(r20) LArCaloPublicResultsUpgrade < AtlasPublic

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---+!!<nop>Public Liquid-Argon Calorimeter Plots on Upgrade

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---+ Introduction

The LAr Upgrade simulation plots below are approved to be shown by ATLAS speakers at conferences and similar events.  

<b>Please do not add figures on your own.</b> Contact the [[mailto:martin.aleksaNOSPAM@cern.ch][LAr project leader]] in case of questions and/or suggestions.

---+ Phase I Upgrade Plots

The plots from the [[https://cds.cern.ch/record/1602230][LAr Phase I Upgrade TDR]] can be found [[https://atlas.web.cern.ch/Atlas/GROUPS/PHYSICS/UPGRADE/CERN-LHCC-2013-017/index.html][here]].

---++ Demonstrator for the ATLAS LAr calorimeter Phase I Trigger Readout Upgrade

Two LAr Phase I trigger upgrade demonstrator boards (2 Demonstrator LTDBs, LAr Trigger Digitizer Boards) were installed in-situ on the LAr detector in July 2014 (coverage: 9&pi;/16 < &phi; < 11&pi;/16, 0 < &eta; < 1.4). To receive the digital super-cell energies ABBA boards (LDPB pre-prototype) were installed in USA15. One ABBA board receives data from one LTDB 320 super cells. Super-cell data has been recorded for a large number of time slices with this pre-prototype backend electronics.

---+++ Data from 2017 runs and event displays
   * The plots show data from pp collisions, physics run 328099, recorded between June 27 and June 28, 2017.
   * Events were triggered by dedicated triggers requiring either a Level 1 electromagnetic cluster (EM) with E<sub>T</sub> > 20 !GeV or a Level 1 Jet with  E<sub>T</sub> > 100 !GeV within the demonstrator acceptance (for EM(Jet) 1.6 < &phi; < 2.2(2.3), 0 < &eta; < 1.5). Those triggers were prescaled to have a combined event rate of approximately 1 Hz.
   * Events from the LAr demonstrator are matched to events collected in the main read-out using their bunch-crossing ID and brunch-crossing time. An alternative method is the matching according to the L1 ID of the events.

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*Correlation of energy measurements for each layer:* The measured supercell (SC) energies of the LAr Phase I demonstrator are compared to summed LAr cell energies in ATLAS for E<sub>SC</sub> > 1 !GeV. The supercells in the presampler, front, middle and back layer consist of 4, 8, 4 and 8 LAr cells, respectively. Good agreement is observed between the two read-outs.

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%PLOT{scatter_presampler}%<br/>
%PLOT{scatter_front}%<br/>
%PLOT{scatter_middle}%<br/>
%PLOT{scatter_back}%

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*Difference of energy measurements for each layer:*
The measured supercell (SC) energies of the LAr Phase I demonstrator are compared to summed LAr cell energies in ATLAS by calculating the difference (E<sub>SC</sub> &#8722; &Sigma;<sub>SC</sub> E<sub>cells</sub>) for E<sub>SC</sub> > 2 !GeV.
The supercells in the presampler, front, middle and back layer consist of 4, 8, 4 and 8 LAr
cells, respectively.
Good agreement is observed between the two read-outs.
The width of the distribution is compatible with the expected noise level.
The shift of the means is due to the preliminary calibration of the supercells.

</td><td align="center">

%PLOT{difference_presampler}%<br/>
%PLOT{difference_front}%<br/>
%PLOT{difference_middle}%<br/>
%PLOT{difference_back}%

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*Event display of the partial demonstrator region:*
Supercell energies of the LAr Phase I demonstrator and summed LAr cell energies in ATLAS are given for the same shower.
The event with ID 1912797011 was observed in the pp physics run 328099, obtained between June 27 and June 28, 2017.
The geometrical coverage of the demonstrator system is partially shown.
The volume of the depicted boxes is proportional to the deposited energy.
Only energy deposits above 1% of E<sub>max</sub><sup>SC</sup> are plotted.

</td><td align="center">

<table><tr><td align="center">
%HALFPLOT{Event_0_Demonstrator_Partial}%
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%HALFPLOT{Event_0_Main_Partial}%
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*Event display of the demonstrator region:*
Supercell energies of the LAr Phase I demonstrator and summed LAr cell energies in ATLAS are given for the same shower.
The event with ID 2214598379 was observed in the pp physics run 328099, obtained between June 27 and June 28, 2017.
The full geometrical coverage of the demonstrator system is shown.
The volume of the depicted boxes is proportional to the deposited energy.
Only energy deposits above 1% of E<sub>max</sub><sup>SC</sup> are plotted.

</td><td align="center">

<table><tr><td align="center">
%HALFPLOT{Event_0_Demonstrator_Full}%
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%HALFPLOT{Event_0_Main_Full}%
</td></tr></table>

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%HALFPLOT{Event_1_Demonstrator}%
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%HALFPLOT{Event_1_Main}%
</td></tr></table>

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%HALFPLOT{Event_2_Demonstrator}%
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%HALFPLOT{Event_2_Main}%
</td></tr></table>

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%HALFPLOT{Event_3_Demonstrator}%
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%HALFPLOT{Event_3_Main}%
</td></tr></table>

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</table>

---+++ Noise and calibration pulse shapes
Noise values and calibration pulses with several amplitudes are shown in the following. Plots show ADC counts (12 bits ADC) as well as their equivalent transverse energies for the different sections of the calorimeter.


<table class="twikiTable" width="100%" bgcolor=#f5f5fa  border=1 cellpadding=10 cellspacing=10>

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*Super-cell pulse shapes for each layer:*
Responses of four super cells (one from each layer) from the LAr Phase I demonstrator installed in ATLAS to injected calibration pulses (DAC = 1000 counts to each LAr cell), the equivalent energy for DAC = 1000 is shown in subsequent plots.
The super cell  outputs are the sums of 4, 8, 4 and 8 LAr cells for Presampler, Front, Middle and Back layer, respectively. 
Size and shape of pulses are as expected and vary due to different  detector and electronics properties.

</td><td align="center">


[[https://twiki.cern.ch/twiki/pub/AtlasPublic/LArCaloPublicResultsUpgrade/fig1.png][<img width="350" alt="https://twiki.cern.ch/twiki/pub/AtlasPublic/LArCaloPublicResultsUpgrade/fig1.png" src="https://twiki.cern.ch/twiki/pub/AtlasPublic/LArCaloPublicResultsUpgrade/fig1.png"></img>]] 
<br>
[[https://twiki.cern.ch/twiki/pub/AtlasPublic/LArCaloPublicResultsUpgrade/fig1.eps][eps version]], [[https://twiki.cern.ch/twiki/pub/AtlasPublic/LArCaloPublicResultsUpgrade/fig1.pdf][pdf version]] 

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*Pulse maximum in ADC counts for each layer:*
Rapidity dependence of the  pulse maximum in ADC counts (pedestal subtracted) for  the super cells from the LAr Phase I demonstrator in ATLAS for injected calibration pulses (DAC = 1000 counts to each LAr cell), the equivalent energy for DAC = 1000 is shown in subsequent plots.
The super cell  outputs are the sums of 4, 8, 4 and 8 LAr cells for Presampler, Front, Middle and Back layer, respectively. 
The variations in response, especially in the back layer and at &eta; = 0.8, are  due to  the change in electrode segmentation, calibration and readout electronics.


</td><td align="center">


[[https://twiki.cern.ch/twiki/pub/AtlasPublic/LArCaloPublicResultsUpgrade/fig2.png][<img width="350" alt="https://twiki.cern.ch/twiki/pub/AtlasPublic/LArCaloPublicResultsUpgrade/fig2.png" src="https://twiki.cern.ch/twiki/pub/AtlasPublic/LArCaloPublicResultsUpgrade/fig2.png"></img>]] 
<br>
[[https://twiki.cern.ch/twiki/pub/AtlasPublic/LArCaloPublicResultsUpgrade/fig2.eps][eps version]], [[https://twiki.cern.ch/twiki/pub/AtlasPublic/LArCaloPublicResultsUpgrade/fig2.pdf][pdf version]] 

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*Equivalent transverse energy for each layer:*
Rapidity dependence of the equivalent transverse energy for an injected calibration pulse of DAC = 1000 counts into each LAr cell.
The super cell outputs are the sums of 4, 8, 4 and 8 LAr cells for Presampler, Front, Middle and Back layer, respectively. The jump seen at &eta; = 0.8 reflects the change of absorber thickness, electrodes and calibration resistors.

</td><td align="center">


[[https://twiki.cern.ch/twiki/pub/AtlasPublic/LArCaloPublicResultsUpgrade/fig3.png][<img width="350" alt="https://twiki.cern.ch/twiki/pub/AtlasPublic/LArCaloPublicResultsUpgrade/fig3.png" src="https://twiki.cern.ch/twiki/pub/AtlasPublic/LArCaloPublicResultsUpgrade/fig3.png"></img>]] 
<br>
[[https://twiki.cern.ch/twiki/pub/AtlasPublic/LArCaloPublicResultsUpgrade/fig3.eps][eps version]], [[https://twiki.cern.ch/twiki/pub/AtlasPublic/LArCaloPublicResultsUpgrade/fig3.pdf][pdf version]] 

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*Noise level of super cells in ADC counts:*
Rapidity dependence of the noise (RMS) in ADC counts for  the super cells from the LAr Phase I demonstrator in ATLAS.
The super cell  outputs are the sums of 4, 8, 4 and 8 LAr cells for Presampler, Front, Middle and Back layer, respectively. 
The jump seen at &eta; = 0.8 reflects the change of electrodes’ segmentation at that position.  The noise level is well below 1 ADC count and consistent with test bench measurements. 


