Properties of the Higgs-like boson in the decay H → ZZ → 4l in pp collisions at √s = 7 and 8 TeV

Table of contents:

Abstract

The properties of the new boson with the mass around 125 GeV are reported. The boson is observed in the search for the standard model Higgs boson in the mass range110 < mH < 1000 GeV in the H → ZZ decay channel. The search considers final states where both Z's decay to electron, muon, or tau lepton pairs. The analysis uses pp collision data recorded by the CMS detector at the LHC, corresponding to integrated luminosities of 5.1 fb-1 at √s = 7 TeV and 19.6 fb-1 at √s = 8 TeV. It makes use of the measured four-lepton mass, the mass uncertainty, kinematic discriminants, and information sensitive to the production mechanism, such as associated dijet characteristics and transverse momentum of the four-lepton system. The boson is observed in channels with electron and muon pairs with a local significance above the expected background of 6.7 standard deviations with the mass 125.8 0.5(stat.) 0.2(syst.) GeV. The signal strength μ, relative to the expectation for the standard model Higgs boson, is measured to be μ = 0.91+0.30-0.24. The signal strength modifiers associated with vector bosons and fermions in production are measured to be μV = 1.0+2.4-2.3 and μF = 0.9+0.5-0.4, thus consistent with the standard model expectations. The spin-parity of the boson is studied and the pure scalar hypothesis is found to be consistent with the observation when compared to six other spin-parity hypotheses. The data disfavour the pure pseudoscalar hypothesis 0- with a CLs value of 0.16%, and disfavour the pure spin-2 hypothesis of a narrow resonance with the minimal couplings to the vector bosons with a CLs value of 1.5%. The spin-1 hypotheses are disfavoured with an even higher confidence. No other significant standard model Higgs-like excess is found in the search and upper limits at 95\% confidence level exclude the range 130-827 GeV.

4l plots

Mass plots

Animation Description

Linked version : gif
Slower version : gif
Evolution in 2011 and 2012 data of distribution of the four-lepton reconstructed mass in full mass range for the sum of the 4e, 4μ, and 2e2μ channels. Points represent the data, shaded histograms represent the background and unshaded histogram the signal expectations. The expected distributions are presented as stacked histograms.
Figure Description
Distribution of the four-lepton reconstructed mass in full mass range for the sum of the 4e, 4μ, and 2e2μ channels. Points represent the data, shaded histograms represent the background and unshaded histogram the signal expectations. The expected distributions are presented as stacked histograms. The measurements are presented for the sum of the data collected at √s = 7 TeV and √s = 8 TeV. [70-180] GeV range - 3 GeV bin width

No KD cut : eps,png
KD > 0.3 : eps,png
KD > 0.5 : eps,png
Distribution of the four-lepton reconstructed mass in full mass range for the sum of the 4e, 4μ, and 2e2μ channels. Points represent the data, shaded histograms represent the background and unshaded histogram the signal expectations. The expected distributions are presented as stacked histograms. The measurements are presented for the sum of the data collected at √s = 7 TeV and √s = 8 TeV. [100-180] GeV range - 3 GeV bin width

No KD cut : pdf,png
No KD cut + ideogram : pdf,png
KD > 0.3 : pdf,png
KD > 0.5 : pdf,png
Distribution of the four-lepton reconstructed mass in full mass range for the sum of the 4e, 4μ, and 2e2μ channels. Points represent the data, shaded histograms represent the background and unshaded histogram the signal expectations. The expected distributions are presented as stacked histograms. The measurements are presented for the sum of the data collected at √s = 7 TeV and √s = 8 TeV. [100-180] GeV range - 3 GeV bin width. Also shown are the central values and individual candidate mass measurement uncertainties.
Distribution of the four-lepton reconstructed mass in full mass range for the sum of the 4e, 4μ, and 2e2μ channels. Points represent the data, shaded histograms represent the background and unshaded histogram the signal expectations. The expected distributions are presented as stacked histograms. The measurements are presented for the sum of the data collected at √s = 7 TeV and √s = 8 TeV. [70-1000] GeV range - 3 GeV bin width
Distribution of the four-lepton reconstructed mass in full mass range for the sum of the 4e, 4μ, and 2e2μ channels. Points represent the data, shaded histograms represent the background and unshaded histogram the signal expectations. The expected distributions are presented as stacked histograms. The measurements are presented for the sum of the data collected at √s = 7 TeV and √s = 8 TeV. [70-600] GeV range - 10 GeV bin width
Distribution of the four-lepton reconstructed mass in full mass range for the sum of the 4e, 4μ, and 2e2μ channels. Points represent the data, shaded histograms represent the background and unshaded histogram the signal expectations. The expected distributions are presented as stacked histograms. The measurements are presented for the sum of the data collected at √s = 7 TeV and √s = 8 TeV. [70-800] GeV range - 10 GeV bin width

untagged: eps,pdf,png
di-jet tagged eps,pdf,png
Distribution of the four-lepton reconstructed mass in full mass range for the sum of the 4e, 4μ, and 2e2μ channels, for the untagged category (left) and di-jet tagged category (right). Points represent the data, shaded histograms represent the background and unshaded histogram the signal expectations. The expected distributions are presented as stacked histograms. The measurements are presented for the sum of the data collected at √s = 7 TeV and √s = 8 TeV. [100-160] GeV range - 3 GeV bin width
Distribution of the Z1 reconstructed mass for the sum of the 4e, 4μ, and 2e2μ channels for events with the four-lepton reconstructed mass > 100 GeV. Points represent the data, shaded histograms represent the background and unshaded histogram the signal expectations. The measurements are presented for the sum of the data collected at √s = 7 TeV and √s = 8 TeV.
Distribution of the Z2 reconstructed mass for the sum of the 4e, 4μ, and 2e2μ channels for events with the four-lepton reconstructed mass > 100 GeV. Points represent the data, shaded histograms represent the background and unshaded histogram the signal expectations. The measurements are presented for the sum of the data collected at √s = 7 TeV and √s = 8 TeV.
Distribution of the Kinematical Discriminant (KD) of the four-lepton candidates in [100-180] GeV mass range for the sum of the 4e, 4μ, and 2e2μ channels. Points represent the data, shaded histograms represent the background and unshaded histogram the signal expectations. The measurements are presented for the sum of the data collected at √s = 7 TeV and √s = 8 TeV.

Distributions with 121.5 < m4l < 130.5 GeV

Figure Description
Distribution of the Z1 reconstructed mass of the four-lepton candidates in [121.5-130.5] GeV mass range for the sum of the 4e, 4μ, and 2e2μ channels. Points represent the data, shaded histograms represent the background and unshaded histogram the signal expectations. The measurements are presented for the sum of the data collected at √s = 7 TeV and √s = 8 TeV.
Distribution of the Z2 reconstructed mass of the four-lepton candidates in [121.5-130.5] GeV mass range for the sum of the 4e, 4μ, and 2e2μ channels. Points represent the data, shaded histograms represent the background and unshaded histogram the signal expectations. The measurements are presented for the sum of the data collected at √s = 7 TeV and √s = 8 TeV.
Distribution of the Kinematic Discriminant (KD) of the four-lepton candidates in [121.5-130.5] GeV mass range for the sum of the 4e, 4μ, and 2e2μ channels. Points represent the data, shaded histograms represent the background and unshaded histogram the signal expectations. The measurements are presented for the sum of the data collected at √s = 7 TeV and √s = 8 TeV.
Distribution of the number of jets in [121.5-130.5] GeV mass range for the sum of the 4e, 4μ, and 2e2μ channels. Points represent the data, shaded histograms represent the background and unshaded histogram the signal expectations. The measurements are presented for the sum of the data collected at √s = 7 TeV and √s = 8 TeV.
Distribution of the pT/m4l in untagged category in [121.5-130.5] GeV mass range for the sum of the 4e, 4μ, and 2e2μ channels. Points represent the data, shaded histograms represent the background and unshaded histogram the signal expectations. The measurements are presented for the sum of the data collected at √s = 7 TeV and √s = 8 TeV.
Distribution of the VBF discriminant in di-jet tagged category in [121.5-130.5] GeV mass range for the sum of the 4e, 4μ, and 2e2μ channels. Points represent the data, shaded histograms represent the background and unshaded histogram the signal expectations. The measurements are presented for the sum of the data collected at √s = 7 TeV and √s = 8 TeV.
Distribution of the reconstructed mass of the second lepton pair (MZ2) versus the reconstructed mass of the first lepton pair (MZ1) for the 4e, 4μ, and 2e2μ final states. Shaded histograms represent the expectations for a signal with mH=126 GeV.The measurements are presented for the sum of the data collected at √s = 7 TeV and √s = 8 TeV.

