Earth Surf. Dynam., 3, 5565, 2015 www.earth-surf-dynam.net/3/55/2015/ doi:10.5194/esurf-3-55-2015 Author(s) 2015. CC Attribution 3.0 License.
A. C. Cunningham1,2, J. Wallinga3, N. Hobo3,4,5, A. J. Versendaal3, B. Makaske3,4, and H. Middelkoop5
1School of Geosciences, University of the Witwatersrand, Johannesburg, South Africa
2Centre for Archaeological Science, School of Earth and Environmental Sciences, University of Wollongong, Wollongong, Australia
3Soil Geography and Landscape group & Netherlands Centre for Luminescence dating, Wageningen University, Wageningen, the Netherlands
4Alterra, Wageningen University and Research Centre, Wageningen, the Netherlands
5Department of Physical Geography, Utrecht University, Utrecht, the Netherlands
Correspondence to: A. C. Cunningham ([email protected])
Received: 20 June 2014 Published in Earth Surf. Dynam. Discuss.: 2 July 2014 Revised: 24 November 2014 Accepted: 22 December 2014 Published: 16 January 2015
Abstract. The optically stimulated luminescence (OSL) signal from uvial sediment often contains a remnant from the previous deposition cycle, leading to a partially bleached equivalent-dose distribution. Although identication of the burial dose is of primary concern, the degree of bleaching could potentially provide insights into sediment transport processes. However, comparison of bleaching between samples is complicated by sample-to-sample variation in aliquot size and luminescence sensitivity. Here we begin development of an age model to account for these effects. With measurement data from multi-grain aliquots, we use Bayesian computational statistics to estimate the burial dose and bleaching parameters of the single-grain dose distribution. We apply the model to 46 samples taken from uvial sediment of Rhine branches in the Netherlands, and compare the results with environmental predictor variables (depositional environment, texture, sample depth, depth relative to mean water level, dose rate). Although obvious correlations with predictor variables are absent, there is some suggestion that the best-bleached samples are found close to the modern mean water level, and that the extent of bleaching has changed over the recent past. We hypothesise that sediment deposited near the transition of channel to overbank deposits receives the most sunlight exposure, due to local reworking after deposition. However, nearly all samples are inferred to have at least some well-bleached grains, suggesting that bleaching also occurs during uvial transport.
1 Introduction
The use of optically stimulated luminescence (OSL) for dating Holocene uvial deposits is widespread. However, u-vial sediments are not ideal for OSL dating because the intensity of sunlight under water may not be sufcient to reset the OSL signal in some grains prior to their deposition.The remnant OSL signal can then cause the burial dose to be overestimated, leading to an overestimate of the age. This
Re-evaluating luminescence burial doses and bleaching of uvial deposits using Bayesian computational statistics
phenomenon is referred to as poor, partial or heterogeneous bleaching (e.g. Wallinga, 2002a).
While the burial age is usually the primary consideration, there are good reasons to quantify the degree of bleaching too. Firstly, it may provide information on the robustness of an OSL age. Secondly, the degree of bleaching might yield information on the sediment source or sediment-transport processes (e.g. Reimann et al., 2015). For instance, if a tsunami deposit appears well bleached, it could indicate that shallow shore-face or intertidal deposits provided the pri-
Published by Copernicus Publications on behalf of the European Geosciences Union.
56 A. C. Cunningham et al.: Re-evaluating burial doses and bleaching of uvial deposits
mary sediment source (Murari et al., 2007). For uvial deposits, poor bleaching might, for instance, reect short transport distances or an old deposit acting as the primary source.
To compare the bleaching between samples, it is rst necessary to distinguish between the part of the equivalent dose (De) built up since the time of deposition and the poorly bleached remnant dose. Previous studies have avoided this issue by deliberately sampling modern or known-age sediment. Such studies have indicated that bleaching is better in coarse sand-sized grains compared to ner grains (Olley et al., 1998; Truelsen and Wallinga, 2003), and may be dependent on depositional context (Murray et al., 1995; Schielein and Lomax, 2013) and transport distance (Stokes et al., 2001;Jain et al., 2004; and references therein).
Nevertheless, the inherent variability from sample to sample makes denitive conclusions hard to come by. The main problem arises in distinguishing signal from noise: how much of the sample-to-sample variation in bleaching is due to physical processes, as opposed to random statistical uctuations? Studies focusing on modern or known-age deposits seldom have enough samples for condent conclusions to be drawn, and no study has quantied the variation between adjacent samples. Moreover, the review of Jain et al. (2004) showed a discrepancy in residual doses of modern uvial samples compared to young known-age samples, with modern samples yielding larger residual doses. They argued that modern deposits may yet be remobilised, so their transport history is not representative of deposits preserved in the stratigraphic record.
Here we focus not on modern samples but on samples of various ages that have already been used for age estimation.This approach allows for more samples to be included, and avoids the bad-modern-analogue issue, but presents the additional problem of separating out the burial dose from the remnant dose. For this purpose we have designed an age model specically for these young, partially bleached De distributions. We dene the degree of bleaching by the proportion of grains that were well bleached upon deposition, rather than by the remnant dose. We apply the model to a suite of 46 samples from embanked oodplains of the lower Rhine in the Netherlands, and correlate the outcome with geomorphic data for each sample.
2 Methods
2.1 Samples and measurements
We use a data set of OSL measurements on a suite of 46 samples from embanked oodplain deposits formed during the past 700 years. Different parts of the data set have been presented by Hobo et al. (2010, 2014) and Wallinga et al. (2010).Samples come from four different sites, all located in the Rhine Delta in the Netherlands (Fig. 1). At each of the sites, several cores (diameter 1419 cm) were taken in a cross section perpendicular to the river course (see Hobo et al., 2010,
Figure 1. Map showing the sample sites. The sites Brummen and Zwolle are along the river IJssel, whereas the other two sites (Neerijnen and OB1-3) are along the river Waal. Both are branches of the river Rhine. OB1-3 refers to two cores from the Hiensche Uiterwaarden and one core from the Gouverneursche polder.
for examples). Samples were extracted from the cores in subdued orange light and prepared using methods described by Wallinga et al. (2010). For each of the sample sites, cross sections were constructed based on the borehole database of Utrecht University (Berendsen and Stouthamer, 2002) and additional hand corings. The cross sections were interpreted to identify morphogenetic units (see also Hobo et al., 2014).
