[ Previous ] [ Home ] [ ]

Numerical Analysis and Innovative Simulation
Techniques for Designing Advanced MRAM

\(\newcommand{\footnotename}{footnote}\) \(\def \LWRfootnote {1}\) \(\newcommand {\footnote }[2][\LWRfootnote ]{{}^{\mathrm {#1}}}\) \(\newcommand {\footnotemark }[1][\LWRfootnote ]{{}^{\mathrm {#1}}}\) \(\let \LWRorighspace \hspace \) \(\renewcommand {\hspace }{\ifstar \LWRorighspace \LWRorighspace }\) \(\newcommand {\TextOrMath }[2]{#2}\) \(\newcommand {\mathnormal }[1]{{#1}}\) \(\newcommand \ensuremath [1]{#1}\) \(\newcommand {\LWRframebox }[2][]{\fbox {#2}} \newcommand {\framebox }[1][]{\LWRframebox } \) \(\newcommand {\setlength }[2]{}\) \(\newcommand {\addtolength }[2]{}\) \(\newcommand {\setcounter }[2]{}\) \(\newcommand {\addtocounter }[2]{}\) \(\newcommand {\arabic }[1]{}\) \(\newcommand {\number }[1]{}\) \(\newcommand {\noalign }[1]{\text {#1}\notag \\}\) \(\newcommand {\cline }[1]{}\) \(\newcommand {\directlua }[1]{\text {(directlua)}}\) \(\newcommand {\luatexdirectlua }[1]{\text {(directlua)}}\) \(\newcommand {\protect }{}\) \(\def \LWRabsorbnumber #1 {}\) \(\def \LWRabsorbquotenumber "#1 {}\) \(\newcommand {\LWRabsorboption }[1][]{}\) \(\newcommand {\LWRabsorbtwooptions }[1][]{\LWRabsorboption }\) \(\def \mathchar {\ifnextchar "\LWRabsorbquotenumber \LWRabsorbnumber }\) \(\def \mathcode #1={\mathchar }\) \(\let \delcode \mathcode \) \(\let \delimiter \mathchar \) \(\def \oe {\unicode {x0153}}\) \(\def \OE {\unicode {x0152}}\) \(\def \ae {\unicode {x00E6}}\) \(\def \AE {\unicode {x00C6}}\) \(\def \aa {\unicode {x00E5}}\) \(\def \AA {\unicode {x00C5}}\) \(\def \o {\unicode {x00F8}}\) \(\def \O {\unicode {x00D8}}\) \(\def \l {\unicode {x0142}}\) \(\def \L {\unicode {x0141}}\) \(\def \ss {\unicode {x00DF}}\) \(\def \SS {\unicode {x1E9E}}\) \(\def \dag {\unicode {x2020}}\) \(\def \ddag {\unicode {x2021}}\) \(\def \P {\unicode {x00B6}}\) \(\def \copyright {\unicode {x00A9}}\) \(\def \pounds {\unicode {x00A3}}\) \(\let \LWRref \ref \) \(\renewcommand {\ref }{\ifstar \LWRref \LWRref }\) \( \newcommand {\multicolumn }[3]{#3}\) \(\require {textcomp}\) \(\newcommand {\mathlarger }[1]{#1}\) \(\newcommand {\mathsmaller }[1]{#1}\) \(\newcommand {\intertext }[1]{\text {#1}\notag \\}\) \(\let \Hat \hat \) \(\let \Check \check \) \(\let \Tilde \tilde \) \(\let \Acute \acute \) \(\let \Grave \grave \) \(\let \Dot \dot \) \(\let \Ddot \ddot \) \(\let \Breve \breve \) \(\let \Bar \bar \) \(\let \Vec \vec \) \(\newcommand {\toprule }[1][]{\hline }\) \(\let \midrule \toprule \) \(\let \bottomrule \toprule \) \(\def \LWRbooktabscmidruleparen (#1)#2{}\) \(\newcommand {\LWRbooktabscmidrulenoparen }[1]{}\) \(\newcommand {\cmidrule }[1][]{\ifnextchar (\LWRbooktabscmidruleparen \LWRbooktabscmidrulenoparen }\) \(\newcommand {\morecmidrules }{}\) \(\newcommand {\specialrule }[3]{\hline }\) \(\newcommand {\addlinespace }[1][]{}\) \(\newcommand {\bm }[1]{\boldsymbol {#1}}\) \(\newcommand {\LWRsubmultirow }[2][]{#2}\) \(\newcommand {\LWRmultirow }[2][]{\LWRsubmultirow }\) \(\newcommand {\multirow }[2][]{\LWRmultirow }\) \(\newcommand {\mrowcell }{}\) \(\newcommand {\mcolrowcell }{}\) \(\newcommand {\STneed }[1]{}\) \(\newcommand {\tothe }[1]{^{#1}}\) \(\newcommand {\raiseto }[2]{{#2}^{#1}}\) \(\newcommand {\LWRsiunitxEND }{}\) \(\def \LWRsiunitxang #1;#2;#3;#4\LWRsiunitxEND {\ifblank {#1}{}{\num {#1}\degree }\ifblank {#2}{}{\num {#2}^{\unicode {x2032}}}\ifblank {#3}{}{\num {#3}^{\unicode {x2033}}}}\) \(\newcommand {\ang }[2][]{\LWRsiunitxang #2;;;\LWRsiunitxEND }\) \(\def \LWRsiunitxdistribunit {}\) \(\newcommand {\LWRsiunitxENDTWO }{}\) \(\def \LWRsiunitxprintdecimalsubtwo #1,#2,#3\LWRsiunitxENDTWO {\ifblank {#1}{0}{\mathrm {#1}}\ifblank {#2}{}{{\LWRsiunitxdecimal }\mathrm {#2}}}\) \(\def \LWRsiunitxprintdecimalsub #1.#2.#3\LWRsiunitxEND {\LWRsiunitxprintdecimalsubtwo #1,,\LWRsiunitxENDTWO \ifblank {#2}{}{{\LWRsiunitxdecimal }\LWRsiunitxprintdecimalsubtwo #2,,\LWRsiunitxENDTWO }}\) \(\newcommand {\LWRsiunitxprintdecimal }[1]{\LWRsiunitxprintdecimalsub #1...\LWRsiunitxEND }\) \(\def \LWRsiunitxnumplus #1+#2+#3\LWRsiunitxEND {\ifblank {#2}{\LWRsiunitxprintdecimal {#1}}{\ifblank {#1}{\LWRsiunitxprintdecimal {#2}}{\LWRsiunitxprintdecimal {#1}\unicode {x02B}\LWRsiunitxprintdecimal {#2}}}\LWRsiunitxdistribunit }\) \(\def \LWRsiunitxnumminus #1-#2-#3\LWRsiunitxEND {\ifblank {#2}{\LWRsiunitxnumplus #1+++\LWRsiunitxEND }{\ifblank {#1}{}{\LWRsiunitxprintdecimal {#1}}\unicode {x02212}\LWRsiunitxprintdecimal {#2}\LWRsiunitxdistribunit }}\) \(\def \LWRsiunitxnumpmmacro #1\pm #2\pm #3\LWRsiunitxEND {\ifblank {#2}{\LWRsiunitxnumminus #1---\LWRsiunitxEND }{\LWRsiunitxprintdecimal {#1}\unicode {x0B1}\LWRsiunitxprintdecimal {#2}\LWRsiunitxdistribunit }}\) \(\def \LWRsiunitxnumpm #1+-#2+-#3\LWRsiunitxEND {\ifblank {#2}{\LWRsiunitxnumpmmacro #1\pm \pm \pm \LWRsiunitxEND }{\LWRsiunitxprintdecimal {#1}\unicode {x0B1}\LWRsiunitxprintdecimal {#2}\LWRsiunitxdistribunit }}\) \(\newcommand {\LWRsiunitxnumscientific }[2]{\ifblank {#1}{}{\ifstrequal {#1}{-}{-}{\LWRsiunitxprintdecimal {#1}\times }}10^{\LWRsiunitxprintdecimal {#2}}\LWRsiunitxdistribunit }\) \(\def \LWRsiunitxnumD #1D#2D#3\LWRsiunitxEND {\ifblank {#2}{\LWRsiunitxnumpm #1+-+-\LWRsiunitxEND }{\mathrm {\LWRsiunitxnumscientific {#1}{#2}}}}\) \(\def \LWRsiunitxnumd #1d#2d#3\LWRsiunitxEND {\ifblank {#2}{\LWRsiunitxnumD #1DDD\LWRsiunitxEND }{\mathrm {\LWRsiunitxnumscientific {#1}{#2}}}}\) \(\def \LWRsiunitxnumE #1E#2E#3\LWRsiunitxEND {\ifblank {#2}{\LWRsiunitxnumd #1ddd\LWRsiunitxEND }{\mathrm {\LWRsiunitxnumscientific {#1}{#2}}}}\) \(\def \LWRsiunitxnume #1e#2e#3\LWRsiunitxEND {\ifblank {#2}{\LWRsiunitxnumE #1EEE\LWRsiunitxEND }{\mathrm {\LWRsiunitxnumscientific {#1}{#2}}}}\) \(\def \LWRsiunitxnumx #1x#2x#3x#4\LWRsiunitxEND {\ifblank {#2}{\LWRsiunitxnume #1eee\LWRsiunitxEND }{\ifblank {#3}{\LWRsiunitxnume #1eee\LWRsiunitxEND \times \LWRsiunitxnume #2eee\LWRsiunitxEND }{\LWRsiunitxnume #1eee\LWRsiunitxEND \times \LWRsiunitxnume #2eee\LWRsiunitxEND \times \LWRsiunitxnume #3eee\LWRsiunitxEND }}}\) \(\newcommand {\num }[2][]{\LWRsiunitxnumx #2xxxxx\LWRsiunitxEND }\) \(\newcommand {\si }[2][]{\mathrm {\gsubstitute {#2}{~}{\,}}}\) \(\def \LWRsiunitxSIopt #1[#2]#3{\def \LWRsiunitxdistribunit {\,\si {#3}}{#2}\num {#1}\def \LWRsiunitxdistribunit {}}\) \(\newcommand {\LWRsiunitxSI }[2]{\def \LWRsiunitxdistribunit {\,\si {#2}}\num {#1}\def \LWRsiunitxdistribunit {}}\) \(\newcommand {\SI }[2][]{\ifnextchar [{\LWRsiunitxSIopt {#2}}{\LWRsiunitxSI {#2}}}\) \(\newcommand {\numlist }[2][]{\text {#2}}\) \(\newcommand {\numrange }[3][]{\num {#2}\ \LWRsiunitxrangephrase \ \num {#3}}\) \(\newcommand {\SIlist }[3][]{\text {#2}\,\si {#3}}\) \(\newcommand {\SIrange }[4][]{\num {#2}\,#4\ \LWRsiunitxrangephrase \ \num {#3}\,#4}\) \(\newcommand {\tablenum }[2][]{\mathrm {#2}}\) \(\newcommand {\ampere }{\mathrm {A}}\) \(\newcommand {\candela }{\mathrm {cd}}\) \(\newcommand {\kelvin }{\mathrm {K}}\) \(\newcommand {\kilogram }{\mathrm {kg}}\) \(\newcommand {\metre }{\mathrm {m}}\) \(\newcommand {\mole }{\mathrm {mol}}\) \(\newcommand {\second }{\mathrm {s}}\) \(\newcommand {\becquerel }{\mathrm {Bq}}\) \(\newcommand {\degreeCelsius }{\unicode {x2103}}\) \(\newcommand {\coulomb }{\mathrm {C}}\) \(\newcommand {\farad }{\mathrm {F}}\) \(\newcommand {\gray }{\mathrm {Gy}}\) \(\newcommand {\hertz }{\mathrm {Hz}}\) \(\newcommand {\henry }{\mathrm {H}}\) \(\newcommand {\joule }{\mathrm {J}}\) \(\newcommand {\katal }{\mathrm {kat}}\) \(\newcommand {\lumen }{\mathrm {lm}}\) \(\newcommand {\lux }{\mathrm {lx}}\) \(\newcommand {\newton }{\mathrm {N}}\) \(\newcommand {\ohm }{\mathrm {\Omega }}\) \(\newcommand {\pascal }{\mathrm {Pa}}\) \(\newcommand {\radian }{\mathrm {rad}}\) \(\newcommand {\siemens }{\mathrm {S}}\) \(\newcommand {\sievert }{\mathrm {Sv}}\) \(\newcommand {\steradian }{\mathrm {sr}}\) \(\newcommand {\tesla }{\mathrm {T}}\) \(\newcommand {\volt }{\mathrm {V}}\) \(\newcommand {\watt }{\mathrm {W}}\) \(\newcommand {\weber }{\mathrm {Wb}}\) \(\newcommand {\day }{\mathrm {d}}\) \(\newcommand {\degree }{\mathrm {^\circ }}\) \(\newcommand {\hectare }{\mathrm {ha}}\) \(\newcommand {\hour }{\mathrm {h}}\) \(\newcommand {\litre }{\mathrm {l}}\) \(\newcommand {\liter }{\mathrm {L}}\) \(\newcommand {\arcminute }{^\prime }\) \(\newcommand {\minute }{\mathrm {min}}\) \(\newcommand {\arcsecond }{^{\prime \prime }}\) \(\newcommand {\tonne }{\mathrm {t}}\) \(\newcommand {\astronomicalunit }{au}\) \(\newcommand {\atomicmassunit }{u}\) \(\newcommand {\bohr }{\mathit {a}_0}\) \(\newcommand {\clight }{\mathit {c}_0}\) \(\newcommand {\dalton }{\mathrm {D}_\mathrm {a}}\) \(\newcommand {\electronmass }{\mathit {m}_{\mathrm {e}}}\) \(\newcommand {\electronvolt }{\mathrm {eV}}\) \(\newcommand {\elementarycharge }{\mathit {e}}\) \(\newcommand {\hartree }{\mathit {E}_{\mathrm {h}}}\) \(\newcommand {\planckbar }{\mathit {\unicode {x210F}}}\) \(\newcommand {\angstrom }{\mathrm {\unicode {x212B}}}\) \(\let \LWRorigbar \bar \) \(\newcommand {\bar }{\mathrm {bar}}\) \(\newcommand {\barn }{\mathrm {b}}\) \(\newcommand {\bel }{\mathrm {B}}\) \(\newcommand {\decibel }{\mathrm {dB}}\) \(\newcommand {\knot }{\mathrm {kn}}\) \(\newcommand {\mmHg }{\mathrm {mmHg}}\) \(\newcommand {\nauticalmile }{\mathrm {M}}\) \(\newcommand {\neper }{\mathrm {Np}}\) \(\newcommand {\yocto }{\mathrm {y}}\) \(\newcommand {\zepto }{\mathrm {z}}\) \(\newcommand {\atto }{\mathrm {a}}\) \(\newcommand {\femto }{\mathrm {f}}\) \(\newcommand {\pico }{\mathrm {p}}\) \(\newcommand {\nano }{\mathrm {n}}\) \(\newcommand {\micro }{\mathrm {\unicode {x00B5}}}\) \(\newcommand {\milli }{\mathrm {m}}\) \(\newcommand {\centi }{\mathrm {c}}\) \(\newcommand {\deci }{\mathrm {d}}\) \(\newcommand {\deca }{\mathrm {da}}\) \(\newcommand {\hecto }{\mathrm {h}}\) \(\newcommand {\kilo }{\mathrm {k}}\) \(\newcommand {\mega }{\mathrm {M}}\) \(\newcommand {\giga }{\mathrm {G}}\) \(\newcommand {\tera }{\mathrm {T}}\) \(\newcommand {\peta }{\mathrm {P}}\) \(\newcommand {\exa }{\mathrm {E}}\) \(\newcommand {\zetta }{\mathrm {Z}}\) \(\newcommand {\yotta }{\mathrm {Y}}\) \(\newcommand {\percent }{\mathrm {\%}}\) \(\newcommand {\meter }{\mathrm {m}}\) \(\newcommand {\metre }{\mathrm {m}}\) \(\newcommand {\gram }{\mathrm {g}}\) \(\newcommand {\kg }{\kilo \gram }\) \(\newcommand {\of }[1]{_{\mathrm {#1}}}\) \(\newcommand {\squared }{^2}\) \(\newcommand {\square }[1]{\mathrm {#1}^2}\) \(\newcommand {\cubed }{^3}\) \(\newcommand {\cubic }[1]{\mathrm {#1}^3}\) \(\newcommand {\per }{\,\mathrm {/}}\) \(\newcommand {\celsius }{\unicode {x2103}}\) \(\newcommand {\fg }{\femto \gram }\) \(\newcommand {\pg }{\pico \gram }\) \(\newcommand {\ng }{\nano \gram }\) \(\newcommand {\ug }{\micro \gram }\) \(\newcommand {\mg }{\milli \gram }\) \(\newcommand {\g }{\gram }\) \(\newcommand {\kg }{\kilo \gram }\) \(\newcommand {\amu }{\mathrm {u}}\) \(\newcommand {\pm }{\pico \metre }\) \(\newcommand {\nm }{\nano \metre }\) \(\newcommand {\um }{\micro \metre }\) \(\newcommand {\mm }{\milli \metre }\) \(\newcommand {\cm }{\centi \metre }\) \(\newcommand {\dm }{\deci \metre }\) \(\newcommand {\m }{\metre }\) \(\newcommand {\km }{\kilo \metre }\) \(\newcommand {\as }{\atto \second }\) \(\newcommand {\fs }{\femto \second }\) \(\newcommand {\ps }{\pico \second }\) \(\newcommand {\ns }{\nano \second }\) \(\newcommand {\us }{\micro \second }\) \(\newcommand {\ms }{\milli \second }\) \(\newcommand {\s }{\second }\) \(\newcommand {\fmol }{\femto \mol }\) \(\newcommand {\pmol }{\pico \mol }\) \(\newcommand {\nmol }{\nano \mol }\) \(\newcommand {\umol }{\micro \mol }\) \(\newcommand {\mmol }{\milli \mol }\) \(\newcommand {\mol }{\mol }\) \(\newcommand {\kmol }{\kilo \mol }\) \(\newcommand {\pA }{\pico \ampere }\) \(\newcommand {\nA }{\nano \ampere }\) \(\newcommand {\uA }{\micro \ampere }\) \(\newcommand {\mA }{\milli \ampere }\) \(\newcommand {\A }{\ampere }\) \(\newcommand {\kA }{\kilo \ampere }\) \(\newcommand {\ul }{\micro \litre }\) \(\newcommand {\ml }{\milli \litre }\) \(\newcommand {\l }{\litre }\) \(\newcommand {\hl }{\hecto \litre }\) \(\newcommand {\uL }{\micro \liter }\) \(\newcommand {\mL }{\milli \liter }\) \(\newcommand {\L }{\liter }\) \(\newcommand {\hL }{\hecto \liter }\) \(\newcommand {\mHz }{\milli \hertz }\) \(\newcommand {\Hz }{\hertz }\) \(\newcommand {\kHz }{\kilo \hertz }\) \(\newcommand {\MHz }{\mega \hertz }\) \(\newcommand {\GHz }{\giga \hertz }\) \(\newcommand {\THz }{\tera \hertz }\) \(\newcommand {\mN }{\milli \newton }\) \(\newcommand {\N }{\newton }\) \(\newcommand {\kN }{\kilo \newton }\) \(\newcommand {\MN }{\mega \newton }\) \(\newcommand {\Pa }{\pascal }\) \(\newcommand {\kPa }{\kilo \pascal }\) \(\newcommand {\MPa }{\mega \pascal }\) \(\newcommand {\GPa }{\giga \pascal }\) \(\newcommand {\mohm }{\milli \ohm }\) \(\newcommand {\kohm }{\kilo \ohm }\) \(\newcommand {\Mohm }{\mega \ohm }\) \(\newcommand {\pV }{\pico \volt }\) \(\newcommand {\nV }{\nano \volt }\) \(\newcommand {\uV }{\micro \volt }\) \(\newcommand {\mV }{\milli \volt }\) \(\newcommand {\V }{\volt }\) \(\newcommand {\kV }{\kilo \volt }\) \(\newcommand {\W }{\watt }\) \(\newcommand {\uW }{\micro \watt }\) \(\newcommand {\mW }{\milli \watt }\) \(\newcommand {\kW }{\kilo \watt }\) \(\newcommand {\MW }{\mega \watt }\) \(\newcommand {\GW }{\giga \watt }\) \(\newcommand {\J }{\joule }\) \(\newcommand {\uJ }{\micro \joule }\) \(\newcommand {\mJ }{\milli \joule }\) \(\newcommand {\kJ }{\kilo \joule }\) \(\newcommand {\eV }{\electronvolt }\) \(\newcommand {\meV }{\milli \electronvolt }\) \(\newcommand {\keV }{\kilo \electronvolt }\) \(\newcommand {\MeV }{\mega \electronvolt }\) \(\newcommand {\GeV }{\giga \electronvolt }\) \(\newcommand {\TeV }{\tera \electronvolt }\) \(\newcommand {\kWh }{\kilo \watt \hour }\) \(\newcommand {\F }{\farad }\) \(\newcommand {\fF }{\femto \farad }\) \(\newcommand {\pF }{\pico \farad }\) \(\newcommand {\K }{\mathrm {K}}\) \(\newcommand {\dB }{\mathrm {dB}}\) \(\newcommand {\kibi }{\mathrm {Ki}}\) \(\newcommand {\mebi }{\mathrm {Mi}}\) \(\newcommand {\gibi }{\mathrm {Gi}}\) \(\newcommand {\tebi }{\mathrm {Ti}}\) \(\newcommand {\pebi }{\mathrm {Pi}}\) \(\newcommand {\exbi }{\mathrm {Ei}}\) \(\newcommand {\zebi }{\mathrm {Zi}}\) \(\newcommand {\yobi }{\mathrm {Yi}}\) \(\let \unit \si \) \(\let \qty \SI \) \(\let \qtylist \SIlist \) \(\let \qtyrange \SIrange \) \(\let \numproduct \num \) \(\let \qtyproduct \SI \) \(\let \complexnum \num \) \(\newcommand {\complexqty }[3][]{(\complexnum {#2})\si {#3}}\) \(\require {mathtools}\) \(\newcommand {\vcentcolon }{\mathrel {\unicode {x2236}}}\) \(\newcommand {\approxcolon }{\approx \vcentcolon }\) \(\newcommand {\Approxcolon }{\approx \dblcolon }\) \(\newcommand {\simcolon }{\sim \vcentcolon }\) \(\newcommand {\Simcolon }{\sim \dblcolon }\) \(\newcommand {\dashcolon }{\mathrel {-}\vcentcolon }\) \(\newcommand {\Dashcolon }{\mathrel {-}\dblcolon }\) \(\newcommand {\colondash }{\vcentcolon \mathrel {-}}\) \(\newcommand {\Colondash }{\dblcolon \mathrel {-}}\) \(\newenvironment {crampedsubarray}[1]{}{}\) \(\newcommand {\smashoperator }[2][]{#2\limits }\) \(\newcommand {\SwapAboveDisplaySkip }{}\) \(\newcommand {\LaTeXunderbrace }[1]{\underbrace {#1}}\) \(\newcommand {\LaTeXoverbrace }[1]{\overbrace {#1}}\) \(\Newextarrow \xLongleftarrow {10,10}{0x21D0}\) \(\Newextarrow \xLongrightarrow {10,10}{0x21D2}\) \(\let \xlongleftarrow \xleftarrow \) \(\let \xlongrightarrow \xrightarrow \) \(\newcommand {\LWRmultlined }[1][]{\begin {multline*}}\) \(\newenvironment {multlined}[1][]{\LWRmultlined }{\end {multline*}}\) \(\let \LWRorigshoveleft \shoveleft \) \(\renewcommand {\shoveleft }[1][]{\LWRorigshoveleft }\) \(\let \LWRorigshoveright \shoveright \) \(\renewcommand {\shoveright }[1][]{\LWRorigshoveright }\) \(\newcommand {\shortintertext }[1]{\text {#1}\notag \\}\) \(\def \LWRsiunitxrangephrase {\TextOrMath { }{\ }\protect \mbox {to}\TextOrMath { }{\ }}\) \(\def \LWRsiunitxdecimal {.}\)