Kinematic Discriminan vs. m4l

Figure Description
Distribution of the kinematic discriminant KD versus the four-lepton reconstructed mass m4l in the low-mass range [100-180] GeV. The points representing the individual events are shown together with their reconstructed mass uncertainties. The contours represent the background expectation.
Distribution of the kinematic discriminant KD versus the four-lepton reconstructed mass m4l in the low-mass range [180-800] GeV. The points representing the individual events are shown together with their reconstructed mass uncertainties. The contours represent the background expectation.
Distribution of the kinematic discriminant KD versus the four-lepton reconstructed mass m4l in the low-mass range [100-180] GeV. The points representing the individual events are shown together with their reconstructed mass uncertainties. The contours represent the signal expectation (mH = 126 GeV).

Background Control

Figure Description

electron fakes: eps,pdf,png
muon fakes: eps,pdf,png
Left: Probability for a reconstructed electron to pass identification and isolation requirements (electron fake ratios), as measured in the Z(ll)+e_reco sample in data, for electrons in barrel (blue) or end caps (red). Right: Probability for a reconstructed muon to pass identification and isolation requirements (muon fake ratios), as measured in the Z(ll)+μ_reco sample in data, for muons in barrel (blue) or end caps (red). The distributions correspond to 19.6 fb−1 of the 8 TeV data.
Invariant mass distribution of events in the control region 2 Prompt +2 Fakes leptons (2P+2F) for the sum of the 4e, 4μ, and 2e2μ channels. The distributions are fitted with the F(x) = Landau(x) x P4(x) function. The distributions correspond to 19.6 fb−1 of the 8 TeV data.
Invariant mass distribution of events in the control region 3 Prompt+1 Fake leptons (3P+1F) for the sum of 4e, 4μ and 2e2μ channels. Distribution of the 2 Prompt +2 Fakes leptons (2P+2F) reducible background (Z+X, ttbar) is estimated from data and is stacked on top of distribution of the irreducible background taken from simulation (ZZ → 4l). The difference of the sum of these distributions with respect to the distribution of observed events is due to contributions from 3P+1F reducible background processes (predominantly Z+gamma events with asymmetric gamma conversion) . This contribution is then properly weighted to estimate the expected 3P+1F events in the signal region. The distributions correspond to 19.6 fb−1 of the 8 TeV data.

SS: pdf,png
OS: pdf,png
Closure tests of the AA method to estimate the reducible background, using same-sign leptons (left) and opposite-sign opposite flavor leptons (right). The dots show the invariant four-lepton mass distribution for the 2012 data. The expectation from Z plus two fake leptons as predicted by method AA is shown by the green histogram. Also shown are the contributions from ZZ events (blue histogram), and from WZ and tt ̄Z production (yellow histogram).

P-values

Figure Description

low mass: eps,png
whole mass eps,png
Significance of the local excess with respect to the standard model background expectation as a function of the Higgs boson mass for the 1D (m4l), 2D (m4l, KD) and 3D (m4l, KD, pT/m4l or VD) models. The results are shown for the full data sample in the range [110-180] GeV (left) and [110-1000] GeV (right) for the sum of the 4e, 4μ, and 2e2μ channels.

low mass: eps,png
whole mass eps,png
Significance of the local excess with respect to the standard model background expectation as a function of the Higgs boson mass for the 7 TeV (red), 8 TeV (blue) and 7 TeV + 8 TeV (black) datasample. The results are shown for the full data sample in the range [110-180] GeV (left) and [110-1000] GeV (right) for the sum of the 4e, 4μ, and 2e2μ channels.

low mass: eps,png
whole mass eps,png
Significance of the local excess with respect to the standard model background expectation as a function of the Higgs boson mass for the di-jet tagged category (green), untagged category (blue) and whole analysis (black). The results are shown for the full data sample in the range [110-180] GeV (left) and [110-1000] GeV (right) for the sum of the 4e, 4μ, and 2e2μ channels.

low mass: eps,png
whole mass eps,png
whole mass + 2l2τ : eps,png
Significance of the local excess with respect to the standard model background expectation as a function of the Higgs boson mass for inclusive analysis. The results are shown for the full data sample in the range [110-180] GeV (left) and [110-1000] GeV (right) for the sum of the 4e, 4μ, and 2e2μ channels.

Signal Strength

Figure Description
Values of μ = σ/σSM for the two categories. The vertical line shows the combined μ, together with its associated 1σ uncertainties shown as green band. The horizonthal bars indicate the 1σ uncertainties on μ for the different categories. The uncertainties include both statistical and systematic sources.

Limits (4l + 2l2tau)

Figure Description

low mass: eps,pdf,png
high mass eps,pdf,png
Expected and observed 95% confidence level limits for a standard model Higgs boson, with mass in the range [110-180] GeV (left) and [110-1000] GeV (right), decaying via ZZ to 4e, 4μ, 2e2μ, 2e2τ, or 2μ2τ. The green band represents the expected limit ± one standard deviation and the yellow band represents the expected limit ± two standard deviations band.

Mass measurement

Figure Description
1D test statistics q(mH)=−2∆lnL scan vs hypothesized Higgs boson mass mH, 68% CL obtained from the 3D test statistics profiling the minimum of the signal strengths, with and without systematics.
1D test statistics q(mH)=−2∆lnL scan vs hypothesized Higgs boson mass mH, 68% CL obtained from the 1D (dotted red), 2D (solid blue), and 3D (solid pink) test statistics profiling the minimum of the signal strengths, with and without systematics.
1D test statistics q(mH)=−2∆lnL scan vs hypothesized Higgs boson mass mH, 68% CL obtained from the 3D test statistics profiling the minimum of the signal strengths, with systematics.
m(4e) = 127.0 -2.3/+1.9 GeV
m(4μ)=125.2 -0.6/+0.5 GeV
m(2e2μ)=127.2 -0.8/+0.8 GeV
Likelihood scan of the mass of the Z boson from Z→4L decays separated by channel and combined. The fit follows the same procedure as the H→ZZ→4L likelihood scan, except in the case of Z→4L, the fit does not use the Higgs-vs-ZZ kinematic discriminant and per-event four-lepton mass uncertainties. The assumed Z boson width is 2.50 GeV. The gray dashed line represents the PDG value of Z boson mass of 91.188 GeV. The horizontal lines at -2Δ ln(L) equal to 1.0 and 3.8 represent the 68% and 95% confidence levels respectively. Results of the fits are as follows:
m(4l) = 91.17 +/- 0.22 GeV
m(4e) = 91.80 +/- 0.80 GeV
m(4μ) = 91.01 +/- 0.27 GeV
m(2e2μ) = 91.43 +/- 0.43 GeV

Production Mechanism

Figure Description

ggH: png,eps
qqH: png,eps
background: png,eps
Distribution of the pT/m4l versus the four-lepton reconstructed mass m4l for 2011 and 2012 data combined. Circles are 4μ events, triangles 4e events and squares 2e2μ events. Event-by-event errors is attached to each event. Low-mass range with contours for ggH signal expectation with mH = 126 GeV (left), with contours for qqH signal expectation with mH = 126 GeV (center), and with contours for background expectation (right).

ggH: png,eps
qqH: png,eps
background: png,eps
Distribution of the Fisher Discriminant versus the four-lepton reconstructed mass m4l for 2011 and 2012 data combined. Circles are 4μ events, triangles 4e events and squares 2e2μ events. Event-by-event errors is attached to each event. Low-mass range with contours for ggH signal expectation with mH = 126 GeV (left), with contours for qqH signal expectation with mH = 126 GeV (center), and with contours for background expectation (right).
Likelihood contours on the signal strength modifiers associated with fermions (μF) and vector bosons (μV) shown at 68% and 95% CL.

