Facilities

The table below lists capabilities and facilities available to all members within the FLEET network and collaborators. Columns can be sorted by clicking on table headings. Use the search box to filter by keywords.

Equipment/FacilityFLEET ResearcherInstitute
Angle-resolved reflectivity measurementsElena OstrovskayaANU
CW Laser: M2 SolsTiS-7W-BRF-R
· Tunable Ti:Sapphire laser; 715 – 885 nm, 1W peak power
Elena OstrovskayaANU
Cryostat: Janis ST-500
· Continuous flow cryostat
· Temperature dependent measurements; 4K – 300K
Elena OstrovskayaANU
Exciton-polariton specific:
· Design and characterisation of optical microcavities and distributed Bragg reflectors for coupling light and excitons.
Elena OstrovskayaANU
Femtosecond Laser: Chameleon Ultra II
· 140-fs, 80-MHz Ti:Sapphire laser
· Tunable (680 – 1080 nm, >3.5 W average power at 800 nm)
Elena OstrovskayaANU
Photoluminescence measurements
· Near-field (real space) and far-field (momentum space) imaging
· Polarisation and time-resolved
· Temperature dependence (4K – 300K)
· Spectral resolution 0.015 nm
· Tunable CW pump: 715 – 885 nm
· Tunable femstosecond pump: 1060 – 1080 nm
· Fixed wavelength CW pump: 532 nm
· ps-resolution photon correlations measurements: g(2)(soon)
· Spatio-temporal coherence measurements: g(1)(r,t)
Elena OstrovskayaANU
Spectrometers: Acton IsoPlane SCT 320, Andor Kymera 328i, Andor Shamrock 500i
· Multi-channel monochromators/spectrographs
· 0.015-nm resolution
Elena OstrovskayaANU
Streak camera: Optronis SC-10
· 2-ps resolution streak camera
· Synchroscan for 80-Mhz laser
· Single-shot triggered mode
Elena OstrovskayaANU
Angle-Resolved Photoemission Spectroscopy Toroidal Analyser. Can be operated with monochromated helium light source off the synchrotron beam. Includes UHV sample preparation capabilities. Low-temperature STM (Omicron Fermi) with in situ sample transfer. Anton TadichAustralian Synchrotron
van der Waals fabrication facility: takes multiple images and constructs optical sample map - compares pictures to reference and uses contrast to identify possible thin-layer samplesJim HoneColumbia University
Nanoscale structural and electronic characterisation via STM, STS and ncAFM at 4KAgustin SchiffrinMonash University
Synchrotron-based x-ray techniques (XPS, NEXAFS, ARPES)Agustin SchiffrinMonash University
4K non-contact (qPlus) atomic force microscope, with optical accessAgustin SchiffrinMonash University
4K scanning tunneling microscope in UHV, with optical accessAgustin SchiffrinMonash University
Growth of low-dimensional organic nanostructures on surfaces. Atomic-scale structural and electronic characterisation via 4K STM, STS, ncAFM. Complementary characterisation via synchrotron based x-ray studies (photoelectron, absorption). Ultrafast pump-spectroscopy using ultrashort laser pulses.Agustin SchiffrinMonash University
Low-dimensional nanostructures and nanomaterialsAgustin SchiffrinMonash University
Ultrafast laser spectroscopyAgustin SchiffrinMonash University
UHV chamber with e-beam evaporator, and low- and high-temperature effucion cells for molecular beam epitaxy, and variable-temperature (50 - 1300 K) sample manipulatorAgustin SchiffrinMonash University
High-power (40 W) ytterbium laser (1028nm) generating <300 fs pulses, for single-cycle THz generation and pumping a tunable wavelength (650-16000 nm) optical parametric amplifier (<100 fs) (in progress)Agustin SchiffrinMonash University
CW pump laser, 532nm, 15 W (Spectra Physics Millennia Pro)Kris HelmersonMonash University
CW, stabilised,Ti:Sapphire tunable laser (Spectra Physics Matisse), 3 W, 750-870nm, dye laser conversion kitKris HelmersonMonash University
EMCCD camera (Andor iXon), single photon sensitivityKris HelmersonMonash University
EMCCD camera (Andor Luca)Kris HelmersonMonash University
Laser based micropipette puller (Sutter P-2000)Kris HelmersonMonash University
Laser scanning confocal microscope (Zeiss Pascal) on inverted microscope (Zeiss Axiovert)Kris HelmersonMonash University
Low temperature refrigerator, -80 CKris HelmersonMonash University