For all samples, radionuclide concentrations were determined with high-resolution gamma-ray spectroscopy, from which dose rates were estimated using standard conversion factors. Sand-sized quartz grains were extracted for single-aliquot regeneration OSL measurements (Murray and Wintle, 2003) for equivalent-dose measurements. Details of the procedure are described by Hobo et al. (2010) and Wallinga et al. (2010). The grain-size fractions varied between samples (180212 m, 180250 m or 90180 m), due to differences in texture of the sampled deposit. The measurement protocols were similar for all samples. The dose response was dened using a single regenerative dose (Wallinga et al., 2010), net OSL signals were dened using the early background subtraction (Cunningham and Wallinga, 2010) and low pre-heat temperatures were selected to avoid thermal transfer (e.g. Truelsen and Wallinga, 2003).
We identied nine variables that could inuence the bleaching of the sample either directly or by proxy. The choice of variables is based on our judgement of possible relevance and data availability. With regard to sample position, we considered the average river water level at the site (recorded in 2001), the height of the present surface at the sample location, the depth of the sample below the present surface, and the depth of the sample relative to the 2001 average water level. With regards to the sample nature, we considered the depositional environment (ordinal classes of
Earth Surf. Dynam., 3, 5565, 2015 www.earth-surf-dynam.net/3/55/2015/
A. C. Cunningham et al.: Re-evaluating burial doses and bleaching of uvial deposits 57
distal overbank, overbank, proximal overbank, channel); the sediment texture (clay, loam, silt, sand, coarse sand/gravel); the dose rate; the De; and the OSL age (although De and
OSL age are derived from the model, they can also be considered as predictor variables; the dose rate may indirectly affect the bleaching statistic). Table S1 (Supplement) provides an overview of all variables that are considered.
2.2 Statistical rationale
We seek to dene a poor-bleaching score based on the measured De distribution, which can then be used to compare bleaching between samples. Previous attempts have applied a statistical model directly to the De distribution to dene a summary statistic (e.g. the F statistic; Spencer et al., 2003 skewness and kurtosis applied to single-grain (SG) distributions; Bailey and Arnold, 2006). This type of approach may be valid if the observed De distribution is a function of the burial dose and remnant dose. For multi-grain (MG) aliquots, the OSL signal comes from many grains; the De for an aliquot is the average of those grains, weighted by their OSL sensitivity (e.g. Wallinga, 2002b; Duller, 2008; Cunningham et al., 2011). Therefore, for MG data sets, the De distribution is a function of the burial and remnant doses, and also the aliquot size and the single-grain OSL sensitivity distribution.
Aliquot size and SG sensitivity may vary between samples, so for a statistic to be useful, it must be independent of these factors for the range of samples considered. A model dened directly on the De distribution of young samples is also likely to be sensitive to the burial dose, as the measurement precision decreases with decreasing De. Our data set contains many samples, measured over several years on different OSL readers. While the SG sensitivity distributions are likely to be similar (as all samples are from Rhine deposits), the aliquot size varies both between and within samples: measurements used either 2 or 3 mm mask size, with grain sizes of 180212, 180250 or 90180 m. A statistic dened from the MG aliquot De distribution (such as the burial dose, overdispersion, degree of bleaching) may not have any real-world meaning, because the data are affected by the confounding variables of aliquot size and SG sensitivity. The meaningful parameters operate at the single-grain level, so the approach we take here is to estimate what combination of single-grain parameters would lead to the measured MG De distribution. There are two parts to the procedure.
First, we dene how the MG De distribution is derived from single-grain parameters. Second, we use Bayesian computational statistics to estimate the value each parameter must take to reproduce the observed MG De distribution.
2.3 From single-grain parameters to the multi-grain-aliquot distribution
2.3.1 The single-grain sensitivity distribution
The magnitude of the OSL signal induced by a given radiation dose varies from grain to grain. The sensitivity distribution also varies between samples (Duller et al., 2000). Quantifying the SG sensitivity is important for dating partially bleached samples, because it governs the extent of averaging across multi-grain aliquots (Cunningham et al., 2011).We therefore need to dene the SG sensitivity distribution in order to simulate an MG De distribution. While this can be done using a single-grain measurement system, there are practical difculties: some grain holes may be empty and some may contain more than one grain, and with many sensitivity values clustered around zero, it is difcult to distinguish signal from noise.
Here we use computational Bayesian statistics to estimate the SG sensitivity distribution from the MG sensitivity data.The rst step is to parameterise the SG sensitivity, for which we use the gamma distribution. The gamma distribution can be formatted with two parameters: a shape parameter a and a scale parameter b. By altering these parameters, the gamma distribution can comfortably t a range of measured SG sensitivity distributions (Fig. 2a). Moreover, when a MG aliquot is simulated from SG sensitivity data, the MG sensitivity distribution can also be tted with a gamma distribution (Fig. 2b). For measured data, we already know the MG sensitivity distribution (from the regenerative-dose signal) and the approximate number of grains in the aliquot (from the grain size and mask size); we can therefore estimate the parameters a and b of the SG sensitivity distribution using a computational Bayesian procedure similar to that described below.
