Top quark mass measurement in the tt̅ all hadronic channel using a matrix element technique in pp̅ collisions at √s=1.96 TeV

We present a measurement of the top quark mass in the all-hadronic channel (\tt $\to$ \bb$q_{1}\bar{q_{2}}q_{3}\bar{q_{4}}$) using 943 pb$^{-1}$ of \ppbar collisions at $\sqrt {s} = 1.96$ TeV collected at the CDF II detector at Fermilab (CDF). We apply the standard model production and decay matrix-element (ME) to $\ttbar$ candidate events. We calculate per-event probability densities according to the ME calculation and construct template models of signal and background. The scale of the jet energy is calibrated using additional templates formed with the invariant mass of pairs of jets. These templates form an overall likelihood function that depends on the top quark mass and on the jet energy scale (JES). We estimate both by maximizing this function. Given 72 observed events, we measure a top quark mass of 171.1 $\pm$ 3.7 (stat.+JES) $\pm$ 2.1 (syst.) GeV/$c^{2}$. The combined uncertainty on the top quark mass is 4.3 GeV/$c^{2}$.

Measurement of the b-hadron production cross section using decays to μ-D0X final states in pp̅ collisions at √s=1.96 TeV

We report a measurement of the production cross section for b hadrons in pp̅ collisions at √s=1.96  TeV. Using a data sample derived from an integrated luminosity of 83  pb-1 collected with the upgraded Collider Detector (CDF II) at the Fermilab Tevatron, we analyze b hadrons, Hb, partially reconstructed in the semileptonic decay mode Hb→μ-D0X. Our measurement of the inclusive production cross section for b hadrons with transverse momentum pT>9  GeV/c and rapidity |y|<0.6 is σ=1.30  μb±0.05  μb(stat)±0.14  μb(syst)±0.07  μb(B), where the uncertainties are statistical, systematic, and from branching fractions, respectively. The differential cross sections dσ/dpT are found to be in good agreement with recent measurements of the Hb cross section and well described by fixed-order next-to-leading logarithm predictions.

Search for Exclusive Z-Boson Production and Observation of High-Mass pp̅ →pγγp̅ →pl+l-p̅ Events in pp̅ Collisions at √s=1.96 TeV

We present a search for exclusive Z boson production in proton-antiproton collisions at sqrt(s) = 1.96 TeV, using the CDF II detector at Fermilab. We observe no exclusive Z->ll candidates and place the first upper limit on the exclusive Z cross section in hadron collisions, sigma(exclu) gammagamma->p+ll+pbar, and measure the cross section for M(ll) > 40 GeV/c2 and |eta(l)|

Measurement of the tt̅ production cross section in 2 fb-1 of pp̅ collisions at √s=1.96 TeV using lepton plus jets events with soft muon b tagging

We present a measurement of the tt̅ production cross section in pp̅ collisions at √s=1.96  TeV using events containing a high transverse momentum electron or muon, three or more jets, and missing transverse energy. Events consistent with tt̅ decay are found by identifying jets containing candidate heavy-flavor semileptonic decays to muons. The measurement uses a CDF run II data sample corresponding to 2  fb-1 of integrated luminosity. Based on 248 candidate events with three or more jets and an expected background of 79.5±5.3 events, we measure a production cross section of 9.1±1.6  pb.

Search for new particles decaying into dijets in proton-antiproton collisions at √s=1.96 TeV

We present a search for new particles whose decays produce two jets (dijets) using proton-antiproton collision data corresponding to an integrated luminosity of 1.13 fb-1 collected with the CDF II detector. The measured dijet mass spectrum is found to be consistent with next-to-leading-order perturbative QCD predictions, and no significant evidence of new particles is found. We set upper limits at the 95% confidence level on cross sections times the branching fraction for the production of new particles decaying into dijets with both jets having a rapidity magnitude |y|

Search for new color-octet vector particle decaying to t tbar in p pbar collisions at sqrt{s} = 1.96 TeV

We present the result of a search for a massive color-octet vector particle, (e.g. a massive gluon) decaying to a pair of top quarks in proton-antiproton collisions with a center-of-mass energy of 1.96 TeV. This search is based on 1.9 fb$^{-1}$ of data collected using the CDF detector during Run II of the Tevatron at Fermilab. We study $t\bar{t}$ events in the lepton+jets channel with at least one $b$-tagged jet. A massive gluon is characterized by its mass, decay width, and the strength of its coupling to quarks. These parameters are determined according to the observed invariant mass distribution of top quark pairs. We set limits on the massive gluon coupling strength for masses between 400 and 800 GeV$/c^2$ and width-to-mass ratios between 0.05 and 0.50. The coupling strength of the hypothetical massive gluon to quarks is consistent with zero within the explored parameter space.

