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Introduction
Single Particle Response.
Single Particle Response
Collision muons
Truncated $\Delta E / \Delta x$ distribution for calorimeter cell D5 module 10 obtained using 2011 experimental and simulated $W\rightarrow\mu\nu$ collision data. For each muon the deposited energy $\Delta E$ is reconstructed at EM scale using a noniterative Optimal Filtering algorithm. The path length $\Delta x$ of the muon through a calorimeter cell was evaluated as the distance between the entrance and exit points. Contact: Marco van Woerden Marius.Cornelis.van.Woerden@cernNOSPAMPLEASE.ch Date: 2nd September 2015 
pdf version of the figure

Schematic overview of the Tile Calorimeter showing the response $\Delta E / \Delta x$ to $W\rightarrow\mu\nu$ muons from collisions for each cell type, obtained from the average in $\phi$ of the truncated means for each cell using 2011 muon experimental data. Cell types with $\eta<0.1$ and the gap/crack scintillators are not taken into account in the analysis. For each muon the deposited energy $\Delta E$ is reconstructed at EM scale using an noniterative Optimal Filtering algorithm. The path length $\Delta x$ of the muon through a calorimeter cell was evaluated as the distance between the entrance and exit points. Contact: Marco van Woerden Marius.Cornelis.van.Woerden@cernNOSPAMPLEASE.ch Date: 2nd September 2015 
pdf version of the figure

Schematic overview of the Tile Calorimeter showing the response $\Delta E / \Delta x$ to $W\rightarrow\mu\nu$ muons from collisions for each cell type, obtained from the average in $\phi$ of the truncated means for each cell using 2012 muon experimental data. Cell types with $\eta<0.1$ and the gap/crack scintillators are not taken into account in the analysis. For each muon the deposited energy $\Delta E$ is reconstructed at EM scale using an noniterative Optimal Filtering algorithm. The path length $\Delta x$ of the muon through a calorimeter cell was evaluated as the distance between the entrance and exit points. Contact: Marco van Woerden Marius.Cornelis.van.Woerden@cernNOSPAMPLEASE.ch Date: 2nd September 2015 
pdf version of the figure

Schematic overview of the Tile Calorimeter showing the double ratio response $\left(\Delta E / \Delta x\right)_\mathrm{data} / \left(\Delta E / \Delta x\right)_\mathrm{MC}$ to $W\rightarrow\mu\nu$ muons from collisions for each cell type, obtained from the average in $\phi$ of the truncated means for each cell using 2011 experimental and simulated data. Cell types with $\eta<0.1$ and the gap/crack scintillators are not taken into account in the analysis. The deposited energy $\Delta E$ is reconstructed at EM scale using a noniterative Optimal Filtering algorithm for experimental and simulated data. The path length $\Delta x$ of the muon through a calorimeter cell was evaluated as the distance between the entrance and exit points. Contact: Marco van Woerden Marius.Cornelis.van.Woerden@cernNOSPAMPLEASE.ch Date: 2nd September 2015 
pdf version of the figure

Schematic overview of the Tile Calorimeter showing the double ratio response $\left(\Delta E / \Delta x\right)_\mathrm{data} / \left(\Delta E / \Delta x\right)_\mathrm{MC}$ to $W\rightarrow\mu\nu$ muons from collisions for each cell type, obtained from the average in $\phi$ of the truncated means for each cell using 2012 experimental and simulated data. Cell types with $\eta<0.1$ and the gap/crack scintillators are not taken into account in the analysis. The deposited energy $\Delta E$ is reconstructed at EM scale using a noniterative Optimal Filtering algorithm for experimental and simulated data. The path length $\Delta x$ of the muon through a calorimeter cell was evaluated as the distance between the entrance and exit points. Contact: Marco van Woerden Marius.Cornelis.van.Woerden@cernNOSPAMPLEASE.ch Date: 2nd September 2015 
pdf version of the figure

Schematic overview of the Tile Calorimeter showing the estimated dispersion of the relative cell response $\left(\Delta E / \Delta x\right)_\mathrm{data} / \left(\Delta E / \Delta x\right)_\mathrm{MC}$ to $W\rightarrow\mu\nu$ muons from collisions for each cell type, obtained from the average in $\phi$ of the truncated means for each cell using 2011 experimental and simulated data. Cell types with $\eta<0.1$ and the gap/crack scintillators are not taken into account in the analysis. The deposited energy $\Delta E$ is reconstructed at EM scale using a noniterative Optimal Filtering algorithm for experimental and simulated data. The path length $\Delta x$ of the muon through a calorimeter cell was evaluated as the distance between the entrance and exit points. Contact: Marco van Woerden Marius.Cornelis.van.Woerden@cernNOSPAMPLEASE.ch Date: 2nd September 2015 
pdf version of the figure

