796 research outputs found
Ocular surface squamous neoplasia among HIV-infected patients in Botswana
Background. Ocular surface squamous neoplasia (OSSN) is a group of ocular tumours that has been rising in incidence among HIVinfected individuals in sub-Saharan Africa. Surgical excision is the mainstay of treatment for OSSN in this region.Methods. This retrospective cohort study examined the clinical characteristics and treatment modalities used for 468 patients with OSSN from a large tertiary referral center in Gaborone, Botswana, over a 10-year period from 1998 to 2008.Results. The estimated annual incidence of OSSN in Botswana reached a peak of 7.0 cases per 100 000 persons per year in 2004. The mean age of the patients in the study was 38 years (interquartile range 30 - 44), and 53.9% were women. Of the patients, 48.5% were known to be HIV-infected, 1.5% were HIV-uninfected, and 50.0% had unknown HIV status. Among HIV-infected patients with CD4 counts, the median CD4 count was 192 cells/ìL. As initial OSSN treatment, 20.7% of patients received simple surgical excision, 70.9% received surgical excision with adjunctive beta radiation, 0.9% received evisceration, 1.3% received enucleation, and 6.2% underwent surgical removal of unknown type. The overall rate of known recurrence was 7.1%; however, among those with at least 6 months of follow-up, the recurrence rate was 24.2%. Rates of known recurrence after simple surgical excision and surgical excision with adjunctive beta-radiation were 10.3% and 5.4%, respectively.Conclusion. This study confirms the high incidence of OSSN among young individuals in Botswana. Further investigation is warranted to determine the most effective treatment modalities to prevent recurrence of OSSN among patients in sub-Saharan Africa
Carbon Monoxide Effects on Electrophysiological Mechanisms of Ventricular Arrhythmogenesis
Increased dissolved carbon monoxide decreases ICa,L IK1 and IKr, and increases late INa currents in rat and guinea pig patch-clamped isolated ventricular myocytes. Action potentials are prolonged. These effects are reproduced by scaling the currents in the Gattoni et al., 2016 (rat) and Luo and Rudy, 1994 (guinea-pig) cell models. Using the same scaling of currents in the O’Hara-Rudy (2011) models the endo-, mid-myo- and epi-cardial APD90 is prolonged. CO abolishes alternans in endo-, and induces alternans in mid-myo -cardial cell models at cycle lengths < 280ms. In the homogenous human ventricular tissue models these CO effects decrease epi-, endocardial conduction velocities from 0.4 to 0.32m/s, and increase the widths of the vulnerable windows by +9%, +8% . In the ventricular wall model (a third each of endo-, mid-myo- and epicardial) CO increased transmural propagation times from 44 to 55 ms and maximal difference in propagating APD from 68 to 73 ms. The computed effects of CO on human ventricular tissue are pro-arrhythmogenic
Porosity of closed carbon nanotubes compressed using hydraulic pressure
Experimental data of nitrogen adsorption (T = 77.3 K) from gaseous phase measured on commercial closed carbon nanotubes are presented. Additionally, we show the results of N2 adsorption on compressed (using hydraulic press) CNTs. In order to explain the experimental observations the results of GCMC simulations of N2 adsorption on isolated or bundled multi-walled closed nanotubes (four models of bundles) are discussed. We show that the changes of the experimental adsorption isotherms are related to the compression of the investigated adsorbents. They are qualitatively similar to the theoretical observations. Taking into account all results it is concluded that in the "architecture" of nanotubes very important role has been played by isolated nanotubes
Study of the reaction e^{+}e^{-} -->J/psi\pi^{+}\pi^{-} via initial-state radiation at BaBar
We study the process with
initial-state-radiation events produced at the PEP-II asymmetric-energy
collider. The data were recorded with the BaBar detector at center-of-mass
energies 10.58 and 10.54 GeV, and correspond to an integrated luminosity of 454
. We investigate the mass
distribution in the region from 3.5 to 5.5 . Below 3.7
the signal dominates, and above 4
there is a significant peak due to the Y(4260). A fit to
the data in the range 3.74 -- 5.50 yields a mass value
(stat) (syst) and a width value (stat)(syst) for this state. We do not
confirm the report from the Belle collaboration of a broad structure at 4.01
. In addition, we investigate the system
which results from Y(4260) decay
Diffractive Dijet Production at sqrt(s)=630 and 1800 GeV at the Fermilab Tevatron
We report a measurement of the diffractive structure function of
the antiproton obtained from a study of dijet events produced in association
with a leading antiproton in collisions at GeV at the
Fermilab Tevatron. The ratio of at GeV to
