Using post-IR IRSL and OSL to date young (< 200 yrs) dryland aeolian dune deposits

Radiation Measurements 126 (2019) 106131

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Radiation Measurements
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Using post-IR IRSL and OSL to date young (< 200 yrs) dryland aeolian dune
deposits

T

Catherine E. Buckland∗, Richard M. Bailey, David S.G. Thomas
School of Geography and the Environment, University of Oxford, South Parks Road, Oxford, OX1 3QY, UK

A R T I C LE I N FO

A B S T R A C T

Keywords:
pIRIR
Young sediments
Luminescence
Natural residual
De(t)

Determining the most appropriate luminescence protocol, coupled with suitable data processing methods, for
dating recently deposited sediments (< 200 years) is important for identifying episodes of sediment movement
and interpreting historical landscape dynamics. Issues of partial bleaching, dim luminescence signals and the
incorrect application of rejection criteria, can lead to inaccurate and imprecise ages of recent sediment deposition. This study first compares the performance of quartz optically stimulated luminescence (OSL) and Kfeldspar post-IR IRSL (pIRIR) measurements in a series of dose recovery preheat plateau, bleachability and
remnant dose tests. Sediments of known historical age are used to identify the most suitable aliquot size and age

model choice for further application on near-surface aeolian dune sediments from the Nebraska Sandhills.
Results show that the ideal conditions for measuring these aeolian sediments are small aliquots (2 mm) of either
quartz or K-feldspar coupled with the relevant protocols (OSL130 pIRIR170) and the unlogged-CAM and unloggedMAM respectively. Results of 4 ± 7 years (quartz) and 4 ± 8 years (K-feldspar) are in excellent agreement with
aeolian sediments of known age 5–6 years. Additionally, we find a revised set of rejection criteria is useful for
accurately identifying the appropriate aliquots or grains for reliable age estimation. Sensitivity testing of recuperation rejection criteria highlights the caution that should be taken to avoid arbitrarily applying rejection
criteria and biasing towards age overestimations.

1. Introduction
Methodological and technological advances in luminescence dating
(e.g. Bøtter-Jensen et al., 2000; Murray and Wintle, 2000), and age
model modifications (e.g. Arnold et al., 2009; Combès et al., 2015;
Cunningham et al., 2015; Cunningham and Wallinga, 2012; Guérin
et al., 2017), have meant that the accuracy of dating recent deposition
events (e.g. < 200 yrs) has greatly improved over recent decades. As
such, a range of existing studies have successfully applied luminescence
dating techniques to young and known-age sedimentary samples (e.g.
Bailey et al., 2001; Ballarini et al., 2003; Banerjee et al., 2001;
Cunningham and Wallinga, 2012, 2009; Madsen et al., 2007; Olley
et al., 1999; Riedesel et al., 2018) with the majority applying optically
stimulated luminescence (OSL) techniques to the quartz fraction to date
the age of deposition. The rapid bleaching of the fast component of the
quartz luminescence signal (Wintle and Murray, 2006) minimises the
likelihood of partial bleaching, and coupled with a seemingly apparent
absence of anomalous fading (Huntley and Lamothe, 2001), quartz-focused studies have dominated young luminescence measurements.
Nevertheless, the application of feldspars to luminescence dating

∗

has many advantages. First, feldspars are widely abundant and can be
found in a variety of sedimentary settings. Second, unlike quartz crystals, feldspars can be selectively measured under infrared excitation

despite the presence of other minerals (Huntley and Lamothe, 2001).
Third, a larger proportion of potassium-rich feldspar (hereafter referred
to as ‘K-feldspar’) grains emit a detectable luminescence signal, which is
generally brighter than the signal emitted from quartz grains (Duller
et al., 2003). Finally, the advantage of high internal dose rates for Kfeldspar sediments aids in producing a brighter luminescence signal
(Reimann et al., 2012; Smedley et al., 2016), which improves the
signal-to-noise ratio of luminescence measurements, boosting the capacity to measure young dim samples.
Until recently, however, comparatively few studies had used the Kfeldspar fraction for dating sedimentological samples. As noted in Brill
et al. (2018), when dating Holocene sediments, K-feldspar IRSL techniques have generally been disregarded in favour of quartz OSL measurements. One of the reasons for the dominance of quartz usage has
been because of the instability of some of the signals in the feldspar
grains, which results in a greater degree of anomalous fading (Wintle,
1973) than that found in quartz crystals, resulting in estimated age

Corresponding author.
E-mail address: (C.E. Buckland).

/>Received 13 March 2018; Received in revised form 4 June 2019; Accepted 11 June 2019
Available online 12 June 2019
1350-4487/ © 2019 The Authors. Published by Elsevier Ltd. This is an open access article under the CC BY license
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Radiation Measurements 126 (2019) 106131

C.E. Buckland, et al.

previous studies have tested the optimum pIRIR conditions for fluvial
and costal samples (e.g. Colarossi et al., 2018; Reimann et al., 2012,
2011; Reimann and Tsukamoto, 2012), this study tests the application
of the pIRIR method to young aeolian sediments extracted from a
dryland location which typically experiences favourable bleaching

conditions. With bleaching conditions considered non-limiting, it is
anticipated that measuring the De of known-age sediments should
identify the lowest potential remnant dose that we can expect to find
when luminescence dating K-feldspars.
With the choice of mineral and measurement conditions explored,
this study also outlines appropriate age model selection and rejection
criteria application for measuring De's that are within errors of 0 Gy,
exhibit noisy decay curves and typically have large uncertainties. With
advances in age model development and a range of considered recuperation thresholds discussed in the literature, this study uses a series
of sensitivity-testing results from known-age sediments to identify the
most suitable combination of rejection criteria and data processing
tools for the near-surface dune sediments presented.

underestimations (Buylaert et al., 2012; Roberts, 2012) unless corrected
for. Previously, users of IRSL techniques corrected for the effects of
anomalous fading with the g-value approach (e.g. Huntley and
Lamothe, 2001), however, the introduction of the pIRIR protocol proposed by Thomsen et al. (2008), which identifies a low fading signal,
has led to a re-exploration of K-feldspar luminescence potential. A
series of recent studies have sought to test the application of different
pIRIR protocols in a range of settings including dating modern and
young sediments (Brill et al., 2018; Madsen et al., 2011; Reimann and
Tsukamoto, 2012; Riedesel et al., 2018), comparing the utility of the
pIRIR and IRSL signal against quartz OSL in attempting to extend the
luminescence age range (Colarossi et al., 2015) and investigate the
impact of varying measurement conditions to minimise residual doses
and fading of the luminescence signal (Buylaert et al., 2009; Colarossi
et al., 2018; Jain et al., 2015; Riedesel et al., 2018; Roberts, 2012).
Whilst the pIRIR signal has been shown to be more stable over time
than previously used IRSL50 protocols, existing research has also suggested that the signal bleaches more slowly and thus results in greater
residual signals than equivalent IRSL50 and quartz OSL measurements

