TY - JOUR
T1 - Pt content dependence of the switching field distributions of CoPtCr-SiO2 perpendicular media characterized by subtracting the effect of thermal agitation
AU - Shimatsu, T.
AU - Kondo, T.
AU - Mitsuzuka, K.
AU - Watanabe, S.
AU - Aoi, H.
AU - Muraoka, H.
AU - Nakamura, Y.
N1 - Funding Information:
ACKNOWLEDGMENT This work was supported in part by the IT Program (RR2002) of MEXT. The authors would like to thank Dr. O. Kitakami and Dr. S. Okamoto for their helpful discussion and some technical support.
PY - 2007/6
Y1 - 2007/6
N2 - The switching field distributions (SFD) of CoPtCr-SiO2 perpendicular media as a function of Pt content were characterized by subtracting the effect of thermal agitation, and discussed in relation to the microstructure. DC demagnetizing (DCD) magnetization curves and minor dc demagnetizing (M-DCD) magnetization curves were measured at applied field sweep rates of ∼10 Oe/s and ∼108 Oe/s. We estimated the width of SFD, ΔSFD, from the difference between the DCD and M-DCD curves, and defined them as ΔHr/Hr (at ∼ 10 Oe/s) and ΔHrP/HrP (at ∼10 8 Oe/s). The values of ΔSFD characterized by subtracting the effect of thermal agitation, ΔHo/Ho, were nearly half those of ΔHr/Hr for 10-nm-thick media. ΔHo/Ho was about 0.10 at 10 at%Pt content, and increased as the Pt content increased, reaching 0.17 at 30 at%Pt content. The increase in ΔHo/Ho was probably caused by an increase in the stacking fault density and the formation of fee layers in the hep CoPtCr lattice. A simple calculation based on the coherent switching of magnetization revealed that the c-axis distribution results in ΔH o/Ho of about 0.08, independent of Pt content. These results suggest that the ΔSFD due to the grain-to-grain anisotropy field variation was small, only 0.02-0.03.
AB - The switching field distributions (SFD) of CoPtCr-SiO2 perpendicular media as a function of Pt content were characterized by subtracting the effect of thermal agitation, and discussed in relation to the microstructure. DC demagnetizing (DCD) magnetization curves and minor dc demagnetizing (M-DCD) magnetization curves were measured at applied field sweep rates of ∼10 Oe/s and ∼108 Oe/s. We estimated the width of SFD, ΔSFD, from the difference between the DCD and M-DCD curves, and defined them as ΔHr/Hr (at ∼ 10 Oe/s) and ΔHrP/HrP (at ∼10 8 Oe/s). The values of ΔSFD characterized by subtracting the effect of thermal agitation, ΔHo/Ho, were nearly half those of ΔHr/Hr for 10-nm-thick media. ΔHo/Ho was about 0.10 at 10 at%Pt content, and increased as the Pt content increased, reaching 0.17 at 30 at%Pt content. The increase in ΔHo/Ho was probably caused by an increase in the stacking fault density and the formation of fee layers in the hep CoPtCr lattice. A simple calculation based on the coherent switching of magnetization revealed that the c-axis distribution results in ΔH o/Ho of about 0.08, independent of Pt content. These results suggest that the ΔSFD due to the grain-to-grain anisotropy field variation was small, only 0.02-0.03.
KW - CoPtCr-SiO perpendicular recording media
KW - Film composition
KW - Pulse field
KW - Switching field distribution
KW - Thermal agitation of magnetization
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U2 - 10.1109/TMAG.2007.892586
DO - 10.1109/TMAG.2007.892586
M3 - Article
AN - SCOPUS:34249090971
SN - 0018-9464
VL - 43
SP - 2091
EP - 2093
JO - IEEE Transactions on Magnetics
JF - IEEE Transactions on Magnetics
IS - 6
ER -