Download presentation
Presentation is loading. Please wait.
Published byDenis McGee Modified over 9 years ago
1
December 11, 2015 1 Study of Ni 3 Si-type core-shell nanoparticles by contrast variation in SANS experiment P. Strunz 1,2, D. Mukherji 3, G. Pigozzi 4, R. Gilles 5, T. Geue 6, K. Pranzas 7 1 Nuclear Physics Institute, CZ-25068 Řež near Prague (strunz@ujf.cas.cz)strunz@ujf.cas.cz 2 Research Centre Řež, CZ-25068 Řež near Prague, Czech Republic 3 TU Braunschweig, IfW, Langer Kamp 8, D-38106 Braunschweig, Germany 4 ETH Zurich, Laboratory for Nanometallurgy, CH-8093 Zürich, Switzerland 5 TU München, ZWE FRM-II, Lichtenbergstr. 1, D-85747 Garching, Germany 6 PSI & ETH Zurich, Laboratory for Neutron Scattering, CH-5232 Villigen PSI, Switzerland 7 GKSS Research Centre, Institute of Materials Research, D-21494 Geesthacht, Germany Project supported by the European Commission under the 6th Framework Programme through the Key Action: Strengthening the European Research Area, Research Infrastructures. Contract n°: RII3-CT-2003-505925 ' Outline Metallic nanoparticles production by ESPD core-shell nanoparticles SANS experiment motivation bulk alloy extracted nanoparticles (contrast variation)
2
December 11, 2015 2 Nano-size particles – production Synthesis of nano-size particles: sputtering, laser ablation, inert gas condensation, mechanical alloying or other means of severe plastic deformation, chemical methods … extraction mesoscale or nanoscale structural entities present in many bulk materials ETH Zurich and TU Braunschwieg: electrochemical selective phase dissolution technique => production of different nano-structures, including nano- particles with a core-shell structure extraction of nano-sized precipitates from simple two phase metallic alloys extraction mesoscale or nanoscale structural entities present in many bulk materials ETH Zurich and TU Braunschwieg: electrochemical selective phase dissolution technique => production of different nano-structures, including nano- particles with a core-shell structure extraction of nano-sized precipitates from simple two phase metallic alloys
3
December 11, 2015 3 Extraction process the technique not new TU Braunschweig and ETH Zurich: significant modifications the technique not new TU Braunschweig and ETH Zurich: significant modifications particle size tailoring diverse compositions (various intermetallic phases) each nano-particle: single crystal particle size tailoring diverse compositions (various intermetallic phases) each nano-particle: single crystal 1. Formation of nano-sized precipitates structure in bulk alloy by heat treatment 2. Separating the nano- structure from the bulk: selective phase dissolution 3. Collection of nano-particles (ultrasound vibrations) flexibility:
4
December 11, 2015 4 Potential applications intermetallic particles: production of exotic/unconventional composites thin coatings Hyperthermia for magnetic particles Catalytic and photonic applications for suitable particles intermetallic particles: production of exotic/unconventional composites thin coatings Hyperthermia for magnetic particles Catalytic and photonic applications for suitable particles Nanoparticles covered by shell potential applications in diverse fields: optical devices, magnetic storage media, health
5
December 11, 2015 5 matrix dissolution process tested on two-phase Ni–Si or Ni–Si– Al alloys: Ni 3 Si particles covered by amorphous shell made of SiO x (ETH Zurich, Institute of Applied Physics) Core-shell particles only in Si containing alloys amorphous Si-O shell is bio-resistant => particles may be suitable for medical applications matrix dissolution process tested on two-phase Ni–Si or Ni–Si– Al alloys: Ni 3 Si particles covered by amorphous shell made of SiO x (ETH Zurich, Institute of Applied Physics) Core-shell particles only in Si containing alloys amorphous Si-O shell is bio-resistant => particles may be suitable for medical applications Nanoparticles covered by shell
6
December 11, 2015 6 Studied material: alloy Ni - 13.3Si - 2Al (at %) Heat treatment: solution treatment - 1100°C 48 h WQ ageing - 600°C 24 h WQ electrochemical selective phase dissolution (ESPD): electrolyte: aqueous solution, 1% citric acid, 1% ammonium sulfate extraction voltages between 1.25 and 1.45 V Studied material: alloy Ni - 13.3Si - 2Al (at %) Heat treatment: solution treatment - 1100°C 48 h WQ ageing - 600°C 24 h WQ electrochemical selective phase dissolution (ESPD): electrolyte: aqueous solution, 1% citric acid, 1% ammonium sulfate extraction voltages between 1.25 and 1.45 V Processing parameters for core-shell particle
7
December 11, 2015 7 Characterization by XRD, TEM, EDS Shell amorphous no precise composition, estimation: Si 15%, O 85% core structure and composition: = precipitates in the bulk alloy apparently: the nanoparticles retain also the shape and size But: these methods alone insufficient Shell amorphous no precise composition, estimation: Si 15%, O 85% core structure and composition: = precipitates in the bulk alloy apparently: the nanoparticles retain also the shape and size But: these methods alone insufficient Shell formation, possibilities : 1. Depletion of Ni from Ni-Si solid solution matrix and re-deposition of Si on particle surface; 2. Depletion of Ni from Ni 3 Si precipitate surface; 3. Depletion of Ni from Ni-Si solid solution matrix and local diffusion of Si on particle surface. Shell formation, possibilities : 1. Depletion of Ni from Ni-Si solid solution matrix and re-deposition of Si on particle surface; 2. Depletion of Ni from Ni 3 Si precipitate surface; 3. Depletion of Ni from Ni-Si solid solution matrix and local diffusion of Si on particle surface.