2.3.2 Modelling the De distribution
The single-grain parameters are as follows:
a. SG sensitivity, drawn from the gamma distribution with parameters:
a describes the shape (i.e. skewness);
b describes the scale.
b. The burial dose, drawn from a normal distribution with parameters:
: mean, in Gy;
SGb: relative standard deviation of the burial dose(xed as 0.20 for this work).
c. The remnant dose, drawn from the positive part of a normal distribution with mean of 0 and:
: standard deviation;
www.earth-surf-dynam.net/3/55/2015/ Earth Surf. Dynam., 3, 5565, 2015
58 A. C. Cunningham et al.: Re-evaluating burial doses and bleaching of uvial deposits
Figure 2. (a) Three SG sensitivity distributions presented by Duller et al. (2000) from SG measurements (dotted lines). Each has been approximated using the gamma distribution, with sample name and shape parameter a indicated. (b) Simple stochastic simulation of a multi-grain-aliquot sensitivity distribution. The simulation uses the measured SG sensitivity data set RBM2 (from Duller et al., 2000), with parameters ng = 200 and na = 1000. The MG sensitiv
ity distribution can also be tted using the gamma distribution, with a = 5.70. The shape of the gamma distribution is indicated in the
gure, with the y scale normalised to the peak of the histogram.
p: proportion of well-bleached grains.
d. Additional parameters:
ng: number of grains in each aliquot;
na: number of aliquots.
The simulated natural OSL signal from na aliquots is the sum of the signal from ng grains, with Poisson noise added. Each grain is assigned a sensitivity value (per Gy) drawn from the gamma distribution with parameters a and b, and an indicative dose. The indicative dose combines the burial dose, drawn from a normal distribution, and a remnant dose, drawn from a half-normal distribution. The number of grains in each aliquot that have a remnant dose is drawn from the binomial distribution with parameters ng and 1 p. The De
Figure 3. Posterior distribution of the burial dose for simulated data of aliquots of (a) 80 grains and (b) 300 grains. The given burial dose is 1 Gy; other parameters are specied in Table 1. The simulated De distributions are visualised with probability density functions (PDFs).
is determined by constructing a dose-response curve in the same way as measured data, i.e. one regenerative point of3 Gy, sensitivity-corrected (although no sensitivity change is added), and subject to the same rejection criteria. Where different aliquot sizes are used in the measured data, these are replicated in the simulation. The number of grains per aliquot (ng) is approximated using the known mask size and grain size, assuming spherical grains and a 0.7 packing density(i.e. quartz grains cover 70 % of the mask surface).
2.4 Computational Bayesian solution
With the De distribution simulated by single-grain parameters, we seek to identify which values the parameters must take to result in the best match between the simulated MG distribution and the measured MG distribution. In Bayesian terms, we seek the posterior distribution, which measures how plausible we consider each possible value of the parameters after we have observed the data. For complex models such as this, the posterior density cannot be calculated directly. Instead, inferences are based on random sampling of
Earth Surf. Dynam., 3, 5565, 2015 www.earth-surf-dynam.net/3/55/2015/
A. C. Cunningham et al.: Re-evaluating burial doses and bleaching of uvial deposits 59
the posterior distribution, which requires intensive computation.
In our model, the posterior is sampled using a Markov chain Monte Carlo (MCMC) process. Single-grain parameters for four Markov chains are drawn from a starting distribution, and these parameters are then corrected to better approximate the target posterior. The approximate distributions are improved at each step using the Metropolis algorithm. When the simulation has run long enough, each step can be considered a random draw from the target distribution.The length of the sequence is determined by the convergence of the Markov chains; this is monitored by comparing the within-chain and between-chain variance, following the procedure of Gelman et al. (2004). The rst half of each Markov chain is discarded to ensure that the choice of starting values does not inuence the result.
2.4.1 Priors
Five parameters are determined in the computational processing: , , p, a and b. Each of these is assigned a prior distribution, which represents our knowledge of these parameters before any measurements are undertaken. The priors could in future be determined from previous measurement data or, in the case of , from the stratigraphic order of the samples. For a and b, the priors are given by the posteriors obtained from the SG sensitivity model. For we use a uniform-positive prior, as we have no information on the burial dose and do not want to restrict it. The situation is different when it comes to p and . There is an unavoidable conict when estimating these two parameters: as the residual dose gets smaller, at some point the De values cannot be distinguished from well-bleached De values. This problem, not unique to our model, could erroneously assign a low p to a well-bleached sample, or high p to a poorly bleached sample (if is very small). To prevent this error, we specify arbitrary cut-offs in the priors: the lower limit for is0.25 Gy, and for p it is 0.05. As such, any sample that is poorly bleached to a very small extent ( < 0.25 Gy) will be inferred to be well bleached (high p). Very few samples are affected by the low-cut priors. In future, it will be useful to nd an objective value for the low cut-off, probably varying with measurement precision.
2.4.2 Density evaluation
Parameters with positive values ( , , a, b) are estimated on the log scale; p must lie between 0 and 1, and is therefore estimated on the logit scale (logit p = log(p/(1 p); this
transforms the unit interval to the real number line). The simulated MG De distribution is compared to the measured distribution using the models of Galbraith et al. (1999) as summary statistics. This provides four summary statistics to compare with the measured data (three from the three-component minimum-age model (MAM3), and one from the central-age
Table 1. Results of the simulation recovery: recovered values are dened by the mean and standard deviation of the posterior distribution. na = 40.
Given ng = 80 ng = 300 1 1.03 0.08 0.88 0.20
2.5 2.81 1.66 2.96 1.32
p 0.7 0.77 0.13 0.59 0.21
a 0.03 0.042 0.011 0.025 0.008
b 600 604 196 539 188
model (CAM)). The likelihood term is dened by projecting these values onto the bootstrap likelihood distribution for the measured data (see Cunningham and Wallinga, 2012).
The model is run in two phases. The rst is a short run, giving an approximate range of the parameter space. The output of the rst run is summarised by a multivariate normal distribution, which is used to dene the starting distribution and jumping distributions for phase two. The second phase is run until convergence.
2.5 Model validation
Here we perform a simulation-recovery test to check that the model is performing as expected. Single-grain parameters are chosen, and then used to simulate De data for two different aliquot sizes (80 and 300 grains). Each data set is used as input for the model, and the SG parameters are then reconstructed. The results are given in Table 1, and plotted in Fig. 3 for the burial dose .
