Konstanz, Univ., Diss., 2001.

The present thesis is devoted to the investigation of novel superconductors by phase-sensitive terahertz transmission and infrared to ultraviolet spectroscopy. In particular, a nominally undoped Pr2CuO4 superconducting thin film, an FeTe0.5Se0.5 thin film, and a LiFeAs single crystal have been investigated. The emphasis is on the low-frequency part of the optical spectrum (i.e., the terahertz and infrared spectrum), as the goal of the study was to shed light on the size and symmetry of the superconducting gaps and also to determine the temperature dependences as well as the absolute values of the penetration depth, which are key input parameters for models applicable for new superconductors. In addition, niobium has been investigated as a reference, so as to see what is expected from conventional superconductors and to clarify the electrodynamics of niobium. A superconducting Nb thin film with Tc of 8.04 K has been investigated by backward wave oscillator-based (BWO-based) and time-domain terahertz (TDT) spectrometers in the frequency range between 4 and 100 cm−1 for temperatures ranging from 2 to 10 K. From these measurements an energy gap of 22.50 cm−1 = 2.79 meV = 4.02kBTc have been determined. The optical conductivity below Tc could nicely be described by calculations according to the Eliashberg theory, with the electron-phonon interaction evaluated from tunneling measurements. Absolute values of the penetration depth have been calculated from phase-sensitive terahertz measurements. The zero-temperature limit of at T = 0 is found to be 115 ± 5 nm. From this value, a London penetration depth of 43 ± 2 nm has been obtained. The overall temperature dependence of the penetration depth follows a behavior typical for conventional s-wave superconductors. A superconducting Pr2CuO4 film with T0 structure and Tc of 27 K has been investigated by use of optical methods in a wide frequency (5 – 55000 cm−1) and temperature (2 – 300 K) range. A Drude-like peak centered at zero frequency is observed in the optical conductivity below 150 K, above which it shifts to finite frequencies. The detailed analysis of the low-frequency conductivity reveals that the Drude peak and a far-infrared (FIR) peak centered at about 300 cm−1 persist at all temperatures. The FIR spectral weight is found to grow at the expense of the Drude spectral weight with increasing temperature. Absolute values of the penetration depth have been obtained from temperature and frequency-dependent measurements. The zero-temperature limit of is estimated to be 1600 ± 100 nm. The overall temperature dependence of follows a behaviour typical for cuprate superconductors. However, a closer look at the penetration depth at T 12 K reveals a flattening in the temperature dependence. A superconducting FeTe0.5Se0.5 thin film with Tc = 19 K has been investigated using a combination of BWO and TDT spectroscopy in the frequency range 4 - 80 cm−1 and between 3 and 150 K. From such measurements, a superconducting energy gap of 30 cm−1, representing a coupling strength = 2.27, is observed. Further, the penetration depth has been derived from the temperature dependence of the imaginary part of complex conductivity with the penetration depth = 530 ± 10 nm at lowest measured temperature. The temperature-dependent normalized superfluid density, just as is the case with most iron-based superconductors, could nicely be described by the so-called two-gap gamma model. Finally, a superconducting LiFeAs single crystal with Tc = 18 K has been investigated by optical spectroscopy in the frequency range 15 - 55000 cm−1 between 5 and 300 K. From these measurements, no clear signature of the superconducting energy-gap opening could be identified in spite of the spectral weight been suppressed in the infrared frequency regime below Tc. This indicates that LiFeAs single crystal is in a clean limit. With the aid of the Ferrell-Glover-Tinkham (FGT) sum rule, an absolute penetration depth of 215 nm has been calculated from the missing area at 5 K.