JP

Figure Description
Distributions of Dbkg in data and MC expectations for background and signal resonance consistent with SM Higgs boson at mH = 126 GeV.

without Dbkg: eps,pdf,png
with Dbkg: eps,pdf,png
Distributions of DJP without (left) and with (right) a requirement Dbkg > 0.5. Distributions in data (points with error bars) and expectations for background and signal are shown. The alternative hypothesis tested is JP = 0-

without Dbkg: eps,pdf,png
with Dbkg: eps,pdf,png
Distributions of DJP without (left) and with (right) a requirement Dbkg > 0.5. Distributions in data (points with error bars) and expectations for background and signal are shown. The alternative hypothesis tested is JP = 0+h

without Dbkg: eps,pdf,png
with Dbkg: eps,pdf,png
Distributions of DJP without (left) and with (right) a requirement Dbkg > 0.5. Distributions in data (points with error bars) and expectations for background and signal are shown. The alternative hypothesis tested is JP = 1+

without Dbkg: eps,pdf,png
with Dbkg: eps,pdf,png
Distributions of DJP without (left) and with (right) a requirement Dbkg > 0.5. Distributions in data (points with error bars) and expectations for background and signal are shown. The alternative hypothesis tested is JP = 1-

without Dbkg: eps,pdf,png
with Dbkg: eps,pdf,png
Distributions of DJP without (left) and with (right) a requirement Dbkg > 0.5. Distributions in data (points with error bars) and expectations for background and signal are shown. The alternative hypothesis tested is JP = 2+gg

without Dbkg: eps,pdf,png
with Dbkg: eps,pdf,png
Distributions of DJP without (left) and with (right) a requirement Dbkg > 0.5. Distributions in data (points with error bars) and expectations for background and signal are shown. The alternative hypothesis tested is JP = 2+qq



mZ1 -- with Dbkg cut: eps,pdf,png / without Dbkg cut: eps,pdf,png
mZ1 -- with Dbkg cut: eps,pdf,png / without Dbkg cut: eps,pdf,png
costhetastar -- with Dbkg cut: eps,pdf,png / without Dbkg cut: eps,pdf,png
costheta1 -- with Dbkg cut: eps,pdf,png / without Dbkg cut: eps,pdf,png
costheta2 -- with Dbkg cut: eps,pdf,png / without Dbkg cut: eps,pdf,png
phi -- with Dbkg cut: eps,pdf,png / without Dbkg cut: eps,pdf,png
phi1 -- with Dbkg cut: eps,pdf,png / without Dbkg cut: eps,pdf,png
Distributions of mZ1, mZ2, costhetastar, costheta1, costheta2, phi1, and phi variables with and without a requirement Dbkg > 0.5 . Distributions in data (points with error bars) and expectations for background, signal, and the alternative hypothesis tested JP = 0- are shown

JP = 0−: signal png,eps,pdf - alt. hyp. png,eps,pdf - back. png,eps,pdf
JP = 0+h: signal png,eps,pdf - alt. hyp. png,eps,pdf - back. png,eps,pdf
JP = 1+: signal png,eps,pdf - alt. hyp. png,eps,pdf - back. png,eps,pdf
JP = 1-: signal png,eps,pdf - alt. hyp. png,eps,pdf - back. png,eps,pdf
JP = 2+qq: signal png,eps,pdf - alt. hyp. png,eps,pdf - back. png,eps,pdf
JP = 2+gg;: signal png,eps,pdf - alt. hyp. png,eps,pdf - back. png,eps,pdf
Distribution of the DJP versus the Dbkg for 2011 and 2012 data combined. Circles are 4μ events, triangles 4e events and squares 2e2μ events. Superimposed are the contours for ggH signal expectation with mH = 126 GeV (left), the contours for alternative hypothesis tested (center), and the contours for background expectation (right).

D1+ vs D1-: png,eps
D1+ vs D2+qq: png,eps
D2+gg vs D2+qq: png,eps
Correlation between two DJP with a requirement Dbkg > 0.5: D1+ vs D1- (left), D1+ vs D2+qq (center), and D1+ vs D2+qq (right). Distributions of data (points) and expectations for signal are shown.



JP = 0−: eps,pdf,png
JP = 0+h: eps,pdf,png
JP = 1+: eps,pdf,png
JP = 1-: eps,pdf,png
JP = 2+mgg: eps,pdf,png
JP = 2+mqq: eps,pdf,png
Distribution of q = −2ln(LJP/LSM) for two signal types (0+ histogram to the right and JP histogram to the left) for mH = 126 GeV shown with a large number of generated experiments. The arrow indicates the observed value. Six alternative hypotheses are tested from top to bottom and left to right: JP = 0−, 0+h , 1+, 1-, 2+mgg, 2+mqq ̄.

−2lnL as a function of fa3 : png,pdf,eps
−2lnL as a function of fa3 and μ: png,pdf,eps
Average expected and observed distribution of −2lnL as a function of fa3 (left) and as a function of fa3 and μ (right).

Leptons

Figure Description
Expected resolution for prompt and isolated electrons in the ECAL barrel as a function of the initial electron energy from the ECAL, the tracker and the combined estimates. The resolution is evaluated as half the minimal width that contains 68.3% of the reconstructed energy or momentum distribution (effective resolution) or using a Gaussian fit of the core of the momentum distribution.

√s = 8 TeV: pdf,png
√s = 7 TeV: pdf,png
Relative difference between the dielectron mass scales in data and simulation for Z → e+e−, J/Ψ and Υ events as a function of the electron transverse momentum and for different pseudorapidity regions. Results are presented for data collected at √s = 8 TeV (left) and at √s = 7 TeV (right).
Instrumental dielectron effective resolution as measured from Z → e+e− events and compared to simulation. Events are categorized according to the electron class and pseudorapidity region of each leg (G1: electron golden or bigbrem, G2: electron showering or crack or badtrack, EB: electron in ECAL barrel, EE: electron in ECAL endcaps). Results are presented for data collected at √s = 8 TeV.

ECAL barrel and non-showering: pdf,png
ECAL endcaps and showering: pdf,png
Dielectron mass distribution from Z → ee events in data and simulation for cases with both electrons in ECAL barrel and non-showering (best category, left) and with both electrons in ECAL endcaps and showering (worst category, right). Blue points are 2012 data (19.6 fb-1) with a fit superimposed (blue line). Open circles is MC with a fit superimposed (red line). Fit was done with a convolution of the Breit-Wigner and Crystal Ball functions. The central value and width of the Breit-Wigner function are fixed to PDG values. The Crystal Ball parameters are free in the fit.
Expected four-lepton mass distribution (4e case) with/without correcting for the scale shift observed between data and simulation as a function of electron pT, η, and class. Fits are done with double Crystal Ball and systematics on the mean extracted. A systematic uncertainty of 0.3% (0.1%) in the 4e (2e2mu) channel is extracted from the difference between the peak positions.

J/Psi: pdf,png
Y(1S)/Y(2S+3S): pdf,png
J/Psi->e+e- reconstructed in barrel with one electron with 7<pT<10 GeV (left). Y(1S) and not resolved Y(2S+3S) reconstructed in ECAL barrel with one electron with 10<pT<15 1GeV (right).
Relative difference between the dielectron mass scales in data and simulation for Z → e+e− events as a function of the number of vertices.

4e channel: png,pdf
4μ channel: png,pdf
2e2μ channel: png,pdf
Expected four-lepton mass distribution for H→ZZ→4e (left), H→ZZ→4μ (middle) and H→ZZ→2e2μ (right) and for mH = 126 GeV. The distributions are fitted with a double-sided Crystal Ball function and the fitted values of the Crystall Ball sigmas are indicated. The values of effective RMS defined as half the smallest width that contains 68.3% of the distribution are also indicated.

4e channel: pdf,png
4μ channel: pdf,png
Expected four-lepton mass distribution for H→ZZ→4e (left) and H→ZZ→2e2μ (right) and for mH = 126 GeV without (black) and with (blue-green) energy regression. The distributions are fitted with a double-sided Crystal Ball function and the fitted values of the Crystall Ball sigmas are indicated. The values of effective RMS defined as half the smallest width that contains 68.3% of the distribution are also indicated.

μ scales: pT pdf,png η pdf,png
μ resolutions: pT pdf,png η pdf,png
Relative difference between the di-muon mass scales (left) and resolutions (right) in data and simulation extracted from J/Ψ, Υ and Z decays, as function of the average muon pT (left) and η (right) for the 2012 data. The uncertainties shown are statistical only.

versus pT: pdf,png
versus abs(η): pdf,png
Expected resolution for prompt muons as a function of pT (left) and abs(η) (right). Events are from a simulate Higgs sample (mH = 126 GeV). The resolution is defined as the sigma of double Crystal Ball function that describes the reconstructed pT distribution around the true pT.

J/ψ → μμ in barrel: pdf,png
J/ψ→ μμ in endcap: pdf,png
Example fits of the dimuon lineshape in 2012 data for the J/Ψ resonances in the bins of average muon pT and η specified in the figures. The fits are done with a single CB and a polynomial background.

Υ(1S,2S,3S) → μμ in barrel: pdf,png
Υ(1S,2S,3S)→μμ in endcap: pdf,png
Example fits of the dimuon lineshape in 2012 data for the Υ(1S,2S,3S) resonances in the bins of average muon pT and η specified in the figures. The fits are done with a single CB and a polynomial background. For the three CB's for the Upsilons, the mass difference is fixed to the PDG, and the σ(M)/M is the same for all three.