For both aliquot sizes, the SG parameters can be reconstructed (Table 1). Reconstruction of the 1 Gy burial dose is reasonably precise (8 %) for the 80-grain aliquots, and very close to the bootstrapped MAM3 estimate of the burial dose on the MG aliquot data set (1.03 0.08 Gy, using b of 0.16.
b is used in the MAM3 to allow for the expected dispersion in De from well-bleached samples, and it changes with aliquot size). For the 300-grain aliquots, the estimate of the burial dose is imprecise but accurate, and lies mostly outside the range of the MG aliquot De distribution. For multi-grain aliquots, it is quite possible that none of the aliquots are indicating the burial dose, if at least one grain contributing to the OSL signal on each aliquot is poorly bleached.The model is able to explore this possibility by making use of the MG sensitivity distribution and aliquots size. In contrast, the bootstrap MAM3 applied to the MG data assumes some well-bleached aliquots exist, and therefore gives an overestimated burial dose of 1.15 0.03 Gy for this data set
(b = 0.08).
As a further step, it would be interesting to see how the age model applied to multi-grain aliquot data compares to single-grain data from the same sample. However, this comparison is not as simple as it sounds. Our model uses multi-grain aliquot data to estimate the assumed parameters of the SG De
www.earth-surf-dynam.net/3/55/2015/ Earth Surf. Dynam., 3, 5565, 2015
60 A. C. Cunningham et al.: Re-evaluating burial doses and bleaching of uvial deposits
A NCL-1110008 B NCL-1107146 C NCL-4110020
Figure 4. Example model output for three samples that are (a) relatively well bleached, (b) moderately bleached and (c) poorly bleached. For each sample the posterior draws are indicated by the blue histograms, showing the burial dose (along with the bootstrap likelihoods of the MAM3 (bootlik MAM3) and a probability density function of the De distribution), the residual dose , and the proportion of well-bleached grains p. Two sensitivity parameters, a and b, are also estimated in the model, but not shown here. All data sets are normalised to their maximum value.
distribution; it does not reconstruct the SG distribution itself.
Testing the model against SG data for a real sample would not distinguish between the performance of the model and validity of the assumptions about SG parameters. The way around this would be to construct an articial sample with a known dose distribution, like Roberts et al. (2000) and Sivia et al. (2004), but such an elaborate approach is outside the scope of this paper. Also, the mode of optical stimulation in single-grain measurement systems (green laser) differs from that used for MG aliquots for our study (blue LEDs). This prevents direct comparison between SG and MG, as component separation is wavelength-dependent (e.g. Singarayer and Bailey, 2003).
3 Results
The reconstructed SG sensitivity distribution is similar for all samples measured here, not surprising as they are all from recent Rhine deposits. The shape parameter a has a mean of 0.008 and standard deviation 0.003, indicating a highly skewed sensitivity distribution (more so than all of the example distributions in Fig. 2). The averaging effect on multi-grain aliquots is therefore very weak. The scale parameter b has a mean of 400 and standard deviation of 220. The estimates of p are evenly spread between 0.2 and 0.95 (not shown). The uncertainty on p is typically large, except for those values close to 1.
The distribution of is positively skewed; the mean is2 Gy, and most values are below 8 Gy. However, high values of have very poor precision, coming from samples with high p in which has little inuence on the De distribution.
The susceptibility of to outliers and to p makes it unsuitable as an indicator of bleaching. The degree of bleaching is best dened by p, the proportion of well-bleached grains.
Three examples of the model output are shown in Fig. 4, each indicating a different degree of bleaching. For each sample, the histograms indicate the posterior density of the burial dose and the two bleaching parameters and p. The two sensitivity parameters a and b are of lesser interest for this study, and are not shown. In Fig. 4a, the sample is inferred to be well bleached, and the burial-dose posterior is similar to the MAM3 bootstrap likelihood. This sample is affected by the problematic low-/high-p distinction alluded to earlier; the posterior is being inuenced by the low-cut prior, causing a low tail in the burial-dose posterior. Figure 4b shows a moderately bleached sample, with mean p = 0.56. The pos
terior is well clear of the low-cut prior, and the burial dose is less precise but potentially more accurate than the MAM3 burial-dose estimate. A poorly bleached sample is shown inFig. 4c (mean p = 0.25, but affected by the prior). The burial-
dose estimate is much less precise than the MAM3 estimate, but is permitted to be smaller than any of the measured MGDe.
When the burial dose is very close to zero, the posterior distribution is shaped like an exponential decay (not shown
Earth Surf. Dynam., 3, 5565, 2015 www.earth-surf-dynam.net/3/55/2015/
aliquots prepared from channel sediments will contain fewer.
These biases lead to an error in the models estimate of the SG sensitivity. The error would also feed through into the estimate of bleaching parameters. We should therefore ignore the correlations involving the sensitivity parameters for this data set, and be cautious about any relationship between bleaching parameters and depositional environment or depth, as both are correlated with sediment texture.
The large degree of uncertainty in our model results prevents convincing conclusions from being drawn. This uncertainty is again down to aliquot size. Firstly, the aliquot sizes used were often too large. Second, our post hoc estimates of the aliquot size were not sufciently accurate (as noted by Heer et al., 2012). These issues affected model efciency and outcome by amplifying the difculty of distinguishing high p and low . By contrast, recent measurements by Cunningham et al. (2015) included a grain-counting step, and allowed more emphatic conclusions to be drawn. Here, we do not feel condent in claiming either the existence or absence of geomorphic controls on the basis of our results.
With these caveats established, it is worth considering two structures in the modelled data that might, possibly, have geomorphic signicance. These concern the relationship between p and mean water level, and between p and model age, which are enlarged for clarity in Fig. 7. Figure 7a shows a cluster of relatively well-bleached samples coming from sediment deposited close to, or just above, the modern mean water level. This cluster might be telling something about the comparative strengths of bleaching during transport and deposition. The attenuation of light (especially UV/blue) underwater is well established (Berger, 1990), and if light intensity at deposition was the main control on bleaching, we might expect shallower sediments to be better bleached (Wallinga, 2002a). The clustering of high p values around the mean water level may therefore reect a period of bleaching that occurs at deposition. However, close examination of the samples that are best bleached (NCL-111004, -5, -7, -8;NCL-2107157, -59, -61; NCL-4110018) shows that some of these are sandy channel deposits, whereas others are sand beds within silty overbank deposits, or silty overbank deposits with sand admixtures. All these samples are indeed within a metre from the transition of channel to overbank deposits. For the samples classied as channel deposits, deposition likely occurred on top of point bars, potentially with swash backwash operating and sub-aerial exposure likely (analogous to coastal beaches, which produce well-bleached quartz; e.g. Ballarini et al., 2003). For the well-bleached samples from overbank deposits, we hypothesise that sand grains may have experienced aeolian reworking prior to nal deposition and burial. Such aeolian reworking of sandy ood deposits has been documented following sand deposition on overbanks during high-discharge events of the Waal and Lek (Isarin et al., 1995; illustrated in Fig. 8).