The present thesis is devoted to the investigation of novel superconductors by phase-sensitive terahertz transmission and infrared to ultraviolet spectroscopy. In particular, a nominally undoped Pr2CuO4 superconducting thin film, an FeTe0.5Se0.5 thin film, and a LiFeAs single crystal have been investigated. The emphasis is on the low-frequency part of the optical spectrum (i.e., the terahertz and infrared spectrum), as the goal of the study was to shed light on the size and symmetry of the superconducting gaps and also to determine the temperature dependences as well as the absolute values of the penetration depth, which are key input parameters for models applicable for new superconductors. In addition, niobium has been investigated as a reference, so as to see what is expected from conventional superconductors and to clarify the electrodynamics of niobium. A superconducting Nb thin film with Tc of 8.04 K has been investigated by backward wave oscillator-based (BWO-based) and time-domain terahertz (TDT) spectrometers in the frequency range between 4 and 100 cm−1 for temperatures ranging from 2 to 10 K. From these measurements an energy gap of 22.50 cm−1 = 2.79 meV = 4.02kBTc have been determined. The optical conductivity below Tc could nicely be described by calculations according to the Eliashberg theory, with the electron-phonon interaction evaluated from tunneling measurements. Absolute values of the penetration depth have been calculated from phase-sensitive terahertz measurements. The zero-temperature limit of at T = 0 is found to be 115 ± 5 nm. From this value, a London penetration depth of 43 ± 2 nm has been obtained. The overall temperature dependence of the penetration depth follows a behavior typical for conventional s-wave superconductors. A superconducting Pr2CuO4 film with T0 structure and Tc of 27 K has been investigated by use of optical methods in a wide frequency (5 – 55000 cm−1) and temperature (2 – 300 K) range. A Drude-like peak centered at zero frequency is observed in the optical conductivity below 150 K, above which it shifts to finite frequencies. The detailed analysis of the low-frequency conductivity reveals that the Drude peak and a far-infrared (FIR) peak centered at about 300 cm−1 persist at all temperatures. The FIR spectral weight is found to grow at the expense of the Drude spectral weight with increasing temperature. Absolute values of the penetration depth have been obtained from temperature and frequency-dependent measurements. The zero-temperature limit of is estimated to be 1600 ± 100 nm. The overall temperature dependence of follows a behaviour typical for cuprate superconductors. However, a closer look at the penetration depth at T 12 K reveals a flattening in the temperature dependence. A superconducting FeTe0.5Se0.5 thin film with Tc = 19 K has been investigated using a combination of BWO and TDT spectroscopy in the frequency range 4 - 80 cm−1 and between 3 and 150 K. From such measurements, a superconducting energy gap of 30 cm−1, representing a coupling strength = 2.27, is observed. Further, the penetration depth has been derived from the temperature dependence of the imaginary part of complex conductivity with the penetration depth = 530 ± 10 nm at lowest measured temperature. The temperature-dependent normalized superfluid density, just as is the case with most iron-based superconductors, could nicely be described by the so-called two-gap gamma model. Finally, a superconducting LiFeAs single crystal with Tc = 18 K has been investigated by optical spectroscopy in the frequency range 15 - 55000 cm−1 between 5 and 300 K. From these measurements, no clear signature of the superconducting energy-gap opening could be identified in spite of the spectral weight been suppressed in the infrared frequency regime below Tc. This indicates that LiFeAs single crystal is in a clean limit. With the aid of the Ferrell-Glover-Tinkham (FGT) sum rule, an absolute penetration depth of 215 nm has been calculated from the missing area at 5 K.

