2020
DOI: 10.48550/arxiv.2004.13441
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Straightening of Superconducting HERA Dipoles for the Any-Light-Particle-Search Experiment ALPS II

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Cited by 6 publications
(7 citation statements)
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“…For instance a hypothetical cylindrical detector with L = 1 m and area A = 0.785 m 2 (corresponding to a radius of 0.5 m) can operate at f 4.3 × 10 7 Hz. It is interesting to notice that the idea behind these detectors is similar to the one underpinning various axion experiments, including telescopes such as CAST [269,270] (decommissioned) and IAXO [271] (planned) and 'light-shining-through-a-wall' experiments such as OSQAR [272,273] (decommissioned), ALPS [274,275] (decommissioned) and ALPS II [276,277] (under construction). Using data already collected in axion experiments such as OSQAR and CAST, it is possible to place bounds on the presence of a stochastic background of GWs at the frequency at which these detectors naturally operate [278], which is extremely high: f ∼ 10 15 Hz and f ∼ 10 18 Hz.…”
Section: Conversion In An External Static Magnetic Fieldmentioning
confidence: 99%
“…For instance a hypothetical cylindrical detector with L = 1 m and area A = 0.785 m 2 (corresponding to a radius of 0.5 m) can operate at f 4.3 × 10 7 Hz. It is interesting to notice that the idea behind these detectors is similar to the one underpinning various axion experiments, including telescopes such as CAST [269,270] (decommissioned) and IAXO [271] (planned) and 'light-shining-through-a-wall' experiments such as OSQAR [272,273] (decommissioned), ALPS [274,275] (decommissioned) and ALPS II [276,277] (under construction). Using data already collected in axion experiments such as OSQAR and CAST, it is possible to place bounds on the presence of a stochastic background of GWs at the frequency at which these detectors naturally operate [278], which is extremely high: f ∼ 10 15 Hz and f ∼ 10 18 Hz.…”
Section: Conversion In An External Static Magnetic Fieldmentioning
confidence: 99%
“…These expressions are valid as long as the GWs and the generated EMWs are in phase coherence throughout their propagation in the magnetic field region. Under the assumption that the external B-field is surrounded by a circular beam tube of diameter d, coherent EMW generation is guaranteed if (see Appendix D): [92,93], MADMAX [94,95], BabyI-AXO and IAXO [96], used to estimate the minimum detectable GW amplitude through magnetic conversions of GWs (gravitons) to EMWs (photons) in vacuum: B is the magnetic field magnitude, L is the magnetic field length, d is the diameter of the magnetized tube, and BLA 1/2 , with A = n tubes πd 2 /4, is the figure of merit for GW detection by magnetic conversion into EMWs. Also shown are the effective lower frequency cut-off Eq.…”
Section: Magnetic Gw-emw Conversion In Vacuummentioning
confidence: 99%
“…of axions into photons or vice versa. In Table 3 we show the parameters of the magnetic field region of the next generation of axion experiments: the LSW experiment ALPS IIc [92,93], the haloscope MADMAX [94,95], and the helioscopes BabyIAXO and IAXO [96]. Unfortunately, the prospects to probe the CGMB exploiting these magnetic conversion facilities appear to be rather slim.…”
Section: Magnetic Gw-emw Conversion In Vacuummentioning
confidence: 99%
“…Both techniques are sensitive to changes in the phase ∆θ. Small fluctuations in ∆θ will move energy into other frequency bins leading to signal losses proportional to ∆θ 2 rms . Larger drifts shift energy into the other quadrature and changes by 180 • will invert the signal leading to its cancellation during the integration.…”
Section: Signal Demodulation and Phase Trackingmentioning
confidence: 99%
“…The fundamental parts of ALPS II are shown in Figure 1. The apparatus consists of two strings of twelve straightened 8.8 m long, 5.3 T HERA magnets which are separated by a light-tight wall [2]. Inside the magnet string on the left side of the wall, some of the photons from a high power laser will be converted into axionlike particles.…”
Section: Introductionmentioning
confidence: 99%