<html><head><meta http-equiv="content-type" content="text/html; charset=utf-8"></head><body dir="auto">Hi Chan,<div><br></div><div>I dont know the details of your classification, but my first impression is yes. If you have a reliable classification then you can (in principle) not apply z vertex cuts. You can just use your butanol events as chosen by the classification And your carbon events for establishing the bound nucleon contributions. This would of course need to be studied in a systematic way and a classification uncertainty needs to be established. It looks like you were also able to remove the ice build up downstream the carbon target. Might be good to see the missing masses originating from the two targets. A quick check for your classification would be to plot the missing mass of events coming with z vertex that selects the first half of your target (any events away from the carbon target ). Then scale this and see if you can get the missing mass distribution to match the one from your classified butanol events. If it does, it means you are correctly removing any contributions from the carbon target which would only contribute to background. If you fail to match the free proton peak and the bound nucleon contributions it means that the classification might need some work.<br><br><div dir="ltr">Sent from my iPhone</div><div dir="ltr"><br><blockquote type="cite">On 28 Dec 2019, at 21:26, Chan Kim <kimchanwook@gwmail.gwu.edu> wrote:<br><br></blockquote></div><blockquote type="cite"><div dir="ltr"><div dir="ltr"><div>Thank you for your replies.</div><div><br></div><div>@Michael, <br></div><div>For the z-vertex plot, only p<300MeV particles are removed. I will change the momentum selection region and see how z-vertex resolution changes as soon as I have other steps finished. I kept them for now, so I can compare my asymmetry with and without particles with p=[300, 400] MeV. <br></div><div><br></div><div>@Nick,</div><div>In regards to free polarized proton contributions in carbon vertex (left tail of the carbon distribution), would it be ok to use classification results from machine learning? Below is a plot of separation of butanol and carbon in small angles. <br></div><div><a href="https://clasweb.jlab.org/rungroups/g9/wiki/images/0/06/Zvrt_1bin_angle.png">https://clasweb.jlab.org/rungroups/g9/wiki/images/0/06/Zvrt_1bin_angle.png</a><br></div><div><br></div><div>Thank you,</div><div>Chan<br></div><div> <br></div></div><br><div class="gmail_quote"><div dir="ltr" class="gmail_attr">On Sat, Dec 28, 2019 at 12:42 PM Nicholas Zachariou <<a href="mailto:nickzachariou@gmail.com">nickzachariou@gmail.com</a>> wrote:<br></div><blockquote class="gmail_quote" style="margin:0px 0px 0px 0.8ex;border-left:1px solid rgb(204,204,204);padding-left:1ex">Dear Chan,<br>
<br>