8
December 11, 2015 8 SANS: motivation confirm core-shell structure by an independent method comparison: precipitates in the bulk alloy and nanoparticles contrast variation (masking the shell) => core and core+shell size, shell SLD comparison: precipitates in the bulk alloy and nanoparticles contrast variation (masking the shell) => core and core+shell size, shell SLD indicate the shell composition indicate which mechanism of shell formation takes place method
9
December 11, 2015 9 Experimental (SANS-II, SINQ, PSI) 1. solid sample from the bulk alloy 2. about 20 mg of nanoparticles dispersed in H 2 O/D 2 O mixture (extracted from the same alloy as the bulk sample) ultrasonic vibration for 30 min: to obtain a cluster free dispersion possible to measure within 30 minutes, then decrease of intensity due to sedimentation used D 2 O volume fractions in H 2 O/D 2 O: 100% (SLD of the mixture 63.3×10 9 cm -2 ), 80% (49.7×10 9 cm -2 ), 67% (40.7×10 9 cm -2 ) 32% (16.3×10 9 cm -2 ) 1. solid sample from the bulk alloy 2. about 20 mg of nanoparticles dispersed in H 2 O/D 2 O mixture (extracted from the same alloy as the bulk sample) ultrasonic vibration for 30 min: to obtain a cluster free dispersion possible to measure within 30 minutes, then decrease of intensity due to sedimentation used D 2 O volume fractions in H 2 O/D 2 O: 100% (SLD of the mixture 63.3×10 9 cm -2 ), 80% (49.7×10 9 cm -2 ), 67% (40.7×10 9 cm -2 ) 32% (16.3×10 9 cm -2 )
10
December 11, 2015 10 Solid sample of Ni-13.3Si-2Al alloy The inter-particle interference peak at low Q magnitudes: dense population of precipitates four precipitate populations necessary to describe the data The inter-particle interference peak at low Q magnitudes: dense population of precipitates four precipitate populations necessary to describe the data model: polydisperse 3D system of particles 2nd population: an extension of the 1st one 3rd and 4th populations in the channels between the larger precipitates model: polydisperse 3D system of particles 2nd population: an extension of the 1st one 3rd and 4th populations in the channels between the larger precipitates Polycrystalline alloy => isotropic => 3D cross section averaged gray: precipitate white: matrix 1 st population 2 nd population 3 rd population4 th population
11
December 11, 2015 11 solid sample, parameters Volume distributions total volume fraction of all populations ~44%
12
December 11, 2015 12 nanopowder sample extracted from bulk alloy SANS from nanoparticles in D 2 O (100%) compared to the precipitates in the bulk alloy from which the nanoparticles are extracted SANS from nanoparticles in D 2 O (100%) compared to the precipitates in the bulk alloy from which the nanoparticles are extracted volume fraction lower, scattering contrast higher => magnitude of scattering similar Shape changed (no influence of interparticle interference) the slope of the scattering curve from the powder in the asymptotic region deviates from Porod law (dΣ/dΩ ~ Q -4 ) volume fraction lower, scattering contrast higher => magnitude of scattering similar Shape changed (no influence of interparticle interference) the slope of the scattering curve from the powder in the asymptotic region deviates from Porod law (dΣ/dΩ ~ Q -4 )
13
December 11, 2015 13 nanopowder sample, contrast variation extracted nanoparticles dispersed in various mixtures of H 2 O/D 2 O all mixtures except 80% D 2 O: the slope at medium-to-large Q deviates from Porod law evolution with changing SLD cannot be explained without the presence of a shell extracted nanoparticles dispersed in various mixtures of H 2 O/D 2 O all mixtures except 80% D 2 O: the slope at medium-to-large Q deviates from Porod law evolution with changing SLD cannot be explained without the presence of a shell nanoparticles represented by a cuboid model, core-shell form core SLD 80.7×10 9 cm −2 distribution of sizes two populations nanoparticles represented by a cuboid model, core-shell form core SLD 80.7×10 9 cm −2 distribution of sizes two populations 1 st population 2 nd population detail model
14
December 11, 2015 14 contrast variation, SLD of the shell SANS measurement: H 2 O/D 2 O mixture with 80% D 2 O: the shell masked Q -4 scattering at medium-to-large Q magnitudes => SLD of the shell: around 49×10 9 cm -2 Calculation: Input (EDS): Oxygen content 85 at% Input: mass density of amorphous silicon oxide 2.20 g/cm 3 => theoretical SLD around 41×10 9 cm -2. Difference: cannot be explained by experimental errors Possible explanations presence of OH ions in the shell density of amorphous SiO x layer higher than assumed SANS measurement: H 2 O/D 2 O mixture with 80% D 2 O: the shell masked Q -4 scattering at medium-to-large Q magnitudes => SLD of the shell: around 49×10 9 cm -2 Calculation: Input (EDS): Oxygen content 85 at% Input: mass density of amorphous silicon oxide 2.20 g/cm 3 => theoretical SLD around 41×10 9 cm -2. Difference: cannot be explained by experimental errors Possible explanations presence of OH ions in the shell density of amorphous SiO x layer higher than assumed 80% D 2 O 100% D 2 O
