Opened 15 years ago
Closed 5 years ago
#142 closed enhancement (duplicate)
Generalized color structures
Reported by: | Juergen Reuter | Owned by: | kilian, ohl, jr_reuter |
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Priority: | P2 | Milestone: | v4.0 |
Component: | omega | Version: | 2.0.0rc2 |
Severity: | major | Keywords: | color correlations |
Cc: |
Description (last modified by )
Generalized color structures (sextets, eps_ijk couplings, etc.) should be supported by the colorizer inside O'Mega.
Change History (25)
comment:1 Changed 15 years ago by
Milestone: | v2.1 → v2.0final |
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Owner: | changed from jr_reuter, cnspeckn to ohl |
Priority: | P3 → P1 |
Severity: | normal → critical |
Type: | task → defect |
Version: | → 2.0rc2 |
comment:2 Changed 15 years ago by
Status: | new → assigned |
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comment:3 Changed 15 years ago by
Milestone: | v2.0.0final → v2.0-rc4 |
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comment:4 Changed 15 years ago by
Owner: | changed from ohl to kilian |
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Status: | assigned → new |
OK, I have new implemented CS's algorithm in the O'Mega color factors. WHIZARD should use the result or reimplement it in Fortran (see src/omega/src/color.ml).
An algorithm using the "(i,-i)-Gluons" runs into two problems:
- it works for gl gl -> H, but requires more and more patchwork in higher orders
- it becomes homelessly inefficient, because too many new color structures must be tried out.
comment:5 Changed 15 years ago by
Priority: | P1 → P3 |
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Severity: | critical → normal |
This now basically depends on ticket #20. Ranking it down.
comment:6 Changed 15 years ago by
Owner: | changed from kilian to ohl |
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Status: | new → assigned |
comment:7 Changed 15 years ago by
Severity: | normal → critical |
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I take the liberty to bump this and raise the severity again as other vertices like graviton-gluon-gluon also depend on this.
comment:8 Changed 15 years ago by
Description: | modified (diff) |
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Milestone: | v2.0-rc4 → v2.1 |
Priority: | P3 → P2 |
Summary: | H -> gg coupling and generalized color structures → Generalized color structures |
Type: | defect → enhancement |
Since #20 is closed, the Hgg part is done and the generalized color structures can be moved to milestone:v2.1
comment:9 Changed 15 years ago by
Milestone: | v2.1 → v2.0.2 |
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Priority: | P2 → P1 |
As this is TOs primary target right now, I move it (optimistically to 2.0.2 first), as the ticket ordering confused several other WHIZARD authors. Furthermore rank it high.
comment:10 Changed 15 years ago by
Priority: | P1 → P2 |
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This was bogus from my side, I confused the tickets. This is the second or third on TOs priority list. Going back to P2 for it.
comment:11 Changed 15 years ago by
Milestone: | v2.0.2 → v2.0.3 |
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comment:12 Changed 15 years ago by
Milestone: | v2.0.3 → v2.0.4 |
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comment:13 Changed 14 years ago by
Milestone: | v2.0.4 → v2.0.5 |
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comment:14 Changed 14 years ago by
Milestone: | v2.0.5 → v2.0.6 |
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comment:15 Changed 14 years ago by
Included a lot of infrastructure in the branch branches/color6, but we have to agree on the data structure for the color flows. Either the rather pedestrian way with Double_Lines and Triple_Lines inside the framework of Module Flow, or the General_Flow set-up. I would rather go for the second one, which is much cleaner and fancier.
comment:16 Changed 14 years ago by
Milestone: | v2.0.6 → v2.1.0 |
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Owner: | changed from ohl to kilian, ohl, jr_reuter |
Status: | assigned → new |
This needs to be a joint effort. And I guess, we better move it to 2.1.0.
comment:17 Changed 13 years ago by
Priority: | P2 → P1 |
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comment:18 Changed 12 years ago by
Milestone: | v2.3.1 → v2.2.0 |
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Priority: | P1 → P2 |
Severity: | critical → major |
That will be also (started to be) resolved with #56. So moving it close.
comment:19 Changed 11 years ago by
Milestone: | v2.2.0 → v2.2.1 |
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comment:20 Changed 11 years ago by
Milestone: | v2.2.1 → v2.3.0 |
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comment:21 Changed 9 years ago by
Milestone: | v2.3.0 → v2.4.0 |
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comment:24 Changed 7 years ago by
Milestone: | v2.6.0 → v4.0 |
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comment:25 Changed 5 years ago by
Resolution: | → duplicate |
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Status: | new → closed |
Transferred to Gitlab issue 322.
I just discussed this with Christian and we've found the solution: introduce a set of "ghost" particles that couple only to color singlets and are counted just like the normal ghosts. Each closed loop of these ghosts receives a (-1) so that we get 9 - 1 = 8. This can be derived formally by treating the Higgs as an external field and using the gluon propagator in this external field (i.e. with Higgs insertions resummed).
This can be implemented directly in O'Mega, once the color summation is moved to O'Mega.