I have done several studies on this that should be documented in my analysis note. As Michael said, the difficulty lies in the determination of the dilution factor. If you are using carbon data to determine this, then you need to make sure you account correctly for free polarised proton contributions within your carbon vertex cut that actually comes from butanol events (this is different than the ice built up). If you are using parametrization of the bound nucleon contributions then the dilution is more straightforward, but you would need to think/study free unpolarised proton contributions to butanol events from the ice built up downstream your carbon target. This can been done by varying the butanol z vertex cut andcomparing your determined observable. There are several ways you can do this and we can chat more if needed.<br>
<br>
Best regard,<br>
Nick<br>
<br>
Sent from my iPhone<br>
<br>
> On 28 Dec 2019, at 16:23, Michael Dugger <<a href="mailto:dugger@jlab.org" target="_blank">dugger@jlab.org</a>> wrote:<br>
> <br>
> Chan,<br>
> <br>
> The variables that are important are polar angle and momentum of the<br>
> identified particle. Did you keep the low momentum protons?<br>
> <br>
> When it comes to choosing the range of vertex selection for each target,<br>
> the method you use for removing the bound nucleon content might be a<br>
> factor. From the plots you created, you can see the difficulty that you<br>
> face at low angle.<br>
> <br>
> At low polar angle you have the case that there very well could be some<br>
> leakage of carbon vertices in your butanol definition. This could cause<br>
> dilution factors to be messed up.<br>
> <br>
> I would cautiously move forward concentrating on the bins that look good.<br>
> Once everything was running well for the "good" stuff, I would start<br>
> trying to fix the more difficult bins.<br>
> <br>
> Take care,<br>
> Michael<br>
> <br>
>> Hello Michael,<br>
>> <br>
>> The pi0 mass shifting from 125MeV (slide 2) to 134MeV (slide 6) happened<br>
>> simply due to a change in number of bins. On slide 6, I tried to have the<br>
>> same binning for both ELOSS and ELOSS+momentum correction<br>
>> distributions,causing inaccurate peak locations. After momentum<br>
>> correction,<br>
>> the mmsq distribution has much sharper peaks. So, 125MeV is the correct<br>
>> value of mmsq after ELOSS distribution, but for ELOSS + momentum<br>
>> correction, I will redo the calculation. Sorry for the confusion.<br>
>> <br>
>> I have another question regarding the z-vertex resolution in angles. Below<br>
>> is a plot that Eugene suggested to make (Z-vertex position in bins of<br>
>> photon energies and angle bins).<br>
>> <a href="https://clasweb.jlab.org/rungroups/g9/wiki/images/a/ac/Zvrt_select_lab.png" rel="noreferrer" target="_blank">https://clasweb.jlab.org/rungroups/g9/wiki/images/a/ac/Zvrt_select_lab.png</a><br>
>> <br>
>> As you can see, the z-vertex resolution is very poor in small scattering<br>
>> angles, unable to clearly distinguish the butanol and carbon region. do<br>
>> you<br>
>> have any suggestions in choosing the selection ranges for small angles..?<br>
>> <br>
>> Thank you,<br>
>> Chan<br>
>> <br>
>> <br>
>> <br>
>> <br>
>> <br>
>> <br>
>> <br>
>> <br>
>> <br>
>>> On Thu, Dec 26, 2019 at 4:53 PM Michael Dugger <<a href="mailto:dugger@jlab.org" target="_blank">dugger@jlab.org</a>> wrote:<br>
>>> <br>
>>> Chan,<br>
>>> <br>
>>> It is probably a good idea to try and keep the low momentum events, but<br>
