bachelor_thesis/notes.org
2020-06-05 09:37:25 +02:00

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* Literatur
** Latex
*** Latex/KOMA Ref-Sheet
- [[file:literature/prog/LaTeX_RefSheet.pdf][Refsheet]]
*** KOMA Docs
- [[file:literature/prog/scrguide.pdf][KOMA Docs]]
*** AUCTeX
- [[file:literature/prog/tex-ref.pdf][Auctex]]
*** Modular Documents
- [[https://en.wikibooks.org/wiki/LaTeX/Modular_Documents][Modular Documents]]
** Feynman Rules
*** Siegert Vorlesung
:LOGBOOK:
CLOCK: [2020-03-18 Wed 10:57]--[2020-03-18 Wed 11:20] => 0:23
:END:
- [[file:literature/feynman/tk-vorlesung.pdf][Vorlesung]]
- [[file:literature/feynman/tk-vorlesung.pdf::54][Kapitel 4.3]]
- Feynman Diags etc...
- [[file:literature/feynman/tk-vorlesung.pdf::64][Kapitel 4.4]]
- Beispiel zur Berechnung
** Particle Physics
*** Thomson
:LOGBOOK:
CLOCK: [2020-03-18 Wed 16:32]--[2020-03-18 Wed 21:01] => 4:29
CLOCK: [2020-03-18 Wed 11:20]--[2020-03-18 Wed 14:21] => 3:01
:END:
- [[file:literature/feynman/Thomson.pdf][Modern Particle Physics]]
- [[file:literature/feynman/Thomson.pdf::100][Spinors]]
- [[file:literature/feynman/Thomson.pdf::107][Spinors, Helicity Eigenstates]]
- [[file:literature/feynman/Thomson.pdf::533][Completeness Pol. Vectors]]
** Rivet
- [[https://gitlab.com/hepcedar/rivet/tree/master/doc/tutorials][getting started]]
- [[https://gitlab.com/hepcedar/rivet/tree/master/doc/tutorials][sherpa and rivet tutorial]]
** Monte Carlo
- [[file:literature/mc/general_purp_evt.pdf::170][Allgemeines zu MC integration, sampling]]
- [[file:literature/mc/vegas.pdf][VEGAS]]
- [[file:literature/mc/vegas_algo.pdf][VEGAS Algorithm]]
** PDFs
- [[file:literature/pdf/lhapdf6.pdf][LHAPDF6]]
** Pseudo Rapidity
- https://physics.stackexchange.com/questions/12258/why-is-pseudorapidity-defined-as-log-tan-theta-2
** Sherpa
-
* Aufgaben
** Erste Aufgabenp
:LOGBOOK:
CLOCK: [2020-03-20 Fri 09:30]
:END:
*** Mail von Siegert
:LOGBOOK:
CLOCK: [2020-03-19 Thu 15:21]--[2020-03-19 Thu 17:25] => 2:04
CLOCK: [2020-03-19 Thu 10:05]--[2020-03-19 Thu 11:56] => 1:51
:END:
Hi Valentin,
alles klar. Das Formular machen wir dann einfach im Nachhinein und
datieren es zurueck.
Dann wuerde ich zur Einarbeitung vorschlagen, Du schaust Dir mal
meinen Aufschrieb zu Feynman-Regeln und der |M|^2-Berechnung aus der
Vorlesung an, Kapitel 4.3 und 4.4 hier:
http://fsiegert.web.cern.ch/fsiegert/tmp/tk-vorlesung.pdf
Versuch das erstmal fuer den gezeigten Prozess nachzuvollziehen, und
schau dann, ob Du folgende Uebungsaufgaben aus meinem Kurs kannst: 4.1
4.2 5.1 5.2 5.3
https://bildungsportal.sachsen.de/opal/auth/RepositoryEntry/11966152704/CourseNode/92162447560998
Wenn Du konzeptionell oder rechnerisch irgendwo haengen bleibst, reden
wir (Skype/Vidyo/Zoom/...), damit ich einzelnes nochmal naeher
erlaeutern kann. Wenn Du damit durch bist, kann ich Dir die
Musterloesungen zur Verfuegung stellen und du schaust nochmal genauer,
ob noch irgendwas unklar ist.
Dann kannst Du mal qq->yy rechnen.
Klingt das OK fuer den Start?
Viele Gruesse, Frank
** Berechnung qq -> γγ
- 4 Anlaeufe :). Idiotischerweise 4-Vektor negiert
- letzter Anlauf mit Casimir Trick erfolgreich
- gute tricks:
- γ auf z Achse
- Symmetrien Beachten -> spart die Haelfte beim umdrehen der Spins
- Vollstaendigkeitsrelation von pol. Vektoren in Form: [[file:literature/feynman/Thomson.pdf::533][Completeness Pol. Vectors]]
** Vergleich mit Sherpa
- [[file:prog/runcards/qqgg/Sherpa.yaml][Runcard]]
- [[file:prog/python/qqgg/analytical_xs.ipynb][Notebook mit Implementierung der XS]]
- Zeigte fehler in Rechnung auf
** Monte Carlo Methods
- implementation as [[file:prog/python/qqgg/monte_carlo.py][module]]
- [[file:prog/python/qqgg/analytical_xs.org::*Numerical Integration][Integration]]
- [[file:prog/python/qqgg/analytical_xs.org::*Sampling and Analysis][Sampling and Analysis]]
