Copyright 1976. All rights reserved

THE URANIUM-SERIES METHODS OF AGE DETERMINATION1

Teh-Lung Ku Department of Geological Sciences, University of Southern California, Los Angeles, California 90007

INTRODUCTION

:-:10061

Of the many nuclear clocks commonly used in geology, those based on the radioactive daughter products of uranium and thorium are perhaps the least known. Extensive applications of this collectively termed uranium-series (disequilibrium) methods are relatively recent, and much developmental work pertaining to their strengths and weaknesses are still underway. Nevertheless, the past decade has seen a steady increase of literature on the subject. Such a trend is almost certain to continue, particularly in view of enhanced interest in deciphering the timing of many profound changes in the physical and biological nature of the Earth that are embodied in the Pleistocene record.

Noideal dating technique applicable to the entire Pleistocene epoch is yet available. For instance, radiocarbon ages of more than 40,000 yr are normally considered unreliable and the dating of the Quaternary with U-He and K-Ar is limited by the scarcity of suitable preserved and datable deposits (Broecker \965). In principle, the various uranium-series methods cover ages ranging from several years to more than a million years and are applicable to a variety of materials. Thus far these methods have contributed to several areas of study, in particular to establishing the chronology of the late Pleistocene climatic fluctuations. They are also potentially valuable to the fields of anthropology and archaeology.

The three naturally occurring uranium and thorium decay series each include nuclides of different nuclear and chemical properties, with a wide range of decay half-lives (Figure 1). These nuclides can be separated through the processes of weathering, transportation, and deposition. Once separated, they tend to restore radioactive equilibria with one another, with rates dictated by their respective decay constants. Such rather unique relationships render those nuclides useful as tracers

1 Contribution No. 355 from the Department of Geological Sdence�, Univer�ity of Southern California.

347

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348 KU

U-238 SERIES Np U U·Z36 U-234

4.49><101 .48.1�

Po 1 Fb-Z34 ] 1.18m

Th rn-Z5-4 tn.-230 24.ld J.5Z-loY

] ·f·

Ac Ra R.-z2I

1622y

Fr 1 Rn Rn·22J

3.65d

At 1 Po Po·ZIB Po-214 MIO

3-05m 16><10"� 138d

Bi 1 Bi-i!14 1 Bi�O 1 !9:'7m SOd

Pb PI>-214 Pb-Z/O Pb·� 26.8m tZ.2y S1dble -

TI

Th-232 SERIES U-235 SERIES i

U-Z35 ! 11�" � 1

1 Fb·23 I I

�""Id'y \ 1h;!3 1n>-i!Z8 h-231

1. 1h-22

1.39"� 1.901 ZS.6h 18.6d

0: ...

AcZZS 1 At-Z2 J ! 6./lh 22.0,/ Ra-ZZE RQ·Zllo �·Z� 6.1y �.64d IUd

1 1 fR..-i!21 /Rn-e19

54.55 192<

1 1 MI6 MIZ MIS 0.165 65% .OIlI6� I.g"oi

1 8i-ZIZ 1 1 Bj·2JJ 60.5171 i.16m

Pb-Z/2

� Pb-i!OI iPb-2JJ 1 1'1>-20 �h stobIe. 36.1", St.bl. .-

TI-Zd, 3·'m 4:'T9m

Figure 1 The three naturally occurring radioactive decay series. Nuclides framed with heavy lines are those of geochronological interest discussed in this paper.

and/or time-measuring tools for the study of a number of oceanographic, hydrologic, meteorologic, and geologic problems. In this review,. we confine our discussion mostly to their use in age determination of geologic materials.

The uranium-series methods encompass a spectrum of techniques involving many isotopes (Figure I; Goldberg & Bruland 1974). However, they can be divided into two categories: (a) methods based on decay of unsupported intermediate members of the series, and (b) methods based on accumulation of decay products of uranium. Either of these situations may be encountered in the dating of igneous rocks. The order of presentation will come under these groupings with emphasis on the applica­tion of the isotope 23°Th (ionium). Such an emphasis is both inevitable and justified in that 23<rrh dating of deep-sea sediments, coral, and mollusks constitutes the bulk of the data in this field of study; it bears on principles, assumptions, and limitations associated with the use of other uranium-series isotopes.

NATURE OF RADIOACTIVE DISEQUILIBRIUM

Because of the relatively short half-lives of the intermediate members of the decay series (Figure 1), normally secular equilibrium among them should have long since been est�blished on the Earth. This is, however, not the case. Take the marine

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URANIUM-SERIES METHODS 349

hydrosphere as an example. Activities of the 238U series nuclides in sea water exhibit the following relationships: 234U2 = 1 .l4e38U), 230Th < O.Ole34U), 226Ra > 30e30Th), 210Pb < 226Ra (except in surface ocean), and so forth. The primary cause for these disequilibria is difference in solubility of the isotopes involved.

During weathering, uranium is oxidized to form UO� + which is quite soluble because anionic complexes, such as U02(C03)�-' are formed (McKelvey et al 1955, Starik & Kolyadin 1 957). Because of the 11.- and f3-decays accompanying the transformation of 238U to 234U, it is more likely that 234U rather than 238U will occupy metastable lattice positions induced by IX-recoil dislocation (Cherdyntsev et al 1 96 1 , Dooley et al 1 966), or that 234U will be in the soluble, +6 valence state (Rosholt et al 1 963, 1 966; Dooley et al 1 966). Either leads to preferential leaching of 234U over 238U from weathered minerals (Cherdyntsev 1955), and thus to 234U;Z38U ratios of larger than unity in natural solutions, including seawater. Kigoshi ( 197 1 ) observed the dissolution of IJ.-recoil 234Th into the solution in contact with mineral grains. Hence, a certain fraction of ' the 234U atoms could have originally been produced in the interstitial fluid of a sediment.

As the oceanic 234U decays to 23°Th, the latter, because of the high ionic potential of the Th4+ ion, is readily adsorbed or precipitated as a hydrolysate. Thus 230Th is greatly depleted in the water column (Koczy et al 1 957) and enriched in the surface bottom deposits (Pettersson 1 937, Isaac & Picciotto 1 953). The excess 226Ra over 230Th in seawater is a result of the diffusion of 226Ra across the sediment-water interface, which is generated by the decay of BOTh in sediments (Kroll 1953; Koczy 1954, 1958). As 226Ra in the ocean further decays to 210Pb, fractionation again occurs. The residence time of 210Pb is considerably shorter than that of 226Ra, so that in most parts of the ocean, 210Pb is depleted with respect to 126Ra (Goldberg 1 963, Craig et al 1 973, Bruland et a1 1 974b) and enriched in surface sediments (Koide et al 1 972).

The kind of fractionation pattern outlined above is also seen in the decay series of 235U and 232Th. The 235U_231 Pa relationship resembles that of 234U_230Th, in that 23! Pa, being insoluble, is hence impoverished relative to 235U in seawater and enriched in sediments (Sackett 1960). In the 232Th series, the diffusional input of 228Ra from sediments results in the excess of 228Ra and 228Th over their progenitor 232Th in the sea (Koczy et a1 1 957, Moore & Sackett 1 964, Moore 1969).

In summary, because of diversities in the chemical and nuclear properties, dis­equilibria among members of the decay series exist. In seawater and other surface solutions, the activities of those isotopes of geochronological interest generally decrease in the following order:

234U > 238U > 226Ra > 210Pb > 23°Th 235U> 231Pa 228Ra > 228Th > 232Th

2 Hereafter, symbols for the isotopic species, when used in equations or figures or when expressed as ratios, all denote activities, i.e. N·). (N is the number of atoms of the species and Ie its decay constant).

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350 KU

Understandably, fractionations such as these will have made their imprints on the associated sediments and other solids precipitated from the solutions. Restoration to radioactive equilibrium of the isotopes in the solid phase is the basis of various geochronological yardsticks discussed below. Several sources that provide further general references and background information on the subject include Koczy (1963),

Broecker (1965), Wetherill & Tilton (1967), Komura & Sakanoue (1967), Bernat (1969), Szabo (1969), Cherdyntsev (1971), and Goldberg & Bruland (1974).

