50,809 research outputs found
Don't sit so close to me: Unconsciously elicited affect automatically provokes social avoidance
Behavior may be automatically prompted by cues in our social environment. Previous research has focused on cognitive explanations for such effects. Here we hypothesize that affective processes are susceptible to similar automatic influences. We propose that exposure to groups stereotyped as dangerous or violent may provoke an anxiety response and, thus, a tendency to move away. In the present experiment, we subliminally exposed participants to images of such a group, and found that they displayed greater avoidance in a subsequent interaction. Critically, this effect was explained by their increased sensitivity to threat-related information. These findings demonstrate an affective mechanism responsible for nonconscious priming effects on interpersonal behavior
When not thinking leads to being and doing: Stereotype suppression and the self
Suppressing stereotypes often results in more stereotype use, an effect attributed to heightened stereotype activation. The authors report two experiments examining the consequences of suppression on two self-relevant outcomes: the active self-concept and overt behavior. Participants who suppressed stereotypes incorporated stereotypic traits into their self-concepts and demonstrated stereotype-congruent behavior compared to those who were exposed to the same stereotypes but did not suppress them. These findings address issues emerging from current theories of suppression, priming, and the active self
Automatic and ironic behavior are both mediated by changes in the self-concept
Recent accounts suggest that prime-to-behavior effects are mediated by changes to the active self-concept. Likewise, recent reports of post-suppression behavioral rebound have attributed changes to behavior to changes in the self-concept. According to such accounts, whenever an activated trait or stereotype can be easily incorporated into the active self, behavioral assimilation (i.e., behavior consistent with the activated concept) is likely to ensue. Yet, little evidence has emerged to directly support the mediating role of changes to the self-concept. The present research was designed to examine whether changes to the active self-concept are responsible for changes in behavior following stereotype suppression and priming. Participants who suppressed or were primed with stereotypes of the elderly were more likely to endorse stereotypic traits as self-descriptive and to behave in stereotypic ways. Critically, the former effect significantly mediated the latter. Implications for theories of concept activation and behavior are discussed. (C) 2011 Elsevier Inc. All rights reserved
Priming in interpersonal contexts: Implications for affect and behavior
Priming stereotypes can lead to a variety of behavioral outcomes, including assimilation, contrast, and response behaviors. However, the conditions that give rise to each of these outcomes are unspecified. Furthermore, theoretical accounts posit that prime-to-behavior effects are either direct (i.e., unmediated) or mediated by cognitive processes, whereas the role of affective processes has been largely unexplored. The present research directly investigated both of these issues. Three experiments demonstrated that priming a threatening social group ("hoodies") influences both affect and behavior in an interpersonal context. Hoodie priming produced both behavioral avoidance and several affective changes (including social apprehension, threat sensitivity, and self-reported anxiety and hostility). Importantly, avoidance following hoodie priming was mediated by anxiety and occurred only under conditions of other-(but not self-) focus. These results highlight multiple routes through which primes influence affect and behavior, and suggest that attention to self or others determine the nature of priming effects
Adaptive Neural Network Feedforward Control for Dynamically Substructured Systems
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Semileptonic Decay Scalar Form Factor and from Lattice QCD
We present a new study of D semileptonic decays on the lattice which employs
the Highly Improved Staggered Quark (HISQ) action for both the charm and the
light valence quarks. We work with MILC unquenched lattices and
determine the scalar form factor for
semileptonic decays. The form factor is obtained from a scalar current matrix
element that does not require any operator matching. We develop a new approach
to carrying out chiral/continuum extrapolations of . The method uses
the kinematic "" variable instead of or the kaon energy and is
applicable over the entire physical range. We find in the chiral plus
continuum limit and hereby improve the theory error on this quantity by a
factor of 4 compared to previous lattice determinations. Combining the
new theory result with recent experimental measurements of the product from BaBar and CLEO-c leads to the most
precise direct determination of the CKM matrix element to date,
, where the first error comes from experiment and the
second is the lattice QCD theory error. We calculate the ratio and find GeV and show
that this agrees with experiment.Comment: 23 pages, 31 figures, 11 tables. Added a paragraph in sction VII, and
updated with PDG 2010 instead of PDG 200
form factors from lattice QCD
We report the first lattice QCD calculation of the form factors for the
standard model tree-level decay . In combination with future
measurement, this calculation will provide an alternative exclusive
semileptonic determination of . We compare our results with previous
model calculations, make predictions for differential decay rates and branching
fractions, and predict the ratio of differential branching fractions between
and . We also present standard model
predictions for differential decay rate forward-backward asymmetries,
polarization fractions, and calculate potentially useful ratios of
form factors with those of the fictitious decay. Our lattice
simulations utilize NRQCD and HISQ light quarks on a subset of the MILC
Collaboration's asqtad gauge configurations, including two lattice
spacings and a range of light quark masses.Comment: 24 pages, 21 figures; Ver. 2 matches published versio
B→Dlν form factors at nonzero recoil and extraction of |Vcb|
We present a lattice QCD calculation of the B→Dlν semileptonic decay form factors f+(q2) and f0(q2) for the entire physical q2 range. Nonrelativistic QCD bottom quarks and highly improved staggered quark charm and light quarks are employed together with Nf=2+1 MILC gauge configurations. A joint fit to our lattice and BABAR experimental data allows an extraction of the Cabibbo-Kobayashi-Maskawa matrix element |Vcb|. We also determine the phenomenologically interesting ratio R(D)=B(B→Dτντ)/B(B→Dlνl) (l=e,μ). We find |Vcb|B→Dexcl=0.0402(17)(13), where the first error consists of the lattice simulation errors and the experimental statistical error and the second error is the experimental systematic error. For the branching fraction ratio we find R(D)=0.300(8)
B and Bs semileptonic decay form factors with NRQCD/HISQ quarks
We discuss our ongoing effort to calculate form factors for several B and Bs
semileptonic decays. We have recently completed the first unquenched
calculation of the form factors for the rare decay B -> K ll. Extrapolated over
the full kinematic range of q^2 via model-independent z expansion, these form
factor results allow us to calculate several Standard Model observables. We
compare with experiment (Belle, BABAR, CDF, and LHCb) where possible and make
predictions elsewhere. We discuss preliminary results for Bs -> K l nu which,
when combined with anticipated experimental results, will provide an
alternative exclusive determination of |Vub|. We are exploring the possibility
of using ratios of form factors for this decay with those for the unphysical
decay Bs -> eta_s as a means of significantly reducing form factor errors. We
are also studying B -> pi l nu, form factors for which are combined with
experiment in the standard exclusive determination of |Vub|. Our simulations
use NRQCD heavy and HISQ light valence quarks on the MILC 2+1 dynamical asqtad
configurations.Comment: 7 pages, 5 figures, presented at the 31st International Symposium on
Lattice Field Theory (Lattice 2013), 29 July - 3 August 2013, Mainz, German
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