There is also structure in Fig. 7b, which shows p in relation to modelled age. Highest p values, indicative of best-
www.earth-surf-dynam.net/3/55/2015/ Earth Surf. Dynam., 3, 5565, 2015
A. C. Cunningham et al.: Re-evaluating burial doses and bleaching of uvial deposits 61
here). Such distributions are not well described by the mean and standard deviation, and thus may need to be summarised differently. We will not dwell on the issue here, but will leave it for future consideration.
The mean (and standard deviation) of the p posterior provides a useful summary statistic for between-sample comparison. In Fig. 5, p is plotted against the potential geomorphic variables (Fig. 5ag), the other model-derived statistics (Fig. 5hk), and nally the dose rate and model-derived age (Fig. 5l, m). A crude table of correlations is provided in the Supplement (Table S2), but is of limited use because it treats the ordinal variables of depositional environment and texture as if they are interval types. Nevertheless, there are some correlations among the predictor variables. For example, deeper samples are older and coarser (being channel deposits), and thus they have lower dose rates than the silty overbank samples. There are also signicant correlations between the sensitivity parameters a and b and several predictor variables; these are probably due to inadequate aliquot-size estimates, as discussed in Sect. 4.
While there are no clear relationships between p and predictor variables, some of the plots appear to indicate structure beyond that expected through chance. Figure 5g shows that most of the best-bleached samples were located close to the modern mean water level. Figure 5k and m show a trend in p for the relatively young samples. In Fig. 6, the burial-dose estimate is compared directly to the original MAM3.The weighted mean ratio of to MAM3 minimum age is0.97 0.025. Samples inferred to be relatively well bleached
return very similar burial doses in both models, with comparable precision. For poorly bleached samples, our model provides a smaller and less precise burial-dose estimate.
4 Discussion
4.1 Inuences on bleaching
There appear to be signicant relationships between the sensitivity parameters a and b, and several predictor variables: both a and b are correlated with sample depth/elevation (Table S1). These relationships are difcult to explain in geomorphic terms, but may be a manifestation of subtle differences in grain size. Most measurements were carried out on grain-size range of 180250 m, with the aliquot size ng estimated from the grain size and mask size. This grain-size range still allows differences in the grain-size distribution of the natural sediment to be reected on the disc. For ne sediments, the selected grain-size range will be at the upper tail of the grain-size distribution, resulting in a prepared fraction with many grains at the lower end of the sieved fraction(i.e. 180 m or just larger). In contrast, for coarse sediments the prepared fraction will be dominated by grains at the upper end of the sieved fraction (i.e. 250 m and somewhat smaller). The aliquots prepared from overbank sediment will therefore contain more grains than assumed in the model, and
62 A. C. Cunningham et al.: Re-evaluating burial doses and bleaching of uvial deposits
A B C D
E F G
H I J
K L M
Figure 5. The bleaching statistic p (proportion of grains well bleached) plotted against possible predictor variables (ag), and other model-derived statistics and the dose rate (hm). (a) Depositional environment on a scale of distal overbank (1) to channel (4). (b) Sediment texture is classed from clay (1) to coarse sand (5). Site classication in (d) is nominal. NAP is Dutch ordnance datum ( mean sea level in
Amsterdam). For classication details see Table S1.
bleached deposits, are obtained for samples with model ages around 0.10 ka. The youngest samples appear to be less
well bleached (i.e. low p), and p varies a lot for the samples older than 0.10 ka. The same trends are observed when
burial dose (Fig. 6k) or MAM3 age (not shown) is used instead of modelled age.
There are three possible reasons for the structure. It could be an artefact of the model through the high-p/low- problem, but examination of the model output for these samples does not conrm this. Alternatively, it might be a sampling effect caused by coring from the oodplain down towards the high-p cluster at mean water level, but most of the high-p samples are older. A more intriguing explanation involves changes in river management over the last few hun-
dred years. Major changes occurred with dike construction from AD 10001300, and river normalisation and groyne emplacement after AD 1850 (Middelkoop, 1997; Hesselink, 2002). Dike construction forced river bends to migrate downstream rather than laterally (see also Hobo et al., 2014), causing the river to rework some of its recent deposits. The lower residual dose in these deposits means that less light exposure would be required for an acceptable degree of bleaching to take place. During this period, sand bars were exposed in the river during low ow, enhancing bleaching conditions for river-transported sediments. Bleaching conditions may have been reduced following the construction of groynes (afterAD 1850), for a number of reasons. Firstly, the groynes prevented bend migration and thus reworking of recent river sed-
Earth Surf. Dynam., 3, 5565, 2015 www.earth-surf-dynam.net/3/55/2015/
A. C. Cunningham et al.: Re-evaluating burial doses and bleaching of uvial deposits 63
0 0 0.25 0.5 0.75 1 1.25
1.2
Modelled burial dose g(Gy)
1
0.8
0.6
0.4
0.2
MAM3 Minimum dose (Gy)
Figure 6. Comparison of burial-dose estimates. The modelled dose is dened by the mean and standard deviation of the posterior, and is compared to the original MAM3 minimum dose (using b of 12 %;
Galbraith et al., 1999). Squares indicate where the unlogged MAM3 was used (Arnold et al., 2009). The best-bleached samples are lled black (p > 0.8), and the worst-bleached samples in red (p < 0.3).
