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Hydrothermal synthesis of nickel doped cobalt ferrite nanoparticles: optical and magnetic properties

机译:镍掺杂钴铁氧体纳米粒子的水热合成:光学和磁性

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摘要

Nickel-doped cobalt ferrite $$[{ext {Co}}_{1- x }hbox {Ni}_{ x }hbox {Fe}_{2}hbox {O}_{4} ,(0le xle 1)]$$ [ Co 1 - x Ni x Fe 2 O 4 ( 0 ≤ x ≤ 1 ) ] nanoparticles are synthesized by means of hydrothermal method. The structural, morphological and microstructural characterization revealed crystallite size was roughly spherical for lower nickel concentration while for higher ones in diamond shape consisting of nanosized grains. The optical band-gap ( $$E_{g}$$ E g ) values decreased with the $${ext {Ni}}^{2+}$$ Ni 2 + ions ( x ) concentration being 2.94 and 2.51 eV for $$x=0$$ x = 0 and $$x=1$$ x = 1 , respectively. The presence of nickel in the cobalt ferrite structure affected the magnetic properties. For instance, the saturation magnetization, $$M_{s}$$ M s and remanent magnetization, $$M_{r}$$ M r decreased from 369 to 256 emu cm_(−3)and 131–45 emu cm_(−3)for $$x=0$$ x = 0 and $$x=1$$ x = 1 , respectively. The $$M_{s}$$ M s data was discussed in term of the three-sublattice of non-collinear spin (canted spin) structure proposed by Yafet and Kittel model. On the other hand the coercivity, $$H_{c}$$ H c from 890 Oe to 1590 Oe for $$x=0$$ x = 0 and $$x=0.6$$ x = 0.6 , and sharply dropped to 50 Oe for $$x=1.$$ x = 1 . The enhanced coercivity was discussed in terms of particles size, defects and residual strain which may act as pinning centers. The cubic magnetocrystalline constant, $$K_{1}$$ K 1 determined by using the “law of approach” to saturation decreases with $${ext {Ni}}^{2+}$$ Ni 2 + ions ( x ) concentration being $$4.9imes 10^{6}$$ 4.9 × 10 6 and $$2.8imes 10^{6}$$ 2.8 × 10 6 erg cm_(−3)for $$x=0$$ x = 0 and $$x=1$$ x = 1 , respectively. These results were discussed in terms of the inter-particle interactions induced by the presence of $${ext {Ni}}^{2+}$$ Ni 2 + ions at the octahedral sites which affected the strength of L–S coupling.
机译:镍掺杂钴铁氧体$$ [{ t​​ext {Co}} _ {1- x} hbox {Ni} _ {x} hbox {Fe} _ {2} hbox {O} _ { 4} ,,(0 le x le 1)] $$ [Co 1-x Ni x Fe 2 O 4(0≤x≤1)]纳米粒子是通过水热法合成的。结构,形态和微结构特征表明,对于较低的镍浓度,微晶尺寸大致为球形,而对于较高的镍,其晶粒尺寸由纳米晶粒组成。光学带隙($$ E_ {g} $$ E g)值随$$ {文本{Ni}} ^ {2 +} $$ Ni 2 +离子(x)浓度为2.94和2.51而减小$$ x = 0 $ x = 0和$$ x = 1 $ x = 1的eV。钴铁氧体结构中镍的存在影响了磁性。例如,饱和磁化强度$$ M_ {s} $$ M s和剩余磁化强度$$ M_ {r} $$ M r从369 emu cm _(-3)和131-45 emu cm _(- 3)分别适用于$$ x = 0 $$ x = 0和$$ x = 1 $$ x = 1的情况。根据Yafet和Kittel模型提出的非共线自旋(倾斜自旋)结构的三个子格讨论了$$ M_ {s} $$ M s数据。另一方面,矫顽力为$$ H_ {c} $$ H c,从$ 890 Oe到1590 Oe,$ xx = 0 $ x = 0和$$ x = 0.6 $ x = 0.6,并急剧下降到$ xx = 1。$$ x = 1时为50 Oe。讨论了提高的矫顽力,涉及颗粒大小,缺陷和可能作为钉扎中心的残余应变。通过使用“接近法则”确定饱和的立方磁晶常数$$ K_ {1} $$ K 1随着$$ {文字{Ni}} ^ {2 +} $$ Ni 2 +离子( x)的浓度为$$ x = 0 $时的$$ 4.9倍10 ^ {6} $$ 4.9×10 6和$$ 2.8 倍10 ^ {6} $$ 2.8×10 6 erg cm _(− 3)对于$$ x = 0 $ $ x = 0和$$ x = 1 = $$ x = 1。根据八面体位点处的$$ {文字{Ni}} ^ {2 +} $$ Ni 2 +离子的存在影响了L–S的强度,讨论了粒子间相互作用的结果。耦合。

著录项

  • 来源
    《Journal of materials science》 |2018年第17期|14657-14667|共11页
  • 作者单位

    Instituto de Física, Universidade Federal de Goiás,Instituto de Química, Universidade Federal de Goias;

    Instituto de Física, Universidade Federal de Goiás,Department of Physics, Gandhi Institute of Technology and Management (GITAM) University;

    Instituto de Física, Universidade Federal de Goiás;

  • 收录信息 美国《科学引文索引》(SCI);美国《工程索引》(EI);美国《生物学医学文摘》(MEDLINE);
  • 原文格式 PDF
  • 正文语种 eng
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