>>> I<br>
>>> would start out by removing them. Once you feel like you have everything<br>
>>> else under control, then you add in the p < 400 MeV/c events.<br>
>>> <br>
>>> You can see if the momentum cut makes the pi0 mass closer to the nominal<br>
>>> value. Essentially, you just recreate slides 2 and 6 from your December<br>
>>> 18<br>
>>> update:<br>
>>> <br>
>>> <a href="https://clasweb.jlab.org/rungroups/g9/wiki/images/9/94/FROST_2019_12_18.pdf" rel="noreferrer" target="_blank">https://clasweb.jlab.org/rungroups/g9/wiki/images/9/94/FROST_2019_12_18.pdf</a><br>
>>> <br>
>>> Note: On slide 2 you have pre-ELOSS mass of pi0 = 196 MeV and post-ELOSS<br>
>>> mass of pi0 = 125 MeV. BUT on slide 6 you have post-ELOSS mass of pi0 =<br>
>>> 134 MeV!! How did that happen? Then after ELOSS + momentum correction<br>
>>> the<br>
>>> pi0 mass = 89 MeV. You want to get that all straightened out with the p<br>
>>>> <br>
>>> 400 MeV/c events. You mass of the pi0 after the ELOSS and momentum<br>
>>> corrections should be the correct value. The momentum correction is<br>
>>> designed to bring the pi0 mass to the correct value.<br>
>>> <br>
>>> Take care,<br>
>>> Michael<br>
>>> <br>
>>>> Hello Michael,<br>
>>>> <br>
>>>> Yes, I now understand what you are saying about the momentum<br>
>>> acceptance<br>
>>>> varying rapidly between 300 and 400 MeV around scattering angle of<br>
>>> 35deg.<br>
>>>> <br>
>>>> Would it be a bad idea to apply different low momentum cuts for<br>
>>> particles<br>
>>>> under 35deg and above 35deg? So, 400MeV for particles with angle <<br>
>>> 35deg<br>
>>>> and 300MeV for particles with angle >35deg.<br>
>>>> Because for higher energy photon events (photon energy > 1 GeV), it<br>
>>> looks<br>
>>>> like there are lots of events in p = [350, 400] MeV region.<br>
>>>> <br>
>>>> Thank you,<br>
>>>> Chan<br>
>>>> <br>
>>>> <br>
>>>> On Tue, Dec 24, 2019 at 3:50 AM Michael Dugger <<a href="mailto:dugger@jlab.org" target="_blank">dugger@jlab.org</a>><br>
>>> wrote:<br>
>>>> <br>
>>>>> Chan,<br>
>>>>> <br>
>>>>> For these sorts of plots it is interesting to make an additional MM^2<br>
>>>>> cut.<br>
>>>>> If you make a missing mass cut near the mass of the pion, you<br>
>>> restrict<br>
>>>>> the<br>
>>>>> events to have the kinematics of<br>
>>>>> <br>
>>>>> gamma p -> p pi0 .<br>
>>>>> <br>
>>>>> As it currently stands, you are showing the theta versus momentum<br>
>>>>> distribution for all possible reactions. This is not a bad thing and<br>
>>> the<br>
>>>>> plots have interesting features.<br>
>>>>> <br>
>>>>> The depletion stripes are probably bad time-of-flight paddles. You<br>
>>> can<br>
>>>>> see<br>
>>>>> from the depletion stripes how the magnetic field is bending the path<br>
>>> of<br>
>>>>> the charged particles as a function of momentum.<br>
>>>>> <br>
>>>>> The enhancement stripes are probably from the reaction gamma p -> p<br>
>>> pi0<br>
>>>>> (compare to<br>
>>> <a href="https://userweb.jlab.org/~dugger/pi0PphaseSpacePlotNew.png" rel="noreferrer" target="_blank">https://userweb.jlab.org/~dugger/pi0PphaseSpacePlotNew.png</a><br>
>>>>> ).<br>
>>>>> <br>