Microbalance (Mettler), 10 µg resolutionKris HelmersonMonash University
Motorised micromanipulators (Sutter M-285), <100nm positioningKris HelmersonMonash University
Photon counting system including APDs and correlatorKris HelmersonMonash University
Portable pumping station (dry pump backed turbomolecular) with residual gas analyserKris HelmersonMonash University
Refrigerated centrifugeKris HelmersonMonash University
Vacuum Oven, 220 degree CKris HelmersonMonash University
Experience in sample preparation capabilitiesMark EdmondsMonash University
UHV low-T STM (1 Micron Fermi)Mark EdmondsMonash University
Scanning Tunnelling Microscope x 2Michael FuhrerMonash University
In situ growth-films deposited through stencil mask onto pre-patterned electrodesMichael FuhrerMonash University
In situ growth-MBE chamber with UHV cold finger, 1T magnetMichael FuhrerMonash University
Chemical vapour deposition furnaces. One- and three-zone furnaces, for atmospheric-pressure or low-pressure CVD growth of materials. We have used these to prepare MoS2 and WS2 monolayers. Michael FuhrerMonash University
Electron-beam lithography. Modified FEI XL-40 scanning electron microscope with NPGS for electron-beam writing. Michael FuhrerMonash University
Low temperature probe station. Sample in vacuum. Can be operated at liquid nitrogen or liquid helium temperature. Michael FuhrerMonash University
Low-temperature scanning tunneling microscope #1: Microscope can be operated at 4.5 K, 77 K, 300 K. Magnetic field up to 1 Tesla. Capable of STM, scanning tunneling spectroscopy (STS), and quasi-particle interference (QPI) mapping. Five electrical contacts on sample holder (plus ground) enables resistivity and Hall effect. Some sample preparation capabilities (thermal evaporation of metals, sputtering). Optical microscope for aligning tip/sample capable of ~+/-10 micron accuracy in tip placement. Michael FuhrerMonash University
Low-temperature scanning tunneling microscope #2: Includes molecular beam epitaxy chamber with several sources (thermal and e-beam evaporation), RHEED. LEED available on transfer chamber. Microscope can be operated at 4.5 K, 77 K, 300 K. Magnetic field up to 1 Tesla. Capable of STM, scanning tunneling spectroscopy (STS), and quasi-particle interference (QPI) mapping. Five electrical contacts on sample holder (plus ground) enables resistivity and Hall effect. Thin film samples can be grown by MBE on pre-existing electrodes for in situ transport measurements. Michael FuhrerMonash University
Oxford cryostat suite (arriving end of 2018) with 14 Tesla magnet, 1.5 K variable temperature insert with one axis sample rotation, 3He refrigerator with one-axis sample rotation, and 3He/4He dilution refrigerator. Michael FuhrerMonash University
Physical Property Measurement System for electrical measurements at temperatures down to 2 K and magnetic fields to 7 Tesla. Michael FuhrerMonash University
Surface modification and electronic transport:-topological Dirac semimetal Na3BiMichael FuhrerMonash University
Surface modification and electronic transport:-topological insulator Bi2Se3Michael FuhrerMonash University
Thermal evaporator for metals deposition (e.g. Cr and Au electrodes).Michael FuhrerMonash University
Van der Waals heterostructure fabrication. One system is operational, includes temperature controlled stage, and is capable of rotational alignment of samples in addition to three-axis translations. This system will be placed in an argon glove box soon. Another system is being developed which should be operating in 2018.Michael FuhrerMonash University
First principles density functional theory models for atomic structure, electronic structure and chemical reactions Nikhil MedhekarMonash University
Large scale molecular dynamics simulations for morphology and chemical reactionsNikhil MedhekarMonash University
Non-equilibrium transport modelsNikhil MedhekarMonash University
Tight binding models for electronic structureNikhil MedhekarMonash University
Wannier functions based models for electronic structure, topological properties of the electronic structureNikhil MedhekarMonash University
