Superconducting YB
We utilize a high-pressure solid-state technique to prepare yttrium hexaboride (YB6) nanowires at very low temperatures of 200–240 °C. The obtained YB6 nanowires are single-crystals grown along [001] direction confirmed by HRTEM and SAED images. From the growth morphology at different time stages an...
Ausführliche Beschreibung
Gespeichert in:
| Autor*in: |
Wang, Zhen [verfasserIn] Han, Wei [verfasserIn] Zhang, Jiang [verfasserIn] Fan, Qinghua [verfasserIn] Zhao, Yanming [verfasserIn] |
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| Format: |
E-Artikel |
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| Sprache: |
Englisch |
| Erschienen: |
2021 |
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| Schlagwörter: |
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| Übergeordnetes Werk: |
Enthalten in: Ceramics international - Amsterdam [u.a.] : Elsevier Science, 1995, 47, Seite 23788-23793 |
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| Übergeordnetes Werk: |
volume:47 ; pages:23788-23793 |
| DOI / URN: |
10.1016/j.ceramint.2021.05.085 |
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ELV006326412 |
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| 520 | |a We utilize a high-pressure solid-state technique to prepare yttrium hexaboride (YB6) nanowires at very low temperatures of 200–240 °C. The obtained YB6 nanowires are single-crystals grown along [001] direction confirmed by HRTEM and SAED images. From the growth morphology at different time stages and EDS evidence, we proposed that YB6 nanowires are nucleated and grown from the submicron particle clusters. The temperature-dependent magnetization results indicate that YB6 nanostructures undergo a superconducting transition with T c = 7.8 K, which is higher than that of reported YB6 bulk single-crystals. Furthermore, the YB6 nanostructures reveal a peak effect in superconducting state observed from the magnetic hysteresis loops, approving that YB6 belongs to a type-II superconductor. The lower and upper critical magnetic fields, Hc1 and Hc2, are determined to be 251 Oe and 1104 Oe, respectively. | ||
| 650 | 4 | |a Yttrium hexaboride | |
| 650 | 4 | |a Nanowire | |
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| 650 | 4 | |a Superconductor | |
| 700 | 1 | |a Han, Wei |e verfasserin |0 (orcid)0000-0001-9662-1415 |4 aut | |
| 700 | 1 | |a Zhang, Jiang |e verfasserin |4 aut | |
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| 700 | 1 | |a Zhao, Yanming |e verfasserin |4 aut | |
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10.1016/j.ceramint.2021.05.085 doi (DE-627)ELV006326412 (ELSEVIER)S0272-8842(21)01471-1 DE-627 ger DE-627 rda eng 670 DE-600 51.60 bkl 58.45 bkl Wang, Zhen verfasserin aut Superconducting YB 2021 nicht spezifiziert zzz rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier We utilize a high-pressure solid-state technique to prepare yttrium hexaboride (YB6) nanowires at very low temperatures of 200–240 °C. The obtained YB6 nanowires are single-crystals grown along [001] direction confirmed by HRTEM and SAED images. From the growth morphology at different time stages and EDS evidence, we proposed that YB6 nanowires are nucleated and grown from the submicron particle clusters. The temperature-dependent magnetization results indicate that YB6 nanostructures undergo a superconducting transition with T c = 7.8 K, which is higher than that of reported YB6 bulk single-crystals. Furthermore, the YB6 nanostructures reveal a peak effect in superconducting state observed from the magnetic hysteresis loops, approving that YB6 belongs to a type-II superconductor. The lower and upper critical magnetic fields, Hc1 and Hc2, are determined to be 251 Oe and 1104 Oe, respectively. Yttrium hexaboride Nanowire High pressure solid state Magnetic Superconductor Han, Wei verfasserin (orcid)0000-0001-9662-1415 aut Zhang, Jiang verfasserin aut Fan, Qinghua verfasserin aut Zhao, Yanming verfasserin aut Enthalten in Ceramics international Amsterdam [u.a.] : Elsevier Science, 1995 47, Seite 23788-23793 Online-Ressource (DE-627)320584305 (DE-600)2018052-4 (DE-576)25523063X 0272-8842 nnns volume:47 pages:23788-23793 GBV_USEFLAG_U SYSFLAG_U GBV_ELV GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_105 GBV_ILN_110 GBV_ILN_150 GBV_ILN_151 GBV_ILN_224 GBV_ILN_370 GBV_ILN_602 GBV_ILN_702 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2008 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2027 GBV_ILN_2034 GBV_ILN_2038 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2056 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2088 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2118 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2190 GBV_ILN_2336 GBV_ILN_2470 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4338 GBV_ILN_4393 51.60 Keramische Werkstoffe Hartstoffe Werkstoffkunde 58.45 Gesteinshüttenkunde AR 47 23788-23793 |