Die Protonentherapie von Aderhautmelanomen wird vor allem für die Behandlung von Tumoren nahe kritischer Strukturen (Sehnerv) und bei großen Tumoren angewandt. Dabei ist die begrenzte Reichweite der Protonen vorteilhaft, die scharf begrenzte Dosisfelder im Auge ermöglicht, und das an den Tumor grenzende gesunde Gewebe bestmöglich schont. Daher erfolgt die Positionierung der Patienten und der Strahlenfelder in der Augentumortherapie, wie auch die regelmäßigen Konstanzprüfungen, mit einer Reichweitengenauigkeit in Wasser von 0,1 mm. Mit einem Multi-Leaf Faraday Cup (MLFC) kann die Reichweite der Protonen in kurzer Zeit sehr genau gemessen werden. Dabei misst der MLFC die differentielle Fluenz der Protonenstrahlen, also das Reichweitenprofil. Er besteht aus einem Stapel Folien, abwechselnd leitend und isolierend. Eindringende Protonen deponieren eine zusätzliche Ladung in der Folie in der sie stoppen. Durch eine gleichzeitige Strommessung an allen Folien misst der MLFC relativ schnell die Reichweite der Protonen. Aufgabe dieser Arbeit ist es, einen MLFC entsprechend den Anforderungen der Augentumortherapie zu entwickeln, aufzubauen und mögliche Anwendungspotentiale zu untersuchen. Dafür wurden Monte-Carlo-Rechnungen mit MCNPX 2.6 und SRIM durchgeführt, verschiedene Folienstapel an Luft und im Vakuum untersucht, verschiedene Messelektroniken zur gleichzeitigen Messung von Strömen im pA-Bereich in vielen Kanälen getestet, ein Absorbersystem für einen variablen Messbereich von 30 MeV bis 70 MeV aufgebaut und die entsprechende Mess- und Steuersoftware in LabVIEW 2011 entwickelt. Es wurde die Genauigkeit der Reichweitenmessungen untersucht und gezeigt, dass der MLFC durch seine Mobilität eine schnelle Energiebestimmung an unterschiedlichen Experimentierplätzen erlaubt. In der Therapie ist neben der einfachen Bestimmung der maximalen Reichweite der Protonen auch die regelmäßige Kontrolle der Modulation der ausgedehnten Bragg-Kurven möglich. / Proton therapy of uveal melanomas is primarily used for the treatment of tumors near critical structures (optic nerve) and in large tumors. The great advantage of protons is their sharply limited range in tissue, which leads to sharp defined dose fields in the eye and the dose absorbed by the healthy tissue around the tumor can be reduced. Therefore, the positioning of the patient and the radiation fields, as well as the regular control measurements in the eye tumor therapy requires an accuracy of 0.1 mm in water. A Multi-Leaf Faraday Cup (MLFC) gives the opportunity to measure the proton range relatively fast and accurate. The MLFC measures the differential fluence, which means the range profile of the proton beam. It consists of a stack of sheets, alternating conductive and insulating, and the penetrating protons bring their additional charge into the sheet in which they stop. By measuring the corresponding current in each conducting sheet at the same time, the MLFC can quickly measure the range of the protons. The task of this work is to develop a MLFC with respect to the requirements of the eye tumor therapy and to explore possible application potentials. Therefore, Monte Carlo calculations with MCNPX 2.6 and SRIM were conducted, various foil stacks were studied in air and in vacuum, different measurement electronics for measuring currents in the pA range in many channels simultaneously were tested, a system of degraders for a variable measuring range from 30 MeV to 70 MeV was developed and the corresponding measurement and control software was written in LabVIEW 2011. The accuracy of the range measurements was examined and it was shown that a quick energy measurement at different target stations can be made by the MLFC due to its mobility. In therapy, in addition to the determination of the maximum range of the proton beam, the regular monitoring of the modulation of the extended Bragg-curves is in principle possible.

Um der Mikrowellenerwärmung als Single- oder Hybridanwendung im industriellen Ofenbau ein weiteres Anwendungsspektrum zu eröffnen, wird dem Anlagenkonstrukteur im Rahmen dieser Arbeit eine Aufstellung von Entwicklungsprioritäten und Konstruktionshinweisen übergeben. Für eine energieeffiziente Ausnutzung des technologischen Potenzials wird hierbei nicht - wie in der Vergangenheit - die Feldstärkenverteilung, sondern das Reflexionsverhalten in den Vordergrund gestellt. Durch die Entwicklung und den Aufbau eines Messplatzes zur Bestimmung temperaturspezifischer Dielektrizitätsparameter konnte die Realitätsnähe der Simulation für die anwendungsorientierte Applikatorentwicklung gesteigert werden. Die Anwendbarkeit der Auslegungskriterien wird im Rahmen der Projektierung und des Aufbaus einer Beispielanlage zur Entbinderung von keramischen Grünkörpern und bei der Entwicklung zahlreicher mikrowellenspezifischer Anlagenbauteile verifiziert.