METHODS BASED ON DECAY OF UNSUPPORTED INTERMEDIATE DAUGHTER NUCLIDES

As mentioned, natural fractionations taking place in the hydrological cycle lead to the preferential precipitation of certain insoluble daughter products in the decay series over their more soluble parents. In bottom deposits, these daughter nuclides could therefore be largely unsupported (or in excess) and will diminish with time through decay. If the original amount of excess daughter nuclides in a freshly

deposited sediment is known, the extent to which this excess has been reduced gives a measure of the time since the settling of that sediment. In this way, the age or accumulation rate of a deposit is determined. Mathematically (the parent nuclides, having much longer half-lives than their respective daughters in excess, can be treated as being stable in the formulation),

c = Co exp(-),t), or t = -(I/A) ln(c/co), (I) where A is the decay constant of the unsupported radiogenic daughter, Co is the initial excess, and c is the excess found t years later. The crucial problem is the assignment of Co.

Dating Deep-Sea Deposits

Unsupported 230Th (tl/2 = 75,200 years) and 231Pa (tl/2 = 34,300 years) have been used for dating deep-sea sediments and ferromanganese nodules. The precipitation of the two isotopes as they are formed from the oceanic uranium is essentially quantitative, with less than 0.05% of the 230Th and less than 0.2�;;' of the 231 Pa remaining in solution (Moore & Sackett 1964). Their concentrations in the deposits, which depend to first order on the accumulation rate of the deposits, and measure­ment techniques will determine the applicable age range. Currently, sediments of up to 350,000 years old are datable by 230Th, and up to 150,000 years old by 231Pa; for the slowly accreted Mn nodules, the corresponding ranges are longer.

BOTh METHOD Attempts to utilize 23°Th for sediment dating began with Piggot & Urry (1939, 1942), who measured 226Ra as an index 0[230Th. They expressed c

and Co of Equation 1 in concentration units (i.e. amount of 23°Th per gram of total sediment) and assumed Co to be constant.

Let t be the age of the sediment layer at depth x, then t = xis, where 5 is the average sedimentation rate (in centimetres per unit time) down to depth x. From Equation 1:

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URANIUM-SERIES METHODS 351

. In C = - ().js)x + In Co, (2)

where A. in the present case is the decay constant of 23oTh. When In c is plotted against x, as customarily done, a straight-line relationship would point to the constancy of both Co and s; it not only serves to validate the constant Co assumption, but also enables the sedimentatiun rate, s, to be assessed from the slope of the straigh t line.

Such an approach has been basically adopted by many of the later investigations on sediment dating. Interestingly, major improvement made on the original work of Piggot & Urry seems to have been only in the analytical realm. The migratory behavior of 226Ra in sediments, first noted by Kroll (1953, 1954), has prompted the direct measurement of 23°Th, which was not feasible before World War II . Further­more, the excess 23°Th used in Equation 2 is obtained by subtracting the measured activity of 234U from that of 23°Th (i.e. 23°Thex = 230Th_234U). This correction arises from the consideration that uranium in a typical pelagic sediment is mostly associated with detrital cia ys (Ku 1965) in which a 234 U-eq ui valen t amoun t of detri tal Z3°Th (U-supported 23°Th) is present. The correction becomes important in deeper strata where the quantity of excess BOTh is reduced. Measurement precision of - 2% for 230Thex using ()(-particie spectrometry can be achieved; however, analytical uncertainties as they now stand may often not be the limiting factor that affects the precision of age determination of sediments.

Shown in Figure 2a is an Equation 2 plot for a Caribbean core V12-122. An average sedimentation rate of 2.52 em 10-3 yr- J over the length of the core is obtained from the slope of the regression line best fitting the data points. The linear regression coefficient (hence the rate derived therefrom) has a standard error of ±4.1%, comparable to the analytical errors as shown. Within this error limit, constancy of Co and s is indicated, implying uniformity in the deposition of both 23°Th and total sediments over the past 300,000 years or so. V12-122 is one of the better cores in terms of showing good linearity in plots like Figure 2. Cores exhibiting larger scattering of data (therefore giving larger errors in rate estimates) than V12·122 are not uncommon, especially those cores with varied lithology.

The nonlinearity plots could be explained if the initial concentration of HOTh varied

' with time. And the suspected culprit is change in the bulk sediment settling

rate, because the very long residence time of uranium (105-106 yr) combined with the very short residence time of 230Th (�100 yr) favors the concept of a constant HOTh precipitation over the datable interval. To cope with this problem, two major modifications of the method have been attempted, They are the 230ThF32Th and the 231Paj230Th methods.

230Th/232Th METHOD Picciotto & Wilgain (1954) suggested using the ratio 23°Th/ 232Th instead of 23°Th per total sediment for c and Co in Equation 2, reasoning that, because of the chemical identity of the two thorium isotopes, 232Th should provide an estimate of the amount of 23°Th initially present in a sediment. In other words, despite variation in the bulk rate of sedimentation, the ratio of the precipi­tated 230Thj232Th in the freshly deposited sediment remains constant through time at a locality. Several investigators have followed the suggestion and applied it (with

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352 KV

5

� E a. "C

";; .5 .. .&:

Ii N

.1

.05

� E .I a. :s �.05

a.. ;;; N

.010

I • I

/ 2.52 t.11 cm/103y

200 400

,,/' 2,47!.14

em 1103 y

100

(a) V12-122

"

600 800 1000

(b)

�

200 DEPTH IN CORE (em)

1200

300

Figure 2 Equation 2 plots for core V 1 2- 1 22 (17°00'N, 74°24'W). The parameter c is expressed as (a) excess 230Th concentrations, and (b) excess 231Pa concentrations. The sedimentation rates are obtained from slopes of the best-fitting straight lines for the data points; in this case, they are from the linear regression coefficients of the In c- x correlation matrix. Analytical data are from Ku (1966) and Broecker & van Donk (1970). Broecker & van Donk ( 1 970) have cited an average rate of 2.35 ± 0.10 cmjl 03 yr for the core.

slight operational variations) to cores from many parts of the ocean. They include, among others, Baranov & Kuzimina3 ( 1958), Goldberg and his co-workers (Goldberg & Koide 1958, 1962, 1963; Goldberg et a11964; Goldberg & Griffin 1964), Almodovar (1960), and Miyake & Sugimura ( 1961) . However, these applications have invited criticisms (Rosholt et al 1961; Koczy 1961, 1 963; Sarma 1964; Sackett 1964; Broecker 1965). Objections stem primarily from the argument that, although they are chemically similar, BOTh and 232Th (or, for that matter, Fe203) vastly differ geo­chemically in their marine cycles. The former is produced in the sea, whereas the latter is mostly an integral part of the continental detritus carried to the sea floor.

The critics' concern is justified. Most 232Th in sediments is detrital in origin. Thorium content of pelagic biogenous (calcareous) components is low (Koczy 1949, Holmes et al 1968); most of the 232Th resides in the nonbiogenous (clay)

3 These authors used ratios of excess 230Th to MnO and Fe203, as they noted that 232Th co-varies with MnO and Fe203 in the cores examined.

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URANIUM"SERIES METHODS 353

components. Thorium content of these clays approximates those of average igneous rocks and shales and does not show any correlative trend with sedimentation rate, water depth, location of occurrence, etc (Ku 1966). Even with the acid-leach technique (Goldberg & Koide 1962), the major fraction of the 232Th analyzed in the 230Thj232Th dating is detrital, not authigenic as intended by the method (Goldberg & Griffin 1964).

The question remains as to the validity of the 230Thj232Th-derived results. Obviously, in cores with nearly constant B2Th distribution, there should be little difference between 230Th expressed as 230Thj232Th ratios and as concentrations. Both are subject to the same uncertainties in case scatter of data in the In c vs depth plot occurs. The situation is exemplified by Figure 3 for core AII42- 13 (Ku et al 1972). In essence, the advantage claimed by the 230Thj232Th method over the Piggot-Urry approach is nullified. For cores of varying 232Th content, however, depth plots of 230Thj232Th and 23°Th per total sediment will be different. For the following reasons the difference can be significantly amplified in high CaC03 cores.

