Ferroelectric AlScN and HfZrO Domain Switching Dynamics.

Roberto Guido, Xuetao Wang, Bohan Xu, Ruben Alcala, Thomas Mikolajick, Uwe Schroeder, Patrick D Lomenzo
Author Information
  1. Roberto Guido: NaMLab gGmbH, Noethnitzer Strasse 64a, 01187 Dresden, Germany. ORCID
  2. Xuetao Wang: NaMLab gGmbH, Noethnitzer Strasse 64a, 01187 Dresden, Germany. ORCID
  3. Bohan Xu: NaMLab gGmbH, Noethnitzer Strasse 64a, 01187 Dresden, Germany. ORCID
  4. Ruben Alcala: NaMLab gGmbH, Noethnitzer Strasse 64a, 01187 Dresden, Germany.
  5. Thomas Mikolajick: NaMLab gGmbH, Noethnitzer Strasse 64a, 01187 Dresden, Germany. ORCID
  6. Uwe Schroeder: NaMLab gGmbH, Noethnitzer Strasse 64a, 01187 Dresden, Germany. ORCID
  7. Patrick D Lomenzo: NaMLab gGmbH, Noethnitzer Strasse 64a, 01187 Dresden, Germany. ORCID

Abstract

The capability to reliably program partial polarization states with nanosecond programming speed and femtojoule energies per bit in ferroelectrics makes them an ideal candidate to realize multibit memory elements for high-density crossbar arrays, which could enable neural network models with a large number of parameters at the edge. However, a thorough understanding of the domain switching dynamics involved in the polarization reversal is required to achieve full control of the multibit capability. Transient current integration measurements are adopted to investigate the domain dynamics in aluminum scandium nitride (AlScN) and hafnium zirconium oxide (HfZrO). The switching dynamics are correlated to the crystal structure of the films. The contributions of domain nucleation and domain wall motion are decoupled by analyzing the rate of change of the time-dependent normalized switched polarization. Thermally activated creep domain wall motion characterizes the AlScN switching dynamics. The statistics of independently nucleating domains and the domain wall creep motion in HfZrO are associated with the spatially inhomogeneous distribution of local switching field due to polymorphism, absence of preferential crystallite orientation, as well as defects and charges that can be located at the grain boundaries. The -axis texture, single-phase nature, and strong likelihood of less fabrication process-induced defects contribute to the homogeneity of the local switching field in AlScN. Nonetheless, defects generated and redistributed upon bipolar electric field switching cycling result in AlScN domain wall pinning. The wake-up effect in HfZrO is explained thorough the continuous addition of switchable regions associated with two independent distributions of characteristic switching times.

Keywords

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Created with Highcharts 10.0.0domainswitchingAlScNwalldynamicsHfZrOmotionpolarizationfielddefectscapabilityferroelectricsmultibitthoroughaluminumscandiumnitridehafniumzirconiumoxidenucleationcreepassociatedlocalreliablyprogrampartialstatesnanosecondprogrammingspeedfemtojouleenergiesperbitmakesidealcandidaterealizememoryelementshigh-densitycrossbararraysenableneuralnetworkmodelslargenumberparametersedgeHoweverunderstandinginvolvedreversalrequiredachievefullcontrolTransientcurrentintegrationmeasurementsadoptedinvestigatecorrelatedcrystalstructurefilmscontributionsdecoupledanalyzingratechangetime-dependentnormalizedswitchedThermallyactivatedcharacterizesstatisticsindependentlynucleatingdomainsspatiallyinhomogeneousdistributionduepolymorphismabsencepreferentialcrystalliteorientationwellchargescanlocatedgrainboundaries-axistexturesingle-phasenaturestronglikelihoodlessfabricationprocess-inducedcontributehomogeneityNonethelessgeneratedredistributeduponbipolarelectriccyclingresultpinningwake-upeffectexplainedcontinuousadditionswitchableregionstwoindependentdistributionscharacteristictimesFerroelectricDomainSwitchingDynamicskinetics

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