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Archeointensity study on baked clay samples taken from the reconstructed ancient kiln: implication for validity of the Tsunakawa-Shaw paleointensity method

Earth, Planets and Space201567:63

https://doi.org/10.1186/s40623-015-0229-8

©  Yamamoto et al.; licensee Springer. 2015

  • Received: 16 January 2015
  • Accepted: 14 April 2015
  • Published:

Abstract

In 1972, a reconstruction experiment of a kiln had been done to reproduce an excavated kiln of the seventh century in Japan. Baked clay samples were taken from the floor surface and −20 cm level, and they have been stored after determinations of the paleomagnetic directions by partial alternating field demagnetizations. We recently applied the Tsunakawa-Shaw method to the samples to assess how reliable archeointensity results are obtained from the samples. A suite of the rock magnetic experiments and the scanning electron microscope observations elucidate that dominant magnetic carriers of the floor surface samples are Ti-poor titanomagnetite grains in approximately 10 nm size with single-domain and/or super-paramagnetic states, whereas contributions of multi-domain grains seem to be relatively large for the −20-cm level samples. From the floor surface samples, six out of the eight successful results were obtained and they give an average of 47.3 μT with a standard deviation of 2.2 μT. This is fairly consistent with the in situ geomagnetic field of 46.4 μT at the time of the reconstruction. They are obtained with a built-in anisotropy correction using anhysteretic remanent magnetization and without any cooling rate corrections. In contrast, only one out of four was successful from the −20-cm level samples. It yields an archeointensity of 31.6 μT, which is inconsistent with the in situ geomagnetic field. Considering from the in situ temperature record during the firing of the kiln and the unblocking temperature spectra of the samples, the floor surface samples acquired full thermoremanent magnetizations (TRMs) as their natural remanent magnetizations whereas the −20-cm level samples only acquired partial TRMs, and these differences probably cause the difference in the archeointensity results between the two sample groups. For archeointensity researches, baked clay samples from a kiln floor are considered to be ideal materials.

Keywords

  • Archeointensity
  • Absolute paleointensity
  • Baked clay
  • Kiln
  • Tsunakawa-Shaw method

Background

Recent advances in archeomagnetism have resulted in sophisticated databases for published archeomagnetic data. For example, the GEOMAGIA50 database (Donadini et al. 2006; Korhonen et al. 2008) involves about 8,000 geomagnetic field directions and intensities for the past 50 kyr. The ARCH3k database by Donadini et al. (2009) contains 2,671 declination, 4,174 inclination, and 2,670 intensity data from archeological artifacts and lavas for the past 3 kyr. Genevey et al. (2008) compiled the Archeoint database for the past 10 kyr which has 3,648 archeointensity records reported from archeological artifacts and lavas.

Concerning the Archeoint database, 70% of the records are from Europe while only 12% of them are from East Asia. Among the East Asia records, 188 data are from Japan: 145 data from archeological artifacts (9 data, Nagata and Arai (1963); 19 data, Sasajima and Maenaka (1966); 56 data, Kitazawa (1970); 6 data, Domen (1977); 58 data, Sakai and Hirooka (1986)) and 43 data from lavas (7 data, Nagata and Arai (1963); 2 data, Sasajima and Maenaka (1966); 6 data, Kono (1978); 1 data, Tanaka (1979); 13 data, Tanaka (1980); 3 data, Tsunakawa and Shaw (1994); 1 data, Takai et al. (2002); 10 data, Yoshihara et al. (2003)).

In broad sense, ‘archeointensity’ stands for an absolute paleointensity of the geomagnetic field during historical period which is estimated from both archeological artifacts and lavas. In narrow sense, the estimation material is limited to archeological artifacts. Generally speaking, archeological artifacts have been considered to be more reliable paleointensity recorders, because they were certainly burned/baked by our ancestors and their natural remanent magnetizations (NRMs) are definitely thermoremanent magnetization (TRM) origin with good thermal stability.