Although knowledge of the precise removal mechanism of 23°Th in the ocean is lacking, there is evidence bearing on the 23°Th precipitation as being facilitated by settling of particulate material of both biogenic and detrital nature. This is in contrast with the detrital affiliation of 232Th. The implication is that depth plots

. of 23°Thj232Th should resemble those of 23°Th per noncarbonate (i.e. 230Th concentration on a carbonate-frec basis), as shown in Figure 3b. In cores with varying but overall high carbonate content, percentagewise, changes in the non­carbonate (hence 232Th) may become much larger than the corresponding changes in carbonate, leading to depth plots of 230Thj232Th that drastically differ from those plots if 230Th per total sediment is used. A case in point is the data on another Mid-Atlantic Ridge core ZEP-15 (Goldberg et al 1 964), located near AII42-13. [Analogous situations can be found in many other cores from the Ridge area, e.g. Goldberg & Griffin ( 1964) and Ku et al (1972).] Carbonate contents in this core vary from 72% to 84%; hence noncarbonates fluctuate between 1 6% and 28%-a variation almost spanning a factor of two. Figure 4 shows two ways of plotting (not shown is the plot using 23°Th per noncarbonate, which would yield patterns close to those of 230ThF32Th, as has been noted). Although in both plots the mean slope of the linear fit for the da ta points are similar -thus gi ving a mean sedimen ta tion rate of about 4 mm 1 0-3 yr-1-details in the scatter are different, especially for the upper portion of the core.

ZEP-15 is one of th� Mid-Atlantic Ridge cores whose 23°Thj232Th chronology has shown serious discrepancies with the 14C data; ages based on 230Thj232Th can be as much as five to ten times too great (Goldberg & Griffin 1964; Goldberg et al 1964; Broecker 1 965). The discrepancies can be attributed chiefly to the manner in which the BOTh data were interpreted (Ku et a1 1 968, 1 972), although viewpoints have differed (Goldberg 1968). In Figure 4a, the 1 .3 mm 10-3 yr- 1 rate shown is based on the assumption of a constant initial 230Thj232Th. In the light of the above discussions, this is clearly unwarranted. The steep slope for the top 11.5 em is mainly induced by a downward decrease of .carbonate content (hence increase of 232Th) in this interval, rather than by 23°Th decay. It is therefore no surprise that the

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354 KU

age of 88,000 years assigned at 1 1.5 cm is too old compared to the 14C age of 17,000 years (Broecker 1965). Figure 4b presems the depth plot of 230Th concentration for ZEP-15. A rGlte of sedimentation of 4.3 mm 10-3 yr-1 for the top 65 cm is estimated from the best-fitting line, which can be compared with the- 5 mm 10-3 yr-l rate for the 0-150 cm interval of core AII42-13 (Figure 3). Both are average rates with some ± 15% to ± 25% uncertainties. They do not specify short-term rate variations within the averaged intervals, because in doing so one has to assume

c; o ::::::: E a. �

')( cu o

0.... � C\I a z «

-)( CD

..c: t­o rt> C\I

(0) ( b) 100,.----,----,

5.0

10

QI

.05

o

I \ / < \ \ \ \

I

1-AII42-13

100

CD � 0:: .c <t f- U

o Z � �

" o

0.5

+

/ QI a 5.0mm/10

w ::> ...J <{ > 0.01

200

...J <{ i= .005 z z o i= u <{ a:: lL.

A1142-13

.001 �_---l.. __ ....1 o 100 200

DEPTH IN CORE (em) Figure 3 Equation 2 plots for core AII42-13 (19°40'N, 42°44'W) : (a) c is expressed as excess 230Th (solid bars) and excess 231 Pa (unfilled diamonds) concentrations. Average sedimentation rates derived from the best-fitting lines for both BOTh and 231 Pa agree. (b) c is expressed as z30Th.xlz3zTh and as z30Th •• per non carbonate (for comparison, the data are normalized against the measured ratios in the uppermost layers). Because carbonate content, and therefore 232Th, in this core is relatively uniform, (a) and (b) plots show similar results (Ku et al 1 972).

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URANIUM-SERIES METHODS 355 a rigid constant Co that both the Piggot-Urry and the Picciotto-Wilgain approaches fail to provide.

Briefly, the function of 230Thj232Th is similar to that of 23°Th per noncarbonate used by Ku & Broecker (1966) and Scott et al (1972). Both methods fail to improve the 230Th per total sediment approach. In fact, they may be more vulnerable to influence by carbonate fluctuations. With this in mind and with cautious data interpretation, the 230Th/2J2Th·-derived results should be usable. The technique offers some analytical convenience in that only ratios of the thorium isotopes are measured. In recent years, nondestructive y-ray techniques have been developed to measure 230Th and 232Th by way of simultaneous analyses of 214Bi and 208Tl (Osmond & Pollard 1967, Yokoyama et a11968, Bhandari et aI1971). They provide rapid, albeit crude, means of surveying oceanic sdimentation rates.

231 Pa/BOTh METHOD The idea of using 231 Pa in conjunction with 23°Th was conceived independently by Sackett (1960) and Rosholt et al (1961). Both nuclides are removed from seawater in a time short compared to their radioactive half-lives.

The relative abundance of their progenitors, 238U, 235U, and 234U, in the ocean has been rather constant (Hamer & Robbins 1960, Thurber 1962), and river con tributions of unsupported 231 Pa and 23°Th are negligible (Scott 1968). Therefore,

(a) (b) 100 100 r--------------------�

50 50 )3mm/103y

.: 3/mm1dy

J- 10 � E r<>

� 88,OOOy Do

� .c:

J- 5 r<> C\I

.: 5 �

0 ZEPI5 r<>

C\I ZEPI5

I 0 20 40 60 I 0 20 40 60 DEPTH I N CORE (em)

Figure 4 Similar comparison as made in Figure 3 for core ZEP-J5 (21006'N, 44°57'W). Here, because of the nonuniform carbonate disti-ibution in the core, the two ways of expressing c in Equation 2 give quite different results. Shown in (a) are rates interpreted

by Goldberg et al (1964) assuming a constant initial 230Th/232Th. An alternative and (in the author's opinion) more correct way of deriving the ages is through the plot and interpretation of (b).

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356 KU

the 231 Pa/23oTh ratio added to the sediment should be fixed at a value close to their production ratio, i.e. 1/11 or 0.091, if no fractionation occurs during precipita­tion of the two species. The age (t) of a sediment with a measured ratio e31PaeJ 230Thex), is then:

(3) where ;'0 and 1'1 are decay constants of 23°Th and 231 Pa, respectively, and e31 Paex/230Thex)0, the ratio of excess 231 Pa to excess 23°Th in newly deposited sediment, assumes the theoretical value 0.091. In practice, 23IPaex = 23 1Pa _ 235U, and BOThex = 230Th _ 234U.

The e31 PaeJ230Thex), ratio in Equation 3 is a function of t only; therefore it is independent of changing oceanic conditions such as fluctuations in bulk sedimenta­tion rate and uranium content of seawater and should decrease with a half-life of about 62,000 years. Depending upon the detectability of the residual excess 231 Pa, this so-called 231 Pa/23°Th method is usually applicable over the last 150,000 years.

The first test of the method would be to see if indeed (231 Paex/23oThex)o is equal to 0.091. This appears to he borne out by some of the early measurements (Sackett 1960; Rosholt et al 1961, 1962). In three cores from the Caribbean Sea, Rosholt et al

(1961, 1962) found a set of dates4 that are consistent with stratigraphic correlation and with the 14C ages in the upper portion of the cores, within the errors of ± (5-20)%. However, subsequent studies have revealed an alarming number of cores showing surface 231 PaeJ23�hex ratios that are much too low (Sackett 1964; Ku 1965, 1966; Ku et al 1972). As an extreme case, surface layer of core AII42-13

(Figure 3a) shows this ratio being as low as in the vicinity of 0.Q1, which according to Equation 3 would have an apparent age of over 150,000 years! The lbw ratios cannot be explained by suggestions (Rosholt et al 1 96 1 , Sackett 1964) such as missing core tops, contamination by reworked sediment, or preferential upward migration of BOTh in the core, as discussed by Ku (1966).

On examining the integrated amounts of unsupported 231 Pa (t231 Paex) and unsupported 230Th (L230Thex) in cores from various parts of the ocean (Ku 1966,

Ku et aI1972), it is evident that the ratio L231 PaeJL230Thex in sediments is less than the 235U;Z34U ratio of 1/25 in sea water. This inequality could be attributable to a deficiency of 231 Pa (Scott 1968, Turekian & Chan 1971 , Ku et aI1 972) or to a surplus of 230Th (Ku 1966, Ku & Broecker 1967a) in sediments with respect to their oceanic supplies from the 235U and 234U parents. On the other hand, the ratio L231PaeJ L23°Thex in deep-sea manganese nodules has been found to be markedly higher than the seawater 235U/2340 ratio (Sackett 1966, Ku & Broecker 1969). Clearly fractionation between 231 Pa and 23°Th must have taken place during their precipita­tion from the sea.