>>>>> You can clearly see the acceptance in polar angle and momentum. For<br>
>>>>> angle<br>
>>>>> above 35 degrees, it looks like the momentum acceptance is rapidly<br>
>>>>> changing between 300 and 400 MeV/c. This is probably the clearest<br>
>>>>> evidence<br>
>>>>> that a cut at 400 MeV/c is appropriate. For angles below ~35 degrees<br>
>>> the<br>
>>>>> momentum acceptance issue is being caused by a bad time-of-flight<br>
>>>>> paddle.<br>
>>>>> <br>
>>>>> Take care,<br>
>>>>> Michael<br>
>>>>> <br>
>>>>>> Hello All,<br>
>>>>>> <br>
>>>>>> Here is a plot of momentum vs lab angle in bins of photon energies.<br>
>>>>>> <br>
>>>>> <br>
>>> <a href="https://clasweb.jlab.org/rungroups/g9/wiki/images/2/2e/Low_mome_select_p_abs_theta.png" rel="noreferrer" target="_blank">https://clasweb.jlab.org/rungroups/g9/wiki/images/2/2e/Low_mome_select_p_abs_theta.png</a><br>
>>>>>> <br>
>>>>>> Thank you,<br>
>>>>>> Chan<br>
>>>>>> <br>
>>>>>> On Mon, Dec 23, 2019 at 3:47 PM Chan Kim<br>
>>> <<a href="mailto:kimchanwook@gwmail.gwu.edu" target="_blank">kimchanwook@gwmail.gwu.edu</a>><br>
>>>>>> wrote:<br>
>>>>>> <br>
>>>>>>> Hello Michael,<br>
>>>>>>> <br>
>>>>>>> Thank you for your suggestion! I should have been more clear about<br>
>>>>> the<br>
>>>>>>> plots. The mmsq distribution I sent out yesterday was prior to any<br>
>>>>> event<br>
>>>>>>> selections.<br>
>>>>>>> <br>
>>>>>>> I have two quick questions..<br>
>>>>>>> 1. For momentum ranges of [0.31, 0.39] GeV, the mmsq distribution<br>
>>>>> (ones<br>
>>>>>>> I<br>
>>>>>>> sent yesterday) look like a gaussian distribution centered near 0,<br>
>>>>> plus<br>
>>>>>>> a<br>
>>>>>>> bump at 1GeV. Are these events bad because of these bumps at 1GeV?<br>
>>>>>>> <br>
>>>>>>> 2. Are events with backward scattering angles not good because<br>
>>> they<br>
>>>>>>> don't<br>
>>>>>>> have information from DC?? since the drift chamber only covers<br>
>>> from<br>
>>>>> 8deg<br>
>>>>>>> to<br>
>>>>>>> 142deg???<br>
>>>>>>> <br>
>>>>>>> Regards,<br>
>>>>>>> Chan<br>
>>>>>>> <br>
>>>>>>> On Mon, Dec 23, 2019 at 3:33 PM Michael Dugger <<a href="mailto:dugger@jlab.org" target="_blank">dugger@jlab.org</a>><br>
>>>>> wrote:<br>
>>>>>>> <br>
>>>>>>>> Hi,<br>
>>>>>>>> <br>
>>>>>>>> The last plot was for pion lab-momentum and lab-angles and the<br>
>>>>>>>> center-of-mass angle definitions were also messed up :(<br>
>>>>>>>> <br>
>>>>>>>> I have a new plot at<br>
>>>>>>>> <br>
>>>>>>>> <a href="https://userweb.jlab.org/~dugger/pi0PphaseSpacePlotNew.png" rel="noreferrer" target="_blank">https://userweb.jlab.org/~dugger/pi0PphaseSpacePlotNew.png</a><br>
>>>>>>>> <br>
>>>>>>>> The above plot shows that the momentum values below 400 MeV ARE<br>
>>>>>>>> important<br>
>>>>>>>> for MANY kinematic bins.<br>
>>>>>>>> <br>
>>>>>>>> However, even with the knowledge that we would be killing a bunch<br>
>>> of<br>
>>>>>>>> bins,<br>
>>>>>>>> we may have to remove events with momentum below 400 MeV due to<br>
>>> our<br>
>>>>>>>> possible inability to reconstruct the missing pi0 at low<br>
>>> momentum.<br>
>>>>>>>> <br>
>>>>>>>> Sorry about any confusion my previous plot may have caused.<br>
>>>>>>>> <br>
