2020-03-30 15:43:55 +02:00
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#+PROPERTY: header-args :exports both :output-dir results
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2020-03-27 15:43:13 +01:00
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2020-03-27 13:39:00 +01:00
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* Init
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** Required Modules
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#+NAME: e988e3f2-ad1f-49a3-ad60-bedba3863283
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2020-03-27 19:34:22 +01:00
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#+begin_src ipython :session :exports both
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import numpy as np
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import matplotlib.pyplot as plt
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#+end_src
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2020-03-27 13:39:00 +01:00
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#+RESULTS: e988e3f2-ad1f-49a3-ad60-bedba3863283
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** Utilities
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#+NAME: 53548778-a4c1-461a-9b1f-0f401df12b08
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2020-03-30 15:43:55 +02:00
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#+BEGIN_SRC ipython :session :exports both
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2020-03-27 13:39:00 +01:00
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%run ../utility.py
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#+END_SRC
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#+RESULTS: 53548778-a4c1-461a-9b1f-0f401df12b08
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2020-03-30 15:43:55 +02:00
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* Implementation
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2020-03-27 13:39:00 +01:00
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#+NAME: 777a013b-6c20-44bd-b58b-6a7690c21c0e
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2020-03-30 15:43:55 +02:00
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#+BEGIN_SRC ipython :session :exports both :results raw drawer :exports code :tangle tangled/xs.py
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2020-03-27 13:39:00 +01:00
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"""
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Implementation of the analytical cross section for q q_bar ->
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gamma gamma
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Author: Valentin Boettcher <hiro@protagon.space>
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"""
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import numpy as np
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from scipy.constants import alpha
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# NOTE: a more elegant solution would be a decorator
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def energy_factor(charge, esp):
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"""
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Calculates the factor common to all other values in this module
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Arguments:
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esp -- center of momentum energy in GeV
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charge -- charge of the particle in units of the elementary charge
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"""
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2020-03-27 14:30:55 +01:00
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return charge**4*(alpha/esp)**2/6
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2020-03-27 13:39:00 +01:00
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2020-03-28 11:43:21 +01:00
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def diff_xs(θ, charge, esp):
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2020-03-27 13:39:00 +01:00
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"""
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Calculates the differential cross section as a function of the
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2020-03-30 15:43:55 +02:00
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azimuth angle θ in units of 1/GeV².
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2020-03-27 13:39:00 +01:00
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Arguments:
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2020-03-28 11:43:21 +01:00
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θ -- azimuth angle
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2020-03-27 13:39:00 +01:00
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esp -- center of momentum energy in GeV
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charge -- charge of the particle in units of the elementary charge
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"""
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f = energy_factor(charge, esp)
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2020-03-28 11:43:21 +01:00
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return f*((np.cos(θ)**+1)/np.sin(θ)**2)
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2020-03-27 13:39:00 +01:00
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2020-03-28 11:53:45 +01:00
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def diff_xs_eta(η, charge, esp):
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2020-03-27 13:39:00 +01:00
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"""
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Calculates the differential cross section as a function of the
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pseudo rapidity of the photons in units of 1/GeV^2.
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Arguments:
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2020-03-28 11:43:21 +01:00
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η -- pseudo rapidity
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2020-03-27 13:39:00 +01:00
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esp -- center of momentum energy in GeV
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charge -- charge of the particle in units of the elementary charge
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"""
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f = energy_factor(charge, esp)
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2020-03-28 11:43:21 +01:00
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return f*(2*np.cosh(η)**2 - 1)
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2020-03-27 13:39:00 +01:00
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2020-03-28 11:53:45 +01:00
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def total_xs_eta(η, charge, esp):
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2020-03-27 13:39:00 +01:00
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"""
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Calculates the total cross section as a function of the pseudo
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rapidity of the photons in units of 1/GeV^2. If the rapditiy is
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specified as a tuple, it is interpreted as an interval. Otherwise
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2020-03-28 11:43:21 +01:00
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the interval [-η, η] will be used.
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2020-03-27 13:39:00 +01:00
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Arguments:
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2020-03-28 11:43:21 +01:00
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η -- pseudo rapidity (tuple or number)
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2020-03-27 13:39:00 +01:00
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esp -- center of momentum energy in GeV
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charge -- charge of the particle in units of the elementar charge
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"""
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f = energy_factor(charge, esp)
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2020-03-28 11:43:21 +01:00
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if not isinstance(η, tuple):
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η = (-η, η)
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2020-03-27 13:39:00 +01:00
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2020-03-28 11:43:21 +01:00
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if len(η) != 2:
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raise ValueError('Invalid η cut.')
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2020-03-27 13:39:00 +01:00
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def F(x):
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return np.tanh(x) - 2*x
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2020-03-28 11:43:21 +01:00
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return 2*np.pi*f*(F(η[0]) - F(η[1]))
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2020-03-27 13:39:00 +01:00
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#+END_SRC
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#+RESULTS: 777a013b-6c20-44bd-b58b-6a7690c21c0e
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:RESULTS:
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:END:
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* Calculations
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** XS qq -> gamma gamma
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First, set up the input parameters.
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#+NAME: 7e62918a-2935-41ac-94e0-f0e7c3af8e0d
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2020-03-27 19:34:22 +01:00
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#+BEGIN_SRC ipython :session :exports both :results raw drawer
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2020-03-28 11:43:21 +01:00
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η = 2.5
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2020-03-27 13:39:00 +01:00
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charge = 1/3
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esp = 200 # GeV
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#+END_SRC
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#+RESULTS: 7e62918a-2935-41ac-94e0-f0e7c3af8e0d
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:RESULTS:
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:END:
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And now calculate the cross section in picobarn.
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#+NAME: cf853fb6-d338-482e-bc55-bd9f8e796495
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2020-03-30 15:43:55 +02:00
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#+BEGIN_SRC ipython :session :exports both :results drawer output file :file xs.tex
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xs_gev = total_xs_eta(η, charge, esp)
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2020-03-28 11:43:21 +01:00
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xs_pb = gev_to_pb(xs_gev)
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2020-03-30 15:43:55 +02:00
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print(tex_value(xs_pb, unit=r'\pico\barn', prefix=r'\sigma = ', prec=5))
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2020-03-27 13:39:00 +01:00
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#+END_SRC
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#+RESULTS: cf853fb6-d338-482e-bc55-bd9f8e796495
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:RESULTS:
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2020-03-30 15:43:55 +02:00
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[[file:results/xs.tex]]
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2020-03-27 14:30:55 +01:00
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:END:
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2020-03-27 15:43:13 +01:00
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Compared to sherpa, it's pretty close.
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2020-03-27 14:30:55 +01:00
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#+NAME: 81b5ed93-0312-45dc-beec-e2ba92e22626
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2020-03-27 19:34:22 +01:00
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#+BEGIN_SRC ipython :session :exports both :results raw drawer
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2020-03-27 14:30:55 +01:00
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sherpa = 0.0538009
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xs_pb/sherpa
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#+END_SRC
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#+RESULTS: 81b5ed93-0312-45dc-beec-e2ba92e22626
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:RESULTS:
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0.9998585425137037
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:END:
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2020-03-27 15:43:13 +01:00
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I had to set the runcard option ~EW_SCHEME: alpha0~ to use the pure
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QED coupling constant.
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