Schematic overview of the Tile Calorimeter showing the estimated dispersion of the relative cell response $\left(\Delta E / \Delta x\right)_\mathrm{data} / \left(\Delta E / \Delta x\right)_\mathrm{MC}$ to $W\rightarrow\mu\nu$ muons from collisions for each cell type, obtained from the average in $\phi$ of the truncated means for each cell using 2012 experimental and simulated data. Cell types with $\eta<0.1$ and the gap/crack scintillators are not taken into account in the analysis. The deposited energy $\Delta E$ is reconstructed at EM scale using a noniterative Optimal Filtering algorithm for experimental and simulated data. The path length $\Delta x$ of the muon through a calorimeter cell was evaluated as the distance between the entrance and exit points. Contact: Marco van Woerden Marius.Cornelis.van.Woerden@cernNOSPAMPLEASE.ch Date: 2nd September 2015 
pdf version of the figure

Schematic overview of the Tile Calorimeter showing the double ratio response change between 2011 and 2012 $\tfrac{R_{2012}  R_{2011}}{R_{2011}}$ to $W\rightarrow\mu\nu$ muons from collisions for each cell type, obtained from the average in $\phi$ of the truncated means for each cell using 2011 and 2012 experimental and simulated data. Cell types with $\eta<0.1$ and the gap/crack scintillators are not taken into account in the analysis. The deposited energy $\Delta E$ is reconstructed at EM scale using a noniterative Optimal Filtering algorithm for experimental and simulated data. The path length $\Delta x$ of the muon through a calorimeter cell was evaluated as the distance between the entrance and exit points. Numbers are in percentage. Contact: Marco van Woerden Marius.Cornelis.van.Woerden@cernNOSPAMPLEASE.ch Date: 2nd September 2015 
pdf version of the figure

Distribution of the the double ratio response changes between 2011 and 2012 $\tfrac{R_{2012}  R_{2011}}{R_{2011}}$ to $W\rightarrow\mu\nu$ muons from collisions for each cell type, obtained from the average in $\phi$ of the truncated means for each cell using 2011 and 2012 experimental and simulated data. Cell types with $\eta<0.1$ and the gap/crack scintillators are not taken into account in the analysis. The deposited energy $\Delta E$ is reconstructed at EM scale using a noniterative Optimal Filtering algorithm for experimental data and simulated data. The path length $\Delta x$ of the muon through a calorimeter cell was evaluated as the distance between the entrance and exit points. Shown are the mean and the statistical error on the mean of the distribution. Numbers are in percentage. Contact: Marco van Woerden Marius.Cornelis.van.Woerden@cernNOSPAMPLEASE.ch Date: 2nd September 2015 
pdf version of the figure

Calorimeter cell responses $\left(\Delta E / \Delta x\right)_\mathrm{data}$ and $\left(\Delta E / \Delta x\right)_\mathrm{MC}$ and ratio $\left(\Delta E / \Delta x\right)_\mathrm{data} / \left(\Delta E / \Delta x\right)_\mathrm{MC}$ versus pseudorapidity $\eta$ for the ATLAS TileCal innermost layer, obtained from the average in $\phi$ of the truncated means for each cell using 2011 experimental and simulated data. Cell types with $\eta<0.1$ and the gap/crack scintillators are not taken into account in the analysis. The deposited energy $\Delta E$ is reconstructed at EM scale using a noniterative Optimal Filtering algorithm for experimental and simulated data. The path length $\Delta x$ of the muon through a calorimeter cell was evaluated as the distance between the entrance and exit points. Statistical errors are shown. Contact: Marco van Woerden Marius.Cornelis.van.Woerden@cernNOSPAMPLEASE.ch Date: 2nd September 2015 
pdf version of the figure

Calorimeter cell responses $\left(\Delta E / \Delta x\right)_\mathrm{data}$ and $\left(\Delta E / \Delta x\right)_\mathrm{MC}$ and ratio $\left(\Delta E / \Delta x\right)_\mathrm{data} / \left(\Delta E / \Delta x\right)_\mathrm{MC}$ versus pseudorapidity $\eta$ for the ATLAS TileCal innermost layer, obtained from the average in $\phi$ of the truncated means for each cell using 2012 experimental and simulated data. Cell types with $\eta<0.1$ and the gap/crack scintillators are not taken into account in the analysis. The deposited energy $\Delta E$ is reconstructed at EM scale using a noniterative Optimal Filtering algorithm for experimental and simulated data. The path length $\Delta x$ of the muon through a calorimeter cell was evaluated as the distance between the entrance and exit points. Statistical errors are shown. Contact: Marco van Woerden Marius.Cornelis.van.Woerden@cernNOSPAMPLEASE.ch Date: 2nd September 2015 
pdf version of the figure