This unexpected finding negates the use of Equation 3 for age determination as orginally proposed for the 231Paj230Th method. However, concentrations of 230Th and 131 Pa when plotted separately according to Equation 2 often give rates consistent

4 The 231PaF30Th dates were calculated without considering the 14% excess 234U over 238U, because this phenomenon was not known at that time.

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URANIUM-SERIES METHODS 357

with each other, within errors, as illustrated in Figures 2 and 3a. It may imply that the initial ratio of the two isotopes at a given depositional site have remained sufficiently constant, even though it shows spatial variations. If so, the 231 Pa/23°Th ratios can be used either via the Equation 2 plot, thus obtaining average sedimentation rates (Sackett 1964, Ku & Broecker 1967a, Broecker & Ku 1969), or via Equation 3 by substituting the measured 231 PaeP30Thex in surface sediments for the theoretical value of 0.091. The first approach is preferred because strict constancy for the initial 231 PaeP30Thex ratios cannot be assured. It should be pointed out that ages obtained from the use of the ratio 231 Pa/BoTh are intrinsically more vulnerable to such errors as introduced by sediment mixing (Sarma 1964), analytical blanks (Broecker & van Donk 1970), uranium corrections (Broecker & Ku 1969), and un­certainties in the decay coflstant of 231 Pa or 230Th than from the use of either isotope alone.

231 Pa METHO D Similar to the Piggot-Urry method for 23°Th, the decrease of unsupported 231 Pa with depth in sediment cores and manganese nodules have been used to derive average accumulation rates over the last 150,000 years (Sarma 1964, Ku 1965, Ku & Broecker 1967b). The technique has proven useful as a complement to the BOTh method, though both are subject to the same limitations as discussed. Figures 2 and 3a illustrate the point.

Sackett (1965) used a different approach in treating the 231 Pa data. His assumption is that the deposition rate of 231 Pa onto a given area of ocean bottom remains constant. If the total amount of excess 231 Pa in the core and the amount of excess 231 Pa below a gi ven level in the core are known, the age at that level can be calculated by a formula similar in form to Equation 1 :

(4)

where )'1

is the decay constant of 231Pa, n is the excess 231Pa below the level with age C, and nl is the total excess 231 Pa in the core. In practice, the core is divided into contiguous, uniform segments; the age at the divisions are to be determined. Each segment is measured of its excess 231 Pa. The deepest segment measured should con tain no excess 231 Pa. Although hinging on the constancy of 231 Pa deposition, ages obtained by this approach are independent of variations in the bulk sedimenta­tion rate. Sackett (1965) has shown results in reasonable agreement with the 14C ages obtained on four cores.

The same approach should be applicable to 230Th. Although Broecker (1965) cited three 23°Th ages by this way and Schornick (1972) attempted the approach on several manganese nodules, the quality of the data base these workers used does not permit a rigorous evaluation. Considering that 230Th can be measured more precisely than 231Pa and that constant 23°Th deposition is indicated at least in some cores, a systematic study of the method using 230Th is warranted.

SYNOPSIS OF DATING DEEP-SEA DEPOSITS The bulk of the data has certainly established the first-order logarithmic decreases of both 230Th and 231 Pa in bottom deposits, strengthening the concept that particIe-by-particIe sedimentation prevails

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358 K U

in the deep sea. Mean sedimentation rates can be determined from the slope of the line best fitting the data points in the Equation 2 plot, using either concentrations of 230Th or 231 Pa, or ratios such as 230Th/232Th and 231 Pa/23°Th. Within error limits of the best linear fits, rates estimated in this manner agree with those derived from other dating tools such as 14C, K-Ar, lOBe, and paleomagnetic reversals [for sediments, see e.g. Ku et al (1968), Dymond (1969), Amin (1970); for manganese nodules, see Ku (1976)]. The error limits can be ±4% or better for very uniformly deposited sediments, but are in general about ± 20%. Short-term sedimentation rate fluctuations (on a time scale of tens of thousands of years or less) are not resolvable by the ratio methods, as had been hoped. Perhaps future investigations into the constant flux of 23°Th (as envisaged by Sackett for 231Pa) may shed some light on this aspect.

Studies of elemental flux and budget in the hydrosphere require knowledges of deep ocean rate processes. Such know ledges are made more accessible by the dating tools described. Sharpening of the tools for greater precision is not crucial at present for the geochemical studies, since the general ± 20% error is more than outweighed by uncertainties in other parameters, such as sediment and nodule bulk density. To fix the chronology of climate over the past several hundred thousand years recorded in deep-sea cores, further improvement over data such as those from core V12-122 would be desirable, as indicated in discussions in Broecker & van Dank (1970), Broecker & Ku (1969), and Emiliani & Rona (1969), for example. It is a challenging task. However, as oxygen isotopic ratios in marine foraminifera have assumed new value as indices of global ice volume and stratigraphic correlation (Shackleton & Opdyke 1973), the task may be tackled by accurate dating of only a few "ideal" cores, like V12-122.

Dating Nearshore Marine and Lake Deposits

The use of 23°Th and 231 Pa is generally limited to sediments deposited at rates of 10 cm 10- 3 yr- I (or 0.1 mmjyr) and less. For deposits such as coastal and lake sedi­ments accumulated at rates of the order of millimeters per year, 21°Pb has proven to be a useful geochronometer. It provides chronologies of the past 100-200 years.

21 0Pb METHOD The isolation of 21 °Pb, a member of the 238U-series with a half-life of 22 years, can be traced back to its precursor 222Rn. This noble gas nuclide tends to escape from the surface of the earth into the atmosphere. Most of the 222Rn atoms entering the atmosphere remain in the troposphere where they decay to 21°Pb through a series of short-lived intermediate nuclides. The residence time for 210Pb in the troposphere is estimated to range from days to about a month before it is removed by precipitation and dry fallout (Francis et a11970, Pierson et al 1966).

This atmospheric flux of unsupported 21°Pb, assumed to have remained constant at a given locality, was initially proposed by Goldberg (J963) to date permanent snow fields, using Equation 2. The general validity of the proposition has since been confirmed (Crozaz et al 1964, Windom 1969). Application of the technique has been extended to lake and coastal marine sediments. Exponential decreases of

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URANIUM-SERIES METHODS 359

210Pbex ( = 210Pb_ 226Ra) with depth in lake cores have given measures of average sedimentation rates that essentially agree with those derived from other lines of evidence such as artificial radioactivity (fission products) and palynology (Krishnaswami et a11971, Koide et a1 1973, Robbins & Edgington 1975). Indications are that input of 2!°Pb from rivers feeding the lakes n1ay be insignificant and most of the excess 210Pb in sediments originates from overhead precipitation (Goldberg 1963, Krishnaswami et aI1971).

In the nearshore marine sediments, the excess 210Pb has an additional source: 226Ra in seawater. The 210Pb formed from this source, together with that from the atmospheric fallout and terrestrial runoff (if any), is scavenged by sinking particulates of both biogenous and detrital origin throughout the water column. The scavenging in the coastal regions is rather efficient. There, the residence time of 21°Pb in the surface mixed layer of the ocean is estimated to range from a few years (Rama et al 1961, Koide et al 1972) to less than a month (Bruland. et al 1974b), depending upon the intensity of biological productivity.

The reliability of the method when applied to the marine environment was first documented in a study of the varved sediment from the Santa Barbara Basin off California (Koide et aI1972). As shown in Figure 5, the 210Pb-derived rate of 3.9 mm! yr, averaged over a 112 year period, compares favorably with the mean annual valve thickness of 3.3 mm in the core. The agreement strengthens the method's critical assumption-relatively constant flux of 2!OPb to a deposition site.

Part of the 210Pb in sediments must be supported by 226Ra. This has not been corrected in the Figure 5 data. As has been noted in discussing BOTh, the correction becomes more important in the deeper strata. In order to date deeper sections in the core, hence to extend the range of the method, the 226Ra corrections were made in subsequent studies (Bruland et al 1974a, Bruland 1974, Murray 1975).

