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Commit 9f264aa1 authored by Klaus Rabbertz's avatar Klaus Rabbertz
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Update Daniels fastNLOTableFormatv21.ods 

git-svn-id: https://ekptrac.physik.uni-karlsruhe.de/svn/fastNLO/trunk@1592 aa5437bd-d6fa-0310-9a40-cbaab9bf9339
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{\small \footnotesize
\begin{verbatim}
******************************************************************************
The table contains the following blocks (separated by ``1234567890''):
- version No and date
- scenario description
- observable-specific flags (reaction, ECM, jet algo, order, available orders...)
- details about the QCD calculation
- technical fastNLO details (Nevt, Nxtot, Ixscheme, Ipdfwgt, ...)
- structure of observable: tot No. of bins, and structure of dimensions in binning
- bin boundaries
- xmin values
- renormalization scales
- factorization scales
- scale variations
- the sigma-tilde
******************************************************************************
******* fastNLO - general definition of tableformat
******* for raw (Nord=1,etc) and sum tables
******************************************************************************
VersionNo ! dbl: Version of Table - for compatibility check (e.g.1.01)
idate ! int: date when sum table was created (yyyymmdd)
* ---- these first two entries are added to the table by nlofast-add !!!!! <<<<<<<
* they are not contained in the raw tables
1234567890 ! --- End-of-block --- now the scenario description
ScenName ! string: name of scenario (e.g. "fnt1001")
iSDescr ! int: No. of Strings for Description of scenario
ScenDescr[1] ! string: Description of scenario
... ! (e.g. hep-ex No., Collaboration, ...)
ScenDescr[iSDescr] !
1234567890 ! --- End-of-block --- now some observable-specific flags
ireaction ! int: reaction: 1 ep, 2 pp, 3ppbar,4gamma-p(dir), 5gamma-p(resolved)
Ecms ! dbl: center-of-mass energy in GeV
iproc ! int: process type 1 incl jets, 2 dijets, ... (just a little info...)
ialgo ! int: jet algo 1 kT, 2 midpoint cone, 3 rsep cone, 4 search cone
JetResol1 ! dbl: jet resolution paramter (kT distance D / R_cone)
JetResol2 ! dbl: 2nd parameter for jet algo (e.g. f_overlap, Rsep, search cone)
1234567890 ! --- End-of-block --- now some info on the QCD calculation
iasflg ! int: Flag (0: w/o alphas 1: alphas already contained in table)
asMZ ! dble: for iasflg=1: asMZ is alphas(Mz)
ipdfflg ! int: Flag (0: w/o PDFs 1: PDFs already included in table)
PDFset ! string: for ipdfflg=1: PDF set included in table (eg:"CTEQ6.1")
>> for resolved Photoproduction only:
igampdfflg ! int: Flag (0: w/o photonPDFs 1: photon-PDFs already included in table)
gamPDFset ! string: for igampdfflg=1: photon-PDF set included in table
nFlav ! int: No of active quark flavors used in calculation
Nord ! int: * in raw table: No. of this table in sum table
! / usually = relative order
! in alpha_s: 1: LO, 2: NLO,
! 3:NNLO or other correction
! * in sum table: tot. No. of single tables in sum table
! in fixed-order calculations =
! highest relative order available
* in raw table:
Npow ! int: absolute order in alpha_s of this raw table
* in sum table:
Npow1 ! int: absolute order in alpha_s for each contribution [1,...,Nord]
... ! (to be used in usercode as power of alpha_s)
Npow[Nord]
* in raw table:
Powlabel ! string: label for the order, e.g ``LO''
* in sum table:
Powlabel1 ! string: label for the order, for each contribution [1,...,Nord]
...
