Gorputz adierazpena lehen hezkuntzan

Liburu honekin zera nahi dugu: Gorputz Hezkuntzako curriculuma ezagutzea, legeak dioena eta eduki multzoen garapena. Eta era berean, motrizitatearen lan metodologiak eta irakasle gisa eskura ditugun baliabideak ezagutzea da.Material honen helburua da Lehen Hezkuntzako Irakasle ikasketetan enborrezko izan den Gorputz Adierazpena irakasgaiaren edukiak zabaltzea du helburu. Hala, Graduko ikasketetan Gorputz Hezkuntzako minorrean hautazkoa izango den Gorputz Adierazpena ikasgairako oinarria izango diren edukiak zabaltzea. Ikasmaterial honek hainbat atal nagusiak ditu: Lehenengo atalean, Gorputz Adierazpenaren kontzeptua, historia eta korronte ideiologikoak aztertzen dira lehen kapituluan. Bigarrenean, Gorputz Adierazpenaren trataera LOE legean eta aurreko legetan, eta honene arabera unibertsitateik gorputz adierazpena lantzeko egiten den proposamen zehatz bat. Hirugarren kapitulutik zazpigarrenera eduki bakoitza aztertzen da (gerturatze teorikoa eta handik unitate didaktiko zehatz bat sortzen da. Bertan, ikasle bakoitzak aipatzen du zer gertatu den praktikara eraman duenean bere proposamena).Ikasmaterial honek hainbat atal nagusiak ditu: Lehenengo atalean, Gorputz Adierazpenaren kontzeptua, historia eta korronte ideiologikoak aztertzen dira lehen kapituluan. Bigarrenean, Gorputz Adierazpenaren trataera LOE legean eta aurreko legetan, eta honene arabera unibertsitateik gorputz adierazpena lantzeko egiten den proposamen zehatz bat. Hirugarren kapitulutik zazpigarrenera eduki bakoitza aztertzen da (gerturatze teorikoa eta handik unitate didaktiko zehatz bat sortzen da. Bertan, ikasle bakoitzak aipatzen du zer gertatu den praktikara eraman duenean bere proposamena).Ikasmaterial honek hainbat atal nagusiak ditu: Lehenengo atalean, Gorputz Adierazpenaren kontzeptua, historia eta korronte ideiologikoak aztertzen dira lehen kapituluan. Bigarrenean, Gorputz Adierazpenaren trataera LOE legean eta aurreko legetan, eta honene arabera unibertsitateik gorputz adierazpena lantzeko egiten den proposamen zehatz bat. Hirugarren kapitulutik zazpigarrenera eduki bakoitza aztertzen da (gerturatze teorikoa eta handik unitate didaktiko zehatz bat sortzen da. Bertan, ikasle bakoitzak aipatzen du zer gertatu den praktikara eraman duenean bere proposamena). Ikasmaterial honek hainbat atal nagusiak ditu: Lehenengo atalean, Gorputz Adierazpenaren kontzeptua, historia eta korronte ideiologikoak aztertzen dira lehen kapituluan. Bigarrenean, Gorputz Adierazpenaren trataera LOE legean eta aurreko legetan, eta honene arabera unibertsitateik gorputz adierazpena lantzeko egiten den proposamen zehatz bat. Hirugarren kapitulutik zazpigarrenera eduki bakoitza aztertzen da (gerturatze teorikoa eta handik unitate didaktiko zehatz bat sortzen da. Bertan, ikasle bakoitzak aipatzen du zer gertatu den praktikara eraman duenean bere proposamena).Liburu honek UPV/EHUko Euskara eta Eleaniztasuneko Errektoreordetzaren dirulaguntza jaso d

Joint Observation of the Galactic Center with MAGIC and CTA-LST-1

MAGIC is a system of two Imaging Atmospheric Cherenkov Telescopes (IACTs), designed to detect very-high-energy gamma rays, and is operating in stereoscopic mode since 2009 at the Observatorio del Roque de Los Muchachos in La Palma, Spain. In 2018, the prototype IACT of the Large-Sized Telescope (LST-1) for the Cherenkov Telescope Array, a next-generation ground-based gamma-ray observatory, was inaugurated at the same site, at a distance of approximately 100 meters from the MAGIC telescopes. Using joint observations between MAGIC and LST-1, we developed a dedicated analysis pipeline and established the threefold telescope system via software, achieving the highest sensitivity in the northern hemisphere. Based on this enhanced performance, MAGIC and LST-1 have been jointly and regularly observing the Galactic Center, a region of paramount importance and complexity for IACTs. In particular, the gamma-ray emission from the dynamical center of the Milky Way is under debate. Although previous measurements suggested that a supermassive black hole Sagittarius A* plays a primary role, its radiation mechanism remains unclear, mainly due to limited angular resolution and sensitivity. The enhanced sensitivity in our novel approach is thus expected to provide new insights into the question. We here present the current status of the data analysis for the Galactic Center joint MAGIC and LST-1 observations