Z→ μμ in barrel: pdf,png
Example fits of the dimuon lineshape in 2012 data for the Z resonance in the bins of average muon pT and η specified in the figures. The fits are done with a single CB and an exponential background.


barrel : png,pdf


endcap : png,pdf

Tag-and-probe results for the muon reconstruction and identification efficiency in data (black dots) compared to simulation (blue shaded histograms). Given that a tracker track exists, the plot show the efficiency as a function of the muon pT in the barrel or endcaps. The measurements is made using J/ψ →μ+μ- events for pT<15 GeV and Z→μ+μ- events for pT>15 GeV. The uncertainties on the fitted efficiency is determined from the likelihood function. As normalizations of signal and background, efficiency of the background, and parameters controlling the shapes of the signal and background are all parameters of the fit, the uncertainty includes, in addition to the statistical contribution, those from the background subtraction procedure.


versus η : png,pdf

Tag-and-probe results for identified muons to pass the significance of the impact parameter cut (SIP < 4.0) in data (black dots) compared to simulation (blue shaded histograms). Given that a tracker track exists, the plot show the efficiency as a function of the muon pT in the barrel or endcaps. The measurements is made using Z→μ+μ- events. The uncertainties on the fitted efficiency is determined from the likelihood function. As normalizations of signal and background, efficiency of the background, and parameters controlling the shapes of the signal and background are all parameters of the fit, the uncertainty includes, in addition to the statistical contribution, those from the background subtraction procedure.


barrel : png,pdf


endcap : png,pdf

Tag-and-probe results for the isolation efficiency of identified muons passing the SIP cut in data (black dots) compared to simulation (blue shaded histograms). The muons are required to have a relative isolation smaller than 0.4. The effect of pile-up on the isolation is corrected using the "Effective Area" method. Given an identified muon, the plot show the efficiency as a function of the muon pT in the barrel or endcaps. The measurements is made using Z→μ+μ- events for the whole pT range. The uncertainties on the fitted efficiency is determined from the likelihood function. As normalizations of signal and background, efficiency of the background, and parameters controlling the shapes of the signal and background are all parameters of the fit, the uncertainty includes, in addition to the statistical contribution, those from the background subtraction procedure.


barrel : png,pdf

Tag-and-probe results for the isolation efficiency of identified muons passing the SIP cut in data (black dots) compared to simulation (blue shaded histograms). The muons are required to have a relative isolation smaller than 0.4. The effect of pile-up on the isolation is corrected using the "Effective Area" method. Given an identified muon, the plot show the efficiency as a function of the muon pT in the barrel or endcaps. The measurements is made using Z→μ+μ- events for the whole pT range. The uncertainties on the fitted efficiency is determined from the likelihood function. As normalizations of signal and background, efficiency of the background, and parameters controlling the shapes of the signal and background are all parameters of the fit, the uncertainty includes, in addition to the statistical contribution, those from the background subtraction procedure.


di-muon: pdf,png
di-electron: pdf,png
Comparison between the resolution as predicted from the per-lepton uncertainties and the resolution measured from di-lepton mass fit for di-muon (left) and di-electron (right) for data (closed symbols) and simulation (open symbols). The dotted lines indicate a deviation of 20%. The presented measurement corresponds to the data collected at √s = 8 TeV.
Relative mass error distribution in the data and compared to simulation for events in a Z → 4l control region (80 < m4l < 100 GeV). The three final states, 4e, 4μ, and 2e2μ, are added together. Results correspond to the data collected at √s = 7 TeV and √s = 8 TeV.
Four-lepton mass distribution in the mass range 50 < m4l < 110 GeV. Data are shown with points. The three final states, 4e, 4μ, and 2e2μ, are added together. The solid line represents an overlay of the best fit as obtained using the same technique as for the mass measurement of the new boson. Expectation from simulation is shown by the colored histograms. Results correspond to the data collected at √s = 7 TeV and √s = 8 TeV.

Tables

Table Description
The number of event candidates observed, compared to the mean expected back- ground and signal rates for each final state. For the Z +X background, the estimates are based on data. The results are given integrated over the full mass measurement range for the SM-like Higgs boson search from 100 to 1000 GeV and for 2011 and 2012 data combined.
The number of event candidates observed, compared to the mean expected back- ground and signal rates for each final state. For the Z +X background, the estimates are based on data. The results are given integrated in the mass range from 110 to 160 GeV.
List of models used in analysis of spin-parity hypotheses corresponding to the pure states of the type noted. The expected separation is quoted for two scenarios, when the sig- nal strength for each hypothesis is pre-determined from the fit to data and when events are generated with SM expectation for the signal yield (μ=1). The observed separation quotes con- sistency of the observation with JP model or the 0+ model, and corresponds to the scenario when the signal strength is pre-determined from the fit to data. The last column quotes CLs criterion.

2l2tau plots

Mass Plots

Figure Label Description
png,pdf The four-lepton reconstructed mass summed for all $\tau$ final states. The data corresponds to an integrated luminosity of 5.1 \fbinv at 7 TeV and 19.3 \fbinv at 8 TeV. The backgrounds are presented as stacked histograms. The background shapes are taken from MC simulation and normalized to the values obtained using the data-driven techniques described in the text. The expected mass distributions for the SM Higgs boson with a mass 350 GeV are also shown for comparison.

Z1 vs Z2 Mass plot

Figure Label Description
png,pdf Distribution of the Z2 reconstructed mass versus the Z1 reconstructed mass of the four-lepton candidates in full mass range for the the all 2l2tau channels. Black points represent the data events selected at √s = 8 TeV, and Red square represent the data events selected at √s = 7 TeV.

Limit Plot

Figure Label Description
png,pdf The expected and observed 95\% CL upper limits on the product of the production cross section and decay branching ratio for a Higgs boson normalized to the SM expectation as a function of $m_{\rm H}$, using data corresponding to integrated luminosity of 5.1 \fbinv at 7 TeV and 19.3 \fbinv at 8 TeV.

Cut Flow Plots

Figure Label Description
png,pdf Cut Flow data-to-MC comparison for eett final state using data collected at √s = 8 TeV.
png,pdf Cut Flow data-to-MC comparison for mmtt final state using data collected at √s = 8 TeV.

Background Control Region plots

Figure Label Description
png,pdf Data to MC comparison in the same sign control region for eett final state at √s = 8 TeV.
png,pdf Data to MC comparison in the same sign control region for mmtt final state at √s = 8 TeV

Figure Label Description
png,pdf Data to MC comparison of jet to tau fake rate for Medium Isolation working point at √s = 8 TeV.
png,pdf Data to MC comparison of jet to tau fake rate for Tight Isolation working point at √s = 8 TeV.

Figure Label Description
png,pdf Data to MC comparison of electron isolation, Leading electron from leading Z in eett final state after relaxing the isolation from both taus at √s = 8 TeV.