There has been a long gap in time since the last internationally recognized archeointensity result was published from archeological artifacts in Japan (e.g., Sakai and Hirooka 1986). In contrast, brand new data with modern paleointensity techniques have been published from East Asia outside Japan, for example, Korea (Yu et al. 2010; Hong et al. 2013) and China (Cai et al. 2014). In 1960s to 1970s, a group of Japanese researchers had made systematic oriented-sample collections from baked clay at many pottery kilns excavated in and around Sakai city, Osaka prefecture, Japan. The collections were associated with a lot of excavations arising from a big demand of housing land developments due to the growing economy in Japan at that time. Paleomagnetic directions for fifth to tenth centuries were intensively measured from these samples, and they were published by Hirooka (1971) and Shibuya (1980). Untreated and/or partially demagnetized samples have been reserved and stored for further archeointensity (paleointensity) researches.

A relatively large number of the reserved samples were partially demagnetized by alternating field (AF) up to 20 to 40 mT. Thus, AF-based paleointensity techniques are thought to be suitable for these samples. The Tsunakawa-Shaw method, which has been previously called the LTD-DHT Shaw method (Tsunakawa and Shaw 1994; Yamamoto et al. 2003), is one of such techniques. Its applicability and validity have been elucidated for various types of volcanic rocks from historical lava flows (e.g., Yamamoto et al. 2003; Mochizuki et al. 2004; Oishi et al. 2005; Yamamoto and Hoshi 2008) but remain unassessed for archeological artifacts including baked clay.

In the vicinity of the archeological sites, Nakajima et al. (1974) conducted a reconstruction experiment: they reconstructed a kiln which was carefully imitating an excavated kiln of the seventh century and measured paleomagnetic directions from baked clay samples taken from the kiln. These samples have been reserved and stored after partial AF demagnetization by 20 to 40 mT in 1972. In the present study, we applied the Tsunakawa-Shaw method to these samples. Because the reconstruction experiment was done after the measurement of the in situ geomagnetic field, we can compare the in situ filed with archeointensity results obtained by the Tsunakawa-Shaw method. We also conducted a suite of rock magnetic experiments and an observation with scanning electron microscope, to characterize rock magnetic properties of the samples.

Reconstruction experiment

The reconstruction experiment was conducted in Sakai city, Osaka, Japan, on January 1972 (Nakajima et al. 1974). A Noborigama kiln, which was carefully imitating an excavated one of the seventh century, was reconstructed and fired with many Sue-type earthenwares in it (Figure 1).
Figure 1
Figure 1

A series of the photographs taken during the reconstruction experiment by Nakajima et al. (1974). (a) Local trees and weeds were trimmed to reconstruct a Noborigama kiln. (b) Ground was dug up. (c) In situ geomagnetic field was measured by a Schmidt-type magnetometer. (d) Thermocouples were embedded in and around the kiln to record in situ temperature variations during firing. (e) White circles indicate example locations of the thermocouple contacts. (f) A body of the kiln was made up with bamboos and tree branches, which were subsequently covered and coated with clay. (g) Sue-type earthenwares to be fired. (h) Firing was done using naturally grown pine trees and other miscellaneous woods taken around the kiln. The bamboos and tree branches were gutted by fire, and baked clay remained as the kiln body. (i) Inside view of the kiln after firing. (j) Cross-section of the fire hole after firing. (k, l) Baked clay was carefully sampled from the floor surface (k) and the −20-cm level (l) using plaster with orientation.

After cutting the trees and weeds (Figure 1a), the ground was dug up (Figure 1b). Then in situ geomagnetic field was measured by a Schmidt-type magnetometer (Figure 1c): declination (Dec) = −5.63°, inclination (Inc) = 46.78°, and intensity (Int) = 46.350 μT. This is fairly consistent with the field calculated from the model of IGRF-11 (IAGA Division V, Working Group V-MOD 2010) at the place for the year of 1972: Dec = −6.23°, Inc = 47.7°, and Int = 46.438 μT. To record in situ temperature variations during the firing, thermocouples were embedded in and around the kiln (Figure 1d,e). After the embedment, the body of the kiln was made up with bamboos and tree branches, and they were subsequently covered and coated with clay (Figure 1f). With Sue-type earthenwares, the firing was done using naturally grown pine trees and other miscellaneous woods taken around the kiln (Figure 1g,h).