8.3 Conclusion

This thesis has demonstrated that the complex physics of ultra-scaled STT-MRAM devices, spanning spin transport across multiple interfaces, interlayer exchange coupling in composite stacks, and deterministic switching phenomena in sub-20nm geometries, can be captured within a single, unified computational framework. The three-dimensional drift-diffusion approach developed here provides spatial resolution of torque densities, spin-accumulation profiles, and magnetization textures that are fundamentally inaccessible to macro-spin or one-dimensional models. This resolution reveals phenomena, including sequential switching, deterministic back-hopping, and the inherently non-additive coupling of spin-transfer torques in multi-segment stacks, that collectively reshape the design paradigm for next-generation devices.

From a practical standpoint, the results establish quantitative design guidelines across seven device configurations spanning four architecture families (ultra-scaled composite FL, SAF-enhanced, hybrid FL, and ds-MTJ). The identification of specific IEC windows for SAF stability, the demonstration of controlled MLC operation through intermediate magnetization states, and the optimization of double spin-torque and hybrid structures for sub-nanosecond switching provide an actionable roadmap for the development of higher-density, faster, and more reliable MRAM.

Looking ahead, the next leap in device performance will likely stem not only from new materials and advances in fabrication, but also from the mathematical capability to simulate them. The transition to higher-order finite elements, parallel-in-time integration, and fully coupled space-time solvers promises to reveal hidden dynamics at the quantum-classical boundary, enabling predictive simulation of phenomena that remain beyond the reach of current methods. This thesis provides both the physical foundation and the computational starting point for that pursuit.

Bibliography

  • [1]  V. Sze, Y.-H. Chen, T.-J. Yang, and J. S. Emer, “Efficient Processing of Deep Neural Networks: A Tutorial and Survey,” Proceedings of the IEEE, vol. 105, no. 12, pp. 2295–2329, 2017. doi: 10.1109/JPROC.2017.2761740.

  • [2]  J. E. Lilienfeld, “Method and Apparatus for Controlling Electric Currents,” US Patent US1,745,175A, January 28, 1930.

  • [3]  J. Bardeen and W. H. Brattain, “The Transistor, a Semiconductor Triode,” Physical Review, vol. 74, pp. 230–231, 1948. doi: 10.1103/PhysRev.74.230.

  • [4]  F. M. Wanlass, “Low Stand-By Power Complementary Field Effect Circuitry,” US Patent US3 356 858A, December 5, 1967.

  • [5]  J. W. Forrester, “Digital Information Storage in Three Dimensions Using Magnetic Cores,” Journal of Applied Physics, vol. 22, no. 1, pp. 44–48, 1951. doi: 10.1063/1.1699817.

  • [6]  B. Dieny, I. L. Prejbeanu, K. Garello, P. Gambardella, P. Freitas et al., “Opportunities and Challenges for Spintronics in the Microelectronics Industry,” Nature Electronics, vol. 3, no. 8, pp. 446–459, 2020. doi: 10.1038/s41928-020-0461-5.

  • [7]  J. Kim, A. Paul, P. A. Crowell, S. J. Koester, S. S. Sapatnekar et al., “Spin-Based Computing: Device Concepts, Current Status, and a Case Study on a High-Performance Microprocessor,” Proceedings of the IEEE, vol. 103, no. 1, pp. 106–130, 2015. doi: 10.1109/JPROC.2014.2361767.

