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Welcome to the CJ-database wiki! For now all info in one page - will make it better later
(Data are provided in both xlsx and csv format under directory data/dataframe
, can be easily read into a dataframe)
-
Extracted data: prepend a
*
(star) sign if the column was extracted using info from original source
The measured values are given by:
-
value
: the value of the measurement -
units
: the units (e.g.mb
,fb
, ....)- If dimensionless, use
1
- If dimensionless, use
-
uncorrelated errors: append
_u
to whatever name you like.-
Example:
stat_u
is the uncorrelated statistical error;syst_u
the uncorrelated systematic error
-
Example:
-
correlated errors: append
_c
to whatever name you like.-
Example:
norm_c
is the overall normalization error.
-
Example:
-
relative vs. absolute errors: Prepend a
%
sign if error expressed as percent of the quotedvalue
of the observable; otherwise, error interpreted as absolute value.
A complete characterization of an unpolarized DIS cross section requires specification of the following information
-
obs
: the kind of observable (see below) -
target
: the kind of target (proton, deuteron, ratios, heavier nuclei) -
lepton beam
: the flavor and charge of the lepton beam -
current
: the vector boson current (neutral or charged)
-
X
orx
: Bjorken x -
Q2
orq2
: four momentum squared (GeV^2/c^2) -
Y
ory
: invariant inelasticity -
Elab
: Lab energy of the collision (GeV/c)
We follow the PDG conventions for structure functions.
-
F2
: F2 structure function -
FL
: longitudinal FL -
R
: for the longitudinal to transverse cross section ratio -
sig_r
: reduced DIS cross section (remove the coefficient in front of F2)
Note that ratios of structure functions or cross sections are indicated in the target
column. E.g., a ratio of proton to deuteron cross sections woudl be indicated as p/d
in that column. Here only the original cross section is indicated.
-
p
for protons -
d
for per-nucleon deuteron target observables, i.e, 0.5*obs(d)-
Note: We may want however to use
N
for "nucleons", instead
-
Note: We may want however to use
-
p/d
for the proton/deuteron ratio, e.g., from NMC -
n/d
for the neutron/deuteron ratio, e.g., from BONUS - Nuclei can also be included in the future, e.g.,
-
A_12_6
for 12C -
A_207_82
for 207Pb - attention: the Dueteron would be
A_2_1
--> so that in the current conventionsA_2_1 = 2*d
-
Combine a flavor and charge labels:
- flavors:
e
,mu
,tau
,nu_e
,nubar_e
, ... - charges:
plus
,minus
, also nothing if unknown
Examples:
-
e_plus
for e+ beam -
mu_minus
for mu- beams -
mu
if no charge is specified in the original paper (it means Q2 is low enough for gamma-Z interference to be negligible)
-
NC
= neutral current -
CC
= charged current
The plain data files in the data/text
directory are used as input files to the CJ global fitting program.
{experiment name}_{observable}{target}
*An additional _c
as suffix indicates the correlated errors are provided.
In data/text/slac_p_c
:
slac,F2,p target
------------- data content
converted from 10010.xlsx
----- additional notes (in this case, the data table ID)
*
0.0210 13
------------------- normalization factor in fraction, and number of correlated errors
In the header column:
x Q2 F2 Ebeam stat sys_tot sys_u dsy dse drc ...
-
stat
: total statistical error -
sys_tot
: total systematic error (all correlated and uncorrelated errors added in quadrature) -
day, dse, doc...
: names of the 13 sources of correlated error.