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[PDF] Top 20 Measurement of the ZZ production cross section in proton-proton collisions at √s=8 TeV using the ZZ → ℓ−ℓ+ℓ′−ℓ′+ and ZZ→ℓ−ℓ+νν⎯⎯⎯ZZ→ℓ−ℓ+νν¯ decay channels with the ATLAS detector

Has 10000 "Measurement of the ZZ production cross section in proton-proton collisions at √s=8 TeV using the ZZ → ℓ−ℓ+ℓ′−ℓ′+ and ZZ→ℓ−ℓ+νν⎯⎯⎯ZZ→ℓ−ℓ+νν¯ decay channels with the ATLAS detector" found on our website. Below are the top 20 most common "Measurement of the ZZ production cross section in proton-proton collisions at √s=8 TeV using the ZZ → ℓ−ℓ+ℓ′−ℓ′+ and ZZ→ℓ−ℓ+νν⎯⎯⎯ZZ→ℓ−ℓ+νν¯ decay channels with the ATLAS detector".

Measurement of the ZZ production cross section in proton proton collisions at s=8 TeV using the ZZ → ℓ−ℓ+ℓ′−ℓ′+ and ZZ→ℓ−ℓ+νν¯ decay channels with the ATLAS detector

Measurement of the ZZ production cross section in proton proton collisions at s=8 TeV using the ZZ → ℓ−ℓ+ℓ′−ℓ′+ and ZZ→ℓ−ℓ+νν¯ decay channels with the ATLAS detector

... The production of electroweak gauge boson pairs provides an opportunity to perform pre- cision studies of the electroweak sector by looking for deviations from the predicted total and differential ... See full document

53

Measurement of the ZZ production cross section in proton-proton collisions at root s=8 TeV using the ZZ -> l(-) l(+) l '(-) l '(+) and ZZ -> l(-) l(+) nu(nu)over-bar decay channels with the ATLAS detector

Measurement of the ZZ production cross section in proton-proton collisions at root s=8 TeV using the ZZ -> l(-) l(+) l '(-) l '(+) and ZZ -> l(-) l(+) nu(nu)over-bar decay channels with the ATLAS detector

... J. Monk 38 , E. Monnier 87 , A. Montalbano 151 , J. Montejo Berlingen 32 , F. Monticelli 73 , S. Monzani 93a,93b , R.W. Moore 3 , N. Morange 118 , D. Moreno 21 , M. Moreno Llácer 56 , P. Morettini 52a , S. ... See full document

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Search for new resonances decaying to a W or Z boson and a Higgs boson in the ℓ<sup>+</sup>ℓ<sup>−</sup>bb¯, ℓνbb¯, and νν¯bb¯ channels with pp collisions at s=13 TeV with the ATLAS detector

Search for new resonances decaying to a W or Z boson and a Higgs boson in the ℓ<sup>+</sup>ℓ<sup>−</sup>bb¯, ℓνbb¯, and νν¯bb¯ channels with pp collisions at s=13 TeV with the ATLAS detector

... The search presented here has been optimized to be sensitive to resonances of mass larger than 1 TeV, hence decaying to highly boosted final-state particles. As a consequence, the Higgs boson de- cay to bottom ... See full document

21

Search for the Higgs boson in the H &gt;WW(*) &gt;ℓ+νℓ ν̅ decay channel in pp collisions at √s=7 TeV with the ATLAS detector

Search for the Higgs boson in the H >WW(*) >ℓ+νℓ ν̅ decay channel in pp collisions at √s=7 TeV with the ATLAS detector

... WW cross sections for the H þ 0 jet and H þ 1 jet channels, and the top cross section for the H þ 1 jet channel are allowed to vary independently; the control regions included in the fit con- ... See full document

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ENHANCED PLANTED(ℓ,D) MOTIF SEARCH PRUNE ALGORITHM FOR PARALLEL ENVIRONMENT

ENHANCED PLANTED(ℓ,D) MOTIF SEARCH PRUNE ALGORITHM FOR PARALLEL ENVIRONMENT

... The algorithm that we proposed has been implemented in the C language using MPI library, Pthread library. The experiment is done in an environment where there is two nodes cluster with each of 2.4GHz Intel ... See full document

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Search for anomalous couplings in boosted W W / W Z → ℓ ν q q ‾ production in proton–proton collisions at s = 8 TeV

Search for anomalous couplings in boosted W W / W Z → ℓ ν q q ‾ production in proton–proton collisions at s = 8 TeV

... We use the MadGraph 5 1.3.30 [9] event generator to produce both the W+jets and Drell–Yan samples, with up to four addi- tional partons in the matrix element calculation. Single top quark and top quark–antiquark pair ... See full document

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Bipolar Anti L-Fuzzy Sub ℓ-HX Group and its Lower Level Sub ℓ-HX Groups