Um der Mikrowellenerwärmung als Single- oder Hybridanwendung im industriellen Ofenbau ein weiteres Anwendungsspektrum zu eröffnen, wird dem Anlagenkonstrukteur im Rahmen dieser Arbeit eine Aufstellung von Entwicklungsprioritäten und Konstruktionshinweisen übergeben. Für eine energieeffiziente Ausnutzung des technologischen Potenzials wird hierbei nicht - wie in der Vergangenheit - die Feldstärkenverteilung, sondern das Reflexionsverhalten in den Vordergrund gestellt. Durch die Entwicklung und den Aufbau eines Messplatzes zur Bestimmung temperaturspezifischer Dielektrizitätsparameter konnte die Realitätsnähe der Simulation für die anwendungsorientierte Applikatorentwicklung gesteigert werden. Die Anwendbarkeit der Auslegungskriterien wird im Rahmen der Projektierung und des Aufbaus einer Beispielanlage zur Entbinderung von keramischen Grünkörpern und bei der Entwicklung zahlreicher mikrowellenspezifischer Anlagenbauteile verifiziert.

Zur Aufklärung der lokalen Magnetisierungs- und magnetischen Streufeldstruktur in ferromagnetischen und supraleitenden Materialien wurden magnetkraftmikroskopische (Magnetkraftmikroskopie-MFM) Untersuchungen durchgeführt und quantitativ ausgewertet. Für eine solch quantitative Auswertung muss der Einfluß der verwendeten MFM-Spitzen auf das MFM-Bild bestimmt und in geeigneter Weise subtrahiert werden. Hierzu wurden Spitzenkalibrierungsroutinen und ein Verfahren zur Entfaltung der gemessenen MFM-Daten implementiert, das auf der Wiener Dekonvolution basiert. Mit Hilfe dieser Prozedur können sowohl die räumliche Ausdehnung als auch die Größe der Streufelder direkt aus gemessenen MFM-Bildern bestimmt werden. Gezeigt wurde diese Anwendung für die Durchmesserbestimmung von Blasendomänen in einer (Co/Pd)-Multilage und für die Bestimmung der temperaturabhängigen magnetischen Eindringtiefe in einem supraleitendem BaFe2(As0.24P0.76)2 Einkristall. Desweiteren konnte durch die Kombination von mikromagnetischen Rechnungen und der quantitativen MFM-Datenanalyse die Existenz einer dreidimensionalen Vortex-Struktur am Ende von Co48Fe52-Nanodrähten nachgewiesen werden. Damit ist es gelungen die Tiefensensitivität der Magnetkraftmikroskopie erfolgreich in die Rekonstruktion der vermessenen Magnetisierungsstruktur einzubeziehen.

The Antimatter Experiment: Gravity, Interferometry, Spectroscopy (AEGIS) at the European Organization for Nuclear Research (CERN) is an experiment investigating the influence of earth’s gravitational force upon antimatter. To perform precise measurements the antimatter needs to be cooled to a temperature of 100 mK. This will be done in a Penning trap, formed by several electrodes, which are charged with several kV and have to be individually electrically insulated. The trap is thermally linked to a mixing chamber of a 3He-4He dilution refrigerator. Two link designs are examined, the Rod design and the Sandwich design. The Rod design electrically connects a single electrode with a heat exchanger, immersed in the helium of the mixing chamber, by a copper pin. An alumina ring and the helium electrically insulate the Rod design. The Sandwich uses an electrically insulating sapphire plate sandwiched between the electrode and the mixing chamber. Indium layers on the sapphire plate are applied to improve the thermal contact. Four differently prepared test Sandwiches are investigated. They differ in the sapphire surface roughness and in the application method of the indium layers. Measurements with static and sinusoidal heat loads are performed to uncover the behavior of the thermal boundary resistances. The thermal total resistance of the best Sandwich shows a temperature dependency of T-2,64 and is significantly lower, with roughly 30 cm2K4/W at 50 mK, than experimental data found in the literature. The estimated thermal boundary resistance between indium and sapphire agrees very well with the value of the acoustic mismatch theory at low temperatures. In both designs, homemade heat exchangers are integrated to transfer the heat to the cold helium. These heat exchangers are based on sintered structures to increase the heat transferring surface and to overcome the significant influence of the thermal resistance (Kapitza resistance). The heat exchangers are optimized concerning the adherence of the sinter to the substrate and its sinter height, e.g. its thermal penetration length. Ruthenium oxide metallic resistors (RuO2) are used as temperature sensors for the investigations. They consist of various materials, which affect the reproducibility. The sensor conditioning and the resulting good reproducibility is discussed as well.

