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Top Physics in WHIZARD (+ NLO/QCD Status) Jrgen R. Reuter, DESY - PowerPoint PPT Presentation

Top Physics in WHIZARD (+ NLO/QCD Status) Jrgen R. Reuter, DESY J.R.Reuter Top Physics in WHIZARD (+NLO/QCD) LCWS 2015, Whistler, 4.11.15 WHIZARD @ WHISTLER J.R.Reuter Top Physics in WHIZARD (+NLO/QCD)


  1. Top Physics in WHIZARD (+ NLO/QCD Status) Jürgen R. Reuter, DESY J.R.Reuter Top Physics in WHIZARD (+NLO/QCD) LCWS 2015, Whistler, 4.11.15

  2. WHIZARD @ WHISTLER J.R.Reuter Top Physics in WHIZARD (+NLO/QCD) LCWS 2015, Whistler, 4.11.15

  3. My tribute to Canada … J.R.Reuter Top Physics in WHIZARD (+NLO/QCD) LCWS 2015, Whistler, 4.11.15

  4. My tribute to Canada … ✦ in memoriam ✦ J.R.Reuter Top Physics in WHIZARD (+NLO/QCD) LCWS 2015, Whistler, 4.11.15

  5. My tribute to Canada … ✦ in memoriam ✦ “Vergeh’ die Welt Jon Vickers, 29.10.1926 - 10.7.2015 meiner jauchzenden Eil’! Die Leuchte verlischt, zu ihr! Isolde!” J.R.Reuter Top Physics in WHIZARD (+NLO/QCD) LCWS 2015, Whistler, 4.11.15

  6. WHIZARD: Overview WHIZARD v2.2.7 (11.08.2015) http://whizard.hepforge.org <whizard@desy.de> WHIZARD Team: Wolfgang Kilian, Thorsten Ohl, JRR Simon Braß/Bijan Chokoufé/Marco Sekulla/Christian Weiss/Soyoung Shim/Florian Staub/Zhijie Zhao + 2 Master (some losses: C. Speckner [software engineering], F. Bach [European Commission], S. Schmidt [Philosophy]) Publication: EPJ C71 (2011) 1742 (and others for O’Mega, Interfaces, color flow formalism) J.R.Reuter Top Physics in WHIZARD (+NLO/QCD) LCWS 2015, Whistler, 4.11.15

  7. WHIZARD: Overview WHIZARD v2.2.7 (11.08.2015) http://whizard.hepforge.org <whizard@desy.de> WHIZARD Team: Wolfgang Kilian, Thorsten Ohl, JRR Simon Braß/Bijan Chokoufé/Marco Sekulla/Christian Weiss/Soyoung Shim/Florian Staub/Zhijie Zhao + 2 Master (some losses: C. Speckner [software engineering], F. Bach [European Commission], S. Schmidt [Philosophy]) Publication: EPJ C71 (2011) 1742 (and others for O’Mega, Interfaces, color flow formalism) LHC K. Desch, DESY Th-WS ‘15 2nd WHIZARD Workshop Würzburg, 03/2015 J.R.Reuter Top Physics in WHIZARD (+NLO/QCD) LCWS 2015, Whistler, 4.11.15

  8. WHIZARD Parton Shower Two independent implementations: kT -ordered QCD and Analytic QCD shower Analytic shower: no shower veto ⇒ exact shower history known, allows reweighting Kilian/JRR/Schmidt/Wiesler, JHEP 1204 013 (2012) Technical overhaul of the shower / merging part Plans: implement GKS matching, QED shower (also interleaved, infrastructure ready) J.R.Reuter Top Physics in WHIZARD (+NLO/QCD) LCWS 2015, Whistler, 4.11.15