Koide et al (1972) postulated postdepositional migrati9n of lead to explain the low surficial concentration of 210Pb in two of the cores they analyzed. Finding no supporting evidence for such a postulation, Robbins & Edgington ( 1975) suggested sediment mixing as an alternative explanation. Their suggestion, however, cannot account for the observed maximum 210Pb values near the sediment-water interface. A more likely I.:ause would be the very high water content of the surficial strata. Failure to remove the interstitial salts could result in a dilution of 210Pb concentra­tion in the analyzed samples, as noted by Bruland (1974). Since high and variable water contents are not uncommon to the newly deposited coastal sediments, expressing 210Pb concentration on a salt-free basis or normalized to aluminum content of the sediment (Goldberg & Bruland 1974) would be desirable. In the Al­normalization, 210Pb is assumed to be principally associated with the aluminum­silicate phases. This needs to be substantiated.

The method was initially tested on anoxic sediments in which bioturbation is minimum. Recent studies (Murray 1975, Murray & Ku 1974) have also indicated its utility in relatively oxygenated areas with sufficiently rapid sedimentation (e.g. > 1 mmjyr); there, disturbances of benthic fauna, if occurring, are commonly limited to a depth of around 5 cm. The applicability of 210Pb to other coastal environments such as estuaries, lagoons, and continental shelves, should be further a·ssessed.

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360 KU

80�------------------------------�

.......

1960-62 58-60

-54-56· 40 6-58

20

52-54 50-52

40-42 - 44-46

� .10-12 E c..

"0 -.Q a.. 0 (\J

10 / 8

3.9mm/y

6

4

CORE 239

1900-02

1890-92

80-82 _70-72

+60-62 50-52

2�--�--�----�--�--�----�--�--� o 5 10 15 20 25 30 :35 40

DEPTH IN CORE (em) Figure 5 Equation 2 plot for core 239 from the Santa Barbara Basin; c is expressed as 210Pb concentrations. The dates assigned to the analyzed layers are derived from counting varves in the sediments. Koide et al (1972).

228Th/232Th METHOD The activity ratio 228Th/232Th in surface and deep waters of the ocean commonly varies between 5 and 30 (averaging about 15) (Nikolayev et al 1962, Moore & Sackett 1964, Somayajulu & Goldberg 1966, Miyake et al 1970, Imai & Sakanoue 1973, Knauss et a1 1975). This means that only a small fraction of the 228Th in these waters is generated from 232Th in solution; the remainder comes mainly from the diffusional input of 22BRa from bottom sediments (Koczy et a1 1957, Moore 1969). Similar situations presumably exist in lacustrine environ­ments. On precipitation, excess 228Th could be detectable in surface layers of near­shore and lake sediments; with time, it should disappear with a half-life of 1.9 yr. Using an acid-leach technique, Koide et a1 (1973) measured 228Th/232Th ratios in sediments and obtained sedimentation rates for the top 4-8 em of two cores. The rates

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URANIUM-SERIES METHODS 361

were comparable to those based on the 21 °Pb chronology. These workers suggested that the 228Th/232Th ratio may be used for dating sediments deposited around the last decade and as permissive evidence for the recovery of the uppermost levels of the deposit during coring operation.

Recent studies (Murray 1975) on 21°Pb_dated sediments of the San Pedro shelf off southern California have shown that surface 228Th/232Th ratios in these sediments, measured by both the acid-leach and total dissolution techniques, are significantly less than the equilibrium value of unity. It appears that extensive 228Ra migration has occurred, rendering the suggested 228Thj232Th method inapplicable to these sediments.

In addition to the methods discussed above, excess 226Ra has been found in freshwater manganese nodules and used to estimate the accretion rates of these lake deposits (Krishnaswami & Moore 1973).

Use 0/234U_238U Disequilibrium

The excess 234U over 238U in natural waters raises the possibility of an age method based on the disappearance of the excess 234U in solids precipitated from such waters. Substituting C = (234U/238U)_1 and Co "" e34U/238U)o_1 in equation 1, we obtain

(5)

where e34U/238U)0 is the initial 234U/238U ratio and A4 is the decay constant of 2340. The age of a deposit can be calculated if e34U /238U)0 is known. For terrestrial waters, conditions are generally too variable to warrant estimation of e34U/238U)o (Cherdyntsev et al 1963, Thurber 1963, Chalov et al 1964, Thompson et al 1975). This is not the case for the ocean. Thurber (1962, 1963) analyzed recent marine corals and oolites and consistently found a 15% excess of 234U over 238U. This finding has been confirmed by later analyses and by direct measurements of uranium in seawater from various parts of the oeean (summary in Goldberg & Bruland 1974). Open ocean 234U/238U values have been estimated, at 95% confidence limits, to be 1.14±0.03; variations shown are comparable to the analytical precisions. The uniformity in isotopic composition as well as concentration of uranium in the ocean (Ku et al 1974), a reflection of uranium's long open ocean residence time, justifies us to assume e34U/238U)0 to be 1.14 or 1.15 for marine precipitates. As 234U decays with a 248,000 year half-life, the 234Uj238U method would potentially be useful to date marine deposits over the last million years. The success of its applications, however, has mostly been limited to unaltered fossil corals, based on agreem'::nt with ages derived from the 230Th/234U (to be discussed later) and He/U methods (Thurber et al 1965, Veeh 1966). Studies of fossil marine mollusks suggest (a) that a sizable fraction of their uranium comes from the sediment matrix, which prevents a reliable estimate of the initial 234U excess, and (b) that in some cases

,continuous exchange of uranium with its surroundings may have occurred (Kaufman et al 1971). With few exceptions (Ku & Broecker 1 967b, Krishnamoorthy et al 1971), Equation 5 is seldom applicable to pelagic deposits. This is because in a typical pelagic sediment (a) most uranium is nonauthigenic, and (b) part of the 234U is

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362 KU

subject to postdepositional migration (Ku 1965). The second statement was reached by a diffusion-model fit of the 134U/238U data observed in three red-clay cores (Figure 6). The fraction of the "mobile" 234U may be related to the oxidation (from + 4 to + 6 valence state) of 234U accompanying radioactive decay (Kolodny & Kaplan 1970), or to the a-recoil range of 234Th in sediments, which is a function of sediment particle size and density (Kigoshi 1971). In any case, because of their recoil nature the in situ-generated 234U atoms do not appear tightly bound. As the number of such atoms increases with depth in the core, upward diffusion of 234U along its concentration gradient would ensue.

.

Although models such as those proposed by Ku (1965) and by Kolodny & Kaplan ( 1970) allow parametric sedimentation rates or ages to be assessed for certain deposits, they provide more geochemical insight than geochronological utility. In this context, one should note that 234U/238U ratios have been used extensively as an index of geochemical processes operating in uranium deposits, soils, and groundwaters (Dooley et al 1966, Rosholt et al 1966, Osmond et al 1974), and to distinguish uranium sources in metalliferous sediments associated with ocean ridge processes (Ku 1969, Veeh & Bostrom 1971, Rydell & Bonatti 1973, Rydell et aI 1974).

1 .00 0 = :3 x 1 0 -8

cm2

/sec

S = 3 m m / 1 03 y Fm= I O%

6 5 �-L __ �� __ -L __ �-J __ � __ L-� __ ���-L __ �� __ � o 200 400 600 800 1000 1200 1400

DEPTH IN CORE (em) Figure 6 Measured 234U/�38U ratios (bars) in a red-clay core V IO-95 (26°31 'N, 5 1 °47'W). The curves refer to the distributional patterns of 234Uj238U if (a) the core has a constant sedimentation rate of 3 mm/103 yr, (b) a fraction, Frn, of the in situ-produced 234U in sediments is subject to postdepositional diffusion, and (c) the diffusion coefficient of this mobile 234U is 3 X 10 - 8 cm2/sec Ku (1965).

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URANIUM-SERIES METHODS 363

Chalov et al (1964) proposed the use of 234Uj238U to date the initiation of closed (no-outflow) lakes. Under the assumption that influx of uranium to the lake is large compared with its removal and bears a constant isotopic composition, e34Uj238U)o as measured in feedwaters, the age of the lake can be calculated from the 234Uj238U ratio of the present lake water (Chalov et al 1 964, see also Komura & Sakanoue 1967) :

( Z34Uj238U) - 1 = W34Uj238U)O - lJ [ 1 - exp ( - A4t)J ()'40- 1 (6)

where A4 is the 234U decay constant. Ages of two alpine lakes as determined by this method were consistent with those derived from chloride accumulation and other geological considerations (Chalov et aI 1964). Noting that the uranium isotopic composition in the feed streams was more uniform than its concentration over yearly cycles, these workers contended that this method should be more reliable than any constant-influx methods using element concentrations. The constancy of the observed feedwater 234U j238U ratios, of course, has to be extrapolated over the entire dating periods of hundr�ds of thousands of years. The extrapolation involves taking risks.

