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Heidelberger Lumineszenzlabor
Geographisches Institut
Universität Heidelberg
Im Neuenheimer Feld 348
69120 Heidelberg, Germany
magdalena.biernacka@uni-heidelberg.de
olaf.bubenzer@uni-heidelberg.de
sebastian.kreutzer@uni-heidelberg.de

 

I am an experimental physicist working with materials that exhibit long-lived stimulated luminescence phenomena. My particular interest is finding explanations for luminescent phenomena in minerals to expand the possibilities of their use in geochronology with a focus on luminescence dating.

 

I am geographer, geomorphologist and geoarchaeologist and heading the working group “Geomorphology and Soil Geography". My main scientific interest is the physical-geographical investigation of drylands and Central Europe during the Quaternary, including human-nature interaction. I am fellow of the Marsilius Kolleg and founding director of the Heidelberg Center for the Environment (HCE).

 
Supervisor: Dr Sebastian Kreutzer

I am a geographer, geochronologist and data scientist. In a broader perspective, as a geographer, I am interested in the recognition of rapid landscape changes during the last 2.58 million years, for example, on aeolian sediment sequences. To achieve this aim, I am working with 'luminescence dating', which I am steadily trying to advance to obtain more accurate and precise ages. A crucial part of my daily work is data analysis and modelling. My preferred language is R.

 
Funding

Project: 101107989 - Lyoluminescence - HORIZON-MSCA-2022-PF-01

 

Research Project

The last formation: dating recrystallisation events of evaporites using lyoluminescence

What are we up to?

We are supporting a sustainable future! Understanding Earth’s past 2.58 million years is crucial for mitigating climate change-induced risks to our modern societies. Climate and landscape change forecast models draw their data from studies about the past. The Marie Skłodowska-Curie project, lyoluminescence (LL), explores innovative ways to date past landscape changes. We aim to achieve a breakthrough in developing lyoluminescence as a dating tool on salts (sodium chloride and potassium chloride) for application in Earth Sciences.

We think that LL, naturally observable in salt minerals, says something about the last recrystallization event. The underlying idea is an old story, and various scholars have suggested the potential of halite as a material for optical luminescence dating, e.g., Bailey et al., (2000); Zhang et al., (2005). However, LL may offer an additional luminescence-dating tool for routine use in geochronology by targeting the crystallization instead of heat or light exposure events. If subsurface processes where hydration matters are of interest, LL may open new ways of understanding those processes.

How does it work? (the nutshell)

Lyoluminescence is a form of chemiluminescence wherein luminescence light is emitted during the solvation of previously irradiated crystals. An example of an LL signal observation experiment is depicted in Fig. 1. Here, sodium chloride previously exposed to ionizing radiation was dissolved in pure water at approximately 60 °C with the aid of magnetic stirring. However, it's important to note that the green glow seen in the right photo is merely an illustration of potential LL emission. Detecting such faint signals requires the use of highly sensitive devices, like a photomultiplier in single photon counting mode. Moreover, such measurements need to be conducted within a meticulously designed measurement chamber to prevent interference from external light sources.

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Figure 1: Stages of conducting an LL experiment: 1) A beaker with distilled water on a magnetic stirrer; 2) Heating the water to a specific temperature; 3) Introducing previously irradiated salt (not depicted in the photo) into the beaker while stirring to observe the LL phenomenon. The green glow was added during the post-processing of the photo to illustrate the lyoluminescence signal. In this instance, the commercial camera sensor lacked the necessary sensitivity to detect the faint LL signal. For a real recording of LL, please see our photos below.

This phenomenon was initially described by Wiedemann and Schmidt in 1895. According to the current, simplified understanding of LL mechanisms (see Fig. 2) proposed by Atari in 1980, when an alkali halide crystal comes into contact with a solvent (such as water), it releases a hydrated electron (e-aq) from an F-center (the defect that captured the electron). Subsequently, the rapid recombination of the hydrated electron, primarily with a V2-center, at the solid-liquid interface results in light emission, known as lyoluminescence (in Fig. 2 depicted as hν). The typical shape of the LL signal (referred to as the LL glow curve) recorded with a photomultiplier tube in time is illustrated in Fig. 2, depicted in the graph on the left. The intensity of LL light increases proportionally with the radiation dose absorbed by the material after crystallization (see Fig. 2 graph on the right). This positive correlation between radiation dose and LL light emission makes crystal lattice defects suitable as natural ionizing radiation dosimeters. For instance, sodium chloride dissolved in pure water exhibits a saturation dose of approximately 10 kGy (Atari et al., 1973). Given realistic dose rates of about 4 Gy/ka (Han et al., 2014), the LL signal from sodium chloride minerals could potentially determine an age of up to 2.5 million years!

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Figure 2: The concept of lyoluminescence.