</td><td align="center">


[[https://twiki.cern.ch/twiki/pub/AtlasPublic/LArCaloPublicResultsUpgrade/fig4.png][<img width="350" alt="https://twiki.cern.ch/twiki/pub/AtlasPublic/LArCaloPublicResultsUpgrade/fig4.png" src="https://twiki.cern.ch/twiki/pub/AtlasPublic/LArCaloPublicResultsUpgrade/fig4.png"></img>]] 
<br>
[[https://twiki.cern.ch/twiki/pub/AtlasPublic/LArCaloPublicResultsUpgrade/fig4.eps][eps version]], [[https://twiki.cern.ch/twiki/pub/AtlasPublic/LArCaloPublicResultsUpgrade/fig4.pdf][pdf version]] 

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*Noise level of super cells in transverse energy:*
Rapidity dependence of the noise (RMS) in transverse energy for  the super cells from the LAr Phase I demonstrator in ATLAS.
The super cell  outputs are the sums of 4, 8, 4 and 8 LAr cells for Presampler, Front, Middle and Back layer, respectively. 
The jump seen at &eta; = 0.8 reflects the change of absorber thickness, electrodes and calibration resistors.
The noise level is as expected between 100 and 250 MeV per super cell. 
 


</td><td align="center">


[[https://twiki.cern.ch/twiki/pub/AtlasPublic/LArCaloPublicResultsUpgrade/fig5.png][<img width="350" alt="https://twiki.cern.ch/twiki/pub/AtlasPublic/LArCaloPublicResultsUpgrade/fig5.png" src="https://twiki.cern.ch/twiki/pub/AtlasPublic/LArCaloPublicResultsUpgrade/fig5.png"></img>]] 
<br>
[[https://twiki.cern.ch/twiki/pub/AtlasPublic/LArCaloPublicResultsUpgrade/fig5.eps][eps version]], [[https://twiki.cern.ch/twiki/pub/AtlasPublic/LArCaloPublicResultsUpgrade/fig5.pdf][pdf version]] 

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*Pulse shapes of a front layer super cell:*
Pulse shapes of a super cell from the LAr Phase I demonstrator installed in ATLAS for injected calibration pulses with different amplitudes (DAC = 2000, 4000, 6000, 8000, 10000 counts), the equivalent energy for these DAC values is shown in subsequent plots.
The super cell outputs are the sums of 8 LAr front layer cells. 
Size and shape of pulses are as expected and show good linearity up to DAC = 8000, while beyond, analog saturation occurs upstream of the demonstrator board.

 


</td><td align="center">


[[https://twiki.cern.ch/twiki/pub/AtlasPublic/LArCaloPublicResultsUpgrade/fig6.png][<img width="350" alt="https://twiki.cern.ch/twiki/pub/AtlasPublic/LArCaloPublicResultsUpgrade/fig6.png" src="https://twiki.cern.ch/twiki/pub/AtlasPublic/LArCaloPublicResultsUpgrade/fig6.png"></img>]] 
<br>
[[https://twiki.cern.ch/twiki/pub/AtlasPublic/LArCaloPublicResultsUpgrade/fig6.eps][eps version]], [[https://twiki.cern.ch/twiki/pub/AtlasPublic/LArCaloPublicResultsUpgrade/fig6.pdf][pdf version]] 

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*Pulse maximum versus DAC value:*
Pulse maximum (in ADC counts) for four different super cells from the LAr Phase I demonstrator installed in ATLAS for injected calibration pulses with different amplitudes (DAC = 2000, 4000, 6000, 8000, 10000 counts), the equivalent energies for these DAC values are shown in subsequent plots.
The super-cell  outputs are the sums of 8 (4) LAr front (middle) layer cells. 
Good linearity up to DAC = 8000 (DAC = 6000) for the front (middle) layer is observed, while beyond, analog saturation occurs upstream of the demonstrator board.


</td><td align="center">


[[https://twiki.cern.ch/twiki/pub/AtlasPublic/LArCaloPublicResultsUpgrade/fig7.png][<img width="350" alt="https://twiki.cern.ch/twiki/pub/AtlasPublic/LArCaloPublicResultsUpgrade/fig7.png" src="https://twiki.cern.ch/twiki/pub/AtlasPublic/LArCaloPublicResultsUpgrade/fig7.png"></img>]] 
<br>
[[https://twiki.cern.ch/twiki/pub/AtlasPublic/LArCaloPublicResultsUpgrade/fig7.eps][eps version]], [[https://twiki.cern.ch/twiki/pub/AtlasPublic/LArCaloPublicResultsUpgrade/fig7.pdf][pdf version]] 

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*Pulse maximum versus transverse energy:*
Pulse maximum (in ADC counts) for four different super cells from the LAr Phase I demonstrator installed in ATLAS for injected calibration pulses with different amplitudes (DAC = 2000, 4000, 6000, 8000, 10000 counts), plotted in units of equivalent transverse energy.
The super-cell outputs are the sums of 8 (4) LAr front (middle) layer cells. 
Analog saturation upstream of the demonstrator board occurs at different transverse energy values depending on the calorimeter layer and rapidity.



</td><td align="center">


[[https://twiki.cern.ch/twiki/pub/AtlasPublic/LArCaloPublicResultsUpgrade/fig8.png][<img width="350" alt="https://twiki.cern.ch/twiki/pub/AtlasPublic/LArCaloPublicResultsUpgrade/fig8.png" src="https://twiki.cern.ch/twiki/pub/AtlasPublic/LArCaloPublicResultsUpgrade/fig8.png"></img>]] 
<br>
[[https://twiki.cern.ch/twiki/pub/AtlasPublic/LArCaloPublicResultsUpgrade/fig8.eps][eps version]], [[https://twiki.cern.ch/twiki/pub/AtlasPublic/LArCaloPublicResultsUpgrade/fig8.pdf][pdf version]] 

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*Total noise on the trigger readout path of the demonstrator test set-up:*
Here the RMS on the trigger readout path in MeV is shown. It was measured in a setup which is equivalent to a crate in ATLAS, with a half-full Front End Crate (FEC) equipped with Front End Boards (FEBs).
Trigger towers 1-14 correspond to an eta-region of 0 to 1.4. Trigger towers 16-29 are the same in eta, but adjacent in phi. The values represented by the full circles were measured by a spectrum analyzer, the values shown in open circles were measured with Flash ADCs. For the computation a pedestal run with 5000 events and 8 samples was used.
</td><td align="center">


[[https://twiki.cern.ch/twiki/pub/AtlasPublic/LArCaloPublicResultsUpgrade/FADC_noise_poster.png][<img width="350" alt="https://twiki.cern.ch/twiki/pub/AtlasPublic/LArCaloPublicResultsUpgrade/FADC_noise_poster.png" src="https://twiki.cern.ch/twiki/pub/AtlasPublic/LArCaloPublicResultsUpgrade/FADC_noise_poster.png"></img>]] 
<br>
[[https://twiki.cern.ch/twiki/pub/AtlasPublic/LArCaloPublicResultsUpgrade/FADC_noise_poster.eps][eps version]] 

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*Fraction of total noise which is coherent for Phase I demonstrator measured in ATLAS:*
Here the total noise which is coherent is shown as fraction of the total noise per readout channel (Coherent Noise Fraction = CNF) The CNF for feedthroughs (FT) 7-12 on the detector has been computed, of which FT 9 and 10 belong to the demonstrator crate I06, FT 7 and 8 to I05 and FT 11 and 12 to I07.
For the computation a pedestal run with 40000 events and 32 samples was used. The board in the first slot reads out the presampler, the boards in the following seven slots read out the front layer, the next two boards the back layer and the last four boards the middle layer of the calorimeter. The last entry is the CNF of the whole halfcrate. The coherent noise fraction rho was calculated using the formula in this [[https://twiki.cern.ch/twiki/pub/AtlasPublic/LArCaloPublicResultsUpgrade/Poster_plots_approval_new.jpg][link]].
</td><td align="center">


[[https://twiki.cern.ch/twiki/pub/AtlasPublic/LArCaloPublicResultsUpgrade/cnf_poster.png][<img width="350" alt="https://twiki.cern.ch/twiki/pub/AtlasPublic/LArCaloPublicResultsUpgrade/cnf_poster.png" src="https://twiki.cern.ch/twiki/pub/AtlasPublic/LArCaloPublicResultsUpgrade/cnf_poster.png"></img>]] 
<br>
[[https://twiki.cern.ch/twiki/pub/AtlasPublic/LArCaloPublicResultsUpgrade/cnf_poster.eps][eps version]]

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*LAr Trigger Digitizer Board (LTDB) demonstrator noise measured on the demonstrator installed in ATLAS:*
Here, the RMS of the 12-bit ADC of the 320 channels of the LTDB demonstrator measured in USA15 is shown. For the computation a pedestal run with 16384 events was used. One ADC count corresponds to roughly 125 MeV..
</td><td align="center">


[[https://twiki.cern.ch/twiki/pub/AtlasPublic/LArCaloPublicResultsUpgrade/LTDB_noise.png][<img width="350" alt="https://twiki.cern.ch/twiki/pub/AtlasPublic/LArCaloPublicResultsUpgrade/LTDB_noise.png" src="https://twiki.cern.ch/twiki/pub/AtlasPublic/LArCaloPublicResultsUpgrade/LTDB_noise.png"></img>]] 
<br>
[[https://twiki.cern.ch/twiki/pub/AtlasPublic/LArCaloPublicResultsUpgrade/LTDB_noise.eps][eps version]]

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*LAr Trigger Digitizer Board (LTDB) demonstrator pedestal measured on the demonstrator installed in ATLAS:*
Here, the pedestal values of the 12-bit ADC of the 320 channels of the LTDB demonstrator measured in USA15 are shown. For the computation a pedestal run with 16384 events was used.
</td><td align="center">


