Effects of Radio-Frequency Sputtering Power of MgO Tunneling Barrier on Tunneling Magneto-Resistance Ratio for Cofeb/MgO-Based Perpendicular-Magnetic Tunnel Junctions
Thus, in our study, in order to obtain the best crystallinity in an MgO tunneling barrier at an ex-situ magnetic annealing temperature greater than 350°C, we investigated how the radio-frequency (RF) sputtering power of a 0.65-1.15 nm thick MgO tunneling barrier affects the TMR ratio and the resistance-area product (RA) for p-MTJ spin valves by using a current-in-plane tunneling (CIPT) technique, and how it affects the tunneling barrier bct crystallinity by using cross-sectional transmission electron microscopy (x-TEM). Figure 1 shows the dependencies of the TMR ratio on the tunnelling barrier RF power for Co2Fe6B2-MgO based p-MTJ spin valves with [Co/Pt]n-SyAF layers. For RF power of 400 to 500 W, the TMR ratio was almost zero (≈5%) when the tunneling barrier thickness (tMgO) was less than 0.7 nm. This indicates that the tunneling barrier’s crystalline structure would be amorphous. The TMR ratio rapidly increased and then increased approximately linearly as the tMgO was increased from 0.8 to 1.15 nm. It is particularly noteworthy that, lower tunneling barrier RF power led to higher TMR ratios; i.e., the highest TMR ratio sequence was obtained at 500, 400, and 300 W. This implies that lower RF power would lead to better tunneling bct crystallinity. In particular, At 300 W, the TMR ratio was 168% for tMgO = 1.15 nm. However, the TMR ratio for all tMgO at 250 W abruptly dropped to almost zero (≈1.2%). we investigated the dependency of the tunneling barrier bct crystallinity on the RF power by x-TEM. For the valve that was RF sputtered at 300 W, the tunneling barrier layer was well bct crystallized and its thickness was very uniformly distributed; in Figure 2(a), it is 1.05 nm. This indicates there is maximum Δ1 coherent tunneling of perpendicular spin-electrons between the free and pinned Co2Fe6B2 layers. However, for the valve that was RF sputtered at 250 W, the tunneling barrier layer had an almost completely amorphous structure with a locally crystallized poly grain. This indicates there is almost no Δ1 coherent tunneling of perpendicular spin-electrons between the free and pinned Co2Fe6B2 layers. A comparison of Figure 2(a) with Figure 2(b) indicates that the tunneling barrier bct crystallinity was abruptly degraded when the tunneling barrier RF power was decreased from 300 to 250 W. As a result, the TMR ratio of the p-MTJ spin valves abruptly decreased from 168 to 2%.
In our presentation, we will review in detail the mechanism by which the RF sputtering power performs a good bct MgO crystallinity. In addition, we will discuss correlation of MgO crystallinity between x-TEM images and optical properties via spectroscopic ellipsometry to understand how the RF power affects the crystallinity of the MgO tunneling barrier.
*This work was supported by Basic Science Research Program through the National Research Foundation of Korea (NRF) grant funded by the Korea government (No. 2014R1A2A1A01006474 & No. 1004608) and Brain Korea 21 PLUS Program in 2014.