Calorimeter cell responses $\left(\Delta E / \Delta x\right)_\mathrm{data}$ and $\left(\Delta E / \Delta x\right)_\mathrm{MC}$ and ratio $\left(\Delta E / \Delta x\right)_\mathrm{data} / \left(\Delta E / \Delta x\right)_\mathrm{MC}$ versus pseudorapidity $\eta$ for the ATLAS TileCal middle layer, obtained from the average in $\phi$ of the truncated means for each cell using 2011 experimental and simulated data. Cell types with $\eta<0.1$ and the gap/crack scintillators are not taken into account in the analysis. The deposited energy $\Delta E$ is reconstructed at EM scale using a noniterative Optimal Filtering algorithm for experimental and simulated data. The path length $\Delta x$ of the muon through a calorimeter cell was evaluated as the distance between the entrance and exit points. Statistical errors are shown. The outliers at $\eta = \pm0.95$ represent the response of the calorimeter cells C10. Contact: Marco van Woerden Marius.Cornelis.van.Woerden@cernNOSPAMPLEASE.ch Date: 2nd September 2015 
pdf version of the figure

Calorimeter cell responses $\left(\Delta E / \Delta x\right)_\mathrm{data}$ and $\left(\Delta E / \Delta x\right)_\mathrm{MC}$ and ratio $\left(\Delta E / \Delta x\right)_\mathrm{data} / \left(\Delta E / \Delta x\right)_\mathrm{MC}$ versus pseudorapidity $\eta$ for the ATLAS TileCal middle layer, obtained from the average in $\phi$ of the truncated means for each cell using 2012 experimental and simulated data. Cell types with $\eta<0.1$ and the gap/crack scintillators are not taken into account in the analysis. The deposited energy $\Delta E$ is reconstructed at EM scale using a noniterative Optimal Filtering algorithm for experimental and simulated data. The path length $\Delta x$ of the muon through a calorimeter cell was evaluated as the distance between the entrance and exit points. Statistical errors are shown. The outliers at $\eta = \pm0.95$ represent the response of the calorimeter cells C10. Contact: Marco van Woerden Marius.Cornelis.van.Woerden@cernNOSPAMPLEASE.ch Date: 2nd September 2015 
pdf version of the figure

Calorimeter cell responses $\left(\Delta E / \Delta x\right)_\mathrm{data}$ and $\left(\Delta E / \Delta x\right)_\mathrm{MC}$ and ratio $\left(\Delta E / \Delta x\right)_\mathrm{data} / \left(\Delta E / \Delta x\right)_\mathrm{MC}$ versus pseudorapidity $\eta$ for the ATLAS TileCal outermost layer, obtained from the average in $\phi$ of the truncated means for each cell using 2011 experimental and simulated data. Cell types with $\eta<0.1$ and the gap/crack scintillators are not taken into account in the analysis. The deposited energy $\Delta E$ is reconstructed at EM scale using a noniterative Optimal Filtering algorithm for experimental and simulated data. The path length $\Delta x$ of the muon through a calorimeter cell was evaluated as the distance between the entrance and exit points. Statistical errors are shown. Contact: Marco van Woerden Marius.Cornelis.van.Woerden@cernNOSPAMPLEASE.ch Date: 2nd September 2015 
pdf version of the figure

Calorimeter cell responses $\left(\Delta E / \Delta x\right)_\mathrm{data}$ and $\left(\Delta E / \Delta x\right)_\mathrm{MC}$ and ratio $\left(\Delta E / \Delta x\right)_\mathrm{data} / \left(\Delta E / \Delta x\right)_\mathrm{MC}$ versus pseudorapidity $\eta$ for the ATLAS TileCal outermost layer, obtained from the average in $\phi$ of the truncated means for each cell using 2012 experimental and simulated data. Cell types with $\eta<0.1$ and the gap/crack scintillators are not taken into account in the analysis. The deposited energy $\Delta E$ is reconstructed at EM scale using a noniterative Optimal Filtering algorithm for experimental and simulated data. The path length $\Delta x$ of the muon through a calorimeter cell was evaluated as the distance between the entrance and exit points. Statistical errors are shown. Contact: Marco van Woerden Marius.Cornelis.van.Woerden@cernNOSPAMPLEASE.ch Date: 2nd September 2015 
pdf version of the figure