Figure 8. A sand bar deposited close to the river Waal during high discharge (photo by Gilbert Maas, Alterra). Due to the absence of vegetation, such deposits may be reworked through aeolian processes, which may enhance bleaching for deposits formed above the mean water level.
iments. Secondly, sand bars within the channel disappeared, perhaps reducing light exposure of channel deposits during low ow. Thirdly, the groynes caused deepening of the channel through bottom scour, enhancing the reworking of the underlying, high-residual-dose Pleistocene deposits.
4.2 Modelling the burial dose
The requirements of this project led us to develop a specic age model for partially bleached, multi-grain-aliquot data. It uses Bayesian computational methods to estimate the parameters of the single-grain dose distribution, without the need for any single-grain measurements. Along the way, the parameters of the single-grain sensitivity distribution are estimated from multi-grain aliquot sensitivity data. Our approach has signicant advantages over existing models:
The interaction of aliquot size and SG sensitivity is incorporated, meaning that prior quantication of the averaging effect is not necessary.
It includes uncertainty deriving from the number of aliquots consistent with the burial dose.
It should provide an unbiased estimate of the burial dose, even when no aliquots are well bleached. Poorly bleached samples give a very imprecise, but still accurate, estimate of the burial dose.
The degree of bleaching is quantied, and is potentially independent of the SG sensitivity, aliquot size and burial dose.
Different data sets from the same sample (i.e. different aliquot sizes) can be combined to produce a single estimate of the burial dose.
www.earth-surf-dynam.net/3/55/2015/ Earth Surf. Dynam., 3, 5565, 2015
(a)
(b)
1
0.8
0.6
p
0.4
0.2
0 4 3 2 1 0 1 2 3
Elevation w.r.t mean water (m)
1
0.8
0.6
p
0.4
0.2
0 0 0.1 0.2 0.3 0.4 0.5 0.6
Age (ka)
Figure 7. Two possible structures in the proportion of well-bleached grains p versus predictor variables of Fig. 5, enlarged here for clarity. (a) Plotted against the sample elevation with respect to mean water level at each sampling site. A cluster of well-bleached samples appears at about the (modern) mean water level. (b) Plotted against model-derived age, showing a trend for the youngest samples (age < 0.10 ka). The onset of groyne construction is indicated at 0.15 ka.
64 A. C. Cunningham et al.: Re-evaluating burial doses and bleaching of uvial deposits
Of course, the validity of the outcome rests on a number of assumptions. The parameterisation of the SG dose and sensitivity distributions must be appropriate and, crucially, the estimate of aliquot size should be reasonable. This paper uses archive data, so aliquot size was estimated only roughly.When applied in future, careful grain counting should take place; this could be performed manually, or with a digital camera plus image-recognition software.
Compared to familiar and well-used age models in OSL dating (e.g. CAM and MAM3), this model is a different beast altogether. It requires more data to be input per sample, and careful consideration and specication of model parameters and priors. It includes the MAM3 (Galbraith et al., 1999) and bootstrap likelihoods (Cunningham and Wallinga, 2012) as a small part of it, and requires 1 h of computer time to run
per sample, provided no errors arise. We provide the code in the Supplement in order to spur further development in this eld; we do not present a rened model for general application.
The model could be immediately improved by treating SGb as an unknown parameter. At present, the model assumes that scatter in the single-grain burial-dose population is exactly 20 %. If it becomes possible to create a sample-specic estimate of SGb (e.g. through radiation transport modelling; Cunningham et al., 2012; Guerin et al., 2012), it could be incorporated as a prior. The posterior SGb would then be estimated along with , and p. A further step would be to incorporate stratigraphic information on sample order and/or age (e.g. Rhodes et al., 2003; Cunningham and Wallinga, 2012), although this would signicantly increase computational time.
5 Conclusions
There are a particular set of challenges in estimating the degree of bleaching for unknown-age OSL samples, and these problems relate closely to the burial-dose calculation. We have begun to refashion the burial-dose calculation by using Bayesian computational statistics to reduce the De distribution into meaningful statistics. There are many novel aspects to our approach, such as parameterising the OSL sensitivity distribution and inferring single-grain statistics from small-aliquot measurements. We found that a good aliquot-size estimate is particularly important for the model, and that our poor knowledge of aliquot size hampered our application of the model to archive data.
Nevertheless, the results do show some interesting features that may point to geomorphic controls on sediment bleaching. We found a concentration of well-bleached samples around the modern mean water level, indicating to us that sediment receives a kick of bleaching upon deposition, through local reworking, in addition to the bleaching that oc-curs during transport. We also speculate on whether changes in the degree of bleaching over time could relate to river man-
agement changes, especially the construction of groynes in the lower Rhine around AD 1850.
Despite the limitations of this study, it seems clear that processes of sediment provenance, transport and deposition can inuence the measured OSL signal. The challenge lies in extracting meaningful information from the OSL data. The computational approach explored in this study has real potential, and we hope aspects of our model will be taken forward.
The Supplement related to this article is available online at http://dx.doi.org/10.5194/-15-55-2015-supplement
Web End =doi:10.5194/-15-55-2015-supplement .
Acknowledgements. This work was partially funded through a Technology Foundation (STW) VIDI grant (DSF.7553). We would like to thank Geoff Duller (Aberystwyth University) for making the data set on single-grain sensitivity distributions available.Zhixiong Shen and an anonymous reviewer are kindly thanked for their constructive comments. Matlab code is available in the supplement les.
Edited by: A. Lang
References
Arnold, L. J., Roberts, R. G., Galbraith, R. F., and DeLong, S. B.: A revised burial dose estimation procedure for optical dating of youngand modern-age sediments, Quatern. Geochronol., 4, 306 325, doi:http://dx.doi.org/10.1016/j.quageo.2009.02.017
Web End =10.1016/j.quageo.2009.02.017 http://dx.doi.org/10.1016/j.quageo.2009.02.017
Web End = , 2009.
Bailey, R. M. and Arnold, L. J.: Statistical modelling of single grain quartz De distributions and an assessment of procedures for estimating burial dose, Quaternary Sci. Rev., 25, 24752502, 2006.Ballarini, M., Wallinga, J., Murray, A. S., Van Heteren, S., Oost, A.P., Bos, A. J. J., and Van Eijk, C. W. E.: Optical dating of young coastal dunes on a decadal time scale, Quaternary Sci. Rev., 22, 10111017, 2003.
