. This will lead
> to a target tensor polarization of about 10%. There are certainly
> other systematic concerns but this is the best we can do target wise.
>
> dustin
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