png,pdf Data to MC comparison of electron isolation, Leading electron from leading Z in mmtt final state after relaxing the isolation from both taus at √s = 8 TeV.
Topic attachments
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PDFpdf KD_2mplus_qqbar_Proj_superKDcut.pdf r1 manage 16.4 K 2013-02-26 - 11:55 RobertoSalerno  
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PDFpdf KD_phi_jhuGenV2PseH126_Proj.pdf r1 manage 15.5 K 2013-03-05 - 14:57 RobertoSalerno  
PNGpng KD_phi_jhuGenV2PseH126_Proj.png r1 manage 12.1 K 2013-03-05 - 14:53 RobertoSalerno  
Unknown file formateps KD_phi_jhuGenV2PseH126_Proj_superKDcut.eps r1 manage 19.2 K 2013-03-05 - 14:57 RobertoSalerno  
PDFpdf KD_phi_jhuGenV2PseH126_Proj_superKDcut.pdf r1 manage 15.5 K 2013-03-05 - 14:57 RobertoSalerno  
PNGpng KD_phi_jhuGenV2PseH126_Proj_superKDcut.png r1 manage 11.5 K 2013-03-05 - 14:53 RobertoSalerno  
Unknown file formateps KD_superKD_Proj.eps r1 manage 21.6 K 2013-02-26 - 12:39 RobertoSalerno  
PDFpdf KD_superKD_Proj.pdf r1 manage 16.5 K 2013-02-26 - 12:39 RobertoSalerno  
PNGpng KD_superKD_Proj.png r1 manage 13.3 K 2013-02-26 - 12:39 RobertoSalerno  
Unknown file formateps KD_z1mass_jhuGenV2PseH126_Proj.eps r1 manage 21.6 K 2013-03-05 - 14:57 RobertoSalerno  
PDFpdf KD_z1mass_jhuGenV2PseH126_Proj.pdf r1 manage 16.3 K 2013-03-05 - 14:57 RobertoSalerno  
PNGpng KD_z1mass_jhuGenV2PseH126_Proj.png r1 manage 13.8 K 2013-03-05 - 14:53 RobertoSalerno  
Unknown file formateps KD_z1mass_jhuGenV2PseH126_Proj_superKDcut.eps r1 manage 21.2 K 2013-03-05 - 14:57 RobertoSalerno  
PDFpdf KD_z1mass_jhuGenV2PseH126_Proj_superKDcut.pdf r1 manage 16.1 K 2013-03-05 - 14:57 RobertoSalerno  
PNGpng KD_z1mass_jhuGenV2PseH126_Proj_superKDcut.png r1 manage 12.9 K 2013-03-05 - 14:53 RobertoSalerno  
Unknown file formateps KD_z2mass_jhuGenV2PseH126_Proj.eps r1 manage 20.5 K 2013-03-05 - 14:55 RobertoSalerno  
PDFpdf KD_z2mass_jhuGenV2PseH126_Proj.pdf r1 manage 16.0 K 2013-03-05 - 14:55 RobertoSalerno  
PNGpng KD_z2mass_jhuGenV2PseH126_Proj.png r1 manage 13.8 K 2013-03-05 - 14:53 RobertoSalerno  
Unknown file formateps KD_z2mass_jhuGenV2PseH126_Proj_superKDcut.eps r1 manage 20.0 K 2013-03-05 - 14:55 RobertoSalerno  
PDFpdf KD_z2mass_jhuGenV2PseH126_Proj_superKDcut.pdf r1 manage 15.8 K 2013-03-05 - 14:55 RobertoSalerno  
PNGpng KD_z2mass_jhuGenV2PseH126_Proj_superKDcut.png r1 manage 12.1 K 2013-03-05 - 14:53 RobertoSalerno  
Unknown file formateps LD_100_180.eps r1 manage 22.6 K 2013-03-04 - 16:16 RobertoSalerno  
PNGpng LD_100_180.png r1 manage 16.4 K 2013-03-04 - 16:16 RobertoSalerno  
PDFpdf LimitPlot_8TeV_7TeV_full_Mass.pdf r1 manage 16.1 K 2013-03-04 - 10:28 RamanKhurana  
PNGpng LimitPlot_8TeV_7TeV_full_Mass.png r2 r1 manage 18.0 K 2013-03-04 - 12:21 RamanKhurana  
Unknown file formateps MZ1.eps r1 manage 17.7 K 2013-03-04 - 17:10 RobertoSalerno  
PDFpdf MZ1.pdf r1 manage 27.3 K 2013-03-04 - 17:10 RobertoSalerno  
PNGpng MZ1.png r1 manage 89.4 K 2013-03-04 - 17:10 RobertoSalerno  
PDFpdf MZ1VSMZ2.pdf r4 r3 r2 r1 manage 22.4 K 2013-03-06 - 14:05 RobertoSalerno  
PNGpng MZ1VSMZ2.png r4 r3 r2 r1 manage 20.5 K 2013-03-06 - 14:05 RobertoSalerno  
Unknown file formateps MZ2.eps r1 manage 20.2 K 2013-03-04 - 17:10 RobertoSalerno  
PDFpdf MZ2.pdf r1 manage 28.5 K 2013-03-04 - 17:11 RobertoSalerno  
PNGpng MZ2.png r1 manage 93.5 K 2013-03-04 - 17:11 RobertoSalerno  
PDFpdf MassResolution_Zee_aftercorrection.pdf r1 manage 14.3 K 2013-03-04 - 12:46 RobertoSalerno  
PNGpng MassResolution_Zee_aftercorrection.png r1 manage 27.3 K 2013-03-04 - 12:46 RobertoSalerno  
PDFpdf MassResolution_Zmm_aftercorrection.pdf r1 manage 14.3 K 2013-03-04 - 12:46 RobertoSalerno  
PNGpng MassResolution_Zmm_aftercorrection.png r1 manage 27.1 K 2013-03-04 - 12:46 RobertoSalerno  
PDFpdf MeettNoIso.pdf r1 manage 16.5 K 2013-03-04 - 10:28 RamanKhurana  
PDFpdf MmmttNoIso.pdf r1 manage 16.5 K 2013-03-04 - 10:28 RamanKhurana  
PDFpdf Moriond13_RedBack_AA_Closure_OSOF.pdf r1 manage 43.4 K 2013-03-06 - 00:10 RobertoSalerno  
PNGpng Moriond13_RedBack_AA_Closure_OSOF.png r1 manage 48.6 K 2013-03-06 - 00:10 RobertoSalerno  
PDFpdf Moriond13_RedBack_AA_Closure_SSSF.pdf r1 manage 40.3 K 2013-03-06 - 00:10 RobertoSalerno  
PNGpng Moriond13_RedBack_AA_Closure_SSSF.png r1 manage 45.4 K 2013-03-06 - 00:10 RobertoSalerno  
Unknown file formateps Ptm_lowMass_bkg.eps r1 manage 38.7 K 2013-03-04 - 18:00 RobertoSalerno  
PNGpng Ptm_lowMass_bkg.png r1 manage 16.3 K 2013-03-04 - 18:00 RobertoSalerno  
Unknown file formateps Ptm_lowMass_ggH.eps r1 manage 39.4 K 2013-03-04 - 18:00 RobertoSalerno  
PNGpng Ptm_lowMass_ggH.png r1 manage 16.6 K 2013-03-04 - 18:00 RobertoSalerno  
Unknown file formateps Ptm_lowMass_qqH.eps r1 manage 41.3 K 2013-03-04 - 18:00 RobertoSalerno  
PNGpng Ptm_lowMass_qqH.png r1 manage 16.9 K 2013-03-04 - 18:00 RobertoSalerno  
Unknown file formateps Pvals_PLP_lowMass_1D2D3D_Final3_no2l2tau_7p8sep.eps r1 manage 23.0 K 2013-03-04 - 15:13 RobertoSalerno  
PNGpng Pvals_PLP_lowMass_1D2D3D_Final3_no2l2tau_7p8sep.png r1 manage 30.9 K 2013-03-04 - 15:13 RobertoSalerno  
Unknown file formateps Pvals_PLP_lowMass_78_Final3_no2l2tau_7p8sep.eps r1 manage 21.8 K 2013-03-04 - 15:12 RobertoSalerno  
PNGpng Pvals_PLP_lowMass_78_Final3_no2l2tau_7p8sep.png r1 manage 30.2 K 2013-03-04 - 15:12 RobertoSalerno  
Unknown file formateps Pvals_PLP_lowMass_Final3_2l2tau_7p8sep.eps r1 manage 18.8 K 2013-03-04 - 15:39 RobertoSalerno  
PNGpng Pvals_PLP_lowMass_Final3_2l2tau_7p8sep.png r1 manage 25.1 K 2013-03-04 - 15:39 RobertoSalerno  
Unknown file formateps Pvals_PLP_lowMass_Final3_no2l2tau_7p8sep.eps r1 manage 18.7 K 2013-03-04 - 15:39 RobertoSalerno  
PNGpng Pvals_PLP_lowMass_Final3_no2l2tau_7p8sep.png r1 manage 24.8 K 2013-03-04 - 15:39 RobertoSalerno  
Unknown file formateps Pvals_PLP_lowMass_tagged_Final3_no2l2tau_7p8sep.eps r1 manage 22.1 K 2013-03-04 - 15:12 RobertoSalerno  
PNGpng Pvals_PLP_lowMass_tagged_Final3_no2l2tau_7p8sep.png r1 manage 31.5 K 2013-03-04 - 15:12 RobertoSalerno  
