72 research outputs found
Measurement of the top quark mass using the matrix element technique in dilepton final states
We present a measurement of the top quark mass in pp¯ collisions at a center-of-mass energy of 1.96 TeV at the Fermilab Tevatron collider. The data were collected by the D0 experiment corresponding to an integrated luminosity of 9.7  fb−1. The matrix element technique is applied to tt¯ events in the final state containing leptons (electrons or muons) with high transverse momenta and at least two jets. The calibration of the jet energy scale determined in the lepton+jets final state of tt¯ decays is applied to jet energies. This correction provides a substantial reduction in systematic uncertainties. We obtain a top quark mass of mt=173.93±1.84  GeV
Predicting site index from climate and soil variables for cork oak (Quercus suber L.) stands in Portugal
Site productivity, assessed through site index, was modelled using partial least
squares regression as a function of soil and climatic variables. Two alternative models were
developed: a full model, considering all available explanatory variables, and a reduced
model, considering only variables that can be obtained without digging a soil pit. The
reduced model was used for mapping the site index distribution in Portugal, on the basis of
existing digital cartography available for the whole country. The developed models indicate
the importance of water availability and soil water holding capacity for site index
value distribution. Site index was related to climate, namely evaporation and frost, and soil
characteristics such as lithology, soil texture, soil depth, thickness of the A horizon and soil
classification. The variability of the estimated values within the map (9.5–16.8 m with an
average value of 13.4 m) reflects the impact of soil characteristics on the site productivity
estimation. These variables should be taken into consideration during the establishment of
new plantations of cork oak, and management of existing plantations. Results confirm the
potential distribution of cork oak in coastal regions. They also suggest the existence of a
considerable area, located both North and South of the Tagus river, where site indices
values of medium (]13;15]) to high (]15;17]) productivity classes may be expected. The
species is then expected to be able to have good productivity along the northern coastal
areas of Portugal, where presently it is not a common species but where, according to
historical records, it occurred until the middle of the sixteenth century. The present
research focused on tree growth. Cork growth and cork quality distribution needs to be
further researched through the establishment of long term experimental sites along the distribution area of cork oak, namely in the central and northern coastal areas of the
countryinfo:eu-repo/semantics/publishedVersio
A hypofractionated radiation regimen avoids the lymphopenia associated with neoadjuvant chemoradiation therapy of borderline resectable and locally advanced pancreatic adenocarcinoma
Studies of X(3872) and ψ(2S) production in p\bar{p}over-bar collisions at 1.96 TeV
We present various properties of the production of the X (3872) and ψ(2S) states based on 10.4fb‾¹ collected by the D0 experiment in Tevatron p\bar{p} collisions at \sqrt{s} = 1.96 TeV. For both states, we measure the nonprompt fraction fNP of the inclusive production rate due to decays of b-flavored hadrons. We find the fNP values systematically below those obtained at the LHC. The fNP fraction for ψ(2S) increases with transverse momentum, whereas for the X(3872) it is constant within large uncertainties, in agreement with the LHC results. The ratio of prompt to nonprompt ψ(2S) production, (1 - fNP)/fNP, decreases only slightly going from the Tevatron to the LHC, but for the X(3872), this ratio decreases by a factor of about 3. We test the soft-pion signature of the X(3872) modeled as a weakly bound charm-meson pair by studying the production of the X(3872) as a function of the kinetic energy of the X(3872) and the pion in the X(3872) π center-of-mass frame. For a subsample consistent with prompt production, the results are incompatible with a strong enhancement in the production of the X(3872) at the small kinetic energy of the X(3872) and the π in the X(3872)π center-of-mass frame expected for the X + soft-pion production mechanism. For events consistent with being due to decays of hadrons, there is no significant evidence for the soft-pion effect, but its presence at the level expected for the binding energy of 0.17 MeV and the momentum scale Λ = M(π) is not ruled out
Properties of Z±c(3900) produced in pp¯ collisions
We study the production of the exotic charged charmoniumlike state
Z
±
c
(
3900
)
in
p
¯
p
collisions through the sequential process
ψ
(
4260
)
→
Z
±
c
(
3900
)
Ï€
∓
,
Z
±
c
(
3900
)
→
J
/
ψ
Ï€
±
. Using the subsample of candidates originating from semi-inclusive weak decays of
b
-flavored hadrons, we measure the invariant mass and natural width to be
M
=
3902.6
+
5.2
−
5.0
(
stat
)
+
3.3
−
1.4
(
syst
)
 
 
MeV
and
Γ
=
3
2
+
28
−
21
(
stat
)
+
26
−
7
(
syst
)
 
 
MeV
, respectively. We search for prompt production of the
Z
±
c
(
3900
)
through the same sequential process. No significant signal is observed, and we set an upper limit of 0.70 at the 95% credibility level on the ratio of prompt production to the production via
b
-hadron decays. The study is based on
10.4
 
 
f
b
−
1
of
p
¯
p
collision data collected by the D0 experiment at the Fermilab Tevatron collider
Combined Tevatron upper limit on gg->H->W+W- and constraints on the Higgs boson mass in fourth-generation fermion models
Report number: FERMILAB-PUB-10-125-EWe combine results from searches by the CDF and D0 collaborations for a standard model Higgs boson (H) in the process gg->H->W+W- in p=pbar collisions at the Fermilab Tevatron Collider at sqrt{s}=1.96 TeV. With 4.8 fb-1 of integrated luminosity analyzed at CDF and 5.4 fb-1 at D0, the 95% Confidence Level upper limit on \sigma(gg->H) x B(H->W+W-) is 1.75 pb at m_H=120 GeV, 0.38 pb at m_H=165 GeV, and 0.83 pb at m_H=200 GeV. Assuming the presence of a fourth sequential generation of fermions with large masses, we exclude at the 95% Confidence Level a standard-model-like Higgs boson with a mass between 131 and 204 GeV.We combine results from searches by the CDF and D0 collaborations for a standard model Higgs boson (H) in the process gg→H→W+W- in pp̅ collisions at the Fermilab Tevatron Collider at √s=1.96  TeV. With 4.8  fb-1 of integrated luminosity analyzed at CDF and 5.4  fb-1 at D0, the 95% confidence level upper limit on σ(gg→H)×B(H→W+W-) is 1.75 pb at mH=120  GeV, 0.38 pb at mH=165  GeV, and 0.83 pb at mH=200  GeV. Assuming the presence of a fourth sequential generation of fermions with large masses, we exclude at the 95% confidence level a standard-model-like Higgs boson with a mass between 131 and 204 GeV.Peer reviewe
Combination of D0 measurements of the top quark mass
We present a combination of measurements of the top quark mass by the D0 experiment in the lepton+jets and dilepton channels. We use all the data collected in Run I (1992–1996) at √s=1.8  TeV and Run II (2001–2011) at √s=1.96  TeV of the Tevatron p¯p collider, corresponding to integrated luminosities of 0.1  fb−1 and 9.7  fb−1, respectively. The combined result is: mt=174.95±0.40(stat)±0.64(syst)  GeV=174.95±0.75  GeV
The Suspensor is a Major Route of Nutrients into Pro embryo, Globular and Heart Stage Phaseolus vulgaris Embryos
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