Il fantastico in alcune espressioni idiomatiche italiane: applicazione didattica

A seconda dei loro significati e riferimenti, le e.i. costituiscono un luogo di incontro tra passato e presente, tradizione e innovazone. Possiamo dire che all’interno della loro struttura si rivelano come frasi da ricordare, come luogo dove ogni generazione lascia tracce e può ritrovare se stessa. È possibile condividere la vitalità della lingua e dei suoi usi figurati tanto come divertimento quanto per lo studio della lingua e cultura. In altre parole le e.i., servono per scoprire l’immaginario mitico, leggendario e le loro trasformazioni attraverso la storia. Sono di uso frequente in letteratura, in tutti i livelli del linguaggio ma anche nel discorso quotidiano. Costituiscono il modo di “parlar coperto”, cioè il riferimento che non nomina espressamente l’oggetto del discorso, ma lo richiama recuperando elementi propri del suo contesto storico, sociale o culturale. Diventano così determinanti per la comprensione dello slittamento dal reale al fantastico. Come utenti ed enunciatori delle e.i., in qualsiasi lingua, l’avvio va prima dal reale al fantastico e, al contrario, quali interpretanti passiamo dal fantastico al reale. Il nostro proposito è allenare e accrescere la competenza enciclopedica a scopo didattico. Questo è in diretto rapporto con la memoria collettiva e l’immaginario linguisto-culturale che spesso nasconde anche in parole comuni lo slittamento di significati originati da complessi processi cognitivi prevalentemente inconsci. A scopo didattico si partirà da una scelta di e.i. del corpus già elicitato e si presenterà prima un profilo dei tratti del fantastico in genere per poi classificare le e.i. a seconda delle loro caratteristiche e dell’immaginario collettivo che richiamano

Azimuthal anisotropy of charged jet production in root s(NN)=2.76 TeV Pb-Pb collisions

We present measurements of the azimuthal dependence of charged jet production in central and semi-central root s(NN) = 2.76 TeV Pb-Pb collisions with respect to the second harmonic event plane, quantified as nu(ch)(2) (jet). Jet finding is performed employing the anti-k(T) algorithm with a resolution parameter R = 0.2 using charged tracks from the ALICE tracking system. The contribution of the azimuthal anisotropy of the underlying event is taken into account event-by-event. The remaining (statistical) region-to-region fluctuations are removed on an ensemble basis by unfolding the jet spectra for different event plane orientations independently. Significant non-zero nu(ch)(2) (jet) is observed in semi-central collisions (30-50% centrality) for 20 <p(T)(ch) (jet) <90 GeV/c. The azimuthal dependence of the charged jet production is similar to the dependence observed for jets comprising both charged and neutral fragments, and compatible with measurements of the nu(2) of single charged particles at high p(T). Good agreement between the data and predictions from JEWEL, an event generator simulating parton shower evolution in the presence of a dense QCD medium, is found in semi-central collisions. (C) 2015 CERN for the benefit of the ALICE Collaboration. Published by Elsevier B.V. This is an open access article under the CC BY license (http://creativecommons.org/licenses/by/4.0/).Peer reviewe

Production of He-4 and (4) in Pb-Pb collisions at root(NN)-N-S=2.76 TeV at the LHC

Results on the production of He-4 and (4) nuclei in Pb-Pb collisions at root(NN)-N-S = 2.76 TeV in the rapidity range vertical bar y vertical bar <1, using the ALICE detector, are presented in this paper. The rapidity densities corresponding to 0-10% central events are found to be dN/dy4(He) = (0.8 +/- 0.4 (stat) +/- 0.3 (syst)) x 10(-6) and dN/dy4 = (1.1 +/- 0.4 (stat) +/- 0.2 (syst)) x 10(-6), respectively. This is in agreement with the statistical thermal model expectation assuming the same chemical freeze-out temperature (T-chem = 156 MeV) as for light hadrons. The measured ratio of (4)/He-4 is 1.4 +/- 0.8 (stat) +/- 0.5 (syst). (C) 2018 Published by Elsevier B.V.Peer reviewe

Forward-central two-particle correlations in p-Pb collisions at root s(NN)=5.02 TeV

Two-particle angular correlations between trigger particles in the forward pseudorapidity range (2.5 2GeV/c. (C) 2015 CERN for the benefit of the ALICE Collaboration. Published by Elsevier B. V.Peer reviewe

Event-shape engineering for inclusive spectra and elliptic flow in Pb-Pb collisions at root(NN)-N-S=2.76 TeV

Peer reviewe

Elliptic flow of muons from heavy-flavour hadron decays at forward rapidity in Pb-Pb collisions at root s(NN)=2.76TeV

The elliptic flow, v(2), of muons from heavy-flavour hadron decays at forward rapidity (2.5 <y <4) is measured in Pb-Pb collisions at root s(NN)= 2.76TeVwith the ALICE detector at the LHC. The scalar product, two- and four-particle Q cumulants and Lee-Yang zeros methods are used. The dependence of the v(2) of muons from heavy-flavour hadron decays on the collision centrality, in the range 0-40%, and on transverse momentum, p(T), is studied in the interval 3 <p(T)<10 GeV/c. A positive v(2) is observed with the scalar product and two-particle Q cumulants in semi-central collisions (10-20% and 20-40% centrality classes) for the p(T) interval from 3 to about 5GeV/c with a significance larger than 3 sigma, based on the combination of statistical and systematic uncertainties. The v(2) magnitude tends to decrease towards more central collisions and with increasing pT. It becomes compatible with zero in the interval 6 <p(T)<10 GeV/c. The results are compared to models describing the interaction of heavy quarks and open heavy-flavour hadrons with the high-density medium formed in high-energy heavy-ion collisions. (C) 2015 CERN for the benefit of the ALICE Collaboration. Published by Elsevier B.V.Peer reviewe