(Buylaert et al., 2012; Colarossi et al., 2018, 2015; Li and Li, 2011;
Riedesel et al., 2018). Experiments conducted by Li and Li (2011) demonstrated the effect of measurement temperature on signal stability
and bleachability (multi-elevated-temperature post-IR IRSL – MET
pIRIR), exploring the capacity to target more stable traps within feldspars through higher stimulation temperatures. A summary of published pIRIR residual results in Smedley et al. (2015) suggests that
under specific measurement conditions, remnant doses from multigrain
aliquots have been recorded < 1 Gy, with the youngest reported age of
a known modern sample at 48 ± 6 years (Madsen et al., 2011). More
recently, Brill et al. (2018) have reported feldspar ages of 8 ± 2 years
and 10 ± 6 years for pIRIR150 for modern storm deposits in Thailand.
These results hint at the potential routine application of pIRIR protocols
when measuring young (e.g. < 200 yrs) sediment samples, particularly
those that demonstrate a dim quartz component.
Aside from identifying suitable mineralogical properties and protocol conditions for dating recently deposited sediments, the selection
of appropriate post-measurement rejection criteria and age model usage
is essential to calculating accurate age estimates of sediment movement
and subsequent deposition over the last 200 years. For example, naturally high recuperation levels as a percentage of equivalent dose are
expected when dating young sediments due to the noisy nature of the
signals and the close proximity of the natural and zero dose points.
Secondly, as shown by Arnold et al. (2009), the application of modified
age models (i.e. un-logged versions of the Central Age and Minimum
Age Models (Galbraith et al., 1999)) is more appropriate for samples
with equivalent doses within errors of zero where logged-age models
result in age overestimations.
Combined, identification of the most suitable mineral, measurement
conditions, and post-measurement data analysis is required in all examples of luminescence dating to ensure that the technique has produced the most accurate age estimates for the sediment samples in
question. In relation to recently buried sediments (i.e. < 200 years),
the importance of deducing the optimum suite of luminescence
methods is even more important when increases in precision and accuracy can allow us to apply luminescence techniques to answer
questions of historical landscape dynamism.
With this in mind, this study aims to identify a protocol for the

luminescence dating of recently deposited (< 200 yrs) aeolian dune
sediments taken from the Nebraska Sandhills. In this study, the remnant
dose (i.e. the dose that remains in the sample at the time of burial) of
known-age near-surface aeolian sediments is used to test the suitability
of the OSL and pIRIR signals when calculating the De of young knownage aeolian sediments. Quartz and K-feldspar fractions have been extracted and measured against blue OSL and pIRIR protocols to identify
how the different minerals perform against a variety of preheat, dose
recovery, anomalous fading and remnant dose experiments. Whilst

2. Methods and instrumentation
2.1. Samples
Sediment samples GSL15/1/2, GSL15/1/3 and BBR15/1/1, extracted from the Nebraska Sandhills in July 2015 as part of a wider
investigation into the recent landscape dynamics of the aeolian dunefield, are used in this study. GSL15/1/2 and GSL15/1/3 are quartz-rich
samples extracted from the backwall of Yao's Blowout in the
Gudmundsen Sandhills Laboratory (42.08627°N, 101.36721°W). 20 cm
black opaque plastic tubing was hammered horizontally into the exposed backwall at Yao's Blowout at 54 cm and 97 cm depth below the
surface of the dune crest to extract samples GSL15/1/2 and GSL15/1/3
respectively. BBR15/1/1 is a 50 cm vertical sediment core extracted
from a lunette dune which has formed on the Barta Brothers Ranch
since 2009 AD (42.24580°N, 99.65433°W). BBR15/1/1 was split
lengthwise during sample preparation and sub-sampled at centimetre
scale (sub-samples are labelled according to depth below the surface –
i.e. BBR15/1/1/X = X cm down core from surface). Sub-samples from
BBR15/1/1 should therefore be of a young age (post-2009 AD c.5–6
years) and provide a suitable test case for determining remnant doses
between the different minerals and protocols.
2.2. Sample preparation and instrumentation
All samples were treated in an excess of hydrochloric acid and hydrogen peroxide to remove carbonates and organics prior to wet-sieving
to the appropriate size fraction (multigrain aliquots: 125–180 μm,
single-grain: 180–210 μm). Quartz fractions were isolated using sodium
polytungstate density separation at 2.72 and 2.62 g/cm3 followed by a

45-min etch with concentrated hydrofluoric acid. K-feldspar fractions
were isolated using sodium polytungstate density separation at < 2.58
g/cm3. All pIRIR experiments referred to in this study were applied to
the K-feldspar fraction of the sediment sample.
All multigrain luminescence measurements were made using an
automated Risø TL/DA 15 reader, equipped with infra-red (IR) (870
nm) and blue (470 nm) LEDs and 90Sr/90Y beta sources for irradiations.
A convex lens placed in front of the photomultiplier tube was used to
focus the signal and increase the number of counts recorded. For quartz
OSL measurement, luminescence was detected in the UV region using
an EMI 9635Q alkali photomultiplier tube fitted with a 7.5 mm Hoya U340 filter, whilst IRSL detection was achieved through a combination of
Corning 7-59 and Schott BG39 filters. Multigrain experiments were
conducted on small aliquots (2 mm mask) and large aliquots (8 mm
mask), with c.109 grains (small) and c.1760 grains (large) expected on
each aliquot based on the grain size fraction 125–180 μm (calculated in
R Studio 1.0.153 (Burow, 2017)).
2


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C.E. Buckland, et al.

Single quartz and K-feldspar grains were measured on single grain
discs with hole diameters of 300 μm. Single grain measurements were
completed on the 180–210 μm size fraction to ensure only single grains
were present within each of the single grain disc holes. Single grain
measurements were performed using an automated Risø TL/DA 15
reader, equipped with infra-red (IR) (870 nm) and green (523 nm) lasers and 90Sr/90Y beta sources for irradiations. For quartz OSL measurement, luminescence was detected in the UV region using an EMI
9635Q alkali photomultiplier tube fitted with a 7.5 mm Hoya U-340

