| 38 |
|
%${\rm p_T}>$ 20~\GeVc\ . |
| 39 |
|
%The second must have ${\rm p_T}>$ 10~\GeVc\ . |
| 40 |
|
% |
| 41 |
– |
%Charged leptons from the decay of ${W, Z}$ bosons, and the new physics |
| 42 |
– |
%we are searching for, are expected to be |
| 43 |
– |
%isolated from other activity in the event. For selected muon and |
| 44 |
– |
%electron candidates, a cone of $\Delta R <$~0.3 is constructed |
| 45 |
– |
%around the track direction at the origin and the scalar sum of the |
| 46 |
– |
%track transverse momenta and calorimeter energy deposits, projected onto |
| 47 |
– |
%a plane transverse to the beam, is calculated. ĘThe contribution from |
| 48 |
– |
%the candidate itself is excluded. Depending on analysis region, we require the value of this scalar sum |
| 49 |
– |
%to be less than 10-15\% of the candidate's transverse momentum to be considered as a prompt lepton. |
| 41 |
|
|
| 42 |
< |
%Jets and \MET were reconstructed based on particle flow reconstruction~\cite{PFT-09-001}~\cite{PFT-10-002}. For jet clustering, we use the anti-$k_T$ algorithm |
| 43 |
< |
%with the distance parameter $R = 0.5$~\cite{anti-kt}. Jets were required to pass standard quality cuts to remove those consistent with calorimeter noise. |
| 44 |
< |
%Jet energies were corrected for residual non-uniformity and non-linearity of the detector response |
| 45 |
< |
%derived using early collision data~\cite{JES}. |
| 46 |
< |
%We required jets to have transverse energy above 30 GeV and to be within $|\eta |<2.5$. |
| 47 |
< |
%We form an $H_T$ observable as the sum of all jets with ${ \Delta R > 0.4}$ to the nearest lepton passing all our requirements. |
| 42 |
> |
Charged leptons from the decay of ${W, Z}$ bosons, and the new physics |
| 43 |
> |
we are searching for, are expected to be |
| 44 |
> |
isolated from other activity in the event. For selected muon and |
| 45 |
> |
electron candidates, a cone of $\Delta R <$~0.3 is constructed |
| 46 |
> |
around the track direction at the origin and the scalar sum of the |
| 47 |
> |
track transverse momenta and calorimeter energy deposits, projected onto |
| 48 |
> |
a plane transverse to the beam, is calculated. ĘThe contribution from |
| 49 |
> |
the candidate itself is excluded. |
| 50 |
> |
|
| 51 |
> |
%Depending on analysis region, we require the value of this scalar sum |
| 52 |
> |
%to be less than 10-15\% of the candidate's transverse momentum to be considered as a prompt lepton. |
| 53 |
|
|
| 54 |
+ |
Jets and \MET were reconstructed based on particle flow reconstruction~\cite{PFT-09-001}~\cite{PFT-10-002}. For jet clustering, we use the anti-$k_T$ algorithm |
| 55 |
+ |
with the distance parameter $R = 0.5$~\cite{anti-kt}. Jets were required to pass standard quality cuts to remove those consistent with calorimeter noise. |
| 56 |
+ |
Jet energies were corrected for residual non-uniformity and non-linearity of the detector response |
| 57 |
+ |
derived using early collision data~\cite{JES}. |
| 58 |
+ |
We required jets to have transverse energy above 30 GeV and to be within $|\eta |<2.5$. |
| 59 |
+ |
We form an $H_T$ observable as the sum of all jets with ${ \Delta R > 0.4}$ to the nearest lepton passing all our requirements. |
