11,208 research outputs found

    A synoptic study of Sudden Phase Anomalies (SPA's) effecting VLF navigation and timing

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    Sudden phase anomalies (SPA's) observed on VLF recordings are related to sudden ionospheric disturbances due to solar flares. Results are presented for SPA statistics on 500 events observed in New York during the ten year period 1961 to 1970. Signals were at 10.2kHz and 13.6kHz emitted from the OMEGA transmitters in Hawaii and Trinidad. A relationship between SPA frequency and sun spot number was observed. For sun spot number near 85, about one SPA per day will be observed somewhere in the world. SPA activity nearly vanishes during periods of low sun spot number. During years of high solar activity, phase perturbations observed near noon are dominated by SPA effects beyond the 95th percentile. The SPA's can be represented by a rapid phase run-off which is approximately linear in time, peaking in about 6 minutes, and followed by a linear recovery. Typical duration is 49 minutes

    Omega VLF timing revision 1

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    The report specifically discusses time dissemination techniques, including epoch determination, frequency determination, and ambiguity resolution. It also discusses operational considerations including equipment, path selection, and adjustment procedure. epoch (the actual location or timing of periodic events) is shown to be both maintainable and calibratable by the techniques described to better than 3-microsecond accuracy; and frequency (the uniformity of the time scale) to about one part in 10 to the 12th power

    Cylindrical surface profile and diameter measuring tool and method

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    A tool is shown having a cross beam assembly made of beams joined by a center box structure. The assembly is adapted to be mounted by brackets to the outer end of a cylindrical case. The center box structure has a vertical shaft rotatably mounted therein and extending beneath the assembly. Secured to the vertical shaft is a radius arm which is adapted to rotate with the shaft. On the longer end of the radius arm is a measuring tip which contacts the cylindrical surface to be measured and which provides an electric signal representing the radius of the cylindrical surface from the center of rotation of the radius arm. An electric servomotor rotates the vertical shaft and an electronic resolver provides an electric signal representing the angle of rotation of the shaft. The electric signals are provided to a computer station which has software for its computer to calculate and print out the continuous circumference profile of the cylindrical surface, and give its true diameter and the deviations from the ideal circle

    Inflation Assisted by Heterotic Axions

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    We explore the possibility of obtaining inflation in weakly coupled heterotic string theory, where the model dependent axions are responsible for driving inflation. This model can be considered as a certain extrapolation of m2ϕ2m^{2}\phi^{2}-inflation, and is an attempt to explicitly realize the so called N-flation proposal in string theory. The instanton generated potential for the axions essentially has two parameters; a natural mass scale MM and the string coupling gsg_{s}. For isotropic compactifications leading to of order O(104)\mathcal{O} (10^4) axions in the four dimensional spectrum we find that with (M,gs)≃(MGUT,0.5)(M, g_{s})\simeq(M_{GUT}, 0.5) the observed temperature fluctuations in the CMB are correctly reproduced. We assume an initially random distribution for the vevs of the axions. The spectral index, nsn_{s}, is generically more red than for m2ϕ2m^{2}\phi^{2}-inflation. The greater the vevs, the more red the spectral index becomes. Allowing for a wide range of vevs 55 ee-foldings from the end of inflation, we find 0.946≲ns≲0.9620.946\lesssim n_{s} \lesssim 0.962. The tensor-to-scalar ratio, rr, is more sensitive to the vevs, but typically smaller than in m2ϕ2m^{2}\phi^{2}-inflation. Furthermore, in the regime where the leading order theory is valid, rr is bounded by r<0.10r < 0.10. The spectral index and the tensor-to-scalar ratio are correlated. For example, ns≃0.951n_{s}\simeq 0.951 corresponds to r≃0.036r\simeq 0.036.Comment: 1+21 pages, 2 figures, v2: Typos corrected, v3: Typos, very minor corrections, reference added, to appear in JCA
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