Zur Aufklärung der lokalen Magnetisierungs- und magnetischen Streufeldstruktur in ferromagnetischen und supraleitenden Materialien wurden magnetkraftmikroskopische (Magnetkraftmikroskopie-MFM) Untersuchungen durchgeführt und quantitativ ausgewertet. Für eine solch quantitative Auswertung muss der Einfluß der verwendeten MFM-Spitzen auf das MFM-Bild bestimmt und in geeigneter Weise subtrahiert werden. Hierzu wurden Spitzenkalibrierungsroutinen und ein Verfahren zur Entfaltung der gemessenen MFM-Daten implementiert, das auf der Wiener Dekonvolution basiert. Mit Hilfe dieser Prozedur können sowohl die räumliche Ausdehnung als auch die Größe der Streufelder direkt aus gemessenen MFM-Bildern bestimmt werden. Gezeigt wurde diese Anwendung für die Durchmesserbestimmung von Blasendomänen in einer (Co/Pd)-Multilage und für die Bestimmung der temperaturabhängigen magnetischen Eindringtiefe in einem supraleitendem BaFe2(As0.24P0.76)2 Einkristall. Desweiteren konnte durch die Kombination von mikromagnetischen Rechnungen und der quantitativen MFM-Datenanalyse die Existenz einer dreidimensionalen Vortex-Struktur am Ende von Co48Fe52-Nanodrähten nachgewiesen werden. Damit ist es gelungen die Tiefensensitivität der Magnetkraftmikroskopie erfolgreich in die Rekonstruktion der vermessenen Magnetisierungsstruktur einzubeziehen.:Introduction 6 1 Contrast formation in Magnetic Force Microscopy (MFM) 9 1.1 Type of interactions . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 9 1.1.1 Relevant interaction forces . . . . . . . . . . . . . . . . . . . . . . . 9 1.1.2 Magnetic interaction mechanisms . . . . . . . . . . . . . . . . . . . 11 1.2 Basic magnetostatics of the tip-sample system . . . . . . . . . . . . . . . . 12 1.2.1 General magnetostatic expressions . . . . . . . . . . . . . . . . . . . 12 1.2.2 Description of the tip sample system . . . . . . . . . . . . . . . . . 14 1.2.3 Magnetostatics in Fourier space . . . . . . . . . . . . . . . . . . . . 15 2 Instrumentation 20 2.1 Scanning Force Microscopy (SFM) . . . . . . . . . . . . . . . . . . . . . . . 20 2.1.1 Measurement principle and operation modes . . . . . . . . . . . . . 20 2.1.2 Dynamic mode SFM . . . . . . . . . . . . . . . . . . . . . . . . . . 21 2.2 Lift mode MFM . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 24 2.3 Non-contact MFM . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 25 2.4 Vibrating Sample Magnetometry . . . . . . . . . . . . . . . . . . . . . . . 26 3 Quantitative Magnetic Force Microscopy 28 3.1 The challenge of MFM image inversion . . . . . . . . . . . . . . . . . . . . 28 3.1.1 Description of the problem and state of the art . . . . . . . . . . . 28 3.1.2 The point probe approximations . . . . . . . . . . . . . . . . . . . . 31 3.1.3 The transfer function approach . . . . . . . . . . . . . . . . . . . . 33 3.2 Tip calibration: Adapted Wiener deconvolution . . . . . . . . . . . . . . . 39 3.2.1 Details of the procedure . . . . . . . . . . . . . . . . . . . . . . . . 39 3.2.2 Evaluation of possible errors . . . . . . . . . . . . . . . . . . . . . . 44 3.3 Noise measurements . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 47 3.4 MFM probes and their specific characteristics . . . . . . . . . . . . . . . . 49 3.5 Calibration samples . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 54 3.6 Detection of tip-sample modification . . . . . . . . . . . . . . . . . . . . . 55 4 Quantitative MFM with iron filled carbon nanotube sensors (Fe-CNT) 56 4.1 The monopole character of Fe-CNT sensors . . . . . . . . . . . . . . . . . . 57 4.1.1 Calibration within the point probe approximation . . . . . . . . . . 57 4.1.2 Calibration results and discussion . . . . . . . . . . . . . . . . . . . 59 4.1.3 Quantitative MFM on a [Co/Pt]/Co/Ru multilayer . . . . . . . . . 62 4.2 Inplane sensitive MFM with Fe-CNT sensors . . . . . . . . . . . . . . . . . 63 4.2.1 Bimodal MFM technique . . . . . . . . . . . . . . . . . . . . . . . . 63 4.2.2 Comparison between calculated and measured in-plane contrast . . 