Magnetic recording media with ultra-high recording density
View Patent ↗An AFC magnetic recording medium having a three-layered ferromagnetic structure capable of reducing noises without deteriorating thermal stability is provided in order to achieve ultra-high recording density. In one embodiment, the AFC magnetic recording medium has a magnetic recording layer formed on a substrate via an underlayer, the magnetic recording medium consisting of a first ferromagnetic layer formed on the underlayer, a second ferromagnetic layer formed on the first ferromagnetic layer via a nonmagnetic layer inducing the antiferromagnetic interaction, and a third ferromagnetic layer formed on the second ferromagnetic layer, wherein the center of gravity G of the magnetic recording medium is defined using the distance t g from the upper surface of the third ferromagnetic layer as: t g =(M s t) eff /(2M S3 ); when the center of gravity G is at the third ferromagnetic layer, t g =((M s t) eff /2−M S3 t 3 )/M S2 +t 3 ; when the center of gravity G is at the second ferromagnetic layer, and when the total film thickness of the magnetic recording layer is t total , the value t g /t total is lower than about 0.33.
1. A magnetic recording medium comprising:
a substrate;
an underlayer formed on the substrate;
a first ferromagnetic layer formed on the underlayer;
a nonmagnetic layer formed on the first ferromagnetic layer;
a second ferromagnetic layer formed on the nonmagnetic layer; and
a third ferromagnetic layer formed on the second ferromagnetic layer,
the first ferromagnetic layer and the second ferromagnetic layer being antiferromagnetically coupled via the nonmagnetic layer, the second ferromagnetic layer and the third ferromagnetic layer being ferromagnetically coupled,
wherein, where the saturation magnetization of the first ferromagnetic layer is M S1 and the film thickness thereof is t 1 , the saturation magnetization of the second ferromagnetic is M S2 and the film thickness thereof is t 2 , the saturation magnetization of the third ferromagnetic layer is M S3 and the film thickness thereof is t 3 , and the film thickness of the nonmagnetic layer is t n , the effective product (M s t) eff of the saturation magnetization and the film thickness of the magnetic recording medium is defined as (M s t) eff =M S2 t 2 +M S3 t 3 −M S1 t 1 , and where the distance t g is defined as the distance from the upper surface of the third ferromagnetic layer to the center of gravity G, and
t g =(M s t) eff /(2M s3 ); when the center of gravity G is at the third ferromagnetic layer,
t g =((M s t) eff /2−M s3 t 3 )/M s2 +t 3 ; when the center of gravity G is at the second ferromagnetic layer,
and,
the value t g /t total obtained by normalizing the distance t g by t 1 +t 2 +t 3 +t n (=t total ) is smaller than about 0.33;
wherein the film thickness of the third ferromagnetic layer is thinner than the film thickness of the second ferromagnetic layer;
wherein the ratio of the saturation magnetization M s3 of the third ferromagnetic layer to the saturation magnetization M s2 of the second ferromagnetic layer is larger than about 1.
2. A magnetic recording medium according to claim 1 ,
wherein the center of gravity G is at the second ferromagnetic layer.
3. A magnetic recording medium according to claim 2 ,
wherein, the film thickness of the third ferromagnetic layer is thinner than the film thickness of the second ferromagnetic layer.
4. A magnetic recording medium according to claim 1 ,
wherein the center of gravity G is at the third ferromagnetic layer, the value t g /t total being about 0.26 or smaller.