>>>>>>>> Take care,<br>
>>>>>>>> Michael<br>
>>>>>>>> <br>
>>>>>>>> <br>
>>>>>>>>> Eugene,<br>
>>>>>>>>> <br>
>>>>>>>>> Thanks for catching that. I think I have pion angles instead of<br>
>>>>>>>> proton.<br>
>>>>>>>>> <br>
>>>>>>>>> I am going to back over the code to fix this.<br>
>>>>>>>>> <br>
>>>>>>>>> Take care,<br>
>>>>>>>>> Michael<br>
>>>>>>>>> <br>
>>>>>>>>>> Mike,<br>
>>>>>>>>>> <br>
>>>>>>>>>> The vertical axis can't be right. The proton can't go<br>
>>> backwards<br>
>>>>> in<br>
>>>>>>>> the<br>
>>>>>>>>>> lab<br>
>>>>>>>>>> system<br>
>>>>>>>>>> <br>
>>>>>>>>>> -Eugene<br>
>>>>>>>>>> <br>
>>>>>>>>>>> -----Original Message-----<br>
>>>>>>>>>>> From: Frost <<a href="mailto:frost-bounces@jlab.org" target="_blank">frost-bounces@jlab.org</a>> On Behalf Of Michael<br>
>>> Dugger<br>
>>>>>>>>>>> Sent: Monday, December 23, 2019 14:07<br>
>>>>>>>>>>> To: Stuart Fegan <<a href="mailto:s.fegan.glasgow@gmail.com" target="_blank">s.fegan.glasgow@gmail.com</a>><br>
>>>>>>>>>>> Cc: <a href="mailto:frost@jlab.org" target="_blank">frost@jlab.org</a><br>
>>>>>>>>>>> Subject: Re: [Frost] [EXTERNAL] Re: Follow up of last FROST<br>
>>>>> meeting<br>
>>>>>>>>>>> <br>
>>>>>>>>>>> Hi,<br>
>>>>>>>>>>> <br>
>>>>>>>>>>> Chan is just trying to answer questions raised about a<br>
>>> possible<br>
>>>>>>>>>>> momentum<br>
>>>>>>>>>>> cut. I suggested that he look at where his events are in<br>
>>> terms<br>
>>>>> of<br>
>>>>>>>>>>> kinematic<br>
>>>>>>>>>>> bins he will report on. My idea was to see if pushing up the<br>
>>>>>>>> momentum<br>
>>>>>>>>>>> cut<br>
>>>>>>>>>>> to perhaps 400 MeV would cause any issues within his<br>
>>> kinematic<br>
>>>>>>>> binning.<br>
>>>>>>>>>>> <br>
>>>>>>>>>>> I just made a plot that can be found at<br>
>>>>>>>>>>> <br>
>>>>>>>>>>> <a href="https://userweb.jlab.org/~dugger/pi0PphaseSpacePlot.png" rel="noreferrer" target="_blank">https://userweb.jlab.org/~dugger/pi0PphaseSpacePlot.png</a><br>
>>>>>>>>>>> <br>
>>>>>>>>>>> that shows the lab angle versus lab momentum for protons<br>
>>> coming<br>
>>>>>>>> from<br>
>>>>>>>>>>> the<br>
>>>>>>>>>>> reaction gamma p -> p pi0. The black curves are for constant<br>
>>>>> photon<br>
>>>>>>>>>>> energy<br>
>>>>>>>>>>> and the blue curves are for constant proton center-of-mass<br>
>>>>> cosine<br>
>>>>>>>>>>> values.<br>
>>>>>>>>>>> <br>
>>>>>>>>>>> The above plot would have to be verified but it looks like<br>
>>> there<br>
>>>>> is<br>
>>>>>>>> no<br>
>>>>>>>>>>> need to<br>
>>>>>>>>>>> worry about low momentum protons.<br>
>>>>>>>>>>> <br>
>>>>>>>>>>> The idea I had was for Chan to produce this type of<br>
>>> information<br>
>>>>>>>> using<br>
>>>>>>>>>>> real<br>
>>>>>>>>>>> data, but I did a poor job of explaining what I meant.<br>
>>>>>>>>>>> <br>
>>>>>>>>>>> I was trying to make life easier, but perhaps did not<br>
>>> accomplish<br>
>>>>>>>> that<br>
>>>>>>>>>>> :(<br>
>>>>>>>>>>> <br>
>>>>>>>>>>> Take care,<br>
>>>>>>>>>>> Michael<br>
>>>>>>>>>>> <br>
>>>>>>>>>>>> Hi Chan,<br>
>>>>>>>>>>>> <br>
>>>>>>>>>>>> I'm going to chuck my two cents in, and reply to the FROST<br>
>>>>> list,<br>
>>>>>>>>>>>> because I missed the meeting last week. Given the<br>
