Raivo Jaaniso

Prof. Raivo Jaaniso

orcid

Research Focus & Metrics

Academic Career Length

41Years (1986-Present)

(Calculated once Scilit publication data is synced: current year − year of first publication + 1)

Representative Publications

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7 October 1991 in Europhysics Letters
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Journal Article
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RJRaivo Jaaniso
Raivo Jaaniso
HBH. Bill
H. Bill

1 January 2013
Verified
Book
Closed access
RJRaivo Jaaniso
Raivo Jaaniso
OTOoi Kiang Tan
Ooi Kiang Tan

1 March 2016 in Sensors and Actuators B: Chemical
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Journal Article
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ASAndris Sutka
Andris Sutka
MKMargus Kodu
Margus Kodu
RPRainer Pärna
Rainer Pärna
RSRaando Saar
Raando Saar
IJInna Juhnevica
Inna Juhnevica
VKVambola Kisand
Vambola Kisand

1 June 2017 in AIP Advances
Verified
Journal Article
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JKJ. Krustok
J. Krustok
RKR. Kaupmees
R. Kaupmees
RJRaivo Jaaniso
Raivo Jaaniso
VKValter Kiisk
Valter Kiisk
ISI. Sildos
I. Sildos
YGY. Gong
Y. Gong
Optical properties of aged WS2 monolayers grown by CVD method on Si/SiO2 substrates are studied using temperature dependent photoluminescence and reflectance contrast spectroscopy. Aged WS2 monolayers have a typical surface roughness about 0.5 nm and, in addition, a high density of nanoparticles (nanocaps) with the base diameter about 30 nm and average height of 7 nm. The A-exciton of aged monolayer has a peak position at 1.951 eV while in as-grown monolayer the peak is at about 24 meV higher energy at room temperature. This red-shift is explained using local tensile strain concept, where strain value of 2.1% was calculated for these nanocap regions. Strained nanocaps have lower band gap energy and excitons will funnel into these regions. At T=10K a double exciton and trion peaks were revealed. The separation between double peaks is about 20 meV and the origin of higher energy peaks is related to the optical band gap energy fluctuations caused by random distribution of local tensile strain due to increased surface roughness. In addition, a wide defect related exciton band XD was found at about 1.93 eV in all aged monolayers. It is shown that the theory of localized excitons describes well the temperature dependence of peak position and halfwidth of the A-exciton band. The possible origin of nanocaps is also discussed.

1 March 2006 in Open Physics
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Journal Article
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ANAhti Niilisk
Ahti Niilisk
MMMart Moppel
Mart Moppel
MPMartti Pärs
Martti Pärs
ISIlmo Sildos
Ilmo Sildos
TJTaavi Jantson
Taavi Jantson
JAJaan Aarik
Jaan Aarik
The Raman spectroscopy method was used for structural characterization of TiO2 thin films prepared by atomic layer deposition (ALD) and pulsed laser deposition (PLD) on fused silica and single-crystal silicon and sapphire substrates. Using ALD, anatase thin films were grown on silica and silicon substrates at temperatures 125–425 °C. At higher deposition temperatures, mixed anatase and rutile phases grew on these substrates. Post-growth annealing resulted in anatase-to-rutile phase transitions at 750 °C in the case of pure anatase films. The films that contained chlorine residues and were amorphous in their as-grown stage transformed into anatase phase at 400 °C and retained this phase even after annealing at 900 °C. On single crystal sapphire substrates, phase-pure rutile films were obtained by ALD at 425 °C and higher temperatures without additional annealing. Thin films that predominantly contained brookite phase were grown by PLD on silica substrates using rutile as a starting material.

1 November 2012 in Journal of Physics D: Applied Physics
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Journal Article
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MDM Chandra Dimri
M Chandra Dimri
HKH Khanduri
H Khanduri
HKH Kooskora
H Kooskora
MKM Kodu
M Kodu
RJRaivo Jaaniso
Raivo Jaaniso
Raivo SternRaivo Stern
Raivo Stern
We report room-temperature ferromagnetism in Ca and Mg stabilized zirconia bulk samples and thin films. Powders were prepared by the citrate-combustion route, and thin films grown on silicon substrates by the pulsed laser deposition technique. X-ray diffractograms and Raman spectra at room temperature reveal the formation of cubic phase zirconia. The observed ferromagnetism is robust at room temperature in both bulk as well as in thin film samples, although it is weaker in thin films. The origin of the ferromagnetism can be related to oxygen vacancies created due to divalent (calcium and magnesium) substitution for tetravalent zirconium ions.