The ATLAS Tile Calorimeter double ratio response $\left(\Delta E / \Delta x\right)_\mathrm{data} / \left(\Delta E / \Delta x\right)_\mathrm{MC}$ to $W\rightarrow\mu\nu$ muons from collisions for each radial layer, obtained from the weighted average in $\eta$ for each cell type using experimental and simulated data. Cell types with $\eta<0.1$ and the gap/crack scintillators are not taken into account in the analysis. The deposited energy $\Delta E$ is reconstructed at EM scale using a noniterative Optimal Filtering algorithm for experimental and simulated data. The path length $\Delta x$ of the muon through a calorimeter cell was evaluated as the distance between the entrance and exit points. Contact: Marco van Woerden Marius.Cornelis.van.Woerden@cernNOSPAMPLEASE.ch Date: 2nd September 2015 
pdf version of the figure

Ratios of the D5+D6 cells muon signals over the noise (SNR), as a function of the muon track η, for standard offline readout of 2012 data and for LVL1 readout as measured in 2011 during pp collisions, zoomed in the region of interest in η. Contact: Marco van Woerden Marius.Cornelis.van.Woerden@cernNOSPAMPLEASE.ch Date: 22nd June 2013 
pdf version of the figure

Ratios of the D5+D6 cells muon signals over the noise (SNR), as a function of the muon track η, for standard offline readout of 2012 data and for LVL1 readout as measured in 2011 during pp collisions, zoomed in the region of interest in η. Contact: Marco van Woerden Marius.Cornelis.van.Woerden@cernNOSPAMPLEASE.ch Date: 22nd June 2013 
pdf version of the figure

Average energy response versus η in TileCal D5 and D6 cells (η>0), using collision muons in 2012 data. Shown is the average response measured by summing the contributions of both PMTs from the double readout eventbyevent, between 200 MeV (lower cut) and 20 GeV (upper cut). The sum D5+D6 is shown in full circles, the individual cells D5 and D6 in open circles. The error bars represent the standard error on the mean. η of the muon is obtained by extrapolating the muon track from the Inner Track through Tile Calorimeter to the Muon Spectrometer. W → μν events are selected using cuts in missing transverse energy E_{T} > 40 GeV and transverse mass M_{T} > 25 GeV. Events are required to have a single reconstructed muon track. Contact: Marco van Woerden Marius.Cornelis.van.Woerden@cernNOSPAMPLEASE.ch Reference: ATLASPLOTTILECAL2013009 Date: 22nd June 2013 

Average energy response versus η in TileCal D5 and D6 cells (η<0), using collision muons in 2012 data. Shown is the average response measured by summing the contributions of both PMTs from the double readout eventbyevent, between 200 MeV (lower cut) and 20 GeV (upper cut). The sum D5+D6 is shown in full circles, the individual cells D5 and D6 in open circles. The error bars represent the standard error on the mean. η of the muon is obtained by extrapolating the muon track from the Inner Track through Tile Calorimeter to the Muon Spectrometer. W → μν events are selected using cuts in missing transverse energy E_{T} > 40 GeV and transverse mass M_{T} > 25 GeV. Events are required to have a single reconstructed muon track. Contact: Marco van Woerden Marius.Cornelis.van.Woerden@cernNOSPAMPLEASE.ch Reference: ATLASPLOTTILECAL2013009 Date: 22nd June 2013 

Average energy response in TileCal D5 (η>0) versus Δφ, using collision muons in 2012 data. Δφ represents the angle from the center of a Tile Calorimeter module to the center of the adjacent module, ranging from 0 to 2π/64 rad. Shown is the average response measured by summing the contributions of both PMTs from the double readout, between 200 MeV (lower cut) and 20 GeV (upper cut), integrated over the entire η ranges of the cell. The error bars represent the standard error on the mean. The decrease in response in the interface between two adjacent modules is 5% due to the gap of a few millimeters that allows for the WLS fibres to run to the outer radius of the calorimeter between two modules. W → μν events are selected using cuts in missing transverse energy E_{T} > 40 GeV and transverse mass M_{T} > 25 GeV. Events are required to have a single reconstructed muon track. Contact: Marco van Woerden Marius.Cornelis.van.Woerden@cernNOSPAMPLEASE.ch Reference: ATLASPLOTTILECAL2013009 Date: 22nd June 2013 

Average energy response in TileCal D5 (η<0) versus Δφ, using collision muons in 2012 data. Δφ represents the angle from the center of a Tile Calorimeter module to the center of the adjacent module, ranging from 0 to 2π/64 rad. Shown is the average response measured by summing the contributions of both PMTs from the double readout, between 200 MeV (lower cut) and 20 GeV (upper cut), integrated over the entire η ranges of the cell. The error bars represent the standard error on the mean. The decrease in response in the interface between two adjacent modules is 5% due to the gap of a few millimeters that allows for the WLS fibres to run to the outer radius of the calorimeter between two modules. W → μν events are selected using cuts in missing transverse energy E_{T} > 40 GeV and transverse mass M_{T} > 25 GeV. Events are required to have a single reconstructed muon track. Contact: Marco van Woerden Marius.Cornelis.van.Woerden@cernNOSPAMPLEASE.ch Reference: ATLASPLOTTILECAL2013009 Date: 22nd June 2013 