| spelling |
10.1016/j.ceramint.2021.05.085 doi (DE-627)ELV006326412 (ELSEVIER)S0272-8842(21)01471-1 DE-627 ger DE-627 rda eng 670 DE-600 51.60 bkl 58.45 bkl Wang, Zhen verfasserin aut Superconducting YB 2021 nicht spezifiziert zzz rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier We utilize a high-pressure solid-state technique to prepare yttrium hexaboride (YB6) nanowires at very low temperatures of 200–240 °C. The obtained YB6 nanowires are single-crystals grown along [001] direction confirmed by HRTEM and SAED images. From the growth morphology at different time stages and EDS evidence, we proposed that YB6 nanowires are nucleated and grown from the submicron particle clusters. The temperature-dependent magnetization results indicate that YB6 nanostructures undergo a superconducting transition with T c = 7.8 K, which is higher than that of reported YB6 bulk single-crystals. Furthermore, the YB6 nanostructures reveal a peak effect in superconducting state observed from the magnetic hysteresis loops, approving that YB6 belongs to a type-II superconductor. The lower and upper critical magnetic fields, Hc1 and Hc2, are determined to be 251 Oe and 1104 Oe, respectively. Yttrium hexaboride Nanowire High pressure solid state Magnetic Superconductor Han, Wei verfasserin (orcid)0000-0001-9662-1415 aut Zhang, Jiang verfasserin aut Fan, Qinghua verfasserin aut Zhao, Yanming verfasserin aut Enthalten in Ceramics international Amsterdam [u.a.] : Elsevier Science, 1995 47, Seite 23788-23793 Online-Ressource (DE-627)320584305 (DE-600)2018052-4 (DE-576)25523063X 0272-8842 nnns volume:47 pages:23788-23793 GBV_USEFLAG_U SYSFLAG_U GBV_ELV GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_105 GBV_ILN_110 GBV_ILN_150 GBV_ILN_151 GBV_ILN_224 GBV_ILN_370 GBV_ILN_602 GBV_ILN_702 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2008 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2027 GBV_ILN_2034 GBV_ILN_2038 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2056 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2088 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2118 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2190 GBV_ILN_2336 GBV_ILN_2470 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4338 GBV_ILN_4393 51.60 Keramische Werkstoffe Hartstoffe Werkstoffkunde 58.45 Gesteinshüttenkunde AR 47 23788-23793 |
| allfields_unstemmed |
10.1016/j.ceramint.2021.05.085 doi (DE-627)ELV006326412 (ELSEVIER)S0272-8842(21)01471-1 DE-627 ger DE-627 rda eng 670 DE-600 51.60 bkl 58.45 bkl Wang, Zhen verfasserin aut Superconducting YB 2021 nicht spezifiziert zzz rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier We utilize a high-pressure solid-state technique to prepare yttrium hexaboride (YB6) nanowires at very low temperatures of 200–240 °C. The obtained YB6 nanowires are single-crystals grown along [001] direction confirmed by HRTEM and SAED images. From the growth morphology at different time stages and EDS evidence, we proposed that YB6 nanowires are nucleated and grown from the submicron particle clusters. The temperature-dependent magnetization results indicate that YB6 nanostructures undergo a superconducting transition with T c = 7.8 K, which is higher than that of reported YB6 bulk single-crystals. Furthermore, the YB6 nanostructures reveal a peak effect in superconducting state observed from the magnetic hysteresis loops, approving that YB6 belongs to a type-II superconductor. The lower and upper critical magnetic fields, Hc1 and Hc2, are determined to be 251 Oe and 1104 Oe, respectively. Yttrium hexaboride Nanowire High pressure solid state Magnetic Superconductor Han, Wei verfasserin (orcid)0000-0001-9662-1415 aut Zhang, Jiang verfasserin aut Fan, Qinghua verfasserin aut Zhao, Yanming verfasserin