Unknown file formateps Pvals_PLP_wholeMass_1D2D3D_Final3_no2l2tau_7p8sep.eps r1 manage 25.2 K 2013-03-04 - 15:12 RobertoSalerno  
PNGpng Pvals_PLP_wholeMass_1D2D3D_Final3_no2l2tau_7p8sep.png r1 manage 30.5 K 2013-03-04 - 15:12 RobertoSalerno  
Unknown file formateps Pvals_PLP_wholeMass_78_Final3_no2l2tau_7p8sep.eps r1 manage 23.8 K 2013-03-04 - 15:12 RobertoSalerno  
PNGpng Pvals_PLP_wholeMass_78_Final3_no2l2tau_7p8sep.png r1 manage 29.4 K 2013-03-04 - 15:12 RobertoSalerno  
Unknown file formateps Pvals_PLP_wholeMass_Final3_2l2tau_7p8sep.eps r1 manage 19.7 K 2013-03-04 - 15:39 RobertoSalerno  
PNGpng Pvals_PLP_wholeMass_Final3_2l2tau_7p8sep.png r1 manage 24.2 K 2013-03-04 - 15:39 RobertoSalerno  
Unknown file formateps Pvals_PLP_wholeMass_Final3_no2l2tau_7p8sep.eps r1 manage 19.6 K 2013-03-04 - 15:39 RobertoSalerno  
PNGpng Pvals_PLP_wholeMass_Final3_no2l2tau_7p8sep.png r1 manage 23.8 K 2013-03-04 - 15:39 RobertoSalerno  
Unknown file formateps Pvals_PLP_wholeMass_tagged_Final3_no2l2tau_7p8sep.eps r1 manage 24.4 K 2013-03-04 - 15:12 RobertoSalerno  
PNGpng Pvals_PLP_wholeMass_tagged_Final3_no2l2tau_7p8sep.png r1 manage 31.2 K 2013-03-04 - 15:12 RobertoSalerno  
PDFpdf RVRF.pdf r1 manage 18.1 K 2013-03-03 - 11:16 RobertoSalerno  
PNGpng RVRF.png r1 manage 105.4 K 2013-03-03 - 11:16 RobertoSalerno  
Unknown file formateps Twiki_HZZ_MuonID_pt_barrel.eps r1 manage 11.0 K 2013-03-05 - 16:29 NicolaDeFilippis  
PDFpdf Twiki_HZZ_MuonID_pt_barrel.pdf r1 manage 10.4 K 2013-03-05 - 16:29 NicolaDeFilippis  
PNGpng Twiki_HZZ_MuonID_pt_barrel.png r1 manage 13.8 K 2013-03-05 - 16:29 NicolaDeFilippis  
Unknown file formateps Twiki_HZZ_MuonID_pt_endcap.eps r1 manage 11.6 K 2013-03-05 - 16:30 NicolaDeFilippis  
PDFpdf Twiki_HZZ_MuonID_pt_endcap.pdf r1 manage 10.5 K 2013-03-05 - 16:30 NicolaDeFilippis  
PNGpng Twiki_HZZ_MuonID_pt_endcap.png r1 manage 13.9 K 2013-03-05 - 16:30 NicolaDeFilippis  
Unknown file formateps Twiki_HZZ_MuonPFEAIso_pt_barrel.eps r1 manage 10.8 K 2013-03-05 - 16:31 NicolaDeFilippis  
PDFpdf Twiki_HZZ_MuonPFEAIso_pt_barrel.pdf r1 manage 10.1 K 2013-03-05 - 16:31 NicolaDeFilippis  
PNGpng Twiki_HZZ_MuonPFEAIso_pt_barrel.png r1 manage 14.5 K 2013-03-05 - 16:31 NicolaDeFilippis  
Unknown file formateps Twiki_HZZ_MuonPFEAIso_pt_endcap.eps r1 manage 10.5 K 2013-03-05 - 16:32 NicolaDeFilippis  
PDFpdf Twiki_HZZ_MuonPFEAIso_pt_endcap.pdf r1 manage 10.1 K 2013-03-05 - 16:32 NicolaDeFilippis  
PNGpng Twiki_HZZ_MuonPFEAIso_pt_endcap.png r1 manage 14.3 K 2013-03-05 - 16:33 NicolaDeFilippis  
Unknown file formateps Twiki_HZZ_MuonPFEAIso_vtx.eps r1 manage 11.7 K 2013-03-05 - 16:33 NicolaDeFilippis  
PDFpdf Twiki_HZZ_MuonPFEAIso_vtx.pdf r1 manage 9.8 K 2013-03-05 - 16:33 NicolaDeFilippis  
PNGpng Twiki_HZZ_MuonPFEAIso_vtx.png r1 manage 14.3 K 2013-03-05 - 16:34 NicolaDeFilippis  
Unknown file formateps Twiki_HZZ_MuonSIP_All_eta.eps r1 manage 12.6 K 2013-03-05 - 16:34 NicolaDeFilippis  
PDFpdf Twiki_HZZ_MuonSIP_All_eta.pdf r1 manage 11.0 K 2013-03-05 - 16:34 NicolaDeFilippis  
PNGpng Twiki_HZZ_MuonSIP_All_eta.png r1 manage 13.6 K 2013-03-05 - 16:35 NicolaDeFilippis  
Unknown file formateps UntaggedMass.eps r1 manage 17.8 K 2013-03-04 - 16:54 RobertoSalerno  
PDFpdf UntaggedMass.pdf r1 manage 28.4 K 2013-03-04 - 16:54 RobertoSalerno  
PNGpng UntaggedMass.png r1 manage 96.6 K 2013-03-04 - 16:54 RobertoSalerno  
Unknown file formateps UntaggedPtOM.eps r1 manage 16.7 K 2013-03-04 - 17:11 RobertoSalerno  
PDFpdf UntaggedPtOM.pdf r1 manage 26.6 K 2013-03-04 - 17:11 RobertoSalerno  
PNGpng UntaggedPtOM.png r1 manage 80.7 K 2013-03-04 - 17:11 RobertoSalerno  
Unknown file formateps UpperLimit_ASCLS_7p8TeV_lowMass_Final2_2l2tau.eps r1 manage 19.3 K 2013-03-01 - 23:29 ChristopheOchando  
PDFpdf UpperLimit_ASCLS_7p8TeV_lowMass_Final2_2l2tau.pdf r1 manage 10.2 K 2013-03-01 - 23:29 ChristopheOchando  
PNGpng UpperLimit_ASCLS_7p8TeV_lowMass_Final2_2l2tau.png r1 manage 27.9 K 2013-03-01 - 23:29 ChristopheOchando  
Unknown file formateps UpperLimit_ASCLS_7p8TeV_wholeMass_Final2_2l2tau.eps r1 manage 24.6 K 2013-03-01 - 23:29 ChristopheOchando  
PDFpdf UpperLimit_ASCLS_7p8TeV_wholeMass_Final2_2l2tau.pdf r1 manage 15.1 K 2013-03-01 - 23:29 ChristopheOchando  
PNGpng UpperLimit_ASCLS_7p8TeV_wholeMass_Final2_2l2tau.png r1 manage 29.8 K 2013-03-01 - 23:29 ChristopheOchando  
Unknown file formateps VAJHU2D_Moriond_background_highmass.eps r1 manage 202.0 K 2013-02-26 - 11:34 RobertoSalerno  
PDFpdf VAJHU2D_Moriond_background_highmass.pdf r1 manage 67.9 K 2013-02-26 - 11:34 RobertoSalerno  
PNGpng VAJHU2D_Moriond_background_highmass.png r1 manage 29.3 K 2013-02-26 - 11:34 RobertoSalerno  
Unknown file formateps VAJHU2D_Moriond_background_lowmass.eps r1 manage 48.8 K 2013-02-26 - 11:34 RobertoSalerno  
PDFpdf VAJHU2D_Moriond_background_lowmass.pdf r1 manage 26.8 K 2013-02-26 - 11:34 RobertoSalerno  
PNGpng VAJHU2D_Moriond_background_lowmass.png r1 manage 24.4 K 2013-02-26 - 11:34 RobertoSalerno  
Unknown file formateps VAJHU2D_Moriond_signal126_lowmass.eps r1 manage 48.1 K 2013-02-26 - 11:34 RobertoSalerno  
PDFpdf VAJHU2D_Moriond_signal126_lowmass.pdf r1 manage 26.5 K 2013-02-26 - 11:34 RobertoSalerno  
PNGpng VAJHU2D_Moriond_signal126_lowmass.png r1 manage 23.1 K 2013-02-26 - 11:34 RobertoSalerno  
Unknown file formateps Z1Mass_wholeRange.eps r1 manage 17.7 K 2013-03-04 - 16:16 RobertoSalerno  
PNGpng Z1Mass_wholeRange.png r1 manage 16.4 K 2013-03-04 - 16:16 RobertoSalerno  
PDFpdf Z1Z2mass.pdf r1 manage 15.8 K 2013-03-04 - 10:28 RamanKhurana  
PNGpng Z1Z2mass.png r1 manage 15.9 K 2013-03-04 - 10:37 RamanKhurana  
Unknown file formateps Z2Mass_wholeRange.eps r1 manage 21.7 K 2013-03-04 - 16:16 RobertoSalerno  
PNGpng Z2Mass_wholeRange.png r1 manage 18.0 K 2013-03-04 - 16:16 RobertoSalerno  
PDFpdf Z4L_BestFit10000bins_7p8TeV.pdf r1 manage 17.6 K 2013-03-04 - 14:16 RobertoSalerno  
PNGpng Z4L_BestFit10000bins_7p8TeV.png r1 manage 128.5 K 2013-03-04 - 14:16 RobertoSalerno  