Even weak LL light can be enhanced and registered!

The intensity of LL depends on several factors, including grain size, sample mass, solvent pH and temperature, absorbed dose, and the type of impurities present. One of the most significant factors affecting the intensity of luminescence is the presence of special chemical compounds, added to enhance the LL signal. These compounds interact with hydrated electrons released during the dissolution of the crystal. As a result, light emission occurs both at the solid-liquid interface (lyoluminescence) and within the solution (chemiluminescence).

Various chemicals were used to achieve this effect, for example, a luminol solution. However, we employed an aqueous solution of copper chloride with an optimally selected concentration as the solvent1, which influences the dissolution process. Copper cations, forming complex compounds with chloride ions in aqueous solution, have significantly accelerated the dissolution process of tested salt samples. More importantly, this solution does not exhibit photoluminescent properties, providing a stable background during measurements, unlike luminol. The light emission produced during dissolution in the copper chloride solution is enhanced at least ten times compared to dissolution in pure water. This approach facilitates the detection of weak LL signals during the dissolution of natural minerals, potentially allowing for practical applications of this method. An example of such emissions, recorded using a high-sensitive EM-CCD camera for gamma-irradiated rock salt, is shown in Figure and Movie 3.

1 in collaboration with Dr hab. Krzysztof Staninski, Prof UAM (Department of Rare Earths, Faculty of Chemistry, Adam Mickiewicz University, Poznań, Poland)

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Fig. and Mov. 3. Actual luminescence emission was captured using an ANDOR iXon Ultra 888 back-illuminated EM-CCD camera during the dissolution of laboratory gamma-irradiated powdered rock salt in a copper chloride solution. Images were taken with a frame rate of one image every 3 s over 30 s. The image and movie were created in collaboration with Dr Michał Sądel (The Henryk Niewodniczański Institute of Nuclear Physics, Polish Academy of Sciences, Kraków, Poland). Note: colours do not correspond to the wavelength of the light emitted during the experiment but were chosen for better visualisation (the actual emission peak sits around 500 nm).

Where can it be applied?

Widely distributed natural deposits (as depicted in Fig. 4), highly soluble in water, and salts such as halite and/or sylvite found in areas of high aridity are promising candidates for LL dating applications. Of particular interest are naturally discoloured alkali halides, including blue variants of rock salt (Atari et al., 1973), which are characterized by a significant concentration of radiation-induced crystal defects (examples of blue halites are shown in Fig. 5).

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Figure 4. Locations of known large salt deposits in Europe.

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Figure 5. Naturally discoloured (top) aggregates of the blue and purple halites surrounded by white sylvite, (bottom) variants of blue and purple halites; Morsleben repository (BGE), Saxony-Anhalt, Germany.

What are the project objectives?
  1. Pooling strategic knowledge on lyoluminescence on evaporites and its potential applications, specifically halite and sylvite.
  2. Design, develop and test a new portable lyoluminescence reader.
  3. Apply the newly developed device to natural salt and develop dating protocols and analysis routines; if successful, map out a commercialization plan.
References
  • Atari, N.A., 1980. Lyoluminescence mechanism of gamma and additively coloured alkali halides in pure water. Journal of Luminescence 21, 305–316. https://doi.org/10.1016/0022-2313(80)90009-5
  • Atari, N.A., Ettinger, K.V., Fremlin, J.H., 1973. Lyoluminescence as a possible basis of radiation dosimetry. Radiation Effects 17, 45–48. https://doi.org/10.1080/00337577308232596
  • Bailey, R.M., Adamiec, G., Rhodes, E.J., 2000. OSL properties of NaCl relative to dating and dosimetry. Radiation Measurements 32, 717–723. https://doi.org/10.1016/S1350-4487(00)00087-1
  • Han, W., Ma, Z., Lai, Z., Appel, E., Fang, X., Yu, L., 2014. Wind erosion on the north‐eastern Tibetan Plateau: constraints from OSL and U‐Th dating of playa salt crust in the Qaidam Basin. Earth Surf Processes Landf 39, 779–789. https://doi.org/10.1002/esp.3483
  • Wiedemann, E., Schmidt, G.C., 1895. Ueber Luminescenz von festen Körpern und festen Lösungen. Annalen der Physik und Chemie 292, 201–254. https://doi.org/10.1002/andp.18952921004
  • Zhang, J.F., Yan, C., Zhou, L.P., 2005. Feasibility of optical dating using halite. Journal of Luminescence 114, 234–240. https://doi.org/10.1016/j.jlumin.2005.01.009
Milestones
    What did we do so far?
  • The first portable LL reader prototype was completed
  • First LL signal from natural samples
  • In progress:
  • New dating protocol for LL
  • Commercialisation strategy for LL equipment
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Letzte Änderung: 17.09.2024
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