  • [8]  X. Wang, “RRAM-Based In-Memory Computing Architecture Designs,” Ph.D. dissertation, University of Michigan, Ann Arbor, MI, 2023. [Online]. Available: https://deepblue.lib.umich.edu/handle/2027.42/178016

  • [9]  J. Liao, S. Dai, R.-C. Peng, J. Yang, B. Zeng et al., “HfO\(_2\)-Based Ferroelectric Thin Film and Memory Device Applications in the Post-Moore Era: A Review,” Fundamental Research, vol. 3, no. 3, pp. 332–345, 2023. doi: 10.1016/j.fmre.2023.02.010.

  • [10]  M. Le Gallo, R. Khaddam-Aljameh, M. Stanisavljevic, A. Vasilopoulos, B. Kersting et al., “A 64-Core Mixed-Signal In-Memory Compute Chip Based on Phase-Change Memory for Deep Neural Network Inference,” Nature Electronics, vol. 6, no. 9, pp. 680–693, 2023. doi: 10.1038/s41928-023-01010-1.

  • [11]  A. D. Kent and D. C. Worledge, “A New Spin on Magnetic Memories,” Nature Nanotechnology, vol. 10, pp. 187–191, 2015. doi: 10.1038/nnano.2015.24.

  • [12]  D. Apalkov, B. Dieny, and J. M. Slaughter, “Magnetoresistive Random Access Memory,” Proceedings of the IEEE, vol. 104, no. 10, pp. 1796–1830, 2016. doi: 10.1109/JPROC.2016.2590142.

  • [13]  T. Hanyu, T. Endoh, D. Suzuki, H. Koike, Y. Ma et al., “Standby-Power-Free Integrated Circuits Using MTJ-Based VLSI Computing,” Proceedings of the IEEE, vol. 104, no. 10, pp. 1844–1863, 2016. doi: 10.1109/JPROC.2016.2574939.

  • [14]  M. Jullière, “Tunneling Between Ferromagnetic Films,” Physics Letters A, vol. 54, no. 3, pp. 225–226, 1975. doi: 10.1016/0375-9601(75)90174-7.

  • [15]  C. Chappert, A. Fert, and F. N. Van Dau, “The Emergence of Spin Electronics in Data Storage,” Nature Materials, vol. 6, no. 11, pp. 813–823, 2007. doi: 10.1038/nmat2024.

  • [16]  S. Maekawa and U. Gafvert, “Electron Tunneling Between Ferromagnetic Films,” IEEE Transactions on Magnetics, vol. 18, no. 2, pp. 707–708, 1982. doi: 10.1109/TMAG.1982.1061834.

  • [17]  J. S. Moodera and G. Mathon, “Spin Polarized Tunneling in Ferromagnetic Junctions,” Journal of Magnetism and Magnetic Materials, vol. 200, no. 1, pp. 248–273, 1999. doi: 10.1016/S0304-8853(99)00515-6.

  • [18]  L. Berger, “Emission of Spin Waves by a Magnetic Multilayer Traversed by a Current,” Physical Review B, vol. 54, pp. 9353–9358, 1996. doi: 10.1103/PhysRevB.54.9353.

  • [19]  J. Slonczewski, “Current-Driven Excitation of Magnetic Multilayers,” Journal of Magnetism and Magnetic Materials, vol. 159, no. 1, pp. L1–L7, 1996. doi: 10.1016/0304-8853(96)00062-5.

  • [20]  D. C. Ralph and M. D. Stiles, “Spin Transfer Torques,” Journal of Magnetism and Magnetic Materials, vol. 320, pp. 1190–1216, 2008. doi: 10.1016/j.jmmm.2007.12.019.

  • [21]  K. Ando, S. Fujita, J. Ito, S. Yuasa, Y. Suzuki et al., “Spin-Transfer Torque Magnetoresistive Random-Access Memory Technologies for Normally Off Computing,” Journal of Applied Physics, vol. 115, no. 17, p. 172607, 2014. doi: 10.1063/1.4869828.

  • [22]  C. Safranski, G. Hu, J. Z. Sun, P. Hashemi, S. L. Brown et al., “Reliable Sub-Nanosecond MRAM with Double Spin-Torque Magnetic Tunnel Junctions,” in 2022 IEEE Symposium on VLSI Technology and Circuits (VLSI Technology and Circuits), 2022, pp. 288–289. doi: 10.1109/VLSITechnologyandCir46769.2022.9830306.

  • [23]  J. Grollier, D. Querlioz, K. Y. Camsari, K. Everschor-Sitte, S. Fukami et al., “Neuromorphic Spintronics,” Nature Electronics, vol. 3, no. 7, pp. 360–370, 2020. doi: 10.1038/s41928-019-0360-9.

  • [24]  D. Marković, A. Mizrahi, D. Querlioz, and J. Grollier, “Physics for Neuromorphic Computing,” Nature Reviews Physics, vol. 2, no. 9, pp. 499–510, 2020. doi: 10.1038/s42254-020-0208-2.

  • [25]  S. S. P. Parkin, C. Kaiser, A. Panchula, P. M. Rice, B. Hughes et al., “Giant Tunnelling Magnetoresistance at Room Temperature with MgO (100) Tunnel Barriers,” Nature Materials, vol. 3, no. 12, pp. 862–867, 2004. doi: 10.1038/nmat1256.

  • [26]  S. Yuasa, T. Nagahama, A. Fukushima, Y. Suzuki, and K. Ando, “Giant Room-Temperature Magnetoresistance in Single-Crystal Fe/MgO/Fe Magnetic Tunnel Junctions,” Nature Materials, vol. 3, no. 12, pp. 868–871, 2004. doi: 10.1038/nmat1257.

  • [27]  A. Brataas, A. D. Kent, and H. Ohno, “Current-Induced Torques in Magnetic Materials,” Nature Materials, vol. 11, no. 5, pp. 372–381, 2012. doi: 10.1038/nmat3311.

  • [28]  S. Ikeda, K. Miura, H. Yamamoto, K. Mizunuma, H. D. Gan et al., “A Perpendicular-Anisotropy CoFeB–MgO Magnetic Tunnel Junction,” Nature Materials, vol. 9, no. 9, pp. 721–724, 2010. doi: 10.1038/nmat2804.

  • [29]  M. Beg, M. Lang, and H. Fangohr, “Ubermag: Toward More Effective Micromagnetic Workflows,” IEEE Transactions on Magnetics, vol. 58, no. 2, pp. 1–5, 2022. doi: 10.1109/TMAG.2021.3078896.

  • [30]  J. J. Joos, P. Bassirian, P. Gypens, J. Mulkers, K. Litzius et al., “Tutorial: Simulating Modern Magnetic Material Systems in Mumax3,” Journal of Applied Physics, vol. 134, no. 17, p. 171101, 2023. doi: 10.1063/5.0160988.

  • [31]  J. Z. Sun, “Spin-Current Interaction with a Monodomain Magnetic Body: A Model Study,” Physical Review B, vol. 62, no. 1, pp. 570–578, 2000. doi: 10.1103/PhysRevB.62.570.

  • [32]  C. Petitjean, D. Luc, and X. Waintal, “Unified Drift-Diffusion Theory for Transverse Spin Currents in Spin Valves, Domain Walls, and Other Textured Magnets,” Physical Review Letters, vol. 109, p. 117204, 2012. doi: 10.1103/PhysRevLett.109.117204.

  • [33]  M. Gajek, J. J. Nowak, J. Z. Sun, P. L. Trouilloud, E. J. O’Sullivan et al., “Spin Torque Switching of 20 nm Magnetic Tunnel Junctions with Perpendicular Anisotropy,” Applied Physics Letters, vol. 100, no. 13, p. 132408, 2012. doi: 10.1063/1.3694270.

  • [34]  S. Bandiera, R. C. Sousa, Y. Dahmane, C. Ducruet, C. Portemont et al., “Comparison of Synthetic Antiferromagnets and Hard Ferromagnets as Reference Layer in Magnetic Tunnel Junctions With Perpendicular Magnetic Anisotropy,” IEEE Magnetics Letters, vol. 1, pp. 3 000 204–3 000 204, 2010. doi: 10.1109/LMAG.2010.2052238.

  • [35]  S. Zhang, P. M. Levy, and A. Fert, “Mechanisms of Spin-Polarized Current-Driven Magnetization Switching,” Physical Review Letters, vol. 88, p. 236601, 2002. doi: 10.1103/PhysRevLett.88.236601.

  • [36]  J.-G. J. Zhu and C. Park, “Magnetic Tunnel Junctions,” Materials Today, vol. 9, no. 11, pp. 36–45, 2006. doi: 10.1016/S1369-7021(06)71693-5.

  • [37]  O. Golonzka, J. G. Alzate, U. Arslan, M. Bohr, P. Bai et al., “MRAM as Embedded Non-Volatile Memory Solution for 22FFL FinFET Technology,” in 2018 IEEE International Electron Devices Meeting (IEDM), 2018, pp. 18.1.1–18.1.4. doi: 10.1109/IEDM.2018.8614620.

  • [38]  S. Bhatti, R. Sbiaa, A. Hirohata, H. Ohno, S. Fukami et al., “Spintronics Based Random Access Memory: A Review,” Materials Today, vol. 20, no. 9, pp. 530–548, 2017. doi: 10.1016/j.mattod.2017.07.007.

  • [39]  J. A. Katine, F. J. Albert, R. A. Buhrman, E. B. Myers, and D. C. Ralph, “Current-Driven Magnetization Reversal and Spin-Wave Excitations in Co/Cu/Co Pillars,” Physical Review Letters, vol. 84, pp. 3149–3152, 2000. doi: 10.1103/PhysRevLett.84.3149.

  • [40]  A. V. Khvalkovskiy, D. Apalkov, S. Watts, R. Chepulskii, R. S. Beach et al., “Basic Principles of STT-MRAM Cell Operation in Memory Arrays,” Journal of Physics D: Applied Physics, vol. 46, no. 7, p. 074001, 2013. doi: 10.1088/0022-3727/46/7/074001.

  • [41]  F. C. Williams and T. Kilburn, “Electronic Digital Computers,” Nature, vol. 162, no. 4117, pp. 487–487, 1948. doi: 10.1038/162487a0.

  • [42]  W. N. Papian, “A Coincident-Current Magnetic Memory Cell for the Storage of Digital Information,” Proceedings of the IRE, vol. 40, no. 4, pp. 475–478, 1952. doi: 10.1109/JRPROC.1952.274045.

  • [43]  R. A. Abbott, W. M. Regitz, and J. A. Karp, “A 4K MOS Dynamic Random-Access Memory,” IEEE Journal of Solid-State Circuits, vol. 8, no. 5, pp. 292–298, 1973. doi: 10.1109/JSSC.1973.1050406.

  • [44]  M. N. Baibich, J. M. Broto, A. Fert, F. Nguyen Van Dau, F. Petroff et al., “Giant Magnetoresistance of (001)Fe/(001)Cr Magnetic Superlattices,” Physical Review Letters, vol. 61, no. 21, pp. 2472–2475, 1988. doi: 10.1103/PhysRevLett.61.2472.

  • [45]  G. Binasch, P. Grünberg, F. Saurenbach, and W. Zinn, “Enhanced Magnetoresistance in Layered Magnetic Structures with Antiferromagnetic Interlayer Exchange,” Physical Review B, vol. 39, no. 7, pp. 4828–4830, 1989. doi: 10.1103/PhysRevB.39.4828.

  • [46]  S. A. Wolf, D. D. Awschalom, R. A. Buhrman, J. M. Daughton, S. von Molnár et al., “Spintronics: A Spin-Based Electronics Vision for the Future,” Science, vol. 294, no. 5546, pp. 1488–1495, 2001. doi: 10.1126/science.1065389.

  • [47]  T. Miyazaki, T. Yaoi, and S. Ishio, “Large Magnetoresistance Effect in 82Ni-Fe/Al-Al\(_2\)O\(_3\)/Co Magnetic Tunneling Junction,” Journal of Magnetism and Magnetic Materials, vol. 98, no. 1, pp. L7–L9, 1991. doi: 10.1016/0304-8853(91)90417-9.

  • [48]  J. S. Moodera, L. R. Kinder, T. M. Wong, and R. Meservey, “Large Magnetoresistance at Room Temperature in Ferromagnetic Thin Film Tunnel Junctions,” Physical Review Letters, vol. 74, no. 16, pp. 3273–3276, 1995. doi: 10.1103/PhysRevLett.74.3273.

  • [49]  W. H. Butler, X.-G. Zhang, T. C. Schulthess, and J. M. MacLaren, “Spin-Dependent Tunneling Conductance of Fe/MgO/Fe(001) Sandwiches,” Physical Review B, vol. 63, no. 5, p. 054416, 2001. doi: 10.1103/PhysRevB.63.054416.

  • [50]  J. Mathon and A. Umerski, “Theory of Tunneling Magnetoresistance of Magnetic Junctions,” Physical Review B, vol. 63, no. 22, p. 220403(R), 2001. doi: 10.1103/PhysRevB.63.220403.

  • [51]  T. Kawahara, K. Ito, R. Takemura, and H. Ohno, “Spin-Transfer Torque RAM Technology: Review and Prospect,” Microelectronics Reliability, vol. 52, no. 4, pp. 613–627, 2012. doi: 10.1016/j.microrel.2011.09.028.

  • [52]  W. Kim, J. H. Jeong, Y. Kim, W. C. Lim, J. H. Kim et al., “Extended Scalability of Perpendicular STT-MRAM Towards Sub-20nm MTJ Node,” in 2011 International Electron Devices Meeting, 2011, pp. 24.1.1–24.1.4. doi: 10.1109/IEDM.2011.6131602.

  • [53]  S. Ikeda, J. Hayakawa, Y. Ashizawa, Y. M. Lee, K. Miura et al., “Tunnel Magnetoresistance of 604 % at 300 K by Suppression of Ta Diffusion in CoFeB/MgO/CoFeB Pseudo-Spin-Valves Annealed at High Temperature,” Applied Physics Letters, vol. 93, no. 8, p. 082508, 2008. doi: 10.1063/1.297643.