National Computing Infrastructure Raijin: Fujitsu Primergy and Lenovo NeXtScale high-performance, distributed-memory clusterNikhil MedhekarNational Computing Infrastructure
RMIT Micro characterization and Microscopy Facility (RMMF)Kourosh Kalantar-zadehRMIT via the Centre for Advanced Electronics and Sensors (CADES)
Micro Nano Research Facility (MNRF)Kourosh Kalantar-zadehRMIT via the Centre for Advanced Electronics and Sensors (CADES)
Experience in electron and spin transport measurements:
-electric field gated device
-quantum oscillations
-point contact AndreeV reflection
-electrical-magneto coupling
Lan WangRMIT
Photon lithography and E-beam lithography routine techniques for device fabricationLan WangRMIT
Experience in magnetic measurements:
-DC magnetometry
-AC magnetometry
-quantum oscillations
Lan WangRMIT
2 glove box system for the fabrication of vdW heterostructuresLan WangRMIT
MPMS: 7 Tesla, 1.8 K for magnetic measurementsLan WangRMIT
PPMS: 9 Tesla, 1.8 K for electronic transport measurementsLan WangRMIT
Dielectric measurementsLan WangRMIT
Electric gated transport measurementsLan WangRMIT
Magnetoelectric coupling measurementsLan WangRMIT
Spin orbital torque measurementsLan WangRMIT
CVD system for the growth of nanostructureLan WangRMIT
Home made dielectric measurement system based on PPMSLan WangRMIT
Home made magnetoelectric coupling measurement system based on PPMSLan WangRMIT
Home made Photo current measurement system at low temperatureLan WangRMIT
Home made spin orbit torque measurement system based on PPMSLan WangRMIT
Magnetic Properties measurement system for magnetic measurements at low temperature up to 7 TeslaLan WangRMIT
Physical Property Measurement System for electrical measurements at temperatures down to 2 K and magnetic fields to 9 Tesla. Lan WangRMIT
Single crystal growth FurnaceLan WangRMIT
VdW stacking system for vdW heterostructure fabricationLan WangRMIT
Charge/exciton transport models in nanostructures.Jared ColeRMIT
Computational models of low dimensional structures (0, 1, 2, 3D).Jared ColeRMIT
Density Functional TheoryJared ColeRMIT
Finite-difference solutions to the Schroedinger equationJared ColeRMIT
Kinetic Monte-Carlo for charge transportJared ColeRMIT
Master equation descriptions of dissipation and dephasingJared ColeRMIT
Mathematical and computational models of advanced spectroscopyJared ColeRMIT
Non-equilibrium Greens function transport modelsJared ColeRMIT
Numerical models of disorderJared ColeRMIT
Superconductivity, superconducting circuit designJared ColeRMIT
Tight-binding modelsJared ColeRMIT
Existing Li-6 apparatus (p-wave, Bragg)Chris ValeSwinburne
Dy microscope (Synthetic TIs)Chris ValeSwinburne
Differential reflectance (absorption) hyperspectral imaging
·spatial resolution <500nm;
·polarization control/measurement
·electrical contacts possible
Jeff DavisSwinburne
Femtosecond transient absorption
·time resolution <20fs
·wavelength range 300nm - 950nm;
·degernerate or non-degenerate pump/probe;
·temperature down to 3K;
·spatial resolution <10um;
·electrical contacts possible;
·polarization control)
Jeff DavisSwinburne
Photoluminescence hyperspectral imaging
·spatial resolution <500nm;
·various cw pump wavelengths (410nm, 450nm, 530nm)
·polarization control/measurement
·electrical contacts possible
Jeff DavisSwinburne
Photocurrent imaging (<500nm resolution; various pump wavelengths)Jeff DavisSwinburne
Multi-dimensional Coherent spectroscopy
·For measurement of coherent dynamics, interactions between various excitations, Homogeneous/inhomogeneous broadening, coherent Raman spectroscopy, in many different configurations
Jeff DavisSwinburne
Time resolved photoluminescence
·(different techniques for different time ranges from <20fs to ms)
·temperature down to 3K;
·spatial resolution <10um;
·electrical contacts possible;
·polarization control/measurement)
Jeff DavisSwinburne
Visible/near-IR pump THz probe (for transient conductivity measurement)Jeff DavisSwinburne
Time domain THz spectroscopy
·can be used to measure conductivity