Other Applications Because unsupported 228Ra (t1/2 = 6.7 yr) is present in coastal surface water, its incorporation into coral skeleton is useful for diciphering the chronology of modern corals. The decay of this 228Ra with depth in corals gives mean skeletal growth rates over the last 30 years, assuming that ratios 228RajCa or 228Ra/226Ra initially incorporated by the corals remain constant in time. Rates thus obtained agreed with the 90Sr and bomb 14C data (Moore et al 1973, Moore & Krishnaswami 1974) and indicated that the density bands as revealed by X-radiography (Knutson et al 1972) are indeed annual (Dodge & Thomson 1974, Moore & Krishnaswami 1974). Similar approach may be attempted using 2 1 0Pb. Strong deviations from the ideal 2 1 OPb/226Ra decay curve were noted in samples showing relatively smooth 228Raj2Z6Ra decrease (Moore & Krishnaswami 1972, Moore et al 1 973), implying a greater variability of 21 °Pb than the radium isotopes in the coastal surface ocean.

White lead is a pigment in painting and lead metal is an important constituent of other works of art, such as pewter and lead-bearing bronzes. The 210Pb_226Ra disequilibrium engendered by the lead extraction from ores could therefore provide a dating tool in the fields of art authentication and archaeology. Keisch ( 1 968) used excess 2 10Pb to distinguish eighteenth-century and earlier paintings from forgeries made in the twentieth century.

METHODS BASED ON ACCUMULATION OF DECA Y PRODUCTS OF URANIUM

The decay products here refer principally to 230Th and 231 Pa. Under this category, most of the work and contributions have so far come from dating carbonate material, chiefly corals, mollusks, and speleothems. This we review at some length.

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364 KU

Dating Carbonates Uranium is coprecipitated with calcite or aragonite from natural waters that are essentially free of thorium and protactinium. In a fossil carbonate, the amounts of 230Th and 231 Pa initially present could be considered negligible in comparison with those subsequently generated by the decay of uranium. If the carbonate remained a: closed system, the amounts of 230Th and 231Pa generated therein are functions of time and uranium content. This forms the basis of the two age methods described below.

230Thj234u METHOD Potratz et al ( 1 955) and Barnes et al ( 1956) first reported the use of 23°Th accumulation for dating corals. Concurrently, Cherdyntsev ( 1956) suggested its application to fossil bones. These and several subsequent workers (e.g. Sackett 1958, Tatsumoto & Goldberg 1959, Blanchard 1963), while exploring the possibility of dating other materials such as oolites and shells, used the relation­ship :

230Th/238U = l - exp ( - Aot) (7)

With the discovery of 234U_ 238U disequilibrium in natural solutions, Equation 7 should be modified to :

23oThj234U = (238uj234U)[I _ exp ( - Aot)] + [1 - (238U/234U)] [ Ao/(Ao - ,1,4)] [1 - exp (,1,4 - Ao)t] (8)

In Equations 7 and 8, ,1,0 and A4 represent respectively the decay constants of 230Th and 234U ; 230Th, 234U, and 238U are measured activities in a sample of t years old. The modification necessitates measurement of 234U/238U as well as 230Th/ 234U for each sample (except for corals and oolites). Figure 7 shows a graphic solution for Equation 8 (Kaufman & Broecker 1965). The current techniques permit measurement back up to 350,000 years.

231Pa/235U METHOD The ingrowth of 231Pa from 235U for dating carbonates was proposed by Sackett ( 1958). The sample age t is calculated from :

(9)

where Al is the decay constant of 23 1 Pa. In practice, 235U is usually obtained from measurement of the more abundant 238U, noting a constant activity ratio 23 5U/ 238U of 0.046 for natural uranium (Hamer & Robbins 1960). This method has a potential range of up to 1 50,000 years. It has not been as widely used as the 230Th/234U method because of the low abundance and analytical tediousness of 23 1 Pa.

EVALUATION OF RESULTS All age-dating methods require that, over the time interval considered, the sample remain closed to gain or loss of nuclides of interest­the closed system assumption. Though implicit in our previous discussion of the

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URANIUM-SERIES METHODS 365

decay methods, this assumption has not been singularly stressed. The reason is threefold.

First, notwithstanding inference being made of possible postdepositional migrations of 230Th and 21°Pb (Sackett 1965, Koide et al 1972), satisfactory mechani$ms or proofs for such migrations have yet to be presented. The diffusion coefficients of 234U and 226Ra in sedimentary columns have been estimated to be of the order of 10- 8_10-9 cmZ/sec (Ku 1965, Koczy & Bourret 1958, Goldberg & Koide 1963). These estimates should be the upper limits for the less soluble isotopes like 230Th, 23 1 Pa, and 21 0Pb. Koczy (1965) set diffusion coefficient for 230Th at about 10- 1 2 cm2/sec, which would be small enough to be negligible in age determination of sediments accumulated at rates of millimeters to centimeters per thousand years. Secular equilibrium between BOTh and 234U has been consistently observed in deeper sections of sediment cores (Ku 1965, 1966).

Second, diffusion of 234U and 226Ra deters direct use of these nuclides in age­dating (the 234U/238U method and the use of 226Ra as an index of 230Th), but does not affeet the use of BOTh and 2 lOPb because the latter nuclides are plentiful relative to 234U and 226Ra in younger deposits.

Third, the decay methods employ the best-fitting procedure, which is essentially an averaging technique to smooth out perturbations of various kinds, including any small-scale migration of isotopes.

2.

1 .()1---'T-.....,. ........ -IL...-.....,-L--�r'--L--I---'-.... --'--.L-L..L4LLL.L.+---.---_,--.J .00 .50 1.00

Figure 7 Variation of 234U/238U and 230Thj234U ratios with time in a closed system (ree of initial 230Th. The near-vertical lines are isochrons (locus of points for samples of the same age but dilTerent initial 234U/238U ratios). The horizontal curves denote age paths of samples with initial ratios 1 . 5, 2.0, and 2.5. Typical error in analysis is also indicated.

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366 KU

For the ingrowth methods discussed here, however, ages are directly related to the parent-daughter ratios, and the closed system requirement becomes rather stringent. Indeed, that stipulation has severely limited the applicability of these methods to certain types of material, like mollusks.

Unaltered fossil corals free of recrystallization or void-filling material have consistently yielded reliable age results. Corals deposit aragonitic skeletons that contain about 3 ppm uranium and negligible thorium and protactinium. Upon death of the organism, the coral skeleton apparently behaves as a closed system until its recrystallization to calcite, during which process preferential loss of U relative to Th and Pa may occur (Sackett 1958). Ample evidence testifies to the reliability of results obtained on the unaltered corals, including (a) concordant dates derived from 230Thj234V, 231Paj235V, and 234Vj238V ratios (assuming an initial 1 5% excess 234U) in the same sample (e.g. Ku 1 968) ; (b) agreement with stratigraphic informa­tion (e.g. Mesolella et al 1969) ; and (c) checkout with other geochronometers such as 14C and He/V (e.g. Thurber et a1 1965, Fanale & Schaeffer, 1965).

Uranium-series dating of corals associated with former shorelines in different geographic locations have produced valuable information on the chronology of Pleistocene glacio eustatic oscillations and in several places on the rates of tectonic uplift. A number of raised reefs from tectonically active regions ha ve been thoroughly dated, such as Barbados (Broecker et al 1968), New Guinea (Veeh & Chappell 1970, Bloom et aI 1974), and the Ryukyu Islands (Sakanoue et a1 1967, Konishi et al 1970). Many dates are also available from more stable areas, such as Florida (Osmond et al 1965, Broecker & Thurber 1 965), Hawaii (Veeh 1 966, Ku et al 1974), the Bahamas (Broecker & Thurber 1965, Neumann & Moore 1 975), and several atolls and small islands in the Pacific and Indian Oceans (Thurber et a1 1965, Labeyrie et al 1 967, Veeh 1966). Chiefly from these studies, a record of the relative sea level changes over the past 1 50,000 years has emerged (Broecker & van Donk 1970, Steinen et al 1973, Bloom et aI 1974). The reef dating appears to have registered major sea level fluctuations with periods of the order of 20,000 years, and the last time the sea stood significantly higher than it does today must have occurred around 1 15,000-140,000 years ago (centred about 125,000 years ago). As the resolution of the present dating techniques is usually about 10,000-20,000 years (Figure 7), refinement or extension of the sea level record requires further analytical improvements as well as extensive field investigations. The Barbados data have indicated that favorable conditions for coral growth also prevailed 1 70,000-240,000 years ago (Mesolella et al 1969).