PDFpdf Z4L_correctedRelerr_all_7p8TeV.pdf r1 manage 15.2 K 2013-03-04 - 14:13 RobertoSalerno  
PNGpng Z4L_correctedRelerr_all_7p8TeV.png r1 manage 21.3 K 2013-03-04 - 14:13 RobertoSalerno  
Unknown file formateps ZZMass_7Plus8TeV_100-180_3GeV.eps r1 manage 19.6 K 2013-02-26 - 17:58 RobertoSalerno  
PNGpng ZZMass_7Plus8TeV_100-180_3GeV.png r1 manage 14.7 K 2013-02-26 - 17:58 RobertoSalerno  
Unknown file formateps ZZMass_7Plus8TeV_100-180_3GeV_KD03.eps r1 manage 19.2 K 2013-03-04 - 18:54 RobertoSalerno  
PNGpng ZZMass_7Plus8TeV_100-180_3GeV_KD03.png r1 manage 14.4 K 2013-03-04 - 18:54 RobertoSalerno  
Unknown file formateps ZZMass_7Plus8TeV_100-180_3GeV_KD05.eps r1 manage 18.8 K 2013-03-04 - 18:54 RobertoSalerno  
PNGpng ZZMass_7Plus8TeV_100-180_3GeV_KD05.png r1 manage 14.2 K 2013-03-04 - 18:54 RobertoSalerno  
PDFpdf ZZMass_7Plus8TeV_70-1000_3GeV.pdf r1 manage 29.5 K 2013-02-26 - 18:01 RobertoSalerno  
PNGpng ZZMass_7Plus8TeV_70-1000_3GeV.png r1 manage 28.5 K 2013-02-26 - 18:01 RobertoSalerno  
Unknown file formateps ZZMass_7Plus8TeV_70-180_3GeV.eps r1 manage 19.0 K 2013-02-26 - 17:46 RobertoSalerno  
PNGpng ZZMass_7Plus8TeV_70-180_3GeV.png r1 manage 14.4 K 2013-02-26 - 17:46 RobertoSalerno  
Unknown file formateps ZZMass_7Plus8TeV_70-600_10GeV.eps r1 manage 21.3 K 2013-02-26 - 17:58 RobertoSalerno  
PNGpng ZZMass_7Plus8TeV_70-600_10GeV.png r1 manage 14.9 K 2013-02-26 - 17:58 RobertoSalerno  
Unknown file formateps ZZMass_7Plus8TeV_70-800_10GeV.eps r1 manage 22.9 K 2013-02-26 - 17:58 RobertoSalerno  
PNGpng ZZMass_7Plus8TeV_70-800_10GeV.png r1 manage 15.2 K 2013-02-26 - 17:58 RobertoSalerno  
PDFpdf Z_invmass_aftermass_EBG1EBG1.pdf r1 manage 27.1 K 2013-03-04 - 14:33 RobertoSalerno  
PNGpng Z_invmass_aftermass_EBG1EBG1.png r1 manage 23.6 K 2013-03-04 - 14:33 RobertoSalerno  
PDFpdf Z_invmass_aftermass_EEG2EEG2.pdf r1 manage 28.1 K 2013-03-04 - 14:33 RobertoSalerno  
PNGpng Z_invmass_aftermass_EEG2EEG2.png r1 manage 25.8 K 2013-03-04 - 14:33 RobertoSalerno  
Unknown file formateps can_scan1D_x_Mor_withAsimov_611.eps r1 manage 10.3 K 2013-03-04 - 17:34 RobertoSalerno  
PDFpdf can_scan1D_x_Mor_withAsimov_611.pdf r1 manage 5.4 K 2013-03-04 - 17:34 RobertoSalerno  
PNGpng can_scan1D_x_Mor_withAsimov_611.png r1 manage 19.7 K 2013-03-04 - 17:34 RobertoSalerno  
PDFpdf compmH126_NomNoRegr_channel1.pdf r1 manage 27.9 K 2013-03-04 - 12:24 RobertoSalerno  
PNGpng compmH126_NomNoRegr_channel1.png r1 manage 28.5 K 2013-03-04 - 12:24 RobertoSalerno  
PDFpdf compmH126_NomNoRegr_channel2.pdf r1 manage 23.8 K 2013-03-04 - 12:24 RobertoSalerno  
PNGpng compmH126_NomNoRegr_channel2.png r1 manage 27.4 K 2013-03-04 - 12:24 RobertoSalerno  
PDFpdf deltaM_vs_PU.pdf r1 manage 13.4 K 2013-02-28 - 17:15 RobertoSalerno  
PNGpng deltaM_vs_PU.png r1 manage 16.2 K 2013-02-28 - 17:15 RobertoSalerno  
PDFpdf eettVector.pdf r1 manage 15.6 K 2013-03-04 - 10:28 RamanKhurana  
PDFpdf effRMSbarrel_withregression_new.pdf r1 manage 18.7 K 2013-02-27 - 16:30 RobertoSalerno  
PNGpng effRMSbarrel_withregression_new.png r1 manage 125.3 K 2013-02-27 - 16:30 RobertoSalerno  
PDFpdf fitM126_channel0.pdf r1 manage 19.3 K 2013-02-27 - 15:31 RobertoSalerno  
PNGpng fitM126_channel0.png r1 manage 26.9 K 2013-02-27 - 15:31 RobertoSalerno  
PDFpdf fitM126_channel1.pdf r1 manage 20.8 K 2013-02-27 - 15:31 RobertoSalerno  
PNGpng fitM126_channel1.png r1 manage 29.7 K 2013-02-27 - 15:31 RobertoSalerno  
PDFpdf fitM126_channel2.pdf r1 manage 19.7 K 2013-02-27 - 15:31 RobertoSalerno  
PNGpng fitM126_channel2.png r1 manage 28.5 K 2013-02-27 - 15:31 RobertoSalerno  
Unknown file formateps gg2mp_ALTSignal_Moriond_signal126_lowmass.eps r1 manage 78.3 K 2013-03-14 - 16:41 RobertoSalerno  
PDFpdf gg2mp_ALTSignal_Moriond_signal126_lowmass.pdf r1 manage 29.0 K 2013-03-14 - 16:41 RobertoSalerno  
PNGpng gg2mp_ALTSignal_Moriond_signal126_lowmass.png r1 manage 15.9 K 2013-03-14 - 16:43 RobertoSalerno  
Unknown file formateps gg2mp_SMSignal_Moriond_signal126_lowmass.eps r1 manage 80.6 K 2013-03-14 - 16:43 RobertoSalerno  
PDFpdf gg2mp_SMSignal_Moriond_signal126_lowmass.pdf r1 manage 29.2 K 2013-03-14 - 16:43 RobertoSalerno  
PNGpng gg2mp_SMSignal_Moriond_signal126_lowmass.png r1 manage 16.3 K 2013-03-14 - 16:43 RobertoSalerno  
Unknown file formateps gg2mp_qqZZBackgr_Moriond_signal126_lowmass.eps r1 manage 69.2 K 2013-03-14 - 16:43 RobertoSalerno  
PDFpdf gg2mp_qqZZBackgr_Moriond_signal126_lowmass.pdf r1 manage 26.6 K 2013-03-14 - 16:43 RobertoSalerno  
PNGpng gg2mp_qqZZBackgr_Moriond_signal126_lowmass.png r1 manage 14.1 K 2013-03-14 - 16:43 RobertoSalerno  
PDFpdf jets.pdf r1 manage 25.7 K 2013-03-04 - 17:10 RobertoSalerno  
PNGpng jets.png r1 manage 80.8 K 2013-03-04 - 17:10 RobertoSalerno  
PDFpdf leadingeleIsoVector.pdf r1 manage 17.4 K 2013-03-04 - 10:28 RamanKhurana  
PNGpng leadingeleIsoVector.png r2 r1 manage 14.1 K 2013-03-04 - 12:21 RamanKhurana  
PDFpdf leadingmuIsoVector.pdf r1 manage 17.4 K 2013-03-04 - 10:28 RamanKhurana  
PNGpng leadingmuIsoVector.png r2 r1 manage 13.9 K 2013-03-04 - 12:21 RamanKhurana  
PDFpdf mH125Shift-8TeV-ch1.pdf r1 manage 38.7 K 2013-02-28 - 15:56 RobertoSalerno  
PNGpng mH125Shift-8TeV-ch1.png r1 manage 162.8 K 2013-02-28 - 15:56 RobertoSalerno  
PDFpdf massZ4lScan10kbins_splitv2.pdf r1 manage 10.9 K 2013-05-23 - 20:59 EmanueleDiMarco mass scans divided by channels
PNGpng massZ4lScan10kbins_splitv2.png r1 manage 164.9 K 2013-05-23 - 20:59 EmanueleDiMarco mass scans divided by channels
PDFpdf mlz_ccc_mH1258.pdf r1 manage 13.2 K 2013-03-04 - 17:37 RobertoSalerno  
PNGpng mlz_ccc_mH1258.png r1 manage 14.2 K 2013-03-04 - 17:37 RobertoSalerno  
PDFpdf mmttVector.pdf r1 manage 15.7 K 2013-03-04 - 10:28 RamanKhurana  
PDFpdf mu_res1_vs_eta_sigma.pdf r1 manage 14.2 K 2013-03-04 - 14:23 RobertoSalerno  
PNGpng mu_res1_vs_eta_sigma.png r1 manage 14.2 K 2013-03-04 - 14:23 RobertoSalerno  
PDFpdf mu_res1_vs_pt_sigma.pdf r1 manage 13.9 K 2013-03-04 - 14:23 RobertoSalerno  
