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Read Back Signals in Magnetic Recording - Research Group Fidler

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<strong>Read</strong> Head Design<br />

Figure 5.2: A comparison (left) of a conventional sp<strong>in</strong> valve and a sp<strong>in</strong> valve us<strong>in</strong>g a<br />

synthetic ferromagnet to fix the p<strong>in</strong>ned layer [20]. The <strong>in</strong>terlayer exchange constant (right)<br />

for two Ni80Co20 layers as function of the Ru spacer layer thickness [32].<br />

The IEC effect has its orig<strong>in</strong> <strong>in</strong> quantum <strong>in</strong>terference of electron states [36]. The exchange<br />

coupl<strong>in</strong>g constant J IEC [J/m 2 ] depends on the nonmagnetic layer thickness t NM like<br />

⎛ tNM<br />

⎞<br />

s<strong>in</strong> ⎜2π +Φ<br />

Λ<br />

⎟<br />

J = J<br />

⎝ ⎠<br />

(5.4)<br />

IEC<br />

0 2<br />

tNM<br />

as shown <strong>in</strong> Figure 5.2. Λ , Φ , and J 0 are constants, depend<strong>in</strong>g on the composition of the<br />

layers. The advantage of sp<strong>in</strong>-valves with a synthetic antiferromagnetic p<strong>in</strong>ned layer is the<br />

very large exchange field of IEC up to 0.5 T. This is an <strong>in</strong>crease of a factor 10 compared to<br />

the direct exchange coupl<strong>in</strong>g with an antiferromagnet. So the stability aga<strong>in</strong>st external fields<br />

is much better due to the higher anisotropy. Moreover the demagnetiz<strong>in</strong>g fields of the two<br />

ferromagnetic layers Fp,1 and Fp,2 cancel each other partially, which leads to a reduced<br />

<strong>in</strong>fluence on the free layer.<br />

5.1.5 Sense Current<br />

The sense current flow<strong>in</strong>g through the GMR sensor generates a magnetic field. This field also<br />

<strong>in</strong>fluences the p<strong>in</strong>ned layer magnetization. For conventional simple sp<strong>in</strong> valves there is one<br />

current direction which is more favorable. The ma<strong>in</strong> part of the current flows through the Cu<br />

layer, due to its higher conductivity compared to the other layers. So the current field either<br />

adds up with the demagnetiz<strong>in</strong>g field of the p<strong>in</strong>ned layer or weakens the field act<strong>in</strong>g on the<br />

62

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