[[https://twiki.cern.ch/twiki/pub/AtlasPublic/LArCaloPublicResultsUpgrade/LTDB_pedestal.png][<img width="350" alt="https://twiki.cern.ch/twiki/pub/AtlasPublic/LArCaloPublicResultsUpgrade/LTDB_pedestal.png" src="https://twiki.cern.ch/twiki/pub/AtlasPublic/LArCaloPublicResultsUpgrade/LTDB_pedestal.png"></img>]] 
<br>
[[https://twiki.cern.ch/twiki/pub/AtlasPublic/LArCaloPublicResultsUpgrade/LTDB_pedestal.eps][eps version]]

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*Total noise on main readout of calorimeter cells of demonstrator crate I06 (ATLAS):*
In this plot, the RMS of the 128 channels of the Front End Boards (FEBs) of the demonstrator crate installed in ATLAS is shown. The FEBs read out the calorimeter cells. There are 28 such boards in one Front End Crate (FEC). The FEBs read out signals from different layers of the calorimeter. The noise levels of the boards vary because different capacitances and gains are applied to their respective cells. For the computation of the RMS a pedestal run with 3000 events and 32 samples was used. The noise level is not higher compared to the neighboring crates on the detector (e.g. see plots for crate I05).
</td><td align="center">


[[https://twiki.cern.ch/twiki/pub/AtlasPublic/LArCaloPublicResultsUpgrade/totalnoise_demonstrator.png][<img width="350" alt="https://twiki.cern.ch/twiki/pub/AtlasPublic/LArCaloPublicResultsUpgrade/totalnoise_demonstrator.png" src="https://twiki.cern.ch/twiki/pub/AtlasPublic/LArCaloPublicResultsUpgrade/totalnoise_demonstrator.png"></img>]] 
<br>
[[https://twiki.cern.ch/twiki/pub/AtlasPublic/LArCaloPublicResultsUpgrade/totalnoise_demonstrator.eps][eps version]]

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*Total noise on main readout of calorimeter cells of crate I05 (ATLAS):*
In this plot, the RMS of all channels of the FEBs of one of the neighbour
crates (I05) of the demonstrator crate I06 in ATLAS is shown. For the computation of the noise a pedestal run with 3000 events and 32 samples was used.
</td><td align="center">


[[https://twiki.cern.ch/twiki/pub/AtlasPublic/LArCaloPublicResultsUpgrade/total_noise_I05.png][<img width="350" alt="https://twiki.cern.ch/twiki/pub/AtlasPublic/LArCaloPublicResultsUpgrade/total_noise_I05.png" src="https://twiki.cern.ch/twiki/pub/AtlasPublic/LArCaloPublicResultsUpgrade/total_noise_I05.png"></img>]] 
<br>
[[https://twiki.cern.ch/twiki/pub/AtlasPublic/LArCaloPublicResultsUpgrade/total_noise_I05.eps][eps version]]

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</table>



---+ Phase II Upgrade Plots

<table class="twikiTable" width="100%" bgcolor=#f5f5fa  border=1 cellpadding=10 cellspacing=10>

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Estimated quantization noise as function of energy in the front layer of the LAr EM barrel calorimeter, with the two gain system proposed for the Phase-II LAr Calorimeter readout (low gain curve in red, high gain curve in blue).
The quantization noise curves assume the use of a 12-bit successive approximation register (SAR) with a dynamic range enhancer (DRE) to obtain a 14-bit ADC with 12-bit precision.
Gain switching occurs close to the highest energy digitized in the high gain.

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%PLOT{intr_electr_res_fl_prel}%<br/>

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Estimated quantization noise as function of energy in the LAr EM middle layer in the endcap outer wheel, with the two gain system proposed for the Phase-II LAr Calorimeter readout (low gain curve in red, high gain curve in blue).
The quantization noise curves assume the use of a 12-bit successive approximation register (SAR) with a dynamic range enhancer (DRE) to obtain a 14-bit ADC with 12-bit precision.
Gain switching occurs close to the highest energy digitized in the high gain.

</td><td align="center">

%PLOT{intr_electr_res_ml_prel}%<br/>

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Bipolar shapers can have different numbers of integration stages, as well as various peaking times, which both affect the total noise (electronics plus pileup) on the analog pulse of the Phase-II LAr Calorimeter readout.
The figure shows the total noise as a function of the level of pileup, &mu;, for a cell from the EM middle layer at &eta; = 0.5, obtained after optimal filtering, for different number of integration stages in the shaper.
The optimal filtering coefficients (OFC) are computed for each case separately.
No significant differences in the noise level can be seen in the EM case.
These results do not include a detailed simulation of the electronics circuit, which could affect the results.

</td><td align="center">

%PLOT{shaper}%<br/>

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Bipolar shapers can have different numbers of integration stages, as well as various peaking times, which both affect the total noise (electronics plus pileup) on the analog pulse of the Phase-II LAr Calorimeter readout.
The figure shows the total noise as a function of the level of pileup, &mu;, for a HEC cell in the first layer at &eta; = 2.35, obtained after optimal filtering, for different number of integration stages in the shaper.
The optimal filtering coefficients (OFC) are computed for each case separately.
For the HEC, a CR-(RC)<sup>3</sup> shaper improves the noise by 5% over a CR-(RC)<sup>2</sup>.
These results do not include a detailed simulation of the electronics circuit, which could affect the results.

</td><td align="center">

%PLOT{Total_Noise}%<br/>

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</table>


---++ NIEL Simulations for HEC Cold Electronics in Phase II

<table class="twikiTable" width="100%" bgcolor=#f5f5fa  border=1 cellpadding=10 cellspacing=10>
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Si NIEL fluence in ATLAS under HL-LHC conditions after 3000 fb<sup>-1</sup> and with an applied safety factor of 2 to account for simulation uncertainties. The color coded fluences in the ASICs are shown at the r-z locations of the corresponding readout regions of the HEC.
</td><td align="center">


[[https://twiki.cern.ch/twiki/pub/AtlasPublic/LArCaloPublicResultsUpgrade/HL-LHC-NIEL-PSB-Region-FLUKA-RBTF2013-2x3000ifb.jpg][<img width="350" alt="https://twiki.cern.ch/twiki/pub/AtlasPublic/LArCaloPublicResultsUpgrade/HL-LHC-NIEL-PSB-Region-FLUKA-RBTF2013-2x3000ifb.jpg" src="https://twiki.cern.ch/twiki/pub/AtlasPublic/LArCaloPublicResultsUpgrade/HL-LHC-NIEL-PSB-Region-FLUKA-RBTF2013-2x3000ifb.jpg"></img>]] 
<br>
[[https://twiki.cern.ch/twiki/pub/AtlasPublic/LArCaloPublicResultsUpgrade/HL-LHC-NIEL-PSB-Region-FLUKA-RBTF2013-2x3000ifb.eps][eps version]], [[https://twiki.cern.ch/twiki/pub/AtlasPublic/LArCaloPublicResultsUpgrade/HL-LHC-NIEL-PSB-Region-FLUKA-RBTF2013-2x3000ifb.pdf][pdf version]]<br><br>

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<td bgcolor=#eeeeee>
Si NIEL fluence in ATLAS under HL-LHC conditions after 3000 fb<sup>-1</sup> and with an applied safety factor of 2 to account for simulation uncertainties. The color coded fluences in the ASICs are shown at the r-z locations of the corresponding readout regions of the HEC.
</td><td align="center">


[[https://twiki.cern.ch/twiki/pub/AtlasPublic/LArCaloPublicResultsUpgrade/HL-LHC-NIEL-PSB-Region-FLUKA-RBTF2013-2x3000ifb.jpg][<img width="350" alt="https://twiki.cern.ch/twiki/pub/AtlasPublic/LArCaloPublicResultsUpgrade/HL-LHC-NIEL-PSB-Region-FLUKA-RBTF2013-2x3000ifb.jpg" src="https://twiki.cern.ch/twiki/pub/AtlasPublic/LArCaloPublicResultsUpgrade/HL-LHC-NIEL-PSB-Region-FLUKA-RBTF2013-2x3000ifb.jpg"></img>]] 
<br>
[[https://twiki.cern.ch/twiki/pub/AtlasPublic/LArCaloPublicResultsUpgrade/HL-LHC-NIEL-PSB-Region-FLUKA-RBTF2013-2x3000ifb.eps][eps version]], [[https://twiki.cern.ch/twiki/pub/AtlasPublic/LArCaloPublicResultsUpgrade/HL-LHC-NIEL-PSB-Region-FLUKA-RBTF2013-2x3000ifb.pdf][pdf version]]<br><br>

</td>
</tr>
</table>


---++ Simulated Noise

<table class="twikiTable" width="100%" bgcolor=#f5f5fa  border=1 cellpadding=10 cellspacing=10>

</tr><tr>
<td bgcolor=#eeeeee>
*Simulated noise in the Liquid Argon and Tile calorimeters at the electron scale (bunch spacing %$\Delta$%t=25ns):* Quadratic sum of simulated electronics and pile-up noise per calorimeter cell for each calorimeter layer as function of pseudo-rapidity. The pile-up simulation is done by overlaying GEANT4 simulated events from PYTHIA (v6.4) including non diffractive and diffractive events.
The overlay takes into account the full sensitive time of the detector (~500ns for the LAr) and the bunch train structure. For proton-proton
collisions at &#8730;s = 14TeV and a bunch spacing of %$\Delta$%t=25ns. The luminosity and corresponding average overlaying interactions per bunch crossing <µ> (pile-up events) are specified below (and inside) each figure. The standard ATLAS electronics are assumed in the simulation. A comparison of data and MC
for <µ> = 0 and  <µ> = 14 can be seen at the corresponding links for the [[https://twiki.cern.ch/twiki/bin/view/AtlasPublic/LArCaloPublicResultsDetStatus][LAr]] and for the [[https://cds.cern.ch/record/1442284][Tile]] calorimeter.
</td><td align="center">