Study of the associated production of photons and b-quark jets in pp̅ collisions at √s=1.96 TeV

The cross section for photon production in association with at least one jet containing a $b$-quark hadron has been measured in proton antiproton collisions at $\sqrt{s}=1.96$ TeV. The analysis uses a data sample corresponding to an integrated luminosity of 340 pb$^{-1}$ collected with the CDF II detector. Both the differential cross section as a function of photon transverse energy $E_T^{\gamma}$, $d \sigma$($p \overline{p} \to \gamma + \geq 1 b$-jet)/$d E_T^{\gamma}$ and the total cross section $\sigma$($p \overline{p} \to \gamma + \geq 1 b$-jet; $E_T^{\gamma}> 20$ GeV) are measured. Comparisons to a next-to-leading order prediction of the process are presented.

Measurement of the b-hadron production cross section using decays to μ-D0X final states in pp̅ collisions at √s=1.96 TeV

We report a measurement of the production cross section for b hadrons in p-pbar collisions at sqrt{s}=1.96 TeV. Using a data sample derived from an integrated luminosity of 83 pb^-1 collected with the upgraded Collider Detector (CDF II) at the Fermilab Tevatron, we analyze b hadrons, H_b, partially reconstructed in the semileptonic decay mode H_b -> mu^- D^0 X. Our measurement of the inclusive production cross section for b hadrons with transverse momentum p_T > 9 GeV/c and rapidity |y|

Measurement of the tt̅ production cross section in 2 fb-1 of pp̅ collisions at √s=1.96 TeV using lepton plus jets events with soft muon b tagging

We present a measurement of the $\ttbar$ production cross section in $\ppbar$ collisions at $\sqrt{s}=1.96$ TeV using events containing a high transverse momentum electron or muon, three or more jets, and missing transverse energy. Events consistent with $\ttbar$ decay are found by identifying jets containing candidate heavy-flavor semileptonic decays to muons. The measurement uses a CDF Run II data sample corresponding to $2 \mathrm{fb^{-1}}$ of integrated luminosity. Based on 248 candidate events with three or more jets and an expected background of $79.5\pm5.3$ events, we measure a production cross section of $9.1\pm 1.6 \mathrm{pb}$.

Study of multi-muon events produced in p\bar{p} interactions at \sqrt{s}=1.96 TeV

We report the results of a study of multi-muon events produced at the Fermilab Tevatron collider and acquired with the CDF II detector using a dedicated dimuon trigger. The production cross section and kinematics of events in which both muon candidates are produced inside the beam pipe of radius 1.5 cm are successfully modeled by known processes which include heavy flavor production. In contrast, we are presently unable to fully account for the number and properties of the remaining events, in which at least one muon candidate is produced outside of the beam pipe, in terms of the same understanding of the CDF II detector, trigger, and event reconstruction.

Search for High-Mass e+e- Resonances in pp̅ Collisions at √s=1.96 TeV

A search for high-mass resonances in the $e^+e^-$ final state is presented based on 2.5 fb$^{-1}$ of $\sqrt{s}=$1.96 TeV $p\bar{p}$ collision data from the CDF II detector at the Fermilab Tevatron. The largest excess over the standard model prediction is at an $e^+e^-$ invariant mass of 240 GeV/$c^2$. The probability of observing such an excess arising from fluctuations in the standard model anywhere in the mass range of 150--1,000 GeV/$c^2$ is 0.6% (equivalent to 2.5 $\sigma$). We exclude the standard model coupling $Z'$ and the Randall-Sundrum graviton for $k/\overline{M}_{Pl}=0.1$ with masses below 963 and 848 GeV/$c^2$ at the 95% credibility level, respectively.

Improvement of electrical conductivity in Pb0.96-yMn0.04SnyTe alloys for high temperature thermoelectric applications

Lead-tin-telluride is a well-known thermoelectric material in the temperature range 350-750 K. Here, this alloy doped with manganese (Pb0.96-yMn0.04SnyTe) was prepared for different amounts of tin. X-ray diffraction showed a decrease of the lattice constant with increasing tin content, which indicated solid solution formation. Microstructural analysis showed a wide distribution of grain sizes from <1 mu m to 10 mm and the presence of a SnTe rich phase. All the transport properties were measured in the range of 300-720 K. The Seebeck coefficient showed that all the samples were p-type indicating holes as dominant carriers in the measurement range. The magnitude increased systematically on reduction of the Sn content due to possible decreasing hole concentration. Electrical conductivity showed the degenerate nature of the samples. Large values of the electrical conductivity could have possibly resulted from a large hole concentration due to a high Sn content and secondly, due to increased mobility by sp-d orbital interaction between the Pb1-ySnyTe sublattice and the Mn2+ ions. High thermal conductivity was observed due to higher electronic contribution, which decreased systematically with decreasing Sn content. The highest zT = 0.82 at 720 K was obtained for the alloy with the lowest Sn content (y = 0.56) due to the optimum doping level.