It was found that the temperature very close to the floor surface (−2-cm level, three different positions) was risen up to approximately 1,000°C while that at the level 20 cm below the floor (−20-cm level) was only up to approximately 350°C during firing (Figure 2). After reaching to the highest temperature of approximately 1,000°C, the fire hole and the chimney of the kiln were blocked to make the inside reductive atmosphere. The kiln was then naturally cooled down for approximately 24 h. After the cooling down (Figure 1i,j), baked clay was carefully sampled from the floor surface (Figure 1k) and the −20-cm level (Figure 1l) using plaster of Paris for accurate orientation. Each sample was cut in laboratory into cubic shape with approximately 3.7 cm on a side.
Figure 2
Figure 2

Variations of the in situ temperatures in the reconstructed kiln during firing. Red curves indicate the temperature variations at the three different locations very close to the floor surface (−2-cm level) while gray one shows that at the −20-cm level. The curves are redrawn from Nakajima et al. (1974).

The samples were subjected to partial AF demagnetization up to 20 to 40 mT. Nakajima et al. (1974) reported that the mean paleomagnetic directions resulted in Dec = −5.03°, Inc = 43.37°, and α95 = 2.42° for the floor surface samples (N = 10) and in Dec = −4.80°, Inc = 43.52°, and α95 = 3.38° for the −20-cm level samples (N = 5). These directions were reasonably consistent with the in situ geomagnetic field direction measured prior to the firing, though the mean inclinations were approximately 3° shallower than the in situ field.

Methods

Samples

The cubic samples had been stored for approximately 40 years in an ambient field after the partial AF demagnetization. In the present study, eight samples from the floor surface (numbered 1, 2, 5, 8, 9, 11, 12, and 13) and four samples from the −20-cm level (numbered 15, 16, 18, and 19) were prepared for the experiments. They were cut vertical to horizontal planes into two pieces, one of which was reserved as an archive while the other was further cut into several mini specimens for paleointensity and rock magnetic experiments (Figure 3a). The floor surface samples are all reddish (Figure 3b) whereas the −20-cm level ones are all grayish (Figure 3c).
Figure 3
Figure 3

Photographs showing the samples used for archeointensity (paleointensity) and rock magnetic experiments. (a) An original cube sample (approximately 3.7 cm on a side) is vertically cut into two pieces. One is reserved as an archive while the other is further cut into several mini specimens for archeointensity (paleointensity) and rock magnetic experiments. Example photographs are shown for sample 1 from the floor surface. (b) An example photograph for sample 5 from the floor surface. (c) An example photograph for sample 16 from the −20-cm level.

Rock magnetic experiments

The hysteresis parameters, saturation magnetization (M s), saturation remanent magnetization (M rs), coercive force (B c), and coercivity of remanence (B rc) were measured for two to four chips from each sample, using a vibrating sample magnetometer (MicroMag 3900 VSM, Princeton Measurements Corporation, Princeton, NJ, USA). Thermomagnetic curve measurements were performed in vacuum (approximately 1 to 10 Pa) on chip samples from most of the samples using a magnetic balance (NMB-89, Natsuhara Giken, Osaka, Japan). In the measurements, chip samples were gradually heated from approximately 30°C to 700°C and then gently cooled to approximately 50°C, with the rate of 10°C/min. Throughout the temperature cycle, a field of 500 mT was kept applied to the sample.

To obtain unblocking temperature (TUB) spectra data for NRMs and isothermal remanent magnetizations (IRMs) both from the floor surface and the −20-cm level samples, each of two mini specimens from the samples 5 and 16 is subjected to thermal demagnetization (ThD) experiments. Because NRMs of the two samples were already demagnetized by AF of 20 mT in Nakajima et al. (1974), for a one set of the specimens, IRMs of 2.5 T were imparted by a pulse magnetizer (MMPM10, Magnetic Measurements, Lancashire, UK) and subsequently demagnetized at 20 mT using an AF demagnetizer (DEM-95, Natsuhara Giken). Stepwise ThD was then conducted on NRMs and IRMs of the mini specimens at 30°C to 50°C steps up to 600°C using a thermal demagnetizer (TDS-1, Natsuhara Giken). Remanent magnetizations were measured by a spinner magnetometer (ASPIN-A, Natsuhara Giken).

Scanning electron microscope (SEM) observation

Sliced pieces from the samples 5 and 16 were impregnated with epoxy and subsequently polished to mirror gloss. The polished surface of the pieces was then thin-coated with platinum and they were observed by a field emission scanning electron microscope (FE-SEM, JSM-6500F, JEOL Ltd., Akishimashi, Tokyo, Japan). We took backscattered electron images (BEIs) and made point analyses based on an energy-dispersive X-ray spectroscopy (EDS). Spatial resolution was as good as 10 to 100 nm in a BEI whereas it was a few micrometers at best for an EDS point analysis.

