2015
DOI: 10.1016/j.nima.2014.10.013
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Design and calibration of the 34 GHz Yale microwave cavity experiment

Abstract: Several proposed models of the cold dark matter in the universe include light neutral bosons with sub-eV masses. In many cases their detection hinges on their infrequent interactions with Standard Model photons at subeV energies. We describe the design and performance of an experiment to search for aberrations from the broadband noise power associated with a 5 K copper resonant cavity in the vicinity of 34 GHz (0.1 meV). The cavity, microwave receiver, and data reduction are described. Several configurations o… Show more

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Cited by 7 publications
(7 citation statements)
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References 44 publications
(63 reference statements)
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“…where Y is the measured ratio of hot/cold noise power spectra and A is the measured hot/cold gain ratio. 15 N A should be independent of the presence of the cavity mode in the spectrum, and empirically it also exhibits no systematic dependence on RF frequency. Thus we can break the degeneracy in Y -factor measurements around the TM 010 resonance by subtracting ( NA ) j , the average receiver added noise obtained from off-resonance Y -factor measurements.…”
Section: A the Rescaling Proceduresmentioning
confidence: 95%
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“…where Y is the measured ratio of hot/cold noise power spectra and A is the measured hot/cold gain ratio. 15 N A should be independent of the presence of the cavity mode in the spectrum, and empirically it also exhibits no systematic dependence on RF frequency. Thus we can break the degeneracy in Y -factor measurements around the TM 010 resonance by subtracting ( NA ) j , the average receiver added noise obtained from off-resonance Y -factor measurements.…”
Section: A the Rescaling Proceduresmentioning
confidence: 95%
“…which did not however adopt our frequency-domain approach or consider the effects of filter-induced correlations. See Ref [15]. for further discussion of this experiment 9.…”
mentioning
confidence: 99%
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“…ADMX is suited to masses < 10 µeV and has currently set constraints between 1.9 µeV < m a < 3.69 µeV [21,46]. Larger masses require adjustments to the cavity and amplification technology [96,97]. The Yale Wright Laboratory experiment of Refs.…”
Section: Discussionmentioning
confidence: 99%
“…Such experiments require less assumptions about the nature of these WISP particles (they do not require the particles to constitute halo dark matter), but are inherently less sensitive as they require two WISP-photon conversions. Several microwave haloscope [23][24][25][26][27][28] and LSW [29][30][31][32][33] experiments have been conducted to date, with no reports of any signals congruent with WISP detection. The majority of these searches have been conducted below 10 GHz due to a multitude of technical issues and limitations.…”
Section: Introductionmentioning
confidence: 99%