15
December 11, 2015 15 contrast variation, nanopowder parameters volume-weighted size distribution of extracted core-shell nanoparticles (all mixtures)
16
December 11, 2015 16 comparison: precipitates vs. nanopowder comparison: precipitates vs. nanopowder 3rd and 4th populations (small precipitates) observed in the bulk sample not present in the nanopowder sample 1st and 2nd distributions (core) correspond well in size scale with the original populations in the solid sample => indication that the particle core was not attacked by the electrolyte during extraction process 3rd and 4th populations (small precipitates) observed in the bulk sample not present in the nanopowder sample 1st and 2nd distributions (core) correspond well in size scale with the original populations in the solid sample => indication that the particle core was not attacked by the electrolyte during extraction process distributions in solid sample compared to extracted nanoparticles displayed distributions: the core and the core + shell distributions in solid sample compared to extracted nanoparticles displayed distributions: the core and the core + shell
17
December 11, 2015 17 1.The existence of a core-shell structure in the extracted nanoparticles is confirmed by SANS measurements. 2.SANS provided quantitative information on the size distribution and volume fraction of nanoparticles. 3.SANS indicates that the selective phase dissolution is very effective for the manufacturing of the core-shell nanoparticles (the matrix dissolved, precipitate unaffected) 4.Dealloying of matrix Ni(Si) provides Si for shell formation; Si deposits on top of extracted nanoparticle core in conjunction with oxidation 1.The existence of a core-shell structure in the extracted nanoparticles is confirmed by SANS measurements. 2.SANS provided quantitative information on the size distribution and volume fraction of nanoparticles. 3.SANS indicates that the selective phase dissolution is very effective for the manufacturing of the core-shell nanoparticles (the matrix dissolved, precipitate unaffected) 4.Dealloying of matrix Ni(Si) provides Si for shell formation; Si deposits on top of extracted nanoparticle core in conjunction with oxidation Summary
18
December 11, 2015 18
19
December 11, 2015 19
20
December 11, 2015 20 Next slides left here only for possible discussion
21
December 11, 2015 21
22
December 11, 2015 22
23
December 11, 2015 23 Potential applications intermetallic particles: production of exotic/unconventional composites thin coatings. Hyperthermia for magnetic particles Catalytic and photonic applications for suitable particles intermetallic particles: production of exotic/unconventional composites thin coatings. Hyperthermia for magnetic particles Catalytic and photonic applications for suitable particles (by product) application can be also for development of evaluation methods for diffraction (profile analysis): no strain, no texture, small size => test of size-broadening formulas (by product) application can be also for development of evaluation methods for diffraction (profile analysis): no strain, no texture, small size => test of size-broadening formulas uniaxial load => directional coarsening (rafting) interconnected lamelae through the sample metallic nanoporous membrane: filtering, separation processes uniaxial load => directional coarsening (rafting) interconnected lamelae through the sample metallic nanoporous membrane: filtering, separation processes
24
December 11, 2015 24 volume fraction, scattering contrast A. absolute magnitude of the cross-section can be used scattering contrast has to be known frequently unknown in multicomponent solids (uncertainties in composition) A. absolute magnitude of the cross-section can be used scattering contrast has to be known frequently unknown in multicomponent solids (uncertainties in composition) B. dense system: interparticle distance determined => geometrical volume fraction => real volume fraction (if homogeneous distribution) contrast back-calculated using the absolute dΣ/dΩ B. dense system: interparticle distance determined => geometrical volume fraction => real volume fraction (if homogeneous distribution) contrast back-calculated using the absolute dΣ/dΩ gray: precipitate white: matrix
Similar presentations
© 2025 SlidePlayer.com. Inc.
All rights reserved.