CMSPublic Web>PhysicsResults>HighLevelTriggerRunIIResults>HLTplots2017DataSummaryElectrons (2018-07-13, ElisabettaGallo)

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Electron trigger performance in CMS with the full 2017 data sample (CMS-DP-2018/030)

Electron trigger performance in CMS with the full 2017 data sample (CMS-DP-2018/030)

Trigger performance in 2017 and comparison with 2016 data

HLT_Ele23_Ele12_CaloIDL_TrackIdL_IsoVL : standard double electron trigger with loose ID and isolation requirements

Pixel match filter efficiency of HLT_Ele23_Ele12_CaloIDL_TrackIdL_IsoVL in 2017, comparison with Monte Carlo

HLT_Ele32_WPTight_Gsf : standard single electron trigger with tight ID + isolation

HLT_Double Ele33_CaloIdL_MW : double electron trigger with loose ID, no isolation, but with "medium" window pixel matching.

HLT_Ele23_Ele12_CaloIDL_TrackIdL_IsoVL

		Ele23 leg efficiency of HLT_Ele23_Ele12_CaloIDL_TrackIdL_IsoVL path as a function of SC ET The efficiency for the Ele23 leg of the HLT_Ele23_Ele12 trigger as a function of supercluster (SC) EΤ for ECAL barrel (left) and ECAL endcap (right) presented for 2016 and 2017 data. Due to the presence of a high pT electron in the event, the L1 threshold on the second electron is lowered to 5 GeV in 2017 which effectively removes L1 turn on effects from the measured efficiency. The rate of the trigger in 2017, corresponding to Run Number 302596 (Average pileup=38) is 8.53 Hz, whereas in 2016 corresponding to Run Number 283885 (Average pileup =43), is 24.83 Hz. We see 70% rate reduction in 2017 with the new pixel detector for a small (1-2%) loss in efficiency. [Get pdf version EB] [Get pdf version EE] Contact: Bhawna Gomber

Ele23 leg efficiency of HLT_Ele23_Ele12_CaloIDL_TrackIdL_IsoVL path as a function of SC ET
The efficiency for the Ele23 leg of the HLT_Ele23_Ele12 trigger as a function of supercluster (SC) EΤ for ECAL barrel (left) and ECAL endcap (right) presented for 2016 and 2017 data. Due to the presence of a high pT electron in the event, the L1 threshold on the second electron is lowered to 5 GeV in 2017 which effectively removes L1 turn on effects from the measured efficiency.
The rate of the trigger in 2017, corresponding to Run Number 302596 (Average pileup=38) is 8.53 Hz, whereas in 2016 corresponding to Run Number 283885 (Average pileup =43), is 24.83 Hz. We see 70% rate reduction in 2017 with the new pixel detector for a small (1-2%) loss in efficiency.
[Get pdf version EB] [Get pdf version EE]
Contact: Bhawna Gomber

	Ele23 leg efficiency of HLT_Ele23_Ele12_CaloIDL_TrackIdL_IsoVL path as a function of SC eta The efficiency for the Ele23 leg of the HLT_Ele23_Ele12 trigger as a function of supercluster (SC) η (with SC ET > 50 GeV) presented for 2016 and 2017 data. Due to the presence of a high pT electron in the event, the L1 threshold on the second electron is lowered to 5 GeV which effectively removes L1 turn on effects from the measured efficiency. The rate of the trigger in 2017, corresponding to Run Number 302596 (Average pileup=38) is 8.53 Hz, whereas in 2016 corresponding to Run Number 283885 (Average pileup =43), is 24.83 Hz. We see 70% rate reduction in 2017 with the new pixel detector for a small (1-2%) loss in efficiency. [Get pdf version] Contact: Bhawna Gomber