filter, whilst IRSL detection was achieved through a combination of
Corning 7-59 and Schott BG39 filters. All feldspar signals were separated from stimulation light using an interference filter with peak
transmission at 410 nm.
3. Selecting appropriate measurement parameters for quartz and
feldspar
Luminescence measurements were made following the Single
Aliquot Regenerative (SAR) protocol (Murray and Wintle, 2000) under
a range of preheat and stimulation temperatures. Preheat conditions
preceding the measurement of the natural, zero, or regenerative dose
signals were the same as those used prior to the test dose signal measurement (Blair et al., 2005).
Recycling ratio tests and an IR-depletion ratio point were included
to monitor sensitivity and identify any feldspar contamination in the
quartz OSL experiments (Duller, 2003). Recuperation levels were recorded and analysed alongside the range of preheat and measurement
temperature variations studied. Given the young nature of the sediments used in this study, dose response curves were fitted against a
linear function and individual equivalent dose estimates were calculated using interpolation of the natural signal onto this line. Uncertainties were calculated following 1,000 Monte Carlo fits of the
curve and propagated with a 2.5% measurement error.
Typical quartz OSL and K-feldspar IRSL decay and dose response
curves are shown in Fig. 1. Based on the young nature of the sediments,
the relatively noisy decay curve and the large contribution from the
medium and slow components, quartz De's were calculated using integration limits which captured a large signal with an early background
subtraction following the recommendation of Cunningham and
Wallinga (2010). Final integration limits used were 0–1.5 s followed by
an immediate background interval 1.6–6 s for quartz, and 0–5 s followed by a late background interval covering the last 20 s of measurement time for feldspar. Sample equivalent doses were calculated
using the un-logged Minimum Age Model (MAM) and Central Age
Models (CAM) (Galbraith et al., 1999) given the young nature of the
samples measured (Arnold et al., 2009).
Initial dose recovery preheat tests (Murray and Wintle, 2003) were
performed for both combinations (quartz OSL and K-feldspar pIRIR) to
determine optimum measurement conditions prior to testing for levels
of anomalous fading and remnant doses. Both quartz and K-feldspar

fractions were bleached prior to dose recovery preheat plateau experiments using blue diodes for two periods of 100 s at room temperature (20 °C) and with a 7.5 mm Hoya U-340 filter fitted. Given the
potential for variable results from daylight bleaching of K-feldspars,
bleaching using blue diodes offers a controlled means for applying
equal bleaching conditions to all grains analysed. Filter combinations
were subsequently changed prior to the given dose and measurement of
the K-feldspar fraction during the SAR cycle and IRSL and pIRIR measurements.
Dose recovery preheat plateau tests were completed on two sizes of
aliquot: small (2 mm mask) and large (8 mm mask). As demonstrated
through single-grain measurements (Duller, 2008; Duller and Murray,
2000; Rhodes, 2007), there is great variability in the luminescence
properties between individual grains within and between different
samples. Rhodes (2007) noted that within a sample there is large variation in the brightness of the OSL signal as well as the proportion of

Fig. 1. Examples of typical luminescence decay curves and dose response
curves associated with the dose recovery preheat plateau measurements performed in Section 3. (a) OSL decay curve and dose response curve associated
with one small aliquot of quartz from sample BBR15/1/1 measured following
OSL130 protocol and preheat temperature 200 °C. (b) IRSL decay curve and dose
response curve associated with one small aliquot of K-feldspar from sample
BBR15/1/1 measured following pIRIR170 protocol and preheat temperature
200 °C. The typical decay curves associated with the quartz OSL and K-feldspar
IRSL measurements suggest a relatively large slow/medium component. Integration intervals identified for the signal and background components are
shown in red and green respectively. (For interpretation of the references to
colour in this figure legend, the reader is referred to the Web version of this
article.)

grains having a detectable OSL signal between samples. As such, larger
aliquots, with a higher volume of grains, produce a greater averaging of
the luminescence characteristics between grains, whilst smaller aliquots
produce a signal dominated by a small proportion of grains from the
overall sample. Dose recovery preheat plateau tests were completed on

small and large aliquots to ensure the measurement conditions selected
were not based solely on an ‘average’ luminescence signal.

3.1. Quartz
Quartz OSL dose recovery preheat tests were completed using
sample GSL15/1/3 with preheats ranging from 160 to 250 °C on small
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C.E. Buckland, et al.

Table 1
Final OSL and pIRIR protocols selected based on dose recovery preheat results (SI: Appendix A). (left) OSL130 protocol used for equivalent dose measurement of
quartz. (right) Modified pIRIR170 protocol used for equivalent dose determination of K-feldspars.
Step

Treatment

Measured

Step

Treatment

Measured

1
2

3
4
5
6

Dose (Natural, 0 Gy, 0.45 Gy, 0.85 Gy, 0.45 Gy)
Preheat (200 °C for 10 s)
OSL 100 s @ 130 °C
Test dose (6.5 Gy)
Preheat (200 °C for 10 s)
OSL 100 s @ 130 °C

Lx
Tx

1
2
3
4
5
6
7
8
9

Dose (Natural, 0 Gy, 0.45 Gy, 0.85 Gy, 0.45 Gy)
Preheat (200 °C for 10 s)
IRSL 100 s @ 50 °C
IRSL 100 s @ 170 °C
Test dose (6.5 Gy)

Preheat (200 °C for 10 s)
IRSL 100 s @ 50 °C
IRSL 100 s @ 170 °C
IRSL 50 s @ 290 °C

Lx
Tx
-

Accordingly, 200 °C was selected as the most appropriate pIRIR
preheat temperature to use for all further experiments of the protocol –
coupled with IRSL50 and pIRIR170 measurements (Table 1). These results are in agreement with other studies (Madsen et al., 2011; Reimann
et al., 2012, 2011; Reimann and Tsukamoto, 2012) which have demonstrated that a lower preheat temperature than pIRIR225 is appropriate for dating young samples. Furthermore, with existing studies
suggesting that the size of the residual dose increases with the stimulation temperature of the pIRIR measurement (Chen et al., 2013; Kars
et al., 2014), a moderate stimulation temperature is more appropriate
to reduce the size of residual signal and the likelihood of age overestimations.
Additionally, results demonstrate that a 290 °C hot bleach is required at the end of each SAR cycle to remove any remaining charge
from the test-dose and prevent transfer to the following Lx measurement
in the SAR cycle (Smedley et al., 2015). Results across both small and
large aliquot suggest that 200 °C is an appropriate preheat temperature
for these samples, with IRSL50 and pIRIR170 measurements coupled
with a hot bleach at the end of each SAR cycle.

and large aliquots. All OSL measurements were made at 130 °C for 100 s
with a 6.5 Gy test dose and 0.65 Gy given dose (Table 1).
Dose recovery ratios from the large aliquots are in line with unity
within errors for all preheat temperatures used, with a slight increase in
the ratio and spread of results found at higher temperatures, suggesting
some evidence of thermal transfer in the signal. As expected, results
from the small aliquots yielded more variability than the large aliquots

due to reduced averaging of individual signals (SI: Appendix A). Results
across all preheat temperatures demonstrate an ability to recover the
given dose within errors, yet a tighter clustering of results is identified
at 200 °C. Large variability and error margins are found on the recuperation levels across all preheat temperatures, but a general increase
with preheat temperature beyond 200 °C is observed.
High recuperation is anticipated since a small given dose was used
(c. 0.65 Gy – low dose replicates a similar signal size to the natural De)
and the recuperation level is proportionally dependent on the size of the
signal. High levels of recuperation as a percentage of the natural dose
are also expected when dating young samples and a normal distribution
of De's exist around the true dose. Rejecting De's which fail a recuperation threshold may result in an over estimation of the overall De
and thus age of the sediment. Therefore, despite some aliquots suggesting higher levels of recuperation than the widely cited 5% threshold
(Jacobs et al., 2006; Murray and Olley, 2002), 200 °C has been selected
as the most appropriate preheat temperature for dating the quartz
fraction of these sediments.