Pseudorapidity and transverse-momentum distributions of charged particles in proton-proton collisions at root s=13 TeV

The pseudorapidity (eta) and transverse-momentum (p(T)) distributions of charged particles produced in proton-proton collisions are measured at the centre-of-mass energy root s = 13 TeV. The pseudorapidity distribution in vertical bar eta vertical bar <1.8 is reported for inelastic events and for events with at least one charged particle in vertical bar eta vertical bar <1. The pseudorapidity density of charged particles produced in the pseudorapidity region vertical bar eta vertical bar <0.5 is 5.31 +/- 0.18 and 6.46 +/- 0.19 for the two event classes, respectively. The transverse-momentum distribution of charged particles is measured in the range 0.15 <p(T) <20 GeV/c and vertical bar eta vertical bar <0.8 for events with at least one charged particle in vertical bar eta vertical bar <1. The evolution of the transverse momentum spectra of charged particles is also investigated as a function of event multiplicity. The results are compared with calculations from PYTHIA and EPOS Monte Carlo generators. (C) 2015 CERN for the benefit of the ALICE Collaboration. Published by Elsevier B.V. This is an open access article under the CC BY license (http://creativecommons.org/licenses/by/4.0/).Peer reviewe

Centrality evolution of the charged-particle pseudorapidity density over a broad pseudorapidity range in Pb-Pb collisions at root s(NN)=2.76TeV

Peer reviewe

Efeito de níveis crescentes de uréia na dieta de vacas em lactação sobre a produção e a composição físico-química do leite Effect of increasing dietary urea levels on milk yield and composition of lactating cows

Avaliou-se o efeito de níveis crescentes de uréia na dieta de vacas em lactação sobre a produção e composição físico-química do leite. Foram utilizadas nove vacas holandesas em lactação, distribuídas em três quadrados latinos 3 x 3, com três tratamentos e três períodos de coleta. O experimento teve duração de 63 dias, divididos em três períodos de 21 dias. Os tratamentos consistiram de uma dieta controle, formulada para suprir 100% das exigências de PB, proteína degradável no rúmen (PDR) e proteína não-degradável no rúmen (PNDR), composta de farelo de soja como principal fonte protéica e cana-de-açúcar como volumoso, e de duas outras dietas, semelhantes à dieta controle, mas com 0,75 ou 1,5% de uréia em substituição ao farelo de soja. As dietas foram isoenergéticas (1,53 Mcal/kg de energia líquida de lactação) e isoprotéicas (16% de PB). Quando os resultados foram analisados por regressão polinomial simples, não houve efeitos das dietas sobre o consumo de MS, as produções de leite e de leite corrigida para 3,5% de gordura, os teores de proteína e gordura e a contagem de células somáticas do leite. Os níveis de substituição do farelo de soja por uréia não influenciaram o pH, a crioscopia ou a densidade do leite. No entanto, verificou-se efeito linear decrescente dos níveis de uréia na dieta sobre a acidez do leite. Os teores de proteína, gordura, lactose, uréia, extrato seco total e extrato seco desengordurado não foram afetados pelas dietas. Os resultados deste estudo sugerem que o uso de até 1,5% de uréia na MS da dieta de vacas em lactação não altera a produção, a composição e as características físico-químicas do leite.<br>The objective of this trial was to evaluate the effects of three different dietary levels of urea on milk yield and composition. Nine lactating Holstein cows were randomly assigned to three replicated 3 x 3 Latin squares with three periods of 21 days each. Treatments were: A) control diet formulated to meet 100% of the requirements of crude protein (CP), rumen undegradable protein (RUP) and rumen degradable protein (RDP) according to the NRC (2001) model by feeding soybean meal and sugar cane; B) replacing soybean meal with 0.75% urea; or C) replacing soybean meal with 1.5% urea. Diets were formulated to be isonitrogenous (16% CP) and isocaloric (1.53 Mcal/kg of NEl). No significant differences in dry matter intake, milk yield, 3.5% fat corrected milk, yields of milk protein and milk fat, and somatic cell count were observed among treatments when data were analyzed by simple polynomial regression. Milk cryoscopy, pH and density were also not affected by increasing the proportion of urea in the diet treatments; however, milk acidity decreased linearly when the levels of urea were increased in the diet. Milk contents of protein, fat, lactose, total solids and non-solids fat and concentration of milk urea all did not differ across diets. Results obtained in this trial indicated that the inclusion of up to 1.5% of urea (% of diet DM) in the diet had no effect on milk yield, milk composition, and milk physical-chemical characteristics in lactating cows

燒津鰹漁業に於ける船仲組織(上) - 本邦漁業に特異なる勞働組織の一例 -

We report on the measurement of freeze-out radii for pairs of identical-charge pions measured in Pb-Pb collisions at √sNN = 2.76 TeV as a function of collision centrality and the average transverse momentum of the pair kT. Three-dimensional sizes of the system (femtoscopic radii), as well as direction-averaged onedimensional radii are extracted. The radii decrease with kT, following a power-law behavior. This is qualitatively consistent with expectations from a collectively expanding system, produced in hydrodynamic calculations. The radii also scale linearly with _dNch/dη_1/3. This behavior is compared to world data on femtoscopic radii in heavy-ion collisions. While the dependence is qualitatively similar to results at smaller √sNN, a decrease in the ratio Rout/Rside is seen, which is in qualitative agreement with a specific prediction from hydrodynamic models: a change from inside-out to outside-in freeze-out configuration. The results provide further evidence for the production of a collective, strongly coupled system in heavy-ion collisions at the CERN Large Hadron Collider