Powlabel[Nord]
ScaleA ! string: default scale (e.g. "pT", "ETmax", "Q", "Mjj" <<<<<<<<<<<<<<<<< new
ScaleB ! string: short description (e.g. computed from two highest pT jets) <<<<<<<<<<< new
ScaleC ! string: more description (e.g. "taken at 40% of the bin") <<<<<<<<<<<<<<<<< new
1234567890 ! --- End-of-block --- now come some technical fastNLO details
* in raw table:
Nevt ! dbl: No of events for this raw table
* in sum table:
Nevt1 ! dbl: No of events for contribution 1 (usually LO)
Nevt2 ! dbl: No of events for contribution 2 (usually NLO)
... ! dbl: No of events for higher order contributions
Nevt[Nord] ! (or resummed correction)
Nxtot ! int: No of eigenfunctions in that cover the x-ranges
ixscheme ! int: No of scheme for EF x-binning 1 log 1/x 2 sqrt(log 1/x)
ipdfwgt ! int: No of scheme for PDF weighting 0 no weigthing 1 'standard weighting'
>> for resolved Photoproduction only:
igampdfwgt ! int: No of scheme for photon-PDF weighting 0 no weigthing 1 'standard weighting'
*** previously we had the No of rap bins together with the rapidity boundaries
*** -> this is now separated: first come all array sizes - afterwards we
*** declare all values (upper & lower values for each interval)
1234567890 ! --- End-of-block --- now: structure of the dimensions
Nbintot ! int: total Number of observable bins
Ndimension ! int: No. of dimensions in variable is binned
! 3-d example: Jet Shape Psi as function of (y,pT,r)
Cdim[1] ! string: which variable corresponds to 1st dimension (eg: ``y'')
... !
Cdim[Ndimension] ! string: which variable corresponds to lasst dimension
!
Ndim1 ! int: No. of intervals in first dimension
! (e.g.: No. of y-ranges)
Ndim2[1] ! int: No. of intervals in 2nd dim for each interval in 1st dim
.... ! (e.g.: No. of pT ranges in each y-range)
Ndim2[Ndim1] !
Ndim3-[1]-[1] ! int: No. of intervals in 3rd dim for each interval in 2nd dim
... ! - for each interval in 1st dim
Ndim3-[1]-[Ndim2[1]] ! (e.g.: No. of r bins in each pT range - in each y-range)
... !
... !
Ndim3-[Ndim1]-[1] !
... !
Ndim3-[Ndim1]-[Ndim2[Ndim1]] !
Ndim'Ndimension'- ..-..-..-..-..
*********** I don't want to write out more than the third dimension :-)
1234567890 ! --- End-of-block --- now come the bin boundaries - for all dimensions
************* not sure: should we first fill all lower values - then all higher values?
************* or: always pairs low/high? I choose the second one for now
Dim1lo[1] ! dbl: lower and higher boundary for 1st interval in dim 1
Dim1hi[1] !
... !
Dim1lo[Ndim1] ! lower and higher boundary for last interval in dim 1
Dim1hi[Ndim1] !
Dim2lo[1]-[1] ! dbl: lower and higher boundary for 1st interval in dim1/dim2
Dim2hi[1]-[1] !
...
Dim2lo[1]-[Ndim2[1]] ! dbl: lower and higher boundary for 1st interval in dim 1
Dim2hi[1]-[Ndim2[1]] !
...
...
...
Dim2lo[Ndim1]-[1]
Dim2hi[Ndim1]-[1]
...
Dim2lo[Ndim1]-[Ndim2[Ndim1]]
Dim2hi[Ndim1]-[Ndim2[Ndim1]]
*** 3rd dimension - if available ...
Dim3lo[1]-[1]-[1] ! dbl: lower and higher boundary for 1st interval in dim1/dim2
Dim3hi[1]-[1]-[1] !
...
Dim3lo[1]-[1]-[Ndim3[1]-[1]]
Dim3hi[1]-[1]-[Ndim3[1]-[1]]
...
...
...
Dim3lo[1]-[Ndim2[1]-[1]
Dim3hi[1]-[Ndim2[1]-[1]
...
Dim3lo[1]-[Ndim2[1]-[Ndim3[1]-[[1]]
Dim3hi[1]-[Ndim2[1]-[Ndim3[1]-[[1]]
....