Ele23 leg efficiency of HLT_Ele23_Ele12_CaloIDL_TrackIdL_IsoVL path as a function of SC eta
The efficiency for the Ele23 leg of the HLT_Ele23_Ele12 trigger as a function of supercluster (SC) η (with SC ET > 50 GeV) presented for 2016 and 2017 data. Due to the presence of a high pT electron in the event, the L1 threshold on the second electron is lowered to 5 GeV which effectively removes L1 turn on effects from the measured efficiency.
The rate of the trigger in 2017, corresponding to Run Number 302596 (Average pileup=38) is 8.53 Hz, whereas in 2016 corresponding to Run Number 283885 (Average pileup =43), is 24.83 Hz. We see 70% rate reduction in 2017 with the new pixel detector for a small (1-2%) loss in efficiency.
[Get pdf version]
Contact: Bhawna Gomber

		Ele23 leg efficiency of HLT_Ele23_Ele12_CaloIDL_TrackIdL_IsoVL path as a function of number of vertices The efficiency for the Ele23 leg of the HLT_Ele23_Ele12 trigger as a function of the number of offline vertices (with SC ET > 50 GeV, SC abs(η) < 2.5) for ECAL barrel (left) and ECAL endcap (right) presented for 2016 and 2017 data. Due to the presence of a high pT electron in the event, the L1 threshold on the second electron is lowered to 5 GeV which effectively removes L1 turn on effects from the measured efficiency. The rate of the trigger in 2017, corresponding to Run Number 302596 (Average pileup=38) is 8.53 Hz, whereas in 2016 corresponding to Run Number 283885 (Average pileup =43), is 24.83 Hz. We see 70% rate reduction in 2017 with the new pixel detector for a small (1-2%) loss in efficiency. [Get pdf version EB] [Get pdf version EE] Contact: Bhawna Gomber

Ele23 leg efficiency of HLT_Ele23_Ele12_CaloIDL_TrackIdL_IsoVL path as a function of number of vertices
The efficiency for the Ele23 leg of the HLT_Ele23_Ele12 trigger as a function of the number of offline vertices (with SC ET > 50 GeV, SC abs(η) < 2.5) for ECAL barrel (left) and ECAL endcap (right) presented for 2016 and 2017 data. Due to the presence of a high pT electron in the event, the L1 threshold on the second electron is lowered to 5 GeV which effectively removes L1 turn on effects from the measured efficiency.
The rate of the trigger in 2017, corresponding to Run Number 302596 (Average pileup=38) is 8.53 Hz, whereas in 2016 corresponding to Run Number 283885 (Average pileup =43), is 24.83 Hz. We see 70% rate reduction in 2017 with the new pixel detector for a small (1-2%) loss in efficiency.
[Get pdf version EB] [Get pdf version EE]
Contact: Bhawna Gomber

Pixel match filter efficiency of HLT_Ele23_Ele12_CaloIDL_TrackIdL_IsoVL

		Efficiency of the pixel match filter for HLT_Ele23_Ele12_CaloIDL_TrackIdL_IsoVL path as a function of SC ET The efficiency of the pixel match filter (where we require supercluster to have 3 matching hits in the pixel detector) for the Ele23 leg of the HLT_Ele23_Ele12 trigger as a function of supercluster EΤ for ECAL barrel (left) and ECAL endcap (right) presented for 2017 data and MC. Due to the presence of a high pT electron in the event, the L1 threshold on the second electron is lowered to 5 GeV which effectively removes L1 turn on effects from the measured efficiency. DCDC converters that provide LV (VA/VD) for pixel detector modules start failing on October 5, 2017. The efficiency is shown for different pixel detector conditions, commissioning period (run<=302026), Nominal WP Pre Oct 5th (302026 <run<304366), and Nominal WP Post Oct 5th (run>=304366). By comparing periods with and without the DCDC issue, the effect on the Egamma trigger performance is estimated to be a few percent, ~1-2%. [Get pdf version EB] [Get pdf version EE] Contact: Bhawna Gomber