aut Enthalten in Ceramics international Amsterdam [u.a.] : Elsevier Science, 1995 47, Seite 23788-23793 Online-Ressource (DE-627)320584305 (DE-600)2018052-4 (DE-576)25523063X 0272-8842 nnns volume:47 pages:23788-23793 GBV_USEFLAG_U SYSFLAG_U GBV_ELV GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_105 GBV_ILN_110 GBV_ILN_150 GBV_ILN_151 GBV_ILN_224 GBV_ILN_370 GBV_ILN_602 GBV_ILN_702 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2008 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2027 GBV_ILN_2034 GBV_ILN_2038 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2056 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2088 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2118 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2190 GBV_ILN_2336 GBV_ILN_2470 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4338 GBV_ILN_4393 51.60 Keramische Werkstoffe Hartstoffe Werkstoffkunde 58.45 Gesteinshüttenkunde AR 47 23788-23793 |
| allfieldsGer |
10.1016/j.ceramint.2021.05.085 doi (DE-627)ELV006326412 (ELSEVIER)S0272-8842(21)01471-1 DE-627 ger DE-627 rda eng 670 DE-600 51.60 bkl 58.45 bkl Wang, Zhen verfasserin aut Superconducting YB 2021 nicht spezifiziert zzz rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier We utilize a high-pressure solid-state technique to prepare yttrium hexaboride (YB6) nanowires at very low temperatures of 200–240 °C. The obtained YB6 nanowires are single-crystals grown along [001] direction confirmed by HRTEM and SAED images. From the growth morphology at different time stages and EDS evidence, we proposed that YB6 nanowires are nucleated and grown from the submicron particle clusters. The temperature-dependent magnetization results indicate that YB6 nanostructures undergo a superconducting transition with T c = 7.8 K, which is higher than that of reported YB6 bulk single-crystals. Furthermore, the YB6 nanostructures reveal a peak effect in superconducting state observed from the magnetic hysteresis loops, approving that YB6 belongs to a type-II superconductor. The lower and upper critical magnetic fields, Hc1 and Hc2, are determined to be 251 Oe and 1104 Oe, respectively. Yttrium hexaboride Nanowire High pressure solid state Magnetic Superconductor Han, Wei verfasserin (orcid)0000-0001-9662-1415 aut Zhang, Jiang verfasserin aut Fan, Qinghua verfasserin aut Zhao, Yanming verfasserin aut Enthalten in Ceramics international Amsterdam [u.a.] : Elsevier Science, 1995 47, Seite 23788-23793 Online-Ressource (DE-627)320584305 (DE-600)2018052-4 (DE-576)25523063X 0272-8842 nnns volume:47 pages:23788-23793 GBV_USEFLAG_U SYSFLAG_U GBV_ELV GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_105 GBV_ILN_110 GBV_ILN_150 GBV_ILN_151 GBV_ILN_224 GBV_ILN_370 GBV_ILN_602 GBV_ILN_702 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2008 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2027 GBV_ILN_2034 GBV_ILN_2038 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2056 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2088 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2118 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2190 GBV_ILN_2336 GBV_ILN_2470 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4338 GBV_ILN_4393 51.60 Keramische Werkstoffe Hartstoffe Werkstoffkunde 58.45 Gesteinshüttenkunde AR 47 23788-23793 |
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10.1016/j.ceramint.2021.05.085 doi (DE-627)ELV006326412 (ELSEVIER)S0272-8842(21)01471-1 DE-627 ger DE-627 rda eng 670 DE-600 51.60 bkl 58.45 bkl Wang, Zhen verfasserin aut Superconducting YB 2021 nicht spezifiziert zzz rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier We utilize a high-pressure solid-state technique to prepare yttrium hexaboride (YB6) nanowires at very low temperatures of 200–240 °C. The obtained YB6 nanowires are single-crystals grown along [001] direction confirmed by HRTEM and SAED images. From the growth morphology at different time stages and EDS evidence, we proposed that YB6 nanowires are nucleated and grown from the submicron particle clusters. The temperature-dependent magnetization results indicate that YB6 nanostructures undergo a superconducting transition with T c = 7.8 K, which is higher than that of reported YB6 bulk single-crystals. Furthermore, the YB6 nanostructures reveal a peak effect in superconducting state observed