4. Comparing rates of anomalous fading
Anomalous fading is a key issue affecting the luminescence dating of
most feldspar grains (Wintle, 1973), potentially resulting in an overall
age underestimation of the sediment if not appropriately accounted for.
To determine levels of anomalous fading, short-term fading experiments were completed for both combinations of sediments (quartz
OSL130 and pIRIR170) by bleaching large aliquots of sample GSL15/1/3
and subsequently providing a known irradiation (Auclair et al., 2003).
Lx/Tx measurements were taken immediately following irradiation and
at various time intervals (up to 236 hours) after irradiation. Samples
were preheated following irradiation prior to storage (Auclair et al.,
2003) and anomalous fading results were quantified by the g-value
(Aitken, 1985). Calculation of the g-value allows for luminescence ages
for fading sediment samples to be corrected if the De lies within the
linear dose response range (Auclair et al., 2003; Huntley and Lamothe,

2001), which is typical of young sediments.
Whilst pIRIR studies have shown the pIRIR signal to be more stable
than the IRSL signal, we would expect pIRIR170 to fade more than
pIRIR225. For this purpose, testing the stability of the luminescence
signal to ensure that there is minimal anomalous fading provides
greater confidence in the natural luminescence signal measured. Fading
results for the K-feldspar pIRIR170 and quartz OSL130 fractions of sediment sample GSL15/1/3 are presented in Fig. 2. Results show that
short-term fading does not appear to be a problem across either protocol, with both values within uncertainties of zero. Quartz is thought
to not suffer from anomalous fading and values in the region
1.3 ± 0.3%/decade have previously been considered as a laboratory
artefact (Thiel et al., 2011) and suggest minimal fading. Equally, the
low values demonstrate that there is minimal short-term fading of the
pIRIR170 signal in these samples and therefore the K-feldspar fraction

3.2. K-feldspar
Existing pIRIR studies have used preheat temperatures ranging from
150 °C–290 °C. Thomsen et al., (2008) recommended a pIRIR225 protocol to reduce fading rates, yet a range of studies dating notably young
sediments have suggested the use of a lower preheat and stimulation
temperature when measuring the pIRIR signal (Madsen et al., 2011;
Reimann et al., 2012, 2011; Reimann and Tsukamoto, 2012). The basic
trade-off when selecting pIRIR temperature is that lower temperatures
bring increased bleachability at the cost of higher athermal fading rates.
Dose recovery preheat plateau experiments were completed using
samples GSL15/1/2 and GSL15/1/3 with 10 s preheats (160–255 °C) on
large and small aliquots. IRSL measurements were made at 50 °C for
100 s followed by a pIRIR measurement for 100 s with a 6.5 Gy test
dose and 0.65 Gy given dose (Table 1). Based on the method described
in Roberts (2012), all pIRIR measurement temperatures were 30 °C
cooler than the corresponding preheat temperatures.
Large aliquot results show that when preheated 160–200 °C the dose

recovery ratio is in agreement with unity, yet increases with temperature beyond this range, indicating the gradual de-trapping of progressively less bleachable traps that may not be fully bleached by 100 s
exposure to blue diodes at room temperature. Likewise, recuperation as
a percentage of the natural appears to increase as a function of temperature beyond 220 °C (increasing beyond 5%). This result is further
corroborated when De is measured on small aliquots (SI: Appendix A).
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C.E. Buckland, et al.

5. Comparing the bleaching rate of quartz and feldspar
Residual bleaching tests were used to identify the residual dose in
the quartz and K-feldspar grains following various periods of exposure
to bleaching conditions. Identifying complicating factors such as residual doses, is imperative to determining the accuracy of the resultant
natural equivalent doses, and thus in addressing the aim of identifying
an appropriate measurement method for dating young samples.
Experiments were completed for both the quartz and K-feldspar
fraction of sediment sample GSL15/1/3. Large aliquots were prepared
of each mineral fraction and exposed to bleaching conditions for various time intervals, before being measured for any residual luminescence signal. Sediments were placed outside on a flat windowsill for
different periods of daylight exposure (1–236 hours). Small aliquot
quartz OSL measurements suggest a natural De of 1.7 ± 0.06 Gy for
sample GSL15/1/3 and can be used for comparison with the residual
dose measured in the quartz and K-feldspar fractions.
Quartz results show that after all bleach times tested, all of the luminescence signal had been depleted and De‘s indistinguishable from
zero at 1σ were measured (Table 2). In comparison, the pIRIR170 signal
of the K-feldspar fraction retained a residual dose after 1.5 (0.276 Gy)
and 8 h (0.152 Gy), but was reduced to zero following an extended 236
h of daylight exposure. Based on a dose rate of 2.891 ± 0.176 Gy/ka
these results suggest that in each pulse of potential sediment activation

and deposition, K-feldspar grains may be retaining a residual dose upwards of c. 100 yrs; a significant over estimation when measuring
young samples for age of deposition (Table 2). These results are in
agreement with previous work which has suggested that the pIRIR
signal from feldspars bleaches more slowly during exposure to daylight
than the OSL signal from quartz (Buylaert et al., 2012) and typically has
a hard-to-bleach component (Kars et al., 2014).

6. Comparison of remnant doses
To test the likelihood of sediments retaining a remnant dose postdeposition in the natural landscape, remnant dose experiments were
completed for both quartz and K-feldspar fractions on known-age sediment sample BBR15/1/1. Samples were measured for their natural De
following standard SAR OSL130 and pIRIR170 protocols. Since these
samples are of known age (post-2009 AD), any luminescence signal
(> 5–6 years) measured is indicative of a remnant dose. A remnant
dose test which uses samples of a known age provides insight into how
well individual minerals have been bleached in the natural environment, under more complex bleaching conditions, which is key to interpreting natural equivalent doses and luminescence ages.
This experiment was completed for a range of aliquot sizes: large,
small and single grain to identify whether any remnant dose is restricted to a few isolated grains and can be excluded from the overall De
calculation, or whether it is more commonly found amongst the grains;
identifying the optimum mode for measuring future natural luminescence signals. Comparing the remnant dose found at a large aliquot,

Fig. 2. Anomalous fading g-values calculated for the K-feldspar and quartz
fractions of sample GSL15/1/3 according to the (a) pIRIR170, (b) IRSL50 and (c)
OSL130. All g-values were calculated using the analyse_FadingMeasurement
function (Kreutzer and Burow, 2017) in R Studio 1.0.153.

should not give an age underestimation if used to date these young
samples. By comparison, as is expected with the IRSL50 signal, a greater
degree of fading is noted in the measurements with a g-value c.4%/
decade.

