Fetching the paper…
Reading the bibliography…
We present the result of a search for a massive color-octet vector particle, (e.g.
K. J. F. Gaemers and F. Hoogeveen, Phys. Lett. B 146 (1984) 347
1984
Earlier work this paper cites.
K. Kondo, J. Phys. Soc. Jpn. 57 (1988) 4126; K. Kondo, hep-ex/0508035
1988
Earlier work this paper cites.
G. Marchesini and B.R. Webber, Nucl. Phys. B 310 (1988) 461; G. Marchesini et al
1992
Earlier work this paper cites.
C.T. Hill and S.J. Parke, Phys. Rev. D 49 (1994) 4454
1994
Earlier work this paper cites.
D. Dicus, A. Stange and S. Willenbrock, Phys. Lett. B 333 (1994) 126
1994
Earlier work this paper cites.
C.T. Hill, Phys. Lett. B 345 (1995) 483
1995
Earlier work this paper cites.
A. D. Martin et al
1995
Earlier work this paper cites.
A. Leike, Phys. Rept. 317 (1999) 143
1999
Earlier work this paper cites.
T. G. Rizzo, Phys. Rev. D 61 (2000) 055005
2000
Earlier work this paper cites.
T. Sjöstrand et al
2001
Cited alongside, same era.
J. Pumplin et al
2002
Cited alongside, same era.
S. Frixione et al
2002
Cited alongside, same era.
M.L. Mangano et al
2003
Cited alongside, same era.
V. M. Abazov et al
2004
Cited alongside, same era.
M. Cacciari et al
2004
Cited alongside, same era.
D. Acosta et al
2005
Cited alongside, same era.
A. Bhatti et al
2006
Cited alongside, same era.
A. Abulencia et al
2006
Later among the works it cites.
2006
Later among the works it cites.
B. Lillie, L. Randall, L.-T. Wang, J. High Energy Phys. 09 (2007) 074
2007
Later among the works it cites.
A. Abulencia et al
2007
Later among the works it cites.
T. Aaltonen et al
2008
Later among the works it cites.
T. Aaltonen et al
2008
Later among the works it cites.
T. M. Abazov et al
2008
Later among the works it cites.
alphaXiv searches the wider corpus for related work and actual follow-ups.
alphaXiv is searching for related work…
We use a coordinate system defined about the proton beam direction, which is taken as the z z axis; the x x axis lies in the horizontal plane. Then θ \theta is the usual polar angle and ϕ \phi is the azimuthal angle. We define the pseudorapidity η \eta of a particle’s three-momentum as η ≡ − ln ( tan θ 2 ) \eta\equiv-\ln(\tan\frac{\theta}{2}) . The transverse energy and momentum are defined as E T = E sin θ E_{T}=E\sin\theta and p T = p sin θ p_{T}=p\sin\theta where E E is the energy measured by the calorimeter and p p is the momentum measured in the tracking system. The missing transverse energy is defined as E T = | − ∑ i E T i n → i | \not\!\!E_{T}=|-\sum_{i}E_{T}^{i}\vec{n}_{i}| where n → i \vec{n}_{i} is a unit vector in the transverse plane that points from the event vertex to the azimuth of the i th i^{\rm th} calorimeter tower
Cited in the paper.
T. Affolder et al
2062
Closest in time.