This paper proposes the novel concept and method of the feed line resonator (FLR). By introducing the external quality factor adjusting line, the feed lines can be transformed to resonators, and can be used not only for providing external coupling, as well as generate extra transmission poles in the passband. The conditions for generating transmission poles by using the FLR are systematically investigated. The key advancement of the FLR method is that extra transmission poles are introduced, without increase the number of conventional resonators, the filter bandwidth can be extended and the selectivity also improved. The triple-mode FLR was proposed which can realize six extra transmission poles in the pass band and n transmission zeros out-of-band. A five-section multi-mode resonator proposed for wideband filter. Single-, two-, three- and four-stage wideband superconducting filters were designed to demonstrate the FLR method. These filters exhibit extreme sharp skirts, the attenuation slop at lower and higher band can reach 273.9 dB/GHz and 523.7 dB/GHz, respectively. The passband is from 2.26 GHz to 5.54 GHz with the FBW (fractional bandwidth) of 95 %. The measure results agree well with the simulated ones.
{"title":"The feed line resonator (FLR) method and it’s application to superconducting wideband filter design with extreme sharp skirt","authors":"Xilong Lu, Rui Zhang, Qingyu Kong, Shi-gang Zhou, Xudong Bai, Liguo Zhou, Guangsong Wei, Xueyang Fang","doi":"10.1088/1361-6668/ad5628","DOIUrl":"https://doi.org/10.1088/1361-6668/ad5628","url":null,"abstract":"\u0000 This paper proposes the novel concept and method of the feed line resonator (FLR). By introducing the external quality factor adjusting line, the feed lines can be transformed to resonators, and can be used not only for providing external coupling, as well as generate extra transmission poles in the passband. The conditions for generating transmission poles by using the FLR are systematically investigated. The key advancement of the FLR method is that extra transmission poles are introduced, without increase the number of conventional resonators, the filter bandwidth can be extended and the selectivity also improved. The triple-mode FLR was proposed which can realize six extra transmission poles in the pass band and n transmission zeros out-of-band. A five-section multi-mode resonator proposed for wideband filter. Single-, two-, three- and four-stage wideband superconducting filters were designed to demonstrate the FLR method. These filters exhibit extreme sharp skirts, the attenuation slop at lower and higher band can reach 273.9 dB/GHz and 523.7 dB/GHz, respectively. The passband is from 2.26 GHz to 5.54 GHz with the FBW (fractional bandwidth) of 95 %. The measure results agree well with the simulated ones.","PeriodicalId":21985,"journal":{"name":"Superconductor Science and Technology","volume":" 16","pages":""},"PeriodicalIF":0.0,"publicationDate":"2024-06-10","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"141366314","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2024-06-09DOI: 10.1088/1361-6668/ad55cf
D. Xi, Xinwei Cai, Qingyang Wang, Chen Guo, Li Li, Meng Song, Yan Zhang, Dongliang Wang, Yanwei Ma, Guo Yan, Furen Wang, Zizhao Gan
In this work, amorphous B coated Mg nanopowder (BCMN) is synthesized and the transport properties of MgB2 superconducting wire is significantly enhanced with different contents of BCMN. BCMN has high reactivity since it contains nanoscale Mg and amorphous B. It allows to obtain MgB2 nanocrystals at only 400 °C with the compression of a lattice parameter and expansion of c lattice parameters compared to MgB2 formed by micron-sized Mg mixed with amorphous B (Mg+B) powders. These MgB2 nanocrystals serve as crystal nuclei and promote the crystallization and growth of MgB2. The mismatch of different lattice parameters prepared using BCMN and M+B powders induces low angle grain boundaries (LAGBs) embedded in MgB2 grains. LAGB acts as plane defects, leading to a dominant surface pinning mechanism and an enhancement in the critical current density dependent on the magnetic field (J c(H)). At 4.2 K in 6 T, transport critical current density (J ct) of wire with 20 wt.% BCMN is 6.7×104 A·cm−2, approximately 1.8 times wire with 0 wt.% BCMN.
{"title":"Amorphous B coated Mg nanopowder induces low angle grain boundaries and enhances J\u0000 c of MgB2 wire","authors":"D. Xi, Xinwei Cai, Qingyang Wang, Chen Guo, Li Li, Meng Song, Yan Zhang, Dongliang Wang, Yanwei Ma, Guo Yan, Furen Wang, Zizhao Gan","doi":"10.1088/1361-6668/ad55cf","DOIUrl":"https://doi.org/10.1088/1361-6668/ad55cf","url":null,"abstract":"\u0000 In this work, amorphous B coated Mg nanopowder (BCMN) is synthesized and the transport properties of MgB2 superconducting wire is significantly enhanced with different contents of BCMN. BCMN has high reactivity since it contains nanoscale Mg and amorphous B. It allows to obtain MgB2 nanocrystals at only 400 °C with the compression of a lattice parameter and expansion of c lattice parameters compared to MgB2 formed by micron-sized Mg mixed with amorphous B (Mg+B) powders. These MgB2 nanocrystals serve as crystal nuclei and promote the crystallization and growth of MgB2. The mismatch of different lattice parameters prepared using BCMN and M+B powders induces low angle grain boundaries (LAGBs) embedded in MgB2 grains. LAGB acts as plane defects, leading to a dominant surface pinning mechanism and an enhancement in the critical current density dependent on the magnetic field (J\u0000 c(H)). At 4.2 K in 6 T, transport critical current density (J\u0000 ct) of wire with 20 wt.% BCMN is 6.7×104 A·cm−2, approximately 1.8 times wire with 0 wt.% BCMN.","PeriodicalId":21985,"journal":{"name":"Superconductor Science and Technology","volume":" 37","pages":""},"PeriodicalIF":0.0,"publicationDate":"2024-06-09","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"141366811","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}