Hitos Demográficos del Siglo XXI: Migración Internacional

La migración ha sido una constante en la historia mundial. Sin embargo, las migraciones que han tenido lugar desde principios del siglo XXI no tienen precedentes, ya que recientemente éstas han alcanzado su mayor volumen en la historia y presentan características que las diferencian de las observadas en periodos anteriores, lo que ha propiciado una nueva conceptualización del fenómeno, enmarcada en lo que algunos estudiosos llaman “la nueva era” de las migraciones internacionales (Arango, 2003, mencionado por Fernández, 2005). Este nuevo ciclo se caracteriza por una profusa re-configuración del mapa migratorio mundial, el cual parece dar cuenta hoy, de una auténtica mundialización migratoria, con una fuerte tendencia a la diversificación de rutas y conexiones origen-destino. El nuevo mapa es el correlato de un escenario de globalización económica, cultural e informacional, que estimula que segmentos amplios de la población respondan cada vez más rápidamente a informaciones y oportunidades que se originan más allá de las fronteras nacionales (CONAPO, 2009). De esta forma la nueva era de la globalización, se ha convertido en un asunto de especial trascendencia. Por un lado, la mejora y expansión de los sistemas de comunicación y transporte y la significativa reducción del tiempo y coste de desplazamiento, así como las disparidades económicas y la existencia de situaciones sociales y políticas extremas han propiciado el crecimiento de los movimientos transnacionales de personas y la intensificación de las presiones migratorias. En este sentido, España nunca ha sido ajena al fenómeno de las corrientes migratorias. Así por ejemplo, en los últimos años y durante la primera mitad del siglo XX y parte de la segunda, grandes contingentes de españoles emigraron hacia diferentes puntos de América Latina y Europa en busca de un empleo y mejor calidad de vida. Pero fue a finales del siglo pasado cuando España, impulsada por el acelerado ritmo de crecimiento económico adoptado en parte gracias a su integración económica en Europa, pasó de ser una economía emisora de emigrantes a una receptora de inmigrantes. Sin embargo, el fenómeno de la inmigración en España cobró verdadera importancia hasta principios del siglo XXI, cuando las fuertes oleadas masivas de personas provenientes de países en vías de desarrollo se dejaron sentir en su estructura poblacional y actividad laboral; de ésta manera, durante el primer quinquenio de este siglo si al 1 de enero del año 2000 los residentes extranjeros en España eran 0.9 millones (que representaban 2.3 por ciento de las personas empadronadas) al 1 de enero de 2005 ya eran 3.7 millones, es decir, 8.5 por ciento de la población residente en el país, habiéndose por tanto cuadriplicado el efectivo de extranjeros en tan sólo cinco años (González, 2006: 2-3; Gil, 2007: 1). Con base en lo anterior, el objetivo del presente trabajo consistió en analizar las características de los flujos de inmigración actuales en España procedentes de países latinoamericanos, enmarcados en la nueva re-configuración del mapa migratorio mundial

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

Rapidity and transverse-momentum dependence of the inclusive J/ψ nuclear modification factor in p-Pb collisions at √sNN = 5.02 TeV

We have studied the transverse-momentum (pT) dependence of the inclusive J/ψ production in p-Pb collisions at sNN−−−√=5.02 TeV, in three center-of-mass rapidity (ycms) regions, down to zero pT. Results in the forward and backward rapidity ranges (2.03<ycms<3.53 and −4.46<ycms<−2.96) are obtained by studying the J/ψ decay to μ+μ−, while the mid-rapidity region (−1.37<ycms<0.43) is investigated by measuring the e+e− decay channel. The pT dependence of the J/ψ production cross section and nuclear modification factor are presented for each of the rapidity intervals, as well as the J/ψ mean pT values. Forward and mid-rapidity results show a suppression of the J/ψ yield, with respect to pp collisions, which decreases with increasing pT. At backward rapidity no significant J/ψ suppression is observed. Theoretical models including a combination of cold nuclear matter effects such as shadowing and partonic energy loss, are in fair agreement with the data, except at forward rapidity and low transverse momentum. The implications of the p-Pb results for the evaluation of cold nuclear matter effects on J/ψ production in Pb-Pb collisions are also discussed

Measurement of dijet kT in p–Pb collisions at √sNN = 5.02 TeV

A measurement of dijet correlations in p-Pb collisions at sNN−−−√=5.02 TeV with the ALICE detector is presented. Jets are reconstructed from charged particles measured in the central tracking detectors and neutral energy deposited in the electromagnetic calorimeter. The transverse momentum of the full jet (clustered from charged and neutral constituents) and charged jet (clustered from charged particles only) is corrected event-by-event for the contribution of the underlying event, while corrections for underlying event fluctuations and finite detector resolution are applied on an inclusive basis. A projection of the dijet transverse momentum, kTy=pch+neT,jetsin(Δφdijet) with Δφdijet the azimuthal angle between a full and charged jet and pch+neT,jet the transverse momentum of the full jet, is used to study nuclear matter effects in p-Pb collisions. This observable is sensitive to the acoplanarity of dijet production and its potential modification in p-Pb collisions with respect to pp collisions. Measurements of the dijet kTy as a function of the transverse momentum of the full and recoil charged jet, and the event multiplicity are presented. No significant modification of kTy due to nuclear matter effects in p-Pb collisions with respect to the event multiplicity or a PYTHIA8 reference is observed