Efficiency of the pixel match filter for HLT_Ele23_Ele12_CaloIDL_TrackIdL_IsoVL path as a function of SC ET
The efficiency of the pixel match filter (where we require supercluster to have 3 matching hits in the pixel detector) for the Ele23 leg of the HLT_Ele23_Ele12 trigger as a function of supercluster EΤ for ECAL barrel (left) and ECAL endcap (right) presented for 2017 data and MC.
Due to the presence of a high pT electron in the event, the L1 threshold on the second electron is lowered to 5 GeV which effectively removes L1 turn on effects from the measured efficiency.
DCDC converters that provide LV (VA/VD) for pixel detector modules start failing on October 5, 2017.
The efficiency is shown for different pixel detector conditions, commissioning period (run<=302026), Nominal WP Pre Oct 5th (302026 <run<304366), and Nominal WP Post Oct 5th (run>=304366). By comparing periods with and without the DCDC issue, the effect on the Egamma trigger performance is estimated to be a few percent, ~1-2%.
[Get pdf version EB] [Get pdf version EE]
Contact: Bhawna Gomber

	Efficiency of the pixel match filter for HLT_Ele23_Ele12_CaloIDL_TrackIdL_IsoVL path as a function of SC eta The efficiency of the pixel match filter (where we require supercluster to have 3 matching hits in the pixel detector) for the Ele23 leg of the HLT_Ele23_Ele12 trigger as a function of supercluster η (with SC ET > 50 GeV) presented for 2017 data and MC. Due to the presence of a high pT electron in the event, the L1 threshold on the second electron is lowered to 5 GeV which effectively removes L1 turn on effects from the measured efficiency. DCDC converters that provide LV (VA/VD) for pixel detector modules start failing on October 5, 2017. The efficiency is shown for different pixel detector conditions, commissioning period (run<=302026), Nominal WP Pre Oct 5th (302026 <run<304366), and Nominal WP Post Oct 5th (run>=304366). By comparing periods with and without the DCDC issue, the effect on the Egamma trigger performance is estimated to be a few percent, ~1-2%. [Get pdf version] Contact: Bhawna Gomber

Efficiency of the pixel match filter for HLT_Ele23_Ele12_CaloIDL_TrackIdL_IsoVL path as a function of SC eta
The efficiency of the pixel match filter (where we require supercluster to have 3 matching hits in the pixel detector) for the Ele23 leg of the HLT_Ele23_Ele12 trigger as a function of supercluster η (with SC ET > 50 GeV) presented for 2017 data and MC. Due to the presence of a high pT electron in the event, the L1 threshold on the second electron is lowered to 5 GeV which effectively removes L1 turn on effects from the measured efficiency.
DCDC converters that provide LV (VA/VD) for pixel detector modules start failing on October 5, 2017.
The efficiency is shown for different pixel detector conditions, commissioning period (run<=302026), Nominal WP Pre Oct 5th (302026 <run<304366), and Nominal WP Post Oct 5th (run>=304366). By comparing periods with and without the DCDC issue, the effect on the Egamma trigger performance is estimated to be a few percent, ~1-2%.
[Get pdf version]
Contact: Bhawna Gomber

		Efficiency of the pixel match filter for HLT_Ele23_Ele12_CaloIDL_TrackIdL_IsoVL path as a function of number of vertices The efficiency of the pixel match filter (where we require supercluster to have 3 matching hits in the pixel detector) for the Ele23 leg of the HLT_Ele23_Ele12 trigger as a function of the number of offline vertices (with SC ET > 50 GeV, SC abs(η) < 2.5) for ECAL barrel (left) and ECAL endcap (right) presented for 2017 data and MC. Due to the presence of a high pT electron in the event, the L1 threshold on the second electron is lowered to 5 GeV which effectively removes L1 turn on effects from the measured efficiency. DCDC converters that provide LV (VA/VD) for pixel detector modules start failing on October 5, 2017. The efficiency is shown for different pixel detector conditions, commissioning period (run<=302026), Nominal WP Pre Oct 5th (302026 <run<304366), and Nominal WP Post Oct 5th (run>=304366). By comparing periods with and without the DCDC issue, the effect on the Egamma trigger performance is estimated to be a few percent, ~1-2%. [Get pdf version EB] [Get pdf version EE] Contact: Bhawna Gomber

