847 research outputs found

    An Effective Field Theory Calculation of the Parity Violating Asymmetry in n+p -> d+gamma

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    Weak interactions are expected to induce a parity violating pion-nucleon coupling, h_{\pi NN}^{(1)}. This coupling should be measurable in a proposed experiment to study the parity violating asymmetry A_\gamma in the process \vec n + p \to d+\gamma. We compute the leading dependence of A_\gamma on the coupling h_{\pi NN}^{(1)} using recently developed effective field theory techniques and find an asymmetry of A_\gamma = +0.17 h_{\pi NN}^{(1)} at leading order. This asymmetry has the opposite sign to that given by Desplanques, Donoghue and Holstein.Comment: 7 pages, 2 figures from 3 eps files, late

    GHRS and ORFEUS-II Observations of the Highly Ionized Interstellar Medium Toward ESO141-055

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    We present Goddard High Resolution Spectrograph and ORFEUS-II measurements of Si IV, CIV, N V, and O VI absorption in the interstellar medium of the Galactic disk and halo toward the nucleus of the Seyfert galaxy ESO141-055. The high ionization absorption is strong, with line strengths consistent with the spectral signature expected for hot (log T = 5-6) collisionally ionized gas in either a ``Galactic fountain'' or an inhomogeneous medium containing a mixture of conductive interfaces and turbulent mixing layers. The total O VI column density of log N ~ 15 suggests that the scale height of O VI is large (>3 kpc) in this direction. Comparison of the high ion column densities with measurements for other sight lines indicates that the highly ionized gas distribution is patchy. The amount of O VI perpendicular to the Galactic plane varies by at least a factor of ~4 among the complete halo sight lines thus far studied. In addition to the high ion absorption, lines of low ionization species are also present in the spectra. With the possible exception of Ar I, which may have a lower than expected abundance resulting from partial photoionization of gas along the sight line, the absorption strengths are typical of those expected for the warm, neutral interstellar medium. The sight line intercepts a cold molecular cloud with log N(H2) ~ 19. The cloud has an identifiable counterpart in IRAS 100-micron emission maps of this region of the sky. We detect a Ly-alpha absorber associated with ESO141-055 at z = 0.03492. This study presents an enticing glimpse into the interstellar and intergalactic absorption patterns that will be observed at high spectral resolution by the Far Ultraviolet Spectroscopic Explorer.Comment: 24 pages + 8 figures, uses aaspp4.sty. Accepted for publication in Ap

    Second Harmonic Coherent Driving of a Spin Qubit in a Si/SiGe Quantum Dot

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    We demonstrate coherent driving of a single electron spin using second harmonic excitation in a Si/SiGe quantum dot. Our estimates suggest that the anharmonic dot confining potential combined with a gradient in the transverse magnetic field dominates the second harmonic response. As expected, the Rabi frequency depends quadratically on the driving amplitude and the periodicity with respect to the phase of the drive is twice that of the fundamental harmonic. The maximum Rabi frequency observed for the second harmonic is just a factor of two lower than that achieved for the first harmonic when driving at the same power. Combined with the lower demands on microwave circuitry when operating at half the qubit frequency, these observations indicate that second harmonic driving can be a useful technique for future quantum computation architectures.Comment: 9 pages, 9 figure

    Gate fidelity and coherence of an electron spin in a Si/SiGe quantum dot with micromagnet

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    The gate fidelity and the coherence time of a qubit are important benchmarks for quantum computation. We construct a qubit using a single electron spin in a Si/SiGe quantum dot and control it electrically via an artificial spin-orbit field from a micromagnet. We measure an average single-qubit gate fidelity of ≈\approx 99%\% using randomized benchmarking, which is consistent with dephasing from the slowly evolving nuclear spins in substrate. The coherence time measured using dynamical decoupling extends up to ≈\approx 400 μ\mus for 128 decoupling pulses, with no sign of saturation. We find evidence that the coherence time is limited by noise in the 10 kHz −- 1 MHz range, possibly because charge noise affecting the spin via the micromagnet gradient. This work shows that an electron spin in a Si/SiGe quantum dot is a good candidate for quantum information processing as well as for a quantum memory, even without isotopic purification