Table 2
Residual doses (Gy) for large aliquots of quartz and K-feldspar grains following various time intervals outside. Residual age is calculated based on GSL15/1/3
environmental dose rate. a Time refers to daylight exposure hours experiencing variable weather conditions during January 2016. Aliquots were placed in sample
holders with a single layer of cling film used to protect aliquots from external contamination, outside on a flat windowsill facing into direct sunlight. b Dose rate based
on natural environmental dose rate from original sample site location and mineral (see Supplementary Information for dosimetry).
Protocol

Bleaching time (hours)

GSL15/1/3

OSL130

GSL15/1/3

pIRIR170

1
8
86.5
236
1.5
8
236

a

Residual ± 1σ (Gy)

Dose rate during burial ± 1σ (Gy/ka)

−0.014 ± 0.018
−0.008 ± 0.018
−0.012 ± 0.012
−0.006 ± 0.015
0.308 ± 0.023
0.134 ± 0.018
−0.072 ± 0.01

2.274 ± 0.139

2.891 ± 0.176

5

b

Equivalent residual age ± 1σ (years)
−6 ± 8
−4 ± 8
−5 ± 5
−3 ± 7
108 ± 8
47 ± 6
−25 ± 4


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C.E. Buckland, et al.

Fig. 3. De distributions of the remnant dose found in the K-feldspar and quartz fractions of sediment samples BBR15/1/1/5 and BBR15/1/1/10 when measured
following the pIRIR170 and OSL130 protocols at the single grain, small aliquot and large aliquot scale. Corresponding estimated ages are reported in Table 3.

estimates ranging from 40 ± 6 to 60 ± 6 years. By contrast, when the
MAMUL is applied to the pIRIR170 small aliquot results, an estimated age
4 ± 8 years highlights the significant potential of pIRIR protocols
when dating young sediments and applying MAM age models in depositional settings with incomplete bleaching. Results from section 5
have previously demonstrated the slower bleaching rate of the K-feldspar pIRIR170 signal relative to the quartz OSL130 signal; justifying the
choice of the minimum age model in this setting. In contrast with
previously published data, the remnant dose measured at the small
aliquot scale in this study is smaller than some previously dated modern
analogue sediments (e.g. Buylaert et al., 2009; Madsen et al., 2011;
Reimann et al., 2012; Thomsen et al., 2008) and compares well with
more recent studies (e.g. Brill et al., 2018) which have highlighted the
potentially very low remnant doses attainable using pIRIR protocols.
These significant results demonstrate the potential application of pIRIR
optical dating of K-feldspar grains to aeolian sediments in semi-arid
locations with the confidence that accurate age estimates are achievable when moderate stimulation temperatures are coupled with appropriate age models.
When measured at the single grain scale, coupled with the unlogged minimum age model, a negative De suggests that this combination is not able to recover the known age of the sediment with

small aliquot, and a single grain scale is essential to identifying the
degree of partial bleaching of sediment samples and should be used to
inform the appropriate mode of measuring natural equivalent doses
from other samples in the region.
Results from the remnant dose test are shown for both protocols
(OSL130 and pIRIR170) against a variety of aliquot sizes, with equivalent
doses calculated following both the unlogged-Minimum Age Model
(MAM-3) and unlogged-Central Age Model (CAM) age models following
the recommendation of Arnold et al. (2009) (Fig. 3 and Table 3). The

results are used to explore whether it is possible to identify an appropriate combination of measurement protocol, mineral and age model
selection which reduces the remnant dose to the expected level.
For the pIRIR170 signals measured, the De distributions are broadly
unimodal, with a multi-modal peak in the large aliquot results potentially a factor of a small sample size or a residual dose associated with a
particular aeolian event. De distributions increase in width as the
number of grains measured decreases (i.e. from large aliquot → small
aliquot → single grain measurements). K-feldspar pIRIR170 results vary
greatly between the single grain and multigrain measurements, especially when modelled through the two different unlogged-age models.
Large aliquot (both MAMUL and CAMUL) results and small aliquot
CAMUL results are dominated by a small remnant dose with age

Table 3
Table comparing the remnant dose results when tested on different minerals, protocols, aliquot size and age model. 1 Samples BBR15/1/1/5 and BBR15/1/1/10 were
used for measurement. Both sub-samples came from vertical sediment core BBR15/1/1 which was extracted from the near-surface sediments of a lunette dune which
has formed since 2009 on the Barta Brothers Ranch. The lunette dune formed on the edge of a grassland destabilisation plot and buried a fence line that was erected in
2009 to surround the circular plot. All 50 cm of the BBR15/1/1 vertical core should theoretically be of ∼6 years old; BBR15/1/1/5 and BBR15/1/1/10 are subsamples from 5 to 10 cm depth respectively. 2 Hot bleach (@ 290 °C for 50 s) included at the end of each SAR cycle in the pIRIR170 protocol. 3 Ages ± 1σ (years).
Moisture content 5 ± 2% and overburden density 1.8 g/cm3 used for all samples. 4 Single grain (180–210 μm). 5 Small aliquots at 2 mm (grain size 125–180 μm). 6
Large aliquots at 8 mm (grain size 125–180 μm).
Mineral

Sample

1

Protocol

Hot Bleach

2

Age ± 1σ (years)
Single Grain

K-Feldspar
Quartz

BBR15/1/1/5 &/10
BBR15/1/1/10

pIRIR170
OSL130

Y
N

3

4

Small Aliquot

5

Large Aliquot

6

MAM-3UL

CAMUL

MAM-3UL

CAMUL

MAM-3UL

CAMUL

−18 ± 7 n = 49
−51 n = 7

52 ± 29 n = 49
−51 n = 7

4 ± 8 n = 11
n/a
n = 27

40 ± 6 n = 11
4 ± 7 n = 27

40 ± 8 n = 6
30 ± 2 n = 6

60 ± 6 n = 6
29 ± 42 n = 6

6

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C.E. Buckland, et al.

