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Equipment

  • 3D-LS

    3D-PCCS

    Photon Cross Correlation Spectroscopy (PCCS) is a powerful extension of the well established Photon Correlation Spectroscopy (PCS). While PCS is limited to highly diluted systems, with PCCS it is possible to study multiple scattering systems like suspensions or emulsions.

    Model: 3D-PCS (LS Instruments) equipped with a He-Ne laser (Thorlabs, wavelength 632.8 nm)

  • ALV

    2D-PCS

    Goniometer setup:

    The setup is equipped with a multiple-τ digital correlator (ALV-Laser Vertriebsgesellschaft mbH, Langen, Germany) and an argon-ion laser; λ = 514.5 nm) as light source.
    Model: ALV-5000 goniometer setup + Spectra Physics argon ion laser (Stabilite 2017) (ALV GmbH )

  • FW

    2D-PCS

    Fixed angle setup:

    Self-build setup with a fixed light scattering detection at an angle of 60°. The used light source is an He-Ne laser with a wavelength of 632.8 nm.
    Model: ALV-5000E correlator; scattering angle: 60°; He-Ne laser (Thorlabs, continuous output 21mW)

  • HT-LS

    High temperture setup:

    Self-build setup with a goniomter and a ALV 7004/USB correlator combined with ALV / LSE-5004 software. The light source is a COMPASS DPSS Laser from Coherent with a wavelengh of 532 nm and 100 mW power. The housing of the index matching bath is made of teflon.

  • DDLS

    Depolarized Dynamic Light Scattering

  • ESS

    Sample Enviroment for SKADI, ESS Lund

    In the framework of the development of the European Spallation Source (ESS) in Lund a sample environment combining in-situ dynamic light scattering (DLS), diffusing wave spectroscopy (DWS) and small angle neutron scattering (SANS) will be developed using an universal carrier system.

    A fibre optical setup with a HeNe laser light source (λ=633 nm) and three phtoton counting detectors will be employed which allows the usage of a sample changer with external temperature control.

    DLS measurments can be carried out at two different q vectors in forward and backscattering geometry. As DLS measurements are limited to highly diluted samples the installation of a DWS unit in transmission mode will also allow the invesigation of turbid samples.

  • TEM

    Cryo-TEM

    Model: JEOL JEM-2200FS

    Acceleration voltage: 80 – 200kV
    ZrO/W(100) Schottky-Emitter
    Piezo controlled sample stage
    TEM-point resolution at 200 kV: 0,23 nm
    In-column energy filter for EFTEM and EELS, energy resolution: 0,8 eV (zero-loss FWHM)
    EDX with SDD-Detektor (JEOL)
    4k x 4k CMOS-Camera (Gatan OneView)
    STEM BF- und DF-Detectors
    Single-tip, analytical double-tip, tomography, heating and cryotransfer specimen holders

    Contact: Yvonne Hannappel

    User services

  • SEM

    SEM

    Details: The Phenom proX-G3 from IB-FT company is a small Desktop scanning electron microscope (SEM) which allows quick and easy measurments. The magnification ranges from 20- to 45000 times with an acceleration voltage between  5,10 or 15kV. The SEM is equipped with a backscattering detector (BSE) with topographic contrast mode and also with a energy dispersive X-ray detector (EDX) for element- detection, -quantification and mapping.

    For the investigation of samples with a low electric conductivity it is often necessary to coat the sample with a thin film of metal. We use a Polaron E-5000 sputter coater unit with a palladium target.

    Model: IB-FT (Thermo) Phenom proX-G3 with BSE and EDX and Polaron E-5000 sputter coater (Pd)

    Contact: Uwe Güth

    REM_Nutzerordnung_2024.pdf

The Xeuss SAXS/WAXS System from Xenocs constists of a GeniX 3D Cu Ultra low divergence source, a collimation system composed of two scatterless slits and a Pilatus 300K Detector from Dectris, 20 Hz. We use the system to analyse and resolve structures from various samples ranging from 0.5 to 120 nm. The system covers experiments including WAXS/SAXS, GISAXS, and Reflectometry.

Model: Xeuss SAXS/WAXS System

Contact: Tim Julian Stank
The instrument Nanotrac Wave II is an analyzer which combines Dynamic Light Scattering (DLS), particle size and zeta potential measurements.
The design of the instrument allows measurements of samples over a wide concentration range, monomodal or multimodal samples, all without prior knowledge of the particle size distribution.

Nanotrac Wave II

Contact: Marco Annegarn
  • Ellipsometry

    Ellipsometry

    The SE 400adv from Sentech is a laser ellipsometer with a sabilized HeNe laser. The ellipsometer can be used to measure the thickness of a single layer film with a precision of up to 0.1 Å. For multiple angle measurements the angle of incidence can be varied from 40° - 90° in 5° steps. Furthermore the ellipsometer can be mounted with a liquid cell.

    Model: Sentech SE 400adv

  • AFM

    AFM

     

    Model: Nanosurf FlexAFM

    Contact: Marco Annegarn

  • Tensiometer

    Tensiometer

    Model:

    Contact:

     

  • Contact angle and Pendent Drop

  • Spinning Drop

The Microtime 200 Time-resolved confocal fluorescence microscope combines the usual confocal setup with a high time resolution (down to ~10 ps). The confocal setup consists of 4 different laser lines (405, 485, 510 and 640 nm), the respective dichroic mirrors (the wavelengths of 485 and 640 nm can be measurements simultaneously with a two-band dichroic) the Olympus IX71 inverted microscope (equipped with a 60x water objective) and different pinholes. A Picoharp 300 together with two Avalanche Photo diodes make up the detection system. Together with a piezo sample stage, this setup allows for example: TCSPC, FLIM, FCS and fluorescence anisotropy.

Model: PicoQuant MicroTime 200

Contact: Andreas Brockhinke
  • FTIR

    FT-Infrared Spectrometer

    Model: Bruker IFS 66v + pulsed Nd:YAG laser (Spectra Physics GCR-12) + OPO (OPTA)

    Contact: AG Tilman Kottke

  • UVVis

    UV/Vis Spectrometer

Princeton Applied Research

The available Physica MCR 101 can be used for various rheological measurements such as oscillatory or steady shear experiments (parallel plate, cone plate or cylinder geometry). With the additional light scattering setup the structure formation in diluted polymer solutions with an applied shear strain can be analyzed. The accompanying software offers an immediate evaluation and graphical display of experimental results.

Model: Physica MCR 101 with 658 nm laser (Anton Paar)
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