Micropropagacion de dos clones de caña de azucar (Saccharum sp.) ISA 96-110 e ISA 96-111

El presente estudio se realizó con el objetivo de desarrollar metodología para la micropropagación a partir de ápices caulinares, utilizando la técnica Spinder, y posteriormente aclimatación de las vitroplantas de dos clones de caña de azúcar (Saccharum sp.) (ISA 96-110 e ISA 96- 111). Se estudió el efecto que sobre el establecimiento tendrian 4 variantes del medio de cultivo MS (1962), suplidas con 0.0, 0.2 y 0.6 mg/1 de 6-BAP. Se utilizaron 15 réplicas por tratamiento. Se evaluó el efecto que sobre la brotación tuvieron 4 variantes del medio MS (1962), a las que se les adicionó 0.0, 0.1 y 0.5 mg/1 de 6 BAP durante tres subcultivos sucesivos. Se utilizaron 5 réplicas por variante en estudio. Para inducir el mayor enraizamiento se probaron 4 variantes líquidas del medio MS ( 1962), suplidas con 0.0, 1.0 y 1.6 mg/1 de AlA. Para el estudio de aclimatación se emplearon 30 plantas por cultivar y se establecieron en un sustrato de lombrices Californiana (Eisenia foetida). El clon ISA 96-110 presentó mayor porcentaje de fenolización y menor curvatura que el clon ISA 96-111. El medio de cultivo MS + 0.60 m g/1 de 6-BAP indujo al menor porcentaje de fenolización (33.0) y mayor de curvatura (60.0) en el clon ISA 96-110, el medio MS + 0.20 mg/1 de 6- BAP en el clon ISA 96-111. La sobrevivencia de las plantas del clon ISA- 111 fue de 100 % en todos los medios de cultivo, para el ISA 96-11O sólo los medios MS + 0.20 y MS + 0.00 mg/1 de 6-BAP. No hubo aumento de los valores de las variables altura de la planta, número de brotes y de hojas con el aumento del número de subcultivos. El medio de cultivo que indujo mayor brotación para el clon ISA 96-11 O fue el MS + 0.30 mg/1, mientras que para el clon ISA 96-111 fue el MS + 0.1 mg/1 de 6- BAP. El clon ISA 96-111 reportó resultados superiores en longitud (5.75 cm) y número de raices (7.4) por planta. El medio de cultivo MS + 1.3 mg/1 de AlA indujo los mejores resultados en ambos clones. El comportamiento de las plantas del clon ISA 96-1 11 fueron superiores a las del clon ISA 96-11O al momento de la aclimatación

Tolerancia del híbrido de sorgo (Sorghum bicolor (L) Moench) H 89-96 a diferentes niveles de daños causados por enfermedades foliares durante la etapa vegetativa, postrera 2006

Con el objetivo de evaluar diferentes niveles de daños causados por enfermedades foliares en la etapa vegetativa de sorgo hibrido H 89-96 y su efecto en el rendimiento durante la época de postrera, se estableció este experimento en tierras que fueron alquiladas por el productor Agapito Ñurinda ubicada en el km 43 carretera Tipitapa Masaya, del departamento de Managua a 12° 08'36"de latitud norte y 86° 09' 49"de longitud oeste, Se utilizó un diseño con bloques completos al azar (BCA), Los tratamientos consistieron en aplicaciones de Benomyl con tres niveles de severidad de enfermedades; siendo el tratamiento uno con 3%, tratamiento dos con 7% tratamiento tres con 20% de severidad. El tratamiento T4 es el testigo al cual no se hizo aplicación alguna. Se realizaron aplicaciones calendarizadas para cogollero con Cypermetrina cada ocho días durante la etapa vegetativa y protección a la panoja con Cypermetrina y Benomyl al inicio de la floración para todos los tratamientos. La toma de datos para la severidad de enfermedades foliares fue basada en la escala de Takhur, utilizando cinco sitios al azar y registrando 10 plantas consecutivas por sitio. Los datos se procesaron mediante el análisis de varianza, para todas las variables evaluadas. No se presentaron condiciones climáticas favorables, para el desarrollo de las enfermedades que comúnmente afectan al cultivo del sorgo, no obstante la antracnosis (Colletotrichum graminicola (ces) G.W.Wison), se presentó en el híbrido de sorgo no alcanzado el 20 % de nivel de daño en estudio. El efecto de la aplicación de fungicida para antracnosis no mostró diferencia estadística entre tratamientos. La enfermedad no superó el 7% de severidad, durante la etapa vegetativa. Durante la etapa reproductiva, las condiciones ambientales favorecieron la incidencia de mohos en un período corto no mostrando diferencias estadísticas significativas. El acame se presentó hasta el momento de cosecha no llegando a tener significancia estadísticas en los tratamientos. Para la variable rendimiento el análisis de varianza no mostró diferencias significativas, sin embargo, los mayores rendimientos se obtuvieron en el T1 (3 % severidad) y T3 con 6 149, 01kg ha¹ y 5 389, 80kg ha¹ respectivamente. El análisis económico indicó que el T1 presentó mayor rentabilidad con un 0.55 %.