  9. Tuning of the WHIZARD Parton Shower First tunes of both kT -ordered QCD and Analytic QCD shower Chokoufe/Englert/JRR, 2015 Di- and Multijet data from LEP as given in RIVET analysis Usage of the PROFESSOR tool for determining the best fit Buckley et al., 2009 J.R.Reuter Top Physics in WHIZARD (+NLO/QCD) LCWS 2015, Whistler, 4.11.15

  10. NLO Development in WHIZARD Need for precision predictions that match (sub-) percent experimental accuracy mainly NLO corrections, but also QED and electroweak (ee) Binoth Les Houches Interface (BLHA): Workflow 1. Process definition in SINDARIN (contract to One-Loop Program [OLP]) 2. OLP generates code (Born/virtual interference), WHIZARD reads contract 3. NLO matrix element library loaded into WHIZARD J.R.Reuter Top Physics in WHIZARD (+NLO/QCD) LCWS 2015, Whistler, 4.11.15

  11. NLO Development in WHIZARD Need for precision predictions that match (sub-) percent experimental accuracy mainly NLO corrections, but also QED and electroweak (ee) Binoth Les Houches Interface (BLHA): Workflow 1. Process definition in SINDARIN (contract to One-Loop Program [OLP]) 2. OLP generates code (Born/virtual interference), WHIZARD reads contract 3. NLO matrix element library loaded into WHIZARD Working NLO interfaces to: � GoSam [G. Cullen et al.] � OpenLoops [F. Cascioli et al.] (first focus on QCD corrections) J.R.Reuter Top Physics in WHIZARD (+NLO/QCD) LCWS 2015, Whistler, 4.11.15

  12. NLO Development in WHIZARD Need for precision predictions that match (sub-) percent experimental accuracy mainly NLO corrections, but also QED and electroweak (ee) Binoth Les Houches Interface (BLHA): Workflow 1. Process definition in SINDARIN (contract to One-Loop Program [OLP]) 2. OLP generates code (Born/virtual interference), WHIZARD reads contract 3. NLO matrix element library loaded into WHIZARD Working NLO interfaces to: � GoSam [G. Cullen et al.] � OpenLoops [F. Cascioli et al.] (first focus on QCD corrections) WHIZARD v2.2.6 contains alpha version QCD corrections (massless and massive emitters) alpha_power = 2 alphas_power = 0 process eett = e1,E1 => t, tbar { nlo_calculation = “full” } J.R.Reuter Top Physics in WHIZARD (+NLO/QCD) LCWS 2015, Whistler, 4.11.15

  13. NLO Development in WHIZARD Need for precision predictions that match (sub-) percent experimental accuracy mainly NLO corrections, but also QED and electroweak (ee) Binoth Les Houches Interface (BLHA): Workflow 1. Process definition in SINDARIN (contract to One-Loop Program [OLP]) 2. OLP generates code (Born/virtual interference), WHIZARD reads contract 3. NLO matrix element library loaded into WHIZARD Working NLO interfaces to: � GoSam [G. Cullen et al.] � OpenLoops [F. Cascioli et al.] (first focus on QCD corrections) WHIZARD v2.2.6 contains alpha version QCD corrections (massless and massive emitters) alpha_power = 2 alphas_power = 0 process eett = e1,E1 => t, tbar { nlo_calculation = “full” } J.R.Reuter Top Physics in WHIZARD (+NLO/QCD) LCWS 2015, Whistler, 4.11.15

  14. NLO Development in WHIZARD Need for precision predictions that match (sub-) percent experimental accuracy mainly NLO corrections, but also QED and electroweak (ee) Binoth Les Houches Interface (BLHA): Workflow 1. Process definition in SINDARIN (contract to One-Loop Program [OLP]) 2. OLP generates code (Born/virtual interference), WHIZARD reads contract 3. NLO matrix element library loaded into WHIZARD Working NLO interfaces to: � GoSam [G. Cullen et al.] � OpenLoops [F. Cascioli et al.] (first focus on QCD corrections) fixedorder 1000 WHIZARD v2.2.6 contains alpha version 800 QCD corrections (massless and massive emitters) 600 σ [fb] alpha_power = 2 400 alphas_power = 0 200 process eett = e1,E1 => t, tbar onshell, LO { nlo_calculation = “full” } onshell, NLO offshell, LO offshell, NLO 0 350 400 450 500 550 600 √ s [GeV] J.R.Reuter Top Physics in WHIZARD (+NLO/QCD) LCWS 2015, Whistler, 4.11.15

