3,211 research outputs found

    Development and Characterisation of a Gas System and its Associated Slow-Control System for an ATLAS Small-Strip Thin Gap Chamber Testing Facility

    Full text link
    A quality assurance and performance qualification laboratory was built at McGill University for the Canadian-made small-strip Thin Gap Chamber (sTGC) muon detectors produced for the 2019-2020 ATLAS experiment muon spectrometer upgrade. The facility uses cosmic rays as a muon source to ionise the quenching gas mixture of pentane and carbon dioxide flowing through the sTGC detector. A gas system was developed and characterised for this purpose, with a simple and efficient gas condenser design utilizing a Peltier thermoelectric cooler (TEC). The gas system was tested to provide the desired 45 vol% pentane concentration. For continuous operations, a state-machine system was implemented with alerting and remote monitoring features to run all cosmic-ray data-acquisition associated slow-control systems, such as high/low voltage, gas system and environmental monitoring, in a safe and continuous mode, even in the absence of an operator.Comment: 23 pages, LaTeX, 14 figures, 4 tables, proof corrections for Journal of Instrumentation (JINST), including corrected Fig. 8b

    Direct measurement of the 14N(p,g)15O S-factor

    Full text link
    We have measured the 14N(p,g)15O excitation function for energies in the range E_p = 155--524 keV. Fits of these data using R-matrix theory yield a value for the S-factor at zero energy of 1.64(17) keV b, which is significantly smaller than the result of a previous direct measurement. The corresponding reduction in the stellar reaction rate for 14N(p,g)15O has a number of interesting consequences, including an impact on estimates for the age of the Galaxy derived from globular clusters.Comment: 5 pages, 3 figures, submitted to Phys. Rev. Let

    Multi-frequency fine resolution imaging radar instrumentation and data acquisition

    Get PDF
    Development of a dual polarized L-band radar imaging system to be used in conjunction with the present dual polarized X-band radar is described. The technique used called for heterodyning the transmitted frequency from X-band to L-band and again heterodyning the received L-band signals back to X-band for amplification, detection, and recording

    Constraining ^(26)Al+p resonances using ^(26)Al(^3He,d)^(27)Si

    Get PDF
    The ^(26)Al(^3He,d)^(27)Si reaction was measured from 0°≤θ_(c.m.)≤35° at E(^3He)=20 MeV using a quadrupole-dipole-dipole-dipole magnetic spectrometer. States in ^(27)Si were observed above the background at 7652 and 7741 keV and upper limits were set for the state at 7592 keV. Implications for the ^(26)Al(p,γ)^(27)Si stellar reaction rate are discussed

    Charge Imbalance and Bilayer 2D Electron Systems at νT=1\nu_T = 1

    Full text link
    We use interlayer tunneling to study bilayer 2D electron systems at νT=1\nu_T = 1 over a wide range of charge density imbalance, Δν=ν1−ν2\Delta \nu =\nu_1-\nu_2, between the two layers. We find that the strongly enhanced tunneling associated with the coherent excitonic νT=1\nu_T = 1 phase at small layer separation can survive at least up to an imbalance of Δν\Delta \nu = 0.5, i.e (ν1,ν2)(\nu_1, \nu_2) = (3/4, 1/4). Phase transitions between the excitonic νT=1\nu_T = 1 state and bilayer states which lack significant interlayer correlations can be induced in three different ways: by increasing the effective interlayer spacing d/ℓd/\ell, the temperature TT, or the charge imbalance, Δν\Delta \nu. We observe that close to the phase boundary the coherent νT=1\nu_T = 1 phase can be absent at Δν\Delta \nu = 0, present at intermediate Δν\Delta \nu, but then absent again at large Δν\Delta \nu, thus indicating an intricate phase competition between it and incoherent quasi-independent layer states. At zero imbalance, the critical d/ℓd/\ell shifts linearly with temperature, while at Δν\Delta \nu = 1/3 the critical d/ℓd/\ell is only weakly dependent on TT. At Δν\Delta \nu = 1/3 we report the first observation of a direct phase transition between the coherent excitonic νT=1\nu_T = 1 bilayer integer quantum Hall phase and the pair of single layer fractional quantized Hall states at ν1\nu_1 = 2/3 and ν2=1/3\nu_2=1/3.Comment: 13 pages, 8 postscript figures. Final published versio
    • …
    corecore