Berendsen, H. J. A. and Stouthamer, E.: Palaeogeographic development of the Rhine-Meuse delta, The Netherlands, Van Gorcum, Assen, p. 268, 2002Berger, G. W.: Effectiveness of natural zeroing of the thermoluminescence in sediments, J. Geophys. Res.-Solid Ea., 95, 12375 12397, 1990.
Cunningham, A. C. and Wallinga, J.: Selection of integration time-intervals for quartz OSL decay curves, Quaterna. Geochronol., 5, 657666, 2010.
Cunningham, A. C. and Wallinga, J.: Realizing the potential of uvial archives using robust OSL chronologies, Quatern.Geochronol., 12, 98106, 2012.
Cunningham, A. C., Wallinga, J., and Minderhoud, P. S. J.: Expectations of scatter in equivalent-dose distributions when using multi-grain aliquots for OSL dating, Geochronometria, 38, 424431, 2011.
Cunningham, A. C., DeVries, D. J., and Schaart, D. R.: Experimental and computational simulation of beta-dose heterogeneity in sediment, Radiat. Measure., 47, 10601067, 2012.
Earth Surf. Dynam., 3, 5565, 2015 www.earth-surf-dynam.net/3/55/2015/
A. C. Cunningham et al.: Re-evaluating burial doses and bleaching of uvial deposits 65
Cunningham, A. C., Evans, M., and Knight, J.: Quantifying bleaching for zero-age uvial sediment: a Bayesian approach, Radiat.Measure., in press, 2015.
Duller, G. A. T.: Single-grain optical dating of Quaternary sediments: why aliquot size matters in luminescence dating, Boreas, 37, 589612, 2008.
Duller, G. A. T., Botter-Jensen, L., and Murray, A. S.: Optical dating of single sand-sized grains of quartz: sources of variability, Radiat. Measure., 32, 453457, 2000.
Galbraith, R. F.: On plotting OSL equivalent doses, Ancient TL, 28,110, 2010.
Galbraith, R. F., Roberts, R. G., Laslett, G. M., Yoshida, H., and Olley, J. M.: Optical dating of single and multiple grains of quartz from Jinmium rock shelter, northern Australia: Part I. Experimental design and statistical models, Archaeometry, 41, 339 364, 1999.
Gelman, A., Carlin, J. B., Stern, H. S., and Rubin, D. B.: Bayesian data analysis, Chapman & Hall/CRC, Boca Raton, Florida, 2004.Guerin, G., Mercier, N., Nathan, R., Adamiec, G., and Lefrais, Y.:
On the use of the innite matrix assumption and associated concepts: A critical review, Radiat. Measure., 47, 778785, 2012.Heer, A. J., Adamiec, G., and Moska, P.: How many grains are there on a single aliquot?, Ancient TL, 30, 916, 2012.
Hesselink, A. W.: History makes a river: Morphological changes and human interference in the river Rhine, the Netherlands, Neth.Geogr. Stud., 292, 177, 2002.
Hobo, N., Makaske, B., Middelkoop, H., and Wallinga, J.: Reconstruction of oodplain sedimentation rates: a combination of methods to optimize estimates, Earth Surf. Proc. Land., 35, 14991515, 2010.
Hobo, N., Makaske, B., Middelkoop, H., and Wallinga, J.: Reconstruction of eroded and deposited sediment volumes of the em-banked river Waal, the Netherlands, for the period AD 1631 present, Earth Surf. Proc. Land., 39, 13011318, 2014.
Isarin, R. F. B., Berendsen, H. J. A., and Schoor, M. M.: De morfodynamiek van de rivierduinen langs de Waal en de Lek, in: Publications and reports of the project Ecological Rehabilitation of the Rivers Rhine and Meuse, RIZA report 49, RIZA Rijksinstituut voor Integraal Zoetwaterbeheer en Afvalwaterbehandeling, Lelystad, 1995.
Jain, M., Murray, A. S., and Botter-Jensen, L.: Optically stimulated luminescence dating: how signicant is incomplete light exposure in uvial environments?, Quaternaire, 15, 143157, 2004.Middelkoop, H.: Embanked oodplains in the Netherlands; Geo-morphological evolution over various time scales, Netherlands Geographical Studies 224, Boca Raton, Florida, p. 341, 1997.Murari, M. K., Achyuthan, H., and Singhvi, A. K.: Luminescence studies on the sediments laid down by the December 2004 tsunami event: Prospects for the dating of palaeo tsunamis and for the estimation of sediment uxes, Current Sci., 92, 367371, 2007.
Murray, A. S. and Wintle, A. G.: The single aliquot regenerative dose protocol: potential for improvements in reliability, Radiat.Measure., 37, 377381, 2003.
Murray, A. S., Olley, J. M., and Caitcheon, G. G.: Measurement of equivalent doses in quartz from contemporary water-lain sediments using optically stimulated luminescence, Quaternary Sci. Rev., 14, 365371, 1995.
Olley, J., Caitcheon, G., and Murray, A.: The distribution of apparent dose as determined by optically stimulated luminescence in small aliquots of uvial quartz: implications for dating young sediments, Quaternary Sci. Rev., 17, 10331040, 1998.
Reimann, T., Notenboom, P. D., De Schipper, M. A., and Wallinga, J.: Testing for sufcient signal resetting during sediment transport using a polymineral multiple-signal luminescence approach, Quatern. Geochronol., 25, 2636., doi:http://dx.doi.org/10.1016/j.quageo.2014.09.002
Web End =10.1016/j.quageo.2014.09.002 http://dx.doi.org/10.1016/j.quageo.2014.09.002
Web End = , 2015.