estimated De dominated by the negative values associated with a
handful of individual grains. A greater volume of measured single grain
measurements could potentially improve this result and yield an estimated age closer to the known age of the sediment. Whereas, results
from the single grain K-feldspar dating coupled with the CAMUL equally
produce age estimates within 2σ errors of the known sediment burial
date (i.e. 2009 AD) and demonstrate the potential for the technique to
be applied as a geochronological tool in historical environmental and
archaeological research. However, the large spread in the single grain
De's, coupled with the large uncertainty estimates, (likely driven by the
noisy nature of the single grain decay curve) restricts the capacity to
calculate more precise age estimates and use in investigating environmental dynamics on timescales at the sub-decadal scale.
For the OSL130 signals measured, the De distributions are unimodal
across the three combinations with the results from the large aliquots
producing the narrowest spread, but also with the greatest remnant
dose due to a bigger combined signal of grains (c.1760 grains for large
aliquot, c.109 grains for small aliquot) with varying levels of bleaching,
and an individual aliquot which produced a larger De outside of the
general unimodal distribution. In comparison, single grain results,
coupled with the minimum or central age model both demonstrated the
lowest residual dose with age estimates indistinguishable from zero. It
is likely that the very young (i.e. 2009 AD) age of the sediments means
that despite the relatively high dose rates found in the sediments (c.2.2
Gy/ka), individual luminescence decay curves are too dim to extract a
measurable decay curve amongst the noise and very few grains are
emitting a measurable signal (i.e. only 6 grains out of 400 grains

measured produced decay curves for the largest regeneration dose
point).
As discussed in Ballarini et al. (2007), the signal levels released by
individual grains from recently deposited samples can be much lower
than in older sedimentary deposits, a function of a smaller absorbed
dose and potentially reduced sensitivity if extracted from newly eroded
material, and coupled with a small percentage of grains giving rise to a
De value (e.g. Duller et al., 2000; Duller and Murray, 2000; Jacobs
et al., 2013). Nevertheless, existing studies have equally shown that
single grain quartz luminescence dating can successfully be applied to
recently deposited sediments, yielding ages within the last 200 years
when applying a modified SAR protocol (incorporating an IR wash prior
to OSL stimulation) (Olley et al., 2004), the minimum age model, and
simulating synthetic small aliquots (e.g. 10 grain aliquots) (e.g. Brooke
et al., 2008; Olley et al., 2004).
As Fig. 4 highlights, if all grains provided the same luminescence
signal, a linear line through the origin would be plotted. However, results from BBR15/1/1/10 s show that over 90% of the OSL signal originates from less than 10% of the grains, suggesting the majority of
grains do not contribute to the overall luminescence signal. Likewise,
the luminescence signal from aliquots of GSL15/1/3, a much older sediment, is largely driven by less than 40% of the total number of grains.
The most appropriate aliquot size and age model combination for
luminescence dating these particular sediments is therefore identified
as small aliquots (2 mm) of either quartz OSL130 coupled with the unlogged central age model which produced an age estimate of 4 ± 7
years or K-feldspar pIRIR170 with the un-logged minimum age model
which produced an age estimate of 4 ± 8 years, both of which are in
good agreement with the known-age of 5–6 years of the sediments.
Given the aeolian dune context of these sediments, we expect quartz
sediments to be well-bleached prior to deposition and thus the central
age model presents the most appropriate age model for quartz analysis
(Bailey and Arnold, 2006). Aeolian sediment deposition in dryland
dune environments is likely followed by rapid further burial from deposited sand grains, relying on the bleaching of the luminescence signal

to occur during transportation and immediate deposition. The requirement for K-feldspars to be exposed to sunlight for much longer
periods of time (e.g. up to 30 days – Table 2) to fully remove the preburial dose cannot be guaranteed in the natural environment. Thus,

Fig. 4. Distribution of signal intensity from single grains of four discs of sediment sample BBR15/1/1/10. The proportion of the total OSL light sum from
the cumulative grains is plotted as a function of the proportion of the brightest
grains. If all grains in a population had the same level of brightness, the results
would plot along the 1:1 diagonal line that runs through the origin. ‘n’ denotes
number of grains measured.

whilst K-feldspar pIRIR170 has reproduced De estimates within errors of
the known sediment age, the results from the quartz OSL130 measurements may be more reliable in a context where we cannot guarantee
long periods of exposure to sunlight. Alternatively, the most wellbleached population of estimated De's could be extracted from pIRIR170
results if combined with the MAM.
Results in this section have suggested that small aliquots of both
quartz OSL130 and K-feldspar pIRIR170 measurements can yield the
expected age when aliquot size and incomplete bleaching are taken into
consideration. Dose distribution results suggest a tighter clustering of
results in the OSL130 example, whilst a larger spread in De is found with
pIRIR170 results (Fig. 3) – likely attributed to a range of incomplete
bleaching. Consequently, the pIRIR170 MAM age estimate (4 ± 8
years) is largely driven by the De associated with a single aliquot
(Fig. 3). Whilst the single aliquot has incidentally yielded the expected
age in this example, it would not be advisable to assume that the MAM
of pIRIR170 results would always yield the correct age unless multiple
discs from this age population could be measured. This being said, the
K-feldspar results shown are promising and offer an alternative method
to OSL protocols across a range of settings. For example, in regions of
rapid bedrock erosion, local quartz sediments that have not been sensitised over numerous cycles of bleaching and deposition may be too
dim to produce useful luminescence signals for dating. By comparison,
as noted earlier, the naturally bright K-feldspar grains coupled with

high internal dose rates offers an alternative approach when partially
bleached signals can be removed using appropriate age model selection.

7. Selection of appropriate rejection criteria for young samples
Whilst section 6 has identified that both quartz and K-feldspar have
the potential to accurately date these young aeolian sediments, this
section discusses the details of the appropriate rejection criteria and
analysis methods for studying young, dim luminescence signals. In
addition to standard recycling and IR-depletion ratio tests, recuperation
thresholds and De(t)-plot analysis of quartz signals were used to identify
the most appropriate criteria for including individual aliquots in overall
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C.E. Buckland, et al.