Average energy response in TileCal D6 (η>0) versus Δφ, using collision muons in 2012 data. Δφ represents the angle from the center of a Tile Calorimeter module to the center of the adjacent module, ranging from 0 to 2π/64 rad. Shown is the average response measured by summing the contributions of both PMTs from the double readout, between 200 MeV (lower cut) and 20 GeV (upper cut), integrated over the entire η ranges of the cell. The error bars represent the standard error on the mean. The decrease in response in the interface between two adjacent modules is 5% due to the gap of a few millimeters that allows for the WLS fibres to run to the outer radius of the calorimeter between two modules. W → μν events are selected using cuts in missing transverse energy E_{T} > 40 GeV and transverse mass M_{T} > 25 GeV. Events are required to have a single reconstructed muon track. Contact: Marco van Woerden Marius.Cornelis.van.Woerden@cernNOSPAMPLEASE.ch Reference: ATLASPLOTTILECAL2013009 Date: 22nd June 2013 
 Average energy response in TileCal D6 (η<0) versus Δφ, using collision muons in 2012 data. Δφ represents the angle from the center of a Tile Calorimeter module to the center of the adjacent module, ranging from 0 to 2π/64 rad. Shown is the average response measured by summing the contributions of both PMTs from the double readout, between 200 MeV (lower cut) and 20 GeV (upper cut), integrated over the entire η ranges of the cell. The error bars represent the standard error on the mean. The decrease in response in the interface between two adjacent modules is 5% due to the gap of a few millimeters that allows for the WLS fibres to run to the outer radius of the calorimeter between two modules. W → μν events are selected using cuts in missing transverse energy E_{T} > 40 GeV and transverse mass M_{T} > 25 GeV. Events are required to have a single reconstructed muon track. Contact: Marco van Woerden Marius.Cornelis.van.Woerden@cernNOSPAMPLEASE.ch Reference: ATLASPLOTTILECAL2013009 Date: 22nd June 2013 

Single hadrons
Mean value of the $E/p$ variable as a function of $\eta$, integrated over all $p$ ranges for 2010 Data and Monte Carlo simulation. $E$ refers to the energy deposited in the Tile Calorimeter ($\eta < 1.7$) by the isolated charged particles with momentum $p$ and pseudorapidity $\eta$ (excluding the energy deposited in the scintillators). Charged particles have been selected applying a MIPlike signal requirement for the energy deposition in the LAr calorimeter. Bottom plot: Data/MC ratio of the mean value of the $E/p$ variable, fitted with a constant function. The error shown is only statistical. Bins with low statistics with track $\eta > 1.6$ have been removed. Contact: Antonella Sucurro Antonella.Sucurro@cernNOSPAMPLEASE.ch
Reference: ATLASPLOTTILECAL2011001
Date: 24 March 2011

eps version of the figure

Mean value of the $E/p$ variable as a function of $\phi$, integrated over all $p$ and $\eta$ ranges for 2010 Data and Monte Carlo simulation. $E$ refers to the energy deposited in the Tile Calorimeter ($\eta < 1.7$) by the isolated charged particles with momentum $p$ and pseudorapidity $\eta$ (excluding the energy deposited in the scintillators). Charged particles have been selected applying a MIPlike signal requirement for the energy deposition in the LAr calorimeter. Bottom plot: Data/MC ratio of the mean value of the $E/p$ variable, fitted with a constant function. The error shown is only statistical. Each bin cover a dphi range of ~0.4 Contact: Antonella Sucurro Antonella.Sucurro@cernNOSPAMPLEASE.ch
Reference: ATLASPLOTTILECAL2011001
Date: 24 March 2011

eps version of the figure

Mean value of the $E/p$ variable as a function of $p$, integrated over all $\eta$ ranges for 2010 Data and Monte Carlo simulation. $E$ refers to the energy deposited in the Tile Calorimeter ($\eta < 1.7$) by the isolated charged particles with momentum $p$ and pseudorapidity $\eta$ (excluding the energy deposited in the scintillators). Charged particles have been selected applying a MIPlike signal requirement for the energy deposition in the LAr calorimeter. Bottom plot: Data/MC ratio of the mean value of the $E/p$ variable, fitted with a constant function. The error shown is only statistical. Bins after 20 GeV due to the lack of statistics. Contact: Antonella Sucurro Antonella.Sucurro@cernNOSPAMPLEASE.ch
Reference: ATLASPLOTTILECAL2011001
Date: 24 March 2011

