OPT-IN:Target and Double Spin Asymmetries of Deeply Virtual Ï0 Production with a Longitudinally Polarized Proton Target and CLAS
Michel Garçon
michel.garcon at cea.fr
Thu Oct 1 07:51:17 EDT 2015
Overall, the article reads well and the message is clear. Nice work ! I have some detailed remarks and corrections though:
Abstract l. 9 : Large VALUES, not amplitudes. The word amplitude is rightly used at the end of the same sentence.
l. 32: Insert after âprocesses.â The sentence
âThe conventional ETbar = 2HTtilde+ET will be used as well hereafter. These GPDs can be accessedâ¦.â
with optional reference to M. Burkardt, PRD 72, 094020 (2005).
Eq. 1: F depends on Q2 as well (evolution)
l. 76: if I am not mistaken, eqs 2 and 3 are quite general, model independent. They only suppose one photon exchange. Then bar âat the leading twistâ. Same applies to l. 243.
l. 82: unpolarized structure functions. Bar âspinâ.
l. 93: [12] only deals with chiral even GPDs and DVCS. It is not the best place to introduce the GGL model in this context. I would just use ref [17]. Same remark for caption of Fig. 4.
l. 136: âemittedâ instead of âscatteredâ photons.
l. 147: âadditionalâ instead of âextraâ
Fig.1 x-label and line 156: use the same notation for missing mass.
l. 184 âpolarization dependentâ instead of âasymmetricalâ
l. 198: âcorresponding beam chargeâ instead of âtotal chargeâ
l. 206: [15] is not enough to calculate the ep spin asymmetry. It gives the formula, but you need a form factor parameterization to get a number. You should quote also the form factor parameterization which you used.
l. 209: remove \simeq .
l. 215: âwere modified from 3sigma to 2.5â¦..â
l. 218: Iâd rather see a range quoted here: âThe corresponding variations of asymmetries ranged from ?? to ??% in all kinematical binsâ. The average in l. 225, including all sources of bin to bin syst. errors, is fine there.
l. 249: full stop after âasymmetriesâ and then âThis observable is importantâ¦â
l. 276: GGL
l. 293-295: 3 articles missing. the target spin asymmetryâ¦.the beam beam asymmetry⦠A moreâ¦.
l. 307: âreal part of the even-odd product â¦â instead of âreal part of chiral-even and chiral-odd GPDs productâ¦â since the quantities in brackets are not the GPDs themselves.
l. 308: The overallâ¦
Ref [17]: the second author is J. O. Gonzales Hernandez (hence the GGL).
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