- Page 2 and 3: Local Organizing CommitteeThomas Ba
- Page 6 and 7: Carbon nanotubes in materials scien
- Page 8 and 9: Temperature Study of Surface Plasmo
- Page 10 and 11: Transmission Electron Microscopy Te
- Page 12 and 13: Transmission Electron Microscopy St
- Page 14 and 15: Effects of pressure on the Boson pe
- Page 16 and 17: Session MON-3Physics of surfaces, t
- Page 18 and 19: Transmission Electron Microscopy of
- Page 20 and 21: Magnetic and Fluorescent ZnO/Iron O
- Page 22 and 23: Slip/no-slip existence at the nanos
- Page 24 and 25: Session MON-4Strongly correlated el
- Page 26 and 27: The multilayer growth was studied b
- Page 28 and 29: Fig.1b: orthorhombic, Pmmn, a=4.78
- Page 30 and 31: Next we present our preliminary res
- Page 32 and 33: Dielectric Properties of La 2 CuO 4
- Page 34 and 35: Photonic interfacing by laser light
- Page 36 and 37: Figure 2. Phononic band structure a
- Page 38 and 39: can support, in addition, phononic
- Page 40 and 41: WO 3 films electrodeposited on a pi
- Page 42 and 43: Compared to electrochromics, the ph
- Page 44 and 45: All-angle Homogenization of Anisotr
- Page 46 and 47: Implantation and Diffusion of Galli
- Page 48 and 49: Session TUE-1Physics of surfaces, t
- Page 50 and 51: Nano-crystalline Mg 2 Si Prepared b
- Page 52 and 53: Strain State and Internal Polarizat
- Page 54 and 55:
From Quantum Dynamics to Supramolec
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A neutron diffraction and magnetiza
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(a)0.12(b)0.050TRM0.110.100.09t w=2
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systems. It is also well known that
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we flip the cluster and n B is the
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the rare earth cation towards 3+ [4
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Development of Smart Polymer-functi
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Silicon Oxy Carbide Nanorings From
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Ordered Mesoporous Silicas as Addit
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Investigation of the Nanomechanical
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Nonlinearity-induced Anomalous Char
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Growth and Properties of Porous Ano
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Session TUE-4Ceramics, composites,m
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the layered materials was examined
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Normalised TL (a.u.)Normalised TL (
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Figure 1: Summary of reactions betw
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without the intermediate drying ste
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For the evaluation of the insertion
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One of another great value is that
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Modeling Nanostructured Materials S
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conductance at the conductance thre
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Pb 5d3/2 peak height (a.u.)0.180.16
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slope might be the same for all cas
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Session WED-2Physics of surfaces, t
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Load, μN500400300200Load, μΝ5000
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In Figs. 2 and 3 the load vs. displ
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Thermally Poled Glasses with Non-li
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Figure 1. HRTEM image of a SiO x fi
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A compared to film B and C, by one
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Surface Enhanced Raman Spectroscopy
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equirements for a variety of bias v
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Phase Solitons in the Spin Ground S
- Page 118 and 119:
Poster Session 1Photonics and optoe
- Page 120 and 121:
Diffraction Grating Thin Film Senso
- Page 122 and 123:
Using a polarised laser source at 6
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EPR and Conductivity Study of the M
- Page 126 and 127:
Electronic transport in nanocrystal
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Carrier Scattering and Hybrid Phono
- Page 130 and 131:
One-phonon processes versus Multi-p
- Page 132 and 133:
Far Infrared Spectra of the AsS 2 a
- Page 134 and 135:
The Effect of Tin Impurities in the
- Page 136 and 137:
Poster Session 1Structural-dynamica
- Page 138 and 139:
Figure 1(b) displays the Raman spec
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Figure 2. Selected area diffraction
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Figure 1: Bright-field XTEM images
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Figure 2: Cross-sectional HRTEM ima
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1 GPa -1 ) [6]. Moreover, the press
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Poster Session 1Strongly correlated
- Page 150 and 151:
Effect Of [Fe(CN) 6 ] 4- Substituti
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Investigations of Orbital and Magne
- Page 154 and 155:
Fig.1 Hysteresis loops of [Ni/Pt] 6
- Page 156 and 157:
the other hand at sample Fe4 the ch
- Page 158 and 159:
the absolute magnetization per site
- Page 160 and 161:
1J1+J2p( Jij ) = ⎡δ( Jij J1) δ(
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Spin order and lattice frustration
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CCIntensity (Counts)120010008006004
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Figure 2. CTEM and HRTEM of Fe 3 O
- Page 168 and 169:
