Skip to content
Snippets Groups Projects
Commit b75eaf6d authored by Tooba Ali's avatar Tooba Ali
Browse files

Update benchmarks/dis/analysis/truth_reconstruction.py

parent f509b846
No related branches found
No related tags found
No related merge requests found
......@@ -168,49 +168,12 @@ for i in range(len(MC_list)): #Repeat the following steps for each variable (mom
plt.savefig(os.path.join(r_path, '%s_%s_%s.png' % (title_list[i],title,config)))
plt.close()
################################################################################################### #Correlation
###################################################################################################
#####For momentum variable
X_s = np.array(ak.flatten(X1))
Y_s = np.array(ak.flatten(Y1))
if i == 0 and particle in particle_dict.keys(): #Momentum in Single events
h, xedges, yedges, image = plt.hist2d(x=X_s,y= Y_s, bins = 11)
else:
h, xedges, yedges, image = plt.hist2d(x=X_s,y= Y_s, bins = 11, range = [x_range,x_range])
plt.close()
col_sum = ak.sum(h,axis=-1) #number of events in each (verticle) column
norm_h = [] #norm_h is the normalized matrix
norm_h_text = []
for j in range(len(col_sum)):
if col_sum[j] != 0:
norm_c = h[j]/col_sum[j] #normalized column = column values divide by sum of the column
else:
norm_c = h[j]
norm_h.append(norm_c)
norm_c_text = [ '%.3f' % elem for elem in norm_c ] #display value to 3 dp
norm_h_text.append(norm_c_text)
fig, axs = plt.subplots(1, 2, figsize=(20, 10))
if i == 0 and particle in particle_dict.keys(): #Momentum in Single events
axs[0].hist2d(x=X_s,y=Y_s, bins = 11)
else:
axs[0].hist2d(x=X_s,y=Y_s, bins = 11,range = [x_range,x_range])
mplhep.hist2dplot(H=norm_h,norm=mpl.colors.LogNorm(vmin= 1e-4, vmax= 1),labels=norm_h_text, xbins = xedges, ybins = yedges, ax=axs[1])
axs[0].set_title('%s Histogram'%(title_list[i]))
axs[0].set_xlabel('%s_mc'%(title_list[i]))
axs[0].set_ylabel('%s_rc'%(title_list[i]))
axs[1].set_xlabel('%s_mc'%(title_list[i]))
axs[1].set_ylabel('%s_rc'%(title_list[i]))
axs[1].set_title('%s Correlation'%(title_list[i]))
fig.suptitle('%s %s events'%(config,Nevents))
plt.savefig(os.path.join(r_path, '%s_correlation_%s.png' % (title_list[i],config)))
#Ratio vs momentum
###################################################################################################
#####For theta, phi, eta variable
if i > 0:
for j in range(len(X_list)):
if i > 0: #for each variable theta, phi, and eta
for j in range(len(X_list)): #Repeat the following steps for each particle (pions,protons,electrons,neutrons,photons)
X = X_list[j]
Y = Y_list[j]
M_mc = M_list[j]
......@@ -247,34 +210,67 @@ for i in range(len(MC_list)): #Repeat the following steps for each variable (mom
ax1.set_title('%s Difference Vs Momentum %s %s events'%(title_list[i],config,Nevents))
plt.savefig(os.path.join(r_path, '%s_difference_vs_momentum_%s.png' % (title_list[i],config)))
################################################################################################### #Phi vs Theta plots
###################################################################################################
#Correlation
###################################################################################################
#Repeat the following steps for each variable (momentum,theta,phi,eta)
X_s = np.array(ak.flatten(X1))
Y_s = np.array(ak.flatten(Y1))