Bipolar Anti L-Fuzzy Sub ℓ-HX Group and its Lower Level Sub ℓ-HX Groups

... degree 0 means that the elements are irrelevant to the corresponding property, the membership degree (0,1] indicates that elements somewhat satisfy the property and the membership degree [−1,0) indicates that elements ... See full document

17

The ℓ translativity of Abel type matrix

The ℓ translativity of Abel type matrix

... In [1], Borwein proved that the Abel-type power series method of summability denoted by Aα α > −1, is translative in the ordinary summability c-c setting.. So, it natural to ask if there[r] ... See full document

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MATRIX TRANSFORMATIONS BETWEEN GENERALIZED RIESZ SEQUENCE SPACES OF NON ABSOLUTE TYPE

MATRIX TRANSFORMATIONS BETWEEN GENERALIZED RIESZ SEQUENCE SPACES OF NON ABSOLUTE TYPE

... A sequence space is defined to be a linear space of real or complex sequences. Throughout the paper ℕ, ℝ and ℂ denote the set of non negative integers, the set of real numbers and the set of complex numbers, ... See full document

8

A modified Kolmogorov Smirnov test for normality

A modified Kolmogorov Smirnov test for normality

... method. If G(L) ≥ 0, there is a solution (µ, σ) for this value of L and if G(L) < 0 no such solution exists. To find the minimum value of L we propose a binary search. The details of the binary search are now ... See full document

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The Abel type transformations into ℓ

The Abel type transformations into ℓ

... The matrix A tn Aα,t by ank = k+α n α,t determines a sequencek to-sequence variant of the Abel-type power series method of summability introduced by Borwein in [1].. The purpose of this [r] ... See full document

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On the h → Vℓ+ ℓ− decays

On the h → Vℓ+ ℓ− decays

... in the vector meson V can be studied by using the formalism of the QCD hard exclusive processes [22–25]. Here we should consider the matrix element of the non-local quark antiquark operator while the vector meson ... See full document

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On ℓ adic representations for a space of noncongruence cuspforms

On ℓ adic representations for a space of noncongruence cuspforms

... by using the data listed in Table 2, that they are absolutely irreducible and ...χ s , where χ s is the quadratic character of G Q with fixed ... See full document

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Thermodynamically-consistent semi-classical ℓ-changing rates

Thermodynamically-consistent semi-classical ℓ-changing rates

... given by VF01. Given that VF01 provide expressions for the transition rate out of an ` = 0 state, a zero inward rate is in clear violation of the detailed balance requirement. The values used in the elliptic integral ... See full document

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Lusztig induction and ℓ-blocks of finite reductive groups

Lusztig induction and ℓ-blocks of finite reductive groups

... It is the main purpose of this paper to unify and extend all of the preceding results in particular from [10] so as to establish a statement in its largest possible generality, without restrictions on the prime `, the ... See full document

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String theory clues for the low–ℓ CMB ?

String theory clues for the low–ℓ CMB ?

... that ϕ can attain during the cosmological evolution. Since in these models the inflaton hosts at least an admixture of the dilaton, the existence of an upper bound for a climbing scalar implies that the climbing behavior ... See full document

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Abel type weighted means transformations into ℓ

Abel type weighted means transformations into ℓ

... Theorem 2 gives an important inclusion result in the - setting that parallels the famous inclusion result that exists between the power series method of summability and its corresponding[r] ... See full document

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Identity-based  Hierarchical  Key-insulated  Encryption  without  Random  Oracles

Identity-based Hierarchical Key-insulated Encryption without Random Oracles

... We compare our scheme in the non-hierarchical case with existing PK-KIE schemes. Dodis et al. [14] (strongly) CCA-secure (non-hierarchical) PK-KIE scheme under decisional Diffie-Hellman (DDH) assump- tion. Namely, this ... See full document

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Search for a standard model Higgs boson in the H &gt;ZZ &gt;ℓ+ℓ νν̅ decay channel with the ATLAS detector

Search for a standard model Higgs boson in the H >ZZ >ℓ+ℓ νν̅ decay channel with the ATLAS detector

... pair production of Z bosons has a final state identical to the signal, and is therefore expected to survive most of the applied selection criteria and form a continuum in the transverse mass distribution (defined ... See full document

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Measurement of event-shape observables in Z→ℓ+ℓ- events in pp collisions at √s=7 TeV with the ATLAS detector at the LHC

Measurement of event-shape observables in Z→ℓ+ℓ- events in pp collisions at √s=7 TeV with the ATLAS detector at the LHC

... M. Proissl 47 , K. Prokofiev 61c , F. Prokoshin 33b , S. Protopopescu 26 , J. Proudfoot 6 , M. Przybycien 39a , D. Puddu 134a,134b , D. Puldon 148 , M. Purohit 26 ,af , P. Puzo 117 , J. Qian 90 , G. Qin 54 , Y. ... See full document

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