Heidelberg Luminescence Laboratory
Institute of Geography
Heidelberg University

Im Neuenheimer Feld 348
Phone: +49 6221 54-4725

Location

 
Postal adress
Heidelberg Luminescence Laboratory
Institute of Geography
Heidelberg University

PO Box: 103980
69029 Heidelberg
Germany
 
Staff
Dr. Annette Kadereit
Felizitas Wolf
Jutta Asmuth
Christian Müller
Prof. Dr. Günther A. Wagner
 

Luminescense Laboratory

The Heidelberg Luminescence Laboratory at the Institute of Geography conducts optical dating of sediments and stone surfaces as well as scientific and technological development of the optical stimulated luminescence technique. The laboratory is endowed by the university with two permanent positions, the laboratory head (Dr. Annette Kadereit) and a technical assistant (Felizitas Wolf).

Luminescence dating

Luminescence dating is a dosimetric dating technique based on the steady decay of radionuclides present almost everywhere in the natural environment and the steadily increasing radiation damage caused in non-conductors, like mineral grains. The natural radioactivity functions as a driving clockwork and the mineral grains serve as a readable clock. The clock ticks within sedimentary deposits and other archives which are used by researchers in the palaeo-environmental and archaeological sciences to reconstruct the evolution of a landscape, the history of an archaeological site or the interaction of man and his environment in the geological and historical past, in disciplines such as geomorphology, geoarchaeology and archaeometry.


Fig. 1: Ionizing radiation in a soil or sediment
Dating is performed with common quartz and feldspar grains that are found more or less ubiquitously on the earth's surface. As a result of the radioactive decay of the radionuclides (mainly 40K and 87Rb) and the radioactive decay chains (mainly from 238U, 235U and 232Th) present in a sedimentary deposit, an ionizing radiation is emitted which leads to measurable radiation damages within the crystal lattices of the quartz and feldspar minerals (Fig. 1). Within the non-conductors the activated electrons are lifted from the valence band to the conduction band and may be trapped at lattice defects where they are stored in meta-stabile states (Fig. 2, top). The larger the amount of trapped electrons is, the longer was the time during which mineral grains were exposed to the ionizing radiation.


Fig. 2: Filling and emptying of OSL-traps as illustrated by the energy-band model


The geo-clock may be read by using luminescence techniques. By supplying energy, the trapped electrons are released from their meta-stable states whereupon they recombine by emitting a cold light: the luminescence signal (Fig. 2, bottom). Depending on the kind of stimulating energy, the technique is called thermally-stimulated luminescence (TL) or optically-stimulated luminescence (OSL) dating. Further specification is possible with respect to the stimulating wavelength, e.g. in the near infrared (infrared-stimulated luminescence = IRSL) or in the visible range, such as, e.g. by blue LEDs (blue-light stimulated luminescence = BLSL). As the strength of the luminescence signal corresponds to the number of trapped electrons which correlate with the time of exposure to the ionizing radiation it is possible to use luminescence techniques for the dating of sediments. Generally, an older sample delivers a stronger luminescence signal than a younger sample. The correlation between the amount of energy a crystal has received, which is denoted in kilojoule per kilogram (kJ/kg) or Gray (Gy), and the strength of the corresponding luminescence signal has to be determined and calibrated for each sample individually. This is done by the construction of a growth-curve, for which the strengths of the luminescence signals of a sample are plotted against known doses administered to the sample in the laboratory using calibrated radioactive sources (Fig. 3). By fitting the strength of the natural luminescence signal of a sample into the sample's growth curve the palaeodose (also equivalent dose (DE)) is then calculated. In order to determine the age of a sample, we also need to know the strength of the ionizing radiation per time-unit (e.g. per thousand years = 1 ka), i.e. the environmental dose rate (Gy/ka). The dose rate can be measured using low level gamma spectrometry, or alpha-counting and beta-counting, or a combination of these. The age of a sample may be calculated according to the simplified age-equation:

age [ka] = dose [Gy]  ⁄  dose rate [Gy/ka]


Fig. 3: Additive (left) and regenerative (right) growth curve

Project cooperations

The Heidelberg Luminescence Laboratory cooperates in projects which need to establish chronometries for past landscape changes induced by environmental changes or human impact. Archives to reconstruct the history of a landscape are usually aeolian, fluvial or colluvial deposits. Sedimentary archives are usually the most important key to the past in geomorphological and geoarchaeological projects (examples 2 - 7). Man-made stoneworks may also be analyzed (example 1). In any case the assumption is that the luminescence clock was reset to zero by daylight at the time of the dating event, similar to a stop-watch, and that it started clicking anew right afterwards due to the surrounding natural radioactivity and the subsequent exclusion of light or heat impact.

For case studies please refer to the German homepage.

History

In the summer of 2007 the Heidelberg Luminescence Laboratory was relocated from the former Research Unit Archaeometry of the Heidelberg Academy of Sciences at the Max-Planck Department of Nuclear Sciences (head until June 2007: Prof. Dr. Günther A. Wagner) to the Institute of Geography of the Heidelberg University.

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Latest Revision: 2011-10-26
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