2016
DOI: 10.1103/physrevaccelbeams.19.082001
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Dependence of trapped-flux-induced surface resistance of a large-grain Nb superconducting radio-frequency cavity on spatial temperature gradient during cooldown throughTc

Abstract: Recent studies by Romanenko et al. revealed that cooling down a superconducting cavity under a large spatial temperature gradient decreases the amount of trapped flux and leads to reduction of the residual surface resistance. In the present paper, the flux expulsion ratio and the trapped-flux-induced surface resistance of a large-grain cavity cooled down under a spatial temperature gradient up to 80 K=m are studied under various applied magnetic fields from 5 to 20 μT. We show the flux expulsion ratio improves… Show more

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Cited by 42 publications
(32 citation statements)
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“…The surface resistance depends on the amplitude H 0 of the RF magnetic field H(t) = H 0 sin ωt and can be significantly altered by the materials treatments. For instance, R s of electropolished Nb cavities 4 at 2 K and 1 GHz increases with the RF field amplitude, consistent with the well-known reduction of a quasiparticle gap and the superfluid density by the RF pairbreaking currents [9][10][11] , grain boundaries and nonsuperconducting precipitates 5 , or trapped vortices [12][13][14][15][16][17][18][19] . However, the Nb cavities doped with nitrogen [20][21][22][23] , titanium 24 or other impurities 25,26 can exhibit a striking reduction of R s (H 0 ) by factors of 2-4 as H 0 increases from 0 to 0.5H c , where H c is the thermodynamic critical field.…”
Section: Introductionsupporting
confidence: 72%
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“…The surface resistance depends on the amplitude H 0 of the RF magnetic field H(t) = H 0 sin ωt and can be significantly altered by the materials treatments. For instance, R s of electropolished Nb cavities 4 at 2 K and 1 GHz increases with the RF field amplitude, consistent with the well-known reduction of a quasiparticle gap and the superfluid density by the RF pairbreaking currents [9][10][11] , grain boundaries and nonsuperconducting precipitates 5 , or trapped vortices [12][13][14][15][16][17][18][19] . However, the Nb cavities doped with nitrogen [20][21][22][23] , titanium 24 or other impurities 25,26 can exhibit a striking reduction of R s (H 0 ) by factors of 2-4 as H 0 increases from 0 to 0.5H c , where H c is the thermodynamic critical field.…”
Section: Introductionsupporting
confidence: 72%
“…If a magnetic field is applied, Abrikosov vortices can penetrate into the sample and modify the local density of states. Hot spots resulting from vortex bundles, trapped during the cavity cooldown through the superconducting critical T c , can essentially limit the performance of SRF cavities [12][13][14][15][16][17][18][19] . Imaging of trapped vortices can give valuable information about the electronic structure of the vortex core in the first few nm at the surface, which plays the key role in RF dissipation.…”
Section: Vorticesmentioning
confidence: 99%
“…However, there are still significant variations in flux trapping and flux expulsion from Nb cavities that are not well understood, for instance, cavities manufactured from Nb sheet with same material specifications produced by the same vendor, and treated by the same recipe produces cavities that expel flux differently 2 . The increase in residual resistance due to the trapped magnetic field has been studied in several SRF cavities with respect to the starting Nb material 24 , surface preparation 18 , and nitrogen diffusion conditions 25 . Theoretically, a multi-scale collective pinning mechanism is suggested for rf dissipation in SRF cavities 26 , and a recent review indicates pinning possibilities could be related to dislocation structures 27 .…”
Section: Introductionmentioning
confidence: 99%
“…Reduction of R s (or improvement of Q) has been the primary interest of researchers of resonant cavities over the last decades. Vortex-free Nb cavities [50][51][52][53][54][55] exhibit huge quality factor Q ∼ 10 10 -10 12 at T < 2 K [56][57][58][59] even under the strong rf current [60][61][62][63] close to the depairing current density. The depairing current density J d is related to the bias current of SSPD and is the maximum current that SRF cavities and superconducting cables can support.…”
Section: Introductionmentioning
confidence: 99%