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Dive into the research topics where Jaakko Julin is active.

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Featured researches published by Jaakko Julin.


Journal of Vacuum Science and Technology | 2015

Nucleation and growth of ZnO on PMMA by low-temperature atomic layer deposition

Mari Napari; Jari Malm; Roope Lehto; Jaakko Julin; Kai Arstila; Timo Sajavaara; Manu Lahtinen

ZnO films were grown by atomic layer deposition at 35 °C on poly(methyl methacrylate) substrates using diethylzinc and water precursors. The film growth, morphology, and crystallinity were studied using Rutherford backscattering spectrometry, time-of-flight elastic recoil detection analysis, atomic force microscopy, scanning electron microscopy, and x-ray diffraction. The uniform film growth was reached after several hundreds of deposition cycles, preceded by the precursor penetration into the porous bulk and island-type growth. After the full surface coverage, the ZnO films were stoichiometric, and consisted of large grains (diameter 30 nm) with a film surface roughness up to 6 nm (RMS). The introduction of Al2O3 seed layer enhanced the initial ZnO growth substantially and changed the surface morphology as well as the crystallinity of the deposited ZnO films. Furthermore, the water contact angles of the ZnO films were measured, and upon ultraviolet illumination, the ZnO films on all the substrates became...


Journal of Vacuum Science and Technology | 2017

Aluminum oxide/titanium dioxide nanolaminates grown by atomic layer deposition: Growth and mechanical properties

Oili M. E. Ylivaara; Lauri Kilpi; Xuwen Liu; Sakari Sintonen; Saima Ali; Mikko Laitinen; Jaakko Julin; Eero Haimi; Timo Sajavaara; Harri Lipsanen; Simo-Pekka Hannula; Helena Ronkainen; Riikka L. Puurunen

Atomic layer deposition (ALD) is based on self-limiting surface reactions. This and cyclic process enable the growth of conformal thin films with precise thickness control and sharp interfaces. A multilayered thin film, which is nanolaminate, can be grown using ALD with tuneable electrical and optical properties to be exploited, for example, in the microelectromechanical systems. In this work, the tunability of the residual stress, adhesion, and mechanical properties of the ALD nanolaminates composed of aluminum oxide (Al 2O3) and titanium dioxide (TiO2) films on silicon were explored as a function of growth temperature (110–300 °C), film thickness (20–300 nm), bilayer thickness (0.1–100 nm), and TiO2 content (0%–100%). Al 2O3 was grown from Me3 Al and H2O, and TiO2 from TiCl4 and H2O. According to wafer curvature measurements, Al 2O3/TiO2 nanolaminates were under tensile stress; bilayer thickness and growth temperature were the major parameters affecting the stress; the residual stress decreased with increasing bilayer thickness and ALD temperature. Hardness increased with increasing ALD temperature and decreased with increasing TiO2 fraction. Contact modulus remained approximately stable. The adhesion of the nanolaminate film was good on silicon.


Review of Scientific Instruments | 2016

Simulations on time-of-flight ERDA spectrometer performance

Jaakko Julin; Kai Arstila; Timo Sajavaara

The performance of a time-of-flight spectrometer consisting of two timing detectors and an ionization chamber energy detector has been studied using Monte Carlo simulations for the recoil creation and ion transport in the sample and detectors. The ionization chamber pulses have been calculated using Shockley-Ramo theorem and the pulse processing of a digitizing data acquisition setup has been modeled. Complete time-of-flight-energy histograms were simulated under realistic experimental conditions. The simulations were used to study instrumentation related effects in coincidence timing and position sensitivity, such as background in time-of-flight-energy histograms. Corresponding measurements were made and simulated results are compared with data collected using the digitizing setup.


Journal of Vacuum Science and Technology | 2016

Unusual stoichiometry control in the atomic layer deposition of manganese borate films from manganese bis(tris(pyrazolyl)borate) and ozone

Joseph P. Klesko; James A. Bellow; Mark Saly; Charles H. Winter; Jaakko Julin; Timo Sajavaara

The atomic layer deposition (ALD) of films with the approximate compositions Mn3(BO3)2 and CoB2O4 is described using MnTp2 or CoTp2 [Tp = tris(pyrazolyl)borate] with ozone. The solid state decomposition temperatures of MnTp2 and CoTp2 are ∼370 and ∼340 °C, respectively. Preparative-scale sublimations of MnTp2 and CoTp2 at 210 °C/0.05 Torr afforded >99% recoveries with <0.1% nonvolatile residues. Self-limited ALD growth was demonstrated at 325 °C for MnTp2 or CoTp2 with ozone as the coreactant. The growth rate for the manganese borate process was 0.19 A/cycle within the ALD window of 300–350 °C. The growth rate for the cobalt borate process was 0.39–0.42 A/cycle at 325 °C. X-ray diffraction of the as-deposited films indicated that they were amorphous. Atomic force microscopy of 35–36 nm thick manganese borate films grown within the 300–350 °C ALD window showed root mean square surface roughnesses of 0.4–0.6 nm. Film stoichiometries were assessed by x-ray photoelectron spectroscopy and time of flight-elasti...