Coherent ρ0 photoproduction in ultra-peripheral Pb–Pb collisions at √sNN = 2.76 TeV

We report the first measurement at the LHC of coherent photoproduction of ρ0 mesons in ultra-peripheral Pb-Pb collisions. The invariant mass and transverse momentum distributions for ρ0 production are studied in the π+π− decay channel at mid-rapidity. The production cross section in the rapidity range |y|<0.5 is found to be dσ/dy=425±10(stat.) +42−50(sys.) mb. Coherent ρ0 production is studied with and without requirement of nuclear breakup, and the fractional yields for various breakup scenarios are presented. The results are compared with those from lower energies and with model predictions based on the Glauber model and the color dipole model. The measured cross section is found to be inconsistent with a scaling of the γ-nucleon cross section using the Glauber model

Measurement of dijet kT in p–Pb collisions at √sNN = 5.02 TeV

A measurement of dijet correlations in p-Pb collisions at sNN−−−√=5.02 TeV with the ALICE detector is presented. Jets are reconstructed from charged particles measured in the central tracking detectors and neutral energy deposited in the electromagnetic calorimeter. The transverse momentum of the full jet (clustered from charged and neutral constituents) and charged jet (clustered from charged particles only) is corrected event-by-event for the contribution of the underlying event, while corrections for underlying event fluctuations and finite detector resolution are applied on an inclusive basis. A projection of the dijet transverse momentum, kTy=pch+neT,jetsin(Δφdijet) with Δφdijet the azimuthal angle between a full and charged jet and pch+neT,jet the transverse momentum of the full jet, is used to study nuclear matter effects in p-Pb collisions. This observable is sensitive to the acoplanarity of dijet production and its potential modification in p-Pb collisions with respect to pp collisions. Measurements of the dijet kTy as a function of the transverse momentum of the full and recoil charged jet, and the event multiplicity are presented. No significant modification of kTy due to nuclear matter effects in p-Pb collisions with respect to the event multiplicity or a PYTHIA8 reference is observed

One-dimensional pion, kaon, and proton femtoscopy in Pb–Pb collisions at √sNN = 2.76 TeV

The size of the particle emission region in high-energy collisions can be deduced using the femtoscopic correlations of particle pairs at low relative momentum. Such correlations arise due to quantum statistics and Coulomb and strong final state interactions. In this paper, results are presented from femtoscopic analyses of π±π±, K±K±, K0SK0S, pp, and p¯¯¯p¯¯¯ correlations from Pb-Pb collisions at sNN−−−√=2.76 TeV by the ALICE experiment at the LHC. One-dimensional radii of the system are extracted from correlation functions in terms of the invariant momentum difference of the pair. The comparison of the measured radii with the predictions from a hydrokinetic model is discussed. The pion and kaon source radii display a monotonic decrease with increasing average pair transverse mass mT which is consistent with hydrodynamic model predictions for central collisions. The kaon and proton source sizes can be reasonably described by approximate mT-scaling

Event shape engineering for inclusive spectra and elliptic flow in Pb–Pb collisions at √sNN = 2.76 TeV

We report on results obtained with the Event Shape Engineering technique applied to Pb-Pb collisions at sNN−−−√=2.76 TeV. By selecting events in the same centrality interval, but with very different average flow, different initial state conditions can be studied. We find the effect of the event-shape selection on the elliptic flow coefficient v2 to be almost independent of transverse momentum pT, as expected if this effect is due to fluctuations in the initial geometry of the system. Charged hadron, pion, kaon, and proton transverse momentum distributions are found to be harder in events with higher-than-average elliptic flow, indicating an interplay between radial and elliptic flow

Elliptic flow of muons from heavy-flavour hadron decays at forward rapidity in Pb–Pb collisions at √sNN = 2.76 TeV

The elliptic flow, v2, of muons from heavy-flavour hadron decays at forward rapidity (2.5<y<4) is measured in Pb--Pb collisions at sNN−−−√~=~2.76 TeV with 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 v2 of muons from heavy-flavour hadron decays on the collision centrality, in the range 0--40\%, and on transverse momentum, pT, is studied in the interval 3<pT<10~GeV/c. A positive v2 is observed with the scalar product and two-particle Q cumulants in semi-central collisions (10--20\% and 20--40\% centrality classes) for the pT interval from 3 to about 5 GeV/c. The v2 magnitude tends to decrease towards more central collisions and with increasing pT. It becomes compatible with zero in the interval 6<pT<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. The model calculations describe the measured v2 within uncertainties

Coherent ψ(2S) photo-production in ultra-peripheral PbPb collisions at √sNN=2.76 TeV

We have performed the first measurement of the coherent ψ(2S) photo-production cross section in ultra-peripheral PbPb collisions at the LHC. This charmonium excited state is reconstructed via the ψ(2S)→l+l− and ψ(2S)→J/ψπ+π− decays, where the J/ψ decays into two leptons. The analysis is based on an event sample corresponding to an integrated luminosity of about 22 μb−1. The cross section for coherent ψ(2S) production in the rapidity interval −0.9<y<0.9 is dσψ(2S)coh/dy=0.83±0.19(stat+syst) mb. The ψ(2S) to J/ψ coherent cross section ratio is 0.34−0.07+0.08(stat+syst). The obtained results are compared to predictions from theoretical models