  • [54]  J. Åkerman, “Toward a Universal Memory,” Science, vol. 308, no. 5721, pp. 508–510, 2005. doi: 10.1126/science.1110549.

  • [55]  T. Sousa, J.-P. Wang, and T. Low, “Bidirectional Switching Assisted by Interlayer Exchange Coupling in Perpendicular MTJs,” Physical Review B, vol. 101, p. 081404(R), 2020. doi: 10.1103/PhysRevB.101.081404.

  • [56]  Y. Saito, T. Roy, S. Ikeda, M. Shirai, H. Honjo et al., “Strong Antiferromagnetic Interlayer Exchange Coupling Induced by Small Additions of Re to an Ir Interlayer in Synthetic Antiferromagnetic Systems,” Scientific Reports, vol. 15, no. 1, p. 8977, 2025. doi: 10.1038/s41598-025-94088-w.

  • [57]  Q. Shao, Z. Wang, Y. Zhou, S. Fukami, D. Querlioz et al., “Spintronic Memristors for Computing,” npj Spintronics, vol. 3, no. 1, p. 16, 2025. doi: 10.1038/s44306-025-00078-z.

  • [58]  B. Dieny, V. S. Speriosu, S. S. P. Parkin, B. A. Gurney, D. R. Wilhoit et al., “Giant Magnetoresistance in Soft Ferromagnetic Multilayers,” Physical Review B, vol. 43, pp. 1297–1300, 1991. doi: 10.1103/PhysRevB.43.1297.

  • [59]  G. A. Prinz, “Spin-Polarized Transport,” Physics Today, vol. 48, no. 4, pp. 58–63, 1995. doi: 10.1063/1.881459.

  • [60]  S. S. P. Parkin, “Spin-Dependent Tunnelling in Magnetic Nanostructures and Magnetic Tunnel Junctions for High Density Magnetic Random Access Memory,” IBM Journal of Research and Development, vol. 44, no. 1/2, pp. 245–262, 2000. doi: 10.1147/rd.441.0245.

  • [61]  M. Bowen, V. Cros, F. Petroff, A. Fert, C. Martínez Boubeta et al., “Large Magnetoresistance in Fe/MgO/FeCo(001) Epitaxial Tunnel Junctions on GaAs(001),” Applied Physics Letters, vol. 79, no. 11, pp. 1655–1657, 2001. doi: 10.1063/1.1404125.

  • [62]  J. Faure-Vincent, C. Tiusan, E. Jouguelet, F. Canet, M. Sajieddine et al., “High Tunnel Magnetoresistance in Epitaxial Fe/MgO/Fe Tunnel Junctions,” Applied Physics Letters, vol. 82, no. 25, pp. 4507–4509, 2003. doi: 10.1063/1.1586785.

  • [63]  J. C. Slonczewski, “Conductance and Exchange Coupling of Two Ferromagnets Separated by a Tunneling Barrier,” Physical Review B, vol. 39, no. 10, pp. 6995–7002, 1989. doi: 10.1103/PhysRevB.39.6995.

  • [64]  Y. Ji, J. Liu, and C. Yang, “Novel Modeling and Dynamic Simulation of Magnetic Tunnel Junctions for Spintronic Sensor Development,” Journal of Physics D: Applied Physics, vol. 50, no. 2, p. 025005, 2016. doi: 10.1088/0022-3727/50/2/025005.

  • [65]  H. Jaffrès, D. Lacour, F. N. V. Dau, J. Briatico, F. Petroff et al., “Angular Dependence of the Tunnel Magnetoresistance in Transition-Metal-Based Junctions,” Physical Review B, vol. 64, no. 6, p. 064427, 2001. doi: 10.1103/PhysRevB.64.064427.

  • [66]  T. Miyazaki and N. Tezuka, “Giant Magnetic Tunneling Effect in Fe/Al\(_2\)O\(_3\)/Fe Junction,” Journal of Magnetism and Magnetic Materials, vol. 139, no. 3, pp. L231–L234, 1995. doi: 10.1016/0304-8853(95)90001-2.

  • [67]  D. Wang, C. Nordman, J. Daughton, Z. Qian, and J. Fink, “70% TMR at Room Temperature for SDT Sandwich Junctions with CoFeB as Free and Reference Layers,” IEEE Transactions on Magnetics, vol. 40, no. 4, pp. 2269–2271, 2004. doi: 10.1109/TMAG.2004.830219.

  • [68]  S. Ikeda, J. Hayakawa, Y. M. Lee, R. Sasaki, T. Meguro et al., “Dependence of Tunnel Magnetoresistance in MgO Based Magnetic Tunnel Junctions on Ar Pressure During MgO Sputtering,” Japanese Journal of Applied Physics, vol. 44, no. 48, pp. L1442–L1445, 2005. doi: 10.1143/JJAP.44.L1442.

  • [69]  S. Yuasa, T. Nagahama, A. Fukushima, and Y. Suzuki, “High TMR Ratio of 410% in Epitaxial Fe/MgO/Fe Tunnel Junctions Annealed at High Temperature,” Applied Physics Letters, vol. 89, no. 23, p. 232510, 2006. doi: 10.1063/1.2398002.

  • [70]  Y. Huai, F. Albert, P. Nguyen, M. Pakala, and T. Valet, “Observation of Spin-Transfer Switching in Deep Submicron-Sized and Low-Resistance Magnetic Tunnel Junctions,” Applied Physics Letters, vol. 84, no. 16, pp. 3118–3120, 2004. doi: 10.1063/1.1707228.

  • [71]  D. C. Worledge, G. Hu, D. W. Abraham, J. Z. Sun, P. L. Trouilloud et al., “Spin Torque Switching of Perpendicular Ta/CoFeB/MgO-Based Magnetic Tunnel Junctions,” Applied Physics Letters, vol. 98, no. 2, p. 022501, 2011. doi: 10.1063/1.3536482.

  • [72]  H. Sato, M. Yamanouchi, K. Miura, S. Ikeda, H. D. Gan et al., “Junction Size Effect on Switching Current and Thermal Stability in CoFeB/MgO Perpendicular Magnetic Tunnel Junctions,” Applied Physics Letters, vol. 99, no. 4, p. 042501, 2011. doi: 10.1063/1.3617429.

  • [73]  T. Devolder, J.-V. Kim, F. Garcia-Sanchez, J. Swerts, W. Kim et al., “Time-Resolved Spin-Torque Switching in MgO-Based Perpendicularly Magnetized Tunnel Junctions,” Physical Review B, vol. 93, p. 024420, 2016. doi: 10.1103/PhysRevB.93.024420.

  • [74]  D. C. Worledge, “Write-error-rate of Spin-Transfer-Torque MRAM (Invited),” in 2023 IEEE International Reliability Physics Symposium (IRPS), 2023, pp. 1–4. doi: 10.1109/IRPS48203.2023.10117666.

  • [75]  L. Wu, M. Taouil, S. Rao, E. J. Marinissen, and S. Hamdioui, “Survey on STT-MRAM Testing: Failure Mechanisms, Fault Models, and Tests,” 2020. [Online]. Available: https://arxiv.org/abs/2001.05463

  • [76]  J. C. Sankey, Y.-T. Cui, J. Z. Sun, J. C. Slonczewski, R. A. Buhrman et al., “Measurement of the Spin-Transfer-Torque Vector in Magnetic Tunnel Junctions,” Nature Physics, vol. 4, no. 1, pp. 67–71, 2008. doi: 10.1038/nphys783.

  • [77]  J. Z. Sun, “Spin Angular Momentum Transfer in Current-Perpendicular Nanomagnetic Junctions,” IBM Journal of Research and Development, vol. 50, no. 1, pp. 81–100, 2006. doi: 10.1147/rd.501.0081.

  • [78]  D. Apalkov, S. Watts, A. Driskill-Smith, E. Chen, Z. Diao et al., “Comparison of Scaling of In-Plane and Perpendicular Spin Transfer Switching Technologies by Micromagnetic Simulation,” IEEE Transactions on Magnetics, vol. 46, no. 6, pp. 2240–2243, 2010. doi: 10.1109/TMAG.2010.2041330.

  • [79]  Z. Guo, J. Yin, Y. Bai, D. Zhu, K. Shi et al., “Spintronics for Energy-Efficient Computing: An Overview and Outlook,” Proceedings of the IEEE, vol. 109, no. 8, pp. 1398–1417, 2021. doi: 10.1109/JPROC.2021.3084997.

  • [80]  W. Zhao, X. Zhao, B. Zhang, K. Cao, L. Wang et al., “Failure Analysis in Magnetic Tunnel Junction Nanopillar with Interfacial Perpendicular Magnetic Anisotropy,” Materials, vol. 9, no. 1, 2016. doi: 10.3390/ma9010041.

  • [81]  R. Sbiaa, H. Meng, and S. N. Piramanayagam, “Materials with Perpendicular Magnetic Anisotropy for Magnetic Random Access Memory,” physica status solidi (RRL) – Rapid Research Letters, vol. 5, no. 12, pp. 413–419, 2011. doi: 10.1002/pssr.201105420.

  • [82]  B. Tudu and A. Tiwari, “Recent Developments in Perpendicular Magnetic Anisotropy Thin Films for Data Storage Applications,” Vacuum, vol. 146, pp. 329–341, 2017. doi: 10.1016/j.vacuum.2017.01.031.

  • [83]  J. Hayakawa, S. Ikeda, Y. M. Lee, R. Sasaki, T. Meguro et al., “Current-Induced Magnetization Switching in MgO Barrier Based Magnetic Tunnel Junctions with CoFeB/Ru/CoFeB Synthetic Ferrimagnetic Free Layer,” Japanese Journal of Applied Physics, vol. 45, no. 10L, p. L1057, 2006. doi: 10.1143/JJAP.45.L1057.

  • [84]  S. Mangin, D. Ravelosona, J. A. Katine, M. J. Carey, B. D. Terris et al., “Current-Induced Magnetization Reversal in Nanopillars with Perpendicular Anisotropy,” Nature Materials, vol. 5, no. 3, pp. 210–215, 2006. doi: 10.1038/nmat1595.

  • [85]  L. Cuchet, B. Rodmacq, S. Auffret, S. Bandiera, B. Dieny et al., “Perpendicular Magnetic Tunnel Junctions with a Synthetic Storage or Reference Layer: A New Route Towards Pt- and Pd-Free Junctions,” Scientific Reports, vol. 6, p. 21246, 2016. doi: 10.1038/srep21246.

  • [86]  J. Igarashi, B. Jinnai, K. Watanabe, T. Shinoda, T. Funatsu et al., “Single-Nanometer CoFeB/MgO Magnetic Tunnel Junctions with High-Retention and High-Speed Capabilities,” npj Spintronics, vol. 2, no. 1, p. 1, 2024. doi: 10.1038/s44306-023-00003-2.

  • [87]  Q. Yang, L. Wang, Z. Zhou, L. Wang, Y. Zhang et al., “Ionic Liquid Gating Control of RKKY Interaction in FeCoB/Ru/FeCoB and (Pt/Co)\(_2\)/Ru/(Co/Pt)\(_2\) Multilayers,” Nature Communications, vol. 9, no. 1, p. 991, 2018. doi: 10.1038/s41467-018-03356-z.

  • [88]  C.-L. Yang and C.-H. Lai, “High Thermal Durability of Ru-Based Synthetic Antiferromagnet by Interfacial Engineering with Re Insertion,” Scientific Reports, vol. 11, no. 1, p. 15214, 2021. doi: 10.1038/s41598-021-94640-4.

  • [89]  W. F. Brown, Micromagnetics, ser. Interscience tracts on physics and astronomy. Interscience Publishers, 1963. [Online]. Available: https://cir.nii.ac.jp/crid/1130282271226285568

  • [90]  C. Abert, “Micromagnetics and Spintronics: Models and Numerical Methods,” The European Physical Journal B, vol. 92, no. 6, p. 120, 2019. doi: 10.1140/epjb/e2019-90599-6.

  • [91]  H. Kronmüller, “General Micromagnetic Theory,” in Handbook of Magnetism and Advanced Magnetic Materials, ser. Micromagnetism, H. Kronmüller and S. S. P. Parkin, Eds. Chichester, UK: John Wiley & Sons, Ltd, 2007, vol. 2, pp. 703–741. ISBN 978-0-470-02218-4. doi: 10.1002/9780470022184.hmm201.

  • [92]  L. D. Landau and E. M. Lifshitz, “On the Theory of the Dispersion of Magnetic Permeability in Ferromagnetic Bodies,” Phys. Z. Sowjetunion, vol. 8, pp. 153–164, 1935. doi: 10.1016/B978-0-08-036364-6.50008-9.

  • [93]  T. Gilbert, “A Phenomenological Theory of Damping in Ferromagnetic Materials,” IEEE Transactions on Magnetics, vol. 40, no. 6, pp. 3443–3449, 2004. doi: 10.1109/TMAG.2004.836740.

  • [94]  I. Cimrák, “A Survey on the Numerics and Computations for the Landau-Lifshitz Equation of Micromagnetism,” Archives of Computational Methods in Engineering, vol. 15, no. 3, pp. 1–37, 2007. doi: 10.1007/BF03024947.

  • [95]  J. D. Jackson, Classical Electrodynamics, 3rd ed. John Wiley & Sons, Ltd, 2003. doi: 10.1002/3527600434.eap109.

  • [96]  W. Heisenberg, “Mehrkörperproblem und Resonanz in der Quantenmechanik,” Zeitschrift für Physik, vol. 38, no. 6–7, pp. 411–426, 1926. doi: 10.1007/BF01397160. English translation: “Many-body Problem and Resonance in Quantum Mechanics”.