Tsunakawa-Shaw paleointensity experiments

The Tsunakawa-Shaw method (Tsunakawa and Shaw 1994; Yamamoto et al. 2003) was applied to mini specimens from all the samples to determine archeointensities (absolute paleointensities). This method estimates archeointensities based on coercivity spectra rather than blocking temperature spectra. Detailed procedures are described in Yamamoto and Tsunakawa (2005).

Main procedures in the present study are as follows:
  1. i.

    A specimen undergoes low-temperature demagnetization (LTD; Ozima et al. 1964). NRM after LTD is subjected to stepwise AF demagnetization. The remanence is measured at each step [NRM].

     
  2. ii.

    Anhysteretic remanent magnetization (ARM) is imparted to the specimen. Then, the specimen undergoes LTD. ARM after LTD is subjected to stepwise AF demagnetization and is measured at each step [ARM0].

     
  3. iii.

    The specimen is heated in a furnace to impart full TRM for the first time. Then, the same procedures as (i) and (ii) are performed for the TRM [TRM1] and ARM [ARM1].

     
  4. iv.

    The specimen is heated in the furnace to impart TRM for the second time. The same procedures as (i) and (ii) are performed for the TRM [TRM2] and ARM [ARM2].

     

For the remanent magnetization measurements, stepwise AF demagnetizations, and the impartment of ARMs, we used an automated spinner magnetometer with an AF demagnetizer (DSPIN, Natsuhara Giken). The demagnetizations were conducted up to 180 mT, with the steps at 2-mT intervals up to 30 mT, at 5-mT intervals up to 100 mT, and 10-mT intervals up to 180 mT. ARMs were imparted using a DC bias field of 50 μT with a peak AF of 180 mT, by setting the bias field direction approximately parallel to the NRM and laboratory TRM directions. LTD was conducted such that specimens were soaked in liquid nitrogen for 10 min and subsequently left at room temperature for 30 min in a zero field. For the impartment of TRMs, we used a thermal demagnetizer equipped with a DC field coil (TDS-1, Natsuhara Giken). The specimens were heated to 610°C in a vacuum (1 to 10 Pa) with the hold time of 10 (TRM1) and 20 (TRM2) min at that temperature and subsequently cooled down to room temperature for approximately 2 h in a 40-μT DC field throughout this process.

Obtained results were analyzed based on NRM-TRM1* and TRM1-TRM2* diagrams. TRM1* and TRM2* denote the TRM imparted in the first (TRM1) and second (TRM2) heating, as corrected using the technique of Rolph and Shaw (1985):
$$ \mathrm{T}\mathrm{R}\mathrm{M}1* = \mathrm{T}\mathrm{R}\mathrm{M}1 \times \left(\mathrm{ARM}0/\mathrm{ARM}1\right) $$
$$ \mathrm{T}\mathrm{R}\mathrm{M}2* = \mathrm{T}\mathrm{R}\mathrm{M}2 \times \left(\mathrm{ARM}1/\mathrm{ARM}2\right) $$
The slope from the NRM-TRM1* diagram was used to calculate the archeointensity, while that from the TRM1-TRM2* diagram was to check the validity of the ARM correction. We adopted the following selection criteria, which are similar to those used in recent paleointensity studies with the Tsunakawa-Shaw method (e.g., Yamamoto et al. 2010; Mochizuki et al. 2013; Yamazaki and Yamamoto 2014).
  1. (1)

    A primary component is resolved from NRM by stepwise AF demagnetization.

     
  2. (2)

    A single linear segment is recognized in the NRM-TRM1* diagram within the coercivity range of the primary NRM component. The segment spans at least 30% of the total extrapolated NRM (f N ≥ 0.30; definition of the extrapolation is the same as in Coe et al. (1978)). The correlation coefficient of the segment is not smaller than 0.995 (r N > = 0.995).

     
  3. (3)

    A single linear segment (f T ≥ 0.30 and r T ≥ 0.995) is also recognized in the TRM1-TRM2* diagram. The slope of the segment is unity within experimental errors (1.05 ≥ slopeT ≥ 0.95) as proof of the validity of the ARM correction.

