Curie temperatures of CoPt ultrathin continuous films

The effects of layer thickness and thermal annealing on Curie temperature have been studied for CoPt ultrathin continuous layers in AlN/CoPt multilayer structures. It is found that there exists a critical thickness below which Curie temperature rapidly decreases due to the loss of spin-spin interactions in the vicinity of interface. After high temperature annealing, the in-plane lattice constant of CoPt film is increased and the exchange coupling parameter is decreased. Consequently, Curie temperatures decrease for some films with large thickness, compared with as-deposited state. Upon annealing at 600 ∘C, CoPt undergoes ordering transformation, which also contributes to the degradation of the Curie temperature. However, when the CoPt film thickness is below 2 nm, the Curie temperature is increased after annealing. Especially for 1 nm thick film, the Curie temperature is strikingly increased from 173 ∘C to 343 ∘C after annealing at 600 ∘C. This effect is attributed to the out-of-plane lattice deformation of CoPt thin layers in AlN/CoPt multilayer structures.

[1]  Huang,et al.  Magnetism in the few-monolayers limit: A surface magneto-optic Kerr-effect study of the magnetic behavior of ultrathin films of Co, Ni, and Co-Ni alloys on Cu(100) and Cu(111). , 1994, Physical review. B, Condensed matter.

[2]  G. Hadjipanayis,et al.  CoPt/Ag nanocomposites for high density recording media , 1998 .

[3]  J. Rodríguez-Viejo,et al.  Nanocalorimetric analysis of the ferromagnetic transition in ultrathin films of nickel , 2008 .

[4]  Q. Jiang,et al.  Size and interface effects on critical temperatures of ferromagnetic, ferroelectric and superconductive nanocrystals , 2005 .

[5]  P. Schweiss,et al.  Finite-size shift of the Curie temperature of ferromagnetic lanthanum cobaltite thin films , 2005 .

[6]  C. Zhao,et al.  Does the Nonmagnetic Surface Layer Exist Throughout Ferromagnetic Nanoparticles , 2007 .

[7]  Z. L. Wang,et al.  Size‐Dependent Chemical and Magnetic Ordering in L10‐FePt Nanoparticles , 2006 .

[8]  C. Leroux,et al.  Magnetic properties and chemical ordering in Co-Pt , 1989 .

[9]  C. Vaz,et al.  Magnetism in ultrathin film structures , 2008 .

[10]  R. F. Willis,et al.  Thickness-dependent Curie temperatures of ultrathin magnetic films: effect of the range of spin-spin interactions. , 2001, Physical review letters.

[11]  D. Goll,et al.  Temperature dependence of the magnetic properties of L10-FePt nanostructures and films , 2010 .

[12]  G. Hadjipanayis,et al.  CoPt and FePt Thin Films for High Density Recording Media , 2000 .

[13]  Michael E. Fisher,et al.  Scaling Theory for Finite-Size Effects in the Critical Region , 1972 .

[14]  Li,et al.  Dimensional crossover in ultrathin Ni(111) films on W(110). , 1992, Physical review letters.

[15]  G. Hadjipanayis,et al.  CoPt/Ag nanocomposites with (001) texture , 2001 .

[16]  Wei Liu,et al.  Roles of L10 ordering in controlling the magnetic anisotropy and coercivity of (111)-oriented CoPt ultrathin continuous layers in CoPt/AlN multilayer films , 2011 .

[17]  Chang Q. Sun,et al.  Coordination Imperfection Suppressed Phase Stability of Ferromagnetic, Ferroelectric, and Superconductive Nanosolids , 2004 .

[18]  S. Piramanayagam Perpendicular recording media for hard disk drives , 2007 .

[19]  X. Meng,et al.  Size-dependent Curie transition of Ni nanocrystals , 2009 .

[20]  Margaret Evans Best,et al.  High K/sub u/ materials approach to 100 Gbits/in/sup 2/ , 2000 .

[21]  Ji Shi,et al.  Controlling the magnetic anisotropy of CoPt∕AlN multilayer films , 2007 .

[22]  C. Zhao,et al.  Size-dependent ordering and Curie temperatures of FePt nanoparticles , 2008 .

[23]  K. Hono,et al.  Particulate structure of L10 ordered ultrathin FePt films for perpendicular recording , 2008 .

[24]  Q. Jiang,et al.  Size and interface effects on ferromagnetic and antiferromagnetic transition temperatures , 2006 .