Non-radial instabilities and progenitor asphericities in core-collapse supernovae

Since core-collapse supernova simulations still struggle to produce robust neutrino-driven explosions in 3D, it has been proposed that asphericities caused by convection in the progenitor might facilitate shock revival by boosting the activity of non-radial hydrodynamic instabilities in the post-shock region. We investigate this scenario in depth using 42 relativistic 2D simulations with multigroup neutrino transport to examine the effects of velocity and density perturbations in the progenitor for different perturbation geometries that obey fundamental physical constraints (like the anelastic condition). As a framework for analysing our results, we introduce semi-empirical scaling laws relating neutrino heating, average turbulent velocities in the gain region, and the shock deformation in the saturation limit of non-radial instabilities. The squared turbulent Mach number, 〈Ma2〉, reflects the violence of aspherical motions in the gain layer, and explosive runaway occurs for 〈Ma2〉 ≳ 0.3, corresponding to a reduction of the critical neutrino luminosity by ∼25∼25 per cent compared to 1D. In the light of this theory, progenitor asphericities aid shock revival mainly by creating anisotropic mass flux on to the shock: differential infall efficiently converts velocity perturbations in the progenitor into density perturbations δρ/ρ at the shock of the order of the initial convective Mach number Maprog. The anisotropic mass flux and ram pressure deform the shock and thereby amplify post-shock turbulence. Large-scale (ℓ = 2, ℓ = 1) modes prove most conducive to shock revival, whereas small-scale perturbations require unrealistically high convective Mach numbers. Initial density perturbations in the progenitor are only of the order of Ma2progMaprog2 and therefore play a subdominant role.

The Status of Multi-Dimensional Core-Collapse Supernova Models

Models of neutrino-driven core-collapse supernova explosions have matured considerably in recent years. Explosions of low-mass progenitors can routinely be simulated in 1D, 2D, and 3D. Nucleosynthesis calculations indicate that these supernovae could be contributors of some lighter neutron-rich elements beyond iron. The explosion mechanism of more massive stars remains under investigation, although first 3D models of neutrino-driven explosions employing multi-group neutrino transport have become available. Together with earlier 2D models and more simplified 3D simulations, these have elucidated the interplay between neutrino heating and hydrodynamic instabilities in the post-shock region that is essential for shock revival. However, some physical ingredients may still need to be added/improved before simulations can robustly explain supernova explosions over a wide range of progenitors. Solutions recently suggested in the literature include uncertainties in the neutrino rates, rotation, and seed perturbations from convective shell burning. We review the implications of 3D simulations of shell burning in supernova progenitors for the ‘perturbations-aided neutrino-driven mechanism,’ whose efficacy is illustrated by the first successful multi-group neutrino hydrodynamics simulation of an 18 solar mass progenitor with 3D initial conditions. We conclude with speculations about the impact of 3D effects on the structure of massive stars through convective boundary mixing.

Flavour symmetries in a renormalizable SO(10) model

In the context of a renormalizable supersymmetric SO(10) Grand Unified Theory, we consider the fermion mass matrices generated by the Yukawa couplings to a 10 circle plus 120 circle plus (126) over bar representation of scalars. We perform a complete investigation of the possibilities of imposing flavour symmetries in this scenario; the purpose is to reduce the number of Yukawa coupling constants in order to identify potentially predictive models. We have found that there are only 14 inequivalent cases of Yukawa coupling matrices, out of which 13 cases are generated by 74 symmetries, with suitable n, and one case is generated by a Z(2) x Z(2) symmetry. A numerical analysis of the 14 cases reveals that only two of them-dubbed A and B in the present paper allow good fits to the experimentally known fermion masses and mixings. (C) 2016 The Authors. Published by Elsevier B.V.

Scotogenic model for co-bimaximal mixing

We present a scotogenic model, i.e. a one-loop neutrino mass model with dark right-handed neutrino gauge singlets and one inert dark scalar gauge doublet eta, which has symmetries that lead to co-bimaximal mixing, i.e. to an atmospheric mixing angle theta(23) = 45 degrees and to a CP-violating phase delta = +/-pi/2, while the mixing angle theta(13) remains arbitrary. The symmetries consist of softly broken lepton numbers L-alpha (alpha = e, mu, tau), a non-standard CP symmetry, and three L-2 symmetries. We indicate two possibilities for extending the model to the quark sector. Since the model has, besides eta, three scalar gauge doublets, we perform a thorough discussion of its scalar sector. We demonstrate that it can accommodate a Standard Model-like scalar with mass 125 GeV, with all the other charged and neutral scalars having much higher masses.

