CMSPublic Web>PhysicsResults>EcalDPGResults>EcalDPGResultsCMSDP2013026 (2013-10-11, FedericoFerri)

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CMS DP-2013/026 ECAL Upgrade performance plots (2)

Abstract: ECAL upgrade performance plots for 2013 LHCC and ECFA

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Figure	Caption
pdf version, eps version	*Contribution of ECAL ageing on the Higgs $\rightarrow\gamma\gamma$ mass resolution* The plot shows the contribution to the Higgs mass resolution due to the ECAL ageing, for the two photon decay of the Higgs boson, as a function of the maximum pseudo-rapidity of the photon pair. The mass resolution is calculated using a sample of $H\rightarrow\gamma\gamma$ events generated with the Pythia Monte Carlo program at $\sqrt{s} = 14$ TeV. For each event the photon energy is smeared using a gaussian smearing according to the test-beam ECAL energy resolution in the Barrel (EB) and Endcaps (EE). The degradation of the energy resolution, due to radiation, is based on the prediction of the crystal light output evolution calculated by the LITRANI program [1] as a function of the γ dose and hadron fluence, given by the MARS program [2] for various integrated luminosities, together with the average VPT response loss expected from laboratory measurements. The ageing contribution to the mass resolution is calculated as the difference in quadrature between the mass resolution calculated with the ageing and the nominal mass resolution. [1] F.-X. Gentit, Nucl. Instr. Meth. A 486 (2002) 35–39, 1036 doi:10.1016/S0168-9002(02)00671-X. [2] P.C. Bhat et al., CERN-CMS-NOTE-2013-001.
pdf version, eps version pdf version, eps version pdf version, eps version pdf version, eps version	*L1 trigger linearization coefficients* Linearization of the L1 trigger response: The signal for each channel (in ADC counts) is multiplied by a factor [1] depending on IC, Gain, η, laser corrections to provide a signal that is proportional to the transverse energy deposited in the crystal. This factor is encoded using 8 bits (mult) with a 4-bit exponent (shift) to keep an optimal resolution for low values ( $f = \mbox{mult}/2^{\mbox{\scriptsize shift}}$ ). It saturates at 255. The plots show the values of these coefficients in the ECAL endcaps for various ageing scenarios. The coefficients have been calculated assuming that the crystal light output evolves according to the predictions of the model by the LITRANI program [2] as a function of the γ dose and hadron fluence, given by the MARS program [3] for various integrated luminosities. The degradation of the light output of the inner EE eta rings cannot be compensated for at the trigger level at these high values of integrated luminosity without significantly increasing the triggering threshold. The electron/photon L1 trigger in EE will therefore gradually lose acceptance from the inner eta rings outwards [1] P. Paganini, J. Phys. Conf. Ser. 160 (2009) 012062. [2] F.-X. Gentit, Nucl. Instr. Meth. A 486 (2002) 35–39, 1036 doi:10.1016/S0168-9002(02)00671-X. [3] P.C. Bhat et al., CERN-CMS-NOTE-2013-001.

Figure

Caption

pdf version, eps version

Contribution of ECAL ageing on the Higgs $\rightarrow\gamma\gamma$ mass resolution

The plot shows the contribution to the Higgs mass resolution due to the ECAL ageing, for the two photon decay of the Higgs boson, as a function of the maximum pseudo-rapidity of the photon pair.
The mass resolution is calculated using a sample of $H\rightarrow\gamma\gamma$ events generated with the Pythia Monte Carlo program at $\sqrt{s} = 14$ TeV. For each event the photon energy is smeared using a gaussian smearing according to the test-beam ECAL energy resolution in the Barrel (EB) and Endcaps (EE). The degradation of the energy resolution, due to radiation, is based on the prediction of the crystal light output evolution calculated by the LITRANI program [1] as a function of the γ dose and hadron fluence, given by the MARS program [2] for various integrated luminosities, together with the average VPT response loss expected from laboratory measurements.
The ageing contribution to the mass resolution is calculated as the difference in quadrature between the mass resolution calculated with the ageing and the nominal mass resolution.
[1] F.-X. Gentit, Nucl. Instr. Meth. A 486 (2002) 35–39, 1036 doi:10.1016/S0168-9002(02)00671-X.
[2] P.C. Bhat et al., CERN-CMS-NOTE-2013-001.