     

For approximate estimations of remanence anisotropies of the samples, ARMs were imparted on unheated sister specimens with two different directions and those after LTD were measured. One direction was approximately parallel to the NRM direction (ARMNRM direction), and the other direction was to the laboratory TRM direction (ARMTRM direction). Conditions of the impartments were same as those in the main experiment.

Results

Rock magnetic experiments

Sample-averaged ratios of B rc/B c and M rs/M s are listed in Table 1 and shown in Figure 4 on a Day plot (Day et al. 1977; Dunlop 2002). Data points in the Day plot are distributed between the single-domain to multi-domain (SD-MD) and SD to super-paramagnetic (SD-SP) mixing curves for magnetites by Dunlop (2002). The points originated from the floor surface samples (red triangles) tend to lie closer to the SD region than those from the −20-cm level samples (gray circles). This tendency is clearly recognized when we consider ground means of the former and latter samples (red and gray squares). It is thought that dominant magnetic carriers are SD and/or SP grains for the floor surface samples while contributions of MD grains seem to be relatively large for the −20-cm level samples.
Table 1

Results of the rock magnetic experiments and the Tsunakawa-Shaw paleointensity experiments

Sample

ARM0 0

N hys

B rc /B c

M rs /M s

LTD

Anisotropy

First heating

Second heating

F

ΔAIC

 

[10 -5 Am 2 /kg]

   

[%]

ratio

H c

Slope A1

Slope N

f N

r N

H c

Slope A2

Slope T

f T

r T

(μT)

 

Floor surface

1

247

2

1.564

0.4267

21.8

1.12

40-180

0.882

1.28

(0.166)

(0.982)

0-180

1.03

(1.05)

0.999

1.00

 

−1.66

2

343

2

2.730

0.2696

9.1

0.972

40-110

0.932

1.08

0.369

1.00

0-180

1.02

0.978

0.986

0.999

43.2

0.17

5

302

2

1.470

0.4252

24.7

1.05

20-180

0.976

1.16

0.570

0.999

0-180

1.00

1.05

1.01

1.00

46.4

5.26

8

274

4

1.581

0.3970

16.5

1.03

20-180

0.991

1.20

0.530

0.999

14-180

1.03

1.05

0.779

0.999

48.0

−0.17

9

171

2

1.702

0.4296

32.9

1.06

20-180

0.939

1.21

0.691

0.999

0-180

1.04

0.984

0.998

1.00

48.4

11.6

11

261

4

2.029

0.3420

14.0

0.980

20-180

0.972

1.24

0.672

0.998

0-180

0.969

1.04

1.01

0.999

49.6

16.3

12

142

4

1.683

0.4074

24.2

1.24

20-180

1.04

1.20

0.503

0.999

0-180

1.01

1.02

0.999

1.00

48.0

0.18

13

262

4

1.750

0.4001

28.5

1.10

45-180

0.925

0.994

(0.233)

0.998

0-180

1.00

1.05

0.993

1.00

 

11.9

 

250

8

1.814

0.3872

21.4

           

47.3

 
 

±66

 

±0.406

±0.0552

±7.9

           

±2.2

 

−20-cm level

15

38.2

2

2.153

0.3064

7.8

1.06

70-180

0.826

1.46

(0.206)

0.995

0-180

1.08

0.984

1.01

1.00

 

0.55

16

21.0

2

2.385

0.2372

4.0

0.986

20-120

1.01

0.790

0.743

0.996

0-180

1.08

0.999

0.977

0.998

31.6

−0.31

18

3.69

2

3.639

0.1344

20.5

0.941

20-180

1.03

0.909

0.623

(0.964)

0-180

0.939

1.01

0.914

0.968

 

−0.92

19

5.35

2

4.905

0.1164

7.5

0.958

20-180

1.00

0.863

0.547

(0.883)

0-180

0.934

0.985

0.970

0.986

 

7.79

 

17.1

4

3.271

0.1986

10.0

           

31.6

 
 

±16.1

 

±1.270

±0.0894

±7.2

             

