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We present a search for Kaluza-Klein (KK) particles predicted by models with universal extra dimensions (UED) using a data set corresponding to an integrated luminosity of 7.3 fb$^{-1}$, collected by the D0 detector at a $p\bar p$ center of mass energy of 1.96 TeV.
R. Brun, F. Carminati and S. Giani, CERN-W5013 (1993)
1993
Earlier work this paper cites.
G. C. Blazey et al
2000
Earlier work this paper cites.
H. L. Lai et al
2000
Earlier work this paper cites.
T. Appelquist, H.-C. Cheng and B. A. Dobrescu, Phys. Rev. D 64
2001
Earlier work this paper cites.
K. Agashe, N. G. Deshpande and G. H. Wu, Phys. Lett. B 514
2001
Earlier work this paper cites.
H.-C. Cheng, K. T. Matchev and M. Schmaltz, Phys. Rev. D 66
2002
Earlier work this paper cites.
H.-C. Cheng, J. L. Feng and K. T. Matchev, Phys. Rev. Lett. 89
2002
Earlier work this paper cites.
T. Junk, Nucl. Instrum. Methods in Phys. Res. A 434
2002
Cited alongside, same era.
M. L. Mangano et al
2003
Cited alongside, same era.
J. Pumplin et al
2003
Cited alongside, same era.
J. Campbell and R. K. Ellis, Phys. Rev. D 65
2003
Cited alongside, same era.
V. M. Abazov et al
2006
Cited alongside, same era.
T. Sjöstrand, S. Mrenna and P. Skands, J. High Energy Phys. 05
2006
Cited alongside, same era.
W. Fisher, FERMILAB-TM-2386-E (2006)
2006
Cited alongside, same era.
A. Hoecker et al
2007
Later among the works it cites.
S. Moch and P. Uwer, Phys. Rev. D 78
2008
Later among the works it cites.
V. M. Abazov et al
2010
Later among the works it cites.
G. Aad et al
2011
Closest in time.
G. Aad et al
2011
Closest in time.
V. M. Abazov et al
2011
Closest in time.
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The D0 detector coordinate system is right-handed with the z z axis pointing in the proton beam direction. The y y axis points upward and the azimuthal angle ϕ \phi is measured from the x x axis. Pseudorapidity is defined as η = − ln [ tan ( θ / 2 ) ] \eta=-\ln[\tan(\theta/2)] , where θ \theta is the polar angle
Cited in the paper.
Missing transverse energy is defined as E → T = − ∑ i ( E T , x i , E T , y i ) \mbox{$\not\!\!\vec{E}_{T}$}=-\displaystyle\sum_{i}(E^{i}_{T,x},E^{i}_{T,y}) , where E i T , x = E i sin θ i cos ϕ i , E i T , y = E i sin θ i sin ϕ i E^{i}_{T,x}=E^{i}\sin\theta^{i}\cos\phi^{i},E^{i}_{T,y}=E^{i}\sin\theta^{i}\sin\phi^{i} . Here E i E^{i} is the energy deposited in i t h i^{th} calorimeter cell and the angles θ i \theta^{i} and ϕ i \phi^{i} define the direction from the origin of the coordinate system to the i t h i^{th} calorimeter cell. We also define E T ≡ | E → T | \mbox{$\not\!\!E_{T}$}\equiv|\mbox{$\not\!\!\vec{E}_{T}$}|
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