Efficiency of the pixel match filter for HLT_Ele23_Ele12_CaloIDL_TrackIdL_IsoVL path as a function of number of vertices
The efficiency of the pixel match filter (where we require supercluster to have 3 matching hits in the pixel detector) for the Ele23 leg of the HLT_Ele23_Ele12 trigger as a function of the number of offline vertices (with SC ET > 50 GeV, SC abs(η) < 2.5) for ECAL barrel (left) and ECAL endcap (right) presented for 2017 data and MC. Due to the presence of a high pT electron in the event, the L1 threshold on the second electron is lowered to 5 GeV which effectively removes L1 turn on effects from the measured efficiency.
DCDC converters that provide LV (VA/VD) for pixel detector modules start failing on October 5, 2017.
The efficiency is shown for different pixel detector conditions, commissioning period (run<=302026), Nominal WP Pre Oct 5th (302026 <run<304366), and Nominal WP Post Oct 5th (run>=304366).
By comparing periods with and without the DCDC issue, the effect on the Egamma trigger performance is estimated to be a few percent, ~1-2%.
[Get pdf version EB] [Get pdf version EE]
Contact: Bhawna Gomber

HLT_Ele32_WPTight_Gsf

		Efficiency of HLT_Ele32_WPTight path as a function of SC ET The efficiency of HLT_Ele32_WPTight_Gsf trigger as a function of supercluster EΤ for ECAL barrel (left) and ECAL endcap (right) presented for 2016H and 2017D data. The rate of the trigger in 2017, corresponding to Run Number 302596 (Average pileup=38) is 62.87 Hz, whereas in 2016 corresponding to Run Number 283885 (Average pileup =43), is 59.78 Hz. We see improvement in efficiency in the ecal endcap with the new Egamma working point which resulted in no change in trigger rate. [Get pdf version EB] [Get pdf version EE] Contact: Bhawna Gomber

Efficiency of HLT_Ele32_WPTight path as a function of SC ET
The efficiency of HLT_Ele32_WPTight_Gsf trigger as a function of supercluster EΤ for ECAL barrel (left) and ECAL endcap (right) presented for 2016H and 2017D data.
The rate of the trigger in 2017, corresponding to Run Number 302596 (Average pileup=38) is 62.87 Hz, whereas in 2016 corresponding to Run Number 283885 (Average pileup =43), is 59.78 Hz. We see improvement in efficiency in the ecal endcap with the new Egamma working point which resulted in no change in trigger rate.
[Get pdf version EB] [Get pdf version EE]
Contact: Bhawna Gomber

	Efficiency of HLT_Ele32_WPTight path as a function of SC eta The efficiency of HLT_Ele32_WPTight_Gsf trigger as a function of supercluster eta; (with SC ET > 50 GeV) presented for 2016H and 2017D data. The rate of the trigger in 2017, corresponding to Run Number 302596 (Average pileup=38) is 62.87 Hz, whereas in 2016 corresponding to Run Number 283885 (Average pileup =43), is 59.78 Hz. We see improvement in efficiency in the ecal endcap with the new Egamma working point which resulted in no change in trigger rate. [Get pdf version] Contact: Bhawna Gomber

Efficiency of HLT_Ele32_WPTight path as a function of SC eta
The efficiency of HLT_Ele32_WPTight_Gsf trigger as a function of supercluster eta; (with SC ET > 50 GeV) presented for 2016H and 2017D data.
The rate of the trigger in 2017, corresponding to Run Number 302596 (Average pileup=38) is 62.87 Hz, whereas in 2016 corresponding to Run Number 283885 (Average pileup =43), is 59.78 Hz. We see improvement in efficiency in the ecal endcap with the new Egamma working point which resulted in no change in trigger rate.
[Get pdf version]
Contact: Bhawna Gomber

