Creativity assessment in psychological research: (Re)setting the standards

This commentary discusses common relevant themes that have been highlighted across contributions in this special issue on \u27Creativity Assessment: Pitfalls, Solutions, and Standards.\u27 We first highlight the challenges of operationalizing creativity through the use of a range of measurement approaches that are simply not tapping into the same aspect of creativity. We then discuss pitfalls and challenges of the three most popular measurement methods employed in the field, namely divergent thinking tasks, product-based assessment using the consensual assessment techniques, and self-report methodology. Finally, we point to two imperative standards that emerged across contributions in this collection of articles, namely transparency (need to accurately define, operationalize, and report on the specific aspect[s] of creativity studied) and homogenization of creativity assessment (identification and consistent use of an optimal \u27standard\u27 measure for each major aspect of creativity). We conclude by providing directions on how the creativity research community and the field can meet these standards

Electroweak Evolution Equations

Enlarging a previous analysis, where only fermions and transverse gauge bosons were taken into account, we write down infrared-collinear evolution equations for the Standard Model of electroweak interactions computing the full set of splitting functions. Due to the presence of double logs which are characteristic of electroweak interactions (Bloch-Nordsieck violation), new infrared singular splitting functions have to be introduced. We also include corrections related to the third generation Yukawa couplings.Comment: 15 pages, 3 figure

Geometry and observables in (2+1)-gravity

We review the geometrical properties of vacuum spacetimes in (2+1)-gravity with vanishing cosmological constant. We explain how these spacetimes are characterised as quotients of their universal cover by holonomies. We explain how this description can be used to clarify the geometrical interpretation of the fundamental physical variables of the theory, holonomies and Wilson loops. In particular, we discuss the role of Wilson loop observables as the generators of the two fundamental transformations that change the geometry of (2+1)-spacetimes, grafting and earthquake. We explain how these variables can be determined from realistic measurements by an observer in the spacetime.Comment: Talk given at 2nd School and Workshop on Quantum Gravity and Quantum Geometry (Corfu, September 13-20 2009); 10 pages, 13 eps figure

Fuchsian convex bodies: basics of Brunn--Minkowski theory

The hyperbolic space \H^d can be defined as a pseudo-sphere in the $(d+1)$ Minkowski space-time. In this paper, a Fuchsian group $\Gamma$ is a group of linear isometries of the Minkowski space such that \H^d/\Gamma is a compact manifold. We introduce Fuchsian convex bodies, which are closed convex sets in Minkowski space, globally invariant for the action of a Fuchsian group. A volume can be associated to each Fuchsian convex body, and, if the group is fixed, Minkowski addition behaves well. Then Fuchsian convex bodies can be studied in the same manner as convex bodies of Euclidean space in the classical Brunn--Minkowski theory. For example, support functions can be defined, as functions on a compact hyperbolic manifold instead of the sphere. The main result is the convexity of the associated volume (it is log concave in the classical setting). This implies analogs of Alexandrov--Fenchel and Brunn--Minkowski inequalities. Here the inequalities are reversed

Micro-object pose estimation with sim-to-real transfer learning using small dataset

International audience<span style="color: rgb(34, 34, 34); font-family: -apple-system, BlinkMacSystemFont, &quot;Segoe UI&quot;, Roboto, Oxygen-Sans, Ubuntu, Cantarell, &quot;Helvetica Neue&quot;, sans-serif; font-size: 18px;"&gtThree-dimensional (3D) pose estimation of micro/nano-objects isessential for the implementation of automatic manipulation inmicro/nano-robotic systems. However, out-of-plane pose estimationof a micro/nano-object is challenging, since the images aretypically obtained in 2D using a scanning electron microscope (SEM)or an optical microscope (OM). Traditional deep learning basedmethods require the collection of a large amount of labeled datafor model training to estimate the 3D pose of an object from amonocular image. Here we present a sim-to-real learning-to-matchapproach for 3D pose estimation of micro/nano-objects. Instead ofcollecting large training datasets, simulated data is generated toenlarge the limited experimental data obtained in practice, whilethe domain gap between the generated and experimental data isminimized via image translation based on a generative adversarialnetwork (GAN) model. A learning-to-match approach is used to mapthe generated data and the experimental data to a low-dimensionalspace with the same data distribution for different pose labels,which ensures effective feature embedding. Combining the labeleddata obtained from experiments and simulations, a new trainingdataset is constructed for robust pose estimation. The proposedmethod is validated with images from both SEM and OM, facilitatingthe development of closed-loop control of micro/nano-objects withcomplex shapes in micro/nano-robotic systems.</span&g

Integrating Simulink Models into the Model Checker Cosmos

International audienceWe present an implementation for Simulink model executions in the statistical model-checker Cosmos. We take profit of this implementation for hybrid modeling and simulations combining Petri nets and Simulink models.Nous présentons une implémentation pour l'exécution de modèles Simulink dans le model-checker Cosmos. Cette implémentation est ensuite utilisée pour la simulation de modèles hybrides, combinant des réseaux de Petri et des modèles Simulink

Particle Physics Explanations for Ultra High Energy Cosmic Ray Events

The origin of cosmic ray events with E \gsim 10^{11} GeV remains mysterious. In this talk I briefly summarize several proposed particle physics explanations: a breakdown of Lorentz invariance, the ``$Z-$burst'' scenario, new hadrons with masses of several GeV as primaries, and magnetic monopoles with mass below $10^{10}$ GeV as primaries. I then describe in a little more detail the idea that these events are due to the decays of very massive, long--lived exotic particles.Comment: Invited plenary talk at PASCOS03, Mumbai, India, January 2003; 13 pages, 1 figur

Electroweak jet cascading in the decay of superheavy particles

We study decays of superheavy particles $X$ into leptons. We show that they initiate cascades similar to QCD parton jets, if m_X\gsim 10^6 GeV. Electroweak cascading is studied and the energy spectra of the produced leptons are calculated in the framework of a broken SU(2) model of weak interactions. As application, important for the Z-burst model for ultrahigh energy cosmic rays, we consider decays of superheavy particles coupled on tree-level only to neutrinos and derive stringent limit for these decays from the observed diffuse extragalactic $\gamma$-ray flux.Comment: 4 pages, 1 eps figur

Ultra-High Energy Neutrino Fluxes: New Constraints and Implications

We apply new upper limits on neutrino fluxes and the diffuse extragalactic component of the GeV gamma-ray flux to various scenarios for ultra high energy cosmic rays and neutrinos. As a result we find that extra-galactic top-down sources can not contribute significantly to the observed flux of highest energy cosmic rays. The Z-burst mechanism where ultra-high energy neutrinos produce cosmic rays via interactions with relic neutrinos is practically ruled out if cosmological limits on neutrino mass and clustering apply.Comment: 10 revtex pages, 9 postscript figure

Polygon model from first order gravity

The gauge fixed polygon model of 2+1 gravity with zero cosmological constant and arbitrary number of spinless point particles is reconstructed from the first order formalism of the theory in terms of the triad and the spin connection. The induced symplectic structure is calculated and shown to agree with the canonical one in terms of the variables.Comment: 20 pages, presentation improved, typos correcte