  • [97]  D. J. Griffiths and D. F. Schroeter, Introduction to Quantum Mechanics, 3rd ed. Cambridge University Press, 2018. doi: 10.1017/9781316995433.

  • [98]  W. Döring, “Mikromagnetismus,” in Handbuch der Physik, 1st ed., ser. Encyclopedia of Physics. Berlin, Heidelberg: Springer, 1966, vol. 18, no. 2, pp. 314–437. ISBN 978-3-642-46035-7. doi: 10.1007/978-3-642-46035-7.

  • [99]  A. Hubert and R. Schäfer, Magnetic Domains: The Analysis of Magnetic Microstructures. Berlin, Heidelberg: Springer, 1998. doi: 10.1007/978-3-540-85054-0.

  • [100]  J. E. Miltat and M. J. Donahue, “Numerical Micromagnetics: Finite Difference Methods,” in Handbook of Magnetism and Advanced Magnetic Materials, H. Kronmüller, S. Parkin, J. E. Miltat, and M. R. Scheinfein, Eds. John Wiley & Sons, Ltd, 2007. ISBN 978-0-470-02218-4. doi: 10.1002/9780470022184.hmm202.

  • [101]  M. Labrune and J. Miltat, “Wall Structures in Ferro/Antiferromagnetic Exchange-Coupled Bilayers: A Numerical Micromagnetic Approach,” Journal of Magnetism and Magnetic Materials, vol. 151, no. 1, pp. 231–245, 1995. doi: 10.1016/0304-8853(95)00328-2.

  • [102]  A. Aharoni, “Demagnetizing Factors for Rectangular Ferromagnetic Prisms,” Journal of Applied Physics, vol. 83, no. 6, pp. 3432–3434, 1998. doi: 10.1063/1.367113.

  • [103]  A. Makarov, “Modeling of Emerging Resistive Switching Based Memory Cells,” Ph.D. dissertation, Technische Universität Wien, 2014. doi: 10.34726/hss.2014.23875.

  • [104]  J.-B. Biot and F. Savart, “Note Sur Le Magnétisme De La Pile De Volta,” Annales de Chimie et de Physique, vol. 15, pp. 222–223, 1820, english translation: “Note On The Magnetism Of The Voltaic Pile”.

  • [105]  G. Finocchio, M. Carpentieri, B. Azzerboni, L. Torres, E. Martinez et al., “Micromagnetic Simulations of Nanosecond Magnetization Reversal Processes in Magnetic Nanopillar,” Journal of Applied Physics, vol. 99, no. 8, p. 08G522, 2006. doi: 10.1063/1.2177049.

  • [106]  J. L. García-Palacios and F. J. Lázaro, “Langevin-Dynamics Study of the Dynamical Properties of Small Magnetic Particles,” Physical Review B, vol. 58, pp. 14 937–14 958, 1998. doi: 10.1103/PhysRevB.58.14937.

  • [107]  G. Finocchio, B. Azzerboni, G. D. Fuchs, R. A. Buhrman, and L. Torres, “Micromagnetic Modeling of Magnetization Switching Driven by Spin-Polarized Current in Magnetic Tunnel Junctions,” Journal of Applied Physics, vol. 101, no. 6, p. 063914, 2007. doi: 10.1063/1.2496202.

  • [108]  M. A. Ruderman and C. Kittel, “Indirect Exchange Coupling of Nuclear Magnetic Moments by Conduction Electrons,” Physical Review, vol. 96, no. 1, pp. 99–102, 1954. doi: 10.1103/PhysRev.96.99.

  • [109]  T. Kasuya, “A Theory of Metallic Ferro- and Antiferromagnetism on Zener’s Model,” Progress of Theoretical Physics, vol. 16, no. 1, pp. 45–57, 1956. doi: 10.1143/PTP.16.45.

  • [110]  K. Yosida, “Magnetic Properties of Cu-Mn Alloys,” Physical Review, vol. 106, no. 5, pp. 893–898, 1957. doi: 10.1103/PhysRev.106.893.

  • [111]  P. Bruno, “Tight-Binding Approach to the Orbital Magnetic Moment and Magnetocrystalline Anisotropy of Transition-Metal Monolayers,” Physical Review B, vol. 52, no. 1, pp. 411–439, 1995. doi: 10.1103/PhysRevB.52.411.

  • [112]  E. Tsymbal and D. Pettifor, “Perspectives of Giant Magnetoresistance,” Solid State Physics, vol. 56, pp. 113–237, 2001. doi: 10.1016/S0081-1947(01)80019-9.

  • [113]  S. S. P. Parkin, R. Bhadra, and K. P. Roche, “Oscillations in Exchange Coupling and Magnetoresistance in Metallic Superlattices,” Physical Review Letters, vol. 66, pp. 2152–2155, 1991. doi: 10.1103/PhysRevLett.66.2152.

  • [114]  B. Dieny, “Giant Magnetoresistance in Spin-Valve Multilayers,” Journal of Magnetism and Magnetic Materials, vol. 136, no. 3, pp. 335–359, 1994. doi: 10.1016/0304-8853(94)90046-9.

  • [115]  J. C. Slonczewski, “Fluctuation Mechanism for Biquadratic Exchange Coupling in Magnetic Multilayers,” Physical Review Letters, vol. 67, no. 23, pp. 3172–3175, 1991. doi: 10.1103/PhysRevLett.67.3172.

  • [116]  M. Bendra, R. L. d. Orio, S. Selberherr, W. Goes, and V. Sverdlov, “Advanced Modeling and Simulation of Multilayer Spin-Transfer Torque Magnetoresistive Random Access Memory with Interface Exchange Coupling,” Micromachines, vol. 15, no. 5, 2024. doi: 10.3390/mi15050568.

  • [117]  J. Slonczewski, “Currents and Torques in Metallic Magnetic Multilayers,” Journal of Magnetism and Magnetic Materials, vol. 247, no. 3, pp. 324–338, 2002. doi: 10.1016/S0304-8853(02)00291-3.

  • [118]  M. Chshiev, A. Manchon, A. Kalitsov, N. Ryzhanova, A. Vedyayev et al., “Analytical Description of Ballistic Spin Currents and Torques in Magnetic Tunnel Junctions,” Physical Review B, vol. 92, p. 104422, 2015. doi: 10.1103/PhysRevB.92.104422.

  • [119]  J. C. Slonczewski, “Currents, Torques, and Polarization Factors in Magnetic Tunnel Junctions,” Physical Review B, vol. 71, p. 024411, 2005. doi: 10.1103/PhysRevB.71.024411.

  • [120]  S. Lepadatu, “Unified Treatment of Spin Torques Using a Coupled Magnetisation Dynamics and Three-Dimensional Spin Current Solver,” Scientific Reports, vol. 7, no. 1, p. 12937, 2017. doi: 10.1038/s41598-017-13181-x.

  • [121]  P. Graczyk and M. Krawczyk, “Nonresonant Amplification of Spin Waves Through Interface Magnetoelectric Effect and Spin-Transfer Torque,” Scientific Reports, vol. 11, no. 1, p. 15692, 2021. doi: 10.1038/s41598-021-95267-1.

  • [122]  P. M. Haney, H.-W. Lee, K.-J. Lee, A. Manchon, and M. D. Stiles, “Current Induced Torques and Interfacial Spin-Orbit Coupling: Semiclassical Modeling,” Physical Review B, vol. 87, no. 17, p. 174411, 2013. doi: 10.1103/PhysRevB.87.174411.

  • [123]  S. Fiorentini, M. Bendra, J. Ender, R. L. de Orio, W. Goes et al., “Spin and Charge Drift-Diffusion in Ultra-Scaled MRAM Cells,” Scientific Reports, vol. 12, no. 1, p. 20958, 2022. doi: 10.1038/s41598-022-25586-4.

  • [124]  S. Fiorentini, N. P. Jørstad, J. Ender, R. L. de Orio, S. Selberherr, and M. Bendra, “Finite Element Approach for the Simulation of Modern MRAM Devices,” Micromachines, vol. 14, no. 5, p. 898, 2023. doi: 10.3390/mi14050898.

  • [125]  S. Fiorentini, “Computation of Torques in Magnetic Tunnel Junctions,” Ph.D. dissertation, Technische Universität Wien, 2023. doi: 10.34726/hss.2023.109800.

  • [126]  D. Berkov, K. Ramstöck, and A. Hubert, “Solving Micromagnetic Problems: Towards an Optimal Numerical Method,” physica status solidi (a), vol. 137, no. 1, pp. 207–225, 1993. doi: 10.1002/pssa.2211370122.

  • [127]  C. Seberino and H. N. Bertram, “Concise, Efficient Three-Dimensional Fast Multipole Method for Micromagnetics,” IEEE Transactions on Magnetics, vol. 37, no. 2, pp. 1078–1081, 2001. doi: 10.1109/20.917510.

  • [128]  C. Grossmann, H.-G. Roos, and M. Stynes, Numerical Treatment of Partial Differential Equations. Berlin: Springer, 2007. doi: 10.1007/978-3-540-71584-9.

  • [129]  H. P. Langtangen and S. Linge, Finite Difference Computing with PDEs: A Modern Software Approach, ser. Texts in Computational Science and Engineering. Springer Cham, 2017. doi: 10.1007/978-3-319-55456-3.

  • [130]  R. J. LeVeque, Finite Difference Methods for Ordinary and Partial Differential Equations: Steady-State and Time-Dependent Problems. Philadelphia, PA: Society for Industrial and Applied Mathematics, 2007. doi: 10.1137/1.9780898717839.

  • [131]  Y. Saad, Iterative Methods for Sparse Linear Systems, 2nd ed. Philadelphia, PA: Society for Industrial and Applied Mathematics, 2003. doi: 10.1137/1.9780898718003.

  • [132]  D. M. Young, “Iterative Methods for Solving Partial Difference Equations of Elliptic Type,” Transactions of the American Mathematical Society, vol. 76, pp. 92–111, 1954. doi: 10.1090/S0002-9947-1954-0059635-7.

  • [133]  A. Kákay, “Numerical Investigations of Micromagnetic Structures,” Ph.D. dissertation, Research Institute for Solid State Physics and Optics, Hungarian Academy of Sciences, Budapest, Hungary, 2005. [Online]. Available: https://repozitorium.omikk.bme.hu/bitstreams/58e4eecb-0672-418d-be04-59e763811136/download

  • [134]  D. Tomáš, “Modelling of Micromagnetic Structures,” Ph.D. dissertation, Paris-Sud University, Orsay and Charles University, Prague, France and Czech Republic, 1999.

  • [135]  F. Alouges, “A New Finite Element Scheme for Landau-Lifshitz Equations,” Discrete and Continuous Dynamical Systems - S, vol. 1, no. 2, pp. 187–196, 2008. doi: 10.3934/dcdss.2008.1.187.

  • [136]  K. Ito, T. Devolder, C. Chappert, M. J. Carey, and J. A. Katine, “Probabilistic Behavior in Subnanosecond Spin Transfer Torque Switching,” Journal of Applied Physics, vol. 99, no. 8, p. 08G519, 2006. doi: 10.1063/1.2176869.

  • [137]  T. J. R. Hughes, The Finite Element Method: Linear Static and Dynamic Finite Element Analysis, ser. Dover Civil and Mechanical Engineering. Mineola, NY: Courier Corporation, 2012. ISBN 978-0-486-13502-1

  • [138]  A. Ern and J.-L. Guermond, Theory and Practice of Finite Elements, ser. Applied Mathematical Sciences. New York, NY: Springer, 2004, vol. 159. doi: 10.1007/978-1-4757-4355-5.

  • [139]  S. C. Brenner and L. R. Scott, The Mathematical Theory of Finite Element Methods, 3rd ed., ser. Texts in Applied Mathematics. New York, NY: Springer, 2008. doi: 10.1007/978-0-387-75934-0.

  • [140]  A. Quarteroni and A. Valli, Numerical Approximation of Partial Differential Equations, 1st ed., ser. Springer Series in Computational Mathematics. Springer-Verlag Berlin Heidelberg, 1994, vol. 23. doi: 10.1007/978-3-540-85268-1.

  • [141]  J. Nitsche, “Über ein Variationsprinzip zur Lösung von Dirichlet-Problemen bei Verwendung von Teilräumen, die keinen Randbedingungen unterworfen sind,” Abhandlungen aus dem Mathematischen Seminar der Universität Hamburg, vol. 36, no. 1, pp. 9–15, 1971. doi: 10.1007/BF02995904.

  • [142]  A. Logg, K.-A. Mardal, and G. N. Wells, Eds., Automated Solution of Differential Equations by the Finite Element Method: The FEniCS Book, ser. Lecture Notes in Computational Science and Engineering. Berlin, Heidelberg: Springer, 2012. doi: 10.1007/978-3-642-23099-8.

  • [143]  ViennaSpinMag, “An Open Access Finite Element-based Application for Calculating the Magnetization Dynamics of Multi-layered Structures Composed of Ferromagnets, Metal Spacers and Tunnel Barriers,” 2025, Accessed: 19.07.2025. [Online]. Available: https://www.iue.tuwien.ac.at/viennaspinmag

  • [144]  R. Anderson, J. Andrej, A. Barker, J. Bramwell, J.-S. Camier et al., “MFEM: A Modular Finite Element Methods Library,” Computers & Mathematics with Applications, vol. 81, pp. 42–74, 2021. doi: 10.1016/j.camwa.2020.06.009.

  • [145]  T. Kolev and V. Dobrev, “Modular Finite Element Methods (MFEM),” Jun. 2010, MFEM is a modular parallel C++ library for finite element methods. Its goal is to enable high-performance scalable finite element discretization research and application development on a wide variety of platforms, ranging from laptops to supercomputers. [Online]. Available: https://doi.org/10.11578/dc.20171025.1248

  • [146]  D. Braess, Finite Elements: Theory, Fast Solvers, and Applications in Solid Mechanics, 3rd ed. Cambridge University Press, 2007. doi: 10.1017/CBO9780511618635.