[[https://twiki.cern.ch/twiki/pub/AtlasPublic/LArCaloPublicResultsUpgrade/noise_tot_plot_OFLCOND-MC12-HPS-19-30-25.png][<img width="350" alt="https://twiki.cern.ch/twiki/pub/AtlasPublic/LArCaloPublicResultsUpgrade/noise_tot_plot_OFLCOND-MC12-HPS-19-30-25.png" src="https://twiki.cern.ch/twiki/pub/AtlasPublic/LArCaloPublicResultsUpgrade/noise_tot_plot_OFLCOND-MC12-HPS-19-30-25.png"></img>]] <br> 
Total noise for L=1.09x10<sup>34</sup> corresponding to <µ>=30 <br>
[[https://twiki.cern.ch/twiki/pub/AtlasPublic/LArCaloPublicResultsUpgrade/noise_tot_plot_OFLCOND-MC12-HPS-19-30-25.eps][eps version]]<br><br>

[[https://twiki.cern.ch/twiki/pub/AtlasPublic/LArCaloPublicResultsUpgrade/noise_tot_plot_OFLCOND-MC12-HPS-19-40-25.png][<img width="350" alt="https://twiki.cern.ch/twiki/pub/AtlasPublic/LArCaloPublicResultsUpgrade/noise_tot_plot_OFLCOND-MC12-HPS-19-40-25.png" src="https://twiki.cern.ch/twiki/pub/AtlasPublic/LArCaloPublicResultsUpgrade/noise_tot_plot_OFLCOND-MC12-HPS-19-40-25.png"></img>]] <br> 
Total noise for L=1.45x10<sup>34</sup> corresponding to <µ>=40 <br>
[[https://twiki.cern.ch/twiki/pub/AtlasPublic/LArCaloPublicResultsUpgrade/noise_tot_plot_OFLCOND-MC12-HPS-19-40-25.eps][eps version]]<br><br>

[[https://twiki.cern.ch/twiki/pub/AtlasPublic/LArCaloPublicResultsUpgrade/noise_tot_plot_OFLCOND-MC12-HPS-19-60-25.png][<img width="350" alt="https://twiki.cern.ch/twiki/pub/AtlasPublic/LArCaloPublicResultsUpgrade/noise_tot_plot_OFLCOND-MC12-HPS-19-60-25.png" src="https://twiki.cern.ch/twiki/pub/AtlasPublic/LArCaloPublicResultsUpgrade/noise_tot_plot_OFLCOND-MC12-HPS-19-60-25.png"></img>]] <br> 
Total noise for L=2.17x10<sup>34</sup> corresponding to <µ>=60 <br>
[[https://twiki.cern.ch/twiki/pub/AtlasPublic/LArCaloPublicResultsUpgrade/noise_tot_plot_OFLCOND-MC12-HPS-19-60-25.eps][eps version]]<br><br>

[[https://twiki.cern.ch/twiki/pub/AtlasPublic/LArCaloPublicResultsUpgrade/noise_tot_plot_OFLCOND-MC12-HPS-19-80-25.png][<img width="350" alt="https://twiki.cern.ch/twiki/pub/AtlasPublic/LArCaloPublicResultsUpgrade/noise_tot_plot_OFLCOND-MC12-HPS-19-80-25.png" src="https://twiki.cern.ch/twiki/pub/AtlasPublic/LArCaloPublicResultsUpgrade/noise_tot_plot_OFLCOND-MC12-HPS-19-80-25.png"></img>]] <br> 
Total noise for L=2.90x10<sup>34</sup> corresponding to <µ>=80 <br>
[[https://twiki.cern.ch/twiki/pub/AtlasPublic/LArCaloPublicResultsUpgrade/noise_tot_plot_OFLCOND-MC12-HPS-19-80-25.eps][eps version]]<br><br>

[[https://twiki.cern.ch/twiki/pub/AtlasPublic/LArCaloPublicResultsUpgrade/noise_tot_plot_OFLCOND-MC12-HPS-19-100-25.png][<img width="350" alt="https://twiki.cern.ch/twiki/pub/AtlasPublic/LArCaloPublicResultsUpgrade/noise_tot_plot_OFLCOND-MC12-HPS-19-100-25.png" src="https://twiki.cern.ch/twiki/pub/AtlasPublic/LArCaloPublicResultsUpgrade/noise_tot_plot_OFLCOND-MC12-HPS-19-100-25.png"></img>]] <br> 
Total noise for L=3.62x10<sup>34</sup> corresponding to <µ>=100 <br>
[[https://twiki.cern.ch/twiki/pub/AtlasPublic/LArCaloPublicResultsUpgrade/noise_tot_plot_OFLCOND-MC12-HPS-19-100-25.eps][eps version]]<br><br>

[[https://twiki.cern.ch/twiki/pub/AtlasPublic/LArCaloPublicResultsUpgrade/noise_tot_plot_OFLCOND-MC12-HPS-19-140-25.png][<img width="350" alt="https://twiki.cern.ch/twiki/pub/AtlasPublic/LArCaloPublicResultsUpgrade/noise_tot_plot_OFLCOND-MC12-HPS-19-140-25.png" src="https://twiki.cern.ch/twiki/pub/AtlasPublic/LArCaloPublicResultsUpgrade/noise_tot_plot_OFLCOND-MC12-HPS-19-140-25.png"></img>]] <br> 
Total noise for L=5.07x10<sup>34</sup> corresponding to <µ>=140 <br>
[[https://twiki.cern.ch/twiki/pub/AtlasPublic/LArCaloPublicResultsUpgrade/noise_tot_plot_OFLCOND-MC12-HPS-19-140-25.eps][eps version]]<br><br>

[[https://twiki.cern.ch/twiki/pub/AtlasPublic/LArCaloPublicResultsUpgrade/noise_tot_plot_OFLCOND-MC12-HPS-19-200-25.png][<img width="350" alt="https://twiki.cern.ch/twiki/pub/AtlasPublic/LArCaloPublicResultsUpgrade/noise_tot_plot_OFLCOND-MC12-HPS-19-200-25.png" src="https://twiki.cern.ch/twiki/pub/AtlasPublic/LArCaloPublicResultsUpgrade/noise_tot_plot_OFLCOND-MC12-HPS-19-200-25.png"></img>]] <br> 
Total noise for L=7.25x10<sup>34</sup> corresponding to <µ>=200 <br>
[[https://twiki.cern.ch/twiki/pub/AtlasPublic/LArCaloPublicResultsUpgrade/noise_tot_plot_OFLCOND-MC12-HPS-19-200-25.eps][eps version]]<br><br>

</td>
</tr><tr>
</table>

<table class="twikiTable" width="100%" bgcolor=#f5f5fa  border=1 cellpadding=10 cellspacing=10>

</tr><tr>
<td bgcolor=#eeeeee>
*Simulated noise in the Liquid Argon and Tile calorimeters at the electron scale (bunch spacing %$\Delta$%t=50ns):* Quadratic sum of simulated electronics and pile-up noise per calorimeter cell for each calorimeter layer as function of pseudo-rapidity. The pile-up simulation is done by overlaying GEANT4 simulated events from PYTHIA (v6.4) including non diffractive and diffractive events.
The overlay takes into account the full sensitive time of the detector (~500ns for the LAr) and the bunch train structure. For proton-proton
collisions at &#8730;s = 14TeV and a bunch spacing of %$\Delta$%t=50ns. The luminosity and corresponding average overlaying interactions per bunch crossing <µ> (pile-up events) are specified below (and inside) each figure. The standard ATLAS electronics are assumed in the simulation. A comparison of data and MC
for <µ> = 0 and  <µ> = 14 can be seen at the corresponding links for the [[https://twiki.cern.ch/twiki/bin/view/AtlasPublic/LArCaloPublicResultsDetStatus][LAr]] and for the [[https://cds.cern.ch/record/1442284][Tile]] calorimeter.
</td><td align="center">


[[https://twiki.cern.ch/twiki/pub/AtlasPublic/LArCaloPublicResultsUpgrade/noise_tot_plot_OFLCOND-MC12-HPS-19-30-50.png][<img width="350" alt="https://twiki.cern.ch/twiki/pub/AtlasPublic/LArCaloPublicResultsUpgrade/noise_tot_plot_OFLCOND-MC12-HPS-19-30-50.png" src="https://twiki.cern.ch/twiki/pub/AtlasPublic/LArCaloPublicResultsUpgrade/noise_tot_plot_OFLCOND-MC12-HPS-19-30-50.png"></img>]] <br> 
Total noise for L=0.54x10<sup>34</sup> corresponding to <µ>=30 <br>
[[https://twiki.cern.ch/twiki/pub/AtlasPublic/LArCaloPublicResultsUpgrade/noise_tot_plot_OFLCOND-MC12-HPS-19-30-50.eps][eps version]]<br><br>

[[https://twiki.cern.ch/twiki/pub/AtlasPublic/LArCaloPublicResultsUpgrade/noise_tot_plot_OFLCOND-MC12-HPS-19-40-50.png][<img width="350" alt="https://twiki.cern.ch/twiki/pub/AtlasPublic/LArCaloPublicResultsUpgrade/noise_tot_plot_OFLCOND-MC12-HPS-19-40-50.png" src="https://twiki.cern.ch/twiki/pub/AtlasPublic/LArCaloPublicResultsUpgrade/noise_tot_plot_OFLCOND-MC12-HPS-19-40-50.png"></img>]] <br> 
Total noise for L=0.73x10<sup>34</sup> corresponding to <µ>=40 <br>
[[https://twiki.cern.ch/twiki/pub/AtlasPublic/LArCaloPublicResultsUpgrade/noise_tot_plot_OFLCOND-MC12-HPS-19-40-50.eps][eps version]]<br><br>