		Efficiency of HLT_Ele32_WPTight path as a function of SC number of vertices The efficiency of HLT_Ele32_WPTight_Gsf trigger as a function of the number of offline vertices (with SC ET > 50 GeV, SC abs(η) < 2.5) for ECAL barrel (left) and ECAL endcap (right) presented for 2016H and 2017D data. The rate of the trigger in 2017, corresponding to Run Number 302596 (Average pileup=38) is 62.87 Hz, whereas in 2016 corresponding to Run Number 283885 (Average pileup =43), is 59.78 Hz. We see improvement in efficiency in the ecal endcap with the new Egamma working point which resulted in no change in trigger rate. [Get pdf version EB] [Get pdf version EE] Contact: Bhawna Gomber

Efficiency of HLT_Ele32_WPTight path as a function of SC number of vertices
The efficiency of HLT_Ele32_WPTight_Gsf trigger as a function of the number of offline vertices (with SC ET > 50 GeV, SC abs(η) < 2.5) for ECAL barrel (left) and ECAL endcap (right) presented for 2016H and 2017D data.
The rate of the trigger in 2017, corresponding to Run Number 302596 (Average pileup=38) is 62.87 Hz, whereas in 2016 corresponding to Run Number 283885 (Average pileup =43), is 59.78 Hz. We see improvement in efficiency in the ecal endcap with the new Egamma working point which resulted in no change in trigger rate.
[Get pdf version EB] [Get pdf version EE]
Contact: Bhawna Gomber

HLT_Double Ele33_CaloIdL_MW

		Efficiency of HLT_DoubleEle33_CaloID_MW path as a function of SC ET The efficiency for the seeded leg of the HLT_DoubleEle33_CaloIdL_MW trigger as a function of supercluster EΤ for ECAL barrel (left) and ECAL endcap (right) presented for 2016 and 2017 data. Due to the presence of a high pT electron in the event, the L1 threshold on the second electron is lowered to 5 GeV which effectively removes L1 turn on effects from the measured efficiency. The rate of the trigger in 2017, corresponding to Run Number 302596 (Average pileup=38) is 4.59 Hz, whereas in 2016 corresponding to Run Number 283885 (Average pileup =43), is 8.57 Hz. We see 50% rate reduction in 2017 with the new pixel detector for the small (1-2%) loss in efficiency. [Get pdf version EB] [Get pdf version EE] Contact: Bhawna Gomber

Efficiency of HLT_DoubleEle33_CaloID_MW path as a function of SC ET
The efficiency for the seeded leg of the HLT_DoubleEle33_CaloIdL_MW trigger as a function of supercluster EΤ for ECAL barrel (left) and ECAL endcap (right) presented for 2016 and 2017 data. Due to the presence of a high pT electron in the event, the L1 threshold on the second electron is lowered to 5 GeV which effectively removes L1 turn on effects from the measured efficiency.
The rate of the trigger in 2017, corresponding to Run Number 302596 (Average pileup=38) is 4.59 Hz, whereas in 2016 corresponding to Run Number 283885 (Average pileup =43), is 8.57 Hz. We see 50% rate reduction in 2017 with the new pixel detector for the small (1-2%) loss in efficiency.
[Get pdf version EB] [Get pdf version EE]
Contact: Bhawna Gomber

	Efficiency of HLT_DoubleEle33_CaloID_MW path as a function of SC eta The efficiency for the seeded leg of the HLT_DoubleEle33_CaloIdL_MW as a function of supercluster η (with SC ET > 50 GeV) presented for 2016 and 2017 data. Due to the presence of a high pT electron in the event, the L1 threshold on the second electron is lowered to 5 GeV which effectively removes L1 turn on effects from the measured efficiency. The rate of the trigger in 2017, corresponding to Run Number 302596 (Average pileup=38) is 4.59 Hz, whereas in 2016 corresponding to Run Number 283885 (Average pileup =43), is 8.57 Hz. We see 50% rate reduction in 2017 with the new pixel detector for the small (1-2%) loss in efficiency. [Get pdf version Contact: Bhawna Gomber

