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Institute for Nanoscale Physics and Chemistry INPAC’s mission: Investigation of the effect of nanostructuring and nanoscale confinement of charges, spins, and photons on the electrical, magnetic, optical, and chemical properties of inorganic, organic, and biomaterials in order to reveal the fundamental relation between quantized confined states and physical and chemical properties of these materials www.kuleuven.be/inpac

Institute for Nanoscale Physics and Chemistry · X-ray diffraction (XRD) Auger spectroscopy X-rayphotoelectronspectroscopy(XPS) Micro-Raman and resonant Raman spectroscopy Rutherford

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Page 1: Institute for Nanoscale Physics and Chemistry · X-ray diffraction (XRD) Auger spectroscopy X-rayphotoelectronspectroscopy(XPS) Micro-Raman and resonant Raman spectroscopy Rutherford

Institute for Nanoscale Physics and Chemistry

INPAC’s mission:

Investigation of the effect of nanostructuring and nanoscaleconfinement of charges, spins, and photons on the electrical, magnetic, optical, and chemical properties of inorganic, organic, and biomaterials in order to reveal the fundamental relation between quantized confined states and physical and chemical properties of these materials

www.kuleuven.be/inpac

Page 2: Institute for Nanoscale Physics and Chemistry · X-ray diffraction (XRD) Auger spectroscopy X-rayphotoelectronspectroscopy(XPS) Micro-Raman and resonant Raman spectroscopy Rutherford

Nanosuperconductors

Nanoscale evolution of superconductivity Confined flux in individual 2D and 3D nanostructures Superconductors with nanoengineered periodic pinning arrays Nanoscale evolution of superconductivity Exploration of the ability of biomolecules to form templates for deposition of nanomodulated films

Research Activities

Nanomagnets

µm

0

2

4

6

0

2

4

6µm

0

2

4

6

0

2

4

6

0

2

4

6

0

2

4

6

04

812

16

µm0

4

8

12

16

04

812

16

04

812

16

µm0

4

8

12

16

0

4

8

12

16

TC (Φ/Φ0) for a superconducting ring

Superconducting dotsAntidots (holes) for

vortex ratchets

Cover (from top to bottom): Simulated vortex distribution in a superconducting square, cluster deposited on a surface, STM imaging of molecules.

To study the single entity properties through shrinking its dimensions (i.e., the evolution of magnetism at nanoscale)

To study superstructures (superlattices and cluster arrays) through combining the single magnetic entities (the drive in chemistry to make advanced structures from elementary building blocks)

To understand the properties of both the elementary "magnetic building blocks" (nanocells - magnetic clusters, etc.) as well as their collective behaviour when put together

HOMO

LUMO( ) -6.72 eVa1

(1 )s

(1 ), (1 )d dxy x -y ² ²

( ) -8.15 eVe3

( ) -8.10 eVe2

(1 )pz

Ag 4 bandd

(1 ), (1 )d dxz yz

(1 )dz²

X-ray reflectometry mapping of a patterned magnetic structure

Magnetic domains in an antiferromagnetic Fe/Cr superlattice

Calculated electronic structure of a Ag cluster containing magnetic Co dopants

Page 3: Institute for Nanoscale Physics and Chemistry · X-ray diffraction (XRD) Auger spectroscopy X-rayphotoelectronspectroscopy(XPS) Micro-Raman and resonant Raman spectroscopy Rutherford

Institute for Nanoscale Physics and Chemistry

Carbon nanosystems

Superconductor/Ferromagnet hybrid nanosystems

Vortex matter in superconductors with magnetic dots and in superconductor / ferromagnet planar hybrids New possibilities of vortex manipulation with nanoscale magnetic pinning sites and magnetic textures Novel phenomena such as field-induced superconductivity and domain wall superconductivity

Research Activities

Lattice of magnetic dotson top of a superconducting thin film

Field induced superconductivity

Order parameter distributionin a superconducting square with a magnetic dot on top

(vorticity= -27)

Magnetic domains inBaFe12O19

Carbon nanotubes and related materials, including fullerenes, are unique nanosystems with great scientific and technological potential

Realistic modeling of the electronic structure of carbon nanomaterialsExperimental probing of electrical and mechanical properties

