FM is performed by inserting a Bertrand lens in the light path of a conventional microscope with Köhler illumination which images the Fourier image formed at the back focal plane of the objective. It allows to determine the structure of fluid and crystalline ordered suspensions (Phys. Rev. E. 77, 061401 (2008)).
If an additional aperture is placed at the back focal plane, the q-range from which the image is constructed may be restricted. This can be used to omit any positional information of particles within a crystal and construct the image from zeroth order light and incoherently superimposed 1st order diffractions of uncorrelated objects like grain boundaries, holes, dislocations etc. The Bragg diffracted light is missing from the zeroth order diffraction leading to a colour coding of different crystal structures. missing Such a technique is useful for fast wide area scans of crystal quality and structure.
BM in principle is an inverted light scattering experiment. Instead of illuminating the sample in a direction normal to its surface and recording the Bragg diffracted light, it is illuminated under an angle fulfilling the Laue condition and only the light of properly oriented crystals is reflected into the objective of the microscope. This e.g. allows to monitor the competing growth of wall and bulk crystals or of oriented twin domains after succession of shear (J. Chem. Phys. 137, 094906 (2012)).
Further, Differential Interference Contrast Microscopy, Phase Contrast Microscopy, Polarization Microscopy, particle location and tracking analysis, and standard AFM are frequently used. Examples show particle trajectories towards a growing crystallite with three domains grown at an HCl releasing seed. Particles are identified to be in a crystalline environment by bond-order analysis.
Continuous deionization of Colloids
Working with charged sphere suspensions requires salt concentration levels of 10-6M and below. We have developed and perfected a continuous conditioning system, which guarantees such values, but also allows to adjust higher levels under conductometric control (J. Phys. Chem. 96, 8180-8183 (1992)). Further it shear melts all colloidal crystals, homogenizes the suspension prior to investigation, and is flexibly connecting to all our experiments (J. Chem. Phys. 114, 7556 - 7562 (2001)).
Combined Bragg and Small Angle light scattering
Both the bragg scattering and the small angle scattering regime are accessible with this instrument with high angular and temporal resolution, thus probing the sample both at the length scale of typical particle distances and lattice constants and the length scale of its micro-structure. The two rotating detector arms collect light from the full azimuthal range and leave the fragile sample undisturbed (PRX submitted 1.2014). This set-up and its prototype (Nuovo Cimento D 16, 1149-1157 (1994)) herited from late K. Schätzel were used to study the solidification kinetics of sterically stabilized PMMA hard spheres (J. Coll. Interface Sci. 207, 119 - 127 (1998), collaboration with W. v. Megen) and PS-microgel hard spheres (J. Chem Phys. 130, 084502 (2009), Phys. Rev. E 79, 010601(R) (2009), Phys. Rev. Lett. 102, 038302 (2009), collaboration with E. Bartsch and H. J. Schöpe). In the shown example the SALS signal exhibits dynamic scaling and originates from a foam-like micro structure formed within the polycrystalline sample during coarsening (Phys. Rev. E 81, 051401 (1-20) (2010)).
Combination Light Scattering Experiment
This is one of our main work horses, as it allows the simultaneous measurement of static, dynamic and elastic properties of our samples on a two arm goniometer with three independently optimized illumination and detection optics (J. Colloid Interface Sci. 234, 149-161 (2001). Combination with the continuous deionization further facilitates additional simultaneous measurements of e.g. conductivity) It was e.g. used to determine structure and concentration dependent elasticity (J. Chem. Phys. 109, 10068 - 10074 (1998)), compare different experimental effective charges to theoretical calculations (J. Chem. Phys. 116, 10981 – 10988 (2002), Colloid. Surf. A 270, 220 - 225 (2005), J. Chem. Phys. 125, 194714 (2006)) and test theoretical expectations for the phase behaviour and properties of binary charged sphere mixtures (Phys. Rev. E 80, 021407 (2009), J. Chem. Phys. 133, 104501 (2010).
2-Colour Cross Correlation
Dynamic Light Scattering (DLS) is a standard technique to investigate the particle dynamics of colloidal suspensions. These particle dynamics are described by the Intermediate Scattering Function (ISF). The ISF is not directly accessible with a standard DLS experiment in non-ergodic samples. Many techniques have been developed to measure the ensemble averaged particle dynamics in non-ergodic samples: Interleaved sampling (Prog. Colloid Polymer Sci. 100, 121-126 (1996), Echo method (Rev. Sci. Instrum. 75, 2419 (2004)). and Multispeckle Correlation Spectroscopy (MSCS) (J. Chem. Phys. 104, 1758-1761 (1996)). In our group, we use MSCS with a special optical detection setup to determine the ensemble averaged as well as the subensemble resolved particle dynamics simultaneously (AIP Conf. Proc. 1518, 304-307 (2013)). This makes the MSCS a powerful tool to investigate e.g. the ageing behavior of colloidal glasses or the dynamical heterogeneities in meta-stable colloidal samples.
Differential Dynamic Microscopy
Superheterodyne Doppler Velocimetry
For electrokinetic measurements we employ a low angle, incoherent, super-heterodyne, integral Laser Doppler Velocimetry in reference beam mode. This new machine (Condens. Matter 24, 464109 (19pp) (2012)) combines the advantages of integral measurements across the complete cell cross section (allowing simultaneous determination of electro-phoresis and electro-osmosis) with super-heterodyning (allowing separation of the actual heterodyne signal from low frequency noise and homodyne contributions) and low angle measurements (allowing measurements independent of system structure). This machine is used for concentration dependent mobility measurements in electric fields (Phys. Rev. Lett. 98, 176105 (1-4) (2007)) as well as structural changes under hydrostatic and/or electro-phoretic flow (J. Chem. Phys. 119, 3360 – 3370 (2003), Colloid Surfaces B 56, 210 – 219 (2007)). The example shows the distribution of coexisting meta-stable phases under electro-phoretic shear as inferred from simultaneous Velocimetry and structure measurements in the XY cross section.