TY - GEN A1 - Tallarida, Massimo A1 - Weisheit, Martin A1 - Kolanek, Krzysztof A1 - Michling, Marcel A1 - Engelmann, Hans-Jürgen A1 - Schmeißer, Dieter T1 - Atomic layer deposition of nanolaminate oxide films on Si T2 - Journal of Nanoparticle Research Y1 - 2011 U6 - https://doi.org/10.1007/s11051-011-0319-x VL - 13 IS - 11 SP - 5975 EP - 5983 ER - TY - GEN A1 - Kolanek, Krzysztof A1 - Tallarida, Massimo A1 - Michling, Marcel A1 - Karavaev, Konstantin A1 - Schmeißer, Dieter T1 - Atomic layer deposition reactor for fabrication of metal oxides Y1 - 2011 ER - TY - GEN A1 - Tallarida, Massimo A1 - Kukli, Kaupo A1 - Michling, Marcel A1 - Ritala, Mikko A1 - Leskelä, Markku A1 - Schmeißer, Dieter T1 - Substrate Reactivity Effects in the Atomic Layer Deposition of Aluminum Oxide from Trimethylaluminum on Ruthenium T2 - Chemistry of Materials Y1 - 2011 SN - 0897-4756 VL - 23 IS - 13 SP - 3159 EP - 3168 ER - TY - GEN A1 - Tallarida, Massimo A1 - Friedrich, Daniel A1 - Städter, Matthias A1 - Michling, Marcel A1 - Schmeißer, Dieter T1 - Growth of TiO2 with Thermal and Plasma Enhanced Atomic Layer Deposition T2 - Journal of Nanoscience and Nanotechnology Y1 - 2011 SN - 1533-4880 VL - 11 IS - 9 SP - 8049 EP - 8053 ER - TY - GEN A1 - Kolanek, Krzysztof A1 - Tallarida, Massimo A1 - Michling, Marcel A1 - Schmeißer, Dieter T1 - In situ study of the atomic layer deposition of HfO2 on Si T2 - Journal of Vacuum Science and Technology Y1 - 2012 SN - 0734-2101 IS - A 30 SP - 01A143-1 EP - 01A143-15 ER - TY - CHAP A1 - Michling, Marcel A1 - Tallarida, Massimo A1 - Kolanek, Krzysztof A1 - Schmeißer, Dieter T1 - In-situ EELS and UPS measurements on HfO2 ALD layers T2 - Verhandlungen der Deutschen Physikalischen Gesellschaft, Reihe 6, Bd. 45 N2 - In this contribution we report on our in-situ cycle-by-cycle (up to 10 cycles) investigations of the HfO2 ALD process using the methods of EELS and UPS. We used TDMA-Hf as a precursor and p-type Si wafer with natural oxide as the substrate. The EELS measurements were done with a primary energy of 52,5 eV and the UPS measurements with He I (21,218 eV). The change in the onset of the loss function is readily observed. Already after two cycles the value approach to the bulk value of HfO2. Upon ALD growth there is a remarkable decrease in the intensity of states within the gap. They are rather smooth and saturate after 10 cycles. With UPS we follow the variation of the VB onset and changes in the secondary electron onset. We summarize our data in a band diagram not based on bulk values but on cycle dependent quantities. With these cycle-by-cycle experiments we study the initial growth of HfO2 especially in the very first cycles. Y1 - 2010 UR - http://www.dpg-verhandlungen.de/year/2010/conference/regensburg/part/ds/session/24/contribution/5 SN - 0420-0195 PB - Deutsche Physikalische Gesellschaft CY - Bad Honnef ER - TY - CHAP A1 - Michling, Marcel A1 - Kolanek, Krzysztof A1 - Schmeißer, Dieter A1 - Tallarida, Massimo T1 - A growth model for the HfO2 ALD process T2 - Verhandlungen der Deutschen Physikalischen Gesellschaft, Reihe 6, Bd. 46 N2 - In this contribution we report on our in-situ2 cycle-by-cycle (up to the 25 cycles) investigation of the HfO2 atomic layer deposition (ALD) process using the method of x-ray photoelectron spectroscopy (XPS) and electron energy loss spectroscopy (EELS). We used Tetrakis-Dimethyl-Amino-Hafnium (TDMA-Hf) and H2O as precursors and p-type Si wafer with native oxide as a substrate. The XPS measurements were carried out at BESSY II in Berlin with primary energies of 150 eV and 640 eV and the EELS measurements were done with a primary energy of 50 eV. We measured the O1s, Si2p core level and the valence band including the Hf 4f