*** DONE Check Statistics
- 100 mal.... 67, check with random seed
- error bars in histtype
*** DONE Variablen Trafo geschickt waehlen.
- stratified sampling, vegas
**** TODO Something fishy about that variance estimate in vegas!!!
- overesimate even stronger if evaluation point number increased
*** DONE Sherpa + Rivet
- analyse + histogramme
- Analysis: ~MC_DIPHOTON~, [[https://rivet.hepforge.org/analyses/MC_DIPHOTON.html][analysis reference]]
- sherpa configure: ~../configure --enable-rivet=/usr/bin/rivet --prefix=/usr --enable-hepmc2=/usr~
- manual
** Parton Density functions
- [[https://lhapdf.hepforge.org/][pdf library]]
** Phaeono
*** pT sortieren
*** TODO Shower
- pT only works with showers
- remnants of proton create showers -> without fragmentation: no hadrons
- can create more photons
- limited -> conserves m_yy
- Other recoil scheme [[https://sherpa-team.gitlab.io/sherpa/master/manual/parameters/parton-showers.html#cs-shower-options][CSS_KIN_SCHEME=0]] could fix that
*** TODO Fragmentation,
- https://sherpa-team.gitlab.io/sherpa/master/manual/parameters/hadronization.html?highlight=fragmentation#id18
- showers recombinate to hadrons
- more photons
*** TODO MI
- multiple partons interact, create showers etc
* Clock Table
#+BEGIN: clocktable :scope file :maxlevel 2
#+CAPTION: Clock summary at [2020-03-18 Wed 21:01]
| Headline | Time | |
|----------------------+--------+------|
| *Total time* | *7:53* | |
|----------------------+--------+------|
| Literatur | 7:53 | |
| \_ Feynman Rules | | 0:23 |
| \_ Particle Physics | | 7:30 |
#+END:
* Fragen
** Lorentz Invar. Matrixelement
- Ich stand ganz schoen auf dem Schlauch: Lorentz Invar = selbe Form
in allen BS (muss nicht unb. konst bei LT sein), lorentzskalarfeld
** Impulserhaltung aus dem Gefuehl... (ohne deltas) ok?
** Normierung Photonenfeld?
** Globaler Spin bei pol. Vektoren?
** Spin nicht erhalten?
** Abweichungen im vergeich weiter diskutieren?
** Flavours im Proton
** Sind quark verhaeltnisse in PDF enthalten (2:1 fuer proton)
** beide finalstate photonen behalten?
** PDF members
** Sensitivity detectors cite! -> separation from beam
** was fuer eine pdf ist das NNPDF31lo
** four mom. conservation errors
** Warum Veto nur fuer MUONS
- ich habe auch photons gevetoed
** Initial und finals state radiation?
** MPI
- nur QCD -> wichtigste prozesse modelliert
- The Jimmy model stops here, considering only hard events, and so
it can only be applied to underlying event.
- doesn't the mpi contain soft inclusive physics
** Jet algos
- what are jet xs? -> particles jets as legs
- why ist double counting a problem -> in exact calculation -> same diagramm
- IS radiation: all partons?
** Soft Inclusive
- wtf are those processes
** what does inclusive mean
** Normalize to XS
** y axis label for normalized histos
** TODO PDF cannot be derived: in principle?
** TODO still compatible?
** TODO cite atlas paper (analysis?)
* Work Log
** 18.03
- habe mich in manche konzeptionelle Dinge ziemlich verrannt!
* Todo
** TODO lab xs kuerzen
** TODO shower scale anpassen
** TODO effekt shower und kperp
** DONE y-axis a.u.!
** DONE mean, var einzeichnen
** DONE Variance of vegas weighted f!
** DONE look at xs plot -> they seem different
** TODO take new sample: still bias?
* Observations
** Azimuthal Angle
- 0 for basic
- converge at large angle -> expected
- smaller angle with PS but also last bin smaller
- all otherssimilar, at lower -> MI/Hadrons (copatible) a little higher
- in general flattens out
** Cos Θ
- similar shape as before
- all others a little bit enhanced over basic
- Hadonization usually highest but within range of others
- converge at big angles
- MI a little lower in center region
** η
- big drop at extremes
- more weight towards center (isolation?)
- drop already with PS, mode With hadronization
- most drop with MI and pT -> why that difference with hadronization
- could still be statistical
- hadronized xs seems enhanced
- but shape change dominated through PSeudo
** Invariant Mass
- very similar to basic process, no huge effects
- max ~ 300 Gev
- generally shiftet to lower energies (under the cuts, additional pT -> pass cut)
- all but basic copatible with ps,ps+pt enhanced over hadrons (noise?)
- very few smaller than cut with mi
- PS alone enhanced towards high myy but low in last bin
- mi seems ban
** Scattering Angle
- enhanced at small angles
- all converge to zero
- mostly compatible
- mi lower
** Scattering Angle in CS Frame
- similar to lab frame (total pT not that big on average ~1 GeV, Around 500 GeV max)
- all effects converge to the same non-zero
- finite pT -> photons with small scattering angle pass cuts
- likeness to lab frame -> good generalisation, interesting effect may be isolated
- mi lower on average
** pT leading
- first 2 bins lower than basic, others bigger
- shifting the pT distribution -> intrinsic + jet pT
- PS a little bit enhanced in first bin
- from pT on all similar
- mi lower on average
** pT subleading
- very similar in shape
- almost constant factor smaller with PS, pT
- pT, hadrons compat, mi a little lower
- total pT shift -> subleading gets less pT
** total pT
- most at ~ 2 Gev
- max around 100 Gev (as inv mass)
- steep drop after ~ 50 GeV
- pig differences at low pT, MI enhnaced (here isolation seems to work better, less transverse jets?), statistics
- pS not enough, only with pT (remnants) conclusive picture
** XS
- with all other effects similar
- why is MI not bigger? -> does not modify IS!
** overal
- mi lower
- remnants+pT usually pretty good approx