Que farei com este cânone?: Uma leitura de “O cadáver de James Joyce”, de José Luís Peixoto

«O Cadáver de James Joyce», conto publicado por José Luís Peixoto na revista Ficções em 2004, é um exercício que explora os territórios ambíguos que se situam na intersecção da “realidade” com a “imaginação”, da biografia com a ficção. O narrador-protagonista, José Luís Peixoto – epónimo do autor, portanto -, narra em poucas páginas a viagem impossível que faz a Zurique e a Dublin com o propósito único de secretamente devolver os restos mortais de James Joyce à cidade natal do escritor irlandês. A brevidade da narrativa acolhe a magnitude do feito narrado operando uma redimensionação do mundo, que por um lado o miniaturiza e por outro o esquematiza e, por essa via, irrealiza. A própria linguagem do conto acompanha este movimento de esquematização e síntese: a frase tende a encurtar-se, essencializa-se – e esta compressão da linguagem reforça o efeito da compressão do mundo representado. Pela forma como problematiza as relações entre a linguagem e o mundo, entre a literatura e a realidade, «O Cadáver de James Joyce» encena, em última instância, a dimensão simultaneamente grandiosa e precária da criação literária.

Basis invariant conditions for supersymmetry in the two-Higgs-doublet model

The minimal supersymmetric standard model involves a rather restrictive Higgs potential with two Higgs fields. Recently, the full set of classes of symmetries allowed in the most general two-Higgs-doublet model was identified; these classes do not include the supersymmetric limit as a particular class. Thus, a physically meaningful definition of the supersymmetric limit must involve the interaction of the Higgs sector with other sectors of the theory. Here we show how one can construct basis invariant probes of supersymmetry involving both the Higgs sector and the gaugino-Higgsino-Higgs interactions.

Geometric picture of generalized-CP and Higgs-family transformations in the two-Higgs-doublet model

In the two-Higgs-doublet model (THDM), generalized-CP transformations (phi(i) -> X-ij phi(*)(j) where X is unitary) and unitary Higgs-family transformations (phi(i) -> U-ij phi(j)) have recently been examined in a series of papers. In terms of gauge-invariant bilinear functions of the Higgs fields phi(i), the Higgs-family transformations and the generalized-CP transformations possess a simple geometric description. Namely, these transformations correspond in the space of scalar-field bilinears to proper and improper rotations, respectively. In this formalism, recent results relating generalized CP transformations with Higgs-family transformations have a clear geometric interpretation. We will review what is known regarding THDM symmetries, as well as derive new results concerning those symmetries, namely how they can be interpreted geometrically as applications of several CP transformations.

Intervenção com procedimentos de autossugestão na autoeficácia e controlo da dor

Introdução – A dor predomina em muitas patologias médicas e acarreta diversas implicações para o doente. O presente estudo visou avaliar a eficácia de uma intervenção autossugestiva, como complemento ao tratamento médico, no aumento da autoeficácia e controlo da dor. Metodologia – Para a concretização deste objetivo, 205 pacientes adultos com dor foram distribuídos aleatoriamente por dois grupos que se distinguiram quanto à intervenção recebida durante 12 semanas, nomeadamente IAS (intervenção autossugestiva) e ISAS (intervenção sem autossugestão). Os dois grupos foram comparados quanto à evolução da autoeficácia e do controlo da dor ao longo desse período. Resultados e discussão – Os resultados mostraram um aumento estatisticamente significativo destas variáveis no grupo IAS mas não no grupo ISAS, sugerindo a eficácia da intervenção autossugestiva. Este estudo representa, assim, um importante contributo para a prática clínica com os doentes com dor.

Mass-degenerate Higgs bosons at 125 GeV in the two-Higgs-doublet model

The analysis of the Higgs boson data by the ATLAS and CMS Collaborations appears to exhibit an excess of h -> gamma gamma events above the Standard Model (SM) expectations, whereas no significant excess is observed in h -> ZZ* -> four lepton events, albeit with large statistical uncertainty due to the small data sample. These results (assuming they persist with further data) could be explained by a pair of nearly mass-degenerate scalars, one of which is an SM-like Higgs boson and the other is a scalar with suppressed couplings to W+W- and ZZ. In the two-Higgs-doublet model, the observed gamma gamma and ZZ* -> four lepton data can be reproduced by an approximately degenerate CP-even (h) and CP-odd (A) Higgs boson for values of sin (beta - alpha) near unity and 0: 70 less than or similar to tan beta less than or similar to 1. An enhanced gamma gamma signal can also arise in cases where m(h) similar or equal to m(H), m(H) similar or equal to m(A), or m(h) similar or equal to m(H) similar or equal to m(A). Since the ZZ* -> 4 leptons signal derives primarily from an SM-like Higgs boson whereas the gamma gamma signal receives contributions from two (or more) nearly mass-degenerate states, one would expect a slightly different invariant mass peak in the ZZ* -> four lepton and gamma gamma channels. The phenomenological consequences of such models can be tested with additional Higgs data that will be collected at the LHC in the near future. DOI: 10.1103/PhysRevD.87.055009.

Probing wrong-sign Yukawa couplings at the LHC and a future linear collider

We consider the two-Higgs-doublet model as a framework in which to evaluate the viability of scenarios in which the sign of the coupling of the observed Higgs boson to down-type fermions (in particular, b-quark pairs) is opposite to that of the Standard Model (SM), while at the same time all other tree-level couplings are close to the SM values. We show that, whereas such a scenario is consistent with current LHC observations, both future running at the LHC and a future e(+)e(-) linear collider could determine the sign of the Higgs coupling to b-quark pairs. Discrimination is possible for two reasons. First, the interference between the b-quark and the t-quark loop contributions to the ggh coupling changes sign. Second, the charged-Higgs loop contribution to the gamma gamma h coupling is large and fairly constant up to the largest charged-Higgs mass allowed by tree-level unitarity bounds when the b-quark Yukawa coupling has the opposite sign from that of the SM (the change in sign of the interference terms between the b-quark loop and the W and t loops having negligible impact).

Preserving the validity of the two-Higgs-doublet model up to the Planck scale

We examine the constraints on the two Higgs doublet model (2HDM) due to the stability of the scalar potential and absence of Landau poles at energy scales below the Planck scale. We employ the most general 2HDM that incorporates an approximately Standard Model (SM) Higgs boson with a flavor aligned Yukawa sector to eliminate potential tree-level Higgs-mediated flavor changing neutral currents. Using basis independent techniques, we exhibit robust regimes of the 2HDM parameter space with a 125 GeV SM-like Higgs boson that is stable and perturbative up to the Planck scale. Implications for the heavy scalar spectrum are exhibited.