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2023:groups:smhiggs:ggf-an3lo:start [2023/06/18 09:33]
stephen.jones
2023:groups:smhiggs:ggf-an3lo:start [2023/06/18 14:50] (current)
stephen.jones
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 ---- ----
 +=== Settings ===
  
 **Energies:​** ​ **Energies:​** ​
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 **PDF Sets:** **PDF Sets:**
-^ NNLO PDFs      ^ aN3LO PDFs ^ +^ NNLO PDFs      ^ aN3LO PDFs        
-| MSHT           | MSHT       ​+| MSHT           | MSHT              
-| NNPDF4.0 ​      ​| ​           +| NNPDF4.0 ​      ​| ​NNPDF4.0 (prelim) ​
-| PDF4LHC21 ​     |            |+| PDF4LHC21 ​     |                   | 
 + 
 +**Coefficient Function:​** 
 +Always N3LO (even when using NNLO PDFs) 
 + 
 +**iHixs Runcard (defines defaults):​**  
 +[[https://​phystev.cnrs.fr/​wiki/​_media/​2023:​groups:​smhiggs:​ggf-an3lo:​run3.txt|run3.card]]  
 +[[https://​phystev.cnrs.fr/​wiki/​_media/​2023:​groups:​smhiggs:​ggf-an3lo:​13.6_125.09_log.txt|log]] 
 +[[https://​phystev.cnrs.fr/​wiki/​_media/​2023:​groups:​smhiggs:​ggf-an3lo:​13.6_125.09_out.txt|out]]
  
 === 1. ggF Stacked Error Plots (iHixs) === === 1. ggF Stacked Error Plots (iHixs) ===
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 Recreate plots similar to Fig. 2 in [[https://​arxiv.org/​pdf/​1802.00827.pdf|iHixs]],​ showing only the uncertainties: ​ Recreate plots similar to Fig. 2 in [[https://​arxiv.org/​pdf/​1802.00827.pdf|iHixs]],​ showing only the uncertainties: ​
   * $\delta(PDF)$, ​   * $\delta(PDF)$, ​
-  * $\delta(PDF-TH)$, +  * $\delta(PDF_{TH})$, 
   * $\delta(\mathrm{scale})$   * $\delta(\mathrm{scale})$
 or (for aN3LO PDFs): or (for aN3LO PDFs):
-  * $\delta(PDFincTH)$, +  * $\delta(PDF+PDF_{TH})$, 
   * $\delta(\mathrm{scale})$.   * $\delta(\mathrm{scale})$.
 We will omit uncertainties not relevant to the study (namely $\delta(EW)$,​ $\delta(\alpha_s),​ \delta(1/​m_t),​ \delta(t,​b,​c)$. We will omit uncertainties not relevant to the study (namely $\delta(EW)$,​ $\delta(\alpha_s),​ \delta(1/​m_t),​ \delta(t,​b,​c)$.
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   * $\delta(\sigma)$ breakdown of the errors on the cross section (see Study 1 for details)   * $\delta(\sigma)$ breakdown of the errors on the cross section (see Study 1 for details)
  
-Comments made by observing preliminary results presented in the initial session: The aN3LO/NNLO k-factor for MSHT ~0.98 and for NNPDF looked ~1 (very preliminary). The NNPDF NNLO result is above the MSHT result and so at aN3LO we may see an even larger disagreement.+Comments made by observing preliminary results presented in the initial session: The aN3LO/NNLO k-factor for MSHT ~0.98 and for NNPDF looked ~1 (warning: ​preliminary). The NNPDF NNLO result is above the MSHT result and so at aN3LO we may see an even larger disagreement.
  
-=== 3. Gluon Lumi Comparison ===+=== 3. Gluon Lumi Comparison ​($\sqrt{s}=13.6\ \mathrm{TeV}$) ​===
  
 Ratio plots for PDFs and Luminosities. Ratio plots for PDFs and Luminosities.
  
-                      ​^ Order            ^ Sets          ^ +                         ^ Order            ^ Sets          ^ 
-$xg(x)$ ​                | aN3LO/​NNLO ​      | MSHT/​MSHT ​    | +|  ​$xg(x)$ ​                | aN3LO/​NNLO ​      | MSHT/​MSHT ​    | 
-$\mathcal{L}_gg       | aN3LO/​NNLO ​      | MSHT/​MSHT ​    | +|  :::                     | :::              | NNPDF/​NNPDF ​  | 
-$\mathcal{L}_gg       | NNLO/​NNLO ​       | MSHT/​PDF4LHC ​ | +|  ​$\mathcal{L}_{gg}     | aN3LO/​NNLO ​      | MSHT/​MSHT ​    | 
-:::                     | :::              | NNPDF/​PDF4LHC |+|  :::                     | :::              | NNPDF/​NNPDF ​  | 
 +|  ​$\mathcal{L}_{gg}     | NNLO/​NNLO ​       | MSHT/​PDF4LHC ​ | 
 +|  ​:::                     | :::              | NNPDF/​PDF4LHC |
  
 The luminosity plots should also be created with $|y_X| < 2.5$ to see the impact of the Higgs rapidity cut. The luminosity plots should also be created with $|y_X| < 2.5$ to see the impact of the Higgs rapidity cut.
2023/groups/smhiggs/ggf-an3lo/start.1687073632.txt.gz · Last modified: 2023/06/18 09:33 by stephen.jones