Optimasi Portofolio Resiko Menggunakan Model Markowitz MVO Dikaitkan dengan Keterbatasan Manusia dalam Memprediksi Masa Depan dalam Perspektif Al-Qur`an

Risk portfolio on modern finance has become increasingly technical, requiring the use of sophisticated mathematical tools in both research and practice. Since companies cannot insure themselves completely against risk, as human incompetence in predicting the future precisely that written in Al-Quran surah Luqman verse 34, they have to manage it to yield an optimal portfolio. The objective here is to minimize the variance among all portfolios, or alternatively, to maximize expected return among all portfolios that has at least a certain expected return. Furthermore, this study focuses on optimizing risk portfolio so called Markowitz MVO (Mean-Variance Optimization). Some theoretical frameworks for analysis are arithmetic mean, geometric mean, variance, covariance, linear programming, and quadratic programming. Moreover, finding a minimum variance portfolio produces a convex quadratic programming, that is minimizing the objective function ðð¥with constraintsð ð 𥠥 ðandð´ð¥ = ð. The outcome of this research is the solution of optimal risk portofolio in some investments that could be finished smoothly using MATLAB R2007b software together with its graphic analysis

Search for heavy resonances decaying to two Higgs bosons in final states containing four b quarks

A search is presented for narrow heavy resonances X decaying into pairs of Higgs bosons (H) in proton-proton collisions collected by the CMS experiment at the LHC at root s = 8 TeV. The data correspond to an integrated luminosity of 19.7 fb(-1). The search considers HH resonances with masses between 1 and 3 TeV, having final states of two b quark pairs. Each Higgs boson is produced with large momentum, and the hadronization products of the pair of b quarks can usually be reconstructed as single large jets. The background from multijet and t (t) over bar events is significantly reduced by applying requirements related to the flavor of the jet, its mass, and its substructure. The signal would be identified as a peak on top of the dijet invariant mass spectrum of the remaining background events. No evidence is observed for such a signal. Upper limits obtained at 95 confidence level for the product of the production cross section and branching fraction sigma(gg -> X) B(X -> HH -> b (b) over barb (b) over bar) range from 10 to 1.5 fb for the mass of X from 1.15 to 2.0 TeV, significantly extending previous searches. For a warped extra dimension theory with amass scale Lambda(R) = 1 TeV, the data exclude radion scalar masses between 1.15 and 1.55 TeV

Search for supersymmetry in events with one lepton and multiple jets in proton-proton collisions at root s=13 TeV

Peer reviewe

Measurement of the top quark mass using charged particles in pp collisions at root s=8 TeV

Peer reviewe

Search for anomalous couplings in boosted WW/WZ -> l nu q(q)over-bar production in proton-proton collisions at root s=8TeV

Peer reviewe

Measurement of the underlying event activity in inclusive Z boson production in proton-proton collisions at root s=13 TeV

This paper presents a measurement of the underlying event activity in proton-proton collisions at a center-of-mass energy of 13TeV, performed using inclusive Z boson production events collected with the CMS experiment at the LHC. The analyzed data correspond to an integrated luminosity of 2.1 fb(-1). The underlying event activity is quantified in terms of the charged particle multiplicity, as well as of the scalar sum of the charged particles' transverse momenta in different topological regions defined with respect to the Z boson direction. The distributions are unfolded to the stable particle level and compared with predictions from various Monte Carlo event generators, as well as with similar CDF and CMS measurements at center-of-mass energies of 1.96 and 7TeV respectively.Peer reviewe

Measurement of associated Z plus charm production in proton-proton collisions at root s=8TeV

A study of the associated production of a Z boson and a charm quark jet (Z + c), and a comparison to production with a b quark jet (Z + b), in pp collisions at a centre-of-mass energy of 8 TeV are presented. The analysis uses a data sample corresponding to an integrated luminosity of 19.7 fb(-1), collected with the CMS detector at the CERN LHC. The Z boson candidates are identified through their decays into pairs of electrons or muons. Jets originating from heavy flavour quarks are identified using semileptonic decays of c or b flavoured hadrons and hadronic decays of charm hadrons. The measurements are performed in the kinematic region with two leptons with pT(l) > 20 GeV, vertical bar eta(l)vertical bar 25 GeV and vertical bar eta(jet)vertical bar Z + c + X) B(Z -> l(+)l(-)) = 8.8 +/- 0.5 (stat)+/- 0.6 (syst) pb. The ratio of the Z+c and Z+b production cross sections is measured to be sigma(pp -> Z+c+X)/sigma (pp -> Z+b+X) = 2.0 +/- 0.2 (stat)+/- 0.2 (syst). The Z+c production cross section and the cross section ratio are also measured as a function of the transverse momentum of theZ boson and of the heavy flavour jet. The measurements are compared with theoretical predictions.Peer reviewe