>>> pion<br>
>>>>> is<br>
>>>>>>>>>>>> reconstructed from the proton missing mass, what's the<br>
>>>>> motivation<br>
>>>>>>>> for<br>
>>>>>>>>>>>> looking at proton momenta below the threshold where it can<br>
>>>>>>>> reliably<br>
>>>>>>>>>>>> reconstructed in CLAS as a proton? Is this to tune<br>
>>> the<br>
>>>>> cut,<br>
>>>>>>>> perform<br>
>>>>>>>>>>>> systematic studies, or is there a physics motivation here<br>
>>> that<br>
>>>>>>>> I'm<br>
>>>>>>>>>>> missing?<br>
>>>>>>>>>>>> <br>
>>>>>>>>>>>> Cheers,<br>
>>>>>>>>>>>> <br>
>>>>>>>>>>>> Stuart<br>
>>>>>>>>>>>> <br>
>>>>>>>>>>>> On 23/12/2019 11:47, Michael Dugger wrote:<br>
>>>>>>>>>>>>> Chan,<br>
>>>>>>>>>>>>> <br>
>>>>>>>>>>>>> It is a bit of a data dump.<br>
>>>>>>>>>>>>> <br>
>>>>>>>>>>>>> What is your binning going to by for the analysis? Are you<br>
>>>>>>>> really<br>
>>>>>>>>>>>>> going to report values for E_gamma near 400 MeV?<br>
>>>>>>>>>>>>> <br>
>>>>>>>>>>>>> On slide 3 you show MM^2 and state that MM^2 for p < 280<br>
>>>>> MeV/c<br>
>>>>>>>> don't<br>
>>>>>>>>>>>>> look like the others. I'm not convinced that you can say<br>
>>> much<br>
>>>>>>>> about<br>
>>>>>>>>>>>>> the MM^2 shown above p = 280 MeV/c.<br>
>>>>>>>>>>>>> <br>
>>>>>>>>>>>>> For your previous presentation:<br>
>>>>>>>>>>>>> <br>
>>>>>>>>>>>>> <br>
>>>>>>>>>>> <br>
>>>>> <a href="https://clasweb.jlab.org/rungroups/g9/wiki/images/9/94/FROST_2019_12_" rel="noreferrer" target="_blank">https://clasweb.jlab.org/rungroups/g9/wiki/images/9/94/FROST_2019_12_</a><br>
>>>>>>>>>>>>> 18.pdf<br>
>>>>>>>>>>>>> <br>
>>>>>>>>>>>>> on slide 2 you had a nice fit to the MM^2 distribution<br>
>>> where<br>
>>>>> you<br>
>>>>>>>>>>>>> pulled off a pi0 mass. Are you able to do that for the low<br>
>>>>>>>> momentum?<br>
>>>>>>>>>>>>> Is it possible that you can not pull out any pi0 from the<br>
>>> low<br>
>>>>>>>>>>>>> momentum data? I just do not see any pi0. Am I missing<br>
>>>>>>>> something?<br>
>>>>>>>>>>>>> <br>
>>>>>>>>>>>>> Take care,<br>
>>>>>>>>>>>>> Michael<br>
>>>>>>>>>>>>> <br>
>>>>>>>>>>>>>> <br>
>>>>>>>>>>>>>> <br>
>>>>>>>>>>>>>> Dear FROST run group,<br>
>>>>>>>>>>>>>> <br>
>>>>>>>>>>>>>> Hello, below is a link to my slides for follow up of last<br>
>>>>> FROST<br>
>>>>>>>>>>>>>> meeting(12/19):<br>
>>>>>>>>>>>>>> <br>
>>>>>>>>>>> <br>
>>>>> <a href="https://clasweb.jlab.org/rungroups/g9/wiki/images/e/ed/FROST_2019_12" rel="noreferrer" target="_blank">https://clasweb.jlab.org/rungroups/g9/wiki/images/e/ed/FROST_2019_12</a><br>
>>>>>>>>>>>>>> _22.pdf<br>
>>>>>>>>>>>>>> <br>
>>>>>>>>>>>>>> 1. Distributions of kinematics (MMSQ, dt, d\beta) for<br>
>>>>> particles<br>
>>>>>>>> in<br>
>>>>>>>>>>>>>> lower momentum ranges are plotted to see whether lower<br>
>>>>> momentum<br>
>>>>>>>>>>>>>> particles are of any use for my asymmetry calculation.<br>
>>>>>>>>>>>>>> <br>
>>>>>>>>>>>>>> 2. Proton selection, using beta difference, was revised<br>
>>> to a<br>
>>>>>>>>>>> simpler<br>
>>>>>>>>>>>>>> version where static cuts on beta diff are applied at +/-<br>
>>>>> 0.06<br>
>>>>>>>>>>>>>> <br>
>>>>>>>>>>>>>> <br>
>>>>>>>>>>>>>> Thank you,<br>