[[https://twiki.cern.ch/twiki/pub/AtlasPublic/LArCaloPublicResultsUpgrade/noise_tot_plot_OFLCOND-MC12-HPS-19-60-50.png][<img width="350" alt="https://twiki.cern.ch/twiki/pub/AtlasPublic/LArCaloPublicResultsUpgrade/noise_tot_plot_OFLCOND-MC12-HPS-19-60-50.png" src="https://twiki.cern.ch/twiki/pub/AtlasPublic/LArCaloPublicResultsUpgrade/noise_tot_plot_OFLCOND-MC12-HPS-19-60-50.png"></img>]] <br> 
Total noise for L=1.09x10<sup>34</sup> corresponding to <µ>=60 <br>
[[https://twiki.cern.ch/twiki/pub/AtlasPublic/LArCaloPublicResultsUpgrade/noise_tot_plot_OFLCOND-MC12-HPS-19-60-50.eps][eps version]]<br><br>

[[https://twiki.cern.ch/twiki/pub/AtlasPublic/LArCaloPublicResultsUpgrade/noise_tot_plot_OFLCOND-MC12-HPS-19-80-50.png][<img width="350" alt="https://twiki.cern.ch/twiki/pub/AtlasPublic/LArCaloPublicResultsUpgrade/noise_tot_plot_OFLCOND-MC12-HPS-19-80-50.png" src="https://twiki.cern.ch/twiki/pub/AtlasPublic/LArCaloPublicResultsUpgrade/noise_tot_plot_OFLCOND-MC12-HPS-19-80-50.png"></img>]] <br> 
Total noise for L=1.45x10<sup>34</sup> corresponding to <µ>=80 <br>
[[https://twiki.cern.ch/twiki/pub/AtlasPublic/LArCaloPublicResultsUpgrade/noise_tot_plot_OFLCOND-MC12-HPS-19-80-50.eps][eps version]]<br><br>

[[https://twiki.cern.ch/twiki/pub/AtlasPublic/LArCaloPublicResultsUpgrade/noise_tot_plot_OFLCOND-MC12-HPS-19-100-50.png][<img width="350" alt="https://twiki.cern.ch/twiki/pub/AtlasPublic/LArCaloPublicResultsUpgrade/noise_tot_plot_OFLCOND-MC12-HPS-19-100-50.png" src="https://twiki.cern.ch/twiki/pub/AtlasPublic/LArCaloPublicResultsUpgrade/noise_tot_plot_OFLCOND-MC12-HPS-19-100-50.png"></img>]] <br> 
Total noise for L=1.81x10<sup>34</sup> corresponding to <µ>=100 <br>
[[https://twiki.cern.ch/twiki/pub/AtlasPublic/LArCaloPublicResultsUpgrade/noise_tot_plot_OFLCOND-MC12-HPS-19-100-50.eps][eps version]]<br><br>

[[https://twiki.cern.ch/twiki/pub/AtlasPublic/LArCaloPublicResultsUpgrade/noise_tot_plot_OFLCOND-MC12-HPS-19-140-50.png][<img width="350" alt="https://twiki.cern.ch/twiki/pub/AtlasPublic/LArCaloPublicResultsUpgrade/noise_tot_plot_OFLCOND-MC12-HPS-19-140-50.png" src="https://twiki.cern.ch/twiki/pub/AtlasPublic/LArCaloPublicResultsUpgrade/noise_tot_plot_OFLCOND-MC12-HPS-19-140-50.png"></img>]] <br> 
Total noise for L=2.54x10<sup>34</sup> corresponding to <µ>=140 <br>
[[https://twiki.cern.ch/twiki/pub/AtlasPublic/LArCaloPublicResultsUpgrade/noise_tot_plot_OFLCOND-MC12-HPS-19-140-50.eps][eps version]]<br><br>

[[https://twiki.cern.ch/twiki/pub/AtlasPublic/LArCaloPublicResultsUpgrade/noise_tot_plot_OFLCOND-MC12-HPS-19-200-50.png][<img width="350" alt="https://twiki.cern.ch/twiki/pub/AtlasPublic/LArCaloPublicResultsUpgrade/noise_tot_plot_OFLCOND-MC12-HPS-19-200-50.png" src="https://twiki.cern.ch/twiki/pub/AtlasPublic/LArCaloPublicResultsUpgrade/noise_tot_plot_OFLCOND-MC12-HPS-19-200-50.png"></img>]] <br> 
Total noise for L=3.62x10<sup>34</sup> corresponding to <µ>=200 <br>
[[https://twiki.cern.ch/twiki/pub/AtlasPublic/LArCaloPublicResultsUpgrade/noise_tot_plot_OFLCOND-MC12-HPS-19-200-50.eps][eps version]]<br><br>

</td>
</tr><tr>


</table>

---++ High Granularity FCal Performance Studies

The below results are based on simulated VBF 2.6 !TeV Higgs boson production and di-jet production at 14 !TeV with &#956;=190-200 assuming the current ATLAS FCal, a high-granularity sFCal and the FCal with reduced acceptance

<table class="twikiTable" width="100%" bgcolor=#f5f5fa  border=1 cellpadding=10 cellspacing=10>
</tr><tr>
<td bgcolor=#eeeeee>
<b>Total Noise Ratio:</b> Noise ratio per calorimeter cell as a function of |&#951;| for all layers for a high- granularity sFCal over FCal at a centre-of-mass energy of 14 !TeV and for a mean number of pile-up event of &#956;=200. Small deviations from 1 in the inner-most (s)FCal1 and full (s)FCal2/3 layers are due to the 6% denser sFCal1 compared to FCal1 which causes inelastic pp collisions to deposit more energy in the first module. In the outer region of sFCal1 the noise is 0.4 times the FCal1 noise. The ratio 1.1/0.4 = 2.75 of ratios for inner over outer cells is non-trivial and indicates that an sFCal with finer granularity improves the separation of hard-scatter signal from pile-up. The granularity ratio is 4. Therefore a double ratio of 4 would mean no improvement at all since all small cells would be fully correlated. A double ratio of 2 would be the maximal possible improvement in case all small cells are uncorrelated. 2.75 lies between these extremes, and since it is smaller than 4 means that the increase in granularity helps to suppress pile-up.
</td><td align="center">


[[https://twiki.cern.ch/twiki/pub/AtlasPublic/LArCaloPublicResultsUpgrade/noise_tot_ratio_sFCal_SmallGaps_over_FCal_mu200-new_prelim.png][<img width="350" alt="https://twiki.cern.ch/twiki/pub/AtlasPublic/LArCaloPublicResultsUpgrade/noise_tot_ratio_sFCal_SmallGaps_over_FCal_mu200-new_prelim.png" src="https://twiki.cern.ch/twiki/pub/AtlasPublic/LArCaloPublicResultsUpgrade/noise_tot_ratio_sFCal_SmallGaps_over_FCal_mu200-new_prelim.png"></img>]] 
<br>
[[https://twiki.cern.ch/twiki/pub/AtlasPublic/LArCaloPublicResultsUpgrade/noise_tot_ratio_sFCal_SmallGaps_over_FCal_mu200-new_prelim.eps][eps version]], [[https://twiki.cern.ch/twiki/pub/AtlasPublic/LArCaloPublicResultsUpgrade/noise_tot_ratio_sFCal_SmallGaps_over_FCal_mu200-new_prelim.pdf][pdf version]]<br><br>

</td>
</tr><tr>

<td bgcolor=#eeeeee>
<b>Number of Jet Constituents:</b> Distribution of the number of constituents (clusters) for quark jets produced in the vector-boson fusion process &#119901;&#119901; &#8594; &#119867; &#119902;&#119902; &#8594; &#119897;<sup>&#8722;</sup>&#119907; &#119897;<sup>+</sup>&#119907; &#119902;&#119902; at 14 !TeV centre-of-mass energy simulated for the current ATLAS FCal, a high-granularity sFCal, and three scenarios with reduced FCal acceptance. The increase in granularity and better separation of signal from pile-up leads to larger number of constituents in the sFCal compared to FCal.
The vector-boson fusion events were simulated with the Powheg and Pythia8 Monte Carlo generators in narrow-width approximation for a hypothetic Higgs boson mass of 2.6 !TeV and an average number of pile-up events, &#956;, between 190 and 210.
</td><td align="center">


[[https://twiki.cern.ch/twiki/pub/AtlasPublic/LArCaloPublicResultsUpgrade/sFCalReview_NConst_VBF2600_prelim.png][<img width="350" alt="https://twiki.cern.ch/twiki/pub/AtlasPublic/LArCaloPublicResultsUpgrade/sFCalReview_NConst_VBF2600_prelim.png" src="https://twiki.cern.ch/twiki/pub/AtlasPublic/LArCaloPublicResultsUpgrade/sFCalReview_NConst_VBF2600_prelim.png"></img>]] 
<br>
[[https://twiki.cern.ch/twiki/pub/AtlasPublic/LArCaloPublicResultsUpgrade/sFCalReview_NConst_VBF2600_prelim.eps][eps version]], [[https://twiki.cern.ch/twiki/pub/AtlasPublic/LArCaloPublicResultsUpgrade/sFCalReview_NConst_VBF2600_prelim.pdf][pdf version]]<br><br>

</td>
</tr><tr>

<td bgcolor=#eeeeee>
<b>Cell Significance:</b> Cell significance (E<sub>cell</sub>/&#963;<sub>cell</sub>) for the cell with the largest absolute cell energy over total noise simulated for the current ATLAS FCal, a high-granularity sFCal, and three scenarios with reduced FCal acceptance. Clusters are seeded when the absolute ratio is above 4. Cluster splitting can lead to entries with smaller ratios. The sFCal distribution is enhanced on the positve side while it remains close to the FCal distribution on the negative side. The negative entries are due to pile-up only, while on the positve side signal and pile- up contribute. The increase of mainly the positive side indicates that the signal detection ability is improved for the sFCal while the background remains on the same level.
The distributions are obtained for vector-boson fusion events &#119901;&#119901; &#8594; &#119867; &#119902;&#119902; &#8594; &#119897;<sup>&#8722;</sup>&#119907; &#119897;<sup>+</sup>&#119907; &#119902;&#119902; at 14 !TeV centre-of-mass energy, simulated with the Powheg and Pythia8 Monte Carlo generators in narrow-width approximation for a hypothetic Higgs boson mass of 2.6 !TeV and an average number of pile-up events, &#956;, between 190 and 210.
</td><td align="center">