  • [147]  M. G. Larson and F. Bengzon, Electromagnetics, 1st ed., ser. Texts in Computational Science and Engineering. Springer, 2013, vol. 10, pp. 327–354. ISBN 978-3-642-33287-6

  • [148]  Q. Chen and A. Konrad, “A Review of Finite Element Open Boundary Techniques for Static and Quasi-Static Electromagnetic Field Problems,” IEEE Transactions on Magnetics, vol. 33, no. 1, pp. 663–676, 1997. doi: 10.1109/20.560095.

  • [149]  D. Fredkin and T. Koehler, “Hybrid Method for Computing Demagnetizing Fields,” IEEE Transactions on Magnetics, vol. 26, no. 2, pp. 415–417, 1990. doi: 10.1109/20.106342.

  • [150]  W. Hackbusch, “A Sparse Matrix Arithmetic Based on H-Matrices. Part I: Introduction to H-Matrices,” Computing, vol. 62, no. 2, pp. 89–108, 1999. doi: 10.1007/s006070050015.

  • [151]  S. Börm, L. Grasedyck, and W. Hackbusch, “Introduction to Hierarchical Matrices with Applications,” Engineering Analysis with Boundary Elements, vol. 27, no. 5, pp. 405–422, 2003. doi: 10.1016/S0955-7997(02)00152-2.

  • [152]  N. C. µMag Modeling Group, “Standard Problem #3.” [Online]. Available: https://www.ctcms.nist.gov/~rdm/spec3.html

  • [153]  C. Abert, L. Exl, G. Selke, A. Drews, and T. Schrefl, “Numerical Methods for the Stray-Field Calculation: A Comparison of Recently Developed Algorithms,” Journal of Magnetism and Magnetic Materials, vol. 326, pp. 176–185, 2013. doi: 10.1016/j.jmmm.2012.08.041.

  • [154]  M. Bendra, J. Ender, S. Fiorentini, T. Hadamek, R. de Orio et al., “Finite Element Method Approach to MRAM Modeling,” in 2021 44th International Convention on Information, Communication and Electronic Technology (MIPRO), 2021, pp. 70–73. doi: 10.23919/MIPRO52101.2021.9597194.

  • [155]  J. M. Camacho and V. Sosa, “Alternative Method to Calculate the Magnetic Field of Permanent Magnets with Azimuthal Symmetry,” Revista mexicana de física E, vol. 59, pp. 8–17, 06 2013. doi: 10.31349/RevMexFisE.21.020701.

  • [156]  E. Hairer and G. Wanner, Solving Ordinary Differential Equations II: Stiff and Differential-Algebraic Problems, 2nd ed., ser. Springer Series in Computational Mathematics. Berlin, Heidelberg: Springer-Verlag, 1996, vol. 14. doi: 10.1007/978-3-642-05221-7.

  • [157]  V. D. Tsiantos, D. Suess, T. Schrefl, and J. Fidler, “Stiffness Analysis for the Micromagnetic Standard Problem No. 4,” Journal of Applied Physics, vol. 89, no. 11, pp. 7600–7602, 2001. doi: 10.1063/1.1355355.

  • [158]  D. Suess, V. Tsiantos, T. Schrefl, J. Fidler, W. Scholz et al., “Time Resolved Micromagnetics Using a Preconditioned Time Integration Method,” Journal of Magnetism and Magnetic Materials, vol. 248, no. 2, pp. 298–311, 2002. doi: 10.1016/S0304-8853(02)00341-4.

  • [159]  D. Shepherd, J. Miles, M. Heil, and M. Mihajlović, “Discretization-Induced Stiffness in Micromagnetic Simulations,” IEEE Transactions on Magnetics, vol. 50, no. 11, pp. 1–4, 2014. doi: 10.1109/TMAG.2014.2325494.

  • [160]  D. Praetorius, M. Ruggeri, and B. Stiftner, “Convergence of an Implicit-Explicit Midpoint Scheme for Computational Micromagnetics,” Computers & Mathematics with Applications, vol. 75, no. 5, pp. 1719–1738, 2018. doi: 10.1016/j.camwa.2017.11.028.

  • [161]  A. C. Hindmarsh, P. N. Brown, K. E. Grant, S. L. Lee, R. Serban et al., “SUNDIALS: Suite of nonlinear and differential/algebraic equation solvers,” ACM Transactions on Mathematical Software, vol. 31, no. 3, pp. 363–396, 2005. doi: 10.1145/1089014.1089020.

  • [162]  U. M. Ascher, S. J. Ruuth, and R. J. Spiteri, “Implicit-Explicit Runge-Kutta Methods for Time-Dependent Partial Differential Equations,” Applied Numerical Mathematics, vol. 25, no. 2–3, pp. 151–167, 1997. doi: 10.1016/S0168-9274(97)00056-1.

  • [163]  M. Benzi, G. H. Golub, and J. Liesen, “Numerical Solution of Saddle Point Problems,” Acta Numerica, vol. 14, pp. 1–137, 2005. doi: 10.1017/S0962492904000212.

  • [164]  Y. Saad and M. H. Schultz, “GMRES: A generalized minimal residual algorithm for solving nonsymmetric linear systems,” SIAM J. Sci. Stat. Comput., vol. 7, no. 3, pp. 856–869, 1986. doi: 10.1137/0907058.

  • [165]  E. Kim and J. Wilkening, “Convergence of a Mass-Lumped Finite Element Method for the Landau-Lifshitz Equation,” Quarterly of Applied Mathematics, vol. 76, no. 2, pp. 383–405, 2018. doi: 10.1090/qam/1485.

  • [166]  N. J. Mauser, C.-M. Pfeiler, D. Praetorius, and M. Ruggeri, “Unconditional Well-Posedness and IMEX Improvement of a Family of Predictor-Corrector Methods in Micromagnetics,” Applied Numerical Mathematics, vol. 180, pp. 33–54, 2022. doi: 10.1016/j.apnum.2022.05.008.

  • [167]  R. E. Bank and D. J. Rose, “Some Error Estimates for the Box Method,” SIAM Journal on Numerical Analysis, vol. 24, no. 4, pp. 777–787, 1987. doi: 10.1137/0724050.

  • [168]  H. A. van der Vorst, “Bi-CGSTAB: A Fast and Smoothly Converging Variant of Bi-CG for the Solution of Nonsymmetric Linear Systems,” SIAM J. Sci. Stat. Comput., vol. 13, no. 2, pp. 631–644, 1992. doi: 10.1137/0913035.

  • [169]  A. M. Bruaset, Krylov Subspace Iterations for Sparse Linear Systems. Boston, MA: Birkhäuser Boston, 1997, pp. 255–280. ISBN 978-1-4612-1984-2

  • [170]  A. Greenbaum, Iterative Methods for Solving Linear Systems. Philadelphia: Society for Industrial and Applied Mathematics, 1997. doi: 10.1137/1.9781611970937.

  • [171]  Lawrence Livermore National Laboratory, “HYPRE: Scalable Linear Solvers and Multigrid Methods,” https://github.com/hypre-space/hypre, 2024.

  • [172]  P. J. Roache, Verification and Validation in Computational Science and Engineering. Albuquerque, NM: Hermosa Publishers, 1998. ISBN 978-0913478080

  • [173]  Micromagnetic Modeling Activity Group, “\(\mu \)MAG Standard Problem #4,” https://www.ctcms.nist.gov/~rdm/std4/spec4.html, 2000, accessed: 2024.

  • [174]  J. Miltat, G. Albuquerque, and A. Thiaville, An Introduction to Micromagnetics in the Dynamic Regime. Berlin, Heidelberg: Springer Berlin Heidelberg, 2002, pp. 1–33. ISBN 978-3-540-40907-6

  • [175]  M. d’Aquino, C. Serpico, and G. Miano, “Geometrical Integration of Landau-Lifshitz-Gilbert Equation Based on the Mid-Point Rule,” Journal of Computational Physics, vol. 209, no. 2, pp. 730–753, 2005. doi: https://doi.org/10.1016/j.jcp.2005.04.001.

  • [176]  G. Di Fratta, C.-M. Pfeiler, D. Praetorius, M. Ruggeri, and B. Stiftner, “Linear Second-Order IMEX-Type Integrator for the (Eddy Current) Landau–Lifshitz–Gilbert Equation,” IMA Journal of Numerical Analysis, vol. 40, no. 4, pp. 2802–2838, 2020. doi: 10.1093/imanum/drz046.

  • [177]  J. Zhan, L. Yang, R. Du, and Z. Cui, “Towards Preserving Geometric Properties of Landau–Lifshitz–Gilbert Equation Using Multistep Methods,” Communications in Computational Physics, vol. 36, no. 4, pp. 1024–1050, 2024. doi: 10.4208/cicp.OA-2023-0201.

  • [178]  P. Chen, C. Li, Z. Liang et al., “Temporal High-Order Accurate Numerical Scheme for the Landau–Lifshitz–Gilbert Equation,” Mathematics, vol. 12, no. 8, p. 1179, 2024. doi: 10.3390/math12081179.

  • [179]  T. Valet and A. Fert, “Theory of the Perpendicular Magnetoresistance in Magnetic Multilayers,” Physical Review B, vol. 48, pp. 7099–7113, 1993. doi: 10.1103/PhysRevB.48.7099.

  • [180]  V. S. Rychkov, S. Borlenghi, H. Jaffres, A. Fert, and X. Waintal, “Spin Torque and Waviness in Magnetic Multilayers: A Bridge between Valet-Fert Theory and Quantum Approaches,” Phys. Rev. Lett., vol. 103, p. 066602, 2009. doi: 10.1103/PhysRevLett.103.066602.

  • [181]  S. Borlenghi, V. Rychkov, C. Petitjean, and X. Waintal, “Multiscale Approach to Spin Transport in Magnetic Multilayers,” Phys. Rev. B, vol. 84, p. 035412, 2011. doi: 10.1103/PhysRevB.84.035412.

  • [182]  M. Bendra, S. Fiorentini, J. Ender, R. L. de Orio, T. Hadámek et al., “Spin Transfer Torques in Ultra-Scaled MRAM Cells,” in 2022 45th Jubilee International Convention on Information, Communication and Electronic Technology (MIPRO), 2022, pp. 129–132. doi: 10.23919/MIPRO55190.2022.9803736.

  • [183]  K. Y. Camsari, S. Ganguly, D. Datta, and S. Datta, “Physics-Based Factorization of Magnetic Tunnel Junctions for Modeling and Circuit Simulation,” in 2014 IEEE International Electron Devices Meeting (IEDM), 2014, pp. 35.6.1–35.6.4. doi: 10.1109/IEDM.2014.7047163.

  • [184]  S. Zhang and Z. Li, “Roles of Nonequilibrium Conduction Electrons on the Magnetization Dynamics of Ferromagnets,” Physical Review Letters, vol. 93, p. 127204, 2004. doi: 10.1103/PhysRevLett.93.127204.

  • [185]  M. Wang, W. Cai, K. Cao, J. Zhou, J. Wrona et al., “Current-induced magnetization switching in atom-thick tungsten engineered perpendicular magnetic tunnel junctions with large tunnel magnetoresistance,” Nature Communications, vol. 9, p. 671, 2018. doi: 10.1038/s41467-018-03140-z.

  • [186]  M. Wang, “Tunnel Junction with Perpendicular Magnetic Anisotropy: Status and Challenges,” Micromachines, vol. 6, no. 8, pp. 1023–1045, 2015. doi: 10.3390/mi6081023.

  • [187]  J. M. Iwata-Harms et al., “Ultrathin perpendicular magnetic anisotropy CoFeB free layers for highly efficient, high speed writing in spin-transfer-torque MRAM,” Scientific Reports, vol. 9, p. 18668, 2019. doi: 10.1038/s41598-019-54466-7.

  • [188]  M. Bendra, S. Fiorentini, J. Ender, R. L. de Orio, T. Hadámek et al., “Back-Hopping in Ultra-Scaled MRAM Cells,” in 2023 46th MIPRO ICT and Electronics Convention (MIPRO), 2023. doi: 10.23919/MIPRO57284.2023.10159788.

  • [189]  K. Watanabe, B. Jinnai, S. Ukami, H. Sato, and H. Ohno, “Shape Anisotropy Revisited in Single-Digit Nanometer Magnetic Tunnel Junctions,” Nature Communications, vol. 9, p. 663, 2018. doi: 10.1038/s41467-018-03003-7.

  • [190]  B. Jinnai, J. Igarashi, K. Watanabe, T. Funatsu, H. Sato et al., “High-Performance Shape-Anisotropy Magnetic Tunnel Junctions Down to 2.3 nm,” in IEEE International Electron Devices Meeting (IEDM), 2020, pp. 24.6.1–24.6.4. doi: 10.1109/IEDM13553.2020.9371972.

  • [191]  K. Nishioka, H. Honjo, S. Ikeda, T. Watanabe, S. Miura et al., “Novel Quad Interface MTJ Technology and its First Demonstration with High Thermal Stability and Switching Efficiency for STT-MRAM Beyond 2Xnm,” in Symposium on VLSI Technology, 2019, pp. T120–T121. doi: 10.23919/VLSIT.2019.8776499.

  • [192]  K. Nishioka, H. Honjo, H. Naganuma, T. V. A. Nguyen, M. Yasuhira et al., “Enhancement of Magnetic Coupling and Magnetic Anisotropy in MTJs with Multiple CoFeB/MgO Interfaces for High Thermal Stability,” AIP Advances, vol. 11, no. 2, p. 025231, 2021. doi: 10.1063/9.0000048.

  • [193]  M. Bendra, R. L. de Orio, S. Selberherr, W. Goes, and V. Sverdlov, “A Multi-Level Cell for Ultra-Scaled STT-MRAM Realized by Back-Hopping,” Solid-State Electronics, 2023. doi: 10.1016/j.sse.2023.108770.