Efficiency of HLT_DoubleEle33_CaloID_MW path as a function of SC eta
The efficiency for the seeded leg of the HLT_DoubleEle33_CaloIdL_MW as a function of supercluster η (with SC ET > 50 GeV) presented for 2016 and 2017 data. Due to the presence of a high pT electron in the event, the L1 threshold on the second electron is lowered to 5 GeV which effectively removes L1 turn on effects from the measured efficiency.
The rate of the trigger in 2017, corresponding to Run Number 302596 (Average pileup=38) is 4.59 Hz, whereas in 2016 corresponding to Run Number 283885 (Average pileup =43), is 8.57 Hz. We see 50% rate reduction in 2017 with the new pixel detector for the small (1-2%) loss in efficiency.
[Get pdf version
Contact: Bhawna Gomber

		Efficiency of HLT_DoubleEle33_CaloID_MW path as a function of number of vertices The efficiency for the seeded leg of the HLT_DoubleEle33_CaloIdL_MW as a function of the number of offline vertices (with SC ET > 50 GeV, SC abs(η) < 2.5) for ECAL barrel (left) and ECAL endcap (right) presented for 2016 and 2017 data. Due to the presence of a high pT electron in the event, the L1 threshold on the second electron is lowered to 5 GeV which effectively removes L1 turn on effects from the measured efficiency. The rate of the trigger in 2017, corresponding to Run Number 302596 (Average pileup=38) is 4.59 Hz, whereas in 2016 corresponding to Run Number 283885 (Average pileup =43), is 8.57 Hz. We see 50% rate reduction in 2017 with the new pixel detector for the small (1-2%) loss in efficiency. [Get pdf version EB] [Get pdf version EE] Contact: Bhawna Gomber

Efficiency of HLT_DoubleEle33_CaloID_MW path as a function of number of vertices
The efficiency for the seeded leg of the HLT_DoubleEle33_CaloIdL_MW as a function of the number of offline vertices (with SC ET > 50 GeV, SC abs(η) < 2.5) for ECAL barrel (left) and ECAL endcap (right) presented for 2016 and 2017 data. Due to the presence of a high pT electron in the event, the L1 threshold on the second electron is lowered to 5 GeV which effectively removes L1 turn on effects from the measured efficiency.
The rate of the trigger in 2017, corresponding to Run Number 302596 (Average pileup=38) is 4.59 Hz, whereas in 2016 corresponding to Run Number 283885 (Average pileup =43), is 8.57 Hz. We see 50% rate reduction in 2017 with the new pixel detector for the small (1-2%) loss in efficiency.
[Get pdf version EB] [Get pdf version EE]
Contact: Bhawna Gomber

