Labs and equipment AG Wende

Labs

Laboratory Room Phone
MBE/XPS Lab MD 441 2974
BESSY/MBE Lab MD 442 2975
Mössbauer Lab MD 443 2940
XRD Lab MD 446 2956
AFM Lab MF 234 2185
SQUID Lab MC 233 2791
PLD Lab I BB 1016 3576
PPMS/PLD Lab II LN 2.46 8136
Workshop MD 447 2388
Chemistry Lab MD 463 2978
F-Praktikum: Experiment 3.1 Mössbauer spectroscopy MD 443 2940
F-Praktikum: Experiment 3.2 Gamma ray spectroscopy MC 227 1915
F-Praktikum: Experiment 11.1 LEED-AES MC 224 1629
XPS/CEMS in MD 441

XPS/CEMS

This chamber is used for the preparation of thin film samples by molecular beam epitaxy (MBE) and in situ characterization via XPS, CEMS and AES.

Read more
MBE/CEMS in MD 442

MBE/CEMS

UHV system for the preparation of samples by MBE and for CEMS measurements.

Read more
MBE chamber in MD 443

MBE

This UHV system serves exclusively for the preperation of thin films by molecular beam epitaxy (MBE). It's fitted with a load lock to transfer samples into and out of the chamber. The sample temperature can be varied between 130 and 970 K. For the computer-controlled evaporation process, up to five resistively heated evaporation cells with Al2O3 crucibles and an electron gun are available.

PLD chamber in BB 1016

Pulsed Laser Deposition PLD

This setup is used for the growing of thin films by laser induced ablation from different premade targets, using a crypton-fluorine excimer laser (KrF, 248nm, power up to 200mJ). This process is usually performed in high vacuum (down to 10-5mbar) or in the presence of oxygen gas if oxide targets are being used. During film growth, the targets are continuously rotating, to avoid excessive local heating and to achieve a homogenous evaporation of the material. The temperature of the substrate can also be controlled up to 900°C in manual or automatic mode. Our PLD setup can be used for multilayer film deposition from three different targets without having to vent the chamber. Before commencing film growth, the deposition rate can be checked by a vibration quartz monitor mounted on a movable arm, also serving as a shutter. Successfully prepared samples include multiferroic cobalt ferrite nanopillars in a barium titanate matrix. (article link)

UHV-PLD in 2.46 (NETZ)

UHV-PLD

To complement the existing PLD system, a new setup was constructed in the NETZ-building, comprising of a UHV-capable PLD system that was put into operation on the 25th of January 2018. The vacuum chamber, made available by the University of Ulm, features a highly developed system for target rotation, translation, and the switching between different target materials. Thanks to this, complex alloys, composites and multilayers can be produced automatically and under controlled conditions.

BESSY-chamber in MD 442

Bessy Chamber

This portable UHV chamber is designed for measurements of X-ray absorption (XAS) at synchrotron sources, especially BESSY in Berlin. As a key component the chamber contains a water-cooled coil system. With its help X-ray magnetic circular dichroism (XMCD) can be measured in a static applied magnetic field (up to 50 mT at present).

Read more
UHV plasma chamber

UHV Plasma Chamber

The UHV plasma chamber has been built within the scope of a bacholor thesis in our group. It is used for in situ low pressure plasma treatment of thin films and nanoparticles. Contaminations like organic ligands or oxides are removed from  the samples, which can then be directly transferred into the main chamber. In general, the plasma chamber is mounted to our BESSY-chamber but may be used together with any other UHV system that uses CF flanges. A seperate pumping station allows the pressure to be controlled independently from the main chamber when mounting or cleaning samples.

The key component of the plasma chamber is a glass recipient with an external induction coil to excite the plasma inductively by a HF field. A precision valve serves as entry gate for the plasma gases, in general hydrogen or oxygen, and allows for pressure control. Typically, the pressure during the cleaning process is kept in the range of 10-2 mbar for best cleaning results.

Mössbauer cryostat in MD 443

Low Temperature Mössbauer Spectrometers

We have several bath cryostats from CryoVac and Thor Cryogenics at our disposal that can be used for Mössbauer transmission measurements with either liquid helium or nitrogen. The internal setup with vacuum-insulation, an outer and an inner tank allow for longterm measurements at stable low temperatures. The sample is surrounded by helium gas to facilitate the heat exchange, but the sample chamber can also be evacuated for higher temperature measurements. Thanks to sample holders with integrated electric heaters, measurements can be performed from 4.3 K up to room temperature.

In addition to Mössbauer spectroscopy, these cryostats can also be used for electrical transport measurements, thanks to the existing electrical connections of the sample holders, allowing the recording of e.g. temperature dependent resistivity curves.

High-field magnet cryostat in MD 443

High-Field Magnet Cryostat

This lHe magnet cryostat from Thor Cryogenics (Project No. 77483) contains a superconducting magnet in split-coil geometry, which is able to apply a magnetic field of up to 5 T.

In standard configuration, this setup is suitable for Mössbauer transmission measurements with an applied field in either in-axis or off-axis direction. The sample temperature can be set between 2.2 K and 300 K by a system with two interconnected helium tanks, also making it possible to perform Hall measurements, as well as the recording of characteristic resistivity curves.