ARM00, initial ARM0 intensity after LTD; Nhys, number of chips for the hysteresis measurements; Brc/Bc, Mrs/Ms, sample-averaged ratios of coercivity of remanence (Brc) to coercive force (Bc) and saturation remanent magnetization (Mrs) to saturation magnetization (Ms); LTD, LT demagnetized fraction of ARM0; anisotropy ratio, ratios of ARMTRM direction to ARMNRM direction before laboratory heating; Hc, the coercivity interval taken for the linear segments; slopeA1, slopeA2, slopes of ARM spectra for Hc in the ARM0-ARM1 and ARM1-ARM2 diagrams; slopeN, slopeT, slopes of the linear segments in the NRM-TRM1* and TRM1-TRM2* diagrams; fN, fT, NRM and TRM1 fractions of the linear NRM-TRM1* and TRM1-TRM2* segments; rN, rT, correlation coefficients of the linear NRM-TRM1* and TRM1-TRM2* segments; F, calculated paleointensity; ΔAIC, AIC difference between linear and quadratic fit (Yamamoto and Tsunakawa, 2005); Numbers in parentheses indicate out of the selection criteria; Numbers in italic are averaged values with their 1 σ for the sample groups.

Figure 4
Figure 4

Measured hysteresis parameters shown on a Day plot. Red diamonds (gray circles) indicate data points for samples from floor surface (−20-cm level). The red (gray) square represents the averaged parameter for samples from floor surface (−20-cm level) with their one standard deviation. Threshold values for single domain (SD), pseudo-single domain (PSD), and multi-domain (MD) regions are adopted from Dunlop (2002). Dotted curves are theoretical mixing curves for SD-MD and SD-SP (super paramagnetic) magnetite grains adapted also from Dunlop (2002).

Thermomagnetic curves show two Curie temperature phases at approximately 250°C and approximately 550°C in heating, and the former phase is disappeared in cooling (Figure 5). In spite of the disappearance, the curves are generally reversible. This suggests that thermal stability in laboratory heating, one of the key factors in absolute paleointensity experiments, is reasonably good. Some prominent characters in the curves are that (1) the curves from −20-cm level samples are obviously noisier than those from floor surface samples and that (2) the phase at approximately 250°C on heating is more prominent in the curves from −20-cm level samples. These characters seem to be originated from possible less formation of Ti-poor titanomagnetites due to the insufficient baking of the −20-cm level samples during firing of the reconstructed kiln. In actual, laboratory-imparted ARMs of the −20-cm level samples resulted in the intensities one order of magnitude smaller than those of the floor surface samples (Table 1).
Figure 5
Figure 5

Representative thermomagnetic curves. The curves are shown for (a) sample 5 from floor surface and (b) sample 16 from −20-cm level. Heating (cooling) curves are indicated in red (blue). Some characteristic behaviors that appeared in the heating curves below approximately 100°C are artifact due to the instrument.

Results of the ThD experiments are shown in Figure 6. They show that unblocking behaviors of IRMs are different between the samples 5 and 16 particularly for the temperature range above 200°C: major unblocking occurs at higher temperature in the sample 5 than in the sample 16. This is probably because of less formation of magnetic grains in the −20-cm level samples due to the insufficient baking as discussed in above. The results also exhibit that unblocking behaviors are similar between NRM and IRM for sample 5 (Figure 6a) while they are different for sample 16 (Figure 6b) as evidenced from NRM/IRM ratios: the ratio is generally constant at approximately 0.02 throughout the temperature range for the sample 5 (Figure 6a) whereas it shows a systematic increase at higher temperature for sample 16 (Figure 6b). This implies that NRM of sample 5 resulted in acquisition of full TRM during firing of the reconstructed kiln while that of sample 16 only in acquisition of partial TRM, assuming that IRM has a similar unblocking behavior with full TRM.
Figure 6
Figure 6

Thermal demagnetization results of NRM and IRM intensities. The curves are shown for (a) sample 5 from floor surface and (b) sample 16 from −20-cm level. Blue (red) curves indicate the demagnetization results for NRM (IRM). Black curves illustrate variations of NRM/IRM ratios.