PNGpng mu_res1_vs_pt_sigma.png r1 manage 14.9 K 2013-03-04 - 14:23 RobertoSalerno  
PDFpdf nEvent_EETT_8TeV.pdf r1 manage 15.6 K 2013-03-04 - 12:39 SimranjitSinghChhibra  
PNGpng nEvent_EETT_8TeV.png r1 manage 14.4 K 2013-03-04 - 12:40 SimranjitSinghChhibra  
PDFpdf nEvent_MMTT_8TeV.pdf r1 manage 15.7 K 2013-03-04 - 12:41 SimranjitSinghChhibra  
PNGpng nEvent_MMTT_8TeV.png r1 manage 14.5 K 2013-03-04 - 12:42 SimranjitSinghChhibra  
Unknown file formateps obs_1d_likelihood_for_moriond_3Dbase_sys.eps r3 r2 r1 manage 10.4 K 2013-03-03 - 17:00 RobertoSalerno  
PDFpdf obs_1d_likelihood_for_moriond_3Dbase_sys.pdf r3 r2 r1 manage 23.9 K 2013-03-03 - 17:00 RobertoSalerno  
PNGpng obs_1d_likelihood_for_moriond_3Dbase_sys.png r3 r2 r1 manage 13.8 K 2013-03-03 - 17:00 RobertoSalerno  
Unknown file formateps obs_1d_likelihood_for_moriond_3sets.eps r1 manage 11.6 K 2013-03-03 - 16:58 RobertoSalerno  
PDFpdf obs_1d_likelihood_for_moriond_3sets.pdf r1 manage 23.6 K 2013-03-03 - 16:58 RobertoSalerno  
PNGpng obs_1d_likelihood_for_moriond_3sets.png r1 manage 13.7 K 2013-03-03 - 16:58 RobertoSalerno  
Unknown file formateps qq2mp_ALTSignal_Moriond_signal126_lowmass.eps r1 manage 76.9 K 2013-03-14 - 16:43 RobertoSalerno  
PDFpdf qq2mp_ALTSignal_Moriond_signal126_lowmass.pdf r1 manage 28.7 K 2013-03-14 - 16:43 RobertoSalerno  
PNGpng qq2mp_ALTSignal_Moriond_signal126_lowmass.png r1 manage 15.5 K 2013-03-14 - 16:43 RobertoSalerno  
Unknown file formateps qq2mp_SMSignal_Moriond_signal126_lowmass.eps r1 manage 77.9 K 2013-03-14 - 16:44 RobertoSalerno  
PDFpdf qq2mp_SMSignal_Moriond_signal126_lowmass.pdf r1 manage 28.9 K 2013-03-14 - 16:44 RobertoSalerno  
PNGpng qq2mp_SMSignal_Moriond_signal126_lowmass.png r1 manage 15.7 K 2013-03-14 - 16:44 RobertoSalerno  
Unknown file formateps qq2mp_qqZZBackgr_Moriond_signal126_lowmass.eps r1 manage 69.1 K 2013-03-14 - 16:44 RobertoSalerno  
PDFpdf qq2mp_qqZZBackgr_Moriond_signal126_lowmass.pdf r1 manage 26.7 K 2013-03-14 - 16:44 RobertoSalerno  
PNGpng qq2mp_qqZZBackgr_Moriond_signal126_lowmass.png r1 manage 14.0 K 2013-03-14 - 16:44 RobertoSalerno  
PDFpdf scale-ptdep-7TeV.pdf r2 r1 manage 16.2 K 2013-03-01 - 15:45 RobertoSalerno  
PNGpng scale-ptdep-7TeV.png r2 r1 manage 150.7 K 2013-03-01 - 15:45 RobertoSalerno  
PDFpdf scale-ptdep-8TeV.pdf r2 r1 manage 17.2 K 2013-03-01 - 15:45 RobertoSalerno  
PNGpng scale-ptdep-8TeV.png r2 r1 manage 154.8 K 2013-03-01 - 15:45 RobertoSalerno  
Unknown file formateps separation_0hp.eps r1 manage 14.1 K 2013-03-04 - 15:54 ChristopheOchando  
PDFpdf separation_0hp.pdf r1 manage 6.0 K 2013-03-04 - 15:54 ChristopheOchando  
PNGpng separation_0hp.png r1 manage 14.6 K 2013-03-04 - 15:54 ChristopheOchando  
Unknown file formateps separation_0mp.eps r1 manage 14.4 K 2013-03-04 - 15:54 ChristopheOchando  
PDFpdf separation_0mp.pdf r1 manage 6.1 K 2013-03-04 - 15:54 ChristopheOchando  
PNGpng separation_0mp.png r1 manage 13.8 K 2013-03-04 - 15:54 ChristopheOchando  
Unknown file formateps separation_1minus.eps r1 manage 14.4 K 2013-03-04 - 15:54 ChristopheOchando  
PDFpdf separation_1minus.pdf r1 manage 6.1 K 2013-03-04 - 15:54 ChristopheOchando  
PNGpng separation_1minus.png r1 manage 13.4 K 2013-03-04 - 15:54 ChristopheOchando  
Unknown file formateps separation_1p.eps r1 manage 14.5 K 2013-03-04 - 15:55 ChristopheOchando  
PDFpdf separation_1p.pdf r1 manage 6.1 K 2013-03-04 - 15:55 ChristopheOchando  
PNGpng separation_1p.png r1 manage 13.9 K 2013-03-04 - 15:55 ChristopheOchando  
Unknown file formateps separation_gg2pmin.eps r1 manage 14.4 K 2013-03-04 - 15:55 ChristopheOchando  
PDFpdf separation_gg2pmin.pdf r1 manage 6.1 K 2013-03-04 - 15:55 ChristopheOchando  
PNGpng separation_gg2pmin.png r1 manage 15.0 K 2013-03-04 - 15:55 ChristopheOchando  
Unknown file formateps separation_qq2pmin.eps r1 manage 14.9 K 2013-03-04 - 15:55 ChristopheOchando  
PDFpdf separation_qq2pmin.pdf r1 manage 6.1 K 2013-03-04 - 15:55 ChristopheOchando  
PNGpng separation_qq2pmin.png r1 manage 177.6 K 2013-03-04 - 17:25 RobertoSalerno  
PDFpdf sigmaOverM.pdf r1 manage 14.6 K 2013-02-27 - 16:45 RobertoSalerno  
PNGpng sigmaOverM.png r1 manage 98.1 K 2013-02-27 - 16:45 RobertoSalerno  
Unknown file formateps sigsep_combine_scan2D_contour_Mor_611_withColorCode.eps r1 manage 151.5 K 2013-03-05 - 12:30 RobertoSalerno  
PDFpdf sigsep_combine_scan2D_contour_Mor_611_withColorCode.pdf r1 manage 33.6 K 2013-03-05 - 12:30 RobertoSalerno  
PNGpng sigsep_combine_scan2D_contour_Mor_611_withColorCode.png r1 manage 91.9 K 2013-03-05 - 12:30 RobertoSalerno  
PDFpdf sqr_mass_scan_1d_allhzz.pdf r1 manage 13.4 K 2013-05-23 - 20:59 EmanueleDiMarco mass scans divided by channels
PDFpdf sqr_mass_scan_1d_allhzz_2.pdf r1 manage 13.4 K 2013-05-23 - 20:59 EmanueleDiMarco mass scans divided by channels
PNGpng sqr_mass_scan_1d_allhzz_2.png r1 manage 178.3 K 2013-05-23 - 21:04 EmanueleDiMarco  
Unknown file formateps taggedMass.eps r1 manage 16.6 K 2013-03-04 - 16:54 RobertoSalerno  
PDFpdf taggedMass.pdf r1 manage 27.0 K 2013-03-04 - 16:54 RobertoSalerno  
PNGpng taggedMass.png r1 manage 88.2 K 2013-03-04 - 16:54 RobertoSalerno  
Unknown file formateps taggedVD.eps r1 manage 16.2 K 2013-03-04 - 17:11 RobertoSalerno  
PDFpdf taggedVD.pdf r1 manage 26.4 K 2013-03-04 - 17:11 RobertoSalerno  
PNGpng taggedVD.png r1 manage 76.6 K 2013-03-04 - 17:11 RobertoSalerno  
PDFpdf tauFR_HPSMediumIso_2012_MC8TeV.pdf r2 r1 manage 19.5 K 2013-03-04 - 12:55 SimranjitSinghChhibra  
PNGpng tauFR_HPSMediumIso_2012_MC8TeV.png r1 manage 17.8 K 2013-03-04 - 12:55 SimranjitSinghChhibra  
PDFpdf tauFR_HPSTightIso_2012_MC8TeV.pdf r1 manage 19.3 K 2013-03-04 - 12:56 SimranjitSinghChhibra  
PNGpng tauFR_HPSTightIso_2012_MC8TeV.png r1 manage 17.0 K 2013-03-04 - 12:56 SimranjitSinghChhibra  
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Topic revision: r61 - 2013-08-02 - EmanueleDiMarco
 
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