Like corals, the inorganically precipitated marine oolites incorporated a few ppm uranium and negligible thorium in their aragonitic crystals when they formed. Un­recrystallized oolites appear also suitable for U-series dating (Tatsumoto & Goldberg 1959, Osmond et al 1965, Broecker & Thurber 1965), although because of their geological occurrences (often in dunes) they are not ideal markers for former sea stands, unlike reef corals.

Uranium-series dating of speleothems (cave-deposited travertines) has recently been reviewed by Harmon et al ( 1975). The most common speleothem forms­stalactite, stalagmite, and fiowstonc-arc developed by slow precipitation of CaC03· Such deposits tend to be macrocrystalline, compact, and not subject to postdeposi-

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URANIUM-SERIES METHODS 367

tional leaching. Pure calcite speleothems with well-preserved internal stratigraphy can be reliably dated by the 230Th/234U method, provided they contain sufficient uranium (U content may range from 10 ppb to 100 ppm). Internally consistent sequences of 230Thj234U ages in a sample were secured, and in a few cases, where comparison among 14C, 2 3 1 Pa/235V; and 230Th/234V ages was made, the agreement was good (Cherdyntsev et al 1965, Spalding & Mathews 1972, Thompson 1 973).

However, the prospect for application of 234V/238V to dating speleothems is not good, because in most cases the initial excess could not be accurately determined (Duplessy et al 1970, Thompson et al 1975).

Besides answering the intriguing question of speleothem growth rates, dating of cave deposits has great utility in geomorphic studies of karst landforms (e.g. Ford 1973). Perhaps more importantly, it offers a unique means of assessing Pleistocene climatic changes in continental areas when combined with 1 80;t60 and D/H studies. Research in this area, which has just begun, has already yielded promising results (Hendy & Wilson 1968, Duplessy et al 1970, Thompson et al 1974, Schwarcz et al 1975). Two interesting studies on the 230Thj234U dating of presently submerged (below sea surface) stalagmites from caves in the Bahamas and Bermuda (Spalding & Mathews 1972, Harmon & Schwarcz 1974) suggested a way to educe heights of the Quaternary low sea stands.

Understandably, the importance of successful dating of molluscan shells, by virtue of their ubiquity and abundance in geologic deposits, cannot be overstated. The subject has indeed commanded much attention. For age dating, the numbers of V-series isotopic analyses done on mollusks probably exceeds that on any other material. Yet, despite these efforts, uncertainties remain about how to distinguish the failures from the successes where ages are not independently known, as noted in a detailed critique by Kaufman et al (1971).

The first glimpse of the complexity in mollusk dating came from the work of Broecker (1963) and Blanchard ( 1963), who reported that fossil marine mollusks typically have much more uranium than living ones. Fossil shells of various ages show mean values in the vicinity of 1 ppm V, whereas 95% of their modern counterparts contain less than 0.5 ppm V (Kaufman et al 1971). Thus most of the uranium in mollusk is of secondary origin. Vranium content in fossils does not tend to increase with age, however, leading Broecker ( 1963) to suggest that the uptake of

uranium occurs shortly after the death of the organism. Data gathered to date seem to indicate that fixation of most of the uranium, a process probably related to the degradation of organic material, ceases after a few thousand years. This will not cripple the method because its age range of interest often goes beyond 50,000 years. But exceptions to this rule may occur (Kaufman et aI 1971), and there is no sure way

to sort them out. The next complication concerns the problem of extraneous 230Th (and 23 1Pa).

Fossil mollusks, unlike their living equivalents and corals, frequently show relatively large amounts of 23 2Th (Blanchard et al 1967). This is especially true for calcitic shells. The 23 2Th was apparently acquired from a continental environment in which the shells are often in contact with silicate sedimentary matrix. The question arises as to whether corrections can be made for the "common" 230Th, which is

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368 KU

presumably incorporated along with the observed 23 2Th. The correction should be R 232Th exp ( - Aot), in which R is the 230Thj232Th ratio entering the shell, ,1,0 is the decay constant of BOTh, and t is the time elapsed since addition of the common 23°Th. R may have a range of values, as reflected by the 230Thj232Th data on natural waters and soils (Szabo 1969, Cherdyntsev 1971). Attempts have been made to estimate R on a regional basis (Kaufman & Broecker 1965, Osmond et al 1 970). Even if this could be done in each case, the problem of assigning t in the correction term remains. The age errors incurred from erroneous common 230Th correction have been discussed (Kaufman et al 1971). There is as yet no data base whereupon corrections for extraneous 2 3 1 Pa (if any) can be formulated. As a working guideline, shells (or corals etc) with 230Th/232Th ratios less than about 20 should be avoided.

The ultimate question lies in whether or not mollusks give reliable uranium­series ages. The answer could be referred to Kaufman et al ( 1 971 ) who concluded that at least half of the mollusk data compiled show a discordance between 230Thj234U ages and 23 1 Paj235U ages and between their 230Thj234U ages and age estimates from paleontology, K-Ar, 14C, and coral 23°Thj234U data. The picture would change little even if these workers' data compilation included additional and more recent published results on concordancy checks (e.g. Sakanoue et al 1 967, Veeh & Valentine 1967, James et al 197 1 , Szabo & Vedder 1971, Ku & Kern 1974, Szabo & Gard 1975). Aside from the secondary uranium and thorium uptake n.oted above, the root

NUMBER OF SAMPLES P E R 0. 1 I N TERVAL OF 230 Th/z34 U 1.40 r----,r----r---r---r--r---.---..--,----,r----r---r---r-.

4 1 3 1 3 1 7 2 2 4 2 42 1 8 1 0 I I 4

1.30

::::) co 1.20 gj ....... ::::)

� ro

1 . 10

1.00 L----'-_--L._....1L_.L...._L---L_--L..._....J.-"!L-..1!:4..=L.JL---'-_-'---' o .2 .4 .6 .8 1 .0 1 .2

230Th / 234 U Figure 8 Data on over 200. marine mollusks in a Figure 7 plot. The rectangles are drawn in for each 0. 1 interval of 230Th/234U such that they include the median 60% of the mollusk data points for that interval. The shaded area represents the range for corals. Note, whereas corals follow the closed system age path with an initial marine 234U/238U of 1 . 1 5, mollusks do not (Kaufman et at ( 1971).

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URANIUM-SERIES METHODS 369

of the problem can be traced to the observed 234U/238U ratios in fossil mollusks of both marine and terrestrial origin : (a) they commonly reftect those of the terrestrial environment (i.e., > 1 . 1 5), and (b) contrary to the prediction of Figure 7, they show an increasing trend as 230Th/234U increases (Figure 8). Clearly, assimila­tion or exchange of uranium and possibly its products took place in a continental environment, and at least half the time the process persisted long enough to pose a serious obstacle to age determination.

To correct the effect of isotope migration, an open system model has been constructed (Rosholt 1 967, Szabo & Rosholt 1 969). The model deals with a certain type of discordant 23 1Pap35U_230Thj234U results and designates a steady-state contamination process with fixed migrational patterns for the isotopes involved. At times the open system dates seem to improve over the closed system ages, but not always. The reality and universality of the model have been questioned (Kaufman et a1 1 971 , Kaufman 1 972).

