Closed cschwan closed 1 year ago
Could you fix also #24 since you are at it?
I'm not quite sure I understand the piso
branches; in there both up and down PDFs are replaced with (up + down) / 2
and the corresponding combination for the anti quarks, but not for strange, charm or bottom. Is this correct? @Radonirinaunimi might know whether this is a correct model of the hadron (which in our cases I think is a deuteron, @scarlehoff is that always true?).
I also fixed the ppbar if
-branches, although we don't seem to use this in any dataset. However, since it sometimes overlaps with with pp
and piso
only partially fixing it is probably worse. The W+/W- branch I didn't touch.
Could you fix also #24 since you are at it?
Done.
I'm not quite sure I understand the
piso
branches; in there both up and down PDFs are replaced with(up + down) / 2
and the corresponding combination for the anti quarks, but not for strange, charm or bottom. Is this correct? @Radonirinaunimi might know whether this is a correct model of the hadron (which in our cases I think is a deuteron, @scarlehoff is that always true?).@cschwan From the branch name at least I would deduce that it is constructing a free isoscalar version of the proton. Isoscalarifying a nucleon basically means that each PDF flavour is replaced by: $$f^{\rm iso}_i (x, Q^2) = \left( \frac{ f^{p}_i (x, Q^2) + f^{n}_i (x, Q^2) }{2} \right)$$ where $f^p$ and $f^n$ are respectively the proton and neutron PDF. The neutron PDF can be extracted from the proton-bound using isospin symmetry which basically boils down to the following relations: $$u^n (x, Q^2) = d^p (x, Q^2) \, d^n (x, Q^2) = u^p (x, Q^2)~\text{(same relations hold for anti-u and anti-d)}$$ and $f^n_i (x, Q^2) = f^p_i (x, Q^2)$ for other flavours. If this is what is implemented, then everything is correct.
@Radonirinaunimi thank you for this great explanation! That's indeed what's being implemented.
I'm merging this. Once I've finished with the E906 problem and check the k-factors (I need to do that with the bugged version for a good comparison) I will release a vrap 1.4 (and update pinefarm accordingly)
This fixes the following assumptions,
and
qq_CE1_lumi
for a ppbar colliderfor all neutral current related processes