Behavior Modification

Excerpt: Behavior modification is learning with a particular intent, namely clinical treatment and change (Ullmann & Krasner, 1965, p. 1). Initially behavior modification referred largely to operant techniques and behavior therapy to respondent techniques. As early as 1965 the terms behavior modification and behavior therapy were used interchangeably (O\u27Donohue & Krasner, 1995). With publication of the journal Behavior Research and Therapy in 1963 and the founding of the Association for the Advancement of Behavior Therapy, behavior therapy became a general term for all of these techniques. Thus behavior therapy will be used in this discussion

Principles of Behavior Therapy and Behavior Modification (Chapter 5 from The Human Reflex)

This chapter examines the theoretical aspects of the application of behavioral psychology (technically, the experimental analysis of behavior) to the process of behavior therapy. Beginning with a brief history, we will then discuss the definition of behavior therapy and behavior modification, survey a conception of problem behavior that grows out of the behavioral approach, examine basic approaches to behavior therapy, look at specific behavior change techniques, discuss biblical parallels, and consider several areas of controversy

Energy Dependence of Jet Quenching and Life-time of the Dense Matter in High-energy Heavy-ion Collisions

Suppression of high $p_T$ hadron spectra in high-energy heavy-ion collisions at different energies is studied within a pQCD parton model incorporating medium induced parton energy loss. The $p_T$ dependence of the nuclear modification factor $R_{AA}(p_T)$ is found to depend on both the energy dependence of the parton energy loss and the power-law behavior of the initial jet spectra. The high $p_T$ hadron suppression at $\sqrt{s}=62.4$ GeV and its centrality dependence are studied in detail. The overall values of the modification factor are found to provide strong constraints on the lifetime of the dense matter.Comment: 6 pages in RevTex with 3 postscript figure

BIF : a behavioral intermediate format for high level synthesis

This report describes a new intermediate format for behavioral synthesis systems, based on annotated state tables. It supports user control of the synthesis process by allowing specification of partial design structures, user-bindings and user modification of compiled designs. It is a simple and uniform representation that can be used as an intermediate exchange format for various behavioral synthesis tools. The format captures synchronous and asynchronous behavior, and serves as a good interface to the user by linking behavior and structure at each level of abstraction in the behavioral synthesis process

Dilepton distributions at backward rapidities

The dilepton production at backward rapidities in $pAu$ and $pp$ collisions at RHIC and LHC energies is investigated in the dipole approach. The results are shown through the nuclear modification ratio $R_{pA}$ considering transverse momentum and rapidity spectra. The dilepton modification ratio presents interesting behavior at the backward rapidities when compared with the already known forward ones, since it is related with the large $x$ kinematical region that is being probed. The rapidity dependence of the nuclear modification ratio in the dilepton production is strongly dependent on the Bjorken $x$ behavior of the nuclear structure function ratio $R_{F_{2}}=F_{2}^{A}/F_{2}^{p}$. The $R_{pA}$ transverse momentum dependence at backward rapidities is modified due to the large $x$ nuclear effects: at RHIC energies, for instance, the ratio $R_{pA}$ is reduced as $p_T$ increases, presenting an opposite behavior when compared with the forward one. It implies that the dilepton production at backward rapidities should carry information of the nuclear effects at large Bjorken $x$, as well as that it is useful to investigate the $p_T$ dependence of the observables in this kinematical regime.Comment: 15 pages, 6 figures. Version published in the Phys. Rev.