Scanning electron microscope (SEM) observation

Representative BEIs are shown in Figure 7 with results of the EDS point analyses. In both the samples from floor surface (sample 5) and −20-cm level (sample 16), Fe-Ti oxide minerals are present. It is clearly recognized that the minerals in approximately 10 nm size are abundant in the floor surface sample (sample 5) while those in approximately 1 to 10 μm size are dispersed in the −20-cm level samples. These observations are consistent with the results from the hysteresis measurements and the thermomagnetic curve measurements.
Figure 7
Figure 7

SEM observation results. The results are shown for (a) sample 5 from floor surface and (b) sample 16 from −20-cm level. Left images are back-scattered electron images. Right diagrams are results of the EDS point analyses made on the points indicated by yellow stars in the left images.

Tsunakawa-Shaw paleointensity experiments

Six successful results were obtained from the floor surface samples by the selection criteria. The representative one is illustrated in Figure 8a. The resultant archeointensities range between 43.2 and 49.6 μT, giving an average of 47.3 μT with a standard deviation of 2.2 μT (Table 1). This is fairly consistent with the in situ geomagnetic field at the time of the reconstruction (46.4 μT). For the successful results, linear portions in the NRM-TRM1* diagrams are derived from the NRM fractions more than 50% of the total extrapolated NRMs (fN ≥ 0.5) except one (sample 2). Degree of alterations in first laboratory heating is suggested to be small, namely at most approximately 7%, based on the slopes estimated from the ARM0-ARM1 diagrams (slopeA1, 0.932 to 1.04, Table 1). Thus, the successful results seem to be of good quality.
Figure 8
Figure 8

Representative successful results of the Tsunakawa-Shaw archeointensity (paleointensity) experiments. The results are shown for (a) sample 5 from floor surface and (b) sample 16 from −20-cm level. The left-hand (right-hand) side diagrams indicate results from the first (second) laboratory heating. Closed symbols correspond to coercivity intervals for the linear segments. Orthogonal vector-end-point diagrams for the AF demagnetization on NRM are also displayed as insets, where closed (open) symbols indicate projections onto horizontal (vertical) planes. Units are in 10−5Am2/kg.

Only one successful result was obtained from the −20-cm level samples by the selection criteria. It yielded an archeointensity of 31.6 μT (Figure 8b and Table 1), which is inconsistent with the in situ geomagnetic field of 46.4 μT. In this result, the archeointensity is estimated from 74% of the total extrapolated NRMs (f N = 0.743) and degree of alteration in first laboratory heating is suggested to be negligible (slopeA1, = 1.01). Quality of this result seems to be also good in spite of the inconsistency.

On average, LTD demagnetized 21.4% and 10.0% of ARM0s for the floor surface and −20-cm level samples, respectively (Table 1). Because LTD treatment is known to be effective technique for selective removal of MD-like remanences in Ti-poor titanomagnetite (Ozima et al. 1964; Dunlop and Ozdemir 2007), it is considered that these samples certainly had such remanences but they are more or less removed.

About the remanence anisotropies of the samples, ratios of ARMTRM direction to ARMNRM direction resulted in 0.941 to 1.12 except for the sample 12 which showed the ratio as 1.24 (Table 1). These values seem to be typical of baked clays, for example, Kovacheva et al. (2009) reported that baked clay and soils collected from archeological sites in France and Bulgaria resulted in TRM anisotropy ratios less than 1.20 for about 80% of the collection.

Discussion

Application of the Tsunakawa-Shaw method yielded the averaged archeointensity of 47.3 μT with a standard deviation of 2.2 μT (N = 6) from the floor surface samples and the archeointensity of 31.6 μT (N = 1) from the −20-cm level samples (Figure 9 and Table 1). The former result is fairly consistent with the in situ geomagnetic field at the time of the reconstruction (46.4 μT) while the latter one is significantly lower than the in situ field. This is probably because the floor surface samples acquired full TRMs as their NRMs during the firing of the reconstructed kiln whereas the −20 cm level samples only acquired partial TRMs.
Figure 9
Figure 9

Summary of the archeointensity results obtained by the Tsunakawa-Shaw method.

From the in situ temperature record during the firing (Figure 2), it is clear that the floor surface samples experienced high temperature of approximately 1,000°C while the −20-cm level samples were only exposed at low temperature, at most approximately 350°C. It is considered that the former samples were baked well above the Curie temperature of magnetite (approximately 580°C) resulting in acquisition of full TRMs, whereas the latter ones were below that temperature leading to acquisition of partial TRMs. The acquisition of full and partial TRMs for the former and latter samples are respectively implied from the results of the ThD experiments (Figure 6). In the Tsunakawa-Shaw experiment, we imparted full TRMs to the samples in laboratory and basically compared them with their NRMs. For the floor surface samples, NRMs are probably full TRMs and the comparison seem to result in the accurate archeointensities. In contrast, for the −20-cm level samples, NRMs are probably weak partial TRMs and thus the comparison would probably result in the weak paleointensity.