Journal of Vacuum Science and Technology | 2018

Comparison of mechanical properties and composition of magnetron sputter and plasma enhanced atomic layer deposition aluminum nitride films

Perttu Sippola; Alexander Pyymaki Perros; Oili M. E. Ylivaara; Helena Ronkainen; Jaakko Julin; Xuwen Liu; Timo Sajavaara; Jarkko Etula; Harri Lipsanen; Riikka L. Puurunen

A comparative study of mechanical properties and elemental and structural composition was made for aluminum nitride thin films deposited with reactive magnetron sputtering and plasma enhanced atomic layer deposition (PEALD). The sputtered films were deposited on Si (100), Mo (110), and Al (111) oriented substrates to study the effect of substrate texture on film properties. For the PEALD trimethylaluminum–ammonia films, the effects of process parameters, such as temperature, bias voltage, and plasma gas (ammonia versus N2/H2), on the AlN properties were studied. All the AlN films had a nominal thickness of 100 nm. Time-of-flight elastic recoil detection analysis showed the sputtered films to have lower impurity concentration with an Al/N ratio of 0.95, while the Al/N ratio for the PEALD films was 0.81–0.90. The mass densities were ∼3.10 and ∼2.70 g/cm3 for sputtered and PEALD AlN, respectively. The sputtered films were found to have higher degrees of preferential crystallinity, whereas the PEALD films were more polycrystalline as determined by x-ray diffraction. Nanoindentation experiments showed the elastic modulus and hardness to be 250 and 22 GPa, respectively, for sputtered AlN on the (110) substrate, whereas with PEALD AlN, values of 180 and 19 GPa, respectively, were obtained. The sputtered films were under tensile residual stress (61–421 MPa), whereas the PEALD films had a residual stress ranging from tensile to compressive (846 to −47 MPa), and high plasma bias resulted in compressive films. The adhesion of both films was good on Si, although sputtered films showed more inconsistent critical load behavior. Also, the substrate underneath the sputtered AlN did not withstand high wear forces as with the PEALD AlN. The coefficient of friction was determined to be ∼0.2 for both AlN types, and their wear characteristics were almost identical.A comparative study of mechanical properties and elemental and structural composition was made for aluminum nitride thin films deposited with reactive magnetron sputtering and plasma enhanced atomic layer deposition (PEALD). The sputtered films were deposited on Si (100), Mo (110), and Al (111) oriented substrates to study the effect of substrate texture on film properties. For the PEALD trimethylaluminum–ammonia films, the effects of process parameters, such as temperature, bias voltage, and plasma gas (ammonia versus N2/H2), on the AlN properties were studied. All the AlN films had a nominal thickness of 100 nm. Time-of-flight elastic recoil detection analysis showed the sputtered films to have lower impurity concentration with an Al/N ratio of 0.95, while the Al/N ratio for the PEALD films was 0.81–0.90. The mass densities were ∼3.10 and ∼2.70 g/cm3 for sputtered and PEALD AlN, respectively. The sputtered films were found to have higher degrees of preferential crystallinity, whereas the PEALD films wer...


Thin Solid Films | 2014

Aluminum oxide from trimethylaluminum and water by atomic layer deposition: The temperature dependence of residual stress, elastic modulus, hardness and adhesion

Oili M. E. Ylivaara; Xuwen Liu; Lauri Kilpi; Dieter Schneider; Mikko Laitinen; Jaakko Julin; Saima Ali; Sakari Sintonen; Maria Berdova; Eero Haimi; Timo Sajavaara; Helena Ronkainen; Harri Lipsanen; Jari Koskinen; Simo-Pekka Hannula; Riikka L. Puurunen


Nuclear Instruments & Methods in Physics Research Section B-beam Interactions With Materials and Atoms | 2014

Time-of-flight - Energy spectrometer for elemental depth profiling - Jyväskylä design

Mikko Laitinen; Mikko Rossi; Jaakko Julin; Timo Sajavaara


Nuclear Instruments & Methods in Physics Research Section B-beam Interactions With Materials and Atoms | 2014

Potku - New analysis software for heavy ion elastic recoil detection analysis

Kai Arstila; Jaakko Julin; Mikko Laitinen; Jarkko Aalto; Timo Konu; Samuli Kärkkäinen; Samuli Rahkonen; Miika Raunio; Jonne Itkonen; Jukka-Pekka Santanen; Tero Tuovinen; Timo Sajavaara


Journal of Low Temperature Physics | 2014

Transition-Edge Sensors for Particle Induced X-ray Emission Measurements

Mikko R. J. Palosaari; Kimmo Kinnunen; Jaakko Julin; Mikko Laitinen; Mari Napari; Timo Sajavaara; W. B. Doriese; J. W. Fowler; Carl D. Reintsema; Daniel S. Swetz; Daniel R. Schmidt; Joel N. Ullom; I. J. Maasilta


Nuclear Instruments & Methods in Physics Research Section B-beam Interactions With Materials and Atoms | 2011

Depth profiling of Al2O3 + TiO2 nanolaminates by means of a time-of-flight energy spectrometer

Mikko Laitinen; Timo Sajavaara; Mikko Rossi; Jaakko Julin; Riikka L. Puurunen; T. Suni; T. Ishida; H. Fujita; Kai Arstila; Bert Brijs; Harry J. Whitlow

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Timo Sajavaara

University of Jyväskylä

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Mikko Laitinen

University of Jyväskylä

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Kai Arstila

University of Jyväskylä

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Mikko Rossi

University of Jyväskylä

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Riikka L. Puurunen

VTT Technical Research Centre of Finland

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Mari Napari

University of Jyväskylä

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Oili M. E. Ylivaara

VTT Technical Research Centre of Finland

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Helena Ronkainen

VTT Technical Research Centre of Finland

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