2012
DOI: 10.1063/1.4752766
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High sensitivity SQUID-detection and feedback-cooling of an ultrasoft microcantilever

Abstract: We measure the motion of an ultrasoft cantilever, carrying a ferromagnetic particle, by means of a superconducting quantum interference device (SQUID). In our scheme, the cantilever motion modulates the magnetic flux in the SQUID due to the coupling with the magnetic particle. For the cantilever fundamental mode, cooled to temperatures below 100 mK, we achieve a dimensionless coupling factor as large as 0.07, displacement sensitivity of 200 fm/Hz, and subattonewton force sensitivity. We demonstrate the outstan… Show more

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Cited by 13 publications
(9 citation statements)
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“…In Fig 4, we have plotted the rms displacement noise of the detection coil with respect to the MRFM setup 19 (position 4 in Fig. 1) versus the integration bandwidth after the implementation of all modifications.…”
Section: Vibration Isolation Of the Cryostatmentioning
confidence: 99%
“…In Fig 4, we have plotted the rms displacement noise of the detection coil with respect to the MRFM setup 19 (position 4 in Fig. 1) versus the integration bandwidth after the implementation of all modifications.…”
Section: Vibration Isolation Of the Cryostatmentioning
confidence: 99%
“…The vibration isolation presented here is intended to be used for a low temperature MFM/MRFM setup, where an ultrasoft resonator is used to measure the properties of various spin systems 17 . Due to the low stiffness and high quality factor of the resonator the system is extremely sensitive to small forces 18 , but also to vibrations. Therefore, we will demonstrate the effectiveness of the vibration isolation by analyzing the displacement noise spectrum and thermal properties of the resonator, showing that our vibration isolation allows us to perform highly sensitive measurements in a cryogen-free dilution refrigerator.…”
Section: Introductionmentioning
confidence: 99%
“…With the flux noise S 1/2 = 220 n 0 / √ Hz, this yields an extremely low value for the predicted displacement sensitivity S 1/2 r = S 1/2 / y = 110 fm/ √ Hz, which is already a factor of 2 below the best value found in the literature. [51][52][53] Still, S r is by far not optimized and could be further improved by using a reduced linewidth for the SQUID arm in the top Nb layer and by increasing the number of spins in the magnet.…”
Section: Displacement Detectionmentioning
confidence: 99%