************ I'm getting lost here ......
1234567890 ! --- End-of-block --- now come the x_min values for all bins
xmin-1-1-? ! dbl: xmin in 1st rapidity bin / 1st pT bin / 1st r bin
.... ! and all other xmin-values
! - same structure as bin-boundaries
>> for resolved Photoproduction only:
xgammamin-1-1-? ! dbl: xmin in 1st rapidity bin / 1st pT bin / 1st r bin
.... ! and all other xmin-values
! - same structure as bin-boundaries
1234567890 ! --- End-of-block --- now come the renorm. scales for all bins
murval-1-1-? ! dbl: Array for all mu_r values -
... ! (same structure as bin-boundaries)
1234567890 ! --- End-of-block --- now come the factoriz. scales for all bins
mufval-1-1-? ! dbl: Array for all mu_f values - for all (y,pT) bins
... ! (same structure as bin-boundaries)
>> for resolved Photoproduction only:
mufvalgamma-1-1-? ! dbl: Array for all mu_f-gamma values - for all (y,pT) bins
... ! (same structure as bin-boundaries)
* - the following is not used in LO tables - only in higher order raw tables and in sum tables
1234567890 ! --- End-of-block --- now come the scale variations
nscalevar ! int: No of scale variations for mu_r and mu_f
murscale[1] ! dbl: renormalisation scale factors with respect to standard scale
... !
murscale[nscalevar] !
mufscale[1] ! dbl: factorisation scale factors with respect to standard scale
... !
mufscale[nscalevar] !
>> for resolved Photoproduction only:
mufscalegamma[1] ! dbl: factorisation scale factors with respect to standard scale
... !
mufscalegamma[nscalevar] !
1234567890 ! --- End-of-block --- now come the sigma_tilde
... ! dbl: each range in dimension 1
... ! each range in dimension 2
... ! ... each range in dimension n
... ! loop over xmax bins
... ! loop over xmin bins (not for ep)
... ! -> for pp from xmin->xmax
... ! -> for photoproduction from xmin->1
... ! loop over scale variations (not for LO table, i.e. Nord=1)
... ! loop over subprocesses (ep:3, pp:7)
???????????? there is a difference in authorcode and nlofast-add:
???????????? authorcode first loops over scales - then subprocesses (as above)
???????????? nlofast-add first loops over subprocesses (when writing!) - then scales
???????????? --> should be the same!!!
1234567890 ! --- End of Table ------------------------------------
\end{verbatim}
}
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{\small \footnotesize
\begin{verbatim}
******************************************************************************
******* fastNLO - general definition of tableformat
******* for raw (Nord=1,etc) and sum tables
*******
******* version 1.4 (not yet written by authorcode
******* - only constructed when adding v13 tables by nlofast-add)
******************************************************************************
1234567890 ! --- End-of-block --- now comes the table header
Itabversion ! int: table version *10000 - e.g.: v1.4 -> 14000
1234567890 ! --- End-of-block --- now come some technical details
ireaction ! int: reaction 1 ep, 2 pp, 3ppbar
Ecms ! dbl: center-of-mass energy in GeV
Ixsectunits ! int: negative power of ten for x-section units (e.g.: 9=nanobarn)
namelabel(1) ! five strings: brief description
namelabel(2) ! - usually: 1st: ``d2sigma/dpT/dy (nb_GeV)''
namelabel(3) ! 2nd: hep-ex No. of publication
namelabel(4) ! 3rd: Collaboration
namelabel(5) !
iproc ! int: process type 1 incl jets, 2 dijets, ... (not very
important - just to add a little info..)
ialgo ! int: jet algo 1 kT, 2 midpoint cone, 3 rsep cone, 4 search cone
JetResol1 ! dbl: jet resolution paramter (kT distance D / R_cone)
JetResol2 ! dbl: 2nd parameter for jet algo (e.g. f_overlap, Rsep, search cone)
Nord ! int: * in raw table: No. of this table in sum table
! / usually = relative order
! in alpha_s: 1: LO, 2: NLO,
! 3:NNLO or other correction
! * in sum table: tot. No. of single tables in sum table
! in fixed-order calculations =
! highest relative order available
* in raw table:
Npow (was Oalphas) ! int: absolute order in alpha_s of this raw table
* in sum table:
Npow1 ! int: absolute order in alpha_s for each contribution [1,...,Nord]
... ! (to be used in usercode as power of alpha_s)
Npow[Nord]
* in raw table:
Powlabel ! string: label for the order, e.g ``LO''
* in sum table:
Powlabel1 ! string: label for the order, for each contribution [1,...,Nord]
Codelabel1 ! string: label which code as used for computation (e.g.: ``NLOJET++'')
...
