La moderna teoria dei fenomeni fisici (radioattività, ioni, elettroni) di Augusto Righi un esempio di divulgazione della teoria dell'elettrone di Lorentz

Augusto Righi (1850 - 1920) è stato un fisico bolognese di prestigio e fama internazionale, i suoi contributi scientifici spaziarono in quasi tutti gli ambiti della fisica noti al tempo; inoltre, egli era rinomato per essere un insegnate chiaro e comprensibile, che si dedicò anche alla comunicazione scientifica con la società. In questo lavoro di tesi: si analizza l’opera La moderna teoria dei fenomeni fisici (radioattività, ioni, elettroni) di Augusto Righi, come esempio divulgativo di successo della teoria degli elettroni di Lorentz; si delinea il quadro culturale e sociale presente a cavallo tra l’Ottocento e il Novecento in Italia, Inghilterra e Francia; si selezionano alcune opere della scena internazionale per meglio collocare il contributo di Righi; si definiscono le differenze terminologiche tra la divulgazione scientifica e la Public Understanding of Science sorta negli ultimi decenni. Si procede dunque col definire una griglia di analisi tramite la quale si studia la trasposizione attuata dagli autori sui contenuti scientifici della teoria degli elettroni, nel momento in cui questi vengono comunicati alla società. Si mostra come la teoria degli elettroni sia stata sviluppata da Lorentz durante la fine dell’Ottocento e come questa sia sviluppata in diversi sui scritti; si ricostruiscono quindi i natali di tale teoria, per poi delinearne le caratteristiche principali esposte da Lorentz, Righi, Pearson e Poincaré. In questo confronto consiste la prima analisi presentata in questo scritto ed effettuata mantenendo una visione ampia sulle opere dei quattro scienziati; successivamente si propone un esempio di analisi più profonda e dettagliata, riguardante in particolare uno dei punti principali della teoria di Lorentz: il rapporto fra la carica elettrica e la massa dell’elettrone.

The theory of electrons and its applications to the phenomena of light and radiant heat /

Includes bibliographical footnotes and index.

Search for Lorentz Invariance and CPT Violation with the MINOS Far Detector

We searched for a sidereal modulation in the MINOS far detector neutrino rate. Such a signal would be a consequence of Lorentz and CPT violation as described by the standard-model extension framework. It also would be the first detection of a perturbative effect to conventional neutrino mass oscillations. We found no evidence for this sidereal signature, and the upper limits placed on the magnitudes of the Lorentz and CPT violating coefficients describing the theory are an improvement by factors of 20-510 over the current best limits found by using the MINOS near detector.

Testing Lorentz Invariance and CPT Conservation with NuMI Neutrinos in the MINOS Near Detector

A search for a sidereal modulation in the MINOS near detector neutrino data was performed. If present, this signature could be a consequence of Lorentz and CPT violation as predicted by the effective field theory called the standard-model extension. No evidence for a sidereal signal in the data set was found, implying that there is no significant change in neutrino propagation that depends on the direction of the neutrino beam in a sun-centered inertial frame. Upper limits on the magnitudes of the Lorentz and CPT violating terms in the standard-model extension lie between 10(-4) and 10(-2) of the maximum expected, assuming a suppression of these signatures by a factor of 10(-17).

Free energy of Lorentz-violating QED at high temperature

In this paper we study the one-and two-loop contribution to the free energy in QED with Lorentz symmetry breaking introduced via constant CPT-even Lorentz-breaking parameters at the high temperature limit. We find the impact of the Lorentz-violating term for the free energy and carry out a numerical estimation for the Lorentz-breaking parameter.

Aetherlike Lorentz-breaking actions

We show that CPT-even aetherlike Lorentz-breaking actions, for the scalar and electromagnetic fields, are generated via their appropriate Lorentz-breaking coupling to spinor fields, in three, four, and five space-time dimensions. Besides, we also show that aetherlike terms for the spinor field can be generated as a consequence of the same couplings. We discuss the dispersion relations in the theories with aetherlike Lorentz-breaking terms and find the tree-level effective (Breit) potential for fermion scattering and the one-loop effective potential corresponding to the action of the scalar field.

Dynamical Lorentz symmetry breaking in 3D and charge fractionalization

We analyze the breaking of Lorentz invariance in a 3D model of fermion fields self-coupled through four-fermion interactions. The low-energy limit of the theory contains various submodels which are similar to those used in the study of graphene or in the description of irrational charge fractionalization.

Ambiguities in the effective action in Lorentz-violating gravity

We investigate the occurrence of ambiguities for the Lorentz-violating gravitational Chern-Simons term. It turns out that this term is accompanied by a coefficient depending on an undetermined parameter, due to an arbitrariness in the choice of the conserved current.