Table 4
Quartz De ± error calculated according to the application of the different recuperation threshold options. Recycling ratio and IR-depletion ratio rejection criteria is
applied to all four combinations, and subsequently combined with a different recuperation threshold based on % of Natural dose, absolute value (seconds), and % of
largest Regeneration dose. De's have been calculated according to the un-logged Central Age Model with moisture content 3 ± 2% and overburden density 1.9 g/cm3
used for all samples.
Sample

Aliquots measured
a

GSL15/1/3

48

e

BBR15/1/1/10

30

e

a
b
c
d
e
f

Passed recycling ratio & IRdepletion ratiob
De ± error (Gy)

Passed recuperation as % of
natural (5%)
De ± error (Gy)

Passed recuperation as absolute
value (1 s)c
De ± error (Gy)

Passed recuperation as % of largest
regen (5%)d

De ± error (Gy)

37 aliquots
1.7 ± 0.06
27 aliquots
0.008 ± 0.01

31 aliquotsf
1.65 ± 0.063
13 aliquots
0.02 ± 0.018

35 aliquotsf
1.65 ± 0.059
21 aliquots
0.023 ± 0.013

37 aliquotsf
1.7 ± 0.06
27 aliquots
0.008 ± 0.01

Small aliquots of fully-prepared quartz grains measured.
Recycling ratio and IR-depletion ratio within ± 10% of unity.
c.0.0647 Gy based on and beta source conversion 0.0647 Gy/s.
Largest regeneration dose ∼ c.9 Gy.
One aliquot of GSL15/1/3 and three aliquots of BBR15/1/10 were rejected due to partial bleaching. See section 7.3 for rationale.
Denotes aliquots that passed recuperation test in addition to the recycling ratio or IR-depletion ratio.

unsuitable for these very young sediments. When measured using the

small aliquot population identified as yielding accurate age estimates
(4 ± 8 years), application of a recuperation threshold as either 5% of
the natural or largest regenerative dose leads to a rejection of all of the
aliquots.
When the recuperation threshold is increased to 7% of the largest
regenerative dose, 64% of the aliquots are accepted and the revised
MAMUL ages overestimate the known age of the sediment. The aliquots
yielding the lowest individual De's have been rejected (0.01 ± 0.01 Gy
and 0.05 ± 0.01 Gy) due to proportionally high recuperation levels,
yet when assessed as an absolute value, the recuperation of these aliquots is indistinguishable from the remaining aliquots. These results
therefore agree with the analysis from the quartz fraction, that recuperation does not appear to systematically vary between the aliquots
and a threshold value runs the risk of arbitrarily biasing the overall age
estimate towards the larger De's measured.

age model calculation.
7.1. Recuperation
As noted above, recuperation values associated with dating young
aeolian sediments need to be treated carefully and a threshold should
be applied with caution. Naturally high recuperation levels are expected when dating young sediments due to the noisy nature of the
signals and the close proximity of the natural and zero dose points.
Whilst an absolute recuperation threshold can be used as opposed to a
relative value as percentage of the natural, this can only be applied if
there is confidence that the natural De is not modern or close to the
threshold set; prior knowledge of the expected age is required.
Alternatively, a recuperation threshold can be applied as a % of the
largest regeneration dose (King et al., 2013).
When applied to the quartz luminescence fraction, a comparison of
the different recuperation thresholds (Table 4) highlights that whilst
the impact on the overall De of older sediments is minimal, it has a
much greater influence on the overall De of a very young sediment age

where the De is more than doubled when recuperation as a percentage
of natural or an absolute value is applied. As noted above these are not
appropriate parameters to reject young luminescence signals and can
lead to an estimated age overestimation. Whereas, the recuperation
rejection when based on a percenteage of the largest regeneration does
not highlight any additional aliquots that needed to be rejected. Since
minimal recuperation has been identified in these particular signals, it
is not considered a key rejection criteria to apply to these sediments
when measured according to the OSL130 protocol.
The results from the K-feldspar pIRIR170 analysis (Table 5) equally
suggest that rejection based on recuperation rejection criteria is

7.2. Identifying partial bleaching and dominant slow components in the
quartz OSL130 signal using De(t) plots
Whilst dose distribution plots and bleachability tests have shown
the partially-bleached nature of the K-feldspar pIRIR170 signal, an alternative approach using a series of De(t)-plots was used to identify
quartz aliquots which would contribute to an age overestimation. If all
components of the OSL130 luminescence signal were reset prior to deposition, movement of the signal interval along the decay curve would
result in a flat De(t)-plot, or rise in the case of partial bleaching (Bailey
et al., 2003).
Results from sediment sample BBR15/1/1/10 highlight three aliquots (referred to as ‘A’, ‘B’,’C’) which demonstrate markedly larger De's

Table 5
K-feldspar De ± error calculated according to the application of the different recuperation threshold options. Recycling ratio rejection criteria is applied to all five
combinations, and subsequently combined with a different recuperation threshold based on % of Natural dose, absolute value (seconds), and % of largest
Regeneration dose. De's have been calculated according to the un-logged Minimum Age Model (identified as the most appropriate age model for these partiallybleached samples as discussed in section 6), with moisture content 3 ± 2% and overburden density 1.9 g/cm3 used for all samples.
Sample

Aliquots
measureda

Passed recycling
ratiob
De ± error (Gy)

Passed recuperation as % of
natural (5%)
De ± error (Gy)

Passed recuperation as
absolute value (1 s)c
De ± error (Gy)

Passed recuperation as % of
largest regen (5%)d
De ± error (Gy)

Passed recuperation as % of
largest regen (7%)d
De ± error (Gy)

BBR15/1/1/
5

11

11 aliquots
0.01 ± 0.02

0 aliquotse

n/a

11 aliquotse
0.01 ± 0.02

0 aliquotse
n/a

7 aliquotse
0.08 ± 0.01

a
b
c
d
e

Small aliquots of fully-prepared K-feldpsar grains measured.
Recycling ratio within ± 10% of unity.
c.0.0647 Gy based on and beta source conversion 0.0647 Gy/s.
Largest regeneration dose ∼ c.9 Gy.
Denotes aliquots that passed recuperation test in addition to the recycling ratio.
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C.E. Buckland, et al.

Fig. 5. (a) Z-value vs. De (based on initial integration window) plot based on De(t)-plots of Bailey (2003). Dashed line: aliquots inside dashed circle represent

partially-bleached signals that contain a greater proportion of the pre-burial dose. Dotted line: aliquots inside dotted circle are those with large Z-values, but low De
values. (b) Z-value vs. De (based on initial window) and De (based on final integration window). Aliquots with typically high Z-values and low De are shown to have
over-lapping initial and final De values. The large uncertainties associated with these aliquots is driven by the noisy dim signal and requires further analysis than > 1
Z-value to qualify as partially bleached. Likewise, some aliquots with high Z-values are artificially driven by negative final De values and equally are not partially
bleached despite Z-value > 1. Three aliquots highlighted in red (‘A’, ‘B’, ‘C’) depict those which show Z-values which suggest partial bleaching – initial and final De
values do not overlap, Z-values > 1, and all De's > 0. For the remaining samples with high Z-values, error bars associated with the Z-values and De estimates
demonstrate that whilst displaying high Z-values, the De's at various integration intervals are within errors and therefore the > 1 Z-values have not been analysed
further. (For interpretation of the references to colour in this figure legend, the reader is referred to the Web version of this article.)

than the remaining aliquots are also those which display rising De(t)plots and Z-values > 1 (Fig. 5). Z-values refer to the ratio of the De
from the final integral to that of the first channel (Bailey, 2003). By
replacing the natural dose with a regeneration dose point, it is possible
to test whether this rising De(t)-plot is driven by partial bleaching, or a
dominant slow component within these sediments. Under controlled
bleaching conditions, we would not expect a rising De(t)-plot associated
with the regenerative dose point unless the signal has been dominated
by the slow component in these samples with an overall low luminescence signal.
When calculated with a regeneration dose point, results suggest
aliquots ‘B’ and ‘C’ were partially bleached (Z-value < 1) (Table 6); it
is likely that these aliquots contain a couple of grains that were not
well-bleached in the reactivation event. Whilst the majority of grains
may be well-bleached, the near-surface nature of the samples may experience post-depositional mixing (Bateman et al., 2007) or partialbleaching of due to deposition at night (insufficient ambient light) or
during a rapid process (e.g. dust storm), preventing every grain from
being fully-bleached. Meanwhile, aliquot ‘A’ continues to demonstrate a
rising De(t)-plot despite being bleached within the SAR cycle prior to
further irradiation and measurement.