Ring currents innanographene

1 µm 50

70

90

110

0

300

MHz

nm

SEM AFM resonance

1 µm 50

70

90

110

0

300

MHz

nm

1 µm 50

70

90

110

0

300

MHz

nm

SEM AFM resonance

SEM and AFM imaging of a coiled carbon nanotube, where the dynamic AFM mode also provides direct information about the mechanical resonance of the windings of the tube

Page 4: Institute for Nanoscale Physics and Chemistry · X-ray diffraction (XRD) Auger spectroscopy X-rayphotoelectronspectroscopy(XPS) Micro-Raman and resonant Raman spectroscopy Rutherford

Materials for nanophotonics

Nanoconfinement in photonics -light wavelength is inherently at the nanoscaleAdding magnetic contribution to the optical response Combining nonlinear optics with single-molecule spectroscopy at the nanoscaleEngineering and applying photonic heterostructures for the development of optical integrated circuits Designing photo - switchable proteins for increasing the spatial resolution of fluorescence microscopy

Silicon nanosystems

To integrate research on Si-based nm particles and 2D structures regarding properties of nanoparticles, layers, interfaces, and surfaces, based on a complementary study of phonons, charges, and spins

Metal-doped Si clusters Phonon and electron states in 2D systems Nanoparticles and embedding Interfaces and point defects

Research Activities

Photonic crystal of silica spheres of 290 nm and monolayer of 417 nm silica spheres

Chiral molecules

Chiral light

hν hν

Si SiMeOx

Au/Al (15 nm)

pA

BIAS

+-

pA

BIAS

-+

Vg>0 Vg <0

Au/Al

Al@Pb12+

IPS

Fe

Fe

FeSi

Intercalated Fe-Si layerin an Fe matrix

Sub-monolayer Fe-deposited(using MBE) on Si(111)

Page 5: Institute for Nanoscale Physics and Chemistry · X-ray diffraction (XRD) Auger spectroscopy X-rayphotoelectronspectroscopy(XPS) Micro-Raman and resonant Raman spectroscopy Rutherford

Institute for Nanoscale Physics and Chemistry

Self-assembled molecular and macromolecular structures

Precise control and creation of nanoscale organic structures (with special attention to chirality)Highly ordered 2D templates for nanostructuresSelf-assembled nanostructures under potential controlMixtures of molecules and polymers self-organizing into bicontinuous percolating systemsCharacterization of the electronic and optical properties of self-assembled structuresSynthesis of new chiral conducting polymers self-assembling into chiral supramolecular structures

Research Activities

Fundamental Research - Technology - Education

Fundamental ResearchINPAC

www.kuleuven.be/inpac

Applied ResearchIMEC

www.imec.be

EducationErasmus Mundus Master of

Nanoscience and Nanotechnologywww.kuleuven.be/MNST

STM image of rosettesformed byπ-conjugated

OPV’s

STM image of monomers and sandwich dimers of

phthalocyanine

STM image of chiral poly-(3,7-dimethyloctyl)thiophenein a chiral mono- and bilayer

INPAC – IMEC – Erasmus Mundus MNST

Chains of bacteria, visualizedby electron microsocopy can be

used as (in this case 1D) templatesto deposit nanoparticles

Page 6: Institute for Nanoscale Physics and Chemistry · X-ray diffraction (XRD) Auger spectroscopy X-rayphotoelectronspectroscopy(XPS) Micro-Raman and resonant Raman spectroscopy Rutherford

Research Facilities

Thin film preparation

Nanostructuring techniques

Molecular beam epitaxySputtering & EvaporationLow energy ion deposition/implantationCluster beam depositionElectro-chemical depositionSpin castingPotentio-control adsorptionLangmuir-Blodgett layer deposition

E-beam patterningIon beam patterningSTM-writingOptical lithographyNanomanipulationSelf-assemblySelf-organized etchingMelt quenching

