microwave surface resistance
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2022 ◽  
Vol 12 (2) ◽  
pp. 546
Author(s):  
Peng Sha ◽  
Weimin Pan ◽  
Jiyuan Zhai ◽  
Zhenghui Mi ◽  
Song Jin ◽  
...  

Medium-temperature (mid-T) furnace baking was conducted at 650 MHz superconducting radio-frequency (SRF) cavity for circular electron positron collider (CEPC), which enhanced the cavity unloaded quality factor (Q0) significantly. In the vertical test (2.0 K), Q0 of 650 MHz cavity reached 6.4 × 1010 at 30 MV/m, which is remarkably high at this unexplored frequency. Additionally, the cavity quenched at 31.2 MV/m finally. There was no anti-Q-slope behavior after mid-T furnace baking, which is characteristic of 1.3 GHz cavities. The microwave surface resistance (RS) was also studied, which indicated both very low Bardeen–Cooper–Schrieffer (BCS) and residual resistance. The recipe of cavity process in this paper is simplified and easy to duplicate, which may benefit the SRF community.


Author(s):  
Patrick Krkotić ◽  
Artur Romanov ◽  
Nikki Tagdulang ◽  
Guilherme Telles ◽  
Teresa Puig ◽  
...  

Abstract To assess the feasibility of using high-temperature superconductors for the beam screens of future circular colliders, we have undertaken a study of the power dependence of the microwave surface resistance in state-of-the-art REBCO coated conductors at about 8GHz and 50K. We have employed a dielectric resonator to produce radio-frequency electromagnetic fields on the surface of the coated conductors having amplitudes similar to those generated by proton bunches circulating in the vacuum chamber of the proposed hadron-hadron Future Circular Collider at CERN. We show that surface resistances in REBCO coated conductors without artificial pinning centers are more affected by a radio-frequency magnetic field than those containing nano-inclusions. Despite that, at 8GHz, 50K, and 9T, most REBCO coated conductors studied outperform copper in terms of surface resistance, with the best sample having a 2.3mΩ surface resistance while being subject to an RF field 2.5 times stronger than that in the FCC-hh. We also extrapolate the measured data to 16T and 1GHz, the actual FCC-hh dipole magnetic field, and mid beam frequency spectrum, demonstrating the possibility of lowering the surface resistance of the vacuum chamber by up to two orders of magnitude compared to copper. Further, we discuss the correlation between the time structure of the electromagnetic fields provided by vector network analyzers compared to the proton bunches' time structure in the collider and present the effect of low alternating magnetic fields on vortex displacement and the possibility of demagnetization of superconducting samples.


2021 ◽  
Vol 69 (1) ◽  
pp. 189-197
Author(s):  
Richard Gumbleton ◽  
Jerome A. Cuenca ◽  
Samuel Hefford ◽  
Kenneth Nai ◽  
Adrian Porch

2020 ◽  
Vol 16 (3) ◽  
pp. 216-223
Author(s):  
Woo Il Yang ◽  
Sungho Lee ◽  
Ho Sang Jung ◽  
Hye-Rim Kim ◽  
Sang Young Lee

2019 ◽  
Vol 64 (10) ◽  
pp. 969
Author(s):  
P. A. Borisenko ◽  
A. O. Pokusinskii ◽  
A. L. Kasatkin

A model for the microwave response of a nanostructured high-Tc superconductor (HTS) film, with implanted nanoparticles and nanorods of a dielectric material or point-like and columnar irradiation defects with a nano-sized cross-section is developed. In this case, the microwave surface resistance Rs(T,H,ω) is calculated both for the Meissner and mixed states of a superconductor film in an applied dc magnetic field. The obtained results indicate that the implantation of dielectric nanoparticles or point-like radiation defects can significantly improve superconductor characteristics at microwave frequencies. Namely, these nano-sized structural defects can decrease the surface resistance in the Meissner state and eliminate the oscillations of Abrikosov vortices and the related microwave energy losses, thus decreasing the contribution of Abrikosov vortices to the Rs value in the mixed state of a HTS film.


2019 ◽  
Vol 15 (5) ◽  
pp. 572-581
Author(s):  
Sungho Lee ◽  
Jiyoung Jang ◽  
Ho Sang Jung ◽  
Won Nam Kang ◽  
Sang Young Lee

2018 ◽  
Vol 32 (7) ◽  
pp. 1903-1908
Author(s):  
Cheng Zeng ◽  
Liu Chen ◽  
Shirong Bu ◽  
Junsong Ning ◽  
Qishao Zhang ◽  
...  

2018 ◽  
Vol 28 (4) ◽  
pp. 1-4 ◽  
Author(s):  
Shigetoshi Ohshima ◽  
N. Takanashi ◽  
Atsushi Saito ◽  
K. Nakajima ◽  
T. Nagayama

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