Powlabel[Nord]
Codelabel[Nord]
1234567890 ! --- End-of-block --- now come some technical details
* in raw table:
Nevt (was: nevtlo+nevtnlo) ! dbl: No of events for this raw table
* in sum table
Nevt1 ! dbl: No of events for contribution 1 (usually LO)
Nevt2 ! dbl: No of events for contribution 2 (usually NLO)
... ! dbl: No of events for higher order contributions
Nevt[Nord] ! (or resummed correction)
nxtot (was: ntot) ! int: No of eigenfunctions in that cover the x-ranges
ixscheme ! int: No of scheme for EF x-binning 1 log 1/x 2 sqrt(log 1/x)
ipdfwgt ! int: No of scheme for PDF weighting 0 no weigthing 1 'standard weighting'
iref ! int: Flag if ``reference'' table (=1) incl alphas/PDFs - or not (=0)
1234567890 ! --- End-of-block --- now come the pT,y bin boundaries
Nbintot ! int: total No. of observable bins in table
Ndimension ! int: No. dimension (usually two: y,pT or eta,ET 0 fixed in v1.4)
Dimlabel1 ! string: 1st - last dimension
... !
Dimlabel[Ndimension] !
Nrapidity ! int: No of rapidity intervals
Rap0 ! dbl: lower boundary of 1st rapidity bin
... !
Rap[Nrapidity] ! dbl: upper boundary of last rapidity bin
Npt1 ! int: No of pT bins in first rapidity interval
... !
Npt[Nrapidity] ! int: No of pT bins in last rapidity interval
Pt-1-0 ! dbl: lower boundary of 1st pT bin in 1st rapidity bin
... !
Pt-1-[Npt1] ! dbl: upper boundary of last pT bin in 1st rapidity bin
... !
... !
Pt-[Nrapidity]-0 ! dbl: lower boundary of 1st pT bin in last rapidity bin
... !
Pt-[Nrapidity]-[Npt?] ! dbl: upper boundary of last pT bin in last rapidity bin
1234567890 ! --- End-of-block --- now come the x_min values for all bins
xmin-1-1 ! dbl: xmin in 1st rapidity bin / 1st pT bin
xmin-1-2 ! dbl: xmin in 1st rapidity bin / 2nd pT bin
... !
xmin-1-[Npt1] ! dbl: xmin in 1st rapidity bin / last pT bin
xmin-2-1 ! dbl: xmin in 2nd rapidity bin / 1st pT bin
... !
xmin-[Nrap]-[Npt?] ! dbl: xmin in last rapidity bin / last pT bin
1234567890 ! --- End-of-block --- now come the renorm. scales
Scalelabel ! string: description what scale is - e.g. ``pT_of_individual_jet''
Nscalebin ! int: No of scale-bins used for eachobservable bins - in v1.4 only 1 is allowed
murval-1-1 ! dbl: Array for all mu_r values - for all (y,pT) bins
... ! (same structure as xmin-Array)
murval-[Nrap]-[Npt?] ! dbl:
1234567890 ! --- End-of-block --- now come the factoriz. scales
mufval-1-1 ! dbl: Array for all mu_f values - for all (y,pT) bins
... ! (same structure as mu_r and xmin Arrays)
mufval-[Nrap]-[Npt?] ! dbl:
* - the following is not used in LO tables - only in higher order raw tables and in sum tables
1234567890 ! --- End-of-block --- now come the scale variations
nscalevar ! int: No of scale variations for mu_r and mu_f, this *includes* the standard scale
murscale1 ! dbl: renormalisation scale factors with respect to standard scale SQUARED
... !
murscale[nscalevar] !
mufscale1 ! dbl: factorisation scale factors with respect to standard scale SQUARED
... !
mufscale[nscalevar] !
1234567890 ! --- End-of-block --- now come the sigma_tilde
... ! dbl: each rapidity range
... ! each pT bin
... ! each xmin-bin
... ! each xmax-bin
... ! each subprocess
... ! nscalevar variations (not for LO table, i.e. Nord=1)
... ! 1: standard scale, 2:1st variation
... ! 3:2nd variation, ..... ]
1234567890 ! --- End of Table ------------------------------------
\end{verbatim}
}
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