Dynamical Lorentz and CPT symmetry breaking in a 4D four-fermion model

In a 4D chiral Thirring model we analyze the possibility that radiative corrections may produce spontaneous breaking of Lorentz and CPT symmetry. By studying the effective potential, we verified that the chiral current (psi) over bar gamma(mu)gamma(5)psi may assume a nonzero vacuum expectation value which triggers Lorentz and CPT violations. Furthermore, by making fluctuations on the minimum of the potential we dynamically induce a bumblebee-like model containing a Chem-Simons term.

S matrix on the Moyal plane: Locality versus Lorentz invariance

Twisted quantum field theories on the Groenewold-Moyal plane are known to be nonlocal. Despite this nonlocality, it is possible to define a generalized notion of causality. We show that interacting quantum field theories that involve only couplings between matter fields, or between matter fields and minimally coupled U(1) gauge fields are causal in this sense. On the other hand, interactions between matter fields and non-Abelian gauge fields violate this generalized causality. We derive the modified Feynman rules emergent from these features. They imply that interactions of matter with non-Abelian gauge fields are not Lorentz- and CPT-invariant.

On entanglement and Lorentz transformations

We study the transformation of maximally entangled states under the action of Lorentz transformations in a fully relativistic setting. By explicit calculation of the Wigner rotation, we describe the relativistic analog of the Bell states as viewed from two inertial frames moving with constant velocity with respect to each other. Though the finite dimensional matrices describing the Lorentz transformations are non-unitary, each single particle state of the entangled pair undergoes an effective, momentum dependent, local unitary rotation, thereby preserving the entanglement fidelity of the bipartite state. The details of how these unitary transformations are manifested are explicitly worked out for the Bell states comprised of massive spin 1/2 particles and massless photon polarizations. The relevance of this work to non-inertial frames is briefly discussed.

Radiatively induced Lorentz and CPT violation in Schwinger constant field approximation

The Schwinger proper-time method is an effective calculation method, explicitly gauge-invariant and nonperturbative. We make use of this method to investigate the radiatively induced Lorentz- and CPT-violating effects in quantum electrodynamics when an axial-vector interaction term is introduced in the fermionic sector. The induced Lorentz- and CPT-violating Chern-Simons term coincides with the one obtained using a covariant derivative expansion but differs from the result usually obtained in other regularization schemes. A possible ambiguity in the approach is also discussed. (C) 2001 Published by Elsevier Science B.V.

Dendrometria de espécies nativas em plantios homogêneos no estado de Roraima: andiroba (Carapa guianensis Aubl), castanha-do-Brasil (Bertholletia excelsa Bonpl.), ipê-roxo (Tabebuia avellanedae Lorentz ex Griseb) e jatobá (Hymenaea courbaril L.)

Estudou-se o crescimento e a seleção de equações para quatro espécies florestais nativas visando identificar espécies promissoras para o plantio em programas de reflorestamentos e em sistemas agroflorestais no Estado de Roraima. O crescimento da andiroba (Carapa guianensis Aubl.), da castanha-do-brasil (Bertholletia excelsa Bonpl.), do ipê-roxo (Tabebuia avellanedae Lorentz ex Griseb.) e do jatobá (Hymenaea courbaril L.), aos sete anos de idade, mostrou-se promissor atingindo incrementos médios anuais em volume comercial de 6.3; 14.6; 6.0 e 2.3 m³.ha-1.ano-1, respectivamente. Em relação ao crescimento em diâmetro, todas as espécies apresentaram incrementos médios anuais em diâmetro maiores do que 1 cm, sendo superiores aos observados para árvores crescendo em florestas naturais. A análise estatística, indicou a equação hipsométrica de Prodan como a de melhor ajuste para estimar a altura em função do diâmetro para as quatro espécies analisadas. No entanto, a análise gráfica indicou que a forma da curva altura/diâmetro variou com a espécie sendo necessário o ajuste em separado. O ajuste de equações de volume comercial com casca e fator de forma comercial mostraram ser necessário o ajuste de diferentes equações em função da espécie. A análise gráfica das curvas de volume comercial e fator de forma indicaram que as espécies diferiram em ambos os parâmetros, indicando que a utilização de um fator de forma médio para todas as espécies deve ser evitado, como forma de aumentar a precisão nas estimativas volumétricas.

Norm inequalities in multidimensional Lorentz spaces

In this paper we obtain necessary and sufficient conditions for double trigonometric series to belong to generalized Lorentz spaces, not symmetric in general. Estimates for the norms are given in terms of coefficients.