[[https://twiki.cern.ch/twiki/pub/AtlasPublic/LArCaloPublicResultsUpgrade/sFCalReview_CellSig_VBF2600_prelim.png][<img width="350" alt="https://twiki.cern.ch/twiki/pub/AtlasPublic/LArCaloPublicResultsUpgrade/sFCalReview_CellSig_VBF2600_prelim.png" src="https://twiki.cern.ch/twiki/pub/AtlasPublic/LArCaloPublicResultsUpgrade/sFCalReview_CellSig_VBF2600_prelim.png"></img>]] 
<br>
[[https://twiki.cern.ch/twiki/pub/AtlasPublic/LArCaloPublicResultsUpgrade/sFCalReview_CellSig_VBF2600_prelim.eps][eps version]], [[https://twiki.cern.ch/twiki/pub/AtlasPublic/LArCaloPublicResultsUpgrade/sFCalReview_CellSig_VBF2600_prelim.pdf][pdf version]]<br><br>

</td>
</tr><tr>

<td bgcolor=#eeeeee>
<b>Average p<sub>T</sub> Density:</b> Shown is the simulated profile of the average median p<sub>T</sub> density, &#961;, evaluated from positive-energy cell towers in the ATLAS LAr calorimeters. For the forward calorimeter, five different scenarios are studied: the current ATLAS FCal, a high-granularity sFCal, and three scenarios with reduced FCal acceptance. When a &#961;-based pile-up suppression will be applied in the jet reconstruction it is expected that a larger amount of p<sub>T</sub> will be removed for jets in the forward region in case of the sFCal.
The distributions are obtained for vector-boson fusion events &#119901;&#119901; &#8594; &#119867; &#119902;&#119902; &#8594; &#119897;<sup>&#8722;</sup>&#119907; &#119897;<sup>+</sup>&#119907; &#119902;&#119902; at 14 !TeV centre-of-mass energy, simulated with the Powheg and Pythia8 Monte Carlo generators in narrow-width approximation for a hypothetic Higgs boson mass of 2.6 !TeV and an average number of pile-up events, &#956;, between 190 and 210.
</td><td align="center">


[[https://twiki.cern.ch/twiki/pub/AtlasPublic/LArCaloPublicResultsUpgrade/MedianDensityProfile_vs_eta.png][<img width="350" alt="https://twiki.cern.ch/twiki/pub/AtlasPublic/LArCaloPublicResultsUpgrade/MedianDensityProfile_vs_eta.png" src="https://twiki.cern.ch/twiki/pub/AtlasPublic/LArCaloPublicResultsUpgrade/MedianDensityProfile_vs_eta.png"></img>]] 
<br>
[[https://twiki.cern.ch/twiki/pub/AtlasPublic/LArCaloPublicResultsUpgrade/MedianDensityProfile_vs_eta.eps][eps version]], [[https://twiki.cern.ch/twiki/pub/AtlasPublic/LArCaloPublicResultsUpgrade/MedianDensityProfile_vs_eta.pdf][pdf version]]<br><br>

</td>
</tr><tr>

<td bgcolor=#eeeeee>
<b>Number of Jets:</b> Simulated integral jet p<sub>T</sub> distribution for hard scattering and pile-up jets and the relative fraction of hard scattering jets detected in the ATLAS FCal and in a high-granularity sFCal. An area-based p<sub>T</sub> subtraction is applied. The amount of p<sub>T</sub> subtracted from a jet is increased by a factor of 10 (thereby effectively killing the jet) in the case that it fails one of the jet shape variable cuts, which are based on jet width, transverse momentum sum of the jet constituents relative to the jet direction and the electromagnetic energy fraction.
The distributions are obtained for vector-boson fusion events &#119901;&#119901; &#8594; &#119867; &#119902;&#119902; &#8594; &#119897;<sup>&#8722;</sup>&#119907; &#119897;<sup>+</sup>&#119907; &#119902;&#119902; at 14 !TeV centre-of-mass energy, simulated with the Powheg and Pythia8 Monte Carlo generators in narrow-width approximation for a hypothetic Higgs boson mass of 2.6 !TeV and an average number of pile-up events, &#956;, between 190 and 210.
</td><td align="center">


[[https://twiki.cern.ch/twiki/pub/AtlasPublic/LArCaloPublicResultsUpgrade/PUSuppression_NJetsAndHSFraction_vs_PtCut.png][<img width="350" alt="https://twiki.cern.ch/twiki/pub/AtlasPublic/LArCaloPublicResultsUpgrade/PUSuppression_NJetsAndHSFraction_vs_PtCut.png" src="https://twiki.cern.ch/twiki/pub/AtlasPublic/LArCaloPublicResultsUpgrade/PUSuppression_NJetsAndHSFraction_vs_PtCut.png"></img>]] 
<br>
[[https://twiki.cern.ch/twiki/pub/AtlasPublic/LArCaloPublicResultsUpgrade/PUSuppression_NJetsAndHSFraction_vs_PtCut.eps][eps version]], [[https://twiki.cern.ch/twiki/pub/AtlasPublic/LArCaloPublicResultsUpgrade/PUSuppression_NJetsAndHSFraction_vs_PtCut.pdf][pdf version]]<br><br>

</td>
</tr><tr>

<td bgcolor=#eeeeee>
<b>Ratio of Pile-Up Jets:</b> Ratio of number of identified pile-up jets and total number of reconstructed jets as a function of efficiency for determining a hard-scattering jet as simulated in di-jet events at 14 !TeV for the ATLAS FCal and a high-granularity sFCal. All jets are selected in the pseudo-rapidity range 3.8<|&#951;|<4.2 and in the p<sub>T</sub> range between 50 !GeV and 70 !GeV. Also shown is the double- ratio comparing the sFCal and FCal performance. The jet classification was performed using a likelihood ratio constructed from the jet width, the jet mass, the transverse momentum sum of the jet constituents relative to the jet direction, and the number of jet constituents (clusters).
</td><td align="center">


[[https://twiki.cern.ch/twiki/pub/AtlasPublic/LArCaloPublicResultsUpgrade/ROC-eff-eta38to42.png][<img width="350" alt="https://twiki.cern.ch/twiki/pub/AtlasPublic/LArCaloPublicResultsUpgrade/ROC-eff-eta38to42.png" src="https://twiki.cern.ch/twiki/pub/AtlasPublic/LArCaloPublicResultsUpgrade/ROC-eff-eta38to42.png"></img>]] 
<br>
[[https://twiki.cern.ch/twiki/pub/AtlasPublic/LArCaloPublicResultsUpgrade/ROC-eff-eta38to42.eps][eps version]], [[https://twiki.cern.ch/twiki/pub/AtlasPublic/LArCaloPublicResultsUpgrade/ROC-eff-eta38to42.pdf][pdf version]]<br><br>

</td>
</tr><tr>

<td bgcolor=#eeeeee>
<b>Number of Pile-Up Jets:</b> Number of identified pile-up jets per event as a function of efficiency for determining a hard-scattering jet in high-mass VBF Higgs events at 14 !TeV for the ATLAS FCal and a high- granularity sFCal. All jets are selected in the pseudo-rapidity range 3.2<|&#951;|<3.8 and in the p<sub>T</sub> range above 20 !GeV. The jet reconstruction requires a positive cluster-vertex-fraction and a pile- up correction based on the average median p<sub>T</sub> density, &#961;, evaluated from positive-energy cell towers in the ATLAS LAr calorimeters. The simulation of charged particle tracks is based on the ITk tracking system assuming a tracking coverage of |&#951;|<4 and an ideal ITk detector resolution. 
The distributions are obtained for vector-boson fusion events &#119901;&#119901; &#8594; &#119867; &#119902;&#119902; &#8594; &#119897;<sup>&#8722;</sup>&#119907; &#119897;<sup>+</sup>&#119907; &#119902;&#119902; at 14 !TeV centre-of-mass energy, simulated with the Powheg and Pythia8 Monte Carlo generators in narrow-width approximation for a hypothetic Higgs boson mass of 2.6 !TeV and an average number of pile-up events, &#956;, between 190 and 210.
</td><td align="center">


[[https://twiki.cern.ch/twiki/pub/AtlasPublic/LArCaloPublicResultsUpgrade/ROC_effHS_pt20_extr_JES_preliminary.png][<img width="350" alt="https://twiki.cern.ch/twiki/pub/AtlasPublic/LArCaloPublicResultsUpgrade/ROC_effHS_pt20_extr_JES_preliminary.png" src="https://twiki.cern.ch/twiki/pub/AtlasPublic/LArCaloPublicResultsUpgrade/ROC_effHS_pt20_extr_JES_preliminary.png"></img>]] 
<br>
[[https://twiki.cern.ch/twiki/pub/AtlasPublic/LArCaloPublicResultsUpgrade/ROC_effHS_pt20_extr_JES_preliminary.eps][eps version]], [[https://twiki.cern.ch/twiki/pub/AtlasPublic/LArCaloPublicResultsUpgrade/ROC_effHS_pt20_extr_JES_preliminary.pdf][pdf version]]<br><br>