eps version of the figure 
RMS value of the $E/p$ variable as a function of $\eta$, integrated over all $p$ ranges for 2010 Data and Monte Carlo simulation. $E$ refers to the energy deposited in the Tile Calorimeter ($\eta < 1.7$) by the isolated charged particles with momentum $p$ and pseudorapidity $\eta$ (excluding the energy deposited in the scintillators). Charged particles have been selected applying a MIPlike signal requirement for the energy deposition in the LAr calorimeter. Bottom plot: Data/MC ratio of the RMS value of the $E/p$ variable, fitted with a constant function. The error shown is only statistical. Bins with low statistics in the range $\eta > 1.6$ have been removed.
Contact: Antonella Sucurro Antonella.Sucurro@cernNOSPAMPLEASE.ch
Reference: ATLASPLOTTILECAL2011001
Date: 24 March 2011

eps version of the figure 
RMS value of the $E/p$ variable as a function of $\phi$, integrated over all $p$ and $\eta$ ranges for 2010 Data and Monte Carlo simulation. $E$ refers to the energy deposited in the Tile Calorimeter ($\eta < 1.7$) by the isolated charged particles with momentum $p$ and pseudorapidity $\eta$ (excluding the energy deposited in the scintillators). Charged particles have been selected applying a MIPlike signal requirement for the energy deposition in the LAr calorimeter. Bottom plot: Data/MC ratio of the RMS value of the $E/p$ variable, fitted with a constant function. The error shown is only statistical. Each bin cover a dphi range of ~0.4.
Contact: Antonella Sucurro Antonella.Sucurro@cernNOSPAMPLEASE.ch
Reference: ATLASPLOTTILECAL2011001
Date: 24 March 2011

eps version of the figure 
RMS value of the $E/p$ variable as a function of $p$, integrated over all $\eta$ ranges for 2010 Data and Monte Carlo simulation. $E$ refers to the energy deposited in the Tile Calorimeter ($\eta < 1.7$) by the isolated charged particles with momentum $p$ and pseudorapidity $\eta$ (excluding the energy deposited in the scintillators). Charged particles have been selected applying a MIPlike signal requirement for the energy deposition in the LAr calorimeter. Bottom plot: Data/MC ratio of the RMS value of the $E/p$ variable, fitted with a constant function. The error shown is only statistical. Bins after 20 GeV are removed due to the lack of statistics.
Contact: Antonella Sucurro Antonella.Sucurro@cernNOSPAMPLEASE.ch
Reference: ATLASPLOTTILECAL2011001
Date: 24 March 2011

eps version of the figure

Calorimeter Response characterised by energy over momentum (E/p) for isolated tracks, as measured with the Tile Calorimeter, using protonproton collision data from 2011 in the Minimum Bias stream. Minimum Bias monte carlo is generated using Pythia 6 and simulated using Geant4, with the QGSP_Bertini physics list. Simulation is normalized to data using 7 bins in pseudorapidity and 16 bins in transverse momentum. The energy of the track is reconstructed using all nearby clusters in a cone of ΔR < 0.2. Selected tracks pass minimum quality criteria, have pT > 2 GeV and deposit less than 1 GeV in the electromagnetic calorimeter. The plot shows the mean of the E/p ratio for hadronic tracks as a function of pseudorapidity, integrated over the phi coverage of Tile Calorimeter. Black dots represent data and red dots represent simulation. The lower plot shows the ratio of data to simulation in the same pseudorapidity bins. The largest disagreement is 10% for 0.9 < η < 1.1.
Contact: David Jennens David.Jennens@cernNOSPAMPLEASE.ch
Reference: ATLASPLOTTILECAL2013011 ATLCOMTILECAL2013034
Date: 10 July 2013

eps version of the figure 
Calorimeter Response characterised by energy over momentum (E/p) for isolated tracks, as measured with the Tile Calorimeter, using protonproton collision data from 2011 in the Minimum Bias stream. Minimum Bias monte carlo is generated using Pythia 6 and simulated using Geant4, with the QGSP_Bertini physics list. Simulation is normalized to data using 7 bins in pseudorapidity and 16 bins in transverse momentum. The energy of the track is reconstructed using all nearby clusters in a cone of ΔR < 0.2. Selected tracks pass minimum quality criteria, have pT > 2 GeV and deposit less than 1 GeV in the electromagnetic calorimeter. The plot shows the mean of the E/p ratio for hadronic tracks, showering predominantly in Layer A, as a function of pseudorapidity, integrated over the phi coverage of Tile Calorimeter. Black dots represent data and red dots represent simulation. The lower plot shows the ratio of data to simulation in the same pseudorapidity bins. The largest disagreement is 10% for 0.9 < η < 1.1.
Contact: David Jennens David.Jennens@cernNOSPAMPLEASE.ch
Reference: ATLASPLOTTILECAL2013011 ATLCOMTILECAL2013034 Date: 10 July 2013