#Histogram
if i == 0 and particle in particle_dict.keys(): #Momentum in Single events
h, xedges, yedges, image = plt.hist2d(x=X_s,y= Y_s, bins = 11)
else:
h, xedges, yedges, image = plt.hist2d(x=X_s,y= Y_s, bins = 11, range = [x_range,x_range])
plt.close()
col_sum = ak.sum(h,axis=-1) #number of events in each (verticle) column
norm_h = [] #norm_h is the normalized matrix
norm_h_text = []
for j in range(len(col_sum)):
if col_sum[j] != 0:
norm_c = h[j]/col_sum[j] #normalized column = column values divide by sum of the column
else:
norm_c = h[j]
norm_h.append(norm_c)
norm_c_text = [ '%.3f' % elem for elem in norm_c ] #display value to 3 dp
norm_h_text.append(norm_c_text)
fig, axs = plt.subplots(1, 2, figsize=(20, 10))
if i == 0 and particle in particle_dict.keys(): #Momentum in Single events
axs[0].hist2d(x=X_s,y=Y_s, bins = 11)
else:
axs[0].hist2d(x=X_s,y=Y_s, bins = 11,range = [x_range,x_range])
mplhep.hist2dplot(H=norm_h,norm=mpl.colors.LogNorm(vmin= 1e-4, vmax= 1),labels=norm_h_text, xbins = xedges, ybins = yedges, ax=axs[1])
axs[0].set_title('%s Histogram'%(title_list[i]))
axs[0].set_xlabel('%s_mc'%(title_list[i]))
axs[0].set_ylabel('%s_rc'%(title_list[i]))
axs[1].set_xlabel('%s_mc'%(title_list[i]))
axs[1].set_ylabel('%s_rc'%(title_list[i]))
axs[1].set_title('%s Correlation'%(title_list[i]))
fig.suptitle('%s %s events'%(config,Nevents))
plt.savefig(os.path.join(r_path, '%s_correlation_%s.png' % (title_list[i],config)))
###################################################################################################
#Phi vs Theta plots
###################################################################################################
def particle_plots(boolean_particle):
theta_mc_fil = ak.Array(theta_mc[simID][booll])[boolean_particle]
#filtered lists w.r.t the particle
theta_mc_fil = ak.Array(theta_mc[simID][booll])[boolean_particle]
theta_rc_fil = ak.Array(theta_rc[recID][booll])[boolean_particle]
phi_mc_fil = ak.Array(phi_mc[simID][booll])[boolean_particle]
phi_rc_fil = ak.Array(phi_rc[recID][booll])[boolean_particle]
theta_mc_fil_len = ak.count(theta_mc_fil,axis=None)
theta_rc_fil_len = ak.count(theta_rc_fil,axis=None)
if theta_mc_fil_len > theta_rc_fil_len:
F_boolean = np.ones_like(theta_rc_fil) == 1
else:
F_boolean = np.ones_like(theta_mc_fil) == 1
theta_mc_F = np.array(ak.flatten(theta_mc_fil[F_boolean]))
theta_rc_F = np.array(ak.flatten(theta_rc_fil[F_boolean]))
phi_mc_F = np.array(ak.flatten(phi_mc_fil[F_boolean]))
phi_rc_F = np.array(ak.flatten(phi_rc_fil[F_boolean]))
ratio = np.array((ak.Array(theta_rc_F)-(ak.Array(theta_mc_F))))
ratio = np.array((ak.Array(theta_rc_fil)-(ak.Array(theta_mc_fil))))
fig = plt.figure()
gs = fig.add_gridspec(2, 2, wspace=0.01)
(ax1, ax2), (ax3, ax4) = gs.subplots(sharex=True, sharey=True)
ax1.scatter(-theta_mc_F, ratio, s = ssize)
ax2.scatter(-theta_rc_F, ratio, s = ssize)
ax3.scatter(-theta_mc_F, phi_mc_F, s = ssize)
ax4.scatter(-theta_rc_F, phi_rc_F, s = ssize)
ax1.scatter(-theta_mc_fil, ratio, s = ssize)
ax2.scatter(-theta_rc_fil, ratio, s = ssize)
ax3.scatter(-theta_mc_fil, phi_mc_fil, s = ssize)
ax4.scatter(-theta_rc_fil, phi_rc_fil, s = ssize)
ax1.set_ylabel('rc-mc')
ax2.set_ylabel('rc-mc')
ax3.set_ylabel('Phi mc')
......
0% Loading or .
You are about to add 0 people to the discussion. Proceed with caution.
Please register or to comment