</td>
</tr><tr>

</table>




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Attachments

Topic attachments
I	Attachment	History	Action	Size	Date	Who	Comment
eps	shaper.eps	r1	manage	13.8 K	2017-09-12 - 15:29	SteffenStaerz	Total Noise, bipolar shaper
pdf	shaper.pdf	r1	manage	14.4 K	2017-09-12 - 15:29	SteffenStaerz	Total Noise, bipolar shaper
png	shaper.png	r1	manage	14.5 K	2017-09-12 - 15:29	SteffenStaerz	Total Noise, bipolar shaper
eps	Total_Noise.eps	r1	manage	10.7 K	2017-09-12 - 19:35	SteffenStaerz	Total Noise (HEC)
pdf	Total_Noise.pdf	r1	manage	14.2 K	2017-09-12 - 19:35	SteffenStaerz	Total Noise (HEC)
png	Total_Noise.png	r1	manage	114.4 K	2017-09-12 - 19:35	SteffenStaerz	Total Noise (HEC)
eps	intr_electr_res_fl_prel.eps	r1	manage	20.2 K	2017-09-14 - 14:31	SteffenStaerz	Quantization noise
pdf	intr_electr_res_fl_prel.pdf	r1	manage	25.1 K	2017-09-14 - 14:31	SteffenStaerz	Quantization noise
png	intr_electr_res_fl_prel.png	r1	manage	43.5 K	2017-09-14 - 14:31	SteffenStaerz	Quantization noise
eps	intr_electr_res_ml_prel.eps	r1	manage	20.4 K	2017-09-14 - 14:31	SteffenStaerz	Quantization noise
pdf	intr_electr_res_ml_prel.pdf	r1	manage	25.0 K	2017-09-14 - 14:31	SteffenStaerz	Quantization noise
png	intr_electr_res_ml_prel.png	r1	manage	45.2 K	2017-09-14 - 14:31	SteffenStaerz	Quantization noise
eps	FADC_noise_poster.eps	r1	manage	17.1 K	2015-02-23 - 17:28	MartinAleksa	Phase I Upgrade Demonstrator Plots (eps)
eps	LTDB_noise.eps	r1	manage	136.9 K	2015-02-23 - 17:28	MartinAleksa	Phase I Upgrade Demonstrator Plots (eps)
eps	LTDB_pedestal.eps	r1	manage	153.2 K	2015-02-23 - 17:28	MartinAleksa	Phase I Upgrade Demonstrator Plots (eps)
eps	cnf_poster.eps	r1	manage	8.8 K	2015-02-23 - 17:28	MartinAleksa	Phase I Upgrade Demonstrator Plots (eps)
eps	total_noise_I05.eps	r2 r1	manage	142.9 K	2015-02-23 - 23:27	MartinAleksa	Phase I Upgrade Demonstrator Plots (eps)
eps	totalnoise_demonstrator.eps	r2 r1	manage	142.9 K	2015-02-23 - 23:28	MartinAleksa	Phase I Upgrade Demonstrator Plots (eps)
png	FADC_noise_poster.png	r1	manage	14.0 K	2015-02-23 - 17:08	MartinAleksa	Phase I Upgrade Demonstrator Plots
png	LTDB_noise.png	r1	manage	14.2 K	2015-02-23 - 17:08	MartinAleksa	Phase I Upgrade Demonstrator Plots
png	LTDB_pedestal.png	r1	manage	15.9 K	2015-02-23 - 17:08	MartinAleksa	Phase I Upgrade Demonstrator Plots
png	cnf_poster.png	r1	manage	12.4 K	2015-02-23 - 17:08	MartinAleksa	Phase I Upgrade Demonstrator Plots
png	total_noise_I05.png	r2 r1	manage	29.2 K	2015-02-23 - 23:28	MartinAleksa	Phase I Upgrade Demonstrator Plots
png	totalnoise_demonstrator.png	r2 r1	manage	28.5 K	2015-02-23 - 23:29	MartinAleksa	Phase I Upgrade Demonstrator Plots
eps	HL-LHC-NIEL-PSB-Region-FLUKA-RBTF2013-2x3000ifb.eps	r1	manage	20.2 K	2014-03-18 - 17:34	MartinAleksa	NIEL Simulations for HEC Cold Electronics in Phase II
jpg	HL-LHC-NIEL-PSB-Region-FLUKA-RBTF2013-2x3000ifb.jpg	r1	manage	237.6 K	2014-03-18 - 17:34	MartinAleksa	NIEL Simulations for HEC Cold Electronics in Phase II
pdf	HL-LHC-NIEL-PSB-Region-FLUKA-RBTF2013-2x3000ifb.pdf	r1	manage	11.0 K	2014-03-18 - 17:34	MartinAleksa	NIEL Simulations for HEC Cold Electronics in Phase II
eps	MedianDensityProfile_vs_eta.eps	r1	manage	41.3 K	2016-10-18 - 14:44	MartinAleksa
pdf	MedianDensityProfile_vs_eta.pdf	r1	manage	35.0 K	2016-10-18 - 14:44	MartinAleksa
png	MedianDensityProfile_vs_eta.png	r1	manage	28.0 K	2016-10-18 - 14:44	MartinAleksa
eps	PUSuppression_NJetsAndHSFraction_vs_PtCut.eps	r1	manage	23.5 K	2016-10-18 - 14:44	MartinAleksa
pdf	PUSuppression_NJetsAndHSFraction_vs_PtCut.pdf	r1	manage	21.2 K	2016-10-18 - 14:44	MartinAleksa
png	PUSuppression_NJetsAndHSFraction_vs_PtCut.png	r1	manage	30.0 K	2016-10-18 - 14:44	MartinAleksa
eps	ROC-eff-eta38to42.eps	r1	manage	1596.5 K	2016-10-18 - 16:12	MartinAleksa
pdf	ROC-eff-eta38to42.pdf	r1	manage	690.8 K	2016-10-18 - 16:12	MartinAleksa
png	ROC-eff-eta38to42.png	r1	manage	655.0 K	2016-10-18 - 16:12	MartinAleksa
eps	ROC_effHS_pt20_extr_JES_preliminary.eps	r1	manage	13.7 K	2016-10-18 - 14:44	MartinAleksa
pdf	ROC_effHS_pt20_extr_JES_preliminary.pdf	r1	manage	19.1 K	2016-10-18 - 14:44	MartinAleksa
png	ROC_effHS_pt20_extr_JES_preliminary.png	r1	manage	27.9 K	2016-10-18 - 14:44	MartinAleksa
eps	noise_tot_ratio_sFCal_SmallGaps_over_FCal_mu200-new_prelim.eps	r1	manage	22.1 K	2016-10-18 - 14:43	MartinAleksa
pdf	noise_tot_ratio_sFCal_SmallGaps_over_FCal_mu200-new_prelim.pdf	r1	manage	21.8 K	2016-10-18 - 14:43	MartinAleksa
png	noise_tot_ratio_sFCal_SmallGaps_over_FCal_mu200-new_prelim.png	r1	manage	23.0 K	2016-10-18 - 14:43	MartinAleksa
eps	sFCalReview_CellSig_VBF2600_prelim.eps	r1	manage	19.3 K	2016-10-18 - 14:43	MartinAleksa
pdf	sFCalReview_CellSig_VBF2600_prelim.pdf	r1	manage	16.2 K	2016-10-18 - 14:43	MartinAleksa
png	sFCalReview_CellSig_VBF2600_prelim.png	r1	manage	26.8 K	2016-10-18 - 14:43	MartinAleksa
eps	sFCalReview_NConst_VBF2600_prelim.eps	r1	manage	28.8 K	2016-10-18 - 14:43	MartinAleksa
pdf	sFCalReview_NConst_VBF2600_prelim.pdf	r1	manage	23.8 K	2016-10-18 - 14:43	MartinAleksa
png	sFCalReview_NConst_VBF2600_prelim.png	r1	manage	28.1 K	2016-10-18 - 14:43	MartinAleksa
png	fig1.png	r2 r1	manage	84.7 K	2015-11-12 - 16:58	MartinAleksa	Demonstrator SC plots (png)
png	fig2.png	r2 r1	manage	63.0 K	2015-11-12 - 16:58	MartinAleksa	Demonstrator SC plots (png)
png	fig3.png	r2 r1	manage	64.2 K	2015-11-12 - 16:58	MartinAleksa	Demonstrator SC plots (png)
png	fig4.png	r2 r1	manage	66.1 K	2015-11-12 - 16:58	MartinAleksa	Demonstrator SC plots (png)
png	fig5.png	r2 r1	manage	69.0 K	2015-11-12 - 16:58	MartinAleksa	Demonstrator SC plots (png)
png	fig6.png	r2 r1	manage	104.8 K	2015-11-12 - 16:58	MartinAleksa	Demonstrator SC plots (png)
png	fig7.png	r2 r1	manage	27.5 K	2015-11-12 - 16:58	MartinAleksa	Demonstrator SC plots (png)
png	fig8.png	r2 r1	manage	29.0 K	2015-11-12 - 16:58	MartinAleksa	Demonstrator SC plots (png)
pdf	fig1.pdf	r2 r1	manage	70.2 K	2015-11-12 - 17:00	MartinAleksa	Demonstrator SC Plots (pdf)
pdf	fig2.pdf	r2 r1	manage	10.0 K	2015-11-12 - 17:00	MartinAleksa	Demonstrator SC Plots (pdf)
pdf	fig3.pdf	r2 r1	manage	10.5 K	2015-11-12 - 17:00	MartinAleksa	Demonstrator SC Plots (pdf)
pdf	fig4.pdf	r2 r1	manage	14.3 K	2015-11-12 - 17:00	MartinAleksa	Demonstrator SC Plots (pdf)
pdf	fig5.pdf	r2 r1	manage	12.9 K	2015-11-12 - 17:00	MartinAleksa	Demonstrator SC Plots (pdf)
pdf	fig6.pdf	r2 r1	manage	84.1 K	2015-11-12 - 17:00	MartinAleksa	Demonstrator SC Plots (pdf)
pdf	fig7.pdf	r2 r1	manage	5.0 K	2015-11-12 - 17:00	MartinAleksa	Demonstrator SC Plots (pdf)
pdf	fig8.pdf	r2 r1	manage	5.3 K	2015-11-12 - 17:00	MartinAleksa	Demonstrator SC Plots (pdf)
eps	fig1.eps	r2 r1	manage	980.0 K	2015-11-12 - 16:59	MartinAleksa	Demonstrator SC Plots (eps)
eps	fig2.eps	r2 r1	manage	20.1 K	2015-11-12 - 16:59	MartinAleksa	Demonstrator SC Plots (eps)
eps	fig3.eps	r2 r1	manage	20.8 K	2015-11-12 - 16:59	MartinAleksa	Demonstrator SC Plots (eps)