The Askaryan radio array

The Askar'yan Radio Array (ARA), a neutrino detector to be situated at the South Pole next to the IceCube detector, will be sensitive to ultrahigh-energy cosmic neutrinos above 0.1 EeV and will have the greatest sensitivity within the favored energy range from 0.1 EeV up to 10 EeV. Neutrinos of this energy are guaranteed by current observations of the GZK-cutoff by the HiRes and Pierre Auger Observatories. The detection method is based on Cherenkov emission by a neutrino induced cascade in the ice, coherent at radio wavelengths, which was predicted by Askar'yan in 1962 and verified in beam tests at SLAC in 2006. The detector is planned to consist of 37 stations with 16 antennas each, deployed at depths of up to 200 m under the ice surface. During the last two polar seasons (2010-2011, 2011-2012), a prototype station and a first detector station were successfully deployed and are taking data. These data have been and are currently being analyzed to study the ambient noise background and the radio frequency properties of the South Pole ice sheet. A worldwide collaboration is working on the planning, construction and data analysis of the detector array. This article will give a short report on the status of the ARA detector and show recent results from the recorded data. © 2013 AIP Publishing LLC.

Fattibilità della misura di cattura neutronica sugli isotopi dispari del gadolinio

In questo lavoro di tesi ci proponiamo di determinare lo spessore degli isotopi ^155Gd e ^157Gd in vista della misura della sezione d’urto di cattura neutronica presso la facility n_TOF del CERN. La principale motivazione dell’esperimento è legata alla necessità di ottenere misure più accurate per le applicazioni ai reattori nucleari. Inoltre, i nuovi risultati, potranno essere sfruttati anche per applicazioni ai recenti sviluppi nella Terapia di Cattura Neutronica e per costruire nuovi rivelatori nell’ambito della ricerca del neutrino. La misura sarà effettuata nella prima area sperimentale EAR-1 di n TOF, equipaggiata con rivelatori, come per esempio gli scintillatori liquidi al benzene deuterato (C6D6) particolarmente adatti per questi tipi di misura. La sezione d’urto di questi due isotopi cambia di molti ordini di grandezza al variare dell’energia dei neutroni incidenti. Per questo motivo, lo studio effettuato in questa tesi ha mostrato che sono necessari due campioni altamente arricchiti per ogni isotopo da misurare: un campione estremamente sottile per energie del neutrone fino a 100 meV, e uno più spesso per energie maggiori. Inoltre per questi campioni sono stati determinati le densità areali necessarie per lo svolgimento dell’esperimento affinchè avvenga il fenomeno di trasmissione dei neutroni.

Studio di fattibilità della ricostruzione del decadimento $D^0\to K^-\mu^+\nu_{\mu}$ ad LHCb

Il Modello Standard delle particelle elementari prevede l’universalità del sapore leptonico, cioè l’uguaglianza della probabilità di accoppiamento dei bosoni di gauge carichi dell’interazione debole con tutti i leptoni. Recentemente, le Collaborazioni LHCb, BaBar e Belle, misurando il rapporto tra i branching ratio dei decadimenti $B^0\to D^{∗− }\tau^+\nu_{\tau} e $B^0 →D^{∗−}\mu^+\nu_{\mu}, hanno osservato una deviazione dai valori previsti dal Modello Standard di 3.9 deviazioni standard. Questo interessante risultato, se confermato, indicherebbe l’esistenza di nuove particelle, come per esempio il bosone di Higgs carico. Analogamente ai decadimenti del mesone $B^0$ , è possibile cercare effetti analoghi anche nel rapporto di branching ratio dei decadimenti $D^0\to K^ −\mu^+\nu_{\mu}$ e $D^0\to K^−e^+\nu_e$ . In questo lavoro di tesi è stato realizzato uno studio preliminare di questa misura. In particolare, è stato studiata, tramite simulazioni Monte Carlo, la ricostruzione del processo $D^{*\pm}\to D^0 (\to K^− \mu+\nu_{\mu})\pi_s^{\pm}$ nell’esperimento LHCb. Questo canale ha la particolarità di avere una particella invisibile, il neutrino, al rivelatore LHCb. Tuttavia, mediante vincoli cinematici e topologici, è possibile ricavare le componenti dell’impulso del neutrino, con risoluzioni non paragonabili a quelle di una particella visibile, ma comunque accettabili. In questa tesi sono riportati i calcoli che permettono di ottenere queste informazioni ed è stata studiata la risoluzione sulla massa invariante del $D^{∗\pm}$ . La tesi è organizzata nel seguente modo: il primo capitolo riporta le motivazioni della misura dei rapporti dei branching ratio e l’attuale stato sperimentale; il secondo capitolo contiene una breve descrizione del rivelatore LHCb; il terzo capitolo, infine, descrive lo studio di fattibilità della ricostruzione del decadimento $D^0\to K^-\mu^+\nu_{\mu}.