·single cycle THz pulse centred at 1THz
·spot size ~3mm
Jeff DavisSwinburne
Second harmonic generation imagingJeff DavisSwinburne
Base temperature <250mKAlex HamiltonUNSW
Beneq Atomic Layer Deposition System for dielectrics on GaAs devices.Alex HamiltonUNSW
Electrical measurements of 2D quantum devices at ultra-low temperatures: Leiden dilution fridge with top-loading insert, temperatures from 0.1-4K, equipped with a 9-5-1 vector magnet.Alex HamiltonUNSW
Electrical measurements of 2D quantum devices in high magnetic fields and at low temperatures: Oxford Kelvinox-400 (wet) dilution fridge, temperatures from 0.15-4K, equipped with a 15/17T magnet and 2 axis sample rotation system accurate to 0.01 degrees.Alex HamiltonUNSW
Electrical measurements of quantum devices at ultra-low temperatures: BlueFors dilution fridge with top-loading insert, temperatures from 0.1-4K, high frequency measurement compatible, equipped with a 5-1-1 vector magnet.Alex HamiltonUNSW
Heliox 3He cryostat with 2T magnetAlex HamiltonUNSW
Rapid electrical characterisation of quantum devices at low temperaturesAlex HamiltonUNSW
Rapid electrical characterisation: Homebuilt 15-300 cryogen free system with 1T resistive magnetAlex HamiltonUNSW
Powerful workstationDimitrie CulcerUNSW
Scanning probe microscopy (SPM) techniques (e.g. AFM, PFM, MFM, c-AFM, STM/STS, EFM, KPFM, ...Jan SeidelUNSW
Wide variety of tools available that work at temperatures from 4-600 K, magnetic fields up to 9 T, various gas environments, under light, under strain etc., that can study electrical, mechanical, magnetic, PV properties at the micron down to atomic length scales.Jan SeidelUNSW
Oxide materials, especially ferroelectric and multiferroic materialsJan SeidelUNSW
Cary 5000 UV-Vis spectroscopy systemKourosh Kalantar-zadehUNSW
HHV ATS 500 e-beam evaporation and sputtering systemKourosh Kalantar-zadehUNSW
Heidelberg MLA100 maskless alignerKourosh Kalantar-zadehUNSW
JEOL JSM-IT500HR/LA FE SEM with Nabity NPGS EBL and EDS functionKourosh Kalantar-zadehUNSW
PIE Scientific Tergeo 150 W plasma cleanerKourosh Kalantar-zadehUNSW
Julabo SL-6 heating circulatorKourosh Kalantar-zadehUNSW
Sonics VCX 750 Ultrasonic ProcessorKourosh Kalantar-zadehUNSW
Renishaw InVia2 micro-Raman/PL with 355, 532, and 830 nm laser;Kourosh Kalantar-zadehUNSW
Synthesis of epitaxial ferroelectric, ferromagnetic and multiferroic thin films using pulsed laser deposition (PLD)Nagy ValanoorUNSW
Synthesis of semiconductor thin films (GaP, etc.) using pulsed laser deposition (PLD)Nagy ValanoorUNSW
X-ray diffraction: D8 Discover rotating anode thin film diffractometerNagy ValanoorUNSW
Philips MRD materials research diffractometerNagy ValanoorUNSW
Pulsed laser deposition:
Pascal (Japan) oxide laser molecular beam epitaxy (L-MBE) system with in-situ confocal laser microscope
Neocera ultrahigh vacuum pulsed laser deposition system (semiconductors, metals, etc.)
Neocera oxide pulsed laser deposition system (complex oxides such as BiFeO3, SrRuO3, PZT, etc.)
Nagy ValanoorUNSW
Rigaku SmartLab rotating anode thin film diffractometerNagy ValanoorUNSW
Expertise in undoped electron and hole mesoscopic devices in GaAs. QED @ UNSW and SP @ Cambridge are the only ones who have developed the required fabrication techniques.Oleh Klochan & Alex HamiltonUNSW & Cambridge
Fabrication facilities at ANFF NSW node:
-Cleanroom class 100: E-beam writer Raith 150TWO, SEM, ALD, Photolithography, Thermal evaporators, annealers, etc
Oleh Klochan & Alex HamiltonUNSW
Cryogenic facilities @QED UNSW:
-Four dilution fridges
-helium 3 system
Oleh Klochan & Alex HamiltonUNSW
Fabrication of semiconductor based mesoscopic devices and their electronic transport characterization at ultralow temperatures and high magnetic fields.Oleh KlochanUNSW
High-performance XPS: Nexsa Surface Analysis system.
- detection
of low concentration components, and a micro-focused spot for small
feature analysis (10um to 400uc in 5um steps)
- Ultra-violet photoelectron spectroscopy, UPS integration
- Dual-mode ion source (MAGCIS) for expanded depth profiling capabilities
Xiaolin WangUOW