  • [194]  M. Bendra, R. L. de Orio, S. Selberherr, W. Goes, and V. Sverdlov, “A Multi-Level Cell for Ultra-Scaled STT-MRAM Realized by Back-Hopping,” Solid-State Electronics, vol. 212, p. 108830, 2024. doi: 10.1016/j.sse.2023.108830. Extended version with Set B material parameters.

  • [195]  T. Devolder, O. Bultynck, P. Bouquin, V. D. Nguyen, S. Rao et al., “Back Hopping in Spin Transfer Torque Switching of Perpendicularly Magnetized Tunnel Junctions,” Physical Review B, vol. 102, p. 184406, 2020. doi: 10.1103/PhysRevB.102.184406.

  • [196]  R. Phoomatna, S. Sampan-a pai, A. Meo, R. W. Chantrell, J. Chureemart et al., “Dimensional Scaling Effects on Critical Current Density and Magnetization Switching in CoFeB-Based Magnetic Tunnel Junction,” Journal of Physics D: Applied Physics, vol. 57, no. 18, p. 185002, 2024. doi: 10.1088/1361-6463/ad1e53.

  • [197]  L. Farcis, B. M. S. Teixeira, P. Talatchian, D. Salomoni, U. Ebels, S. Auffret, B. Dieny, F. A. Mizrahi, J. Grollier, R. C. Sousa, and L. D. Buda-Prejbeanu, “Spiking Dynamics in Dual Free Layer Perpendicular Magnetic Tunnel Junctions,” Nano Letters, vol. 23, no. 17, pp. 7869–7875, 2023. doi: 10.1021/acs.nanolett.3c01597.

  • [198]  R. Matsumoto, S. Lequeux, H. Imamura, and J. Grollier, “Chaos and Relaxation Oscillations in Spin-Torque Windmill Spiking Oscillators,” Phys. Rev. Appl., vol. 11, p. 044093, 2019. doi: 10.1103/PhysRevApplied.11.044093.

  • [199]  M. Bendra, N. P. Jørstad, R. L. de Orio, S. Selberherr, W. Goes, and V. Sverdlov, “Unified Modeling of Ultra-Scaled STT-MRAM Cells: Harnessing Parasitic Effects for Enhanced Data Storage Dynamics,” in 2023 IEEE International Electron Devices Meeting (IEDM), 2023.

  • [200]  M. Bendra, S. Fiorentini, S. Selberherr, W. Goes, and V. Sverdlov, “Simulation of Spin-Torque and Magnetization Dynamics in STT-MRAM Multi-Level Cells,” in International Symposium on Hysteresis Modeling and Micromagnetics (HMM), 2023.

  • [201]  C. Abert, H. Sepehri-Amin, F. Bruckner, C. Vogler, M. Hayashi et al., “Back-Hopping in Spin-Transfer-Torque Devices: Possible Origin and Countermeasures,” Physical Review Applied, vol. 9, p. 054010, 2018. doi: 10.1103/PhysRevApplied.9.054010.

  • [202]  P. Bruno, “Theory of Interlayer Exchange Interactions in Magnetic Multilayers,” Journal of Physics: Condensed Matter, vol. 11, no. 48, 1999. doi: 10.1088/0953-8984/11/48/305.

  • [203]  M. Bendra, R. L. de Orio, S. Selberherr, W. Goes, and V. Sverdlov, “Influence of Interface Exchange Coupling in Multilayered Spintronic Structures,” in 2024 47th MIPRO ICT and Electronics Convention (MIPRO), 2024, pp. 1579–1583. doi: 10.1109/MIPRO60963.2024.10569798.

  • [204]  T. Katayama, S. Yuasa, J. Velev, M. Y. Zhuravlev, S. S. Jaswal et al., “Interlayer Exchange Coupling in Fe/MgO/Fe Magnetic Tunnel Junctions,” Applied Physics Letters, vol. 89, no. 11, p. 112503, 2006. doi: 10.1063/1.2349321.

  • [205]  Y.-C. Weng, C.-W. Cheng, and G. Chern, “Interlayer Exchange Coupling and Perpendicular Magnetic Anisotropy in Co\(_{40}\)Fe\(_{40}\)B\(_{20}\)/MgO/Co\(_{20}\)Fe\(_{60}\)B\(_{20}\) Tunnel Junction Structures,” IEEE Transactions on Magnetics, vol. 49, pp. 4425–4428, 07 2013. doi: 10.1109/TMAG.2013.2245308.

  • [206]  B. Khodadadi, J. B. Mohammadi, J. M. Jones, A. Srivastava, C. Mewes, T. Mewes, and C. Kaiser, “Interlayer Exchange Coupling in Asymmetric \(\mathrm {Co}\text {\ensuremath {-}}\mathrm {Fe}\slash \mathrm {Ru}\slash \mathrm {Co}\text {\ensuremath {-}}\mathrm {Fe}\) Trilayers Investigated with Broadband Temperature-Dependent Ferromagnetic Resonance,” Phys. Rev. Appl., vol. 8, p. 014024, Jul 2017. doi: 10.1103/PhysRevApplied.8.014024.

  • [207]  A. Mouhoub, F. Millo, C. Chappert, J.-V. Kim, J. Létang, A. Solignac, and T. Devolder, “Exchange Energies in CoFeB/Ru/CoFeB Synthetic Antiferromagnets,” Phys. Rev. Mater., vol. 7, p. 044404, Apr 2023. doi: 10.1103/PhysRevMaterials.7.044404.

  • [208]  M. Bendra, R. L. de Orio, S. Selberherr, W. Goes, and V. Sverdlov, “Interlayer Exchange Coupling for Enhanced Performance in Spin-Transfer Torque MRAM Devices,” Solid-State Electronics, vol. 229, p. 109179, 2025. doi: 10.1016/j.sse.2025.109179.

  • [209]  A. Manchon, S. Zhang, and K.-J. Lee, “Signatures of Asymmetric and Inelastic Tunneling on the Spin Torque Bias Dependence,” Phys. Rev. B, vol. 82, p. 174420, 2010. doi: 10.1103/PhysRevB.82.174420.

  • [210]  S.-C. Oh, S.-Y. Park, A. Manchon, M. Chshiev, J.-H. Han et al., “Bias-Voltage Dependence of Perpendicular Spin-Transfer Torque in Asymmetric MgO-Based Magnetic Tunnel Junctions,” Nature Physics, vol. 5, no. 12, pp. 898–902, 2009. doi: 10.1038/nphys1427.

  • [211]  T. Warnatz, B. E. Skovdal, F. Magnus, H. Stopfel, D. Primetzhofer, A. Stein, R. Brucas, and B. Hjörvarsson, “The Influence of Diameter on the magnetic Saturation in Fe\(_{84}\)Cu\(_{16}\)/MgO [001] multilayered islands,” Journal of Magnetism and Magnetic Materials, vol. 496, p. 165864, 2020. doi: https://doi.org/10.1016/j.jmmm.2019.165864.

  • [212]  S. Bin Hamid, R. Dutta, O. Hassan, and M. Z. Baten, “Implementing Bidirectional Logic with Backhopping in Magnetic Tunnel Junctions,” AIP Advances, vol. 14, no. 2, p. 025224, 02 2024. doi: 10.1063/5.0169751.

  • [213]  T. Devolder, J.-V. Kim, F. Garcia-Sanchez, J. Swerts, W. Kim, S. Couet, G. Kar, and A. Furnemont, “Time-Resolved Spin-Torque Switching in MgO-Based Perpendicularly Magnetized Tunnel Junctions,” Phys. Rev. B, vol. 93, p. 024420, Jan 2016. doi: 10.1103/PhysRevB.93.024420.

  • [214]  A. Le Goff, K. Garcia, N. Vernier, T. Tahmasebi, S. Cornelissen, T. Min, and T. Devolder, “Effect of Ta Insertion in Reference Layers of MTJs With Perpendicular Anisotropy,” IEEE Transactions on Magnetics, vol. 50, no. 11, pp. 1–4, 2014. doi: 10.1109/TMAG.2014.2328664.

  • [215]  M. Bendra, R. L. de Orio, W. Goes, S. Selberherr, and V. Sverdlov, “Investigating Reliability Issues in Multi-Layered STT-MRAM with Synthetic Antiferromagnets,” in 2024 IEEE International Symposium on the Physical and Failure Analysis of Integrated Circuits (IPFA), 2024, pp. 1–5. doi: 10.1109/IPFA61654.2024.10690971.

  • [216]  M. Bendra, W. Goes, S. Selberherr, and V. Sverdlov, “Simulation of SAF-enhanced multilayered STT-MRAM structures,” Microelectronic Engineering, vol. 302, p. 112426, 2026. doi: 10.1016/j.mee.2025.112426.

  • [217]  M. Bendra, S. Selberherr, W. Goes, and V. Sverdlov, “Enhancing Sub-Nanosecond Magnetic Tunnel Junctions with Double Spin Torque and Synthetic Antiferromagnetic Layers,” in International Symposium on Hysteresis Modeling and Micromagnetics (HMM), 2025.

  • [218]  M. Bendra, B. Pruckner, R. L. de Orio, S. Selberherr, W. Goes et al., “Advancing Nonvolatile Memory Technologies: Enhancing Reliability and Performance through Double Spin Torque Magnetic Tunnel Junctions and Interlayer Exchange Coupling,” in 2024 Device Research Conference (DRC), 2024, pp. 1–2. doi: 10.1109/DRC61706.2024.10605512.

  • [219]  B. Pruckner, S. Fiorentini, W. Goes, S. Selberherr, and V. Sverdlov, “Micromagnetic Modeling of Double Spin-Torque Magnetic Tunnel Junction Devices,” Physica B: Condensed Matter, vol. 688, p. 416124, 2024. doi: 10.1016/j.physb.2024.416124.

  • [220]  J. Chen, S. Peng, D. Xiong, H. Cheng, H. Zhou et al., “Correlation of Interfacial Perpendicular Magnetic Anisotropy and Interlayer Exchange Coupling in CoFe/W/CoFe Structures,” Journal of Physics D: Applied Physics, vol. 53, no. 33, p. 334001, 2020. doi: 10.1088/1361-6463/ab8bfe.

List of Publications

Journal Articles

  • [1]  M. Bendra, W. Goes, S. Selberherr, and V. Sverdlov, “Simulation of SAF-Enhanced Multilayered STT-MRAM Structures,” Microelectronic Engineering, vol. 302, p. 112426, 2026. doi: 10.1016/j.mee.2025.112426.

  • [2]  M. Bendra, de Orio, Roberto Lacerda, S. Selberherr, W. Goes, and V. Sverdlov, “Interlayer Exchange Coupling for Enhanced Performance in Spin-Transfer Torque MRAM Devices,” Solid-State Electronics, vol. 229, p. 109179, 2025. doi: 10.1016/j.sse.2025.109179.

  • [3]  M. Bendra, de Orio, Roberto Lacerda, S. Selberherr, W. Goes, and V. Sverdlov, “A Multi-Level Cell for Ultra-Scaled STT-MRAM Realized by Back-Hopping,” Solid-State Electronics, vol. 223, p. 109027, 2025. doi: 10.1016/j.sse.2024.109027. Invited.

  • [4]  M. Bendra, de Orio, Roberto Lacerda, S. Selberherr, W. Goes, and V. Sverdlov, “Advanced Modeling and Simulation of Multilayer Spin-Transfer Torque Magnetoresistive Random Access Memory with Interface Exchange Coupling,” Micromachines, vol. 15, no. 5, 2024. doi: 10.3390/mi15050568. Invited.

  • [5]  M. Bendra, de Orio, Roberto Lacerda, S. Selberherr, W. Goes, and V. Sverdlov, “A Multi-Level Cell for Ultra-Scaled STT-MRAM Realized by Back-Hopping,” Solid-State Electronics, vol. 208, p. 108738, 2023. doi: 10.1016/j.sse.2023.108738.

  • [6]  S. Fiorentini, N. P. Jørstad, J. Ender, de Orio, Roberto Lacerda, S. Selberherr, M. Bendra, W. Goes, and V. Sverdlov, “Finite Element Approach for the Simulation of Modern MRAM Devices,” Micromachines, vol. 14, no. 5, 2023. doi: 10.3390/mi14050898. Invited.

  • [7]  M. Bendra, S. Fiorentini, W. Goes, S. Selberherr, and V. Sverdlov, “The Influence of Interface Effects on the Switching Behavior in Ultra-Scaled MRAM Cells,” Solid-State Electronics, vol. 201, p. 108590, 2023. doi: 10.1016/j.sse.2023.108590. Invited.

  • [8]  M. Bendra, S. Fiorentini, W. Goes, S. Selberherr, and V. Sverdlov, “Interface Effects in Ultra-Scaled MRAM Cells,” Solid-State Electronics, vol. 194, p. 108373, 2022. doi: 10.1016/j.sse.2022.108373.

  • [9]  T. Hadámek, S. Fiorentini, M. Bendra, J. Ender, de Orio, Roberto Lacerda, W. Goes, S. Selberherr, and V. Sverdlov, “Temperature Increase in STT-MRAM at Writing: A Fully Three-Dimensional Finite Element Approach,” Solid-State Electronics, vol. 193, p. 108269, 2022. doi: 10.1016/j.sse.2022.108269. Invited.

  • [10]  S. Fiorentini, M. Bendra, J. Ender, de Orio, Roberto Lacerda, T. Hadámek, W. Goes, S. Selberherr, and V. Sverdlov, “Spin and Charge Drift-Diffusion in Ultra-Scaled MRAM Cells,” Scientific Reports, vol. 12, p. 20958, 2022. doi: 10.1038/s41598-022-25586-4.

  • [11]  J. Ender, S. Fiorentini, de Orio, Roberto Lacerda, T. Hadámek, M. Bendra, W. Goes, S. Selberherr, and V. Sverdlov, “Advances in Modeling Emerging Magnetoresistive Random Access Memories: From Finite Element Methods to Machine Learning Approaches,” Proceedings of SPIE, vol. 12157, pp. 1 215 708–1–1 215 708–14, 2022. doi: 10.1117/12.2624595. Invited.