>>>>>>>>>>>>>> Chan<br>
>>>>>>>>>>>>>> <br>
>>>>>>>>>>>>>> _______________________________________________<br>
>>>>>>>>>>>>>> Frost mailing list<br>
>>>>>>>>>>>>>> <a href="mailto:Frost@jlab.org" target="_blank">Frost@jlab.org</a><br>
>>>>>>>>>>>>>> <a href="https://mailman.jlab.org/mailman/listinfo/frost" rel="noreferrer" target="_blank">https://mailman.jlab.org/mailman/listinfo/frost</a><br>
>>>>>>>>>>>>>> <br>
>>>>>>>>>>>>> <br>
>>>>>>>>>>>>> _______________________________________________<br>
>>>>>>>>>>>>> Frost mailing list<br>
>>>>>>>>>>>>> <a href="mailto:Frost@jlab.org" target="_blank">Frost@jlab.org</a><br>
>>>>>>>>>>>>> <a href="https://mailman.jlab.org/mailman/listinfo/frost" rel="noreferrer" target="_blank">https://mailman.jlab.org/mailman/listinfo/frost</a><br>
>>>>>>>>>>>> <br>
>>>>>>>>>>>> --<br>
>>>>>>>>>>>> Dr Stuart Fegan<br>
>>>>>>>>>>>> Honorary Research Associate<br>
>>>>>>>>>>>> Nuclear Physics Group<br>
>>>>>>>>>>>> University of Glasgow<br>
>>>>>>>>>>>> (Currently at the University of York)<br>
>>>>>>>>>>>> <br>
>>>>>>>>>>>> E-mail: <a href="mailto:s.fegan.glasgow@gmail.com" target="_blank">s.fegan.glasgow@gmail.com</a><br>
>>>>>>>>>>>> <br>
>>>>>>>>>>>> _______________________________________________<br>
>>>>>>>>>>>> Frost mailing list<br>
>>>>>>>>>>>> <a href="mailto:Frost@jlab.org" target="_blank">Frost@jlab.org</a><br>
>>>>>>>>>>>> <a href="https://mailman.jlab.org/mailman/listinfo/frost" rel="noreferrer" target="_blank">https://mailman.jlab.org/mailman/listinfo/frost</a><br>
>>>>>>>>>>>> <br>
>>>>>>>>>>> <br>
>>>>>>>>>>> <br>
>>>>>>>>>>> _______________________________________________<br>
>>>>>>>>>>> Frost mailing list<br>
>>>>>>>>>>> <a href="mailto:Frost@jlab.org" target="_blank">Frost@jlab.org</a><br>
>>>>>>>>>>> <a href="https://mailman.jlab.org/mailman/listinfo/frost" rel="noreferrer" target="_blank">https://mailman.jlab.org/mailman/listinfo/frost</a><br>
>>>>>>>>>> <br>
>>>>>>>>> <br>
>>>>>>>>> <br>
>>>>>>>>> <br>
>>>>>>>> <br>
>>>>>>>> <br>
>>>>>>>> _______________________________________________<br>
>>>>>>>> Frost mailing list<br>
>>>>>>>> <a href="mailto:Frost@jlab.org" target="_blank">Frost@jlab.org</a><br>
>>>>>>>> <a href="https://mailman.jlab.org/mailman/listinfo/frost" rel="noreferrer" target="_blank">https://mailman.jlab.org/mailman/listinfo/frost</a><br>
>>>>>>>> <br>
>>>>>>> <br>
>>>>>> <br>
>>>>> <br>
>>>>> <br>
>>>>> _______________________________________________<br>
>>>>> Frost mailing list<br>
>>>>> <a href="mailto:Frost@jlab.org" target="_blank">Frost@jlab.org</a><br>
>>>>> <a href="https://mailman.jlab.org/mailman/listinfo/frost" rel="noreferrer" target="_blank">https://mailman.jlab.org/mailman/listinfo/frost</a><br>
>>>>> <br>
>>>> <br>
>>> <br>
>>> <br>
>>> <br>
>> <br>
> <br>
> <br>
> _______________________________________________<br>
> Frost mailing list<br>
> <a href="mailto:Frost@jlab.org" target="_blank">Frost@jlab.org</a><br>
> <a href="https://mailman.jlab.org/mailman/listinfo/frost" rel="noreferrer" target="_blank">https://mailman.jlab.org/mailman/listinfo/frost</a><br>
</blockquote></div>
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