Pagliari L, Dapiaggi M, Maglia F, Sarkar T, Raychaudhuri A K, Chatterji T, Carpenter M A
Dipartimento di Scienze della Terra, Università degli Studi di Milano, via Botticelli 23, 20133 Milan,Italy.
J Phys Condens Matter. 2014 Oct 29;26(43):435303. doi: 10.1088/0953-8984/26/43/435303. Epub 2014 Oct 9.
Elastic and anelastic properties of La0.5Ca0.5MnO3 determined by resonant ultrasound spectroscopy in the frequency range ∼100-1200 kHz have been used to evaluate the role of grain size in determining the competition between ferromagnetism and Jahn-Teller/charge order of manganites which show colossal magneto resistance. At crystallite sizes of ∼75 and ∼135 nm the dominant feature is softening of the shear modulus as the charge order transition point, Tco (∼225 K), is approached from above and below, matching the form of softening seen previously in samples with 'bulk' properties. This is consistent with a bilinear dominant strain/order parameter coupling, which occurs between the tetragonal shear strain and the Jahn-Teller (Γ3(+)) order parameter. At crystallite sizes of ∼34 and ∼42 nm the charge ordered phase is suppressed but there is still softening of the shear modulus, with a minimum near Tco. This indicates that some degree of pseudoproper ferroelastic behaviour is retained. The primary cause of the suppresion of the charge ordered structure in nanocrystalline samples is therefore considered to be due to suppression of macroscopic strain, even though MnO6 octahedra must develop some Jahn-Teller distortions on a local length scale. This mechanism for stabilizing ferromagnetism differs from imposition of either an external magnetic field or a homogeneous external strain field (from a substrate), and is likely to lead both to local strain heterogeneity within the nanocrystallites and to different tilting of octahedra within the orthorhombic structure. An additional first order transition occurs near 40 K in all samples and appears to involve some very small strain contrast between two ferromagnetic structures.
通过在约100 - 1200 kHz频率范围内的共振超声光谱法测定的La0.5Ca0.5MnO3的弹性和滞弹性性质,已被用于评估晶粒尺寸在确定具有巨磁电阻的锰氧化物的铁磁性与 Jahn - Teller/电荷序之间竞争中的作用。在约75和约135 nm的微晶尺寸下,主要特征是当从高于和低于电荷序转变点Tco(约225 K)接近时,剪切模量软化,这与之前在具有“体”性质的样品中看到的软化形式相匹配。这与四方剪切应变和 Jahn - Teller(Γ3(+))序参量之间发生的双线性主导应变/序参量耦合一致。在约34和约42 nm的微晶尺寸下,电荷有序相受到抑制,但剪切模量仍有软化,在Tco附近有最小值。这表明保留了一定程度的赝本征铁弹性行为。因此,纳米晶样品中电荷有序结构被抑制的主要原因被认为是宏观应变的抑制,尽管MnO6八面体在局部长度尺度上必定会发生一些 Jahn - Teller 畸变。这种稳定铁磁性的机制不同于施加外部磁场或均匀外部应变场(来自衬底),并且可能导致纳米微晶内的局部应变不均匀性以及正交结构内八面体的不同倾斜。在所有样品中,在接近40 K处还出现了一个额外的一级转变,并且似乎涉及两个铁磁结构之间一些非常小的应变对比度。