Transport in Almost Integrable Models: Perturbed Heisenberg Chains

The heat conductivity kappa(T) of integrable models, like the one-dimensional spin-1/2 nearest-neighbor Heisenberg model, is infinite even at finite temperatures as a consequence of the conservation laws associated with integrability. Small perturbations lead to finite but large transport coefficients which we calculate perturbatively using exact diagonalization and moment expansions. We show that there are two different classes of perturbations. While an interchain coupling of strength J_perp leads to kappa(T) propto 1/J_perp^2 as expected from simple golden-rule arguments, we obtain a much larger kappa(T) propto 1/J'^4 for a weak next-nearest neighbor interaction J'. This can be explained by a new approximate conservation law of the J-J' Heisenberg chain.Comment: 4 pages, several minor modifications, title change

Absorption and Emission in quantum dots: Fermi surface effects of Anderson excitons

Recent experiments measuring the emission of exciton recombination in a self-organized single quantum dot (QD) have revealed that novel effects occur when the wetting layer surrounding the QD becomes filled with electrons, because the resulting Fermi sea can hybridize with the local electron levels on the dot. Motivated by these experiments, we study an extended Anderson model, which describes a local conduction band level coupled to a Fermi sea, but also includes a local valence band level. We are interested, in particular, on how many-body correlations resulting from the presence of the Fermi sea affect the absorption and emission spectra. Using Wilson's numerical renormalization group method, we calculate the zero-temperature absorption (emission) spectrum of a QD which starts from (ends up in) a strongly correlated Kondo ground state. We predict two features: Firstly, we find that the spectrum shows a power law divergence close to the threshold, with an exponent that can be understood by analogy to the well-known X-ray edge absorption problem. Secondly, the threshold energy $\omega_0$ - below which no photon is absorbed (above which no photon is emitted) - shows a marked, monotonic shift as a function of the exciton binding energy $U_{\rm exc}$Comment: 10 pages, 9 figure

System Engineering Approach to Development of an End-to-End Space Cargo Handling System

This paper, prepared for the Eighth Space Congress, was developed to illustrate how system engineering techniques were applied in the early conceptual development of an end-to-end (total system, source to user) Space Shuttle Cargo Handling System. The techniques described were applied to a study under contract to NASA, Kennedy Space Center. The paper further shows that continuation of the system engineering practices on subsequent phases of the cargo handling system development will greatly enhance the orderly and timely progression of the system through the conceptual phase into the definition, production, and operational phases. The techniques involved an orderly top-down iterative methodology following the basic guidelines of a uniquely simple system engineering diagram successfully used in the past on complete weapon systems. Methods are shown where streamlined techniques were developed to keep within the confines of calendar time limitations of the initial study and to reduce the magnitude of documentation. While system engineering is more often used for development of a system containing a major prime vehicle end item such as a weapon or an aerospace vehicle, the techniques are readily applied to a system (cargo handling system) where no single end item is dominant, but the system interfaces heavily with several major aerospace vehicles in the forthcoming space program. The conceptual definition of such interfacing aerospace vehicles as the Earth Orbiting Shuttle and the Space Station in fact become part of the baseline inputs to the system engineering progress involving the cargo handling system conceptual development. The cargo handling system is visualized as a total distribution system when treated in an end-to-end fashion

Hadron-Hadron Interactions from Nf=2+1+1N_f=2+1+1 Lattice QCD: isospin-1 KKKK scattering length

We present results for the interaction of two kaons at maximal isospin. The calculation is based on $N_f=2+1+1$ flavour gauge configurations generated by the European Twisted Mass Collaboration with pion masses ranging from about $230$ to $450\,\textrm{MeV}$ at three values of the lattice spacing. The elastic scattering length $a_0^{I=1}$ is calculated at several values of the bare strange and light quark masses. We find $M_K a_0 = -0.385(16)_{\textrm{stat}} (^{+0}_{-12})_{m_s}(^{+0}_{-5})_{Z_P}(4)_{r_f}$ as the result of a combined extrapolation to the continuum and to the physical point, where the first error is statistical, and the three following are systematical. This translates to $a_0 = -0.154(6)_{\textrm{stat}}(^{+0}_{-5})_{m_s} (^{+0}_{-2})_{Z_P}(2)_{r_f}\,\textrm{fm}$.Comment: 28 pages, 18 tables, 14 figure

Temporal pixel multiplexing for simultaneous high-speed, high-resolution imaging

We introduce an imaging modality that, by offsetting pixel-exposure times during capture of a single image frame, embeds temporal information in each frame. This allows simultaneous acquisition of full-resolution images at native detector frame rates and high-speed image sequences at reduced resolution, without increasing bandwidth requirements. We demonstrate this method using macroscopic and microscopic examples, including imaging calcium transients in heart cells at 250 Hz using a 10-Hz megapixel camera

Hadron-Hadron Interactions from Nf=2+1+1N_f=2+1+1 Lattice QCD: isospin-2 ππ\pi\pi scattering length

We present results for the $I=2$ $\pi\pi$ scattering length using $N_f=2+1+1$ twisted mass lattice QCD for three values of the lattice spacing and a range of pion mass values. Due to the use of Laplacian Heaviside smearing our statistical errors are reduced compared to previous lattice studies. A detailed investigation of systematic effects such as discretisation effects, volume effects, and pollution of excited and thermal states is performed. After extrapolation to the physical point using chiral perturbation theory at NLO we obtain $M_\pi a_0=-0.0442(2)_\mathrm{stat}(^{+4}_{-0})_\mathrm{sys}$.Comment: Edited for typos, overhauled figures, more detailed comparison to existing lattice result

Automatic detection of adult cardiomyocyte for high throughput measurements of calcium and contractility

Computer Systems, Imagery and Medi

Isospin-0 ππ\pi\pi s-wave scattering length from twisted mass lattice QCD

We present results for the isospin-0 $\pi\pi$ s-wave scattering length calculated with Osterwalder-Seiler valence quarks on Wilson twisted mass gauge configurations. We use three $N_f = 2$ ensembles with unitary (valence) pion mass at its physical value (250$\sim$MeV), at 240$\sim$MeV (320$\sim$MeV) and at 330$\sim$MeV (400$\sim$MeV), respectively. By using the stochastic Laplacian Heaviside quark smearing method, all quark propagation diagrams contributing to the isospin-0 $\pi\pi$ correlation function are computed with sufficient precision. The chiral extrapolation is performed to obtain the scattering length at the physical pion mass. Our result $M_\pi a^\mathrm{I=0}_0 = 0.198(9)(6)$ agrees reasonably well with various experimental measurements and theoretical predictions. Since we only use one lattice spacing, certain systematics uncertainties, especially those arising from unitary breaking, are not controlled in our result.Comment: 21 pages, 5 figures, 6 table

Training Models in Professional Psychology Education (A Literature Review)

Intense debate on training models used in professional psychology education, including discussion on the specific training models most appropriate for educating future psychologists is far from finished. The authors reviewed articles discussing training models including results of empirical studies in professional psychology programs, which were published in several psychology journals databases (1949 to 2014). The authors have identified (a) the scientist-practitioner; (b) the practitioner model and its derivatives; (c) the clinical-scientist; and (d) the competency-based models. This article also outlines the historical development of each model and a consideration of the main principles espoused by each training model. It seems that discussion on the concept of training models and empirical studies on how these models are used in professional psychology programs outside the context of Western countries, is rare. Thus, this review could serve as a theoretical foundation for the implementation of a study aimed at filling the gap in the discussion of professional psychology program curricula, including the training models used, especially in other contexts than the Western