At the present, the best way to distinguish reliable from questionable ages is a concordancy check between 230Thj234U and 23 1 Par' 'U. Without such a check, one places little confidence in isolated dates. Other proposed closed system criteria such as nonrecrystallization, plausible U and Th concentrations, and 22<;Ra/23°Th and 228Thj232Th ratios (Kaufman & Broecker 1 965, Stearns & Thurber 1965, Blanchard et a1 1 967) are useful but less stringent. There is as yet no effective guideline for selection of suitable samples before analyses. Aside from the preservation appearance, one clue may be that specimens found in carbonate matrices show less signs of radionuclide migration than those found in silicate sediments, as suggested by the results of Stearns & Thurber ( 1965) and James et al ( 1971). Although shells of different initial mineralogy (aragonite vs calcite) have different isotopic charac­teristics, it has not yet been determined which mineralogy is the more suitable (Kaufman et a1 1971 , Broecker & Bender 1972). Data on the solitary corals and their coexisting aragonitic shells in raised Californian marine terraces (silicate sediments) offer some interesting comparison (Veeh & Valentine 1967, Ku & Kern 1974). The aragonitic corals contain primary marine uranium whereas the shells do not. Also the latter consistently give younger 230ThF34u ages than the former. Does this mean that any consideration in mineralogy and sediment matrix is easily over­ridden by the uranium source problem ? Questions and clues such as the foregoing are subjects for future inquiry. Only after much further research into the nature of the disruptive processes at work can one begin attempting to salvage questionable ages via modeling or other measures of a general nature and thereby improve the present dismal success rate of � 50%.

Other works on carbonate material include the dating of marls in the Jordan River-Dead Sea Graben (Kaufman 1971) and of the arid zone calcretes (caliche) in the southwestern U.S. (Ku 1975). Both studies involve inorganically precipitated carbonates mixed with some silicate detrital components which require common 230Th corrections. As reflected in their internally consistent 230Thj234U ages, materials used in these studies apparently form an undisturbed system.In this regard, the absence of organic matter may play a role. Uranium distribution in molluscan shells is not uniform ; higher concentrations are believed to be associated with organic coatings (Lahoud et a1 1 966, Komura & Sakanoue 1967).

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370 KU

Applications to Other Systems Following the early work of Cherdyntsev (1956), dating of fossil bones with the uranium-series nuclides has appeared in several recent articles (Szabo et al 1969, 1 9,73 ; Hansen & Begg 1 970 ; Howell et al 1 972 ; Ward et aI 1 972 ; Szabo & Collins 1975). The situation encountered in the bone system resembles that in mollusks. In bones, uranium is largely secondary and shows rather high concentrations (mostly 20-400 ppm, with 234U/238U of 1.1-1.5). Thorium contents are usually low-of the order of 0.0 X ppm. Therefore correction for the extraneous 2 30Th is hardly required. Cases for open system in fossil bones have been documented by the discordant 230ThF34u and 23 1Paj235U ages. From a survey of the literature, the incidence of such discordancy appears slightly less than 50%. Hence in this respect bones seem to fare better than mollusks ; the high uranium content of the former may be a factor. In view of its potential contribution to archaeology, dating of bones deserves continuous efforts. Calibration of uranium-series dates with those of 14C (on collagen) and fission track would be useful.

Application of the 230Th and 231 Pa ingrowth methods to the following systems have also yielded meaningful age information : marine phosphorites (Kolodny & Kaplan 1970, Veeh et al 1973, Burnett 1974), shallow-water marine manganese nodules (Ku & Glasby 1972), saline deposits of dry lakes (Goddard 1970), and secondary uranium-bearing minerals (e.g. Allegre 1964).

DATING IGNEOUS ROCKS

Chemical fractionation between different elements of the decay chains also occurs during magmatic processes. In unweathered Quaternary igneous rocks, often radio­active equilibrium exists between 234U and 238U; but not between the uranium parents and their daughters : BOTh, 23 ipa, 226Ra, and 2 1 0Pb (Anestad-Fruth 1963 ; Somayajulu et a1 1 966 ; Oversby & Gast 1 968 ; Cherdyntsev et al 1 967, 1968). Dating of these rocks has been done by utilizing the disequilibrium relationship between 23°Th and 238U ; the former nuclide can be either in excess or depleted with respect to the latter. As first attempted by Cerrai et al (1965), one assumes that when a magma solidifies, its different minerals or phases may inherit different Th/U (hence 230Th/234U) but identical 230Thj232Th and 234U/238U ratios. A given mineral, after having acted as a closed system for t years following crystallization, should have its 230ThP32Th ratio as :

230Thj232Th = e30Thoj232Th) exp ( - Aot) + (Z38U/232Th)[I - exp (- Aot)] (10)

where 230Tho is the initial BOTh activity and )'0 the decay constant of 230Th. In this equation, there are two unknowns : 23°Tho/232Th and t. Thus the age can be uniquely determined from two or more minerals of common origin. For instance, for a pair of minerals, A and B. from the same rock,

(11)

where i stands for 230Th/232Th and u stands for 238U/232Th, with subscripts A

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URANIUM-SERIES METHODS 371

and B refering to minerals A and B respectively. It can be seen from this equation that the precision in estimating t depends heavily on the difference in the U-Th fractionation between the two minerals, as denoted by the term U A - UIY

The method has been applied in the studies of various acidic rocks, including granite, lavas, pyroclastics, and pumice (Kigoshi 1967, Taddeucci et al 1967, Discendenti et a1 1970, Fukuoka 1974). These studies have cited general agreement of the 23°Th dates with independent estimates from K-Ar. 14C, fission track, or stratigraphic evidences. Noteworthy is that the 230Th ages thus derived refer to the time of crystallization of minerals, which could take place in the magma chamber, and they are upper limits for the eruption ages.

A graphic presentation of Equation 10 has been used (Kigoshi 1967, Allegre 1968). As shown in Figure 9, minerals of the same formation age from a rock should fall on a single straight line (isochron) with slope 1 - exp ( - }4) and y-intercept

09o

Jr---o'Ti2=----=oT-'�.4---=r�.6=----=OFIB--

I.:.;:IP=----

t = O L- I 0.8

0.6

+ L-2

P-3

..c 05 l-N [(j 04 "-..c I-o �

0.3 G-/

02

0. 1

O �-� ___ _L ___ � ____ L_ __ � ____ -L __ -L ___ � o 0.1 Q2 03 04 05 06 0.7 08

238 U / 232 Th Figure 9 Equation 10 plots for separate fractions isolated from three rocks: a Cretaceous granite (G), a 1 783 A.D. lava (L), and a pumice (P) whose age has been inferred at 35,700 years through 14C dating. Data arc from Kigoshi ( 1967) in which the separated fractions were obtained by partial dissolution or extraction. These chemical procedures may involve hot-atom effect. A better procedure would be to use physically separated mineral phases, as in Taddeucci et al ( 1 967).

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372 KU

e30Tho/232Th) exp ( - Aot). Those not plotted on a defined isochron are products of different crystallization time and melt e30ThF32Th) composition domain. Adopting such concepts, Allegre (1968) suggested significant time differentiation between mineral formation at depth and eruption (by noting the glass phase plotted below the mineral isochron), and Fukuoka & Kigoshi (1974) identified the presence of relic zircon grains (by noting certain zircons plotted above the isochron). On the other hand, Kuptsov et al ( 1969) held that volcanic rocks may involve multiple (more than two) generations of minerals that would defy treatment by the method discussed here. In such cases, these workers suggested the use of Equations 7 and 9 to obtain maximum ages for those minerals showing deficient 23°Th and 23 1 Pa.

Studies of young igneous rocks with the U-series isotopes have apparently just begun. Much more data are needed before their potential contributions to elucidating igneous processes as well as to age dating can be fully appreciated.

CONCLUDING REMARKS

The unique aspect of the uranium-series disequilibrium methods is their diversity in terms of time and material to which they apply, and of the scope of problems they handle. Also, reliability checks can sometimes be made by examining internally several related parent-daughter pairs.

Although Joly (1908) reported the 226Ra enrichment in deep-sea sediments and manganese nodules retrieved from the Challenger Expedition ( 1872-1876)-the first observation of the effect of "disequilibrium" -as early as 1908, utilization of the fractionations produced in nature's laboratory did not progress rapidly until the past two decades. The field, still comparatively young and expanding, offers challenges. New datable material is being discovered and new relationships explored. While some areas are in the midst of seeming vacillations pending strokes of fresh approaches, some are so nascent in their developmental stage that the obstacle to progress is simply lack of data. The speculation and controversy in an expanding field such as this can unsettle those who are mainly interested in applying the methods or their results. If this review helps these consumers and those contemplating entry to realize the status, the problems, and some of the prospects of the field, it

will more than serve its purpose.

ACKNOWLEDGMENTS

I wish to acknowledge the Oceanography and the Earth Science Sections of the National Science Foundation for their support of my studies in this field (current

grants DES72·01 557 and DES72-0166 1). I thank Mu-ching Lin and Carol McCienning for their assistance in the preparation of the manuscript.

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