the combined processes of grain gro
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Assemblies of Magnetic Nanoparticle
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Poster Session 1Physics of surfaces
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Figure 1. The magnetization, M, as
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2). Furthermore, the number of As a
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Development of a model Ziegler-Natt
- Page 180 and 181:
Ab initio study of Semipolar AlN Su
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Adsorption, diffusion and incorpora
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Self-Assembled InGaN Quantum Dot Su
- Page 186 and 187:
Formation of Hexagonal Ni in Ru/Ni
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Deposition of Superparamagnetic Col
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Electron Energy Loss Near Edge Stru
- Page 192 and 193:
Controllable synthesis of iron oxy-
- Page 194 and 195:
Growth and Characterization of Al 2
- Page 196 and 197:
The interaction of metallic Cr with
- Page 198 and 199:
Optical Properties of Metallic Nano
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Load, μN600500400300200100Load, μ
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Figure 2a: AFM image showing thetop
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Structural and electronic propertie
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[2] Wildgoose G. G., Banks C. E., C
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Poster Session 2Physics of surfaces
- Page 210 and 211:
Ab-Initio Calculations of Cu Nanowi
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Surface Functionalization by means
- Page 214 and 215:
Formation of micro-cones by oxygen
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this temperature there is no remark
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Results and DiscussionNanocomposite
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At 300 K, a significant hysteresis
- Page 222 and 223:
Figure 1: TEM micrograph of a film
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12,6A oSi_GOIntensity (a.u.)10,4 A
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In Fig. I we show two representativ
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working area of the periodic table
- Page 230 and 231:
Thermal Treatment of PEDOT:PSS Film
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A Novel Approach for Preparation of
- Page 234 and 235:
Detection of Residual Solvent in Th
- Page 236 and 237:
Brownian dynamics simulations on se
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120016010010001401201200100080E' (
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Metathesis Polymerization of Phenyl
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Microphase Separation in (AB)-Multi
- Page 244 and 245:
Synthesis and Properties of Core/Sh
- Page 246 and 247:
Poster Session 2Ceramics, composite
- Page 248 and 249:
Fig. 1: Influence of temperature an
- Page 250 and 251:
Sample 5-TiO 2 P25 U-5-TiO 2 U-P25
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transient state in the relaxation o
- Page 254 and 255:
σ (A . m 2 /kg)0.650.600.550.500.4
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(a)(b)Fig.2. a) Mean values of flex
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transformation to Si-II and subsequ
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ER/MWCNTs nanocomposites [6]. Moreo
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a H (Å) Me-O (Å)1.9651.9551.9451.
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suspension on glass slide. XRD anal
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Table 1. Rietveld refinement struct
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the real effect of a native oxide a
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where it was shown that further pro
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Calculation of the Penetration Dept
- Page 274 and 275:
Oxidation of zinc hot-dip galvanize
- Page 276 and 277:
An XRD study of galvanized coatings
- Page 278 and 279:
Influence of Wollastonite on the Qu
- Page 280 and 281:
Study of the Bioactive Hydroxyapati
- Page 282 and 283:
Study of the Bioactive Hydroxyapati
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An EPR-Based Method to Probe the Lo
- Page 286 and 287:
Surprisingly, the spectra indicate
- Page 288 and 289:
with O 2 . In the XRD pattern only
- Page 290 and 291:
characteristic strong reflection at
- Page 292 and 293:
indicates abundant volatile compone
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The layers are alternating in a sta
- Page 296 and 297:
(111)(220)MS200MS202Mg2Siintensity
- Page 298 and 299:
MEMS charging the FTIR spectra and
- Page 300 and 301:
possible this particular route for
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produces significantly more accurat
- Page 304 and 305:
Hyperthermia Response of Iron Oxide
- Page 306 and 307:
probably used, however, either this
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1110 cm-1 attributed to the ν 1 vi
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Choulis S.A. ......................
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Ho Rong-Ming ......................
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Malliakas Christos.................
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Simserides C.......................
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318
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23. All-angle Homogenization of Ani
- Page 322 and 323:
K. Karkas and N. Guskos ...........
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C. A. Charitidis,A. Skarmoutsou, A.
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G. Litsardakis and S. Nikolaki.....