obtained from a similar measurement at GeV is compared with
expectations from QCD factorization and with theoretical predictions. We also
report a measurement of the (-Pomeron) and ( of parton in
Pomeron) dependence of at GeV. In the region
, GeV and , is
found to be of the form , which obeys
- factorization.Comment: LaTeX, 9 pages, Submitted to Phys. Rev. Letter
A Study of B0 -> J/psi K(*)0 pi+ pi- Decays with the Collider Detector at Fermilab
We report a study of the decays B0 -> J/psi K(*)0 pi+ pi-, which involve the
creation of a u u-bar or d d-bar quark pair in addition to a b-bar -> c-bar(c
s-bar) decay. The data sample consists of 110 1/pb of p p-bar collisions at
sqrt{s} = 1.8 TeV collected by the CDF detector at the Fermilab Tevatron
collider during 1992-1995. We measure the branching ratios to be BR(B0 -> J/psi
K*0 pi+ pi-) = (8.0 +- 2.2 +- 1.5) * 10^{-4} and BR(B0 -> J/psi K0 pi+ pi-) =
(1.1 +- 0.4 +- 0.2) * 10^{-3}. Contributions to these decays are seen from
psi(2S) K(*)0, J/psi K0 rho0, J/psi K*+ pi-, and J/psi K1(1270)
Search for Kaluza-Klein Graviton Emission in Collisions at TeV using the Missing Energy Signature
We report on a search for direct Kaluza-Klein graviton production in a data
sample of 84 of \ppb collisions at = 1.8 TeV, recorded
by the Collider Detector at Fermilab. We investigate the final state of large
missing transverse energy and one or two high energy jets. We compare the data
with the predictions from a -dimensional Kaluza-Klein scenario in which
gravity becomes strong at the TeV scale. At 95% confidence level (C.L.) for
=2, 4, and 6 we exclude an effective Planck scale below 1.0, 0.77, and 0.71
TeV, respectively.Comment: Submitted to PRL, 7 pages 4 figures/Revision includes 5 figure
Measurement of the average time-integrated mixing probability of b-flavored hadrons produced at the Tevatron
We have measured the number of like-sign (LS) and opposite-sign (OS) lepton
pairs arising from double semileptonic decays of and -hadrons,
pair-produced at the Fermilab Tevatron collider. The data samples were
collected with the Collider Detector at Fermilab (CDF) during the 1992-1995
collider run by triggering on the existence of and candidates
in an event. The observed ratio of LS to OS dileptons leads to a measurement of
the average time-integrated mixing probability of all produced -flavored
hadrons which decay weakly, (stat.)
(syst.), that is significantly larger than the world average .Comment: 47 pages, 10 figures, 15 tables Submitted to Phys. Rev.
Jet energy measurement with the ATLAS detector in proton-proton collisions at root s=7 TeV
The jet energy scale and its systematic uncertainty are determined for jets measured with the ATLAS detector at the LHC in proton-proton collision data at a centre-of-mass energy of √s = 7TeV corresponding to an integrated luminosity of 38 pb-1. Jets are reconstructed with the anti-kt algorithm with distance parameters R=0. 4 or R=0. 6. Jet energy and angle corrections are determined from Monte Carlo simulations to calibrate jets with transverse momenta pT≥20 GeV and pseudorapidities {pipe}η{pipe}<4. 5. The jet energy systematic uncertainty is estimated using the single isolated hadron response measured in situ and in test-beams, exploiting the transverse momentum balance between central and forward jets in events with dijet topologies and studying systematic variations in Monte Carlo simulations. The jet energy uncertainty is less than 2. 5 % in the central calorimeter region ({pipe}η{pipe}<0. 8) for jets with 60≤pT<800 GeV, and is maximally 14 % for pT<30 GeV in the most forward region 3. 2≤{pipe}η{pipe}<4. 5. The jet energy is validated for jet transverse momenta up to 1 TeV to the level of a few percent using several in situ techniques by comparing a well-known reference such as the recoiling photon pT, the sum of the transverse momenta of tracks associated to the jet, or a system of low-pT jets recoiling against a high-pT jet. More sophisticated jet calibration schemes are presented based on calorimeter cell energy density weighting or hadronic properties of jets, aiming for an improved jet energy resolution and a reduced flavour dependence of the jet response. The systematic uncertainty of the jet energy determined from a combination of in situ techniques is consistent with the one derived from single hadron response measurements over a wide kinematic range. The nominal corrections and uncertainties are derived for isolated jets in an inclusive sample of high-pT jets. Special cases such as event topologies with close-by jets, or selections of samples with an enhanced content of jets originating from light quarks, heavy quarks or gluons are also discussed and the corresponding uncertainties are determined. © 2013 CERN for the benefit of the ATLAS collaboration
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