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机译:自旋玻璃$ hbox {FeGa} _ {2} hbox {O} _ {4} $系统的磁行为
Department of Physics,, Kookmin University,, Seoul, Korea;
Arrhenius law; freezing temperature; frozen disordered spin; spin-glass;
机译:$ {hbox {CaO}} hbox {-} {hbox {P}} _ {2} {hbox {O}} _ {5} hbox {-} {hbox {Na}} _ {{2} {hbox {O}} hbox {-} {hbox {Fe}} _ {2} {hbox {O}} _ {3} hbox {-} {hbox {SiO}} _ {2} $玻璃热处理后
机译:$ {hbox {Ba}} _ {1hbox {-} {rm x}} {hbox {La}} _ {rm x} {hbox {Fe}} _ {12} {hbox {O}}的结构和磁性_ {19} $由$ {hbox {Ba}} _ {1hbox {-} {rm x}} {hbox {La}} _ {rm x} {hbox {Fe}} _ {2} {hbox {O }} _ {4} $
机译:<公式的磁性结构式 in>“>
机译:分子磁性材料中的旋转玻璃行为和磁性分裂{n(n-c_4h_9)_4 m〜Ⅱfe〜Ⅲ(c_2o_4)_3} _ n(m = co,mn)
机译:磁性系统中的量子临界行为:Y 3铂4,Y 2铁2铝10和Y 2铂2铅。
机译:蜂窝状Li2RhO3的强磁挫败和反位错导致旋转玻璃行为
机译:$$ hbox {mgo} { - } hbox {al} _ {2} hbox {o} _ {3} { - } hbox {sio} _ {2} $$ Mgo - A1 2 o 3 - SiO 2玻璃陶瓷系统
机译:sc(1-x)U(x)pd3系统的非费米液体和自旋玻璃行为