66 5 Quantification of magnetic nanoobjects in MFM measurements 70 5.1 Bubble domains in a [Co/Pd]80 multilayer . . . . . . . . . . . . . . . . . . 71 5.1.1 Micromagnetic model . . . . . . . . . . . . . . . . . . . . . . . . . . 72 5.1.2 MFM image simulation . . . . . . . . . . . . . . . . . . . . . . . . . 72 5.1.3 Results and discussion . . . . . . . . . . . . . . . . . . . . . . . . . 74 5.2 Quantitative assessment of the magnetic penetration depth in superconductors 78 5.2.1 Comparison of methods . . . . . . . . . . . . . . . . . . . . . . . . 79 5.2.2 Experimental determination of the temperature dependent penetration depth in a BaFe2(As0:24P0:76)2 single crystal . . . . . . . . . . . 83 6 Magnetization studies of CoFe nanowire arrays on a local and global scale 87 6.1 Revisiting the estimation of demagnetizing fields in magnetic nanowire arrays 88 6.1.1 Available approaches . . . . . . . . . . . . . . . . . . . . . . . . . . 88 6.1.2 Calculation of demagnetizing fields in nanowire arrays . . . . . . . . 91 6.2 Micromagnetic Simulations . . . . . . . . . . . . . . . . . . . . . . . . . . . 99 6.3 Combination of demagnetizing field calculations and micromagnetic simulation100 6.4 Experimental details . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 102 6.5 Global hysteresis measurements of CoFe nanowire arrays with varying length 104 6.6 Local magnetic characterization of a CoFe nanowire array by quantitative MFM . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 107 6.6.1 Magnetic structure of individual nanowires . . . . . . . . . . . . . . 107 6.6.2 Magnetization reversal of the nanowire array . . . . . . . . . . . . . 110 6.7 Summary . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 117 Conclusions and Outlook 119 Bibliography 121 Acknowledgements 135

The Antimatter Experiment: Gravity, Interferometry, Spectroscopy (AEGIS) at the European Organization for Nuclear Research (CERN) is an experiment investigating the influence of earth’s gravitational force upon antimatter. To perform precise measurements the antimatter needs to be cooled to a temperature of 100 mK. This will be done in a Penning trap, formed by several electrodes, which are charged with several kV and have to be individually electrically insulated. The trap is thermally linked to a mixing chamber of a 3He-4He dilution refrigerator. Two link designs are examined, the Rod design and the Sandwich design. The Rod design electrically connects a single electrode with a heat exchanger, immersed in the helium of the mixing chamber, by a copper pin. An alumina ring and the helium electrically insulate the Rod design. The Sandwich uses an electrically insulating sapphire plate sandwiched between the electrode and the mixing chamber. Indium layers on the sapphire plate are applied to improve the thermal contact. Four differently prepared test Sandwiches are investigated. They differ in the sapphire surface roughness and in the application method of the indium layers. Measurements with static and sinusoidal heat loads are performed to uncover the behavior of the thermal boundary resistances. The thermal total resistance of the best Sandwich shows a temperature dependency of T-2,64 and is significantly lower, with roughly 30 cm2K4/W at 50 mK, than experimental data found in the literature. The estimated thermal boundary resistance between indium and sapphire agrees very well with the value of the acoustic mismatch theory at low temperatures. In both designs, homemade heat exchangers are integrated to transfer the heat to the cold helium. These heat exchangers are based on sintered structures to increase the heat transferring surface and to overcome the significant influence of the thermal resistance (Kapitza resistance). The heat exchangers are optimized concerning the adherence of the sinter to the substrate and its sinter height, e.g. its thermal penetration length. Ruthenium oxide metallic resistors (RuO2) are used as temperature sensors for the investigations. They consist of various materials, which affect the reproducibility. The sensor conditioning and the resulting good reproducibility is discussed as well.