Difference in the ‘baking’ temperatures between the floor surface samples and the −20-cm level samples would probably also cause the differences in the rock magnetic characters. In the former samples, there are much more SD and/or SP titanomagnetite grains compared with the latter samples, and the former samples have high remanence intensities (e.g., ARM0s). From the view of the rock magnetic properties, the floor surface samples seem to be much more preferable for high-fidelity archeointensity researches.

Importance of the anisotropy correction has been emphasized for accurate archeointensity determinations (e.g., Aitken et al. 1981). The Tsunakawa-Shaw method employs a built-in anisotropy correction using ARMs: ARM0, ARM1, and ARM2 are imparted with their directions approximately parallel to the NRM, TRM1, and TRM2 directions, respectively, and measured along with the stepwise AF demagnetizations; ratios of ARM0/ARM1 and ARM1/ARM2 are used to correct TRM1 and TRM2 into TRM1* and TRM2*, respectively. The floor surface samples yielded the successful archeointensity results fairy consistent with the in situ geomagnetic field, and thus the built-in correction seemed to work well. The degree of the correction is suggested to be 6% to 12% except for sample 12 considering the ratios of ARMTRM direction to ARMNRM direction (Table 1).

Necessity of the cooling rate correction has also been emphasized in many studies because the difference in that rate could result in biased archeointensity estimates (e.g., Mitra et al. 2013; Cai et al. 2014). For example, Usui (2013) reported that the cooling rate effect resulted in a 37% to 46% overestimated paleointensity for an oceanic gabbro, although it is not the case of the archeointensities. In the present study, there is large difference in the cooling rates between the kiln NRMs (approximately 24 h) and the laboratory TRMs (approximately 2 h). However, without such corrections, we obtained the archeointensity results fairy consistent with the in situ geomagnetic field from the floor surface samples. This suggests that the cooling rate correction is dispensable for the Tsunakawa-Shaw method, at least for a baked clay. It is noted that the main magnetic carriers of the floor surface samples might be Ti-poor titanomagnetites in fine PSD sizes, rather than in approximately 10 nm size: Yu (2011) experimentally demonstrated that the cooling rate effect was negligible for a 1.06 μm PSD magnetite.

Conclusions

Application of the Tsunakawa-Shaw method to the baked clay samples taken from a reconstructed kiln shows that the samples from floor surface provide the accurate archeointensity results. They are obtained with a built-in anisotropy correction using ARM and without any cooling rate corrections. A suite of the rock magnetic experiments and the SEM observations elucidate that dominant magnetic carriers of the floor surface samples are Ti-poor titanomagnetite grains in approximately 10 nm size, with SD and/or SP states. For archeointensity researches, baked clay samples from a kiln floor are considered to be ideal materials.

Declarations

Acknowledgements

We thank Tadashi Nakajima and Katsumi Yaskawa for the reconstruction experiment, Kimio Hirooka and Hiroshi Nakamura for long-term storage of the samples, and Yukako Nabeshima for help with the measurements. Constructive comments by Yongjae Yu and Hidetoshi Shibuya improved the manuscript. This study was partly supported by JSPS KAKENHI Grant Numbers 21500991, 23740340, and 25247073 and by the Kochi University Research Project ‘Research Center for Global Environmental Change by Earth Drilling Sciences.’

Authors’ Affiliations

(1)
Center for Advanced Marine Core Research, Kochi University, B200 Monobe, Nankoku Kochi, 783-8502, Japan
(2)
Okayama University of Science, 1-1 Ridaicho Kita Ward, Okayama 700-0005, Japan
(3)
Natsuhara Giken Co. Ltd., 1-13-24 Niitaka, Yodogawa Osaka, 532-0033, Japan

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© Yamamoto et al.; licensee Springer. 2015

This is an Open Access article distributed under the terms of the Creative Commons Attribution License (http://creativecommons.org/licenses/by/4.0), which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly credited.

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