Table 6
Z-values associated with three aliquots for both the natural luminescence signal
and a regeneration dose point. Z-values for aliquots ‘B’ and ‘C’ are < 1 when

replaced with the regeneration dose point, suggesting the natural luminescence
signal was partially bleached.
Aliquot

Z-value (Natural)

Z-value (Regen point)

A
B
C

1.67
16
4.60

1.3
0.42
0.77

Through component fitting of the regenerative dose luminescence
decay curve for aliquot ‘A’, the contribution of each of the individual
components of the OSL decay curve can be calculated. Fig. 6 highlights
that the slow and medium components of the signal are contributing to
almost 60% of the total luminescence signal in the first instance, and
rapidly rise to 100% of the overall signal within 2 s of measurement
time.
The reason for the rise in De(t) remains unclear, but may be associated with incorrect background subtraction (e.g. if there is significant
decay of the slow component in the time prior to background
9

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C.E. Buckland, et al.

the likelihood and size of a residual dose; reducing the applicability of
this protocol to young aeolian sediments if not paired with the most
appropriate age model.
Single-grain pIRIR measurements yield more varied results, likely
attributed to a small sample size and relatively low photon count.
Nonetheless, the success of the small aliquot dating is significant and
demonstrates that pIRIR methods have the scope to produce accurate
luminescence ages with reduced levels of fading than IRSL equivalents.
As expected, both large and small aliquots of quartz OSL130 measurements produce De values in line with the expected age based on historical data. Due to fast bleaching rates the un-logged central age model
provides the most appropriate age model to use when calculating age
estimates.
Additionally, we find a revised set of rejection criteria is useful for
accurately identifying aliquots/grains for reliable age estimation. In
particular, sensitivity testing a range of recuperation rejection criteria
highlights the caution that should be taken to avoid arbitrarily applying
rejection criteria and biasing towards age overestimations. Problems of
incomplete bleaching or slow component dominance of the occasional
grain have highlighted the importance of selecting the most appropriate
aliquot size for measurement and rejection criteria, analysis and agemodel selection post-measurement.
Investigations into aliquot sizes show that without a widespread
issue with partial bleaching in the quartz fraction, single grain analysis
is not needed for De calculation and small aliquots have an advantage of
producing greater signal sizes. Whilst large aliquots would provide an
even greater signal, they are susceptible to partial bleaching or slow

component dominance which lead to an overall age overestimation.
Thus, a trade off option that allows us to maximise the signal but not
miss the aliquots that hide issues of partial bleaching is needed. In this
study, small aliquots of both quartz OSL130 and K-feldspar pIRIR170
have demonstrated the most promising results, allowing us to identify
partial bleaching of K-feldspar through bleachability tests, dose distribution plots and the MAM, whilst partially bleached quartz grains are
identified through the use of De-(t) plots and Z-values, but without the
weak noisy signals of the single grain analysis. When markedly larger
De's are identified within individual aliquots, De(t)-plots and component-fitting analysis can be used to identify the most well-bleached
quartz aliquots and those which have a dominant fast component.

Fig. 6. Luminescence decay curve and component fit of regeneration dose point
aliquot ‘A’. Three components identified: fast, medium, slow with individual
component contributions as % of the total OSL signal listed vs. Time (seconds).
Component fitting completed using the fit_CWCurve function of the
‘Luminescence’ package in R Studio 1.0.153 (Kreutzer, 2017).

measurement). As a conservative measure, we suggest rejecting all
aliquots that display this signal feature in these sediment samples, to
reduce the likelihood of ‘false-positives’. Aliquots which display these
characteristics should either be rejected since they will lead to a significant age overestimation of young samples, or individual fast components need to be extracted from the overall luminescence decay and
De's calculated accordingly for that individual component. Previous
curve fitting experiments (e.g. Jain et al., 2003; Tsukamoto et al., 2003)
have demonstrated that the fast component shows less recuperation due
to thermal transfer when preheating than the slow and medium components; another reason why luminescence signals with a strong fast
component should be selected, especially for young samples with a
comparatively small De.

Acknowledgements
This work was supported by the UK Natural Environment Research

Council (grant: NE/L002612/1), Jesus College Graduate Research
Allowance funding, and Elsevier Travel Grant (October 2015). The first
author is funded by NERC (grant: NE/L002612/1) as part of the
Environmental Research Doctoral Training Program at the University of
Oxford. We thank Drs Paul Hanson and Dave Wedin (University of
Nebraska-Lincoln) and the staff at Gudmundsen Sandhills Laboratory
for assistance and field site access. The authors would like to thank Drs
Tony Reimann and Nathan Brown for their valuable comments and
advice on earlier drafts of the manuscript.

8. Conclusions
In this study, sediments extracted from a very young lunette dune of
known-age (5–6 years) provided a reliable test case for identifying the
most suitable measurement and analysis combinations for dating young
aeolian dune sediments. Given the young nature of the sediments,
identifying the most rapidly bleached signal is imperative to ensure low
remnant doses and a more accurate chronology is produced. Whilst Kfeldspar rich samples showed slower bleachability results when left to
bleach under natural conditions versus quartz counterparts, when
measured using the pIRIR170 protocol and paired with MAMUL, age
estimates of a known age sediment were both accurate and equally as
precise as the quartz OSL130 CAMUL measurements. pIRIR protocols
have increased the suitability of K-feldspar luminescence dating to a
range of research projects, identifying and stimulating deeper electron
traps which exhibit reduced levels of anomalous fading, yet require
much longer bleaching periods to reduce residual doses and improve
dating accuracy when measuring young sediments in a dynamic environment. Results from this study are in agreement with those reported
by Buylaert et al. (2012) which show that the pIRIR signal bleaches
more slowly than that from quartz when exposed to sunlight, increasing

Appendix A. Supplementary data

Supplementary data to this article can be found online at https://
doi.org/10.1016/j.radmeas.2019.106131.
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