core level. From the Hf4f to Si2p ratios taken at each energy we developed a growth model for the first monolayer and for the following layers too. From our data we conclude, that in the first monolayer up to the fourth ALD cycle an island growth occurs. The height of these islands is about 0,5nm. After the first monolayer is completed, a layer- by-layer growth can be expected. In order to proof this observation we have simulated the Hf/Si ratio for different excitation energies and found a very good agreement with our measurement data. The EELS data especially the evaluation of the loss function onset confirm our growth model. Y1 - 2011 UR - http://www.dpg-verhandlungen.de/year/2011/conference/dresden/part/ds/session/12/contribution/1 SN - 0420-0195 SP - S. 294 PB - Deutsche Physikalische Gesellschaft CY - Bad Honnef ER - TY - CHAP A1 - Tallarida, Massimo A1 - Deßmann, Nils A1 - Städter, Matthias A1 - Friedrich, Daniel A1 - Michling, Marcel A1 - Schmeißer, Dieter T1 - Atomic layer deposition of TiO T2 - Verhandlungen der Deutschen Physikalischen Gesellschaft, Reihe 6, Bd. 46 N2 - We present a study of the initial growth of TiO2 on Si(111) by atomic layer deposition (ALD). The Si substrate was etched with NH4F before ALD to remove the native oxide film and to produce a Si-H termination. In−situ experiments by means of photoemission and X-ray absorption spectroscopy were conducted with synchrotron radiation on Ti-oxide films produced using Ti-tetra-iso-propoxide (TTIP) and water as precursors. O1s, Ti2p, C1s, and Si2p core level, and O1s and Ti2p absorption edges show the transition of the Ti-oxide properties during the first layers. The growth starts with a very small growth rate (0.03nm/cycle) due to the growth inhibition of the Si-H termination and proceeds with higher growth rate (0.1nm/cycle) after 1.5nm Ti-oxide has been deposited. Y1 - 2011 UR - http://www.dpg-verhandlungen.de/year/2011/conference/dresden/part/ds/session/12/contribution/2 SN - 0420-0195 PB - Deutsche Physikalische Gesellschaft CY - Bad Honnef ER - TY - CHAP A1 - Tallarida, Massimo A1 - Michling, Marcel A1 - Das, Chittaranjan A1 - Friedrich, Daniel A1 - Städter, Matthias A1 - Schmeißer, Dieter T1 - Role of substrate chemistry in ALD revealed by in-situ techniques T2 - Verhandlungen der Deutschen Physikalischen Gesellschaft, Reihe 6, Bd. 47 N2 - We show recent results of our in-situ investigations where the role of substrate chemistry in ALD is outlined. While the usual strategy to develop new properties of ALD films is to find new precursors or new procedures, the influence of substrate chemistry on the growth properties of ALD films has been often underestimated. This has principally a technical reason, as the usual characterization methods (QMS, FTIR, ellipsometry) are only weakly sensitive to the substrate, and a characterization of substrates before ALD is often not possible. Thanks to the use of in-situ characterization methods, including photoemission and X-ray absorption spectroscopy with synchrotron radiation, we are able to determine chemical properties of substrates before ALD and after either half or complete ALD cycles. The substrate chemistry influences the standard Al2O3 ALD with TMA and water [1,2], as well as the TiO2 ALD with TTIP and either water, O2 or O2-plasma. [1] M. Tallarida, K. Kukli, M. Michling, M. Ritala, M. Leskelä and D. Schmeisser, Chem. Mater. 23, 3159 (2011); [2] M. Tallarida, C. Adelmann, A. Delabie, S. van Elshocht, M. Caymax, and D. Schmeisser, Appl. Phys. Lett. 92, 042906 (2011). Y1 - 2012 UR - http://www.dpg-verhandlungen.de/year/2012/conference/berlin/part/ds/session/22/contribution/3 SN - 0420-0195 PB - Deutsche Physikalische Gesellschaft CY - Bad Honnef ER -