eps	fig4.eps	r2 r1	manage	29.8 K	2015-11-12 - 16:59	MartinAleksa	Demonstrator SC Plots (eps)
eps	fig5.eps	r2 r1	manage	26.6 K	2015-11-12 - 16:59	MartinAleksa	Demonstrator SC Plots (eps)
eps	fig6.eps	r2 r1	manage	115.9 K	2015-11-12 - 16:59	MartinAleksa	Demonstrator SC Plots (eps)
eps	fig7.eps	r2 r1	manage	9.5 K	2015-11-12 - 16:59	MartinAleksa	Demonstrator SC Plots (eps)
eps	fig8.eps	r2 r1	manage	10.1 K	2015-11-12 - 16:59	MartinAleksa	Demonstrator SC Plots (eps)
eps	Event_3_Demonstrator.eps	r1	manage	22.8 K	2017-09-12 - 14:05	SteffenStaerz	Demonstrator event display: event 3
pdf	Event_3_Demonstrator.pdf	r1	manage	17.5 K	2017-09-12 - 14:05	SteffenStaerz	Demonstrator event display: event 3
png	Event_3_Demonstrator.png	r2 r1	manage	96.0 K	2017-09-12 - 14:53	SteffenStaerz	Demonstrator event display: event 3
eps	Event_3_Main.eps	r1	manage	21.4 K	2017-09-12 - 14:05	SteffenStaerz	Demonstrator event display: event 3
pdf	Event_3_Main.pdf	r1	manage	17.0 K	2017-09-12 - 14:05	SteffenStaerz	Demonstrator event display: event 3
png	Event_3_Main.png	r2 r1	manage	94.5 K	2017-09-12 - 14:54	SteffenStaerz	Demonstrator event display: event 3
eps	Event_2_Demonstrator.eps	r1	manage	22.3 K	2017-09-12 - 14:04	SteffenStaerz	Demonstrator event display: event 2
pdf	Event_2_Demonstrator.pdf	r1	manage	17.3 K	2017-09-12 - 14:04	SteffenStaerz	Demonstrator event display: event 2
png	Event_2_Demonstrator.png	r2 r1	manage	97.4 K	2017-09-12 - 14:52	SteffenStaerz	Demonstrator event display: event 2
eps	Event_2_Main.eps	r1	manage	26.2 K	2017-09-12 - 14:04	SteffenStaerz	Demonstrator event display: event 2
pdf	Event_2_Main.pdf	r1	manage	23.6 K	2017-09-12 - 14:04	SteffenStaerz	Demonstrator event display: event 2
png	Event_2_Main.png	r2 r1	manage	104.4 K	2017-09-12 - 14:53	SteffenStaerz	Demonstrator event display: event 2
eps	Event_1_Demonstrator.eps	r1	manage	22.2 K	2017-09-12 - 14:04	SteffenStaerz	Demonstrator event display: event 1
pdf	Event_1_Demonstrator.pdf	r1	manage	17.3 K	2017-09-12 - 14:04	SteffenStaerz	Demonstrator event display: event 1
png	Event_1_Demonstrator.png	r2 r1	manage	97.0 K	2017-09-12 - 14:51	SteffenStaerz	Demonstrator event display: event 1
eps	Event_1_Main.eps	r1	manage	23.9 K	2017-09-12 - 14:04	SteffenStaerz	Demonstrator event display: event 1
pdf	Event_1_Main.pdf	r1	manage	22.4 K	2017-09-12 - 14:04	SteffenStaerz	Demonstrator event display: event 1
png	Event_1_Main.png	r2 r1	manage	98.8 K	2017-09-12 - 14:51	SteffenStaerz	Demonstrator event display: event 1
eps	Event_0_Demonstrator_Partial.eps	r1	manage	20.3 K	2017-09-12 - 14:04	SteffenStaerz	Demonstrator event display: event 0 (zoom)
pdf	Event_0_Demonstrator_Partial.pdf	r1	manage	16.6 K	2017-09-12 - 14:04	SteffenStaerz	Demonstrator event display: event 0 (zoom)
png	Event_0_Demonstrator_Partial.png	r3 r2 r1	manage	102.3 K	2017-09-12 - 14:48	SteffenStaerz	Demonstrator event display: event 0 (zoom)
eps	Event_0_Main_Partial.eps	r1	manage	23.6 K	2017-09-12 - 14:04	SteffenStaerz	Demonstrator event display: event 0 (zoom)
pdf	Event_0_Main_Partial.pdf	r1	manage	17.7 K	2017-09-12 - 14:04	SteffenStaerz	Demonstrator event display: event 0 (zoom)
png	Event_0_Main_Partial.png	r3 r2 r1	manage	110.3 K	2017-09-12 - 14:50	SteffenStaerz	Demonstrator event display: event 0 (zoom)
eps	Event_0_Demonstrator_Full.eps	r1	manage	21.7 K	2017-09-12 - 14:03	SteffenStaerz	Demonstrator event display: event 0 (full)
pdf	Event_0_Demonstrator_Full.pdf	r1	manage	17.1 K	2017-09-12 - 14:03	SteffenStaerz	Demonstrator event display: event 0 (full)
png	Event_0_Demonstrator_Full.png	r2 r1	manage	96.2 K	2017-09-12 - 14:47	SteffenStaerz	Demonstrator event display: event 0 (full)
eps	Event_0_Main_Full.eps	r1	manage	22.8 K	2017-09-12 - 14:03	SteffenStaerz	Demonstrator event display: event 0 (full)
pdf	Event_0_Main_Full.pdf	r1	manage	17.4 K	2017-09-12 - 14:03	SteffenStaerz	Demonstrator event display: event 0 (full)
png	Event_0_Main_Full.png	r2 r1	manage	98.4 K	2017-09-12 - 14:49	SteffenStaerz	Demonstrator event display: event 0 (full)
eps	difference_back.eps	r1	manage	9.2 K	2017-09-12 - 14:01	SteffenStaerz	Demonstrator energy measurement
pdf	difference_back.pdf	r1	manage	13.8 K	2017-09-12 - 14:01	SteffenStaerz	Demonstrator energy measurement
png	difference_back.png	r2 r1	manage	25.7 K	2017-09-12 - 14:55	SteffenStaerz	Demonstrator energy measurement
eps	difference_front.eps	r1	manage	9.0 K	2017-09-12 - 14:01	SteffenStaerz	Demonstrator energy measurement
pdf	difference_front.pdf	r1	manage	13.7 K	2017-09-12 - 14:01	SteffenStaerz	Demonstrator energy measurement
png	difference_front.png	r2 r1	manage	25.4 K	2017-09-12 - 14:55	SteffenStaerz	Demonstrator energy measurement
eps	difference_middle.eps	r1	manage	9.8 K	2017-09-12 - 14:02	SteffenStaerz	Demonstrator energy measurement
pdf	difference_middle.pdf	r1	manage	13.9 K	2017-09-12 - 14:02	SteffenStaerz	Demonstrator energy measurement
png	difference_middle.png	r2 r1	manage	28.3 K	2017-09-12 - 14:55	SteffenStaerz	Demonstrator energy measurement
eps	difference_presampler.eps	r1	manage	9.5 K	2017-09-12 - 14:02	SteffenStaerz	Demonstrator energy measurement
pdf	difference_presampler.pdf	r1	manage	13.9 K	2017-09-12 - 14:02	SteffenStaerz	Demonstrator energy measurement
png	difference_presampler.png	r2 r1	manage	26.6 K	2017-09-12 - 14:55	SteffenStaerz	Demonstrator energy measurement
eps	scatter_back.eps	r1	manage	13.2 K	2017-09-12 - 14:06	SteffenStaerz	Demonstrator energy measurement
pdf	scatter_back.pdf	r1	manage	15.2 K	2017-09-12 - 14:06	SteffenStaerz	Demonstrator energy measurement
png	scatter_back.png	r2 r1	manage	83.9 K	2017-09-12 - 14:55	SteffenStaerz	Demonstrator energy measurement
eps	scatter_front.eps	r1	manage	14.0 K	2017-09-12 - 14:06	SteffenStaerz	Demonstrator energy measurement
pdf	scatter_front.pdf	r1	manage	15.4 K	2017-09-12 - 14:06	SteffenStaerz	Demonstrator energy measurement
png	scatter_front.png	r3 r2 r1	manage	87.0 K	2017-09-12 - 14:55	SteffenStaerz	Demonstrator energy measurement
eps	scatter_middle.eps	r1	manage	18.2 K	2017-09-12 - 14:07	SteffenStaerz	Demonstrator energy measurement
pdf	scatter_middle.pdf	r1	manage	16.6 K	2017-09-12 - 14:07	SteffenStaerz	Demonstrator energy measurement
png	scatter_middle.png	r2 r1	manage	95.1 K	2017-09-12 - 14:55	SteffenStaerz	Demonstrator energy measurement
eps	scatter_presampler.eps	r1	manage	14.6 K	2017-09-12 - 14:07	SteffenStaerz	Demonstrator energy measurement
pdf	scatter_presampler.pdf	r1	manage	15.4 K	2017-09-12 - 14:07	SteffenStaerz	Demonstrator energy measurement
png	scatter_presampler.png	r3 r2 r1	manage	85.0 K	2017-09-12 - 14:55	SteffenStaerz	Demonstrator energy measurement
jpg	Poster_plots_approval_new.jpg	r1	manage	37.7 K	2015-02-23 - 17:19	MartinAleksa	CNF Explanation

Topic revision: r20 - 2017-09-26 - SteffenStaerz

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