6,667 research outputs found

    Teacher Residency Requirements in Buffalo: Reconciling Community Benefits with Marketplace Realities

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    In 2011 Buffalo Public Schools repealed a requirement that its teachers live in the district — a “residency rule”. Because the city’s urban population accounts for only one quarter of the metro population, this rule severely restricted the teacher applicant pools. However, the residency requirement had some benefits to the community — such as providing neighborhood role models and making teachers more aware of the students’ life situations and challenges. Teachers who understand where students are coming from are likely to relate to them more easily – especially when the teachers are identifiable members of the community and share the students’ cultural and racial backgrounds

    PT-Symmetric Quantum Electrodynamics

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    The Hamiltonian for quantum electrodynamics becomes non-Hermitian if the unrenormalized electric charge ee is taken to be imaginary. However, if one also specifies that the potential AμA^\mu in such a theory transforms as a pseudovector rather than a vector, then the Hamiltonian becomes PT symmetric. The resulting non-Hermitian theory of electrodynamics is the analog of a spinless quantum field theory in which a pseudoscalar field ϕ\phi has a cubic self-interaction of the form iϕ3i\phi^3. The Hamiltonian for this cubic scalar field theory has a positive spectrum, and it has recently been demonstrated that the time evolution of this theory is unitary. The proof of unitarity requires the construction of a new operator called C, which is then used to define an inner product with respect to which the Hamiltonian is self-adjoint. In this paper the corresponding C operator for non-Hermitian quantum electrodynamics is constructed perturbatively. This construction demonstrates the unitarity of the theory. Non-Hermitian quantum electrodynamics is a particularly interesting quantum field theory model because it is asymptotically free.Comment: 9 pages, no figures, revtex

    Eigenvalue problems for the complex PT-symmetric potential V(x)= igx

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    The spectrum of complex PT-symmetric potential, V(x)=igxV(x)=igx, is known to be null. We enclose this potential in a hard-box: V(x1)=V(|x| \ge 1) =\infty and in a soft-box: V(x1)=0V(|x|\ge 1)=0. In the former case, we find real discrete spectrum and the exceptional points of the potential. The asymptotic eigenvalues behave as Enn2.E_n \sim n^2. The solvable purely imaginary PT-symmetric potentials vanishing asymptotically known so far do not have real discrete spectrum. Our solvable soft-box potential possesses two real negative discrete eigenvalues if g<(1.22330447)|g|<(1.22330447). The soft-box potential turns out to be a scattering potential not possessing reflectionless states.Comment: no figures, 9 page

    Addendum to SSV Generic OFT First Stage Ascent Base Convective Heating Environments

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    Convective environments for OFT Mission C are presented in graphs for first stage convective heating to the internal surfaces of the OMS nozzle, to the aft facing 8 and 9 RCS nozzles, and to the base (trailing edge) of the vertical tail

    Pseudohermitian Hamiltonians, time-reversal invariance and Kramers degeneracy

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    A necessary and sufficient condition in order that a (diagonalizable) pseudohermitian operator admits an antilinear symmetry T such that T^{2}=-1 is proven. This result can be used as a quick test on the T-invariance properties of pseudohermitian Hamiltonians, and such test is indeed applied, as an example, to the Mashhoon-Papini Hamiltonian.Comment: 6 page

    State Action and the NCAA: Will Tarkanian Sport the Old Look?

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    State Action and the NCAA: Will Tarkanian Sport the Old Look?

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    Microlensing events from the 11-year observations of the Wendelstein Calar Alto Pixellensing Project

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    We present the results of the decade-long M31 observation from the Wendelstein Calar Alto Pixellensing Project (WeCAPP). WeCAPP has monitored M31 from 1997 till 2008 in both R- and I-filters, thus provides the longest baseline of all M31 microlensing surveys. The data are analyzed with the difference imaging analysis, which is most suitable to study variability in crowded stellar fields. We extracted light curves based on each pixel, and devised selection criteria that are optimized to identify microlensing events. This leads to 10 new events, and sums up to a total of 12 microlensing events from WeCAPP, for which we derive their timescales, flux excesses, and colors from their light curves. The color of the lensed stars fall between (R-I) = 0.56 to 1.36, with a median of 1.0 mag, in agreement with our expectation that the sources are most likely bright, red stars at post main-sequence stage. The event FWHM timescales range from 0.5 to 14 days, with a median of 3 days, in good agreement with predictions based on the model of Riffeser et al. (2006).Comment: 44 pages, 16 figures, 5 tables. ApJ accepte

    On the pseudo-Hermitian nondiagonalizable Hamiltonians

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    We consider a class of (possibly nondiagonalizable) pseudo-Hermitian operators with discrete spectrum, showing that in no case (unless they are diagonalizable and have a real spectrum) they are Hermitian with respect to a semidefinite inner product, and that the pseudo-Hermiticity property is equivalent to the existence of an antilinear involutory symmetry. Moreover, we show that a typical degeneracy of the real eigenvalues (which reduces to the well known Kramers degeneracy in the Hermitian case) occurs whenever a fermionic (possibly nondiagonalizable) pseudo-Hermitian Hamiltonian admits an antilinear symmetry like the time-reversal operator TT. Some consequences and applications are briefly discussed.Comment: 22 page

    Stellar kinematics and populations out to 1.5 effective radius in the elliptical galaxy NGC4636

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    We present high quality long slit spectra along the major and minor axes out to 1.5 effective radius (ReR_e) of the massive galaxy NGC4636 taken by Hobby-Eberly Telescope (HET). Using Fourier Correlation Quotient (FCQ) method, we measured the stellar line-of-sight velocity distribution along the axes. Furthermore, six Lick/IDS indices (Hβ,Mgb,Fe5015,Fe5270,Fe5335,Fe5406H\beta,Mgb,Fe_{5015},Fe_{5270},Fe_{5335},Fe_{5406}) are derived from the clean spectrum. By comparing the measured absorption line strengths with the predictions of Simple Stellar Populations (SSP) models, we derived ages, total metallicity and α\alpha abundance profiles of the galaxy. This galaxy presents old and [α/Fe][\alpha/Fe] over abundant stellar populations. Indeed, using the SSP model, we obtained the broadband color profiles. The theoretical colors match well with the measured colors and present red sharp peaks at the galaxy center. The sharp peaks of the colors are mainly shaped by the high metallicity in the galaxy center. Interestingly, the galaxy has steep negative metallicity gradients, but trend flattens outwards. This result likly suggests that the center and outer regions of the galaxy formed through different formation process.Comment: 14 pages, 7 figures, accepted by RA
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