eps version of the figure 
Calorimeter Response characterised by energy over momentum (E/p) for isolated tracks, as measured with the Tile Calorimeter, using protonproton collision data from 2011 in the Minimum Bias stream. Minimum Bias monte carlo is generated using Pythia 6 and simulated using Geant4, with the QGSP_Bertini physics list. Simulation is normalized to data using 7 bins in pseudorapidity and 16 bins in transverse momentum. The energy of the track is reconstructed using all nearby clusters in a cone of ΔR < 0.2. Selected tracks pass minimum quality criteria, have pT > 2 GeV and deposit less than 1 GeV in the electromagnetic calorimeter. The plot shows the mean of the E/p ratio for hadronic tracks, showering predominantly in Layer BC, as a function of pseudorapidity, integrated over the phi coverage of Tile Calorimeter. Black dots represent data and red dots represent simulation. The lower plot shows the ratio of data to simulation in the same pseudorapidity bins. The largest disagreement is 12% for 1.1 < η < 0.9.
Contact: David Jennens David.Jennens@cernNOSPAMPLEASE.ch
Reference: ATLASPLOTTILECAL2013011 ATLCOMTILECAL2013034
Date: 10 July 2013

eps version of the figure

Calorimeter Response characterised by energy over momentum (E/p) for isolated tracks, as measured with the Tile Calorimeter, using protonproton collision data from 2011 in the Minimum Bias stream. Minimum Bias monte carlo is generated using Pythia 6 and simulated using Geant4, with the QGSP_Bertini physics list. Simulation is normalized to data using 7 bins in pseudorapidity and 16 bins in transverse momentum. The energy of the track is reconstructed using all nearby clusters in a cone of ΔR < 0.2. Selected tracks pass minimum quality criteria, have pT > 2 GeV and deposit less than 1 GeV in the electromagnetic calorimeter. The plot shows the mean of the E/p ratio for hadronic tracks as a function of momentum, integrated over the pseudorapidity and phi coverage of Tile Calorimeter. Black dots represent data and red dots represent simulation. The lower plot shows the ratio of data to simulation in the same momentum bins. The largest disagreement is 12% for 11 < p < 12 GeV.
Contact: David Jennens David.Jennens@cernNOSPAMPLEASE.ch
Reference: ATLASPLOTTILECAL2013011 ATLCOMTILECAL2013034
Date: 10 July 2013

eps version of the figure

Calorimeter Response characterised by energy over momentum (E/p) for isolated tracks, as measured with the Tile Calorimeter, using protonproton collision data from 2011 in the Minimum Bias stream. Minimum Bias monte carlo is generated using Pythia 6 and simulated using Geant4, with the QGSP_Bertini physics list. Simulation is normalized to data using 7 bins in pseudorapidity and 16 bins in transverse momentum. The energy of the track is reconstructed using all nearby clusters in a cone of ΔR < 0.2. Selected tracks pass minimum quality criteria, have pT > 2 GeV and deposit less than 1 GeV in the electromagnetic calorimeter. The plot shows the mean of the E/p ratio for hadronic tracks, showering predominantly in Layer A, as a function of momentum, integrated over the pseudorapidity and phi coverage of Tile Calorimeter. Black dots represent data and red dots represent simulation. The lower plot shows the ratio of data to simulation in the same pseudorapidity bins. The largest disagreement is 14% for 11 < p < 12 GeV.
Contact: David Jennens David.Jennens@cernNOSPAMPLEASE.ch
Reference: ATLASPLOTTILECAL2013011 ATLCOMTILECAL2013034
Date: 10 July 2013

eps version of the figure

Calorimeter Response characterised by energy over momentum (E/p) for isolated tracks, as measured with the Tile Calorimeter, using protonproton collision data from 2011 in the Minimum Bias stream. Minimum Bias monte carlo is generated using Pythia 6 and simulated using Geant4, with the QGSP_Bertini physics list. Simulation is normalized to data using 7 bins in pseudorapidity and 16 bins in transverse momentum. The energy of the track is reconstructed using all nearby clusters in a cone of ΔR < 0.2. Selected tracks pass minimum quality criteria, have pT > 2 GeV and deposit less than 1 GeV in the electromagnetic calorimeter. The plot shows the mean of the E/p ratio for hadronic tracks as a function of phi, integrated over the η < 0.7. Black dots represent data and red dots represent simulation. The lower plot shows the ratio of data to simulation in the same phi bins. The largest disagreement is 10% for 0.9 < Φ < 1.1.
Contact: David Jennens David.Jennens@cernNOSPAMPLEASE.ch
Reference: ATLASPLOTTILECAL2013011 ATLCOMTILECAL2013034
Date: 10 July 2013