Mössbauer oven (middle) in MD 443

Mössbauer Oven

This vacuum oven allows us to record Mössbauer spectra at temperatures up to 800 K. Powder samples are usually pressed into flat disks, which are then mounted between two beryllium plates in a heated sample holder. Latter is inserted into a tube that's fitted with thin windows made of aluminated Mylar, allowing radiation to pass through while being able to hold a vacuum. Using an electromagnet, measurements can also be performed in an applied magnetic field perpendicular to the gamma ray direction, at field strenghts of up to 0.9 T.

This setup is also used for the experiment 3.1 "Mössbauer Spektroskopie" of the advanced laboratory training course, to offer students an insight into this measurement method.

MVT-1000 & MVC-450 in MD 443

High-Speed Mössbauer Setup

The Mössbauer Velocity Calibrator MVC-450 from WissEl allows the calibration of the Mössbauer-drive by a laser interferometer, in contrast to the regular method of using an iron foil with known properties. This device is used for high-speed measurements, widening our range by increasing the velocity of the Mössbauer driving unit. The use is necessitated by the fact that the regular method can't offer a precise calibration for higher speeds. This also requires the use of a high-speed Mössbauer Velocity Transducer, the MVT-1000, capable of running at up to 1000 mm/s. An example for high speed measurements are samples with strong temperature-depended line broadening, such as ferrofluids.

Peltier sample holders in MD 443

ex situ Peltier Sample Holder

These special sample holders were constructed for temperature dependend ex situ Mössbauer measurements. Equipped with watercooled Peliter-elements, they allow a sample to be cooled (heated) by 75 K relative to the cooling water temperautre.

They are mainly used for sensitive samples that can't be measured in regular cryostats, such as ferrofluid samples with high water content that would dehydrate in the low pressure sample chamber of a cryostat. To minimize thermal loss, the sample is surrounded by a styrofoam mantle, with the temperature being recorded by a PT100 thermocouple. To further enhance performance, the cooling water temperature is actively controlled by an external refrigeration unit.

CEMS cryostat in MD 443

Low Temperature CEMS

For low temperature conversion electron Mössbauer spectroscopy measurements down to 80 K, several sample holders were fitted with gas feedthroughs, which can be inserted into our existing cryostats.

For measurements down to 4.3 K, a self-built CEMS counter was installed into a CryoVac Helium bath cryostat. This counter uses a channeltron instead of the usual proportional counter. The cryostat has an inner tank filled with liquid helium and an outer tank filled with liquid nitrogen. For measurements above 4.3 K the sample can be electrically heated up to 340 K. By means of an additional electromagnet, CEMS measurements in an external magnetic field of up to 1 T can be performed at temperatures down to 80 K.

CEMS in MD 443

ex situ CEMS

For ex situ CEMS measurements at room temperature, a gas flow proportional counter is used as a detector due to the large solid angle covered. Helium/Methane gas flows continuously through a small proportional counter containing the absorber (sample). The conversion and Auger electrons leaving the sample surface are absorbed in the gas volume with high probability. Using an electrcomagnet, measurements in magnetic fields up to 1.3 T can also be performed. For measurements from RT up to 450 K, a CEMS oven is also available.

XRD in MD 446

X-Ray Diffractometer

For x-ray diffraction measurements (small angle, high angle and Rocking-curves), we use a commercial θ-2θ X-ray diffractometer PW1730 from Philips. It's equipped with a horizontal goniometer, a Cu/Co/Mo anode X-ray tube and a graphite monochromator. The measurements are performed at room temperature.

AFM in MF 234

AFM

An atomic force microscope is available for the nanoscale examination of surface topography. The Q-Scope 350 is equipped with a PC-based video subsystem using a CCD camera for 90 degree tip and sample viewing, and an X-Y translation stage for sample positioning. An acoustic/vibration isolation chamber and a compressed air dampened measurement table provide the environment needed for excellent resolution in sub-micron scan sizes. The system is capable of the following scan modes: Contact Mode, Lateral Force Mode, Intermittent Contact Mode, Phase Mode.

MPMS-5S in MC 233

Superconducting Quantum Interference Device (SQUID) Quantum Design MPMS-5S

The Magnetic Property Measurement System from Quantum Design is a SQUID magnetometer, used for the field and temperature dependent analysis of sample magnetization, possessing a sensitivity of up to 10-11 Am2  (10-8 emu). Its standard equipment includes a superconducting magnet, with which a magnetic field of up to ±5 T can be applied, and a temperature controller, making it possible to set the sample temperature between 4 K and 400 K.

Read more
PPMS in 2.46 (NETZ)

Quantum Design PPMS DynaCool

The Quantum Design Physical Property Measurement System was put into operation in June 2014 and is collectively used by four workgroups. The modular setup allows the use of a wide range of different measurement methods for electric and thermal transport, while a vibrating sample magnetometer (VSM) option facilitates very rapid magnetic measurements with sensitivities of up to 10-9 Am2 (10-6 emu). Magnetic fields of ±9 T can be applied, while the sample temperature can be set between 1.8 K and 400 K in regular operation, or between 300 K and 1000 K with the VSM oven.

Read more
Glovebox & fume hood in MD 463

Chemistry Laboratory Glovebox and Fume Hood

For chemical work such as sample preparation and synthesis, a chemistry lab is available. It's equipped with an argon glovebox, enabling sensitive samples to be prepared and handled in an oxygen- and water-free atmosphere. For any work that might cause a release of gas, aerosol or dust, a fume hood is also available, equipped with the usual gas, water, and electrical outlets.