Rhodes, E. J., Bronk Ramsey, C., Outram, Z., Batt, C., Willis, L.,
Dockrill, S., and Bond, J.: Bayesian methods applied to the interpretation of multiple OSL dates: high precision sediment ages from Old Scatness Broch excavations, Shetland Isles, Quaternary Sci. Rev., 22, 12311244, doi:http://dx.doi.org/10.1016/S0277-3791(03)00046-5
Web End =10.1016/S0277-3791(03)00046-5 http://dx.doi.org/10.1016/S0277-3791(03)00046-5
Web End = , 2003Roberts, R. G., Galbraith, R. F., Yoshida, H., Laslett, G. M., and Olley, J. M.: Distinguishing dose populations in sediment mixtures: a test of single-grain optical dating procedures using mixtures of laboratory-dosed quartz, Radiat. Measure., 32, 459465, 2000. Schielein, P. and Lomax, J.: The effect of uvial environments on sediment bleaching and Holocene luminescence ages A case study from the German Alpine Foreland, Geochronometria, 40, 283293, doi:http://dx.doi.org/10.2478/s13386-013-0120-y
Web End =10.2478/s13386-013-0120-y http://dx.doi.org/10.2478/s13386-013-0120-y
Web End = , 2013.
Singarayer, J. S. and Bailey, R. M.: Further investigations of the quartz optically stimulated luminescence components using linear modulation, Radiat. Measure., 37, 451458, doi:http://dx.doi.org/10.1016/S1350-4487(03)00062-3
Web End =10.1016/S1350-4487(03)00062-3 http://dx.doi.org/10.1016/S1350-4487(03)00062-3
Web End = , 2003.
Sivia, D. S., Burbidge, C., Roberts, R. G., and Bailey, R. M.: A Bayesian approach to the evaluation of equivalent doses in sediment mixtures for luminescence dating, Am. Inst. Phys. Conf. Proc., 735, 305311, 2004.
Spencer, J., Sanderson, D. C. W., Deckers, K., and Sommerville,A. A.: Assessing mixed dose distributions in young sediments identied using small aliquots and a simple two-step SAR procedure: the F-statistic as a diagnostic tool, Radiat. Measure., 37, 425431, 2003.
Stokes, S., Bray, H. E., and Blum, M. D.: Optical resetting in large drainage basins: tests of zeroing assumptions using single-aliquot procedures, Quaternary Sci. Rev., 20, 879885, 2001. Truelsen, J. L. and Wallinga, J.: Zeroing of the OSL signal as a function of grain size: investigating bleaching and thermal transfer for a young uvial sample, Geochronometria, 22, 18, 2003. Wallinga, J.: Optically stimulated luminescence dating of uvial deposits: a review, Boreas, 31, 303322, 2002a.
Wallinga, J.: Detection of OSL age overestimation using single-aliquot techniques, Geochronometria, 21, 1726, 2002b. Wallinga, J., Hobo, N., Cunningham, A. C., Versendaal, A. J.,
Makaske, B., and Middelkoop, H.: Sedimentation rates on em-banked oodplains determined through quartz optical dating, Quatern. Geochronol., 5, 170175, 2010.
www.earth-surf-dynam.net/3/55/2015/ Earth Surf. Dynam., 3, 5565, 2015
You have requested "on-the-fly" machine translation of selected content from our databases. This functionality is provided solely for your convenience and is in no way intended to replace human translation. Show full disclaimer
Neither ProQuest nor its licensors make any representations or warranties with respect to the translations. The translations are automatically generated "AS IS" and "AS AVAILABLE" and are not retained in our systems. PROQUEST AND ITS LICENSORS SPECIFICALLY DISCLAIM ANY AND ALL EXPRESS OR IMPLIED WARRANTIES, INCLUDING WITHOUT LIMITATION, ANY WARRANTIES FOR AVAILABILITY, ACCURACY, TIMELINESS, COMPLETENESS, NON-INFRINGMENT, MERCHANTABILITY OR FITNESS FOR A PARTICULAR PURPOSE. Your use of the translations is subject to all use restrictions contained in your Electronic Products License Agreement and by using the translation functionality you agree to forgo any and all claims against ProQuest or its licensors for your use of the translation functionality and any output derived there from. Hide full disclaimer
Copyright Copernicus GmbH 2015
Abstract
The optically stimulated luminescence (OSL) signal from fluvial sediment often contains a remnant from the previous deposition cycle, leading to a partially bleached equivalent-dose distribution. Although identification of the burial dose is of primary concern, the degree of bleaching could potentially provide insights into sediment transport processes. However, comparison of bleaching between samples is complicated by sample-to-sample variation in aliquot size and luminescence sensitivity. Here we begin development of an age model to account for these effects. With measurement data from multi-grain aliquots, we use Bayesian computational statistics to estimate the burial dose and bleaching parameters of the single-grain dose distribution. We apply the model to 46 samples taken from fluvial sediment of Rhine branches in the Netherlands, and compare the results with environmental predictor variables (depositional environment, texture, sample depth, depth relative to mean water level, dose rate). Although obvious correlations with predictor variables are absent, there is some suggestion that the best-bleached samples are found close to the modern mean water level, and that the extent of bleaching has changed over the recent past. We hypothesise that sediment deposited near the transition of channel to overbank deposits receives the most sunlight exposure, due to local reworking after deposition. However, nearly all samples are inferred to have at least some well-bleached grains, suggesting that bleaching also occurs during fluvial transport.
You have requested "on-the-fly" machine translation of selected content from our databases. This functionality is provided solely for your convenience and is in no way intended to replace human translation. Show full disclaimer
Neither ProQuest nor its licensors make any representations or warranties with respect to the translations. The translations are automatically generated "AS IS" and "AS AVAILABLE" and are not retained in our systems. PROQUEST AND ITS LICENSORS SPECIFICALLY DISCLAIM ANY AND ALL EXPRESS OR IMPLIED WARRANTIES, INCLUDING WITHOUT LIMITATION, ANY WARRANTIES FOR AVAILABILITY, ACCURACY, TIMELINESS, COMPLETENESS, NON-INFRINGMENT, MERCHANTABILITY OR FITNESS FOR A PARTICULAR PURPOSE. Your use of the translations is subject to all use restrictions contained in your Electronic Products License Agreement and by using the translation functionality you agree to forgo any and all claims against ProQuest or its licensors for your use of the translation functionality and any output derived there from. Hide full disclaimer