{"title":"非超导最佳掺杂 PrBCO 铜酸盐中的磁场诱导相变和弱铁磁性","authors":"Mahieddine Lahoubi;Shengli Pu;Weinan Liu;Zhe Yang","doi":"10.1109/LMAG.2024.3350428","DOIUrl":null,"url":null,"abstract":"In this letter, we report anomalous magnetic properties in high dc magnetic fields \n<italic>H</i>\n up to 11 and 16 T from 1.35 up to 20 K on PrBa\n<sub>2</sub>\nCu\n<sub>3</sub>\nO\n<sub>6.95</sub>\n (PrBCO\n<sub>6.95</sub>\n) cuprate ceramic. Significant magnetic-field effects are revealed in the derivative of the magnetization \n<italic>M</i>\n(\n<italic>T</i>\n) versus \n<italic>T</i>\n using two sets of values of \n<italic>H</i>\n selected in the range of 2.5–9.5 T. Anomalies are observed at the low-critical point \n<italic>T</i>\n<sub>cr</sub>\n = 4–5 K, in the region of the spin reorientation phase transition temperature \n<italic>T</i>\n<sub>2</sub>\n = 10.5 K, and around the Néel temperature of the antiferromagnetic ordering of the Pr\n<sup>3+</sup>\n sublattice \n<italic>T</i>\n<sub>N</sub>\n = 14 K. Using Arrott plot analysis, we identified weak field-induced phase transitions at two critical fields, \n<italic>H</i>\n<sub>cr1</sub>\n(\n<italic>T</i>\n) ∼ 3.3 T and \n<italic>H</i>\n<sub>cr2</sub>\n(\n<italic>T</i>\n) ∼ 7.5 T, whose associated transition lines exhibit an almost temperature-independent behavior in the range 1.35 K-\n<italic>T</i>\n<sub>2</sub>\n, and seem to vanish in the vicinity of \n<italic>T</i>\n<sub>N</sub>\n. When \n<italic>T</i>\n decreases from 20 K, an increase occurs in the derivative of the magnetization \n<italic>M</i>\n(\n<italic>H</i>\n) versus \n<italic>H</i>\n for 0.5 T < \n<italic>H</i>\n < 1 T, as well as in the differential susceptibility \n<italic>χ</i>\n<sub>d</sub>\n(\n<italic>T</i>\n) versus \n<italic>T</i>\n where a shape change occurs when crossing \n<italic>T</i>\n<sub>cr</sub>\n. The spontaneous magnetization \n<italic>M</i>\n<sub>S</sub>\n(\n<italic>T</i>\n), which was deduced by extrapolation to zero-field from the field-linear regime up to 2 T, shows an inverse variation with \n<italic>T</i>\n and a shape change when crossing \n<italic>T</i>\n<sub>N</sub>\n and \n<italic>T</i>\n<sub>2</sub>\n. These features, which are taken as evidence for an additional weak ferromagnetic-like component that survives above \n<italic>T</i>\n<sub>N</sub>\n, result from the significant role of the Pr-Cu(2) magnetic coupling.","PeriodicalId":13040,"journal":{"name":"IEEE Magnetics Letters","volume":"15 ","pages":"1-5"},"PeriodicalIF":1.1000,"publicationDate":"2024-01-05","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Magnetic Field-Induced Phase Transition and Weak Ferromagnetism in Nonsuperconducting Optimally Doped PrBCO Cuprate\",\"authors\":\"Mahieddine Lahoubi;Shengli Pu;Weinan Liu;Zhe Yang\",\"doi\":\"10.1109/LMAG.2024.3350428\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"In this letter, we report anomalous magnetic properties in high dc magnetic fields \\n<italic>H</i>\\n up to 11 and 16 T from 1.35 up to 20 K on PrBa\\n<sub>2</sub>\\nCu\\n<sub>3</sub>\\nO\\n<sub>6.95</sub>\\n (PrBCO\\n<sub>6.95</sub>\\n) cuprate ceramic. Significant magnetic-field effects are revealed in the derivative of the magnetization \\n<italic>M</i>\\n(\\n<italic>T</i>\\n) versus \\n<italic>T</i>\\n using two sets of values of \\n<italic>H</i>\\n selected in the range of 2.5–9.5 T. Anomalies are observed at the low-critical point \\n<italic>T</i>\\n<sub>cr</sub>\\n = 4–5 K, in the region of the spin reorientation phase transition temperature \\n<italic>T</i>\\n<sub>2</sub>\\n = 10.5 K, and around the Néel temperature of the antiferromagnetic ordering of the Pr\\n<sup>3+</sup>\\n sublattice \\n<italic>T</i>\\n<sub>N</sub>\\n = 14 K. Using Arrott plot analysis, we identified weak field-induced phase transitions at two critical fields, \\n<italic>H</i>\\n<sub>cr1</sub>\\n(\\n<italic>T</i>\\n) ∼ 3.3 T and \\n<italic>H</i>\\n<sub>cr2</sub>\\n(\\n<italic>T</i>\\n) ∼ 7.5 T, whose associated transition lines exhibit an almost temperature-independent behavior in the range 1.35 K-\\n<italic>T</i>\\n<sub>2</sub>\\n, and seem to vanish in the vicinity of \\n<italic>T</i>\\n<sub>N</sub>\\n. When \\n<italic>T</i>\\n decreases from 20 K, an increase occurs in the derivative of the magnetization \\n<italic>M</i>\\n(\\n<italic>H</i>\\n) versus \\n<italic>H</i>\\n for 0.5 T < \\n<italic>H</i>\\n < 1 T, as well as in the differential susceptibility \\n<italic>χ</i>\\n<sub>d</sub>\\n(\\n<italic>T</i>\\n) versus \\n<italic>T</i>\\n where a shape change occurs when crossing \\n<italic>T</i>\\n<sub>cr</sub>\\n. The spontaneous magnetization \\n<italic>M</i>\\n<sub>S</sub>\\n(\\n<italic>T</i>\\n), which was deduced by extrapolation to zero-field from the field-linear regime up to 2 T, shows an inverse variation with \\n<italic>T</i>\\n and a shape change when crossing \\n<italic>T</i>\\n<sub>N</sub>\\n and \\n<italic>T</i>\\n<sub>2</sub>\\n. These features, which are taken as evidence for an additional weak ferromagnetic-like component that survives above \\n<italic>T</i>\\n<sub>N</sub>\\n, result from the significant role of the Pr-Cu(2) magnetic coupling.\",\"PeriodicalId\":13040,\"journal\":{\"name\":\"IEEE Magnetics Letters\",\"volume\":\"15 \",\"pages\":\"1-5\"},\"PeriodicalIF\":1.1000,\"publicationDate\":\"2024-01-05\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"IEEE Magnetics Letters\",\"FirstCategoryId\":\"101\",\"ListUrlMain\":\"https://ieeexplore.ieee.org/document/10381794/\",\"RegionNum\":4,\"RegionCategory\":\"物理与天体物理\",\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"Q4\",\"JCRName\":\"ENGINEERING, ELECTRICAL & ELECTRONIC\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"IEEE Magnetics Letters","FirstCategoryId":"101","ListUrlMain":"https://ieeexplore.ieee.org/document/10381794/","RegionNum":4,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q4","JCRName":"ENGINEERING, ELECTRICAL & ELECTRONIC","Score":null,"Total":0}
引用次数: 0
摘要
在这封信中,我们报告了 PrBa2Cu3O6.95 (PrBCO6.95) 铜氧化物陶瓷在 1.35 至 20 K 高直流磁场 H 达 11 和 16 T 时的异常磁性能。在低临界点 Tcr = 4-5 K、自旋重新定向相变温度 T2 = 10.利用阿罗特图分析,我们确定了在两个临界场 Hcr1(T) ∼ 3.3 T 和 Hcr2(T) ∼ 7.5 T 处的弱场诱导相变,其相关的过渡线在 1.35 K-T2 范围内表现出几乎与温度无关的行为,并且似乎在 TN 附近消失。当 T 从 20 K 开始降低时,磁化 M(H) 相对于 H 的导数(0.5 T < H < 1 T)以及相对于 T 的差分磁感应强度 χd(T)都会增加。自发磁化 MS(T) 是通过从场-线性机制推断出的零场,最高可达 2 T,显示出随 T 的反向变化,以及在跨越 TN 和 T2 时的形状变化。这些特征被认为是在 TN 以上存在一个额外的弱铁磁样成分的证据,是 Pr-Cu(2) 磁耦合的重要作用所致。
Magnetic Field-Induced Phase Transition and Weak Ferromagnetism in Nonsuperconducting Optimally Doped PrBCO Cuprate
In this letter, we report anomalous magnetic properties in high dc magnetic fields
H
up to 11 and 16 T from 1.35 up to 20 K on PrBa
2
Cu
3
O
6.95
(PrBCO
6.95
) cuprate ceramic. Significant magnetic-field effects are revealed in the derivative of the magnetization
M
(
T
) versus
T
using two sets of values of
H
selected in the range of 2.5–9.5 T. Anomalies are observed at the low-critical point
T
cr
= 4–5 K, in the region of the spin reorientation phase transition temperature
T
2
= 10.5 K, and around the Néel temperature of the antiferromagnetic ordering of the Pr
3+
sublattice
T
N
= 14 K. Using Arrott plot analysis, we identified weak field-induced phase transitions at two critical fields,
H
cr1
(
T
) ∼ 3.3 T and
H
cr2
(
T
) ∼ 7.5 T, whose associated transition lines exhibit an almost temperature-independent behavior in the range 1.35 K-
T
2
, and seem to vanish in the vicinity of
T
N
. When
T
decreases from 20 K, an increase occurs in the derivative of the magnetization
M
(
H
) versus
H
for 0.5 T <
H
< 1 T, as well as in the differential susceptibility
χ
d
(
T
) versus
T
where a shape change occurs when crossing
T
cr
. The spontaneous magnetization
M
S
(
T
), which was deduced by extrapolation to zero-field from the field-linear regime up to 2 T, shows an inverse variation with
T
and a shape change when crossing
T
N
and
T
2
. These features, which are taken as evidence for an additional weak ferromagnetic-like component that survives above
T
N
, result from the significant role of the Pr-Cu(2) magnetic coupling.
期刊介绍:
IEEE Magnetics Letters is a peer-reviewed, archival journal covering the physics and engineering of magnetism, magnetic materials, applied magnetics, design and application of magnetic devices, bio-magnetics, magneto-electronics, and spin electronics. IEEE Magnetics Letters publishes short, scholarly articles of substantial current interest.
IEEE Magnetics Letters is a hybrid Open Access (OA) journal. For a fee, authors have the option making their articles freely available to all, including non-subscribers. OA articles are identified as Open Access.