Riber MBE - IMBL

Thin filmPreparation

0

Nano-StructuringTechniques

1

IntegratedStructuralProperties

2

OpticalTechniques

3

4

LocalProbe

Techniques

IntegratedPhysical

Properties

ModelingTools

INPACK.U.Leuven

AFM in fluidsSPM in fluidsMicro-RamanspectroscopyLT- MFMLT- AFMLT – vacuum

STSLT – vacuum

STM4

5

6

Potentio-controladsorption

Spincasting

Electro-chemicaldeposition

Cluster beamdeposition

Low energyion deposition

Molecularbeam epitaxy

Langmuir-

Blodgett

Melt-

quenching

Rheed

Fluorescent

cell sorter

PAC

Monte-

Carlo

Self- organizedetching

Self-assembly

Nano-manipulator

Opticallithography

STM –writing

Ion beampatterning

E-beampatterning

ChannelingRaman spectroscopyAuger

XRD

Confocalmicroscopy

Transient photo-conductivity

Hyper-Rayleighscattering

Quasi-elasticlight scattering

Photoionizationspectroscopy

Time resolvedspectroscopy

Neutronscattering

X-ray magnetichyperfine spectr.

Mössbauerspectroscopy

High fieldρ, M, CR, PL

Time resolvedcalorimetry

Moleculardynamics

Car – ParrinelloDFT

Kohn – ShamDFT

Abrikosov-Gor’kov

Ab initiocalculation

Bogoliubov-de GennesTD(GL)

SHPM

eBµ ωη

eBµ ωη

eBµ ωη

eBµ ωη

0

1

2

3

4

5

6

XPS

ESR

IPE

SEM

TEM

Sputtering

Evaporation

UV-VIS

MO KERR

SQUID

VSM

Low T CEMS

I-V, C-V, G-V

RBS

ERD

Thin filmPreparation

0

Nano-StructuringTechniques

1

IntegratedStructuralProperties

2

OpticalTechniques

3

4

LocalProbe

Techniques

IntegratedPhysical

Properties

ModelingTools

INPACK.U.Leuven

INPACK.U.Leuven

AFM in fluidsSPM in fluidsMicro-RamanspectroscopyLT- MFMLT- AFMLT – vacuum

STSLT – vacuum

STM4

5

6

Potentio-controladsorption

Spincasting

Electro-chemicaldeposition

Cluster beamdeposition

Low energyion deposition

Molecularbeam epitaxy

Langmuir-

Blodgett

Melt-

quenching

Rheed

Fluorescent

cell sorter

PAC

Monte-

Carlo

Self- organizedetching

Self-assembly

Nano-manipulator

Opticallithography

STM –writing

Ion beampatterning

E-beampatterning

ChannelingRaman spectroscopyAuger

XRD

Confocalmicroscopy

Transient photo-conductivity

Hyper-Rayleighscattering

Quasi-elasticlight scattering

Photoionizationspectroscopy

Time resolvedspectroscopy

Neutronscattering

X-ray magnetichyperfine spectr.

Mössbauerspectroscopy

High fieldρ, M, CR, PL

Time resolvedcalorimetry

Moleculardynamics

Car – ParrinelloDFT

Kohn – ShamDFT

Abrikosov-Gor’kov

Ab initiocalculation

Bogoliubov-de GennesTD(GL)

SHPM

eBµ ωη

eBµ ωη

eBµ ωη

eBµ ωη

0

1

2

3

4

5

6

XPS

ESR

IPE

SEM

TEM

Sputtering

Evaporation

UV-VIS

MO KERR

SQUID

VSM

Low T CEMS

I-V, C-V, G-V

RBS

ERD

Page 7: Institute for Nanoscale Physics and Chemistry · X-ray diffraction (XRD) Auger spectroscopy X-rayphotoelectronspectroscopy(XPS) Micro-Raman and resonant Raman spectroscopy Rutherford

Institute for Nanoscale Physics and Chemistry

Integrated structural properties

Optical techniques

X-ray diffraction (XRD)Auger spectroscopyX-ray photoelectron spectroscopy (XPS)Micro-Raman and resonant Raman spectroscopyRutherford backscattering spectrometry (RBS)Elastic recoil detection analysis (ERD)Ion beam channelingReflection-high energy electron diffraction (RHEED)Scanning electron microscopy (SEM)Transmission electron spectroscopy (TEM)Electron spin resonance spectroscopy (ESR)Internal photoemission spectroscopy (IPE)

Ultraviolet-visible spectrophotometry (UV-VIS)Time resolved spectroscopyPhotoionization spectroscopyMass spectroscopyQuasi-elastic light scatteringHyper-Rayleigh scatteringHigh (pulsed) magnetic field photoluminescenceConfocal microscopyMagneto-optical KERR effectTransient photoconductivityFluorescence assisted cell sorter

