485 research outputs found
Offset fields in perpendicularly magnetized tunnel junctions
We study the offset fields affecting the free layer of perpendicularly
magnetized tunnel junctions. In extended films, the free layer offset field
results from interlayer exchange coupling with the reference layer through the
MgO tunnel oxide. The free layer offset field is thus accompanied with a shift
of the free layer and reference layer ferromagnetic resonance frequencies. The
shifts depend on the mutual orientation of the two magnetizations. The offset
field decreases with the resistance area product of the tunnel oxide.
Patterning the tunnel junction into an STT-MRAM disk-shaped cell changes
substantially the offset field, as the reduction of the lateral dimension comes
with the generation of stray fields by the reference and the hard layer. The
experimental offset field compares best with the spatial average of the sum of
these stray fields, thereby providing guidelines for the offset field
engineering.Comment: Special issue of J. Phys. D: Appl. Phys (2019) on STT-MRA
Annealing stability of magnetic tunnel junctions based on dual MgO free layers and [Co/Ni] based thin synthetic antiferromagnet fixed system
We study the annealing stability of bottom-pinned perpendicularly magnetized
magnetic tunnel junctions based on dual MgO free layers and thin fixed systems
comprising a hard [Co/Ni] multilayer antiferromagnetically coupled to thin a Co
reference layer and a FeCoB polarizing layer. Using conventional magnetometry
and advanced broadband ferromagnetic resonance, we identify the properties of
each sub-unit of the magnetic tunnel junction and demonstrate that this
material option can ensure a satisfactory resilience to the 400C
thermal annealing needed in solid-state magnetic memory applications. The dual
MgO free layer possesses an anneal-robust 0.4 T effective anisotropy and
suffers only a minor increase of its Gilbert damping from 0.007 to 0.010 for
the toughest annealing conditions. Within the fixed system, the ferro-coupler
and texture-breaking TaFeCoB layer keeps an interlayer exchange above 0.8
mJ/m, while the Ru antiferrocoupler layer within the synthetic
antiferromagnet maintains a coupling above -0.5 mJ/m. These two strong
couplings maintain the overall functionality of the tunnel junction upon the
toughest annealing despite the gradual degradation of the thin Co layer
anisotropy that may reduce the operation margin in spin torque memory
applications. Based on these findings, we propose further optimization routes
for the next generation magnetic tunnel junctions
Time-resolved spin-torque switching in MgO-based perpendicularly magnetized tunnel junctions
We study ns scale spin-torque-induced switching in perpendicularly magnetized
tunnel junctions (pMTJ). Although the switching voltages match with the
macrospin instability threshold, the electrical signatures of the reversal
indicate the presence of domain walls in junctions of various sizes. In the
antiparallel (AP) to parallel (P) switching, a nucleation phase is followed by
an irreversible flow of a wall through the sample at an average velocity of 40
m/s with back and forth oscillation movements indicating a Walker propagation
regime. A model with a single-wall locally responding to the spin-torque
reproduces the essential dynamical signatures of the reversal. The P to AP
transition has a complex dynamics with dynamical back-hopping whose probability
increases with voltage. We attribute this back-hopping to the instability of
the nominally fixed layers
SOT-MRAM 300mm integration for low power and ultrafast embedded memories
We demonstrate for the first time full-scale integration of top-pinned
perpendicular MTJ on 300 mm wafer using CMOS-compatible processes for
spin-orbit torque (SOT)-MRAM architectures. We show that 62 nm devices with a
W-based SOT underlayer have very large endurance (> 5x10^10), sub-ns switching
time of 210 ps, and operate with power as low as 300 pJ.Comment: presented at VLSI2018 session C8-
Accommodation of tin in tetragonal ZrO2
Atomic scale computer simulations using density functional theory were used to investigate the behaviour of tin in the tetragonal phase oxide layer on Zr-based alloys. The Sn×ZrSnZr× defect was shown to be dominant across most oxygen partial pressures, with Sn′′ZrSnZr″ charge compensated by V∙∙OVO•• occurring at partial pressures below 10−31 atm. Insertion of additional positive charge into the system was shown to significantly increase the critical partial pressure at which Sn′′ZrSnZr″ is stable. Recently developed low-Sn nuclear fuel cladding alloys have demonstrated an improved corrosion resistance and a delayed transition compared to Sn-containing alloys, such as Zircaloy-4. The interaction between the positive charge and the tin defect is discussed in the context of alloying additions, such as niobium and their influence on corrosion of cladding alloys
Gilbert damping of high anisotropy Co/Pt multilayers
Using broadband ferromagnetic resonance, we measure the damping parameter of
[Co(5 \r{A})/Pt(3 \r{A})] multilayers whose growth was optimized to
maximize the perpendicular anisotropy. Structural characterizations indicate
abrupt interfaces essentially free of intermixing despite the miscible
character of Co and Pt. Gilbert damping parameters as low as 0.021 can be
obtained despite a magneto-crystalline anisotropy as large as
. The inhomogeneous broadening accounts for part of the
ferromagnetic resonance linewidth, indicating some structural disorder leading
to a equivalent 20 mT of inhomogenity of the effective field. The unexpectedly
relatively low damping factor indicates that the presence of the Pt heavy metal
within the multilayer may not be detrimental to the damping provided that
intermixing is avoided at the Co/Pt interfaces
Steady-state modulation of voltage-gated K+ channels in rat arterial smooth muscle by cyclic AMP-dependent protein kinase and protein phosphatase 2B
Voltage-gated potassium channels (Kv) are important regulators of membrane potential in vascular smooth muscle cells, which is integral to controlling intracellular Ca2+ concentration and regulating vascular tone. Previous work indicates that Kv channels can be modulated by receptor-driven alterations of cyclic AMP-dependent protein kinase (PKA) activity. Here, we demonstrate that Kv channel activity is maintained by tonic activity of PKA. Whole-cell recording was used to assess the effect of manipulating PKA signalling on Kv and ATP-dependent K+ channels of rat mesenteric artery smooth muscle cells. Application of PKA inhibitors, KT5720 or H89, caused a significant inhibition of Kv currents. Tonic PKA-mediated activation of Kv appears maximal as application of isoprenaline (a β-adrenoceptor agonist) or dibutyryl-cAMP failed to enhance Kv currents. We also show that this modulation of Kv by PKA can be reversed by protein phosphatase 2B/calcineurin (PP2B). PKA-dependent inhibition of Kv by KT5720 can be abrogated by pre-treatment with the PP2B inhibitor cyclosporin A, or inclusion of a PP2B auto-inhibitory peptide in the pipette solution. Finally, we demonstrate that tonic PKA-mediated modulation of Kv requires intact caveolae. Pre-treatment of the cells with methyl-β-cyclodextrin to deplete cellular cholesterol, or adding caveolin-scaffolding domain peptide to the pipette solution to disrupt caveolae-dependent signalling each attenuated PKA-mediated modulation of the Kv current. These findings highlight a novel, caveolae-dependent, tonic modulatory role of PKA on Kv channels providing new insight into mechanisms and the potential for pharmacological manipulation of vascular tone
Deposition and patterning of magnetic atom trap lattices in FePt films with periods down to 200 nm
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