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000408329 020__ $$a978-3-935702-83-6
000408329 0247_ $$2datacite_doi$$a10.3204/DESY-PROC-2013-04/parker_stephen
000408329 0247_ $$2ISSN$$a1435-8077
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000408329 0881_ $$aDESY-PROC-2013-04
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000408329 1001_ $$0P:(DE-HGF)0$$aParker, S.$$b0$$eCorresponding author
000408329 1112_ $$0C13-06-24.5$$2inspire$$a9th Patras Workshop on Axions, WIMPs and WISPs$$cMainz$$d2013-06-24 - 2013-06-28$$gAXION-WIMP 2013$$wGermany
000408329 245__ $$aHidden sector photon cavity coupling
000408329 260__ $$aHamburg$$bVerlag Deutsches Elektronen-Synchrotron$$c2013
000408329 29510 $$aParker, S. "Hidden sector photon cavity coupling" in Proceedings, 9th Patras Workshop on Axions, WIMPs and WISPs (AXION-WIMP 2013) / Oberlack, Uwe, Sissol, Pierre (eds.), 2013 ; AXION-WIMP 2013 : 9th Patras Workshop on Axions, WIMPs and WISPs , 2013-06-23 - 2013-06-28, Mainz
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000408329 520__ $$aLight shining through a wall microwave cavity experiments have traditionall searched for paraphotons via the transmission of power from an actively driven cavity to a passive receiver cavity, with the two cavities separated by a barrier that is impenetrable to photons. We have extended this measurement technique to account for two-way coupling between the cavities. The presence of a paraphoton field can alter the resonance frequencies of the coupled cavity pair and as such measurements of cavity resonance frequencies can be used to constrain the paraphoton kinetic mixing parameter, $χ$.
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000408329 7001_ $$0P:(DE-HGF)0$$aRybka, G.$$b1
000408329 7001_ $$0P:(DE-HGF)0$$aTobar, M.$$b2
000408329 7870_ $$0PUBDB-2015-05816$$aOberlack, Uwe et. al.$$iisPartOf$$rDESY-PROC-2013-04$$tProceedings, 9th Patras Workshop on Axions, WIMPs and WISPs (AXION-WIMP 2013)
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