Conference Contributions

  • [12]  V. Sverdlov, N. P. Jørstad, B. Pruckner, M. Bendra, W. Goes, and S. Selberherr, “Emerging Magnetoresistive Memories,” in 2025 IEEE 16th International Conference on ASIC (ASICON), Kunming, China, 2025, pp. 1–4. doi: 10.1109/ASICON66040.2025.11326380.

  • [13]  V. Sverdlov, B. Pruckner, N. P. Jørstad, M. Bendra, S. Selberherr, and W. Goes, “Modeling Advanced Magnetoresistive Memories,” in 2025 IEEE European Solid-State Electronics Research Conference (ESSERC), Munich, Germany, 2025, pp. 365–368. doi: 10.1109/ESSERC66193.2025.11214099.

  • [14]  M. Bendra, S. Selberherr, W. Goes, and V. Sverdlov, “Enhancing Sub-Nanosecond Magnetic Tunnel Junctions with Double Spin Torque and Synthetic Antiferromagnetic Layers,” in International Symposium on Hysteresis Modeling and Micromagnetics (HMM), 2025.

  • [15]  M. Bendra, de Orio, Roberto Lacerda, S. Selberherr, W. Goes, and V. Sverdlov, “Influence of Interface Exchange Coupling in Multilayered Spintronic Structures,” in 2024 47th MIPRO ICT and Electronics Convention (MIPRO), 2024, pp. 1579–1583. doi: 10.1109/MIPRO60963.2024.10569798.

  • [16]  M. Bendra, B. Pruckner, de Orio, Roberto Lacerda, S. Selberherr, W. Goes, and V. Sverdlov, “Advancing Nonvolatile Memory Technologies: Enhancing Reliability and Performance through Double Spin Torque Magnetic Tunnel Junctions and Interlayer Exchange Coupling,” in 2024 Device Research Conference (DRC), 2024, pp. 1–2. doi: 10.1109/DRC61706.2024.10605512.

  • [17]  M. Bendra, W. Goes, S. Selberherr, and V. Sverdlov, “Simulation of SAF-Enhanced Multilayered STT-MRAM Structures,” in 2024 Austrochip Workshop on Microelectronics (Austrochip), 2024, pp. 1–4. doi: 10.1109/Austrochip62761.2024.10716241.

  • [18]  M. Bendra, de Orio, Roberto Lacerda, W. Goes, S. Selberherr, and V. Sverdlov, “Investigating Reliability Issues in Multi-Layered STT-MRAM with Synthetic Antiferromagnets,” in 2024 IEEE International Symposium on the Physical and Failure Analysis of Integrated Circuits (IPFA), 2024, pp. 1–5. doi: 10.1109/IPFA61654.2024.10690971.

  • [19]  B. Pruckner, N. P. Jørstad, M. Bendra, T. Hadámek, W. Goes, S. Selberherr, and V. Sverdlov, “Simulation of Advanced MRAM Devices for Sub-ns Switching,” in 2024 International Conference on Simulation of Semiconductor Processes and Devices (SISPAD), 2024, pp. 1–4. doi: 10.1109/SISPAD62626.2024.10733317.

  • [20]  M. Bendra, S. Fiorentini, J. Ender, de Orio, Roberto Lacerda, T. Hadámek, N. P. Jørstad, B. Pruckner, S. Selberherr, W. Goes, and V. Sverdlov, “Back-Hopping in Ultra-Scaled MRAM Cells,” in 46th MIPRO ICT and Electronics Convention (MIPRO), 2023, pp. 159–162. doi: 10.23919/MIPRO57284.2023.10159764.

  • [21]  M. Bendra, S. Fiorentini, S. Selberherr, W. Goes, and V. Sverdlov, “A Multi-Level Cell for Ultra-Scaled STT-MRAM Realized by Back-Hopping,” in 9th Joint International EuroSOI Workshop and International Conference on Ultimate Integration on Silicon (EuroSOI-ULIS), Tarragona, Spain, 2023.

  • [22]  M. Bendra, S. Fiorentini, S. Selberherr, W. Goes, and V. Sverdlov, “Simulation of Spin-Torque and Magnetization Dynamics in STT-MRAM Multi-Level Cells,” in International Symposium on Hysteresis Modeling and Micromagnetics (HMM), 2023.

  • [23]  M. Bendra, de Orio, Roberto Lacerda, W. Goes, V. Sverdlov, and S. Selberherr, “Modeling of Ultra-Scaled Magnetoresistive Random Access Memory,” in International Conference on Microelectronic Devices and Technologies (MicDAT), Funchal, Portugal, 2023, pp. 28–30. ISBN 978-84-09-53748-8

  • [24]  S. Fiorentini, de Orio, Roberto Lacerda, J. Ender, S. Selberherr, M. Bendra, N. P. Jørstad, W. Goes, and V. Sverdlov, “Finite Element Method for MRAM Switching Simulations,” in Proc. of the International Conference on Mathematical Models, Computational Techniques in Science, and Engineering (MMCTSE), Athens, Greece, 2023, invited.

  • [25]  N. P. Jørstad, T. Hadámek, M. Bendra, J. Ender, B. Pruckner, W. Goes, and V. Sverdlov, “Numerical Simulations of Spintronic Magnetoresistive Memories,” in Silvaco Users Global Event (SURGE), Santa Clara, USA, 2023, invited.

  • [26]  V. Sverdlov, S. Fiorentini, M. Bendra, J. Ender, de Orio, Roberto Lacerda, T. Hadámek, N. P. Jørstad, W. Goes, and S. Selberherr, “Comprehensive Modeling of Nanoscale Magnetoresistive Memory,” in 3rd Global Experts Conference on Materials Science & Nanotechnology (GECMSN23), Dubai, UAE, 2023, invited.

  • [27]  V. Sverdlov, M. Bendra, W. Goes, S. Fiorentini, A. Garcia-Barrientos, and S. Selberherr, “Multi-Level Operation in Ultra-Scaled MRAM,” in IEEE Latin American Electron Devices Conference (LAEDC), 2023, pp. 1–4. doi: 10.1109/LAEDC58183.2023.10209117.

  • [28]  V. Sverdlov, M. Bendra, B. Pruckner, S. Fiorentini, W. Goes, and S. Selberherr, “Comprehensive Modeling of Advanced Composite Magnetoresistive Devices,” in IEEE 53rd European Solid-State Device Research Conference (ESSDERC), 2023, pp. 93–96. doi: 10.1109/ESSDERC59256.2023.10268508.

  • [29]  M. Bendra, S. Fiorentini, J. Ender, de Orio, Roberto Lacerda, T. Hadámek, W. J. Loch, N. P. Jørstad, S. Selberherr, W. Goes, and V. Sverdlov, “Spin Transfer Torques in Ultra-Scaled MRAM Cells,” in 45th Jubilee International Convention on Information, Communication and Electronic Technology (MIPRO), 2022, pp. 129–132. doi: 10.23919/MIPRO55190.2022.9803736.

  • [30]  M. Bendra, S. Fiorentini, J. Ender, de Orio, Roberto Lacerda, T. Hadámek, W. J. Loch, N. P. Jørstad, W. Goes, S. Selberherr, and V. Sverdlov, “Interface Effects in Ultra-Scaled MRAM Cells,” in 8th Joint International EuroSOI Workshop and International Conference on Ultimate Integration on Silicon (EuroSOI-ULIS), Udine, Italy, 2022, pp. 1–2.

  • [31]  M. Bendra, W. J. Loch, N. P. Jørstad, S. Fiorentini, S. Selberherr, W. Goes, and V. Sverdlov, “Modeling Ultra-Scaled Multi-Layer STT-MRAM Cells: A Unified Spin and Charge Drift-Diffusion Approach,” in 2022 IEEE International Electron Devices Meeting (IEDM), 2022, poster.

  • [32]  S. Fiorentini, M. Bendra, J. Ender, W. Goes, V. Sverdlov, and S. Selberherr, “Evaluating Spin Transfer Torques in Multilayered Magnetic Tunnel Junctions and Spin Valves,” in Workshop on Innovative Nanoscale Devices and Systems (WINDS), Lihue, HI, USA, 2022.

  • [33]  S. Fiorentini, M. Bendra, J. Ender, T. Hadámek, W. J. Loch, N. P. Jørstad, de Orio, Roberto Lacerda, W. Goes, S. Selberherr, and V. Sverdlov, “Modeling Advanced Spintronic-Based Magnetoresistive Memory,” in International Conference on Microwave & THz Technologies, Wireless Communications and OptoElectronics (IRPhE 2022), 2022, pp. 49–52. doi: 10.1049/icp.2022.2795.

  • [34]  S. Fiorentini, M. Bendra, J. Ender, de Orio, Roberto Lacerda, T. Hadámek, W. J. Loch, N. P. Jørstad, W. Goes, S. Selberherr, and V. Sverdlov, “Spin Torques in ULTRA-Scaled MRAM Devices,” in IEEE 52nd European Solid-State Device Research Conference (ESSDERC), 2022, pp. 348–351. doi: 10.1109/ESSDERC55479.2022.9947196.

  • [35]  S. Fiorentini, W. J. Loch, M. Bendra, N. P. Jørstad, J. Ender, de Orio, Roberto Lacerda, T. Hadámek, W. Goes, V. Sverdlov, and S. Selberherr, “Design Analysis of Ultra-Scaled MRAM Cells,” in IEEE 16th International Conference on Solid-State & Integrated Circuit Technology (ICSICT), 2022, pp. 1–4. doi: 10.1109/ICSICT55466.2022.9963202.

  • [36]  T. Hadámek, M. Bendra, S. Fiorentini, J. Ender, de Orio, Roberto Lacerda, W. Goes, S. Selberherr, and V. Sverdlov, “Temperature Increase in MRAM at Writing: A Finite Element Approach,” in 7th Joint International EuroSOI Workshop and International Conference on Ultimate Integration on Silicon (EuroSOI-ULIS), 2021, pp. 1–4. doi: 10.1109/EuroSOI-ULIS53016.2021.9560669.

  • [37]  M. Bendra, J. Ender, S. Fiorentini, T. Hadámek, de Orio, Roberto Lacerda, W. Goes, V. Sverdlov, and S. Selberherr, “Finite Element Method Approach to MRAM Modeling,” in 44th International Convention on Information, Communication and Electronic Technology (MIPRO), 2021, pp. 70–73. doi: 10.23919/MIPRO52101.2021.9597194.

  • [38]  J. Ender, S. Fiorentini, de Orio, Roberto Lacerda, T. Hadámek, M. Bendra, W. Goes, S. Selberherr, and V. Sverdlov, “Advanced Modeling of Emerging MRAM: From Finite Element Methods to Machine Learning Approaches,” in Proc. of the International Conference Micro-and Nanoelectronics (ICMNE), 2021.

  • [39]  V. Sverdlov, M. Bendra, S. Fiorentini, J. Ender, de Orio, Roberto Lacerda, T. Hadámek, W. J. Loch, N. P. Jørstad, W. Goes, and S. Selberherr, “Advanced Modeling of Emerging Devices for Digital Spintronics,” in Proc. of the International Conference on Nanoscience and Nanotechnology, Dubai, UAE, 2022, invited.

  • [40]  V. Sverdlov, M. Bendra, S. Fiorentini, J. Ender, de Orio, Roberto Lacerda, T. Hadámek, W. J. Loch, N. P. Jørstad, W. Goes, and S. Selberherr, “Advanced Modeling of Emerging Magnetoresistive Memory,” in Proc. of the International Meet & Expo on Nanotechnology (NANOMEET), Edinburgh, UK, 2022, invited.

  • [41]  V. Sverdlov, M. Bendra, S. Fiorentini, J. Ender, de Orio, Roberto Lacerda, T. Hadámek, W. J. Loch, N. P. Jørstad, W. Goes, and S. Selberherr, “Emerging Devices for Digital Spintronics,” in 2nd Global Conference & Expo on Nanotechnology & Nanoscience, 2022, pp. 32–33, invited.

  • [42]  V. Sverdlov, M. Bendra, S. Fiorentini, J. Ender, de Orio, Roberto Lacerda, T. Hadámek, W. J. Loch, N. P. Jørstad, W. Goes, and S. Selberherr, “Modeling Advanced Magnetoresistive Memory: A Journey from Finite Element Methods to Machine Learning Approaches,” in 2nd Global Webinar on Nanoscience & Nanotechnology, 2022, invited.

  • [43]  V. Sverdlov, W. J. Loch, M. Bendra, S. Fiorentini, J. Ender, de Orio, Roberto Lacerda, T. Hadámek, N. P. Jørstad, W. Goes, and S. Selberherr, “Modeling Approach to Ultra-Scaled MRAM Cells,” in Book of Abstracts of the International Meet on Applied Science, Engineering and Technology (ASETMEET), 2022, pp. 7–8, invited.

  • [44]  W. J. Loch, S. Fiorentini, N. P. Jørstad, J. Ender, de Orio, Roberto Lacerda, T. Hadámek, M. Bendra, W. Goes, S. Selberherr, and V. Sverdlov, “Double Reference Layer STT-MRAM Structures with Improved Performance,” in 8th Joint International EuroSOI Workshop and International Conference on Ultimate Integration on Silicon (EuroSOI-ULIS), Udine, Italy, 2022, pp. 1–2.

  • [45]  N. P. Jørstad, S. Fiorentini, J. Ender, de Orio, Roberto Lacerda, T. Hadámek, W. J. Loch, M. Bendra, W. Goes, S. Selberherr, and V. Sverdlov, “Finite Element Modeling of Spin-Orbit Torques,” in Proc. of the 8th Joint International EuroSOI Workshop and International Conference on Ultimate Integration on Silicon (EuroSOI-ULIS), Udine, Italy, 2022.