Fetching the paper…
Reading the bibliography…
We present the results of a search for Higgs bosons predicted in two-Higgs-doublet models, in the case where the Higgs bosons decay to tau lepton pairs, using 1.8 inverse fb of integrated luminosity of proton-antiproton collisions recorded by the CDF II experiment at the Fermilab Tevatron.
P. W. Higgs, Phys. Lett. 12
1966
Earlier work this paper cites.
S. L. Glashow and S. Weinberg, Phys. Rev. D 15
1979
Earlier work this paper cites.
R. Brun and F. Carminati, CERN Programming Library Long Writeup W5013 (1993)
1993
Earlier work this paper cites.
S. Dawson, A. Djouadi, and M. Spira, Phys. Rev. Lett. 77
1996
Earlier work this paper cites.
S.P. Martin, arXiv:hep-ph/9709356 (1997), and references therein
1997
Earlier work this paper cites.
H.L. Lai et al
2000
Earlier work this paper cites.
T. Sjöstrand et al
2001
Earlier work this paper cites.
Z. Was et al
2001
Earlier work this paper cites.
J. Pumplin et al
2002
Cited alongside, same era.
F. Maltoni, Z. Sullivan, and S. Willenbrock, Phys. Rev. D 67
2003
Cited alongside, same era.
S. Klimenko, J. Konigsberg, and T.M. Liss, FERMILAB-FN-0741 (2003)
2003
Cited alongside, same era.
M. Carena et al
2003
Cited alongside, same era.
A. Anastassov et al
2004
Cited alongside, same era.
D. H. J. Chung et al
2005
Cited alongside, same era.
D. Acosta et al
2005
Cited alongside, same era.
A. Abulencia et al
2005
Later among the works it cites.
A. Abulencia et al
2006
Later among the works it cites.
S. Schael et al
2006
Later among the works it cites.
M. Carena et al
2006
Later among the works it cites.
A. Abulencia et al
2007
Later among the works it cites.
C. Cuenca Almenar, Search for the neutral MSSM Higgs bosons in the τ τ \tau\tau decay channels at CDF Run II
2008
Later among the works it cites.
V. 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 and the y y axis points upward. Then θ \theta is the usual polar 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 | \,/\!\!\!\!E_{T}=|-\sum_{i}E_{T}^{i}\vec{n}_{i}| where n → i \vec{n}_{i} is a unit vector perpendicular to the beam axis and pointing from the beam axis to the i th i^{\rm th} calorimeter tower
Cited in the paper.