Local probe techniques

Integrated physical properties

Scanning tunnelling microscopy(low temperature and vacuum)Scanning tunnelling spectroscopy(low temperature and vacuum)Atomic force microscopy(low temperature, ambient, in fluids)Magnetic force microscopy (low temperature)Scanning probe microscopy in fluidsScanning Hall probe microscopy

Time resolved, laser induced optoacoustic calorimetrySQUID magnetometryVibrating sample magnetometryHigh (pulsed) magnetic field resistivity and magnetizationMössbauer spectroscopyX-ray magnetic hyperfine spectroscopyNeutron scatteringCenter of mass spectroscopy (low temperature)Perturbed angular correlation spectroscopyI-V, C-V, and σ−V analysis

Modeling toolsTime dependent Ginzburg-LandauBogoliubov-de GennesAb-initio calculationsAbrikosov-Gor'kovKohn-Sham density functional theoremCar-Parrinello density functional theoremMolecular dynamics simulationsMonte-Carlo simulations

Scanning probe microscope

Cluster sourceand vaporisation laser

Calculated isosurfaces for the difference charge density in USn3

Page 8: Institute for Nanoscale Physics and Chemistry · X-ray diffraction (XRD) Auger spectroscopy X-rayphotoelectronspectroscopy(XPS) Micro-Raman and resonant Raman spectroscopy Rutherford

Institute for Nanoscale Physics and Chemistry

steering committeeProf. Victor V. MoshchalkovDirector INPACInstitute for Nanoscale Physics and ChemistryCelestijnenlaan 200 D, B-3001 LeuvenPhone: +32 16 327618Fax: + 32 16 327983E-mail: [email protected]

Prof. Arnout CeulemansVice-director INPACDepartment of ChemistryQuantum Chemistry and Physical ChemistryCelestijnenlaan 200F, B-3001 Leuven Phone: +32 16 327363 or +32 16 327356 Fax: +32 16 327992 E-mail: [email protected]

Prof. Mark Van der AuweraerDepartment of ChemistryMolecular and NanomaterialsPhotochemistry and SpectroscopyCelestijnenlaan 200F, B-3001 Leuven Phone: +32 16 327496 or +32 16 327418 Fax: +32 16 327990 E-mail: [email protected]

Prof. Chris Van HaesendonckDepartment of Physics and AstronomySolid State Physics and MagnetismNanophysics with Scanning ProbesCelestijnenlaan 200D, B-3001 Leuven Phone: +32 16 327501 or +32 16 327184 Fax: +32 16 327983 E-mail: [email protected]

Prof. André VantommeDepartment of Physics and AstronomyNuclear and Radiation PhysicsNuclear Solid State PhysicsCelestijnenlaan 200D, B-3001 Leuven Phone: +32 16 327514 or +32 16 327680 Fax: +32 16 327985 E-mail: [email protected]

E-mail: [email protected]: www.kuleuven.be/inpac

Prof. Koen ClaysDepartment of ChemistryMolecular and NanomaterialsMolecular Electronics and PhotonicsCelestijnenlaan 200D, B-3001 Leuven Phone: +32 16 327508 Fax: +32 16 327982 E-mail: [email protected]

Prof. Peter LievensDepartment of Physics and AstronomySolid State Physics and MagnetismClusters and Laser SpectroscopyCelestijnenlaan 200D, B-3001 Leuven Phone: +32 16 327207 or +32 16 327184 Fax: +32 16 327983 E-mail: [email protected]

Prof. Andre StesmansDepartment of Physics and AstronomySemiconductor PhysicsElectron Spin ResonanceCelestijnenlaan 200D, B-3001 Leuven Phone: +32 16 327179 or +32 16 327281 Fax: +32 16 327987 E-mail: [email protected]

Prof. Jozef VanderleydenDepartment of Microbial and Molecular Systems (M2S) Centre of Microbial and Plant GeneticsCell-cell interactionsKasteelpark Arenberg 20, B-3001 Leuven Phone: +32 16 329679 or +32 16 321631 Fax: +32 16 321966 E-mail: [email protected]

Prof. Johan VanackenScientific secretary INPACInstitute for Nanoscale Physics and ChemistryCelestijnenlaan 200 D, B-3001 LeuvenPhone: +32 16 327198Fax: + 32 16 327983E-mail: [email protected]

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