  15. FKS Subtraction (Frixione/Kunszt/Signer) Subtraction formalism to make real and virtual contributions separately finite Z Z Z � d σ R − d σ S � d σ NLO = d σ S + d σ V + n +1 n +1 n | {z } | {z } finite finite J.R.Reuter Top Physics in WHIZARD (+NLO/QCD) LCWS 2015, Whistler, 4.11.15

  16. FKS Subtraction (Frixione/Kunszt/Signer) Subtraction formalism to make real and virtual contributions separately finite Z Z Z � d σ R − d σ S � d σ NLO = d σ S + d σ V + n +1 n +1 n | {z } | {z } finite finite Automated subtraction terms in WHIZARD, algorithm: ✴ Find all singular pairs I = { (1 , 5) , (1 , 6) , (2 , 5) , (2 , 6) , (5 , 6) } ✴ Partition phase space according to singular regions X 1 = S α ( Φ ) α ∈ I ✴ Generate subtraction terms for singular regions J.R.Reuter Top Physics in WHIZARD (+NLO/QCD) LCWS 2015, Whistler, 4.11.15

  17. FKS Subtraction (Frixione/Kunszt/Signer) Subtraction formalism to make real and virtual contributions separately finite Z Z Z � d σ R − d σ S � d σ NLO = d σ S + d σ V + n +1 n +1 n | {z } | {z } finite finite Automated subtraction terms in WHIZARD, algorithm: ✴ Find all singular pairs I = { (1 , 5) , (1 , 6) , (2 , 5) , (2 , 6) , (5 , 6) } ✴ Partition phase space according to singular regions X 1 = S α ( Φ ) α ∈ I ✴ Generate subtraction terms for singular regions J.R.Reuter Top Physics in WHIZARD (+NLO/QCD) LCWS 2015, Whistler, 4.11.15

  18. Examples and Validation Simplest benchmark process: / σ LO = α s / π e + e − → q ¯ σ NLO − σ LO � � q with Plot for total cross section for fixed strong coupling constant List of validated QCD NLO processes e + e − → q ¯ q • e + e − → q ¯ qg • • Cross-checks with MG5_aMC@NLO e + e − → ` + ` − q ¯ q • • Phase space integration for virtuals performs great e + e − → ` + ⌫ ` q ¯ q • e + e − → t ¯ t • e + e − → tW − b • e + e − → W + W − b ¯ b • e + e − → t ¯ tH • J.R.Reuter Top Physics in WHIZARD (+NLO/QCD) LCWS 2015, Whistler, 4.11.15

  19. Examples and Validation Simplest benchmark process: / σ LO = α s / π e + e − → q ¯ σ NLO − σ LO � � q with Plot for total cross section for fixed strong coupling constant List of validated QCD NLO processes e + e − → q ¯ q • e + e − → q ¯ qg • • Cross-checks with MG5_aMC@NLO e + e − → ` + ` − q ¯ q • • Phase space integration for virtuals performs great e + e − → ` + ⌫ ` q ¯ q • e + e − → t ¯ t • ✦ QCD NLO infrastructure in pp complete e + e − → tW − b • ✦ First attempts on electroweak corrections, e + e − → W + W − b ¯ b • interfacing the RECOLA code [Denner et al.] e + e − → t ¯ tH • J.R.Reuter Top Physics in WHIZARD (+NLO/QCD) LCWS 2015, Whistler, 4.11.15

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