eps version of the figure

Calorimeter Response characterised by energy over momentum (E/p) for isolated tracks, as measured with the Tile Calorimeter, using protonproton collision data from 2012 in the Minimum Bias stream. Minimum Bias monte carlo is generated using Pythia 6 and simulated using Geant4, with the QGSP_Bertini physics list. Simulation is normalized to data using 8 bins in pseudorapidity and 16 bins in momentum. The energy of the isolated hadron is reconstructed using all nearby clusters in a cone of ΔR < 0.2. Selected tracks pass minimum quality criteria, have pT > 2 GeV and deposit less than 1 GeV in the electromagnetic calorimeter. The plot shows the mean of the E/p ratio for hadronic tracks as a function of pseudorapidity, integrated over the phi coverage of Tile Calorimeter. Black dots represent data and red dots represent simulation. The lower plot shows the ratio of data to simulation in the same pseudorapidity bins. The largest disagreement is 9% for η < 1.5.
Contact: Leonor Cerda Alberich and Carlos Solans
Reference: ATLASPLOTTILECAL2015014
Date: 2nd March 2015

pdf version of the figure

Calorimeter Response characterised by energy over momentum (E/p) for isolated tracks, as measured with the Tile Calorimeter, using protonproton collision data from 2012 in the Minimum Bias stream. Minimum Bias monte carlo is generated using Pythia 6 and simulated using Geant4, with the QGSP_Bertini physics list. Simulation is normalized to data using 8 bins in pseudorapidity and 16 bins in momentum. The energy of the isolated hadron is reconstructed using all nearby clusters in a cone of ΔR < 0.2. Selected tracks pass minimum quality criteria, have pT > 2 GeV and deposit less than 1 GeV in the electromagnetic calorimeter. The plot shows the mean of the E/p ratio for hadronic tracks as a function of momentum, integrated over the pseudorapidity and phi coverage of Tile Calorimeter. Black dots represent data and red dots represent simulation. The lower plot shows the ratio of data to simulation in the same momentum bins. The largest disagreement is 18% for 9 < p < 10 GeV.
Contact: Leonor Cerda Alberich and Carlos Solans
Reference: ATLASPLOTTILECAL2015014
Date: 2nd March 2015

pdf version of the figure

Calorimeter Response characterised by energy over momentum (E/p) for isolated tracks, as measured with the Tile Calorimeter, using protonproton collision data from 2012 in the Minimum Bias stream. Minimum Bias monte carlo is generated using Pythia 6 and simulated using Geant4, with the QGSP_Bertini physics list. Simulation is normalized to data using 8 bins in pseudorapidity and 16 bins in momentum. The energy of the isolated hadron is reconstructed using all nearby clusters in a cone of ΔR < 0.2. Selected tracks pass minimum quality criteria, have pT > 2 GeV and deposit less than 1 GeV in the electromagnetic calorimeter. The plot shows the mean of the E/p ratio for hadronic tracks as a function of phi, integrated over the η coverage of Tile Calorimeter. Black dots represent data and red dots represent simulation. The lower plot shows the ratio of data to simulation in the same phi bins. The largest disagreement is 11% for 0.6 < φ < 0.4.
Contact: Leonor Cerda Alberich and Carlos Solans
Reference: ATLASPLOTTILECAL2015014
Date: 2nd March 2015

pdf version of the figure

Calorimeter Response characterised by energy over momentum (E/p) for isolated tracks, as measured with the Tile Calorimeter, using protonproton collision data from 2012 in the Minimum Bias stream. Minimum Bias monte carlo is generated using Pythia 6 and simulated using Geant4, with the QGSP_Bertini physics list. Simulation is normalized to data using 8 bins in pseudorapidity and 16 bins in momentum. The energy of the isolated hadron is reconstructed using all nearby clusters in a cone of ΔR < 0.2. Selected tracks pass minimum quality criteria, have pT > 2 GeV and deposit less than 1 GeV in the electromagnetic calorimeter. The plot shows the mean of the E/p ratio for hadronic tracks as a function of μ, integrated over the pseudorapidity and phi coverage of Tile Calorimeter. Black dots represent data and red dots represent simulation. The lower plot shows the ratio of data to simulation in the same μ bins. The largest disagreement is 4% for 6 < μ < 9.
Contact: Leonor Cerda Alberich and Carlos Solans
Reference: ATLASPLOTTILECAL2015014
Date: 2nd March 2015

pdf version of the figure

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