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Electrical characterization of resistive switching memories and development of automated scalpel-SPM methodologies

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dc.contributor.author Drilakis, Christos en
dc.contributor.author Δριλάκης, Χρήστος el
dc.date.accessioned 2021-01-08T07:48:50Z
dc.date.available 2021-01-08T07:48:50Z
dc.identifier.uri https://dspace.lib.ntua.gr/xmlui/handle/123456789/52741
dc.identifier.uri http://dx.doi.org/10.26240/heal.ntua.20439
dc.description Εθνικό Μετσόβιο Πολυτεχνείο--Μεταπτυχιακή Εργασία. Διεπιστημονικό-Διατμηματικό Πρόγραμμα Μεταπτυχιακών Σπουδών (Δ.Π.Μ.Σ.) “Μικροσυστήματα και Νανοδιατάξεις” el
dc.rights Default License
dc.subject Resistive switching memories en
dc.subject Titanium oxide en
dc.subject Nanoparticles en
dc.subject Conductive filament observation en
dc.subject AFM en
dc.subject Μνήμες εναλλαγής αντίστασης el
dc.subject Οξείδιο του τιτανίου el
dc.subject Νανοσωματίδια el
dc.subject Απεικόνιση αγώγιμου δρόμου el
dc.subject Μικροσκόπιο ατομικής δύναμης el
dc.title Electrical characterization of resistive switching memories and development of automated scalpel-SPM methodologies en
heal.type masterThesis
heal.secondaryTitle Χαρακτηρισμός διατάξεων εναλλαγής αντίστασης και ανάπτυξη αυτοματοποιημένου συστήματος el
heal.classification Physics en
heal.classification Φυσική el
heal.language en
heal.access campus
heal.recordProvider ntua el
heal.publicationDate 2020-11-04
heal.abstract Filamentary-based resistive switching memories represent an intriguing class of emerging electronic devices. They rely on ion migration in order to create or dissolve nanoscale conductive filaments (CF) within insulating materials. Depending on the formation or rupture of the CF, the device switches its resistance state and stores a logical bit. The characterization and understanding of these devices have been a challenge for the scientific community for many years. Conductive Atomic Force Microscopy (C-AFM) is a powerful technique that enables the physical and electrical characterization of any type of surface, including thin films for resistive switching memories applications. Particularly, a recently advanced technique called SPM tomography or Scalpel SPM provides depth profiling by tip-induced material removal, while also probing the local conductivity. This can generate multiple planar conductive maps of a resistive memory cell that can be used for a 3D tomogram production. In this work, we studied Valence Change Memories that can be used as nonvolatile storage class devices. Specifically, our devices were based on a MIM structure (Metal-Insulator-Metal) with Au and Ti as top electrodes, a sub-stoichiometric titanium oxide bilayer configuration as the active switching layer and Au as bottom electrode. We tested two kinds of devices, the reference sample and an identical one with embedded Pt nanoparticles (NPs) in the middle of the resistive layer. The NPs incorporation provided enhanced performance in terms of memory window and DC endurance over consecutive cycles as well as wider CF, mainly due to enhancement of the electric field in the vicinity of the NPs during the set process. The reference sample had a memory window of 102 and the NPs sample had 103. Moreover, the NPs sample maintained the same memory window for 10 DC consecutive cycles, whereas the reference sample window started degrading immediately after the first cycle. Moreover, we utilized the Scalpel-SPM technique in order to perform a 3D imaging of the CF for our two devices. After unsuccessful attempts on removing the top electrode (TE), we used a Pt tip directly in the oxide region as a TE to set the device in the ON state. Afterwards, we were able to produce a 3D tomogram of the CF for the two samples. The CF in the reference sample showed a relatively constant size, whereas in the nanoparticles-embedded sample it resembled a cone. The larger size of the filament in the NPs vicinity is related to enhanced oxygen vacancy generation probability during the set process. Additionally, we observed a more localized and standard-shaped filament in the NPs sample than the one in the reference sample which was randomly shaped and positioned, indicating the imposition of the CF formation/rupture into specific locations by the NPs. The maximum current for the CF and another conductive spot in the current map disclosed similar values in the second oxide layer, indicating that the resistive switching process takes place mostly in the first layer. The area calculation for the CF showed a conical shape for both samples, with the NPs-embedded sample filament size increasing in a faster rate as a function of the depth. The CF in both cases is smaller close to the surface and bigger in the bottom, caused by the accumulation of oxygen anions in the surface (less oxygen vacancies) during the set process. The theoretical resistance of the filament showed similar evolution with the corresponding experimental one during scalpeling, while having significant value difference, mostly due to high tip-sample contact resistance. Finally, we provide insights regarding the difficulty of analyzing a Scalpel SPM dataset which consists of numerus images and requires a lot of processing time. This effect lead to the development of automated routine, by creating scripts in Python that could speed up the editing of our experiments. For that reason, we created algorithms that could automate many steps of a Scalpel-SPM analysis, like the leveling of read-out images, depth and removal rate calculation and current map auto scale setting. In that way, we can have a complete and rapid understanding of our experiments result. en
heal.advisorName Tsoukalas, Dimitris en
heal.advisorName Τσουκαλάς, Δημήτριος el
heal.committeeMemberName Raptis, Yannis en
heal.committeeMemberName Ράπτης, Ιωάννης el
heal.committeeMemberName Giannakopoulos, Konstantinos en
heal.committeeMemberName Γιαννακόπουλος, Κωνσταντίνος el
heal.academicPublisher Εθνικό Μετσόβιο Πολυτεχνείο. Σχολή Εφαρμοσμένων Μαθηματικών και Φυσικών Επιστημών el
heal.academicPublisherID ntua
heal.numberOfPages 71 σ. el
heal.fullTextAvailability false


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