    A programmable two-qubit quantum processor in silicon

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    With qubit measurement and control fidelities above the threshold of fault-tolerance, much attention is moving towards the daunting task of scaling up the number of physical qubits to the large numbers needed for fault tolerant quantum computing. Here, quantum dot based spin qubits may offer significant advantages due to their potential for high densities, all-electrical operation, and integration onto an industrial platform. In this system, the initialisation, readout, single- and two-qubit gates have been demonstrated in various qubit representations. However, as seen with other small scale quantum computer demonstrations, combining these elements leads to new challenges involving qubit crosstalk, state leakage, calibration, and control hardware which provide invaluable insight towards scaling up. Here we address these challenges and demonstrate a programmable two-qubit quantum processor in silicon by performing both the Deutsch-Josza and the Grover search algorithms. In addition, we characterise the entanglement in our processor through quantum state tomography of Bell states measuring state fidelities between 85-89% and concurrences between 73-80%. These results pave the way for larger scale quantum computers using spins confined to quantum dots

    Learning the rules of the ‘student game’: Transforming the ‘student habitus’ through [im]mobility

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    In recent years, a growing body of literature has emerged concerning the mobilities of students, specifically relating to the interactions between local and non-local students, which can accentuate unequal access to education; social interactions and learner outcomes. Central to much of this literature is a sense that being mobile in institutional choice is the most appropriate and expected approach to successful university life. Conversely, local students, disadvantaged by their age, history, external commitments and immobility, are thought to be unlikely to share the same ‘student experiences’ as their traditional counterparts, leading to feelings of alienation within the student community. This paper will seek to problematise this binary by examining the experiences of a group of local and non-local students studying at the University of Portsmouth using Bourdieu’s reading of habitus and capital. This is useful as it provides a more critical insight into how students’ [dis]advantaged learner identities are [re]produced through their everyday sociability. Moreover, these findings extend previous discussions of first year transitions by questioning the influence of accommodation upon the formation of identities and the initial experiences of ‘being’, or ‘becoming’ students. This paper also seeks to extend previous theoretical tendencies that privilege identity formation through mobility rather than stasis

    Two Photon Contribution to Polarization in K+→π+μ+μ−K^+ \rightarrow \pi^+ \mu^+ \mu^-

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    Short distance physics involving virtual top and charm quarks contributes to μ+\mu^+ (and μ−\mu^-) polarization in the decay K+→π+μ+μ−K^+ \rightarrow \pi^+ \mu^+ \mu^-. Measurement of the parity violating asymmetry (ΓR−ΓL)/(ΓR+ΓL)(\Gamma_R - \Gamma_L)/(\Gamma_R + \Gamma_L), where ΓR\Gamma_R and ΓL\Gamma_L are the rates to produce right and left-handed μ+\mu^+, may provide valuable information on the unitarity triangle. The parity violating asymmetry also gets a contribution from Feynman diagrams with two photon intermediate states. We estimate this two photon contribution to the asymmetry and discuss briefly the two photon contribution to time reversal odd asymmetries that involve both the μ+\mu^+ and μ−\mu^- polarizations.Comment: (19 pages, 5 figures available on request. Uses phyzzx), CALT-68-1798, UCSD/PTH 92-2

    Final State Interactions and CP Violation in KL→π+π−e+e−K_L \to \pi^+ \pi^- e^+ e^-

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    Using chiral perturbation theory we calculate the imaginary parts of the KL→π+π−e+e−K_L \rightarrow \pi^+ \pi^- e^+ e^- form factors that arise from ππ→π+π−\pi \pi \rightarrow \pi^+ \pi^- and ππ→π+π−γ∗\pi \pi \rightarrow \pi^+ \pi^- \gamma^* rescattering. We discuss their influence on CP violating variables in KL→π+π−e+e−K_L \rightarrow \pi^+ \pi^- e^+ e^-.Comment: ; 12 pages, 2 figures, TeX format; uses epsf.tex, tables.tex, and phyzzx.te
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