from the magnetic hysteresis loops, approving that YB6 belongs to a type-II superconductor. The lower and upper critical magnetic fields, Hc1 and Hc2, are determined to be 251 Oe and 1104 Oe, respectively. Yttrium hexaboride Nanowire High pressure solid state Magnetic Superconductor Han, Wei verfasserin (orcid)0000-0001-9662-1415 aut Zhang, Jiang verfasserin aut Fan, Qinghua verfasserin aut Zhao, Yanming verfasserin aut Enthalten in Ceramics international Amsterdam [u.a.] : Elsevier Science, 1995 47, Seite 23788-23793 Online-Ressource (DE-627)320584305 (DE-600)2018052-4 (DE-576)25523063X 0272-8842 nnns volume:47 pages:23788-23793 GBV_USEFLAG_U SYSFLAG_U GBV_ELV GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_105 GBV_ILN_110 GBV_ILN_150 GBV_ILN_151 GBV_ILN_224 GBV_ILN_370 GBV_ILN_602 GBV_ILN_702 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2008 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2027 GBV_ILN_2034 GBV_ILN_2038 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2056 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2088 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2118 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2190 GBV_ILN_2336 GBV_ILN_2470 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4338 GBV_ILN_4393 51.60 Keramische Werkstoffe Hartstoffe Werkstoffkunde 58.45 Gesteinshüttenkunde AR 47 23788-23793 |
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Wang, Zhen Han, Wei Zhang, Jiang Fan, Qinghua Zhao, Yanming |
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We utilize a high-pressure solid-state technique to prepare yttrium hexaboride (YB6) nanowires at very low temperatures of 200–240 °C. The obtained YB6 nanowires are single-crystals grown along [001] direction confirmed by HRTEM and SAED images. From the growth morphology at different time stages and EDS evidence, we proposed that YB6 nanowires are nucleated and grown from the submicron particle clusters. The temperature-dependent magnetization results indicate that YB6 nanostructures undergo a superconducting transition with T c = 7.8 K, which is higher than that of reported YB6 bulk single-crystals. Furthermore, the YB6 nanostructures reveal a peak effect in superconducting state observed from the magnetic hysteresis loops, approving that YB6 belongs to a type-II superconductor. The lower and upper critical magnetic fields, Hc1 and Hc2, are determined to be 251 Oe and 1104 Oe, respectively. |
| abstractGer |
We utilize a high-pressure solid-state technique to prepare yttrium hexaboride (YB6) nanowires at very low temperatures of 200–240 °C. The obtained YB6 nanowires are single-crystals grown along [001] direction confirmed by HRTEM and SAED images. From the growth morphology at different time stages and EDS evidence, we proposed that YB6 nanowires are nucleated and grown from the submicron particle clusters. The temperature-dependent magnetization results indicate that YB6 nanostructures undergo a superconducting transition with T c = 7.8 K, which is higher than that of reported YB6 bulk single-crystals. Furthermore, the YB6 nanostructures reveal a peak effect in superconducting state observed from the magnetic hysteresis loops, approving that YB6 belongs to a type-II superconductor. The lower and upper critical magnetic fields, Hc1 and Hc2, are determined to be 251 Oe and 1104 Oe, respectively. |
| abstract_unstemmed |
We utilize a high-pressure solid-state technique to prepare yttrium hexaboride (YB6) nanowires at very low temperatures of 200–240 °C. The obtained YB6 nanowires are single-crystals grown along [001] direction confirmed by HRTEM and SAED images. From the growth morphology at different time stages and EDS evidence, we proposed that YB6 nanowires are nucleated and grown from the submicron particle clusters. The temperature-dependent magnetization results indicate that YB6 nanostructures undergo a superconducting transition with T c = 7.8 K, which is higher than that of reported YB6 bulk single-crystals. Furthermore, the YB6 nanostructures reveal a peak effect in superconducting state observed from the magnetic hysteresis loops, approving that YB6 belongs to a type-II superconductor. The lower and upper critical magnetic fields, Hc1 and Hc2, are determined to be 251 Oe and 1104 Oe, respectively. |
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