pdf version, eps version

pdf version, eps version

pdf version, eps version

pdf version, eps version

L1 trigger linearization coefficients

Linearization of the L1 trigger response: The signal for each channel (in ADC counts) is multiplied by a factor [1] depending on IC, Gain, η, laser corrections to provide a signal that is proportional to the transverse energy deposited in the crystal. This factor is encoded using 8 bits (mult) with a 4-bit exponent (shift) to keep an optimal resolution for low values ( $f = \mbox{mult}/2^{\mbox{\scriptsize shift}}$ ). It saturates at 255. The plots show the values of these coefficients in the ECAL endcaps for various ageing scenarios.
The coefficients have been calculated assuming that the crystal light output evolves according to the predictions of the model by the LITRANI program [2] as a function of the γ dose and hadron fluence, given by the MARS program [3] for various integrated luminosities.
The degradation of the light output of the inner EE eta rings cannot be compensated for at the trigger level at these high values of integrated luminosity without significantly increasing the triggering threshold. The electron/photon L1 trigger in EE will therefore gradually lose acceptance from the inner eta rings outwards
[1] P. Paganini, J. Phys. Conf. Ser. 160 (2009) 012062.
[2] F.-X. Gentit, Nucl. Instr. Meth. A 486 (2002) 35–39, 1036 doi:10.1016/S0168-9002(02)00671-X.
[3] P.C. Bhat et al., CERN-CMS-NOTE-2013-001.

Attachments

Topic attachments
I	Attachment	History	Action	Size	Date	Who
ppt	ECAL_upgrade_plots.ppt	r1	manage	422.5 K	2013-10-09 - 18:20	FedericoFerri
eps	ageing_resolution.eps	r1	manage	83.8 K	2013-10-10 - 05:21	FedericoFerri
pdf	ageing_resolution.pdf	r1	manage	34.4 K	2013-10-10 - 05:21	FedericoFerri
png	ageing_resolution.png	r1	manage	76.5 K	2013-10-10 - 05:21	FedericoFerri
eps	lumi_209475_EELinear_0_log.eps	r1	manage	195.9 K	2013-10-10 - 05:17	FedericoFerri
pdf	lumi_209475_EELinear_0_log.pdf	r1	manage	45.5 K	2013-10-10 - 05:17	FedericoFerri
png	lumi_209475_EELinear_0_log.png	r1	manage	168.2 K	2013-10-10 - 05:17	FedericoFerri
eps	lumi_400500_EELinear_0_log.eps	r1	manage	199.4 K	2013-10-10 - 05:17	FedericoFerri
pdf	lumi_400500_EELinear_0_log.pdf	r1	manage	46.1 K	2013-10-10 - 05:17	FedericoFerri
png	lumi_400500_EELinear_0_log.png	r1	manage	171.6 K	2013-10-10 - 05:17	FedericoFerri
eps	lumi_401000_EELinear_0_log.eps	r1	manage	199.9 K	2013-10-10 - 05:17	FedericoFerri
pdf	lumi_401000_EELinear_0_log.pdf	r1	manage	46.7 K	2013-10-10 - 05:17	FedericoFerri
png	lumi_401000_EELinear_0_log.png	r1	manage	173.1 K	2013-10-10 - 05:17	FedericoFerri
eps	lumi_403000_EELinear_0_log.eps	r1	manage	195.8 K	2013-10-10 - 05:21	FedericoFerri
pdf	lumi_403000_EELinear_0_log.pdf	r1	manage	46.9 K	2013-10-10 - 05:21	FedericoFerri
png	lumi_403000_EELinear_0_log.png	r1	manage	172.4 K	2013-10-10 - 05:17	FedericoFerri

Topic revision: r14 - 2013-10-11 - FedericoFerri

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