-- ElisabettaGallo - 2018-07-08

Attachments

Topic attachments
I	Attachment	History	Action	Size	Date	Who
pdf	Ele23_Et_EB.pdf	r1	manage	18.3 K	2018-07-08 - 17:09	ElisabettaGallo
png	Ele23_Et_EB.png	r1	manage	24.4 K	2018-07-13 - 20:16	ElisabettaGallo
pdf	Ele23_Et_EE.pdf	r1	manage	18.2 K	2018-07-08 - 17:09	ElisabettaGallo
png	Ele23_Et_EE.png	r1	manage	25.1 K	2018-07-13 - 20:16	ElisabettaGallo
pdf	Ele23_Eta.pdf	r1	manage	18.4 K	2018-07-08 - 17:09	ElisabettaGallo
png	Ele23_Eta.png	r1	manage	23.7 K	2018-07-13 - 20:16	ElisabettaGallo
pdf	Ele23_Nvtx_EB.pdf	r1	manage	20.8 K	2018-07-08 - 17:09	ElisabettaGallo
png	Ele23_Nvtx_EB.png	r1	manage	27.4 K	2018-07-13 - 20:16	ElisabettaGallo
pdf	Ele23_Nvtx_EE.pdf	r1	manage	20.5 K	2018-07-08 - 17:09	ElisabettaGallo
png	Ele23_Nvtx_EE.png	r1	manage	27.2 K	2018-07-13 - 20:16	ElisabettaGallo
pdf	Et_EB.pdf	r1	manage	17.9 K	2018-07-08 - 17:11	ElisabettaGallo
png	Et_EB.png	r1	manage	24.1 K	2018-07-13 - 20:18	ElisabettaGallo
pdf	Et_EE.pdf	r1	manage	18.6 K	2018-07-08 - 17:11	ElisabettaGallo
png	Et_EE.png	r1	manage	24.9 K	2018-07-13 - 20:18	ElisabettaGallo
pdf	Eta.pdf	r1	manage	18.8 K	2018-07-08 - 17:11	ElisabettaGallo
png	Eta.png	r1	manage	23.6 K	2018-07-13 - 20:18	ElisabettaGallo
pdf	Nvtx_EB.pdf	r1	manage	20.2 K	2018-07-08 - 17:11	ElisabettaGallo
png	Nvtx_EB.png	r1	manage	27.0 K	2018-07-13 - 20:18	ElisabettaGallo
pdf	Nvtx_EE.pdf	r1	manage	20.2 K	2018-07-08 - 17:11	ElisabettaGallo
png	Nvtx_EE.png	r1	manage	27.4 K	2018-07-13 - 20:18	ElisabettaGallo
pdf	PixelMatch_Et_EB.pdf	r1	manage	26.1 K	2018-07-08 - 17:11	ElisabettaGallo
png	PixelMatch_Et_EB.png	r1	manage	34.7 K	2018-07-13 - 20:18	ElisabettaGallo
pdf	PixelMatch_Et_EE.pdf	r1	manage	26.8 K	2018-07-08 - 17:11	ElisabettaGallo
png	PixelMatch_Et_EE.png	r1	manage	35.6 K	2018-07-13 - 20:18	ElisabettaGallo
pdf	PixelMatch_Eta.pdf	r1	manage	23.1 K	2018-07-08 - 17:11	ElisabettaGallo
png	PixelMatch_Eta.png	r1	manage	30.8 K	2018-07-13 - 20:18	ElisabettaGallo
pdf	PixelMatch_Nvtx_EB.pdf	r1	manage	26.8 K	2018-07-08 - 17:11	ElisabettaGallo
png	PixelMatch_Nvtx_EB.png	r1	manage	33.2 K	2018-07-13 - 20:18	ElisabettaGallo
pdf	PixelMatch_Nvtx_EE.pdf	r1	manage	27.2 K	2018-07-08 - 17:11	ElisabettaGallo
png	PixelMatch_Nvtx_EE.png	r1	manage	32.1 K	2018-07-13 - 20:18	ElisabettaGallo
pdf	Seeded_Et_EB.pdf	r1	manage	18.1 K	2018-07-08 - 17:09	ElisabettaGallo
png	Seeded_Et_EB.png	r1	manage	23.1 K	2018-07-13 - 20:16	ElisabettaGallo
pdf	Seeded_Et_EE.pdf	r1	manage	18.0 K	2018-07-08 - 17:09	ElisabettaGallo
png	Seeded_Et_EE.png	r1	manage	23.8 K	2018-07-13 - 20:16	ElisabettaGallo
pdf	Seeded_Eta.pdf	r1	manage	18.9 K	2018-07-08 - 17:09	ElisabettaGallo
png	Seeded_Eta.png	r1	manage	23.6 K	2018-07-13 - 20:16	ElisabettaGallo
pdf	Seeded_Nvtx_EB.pdf	r1	manage	20.9 K	2018-07-08 - 17:09	ElisabettaGallo
png	Seeded_Nvtx_EB.png	r1	manage	26.6 K	2018-07-13 - 20:16	ElisabettaGallo
pdf	Seeded_Nvtx_EE.pdf	r1	manage	20.6 K	2018-07-08 - 17:09	ElisabettaGallo
png	Seeded_Nvtx_EE.png	r1	manage	27.1 K	2018-07-13 - 20:16	ElisabettaGallo

Topic revision: r3 - 2018-07-13 - ElisabettaGallo

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