Timing and duration of mare volcanism in the central region of the northern farside of the Moon
© The Society of Geomagnetism and Earth, Planetary and Space Sciences (SGEPSS); The Seismological Society of Japan; The Volcanological Society of Japan; The Geodetic Society of Japan; The Japanese Society for Planetary Sciences; TERRAPUB. 2011
Received: 19 August 2009
Accepted: 22 February 2010
Published: 21 February 2011
Age determinations of lunar mare basalts are essential for understanding the thermal evolution of the Moon. In this study, we performed new crater size-frequency measurements in mare deposits in the central region of the northern farside, consisting of Lacus Luxuriae, Buys-Ballot, Campbell, and Kohlschutter, using high-resolution images obtained by SELENE (Kaguya) Terrain Camera. The estimated model ages of the mare deposits range from 2.7 to 3.5 Ga. On the basis of model ages for all investigated mare deposits in the central part of the northern farside, considering the results of previous studies, we concluded that mare volcanism in this region began at least as early as 3.9 Ga and continued until ∼2.6 Ga. From a comparison of model ages in the region and the South Pole-Aitken basin, we found that mare volcanism in these regions ended at the same time, suggesting that the South Pole-Aitken basin formation impact had a minor effect on mare volcanism in the region.
Key wordsMoon mare volcanism lunar farside Feldspathic Highland Terrane the South Pole-Aitken basin crater size-frequency measurement
Unraveling the volcanic history of the Moon is essential for understanding its origin and thermal evolution. Lunar mare basalts, which are the most common volcanic features on the Moon, cover 17% of its total surface area and occur preferentially in topographic lows on the nearside (e.g., Head, 1975; Head and Wilson, 1992). On the farside, limited numbers of maria occur in some basins and craters. The asymmetrical distribution of exposed mare basalts has evoked many questions concerning the generation and emplacement mechanisms of mare basalts (e.g., Solomon, 1975; Wasson and Warren, 1980; Head and Wilson, 1992; Zhong et al., 2000; Werner and Loper, 2002). To reconstruct and understand the mechanisms, it is critical to determine the ages, volumes, and compositions of mare basalts.
A considerable number of nearside maria have been dated by using image data from Lunar Orbiters and Apollo missions (e.g., Wilhelms and McCauley, 1971; Boyce, 1976; Wilhelms, 1987; Hiesinger et al., 2000, 2003, 2006, 2008; Bugiolacchi and Guest, 2008). These studies revealed that the largest number of mare basalts formed in the Late Imbrian Epoch at 3.2 to 3.8 Ga, indicating good agreement with radiometric ages for returned basaltic rocks, and that mare volcanism lasted until the Eratosthenian Period (e.g., Boyce, 1976) or even until the Copernican Period (Wilhelms, 1987; Hiesinger et al., 2003, 2008), suggesting that the total duration of lunar volcanism was 1.5 to 3.0 Ga.
Prior to the SELENE (Kaguya) mission (Kato et al., 2008), accurate age determinations of most maria on the farside had not been performed because of the lack of high spatial resolution images. Therefore, a systematic, high-resolution mapping of the entire lunar surface, particularly the farside, is a primary objective of the SELENE mission. The Terrain Camera (TC) onboard SELENE is a panchromatic push-broom imager with two optical heads that acquire stereo data for the entire surface of the Moon with an average resolution of 10 m/pixel (Haruyama et al., 2008). The TC has obtained high-resolution images of most areas of the lunar farside at solar elevation angles lower than 10°. Using the high-resolution images, Haruyama et al. (2009) carried out crater size-frequency measurements in farside mare deposits within the South Pole-Aitken (SPA) basin and Mare Moscoviense, and found that mare volcanism on the lunar farside lasted ∼2.5 Ga, longer than was previously considered.
The SPA basin is the largest impact feature on the Moon. It is more than 8 km deep and extends ∼2500 km from the South Pole to the crater Aitken (e.g., Wilhelms, 1987; Spudis et al., 1994; Smith et al., 1997), which is located 15° south of the equator. According to lunar crustal thickness models (e.g., Neumann et al., 1996; Wieczorek and Phillips, 1998), the mean crustal thickness within the SPA basin is less than a half of that in the central region of the northern farside. We will discuss the effects of the large impact on mare formation from the viewpoint of the duration of mare volcanism by comparing the model ages for mare basalts in the FHT and SPA basin.
2. Technique of Age Determination
Crater counting is a well-established technique for deriving the relative and absolute ages of planetary surfaces. Based on the simple idea that older surfaces accumulate more craters, we can infer the relative and absolute ages by measuring the crater size-frequency distribution (CSFD) with image data. This technique has been described in detail in a number of papers (e.g., Arvidson et al., 1979; Neukum and Ivanov, 1994; Hiesinger et al., 2000, 2003; Hartmann and Neukum, 2001; Neukum et al., 2001; Wagner et al., 2002). Therefore we will just briefly present the procedure.
Determining the ages of photogeologic units with crater size-frequency measurements requires two procedures: (1) measuring the surface area of the unit and (2) measuring primary crater diameters within the unit (Hiesinger et al., 2000). In this study, we manually performed crater counts on the computer. We used images that are converted to stereographic projection with a resolution of 10 m/pixel at the projection center because the projection introduces little distortion in a narrow area. The diameters of small craters were calculated by multiplying a crater diameter in units of image pixels and the pixel resolution (10 m/pixel).
Age estimates from crater size-frequency measurements are sensitive to any contamination by secondary craters. It has been discussed in previous studies of lunar and Martian crater densities that the majority of small craters, not only those in clusters or rays, are secondary in origin, and that some of these secondary craters may not be obvious (e.g., Namiki and Honda, 2003; McEwen et al., 2005; Hirata and Nakamura, 2006; McEwen and Bierhaus, 2006; Dundas and McEwen, 2007). However, this argument has been challenged by various observations. The encounter rates of bolides with Earth’s atmosphere determined from satellite records and the small crater production function on the Moon appear to be in good agreement (e.g., Ivanov, 2006). Also, the size-frequency distributions of lunar and Martian craters appear invariant over long time scales (e.g., Neukum and Ivanov, 1994; Werner et al., 2009). Therefore, we believe that craters over a wide diameter range are primary, although the contribution of secondary craters to the population of small craters must continue to be studied. In this study, we eliminated obvious secondary craters based on their morphological characteristics (e.g., chain craters, elliptical craters, and clusters) (Melosh, 1989).
Model ages from crater counts are principally limited by statistical errors (Neukum et al., 2001). The statistical error of individual data points in our crater frequency measurements is mostly < 20% (1σ); the errors of ages based on the chronology model are ±0.02 Ga for > 3.5 Ga, 0.01 to 0.03 Ga for between 3.2 and 3.0 Ga, and < ±20% for < 3.0 Ga (Hiesinger et al., 2000). It must be noted that these are uncertainties of each data point in CSFD, and the variation from point to point is not represented by these errors.
The synchronous rotation of the Moon generates an apex-antapex asymmetry in cratering production rate (Morota and Furumoto, 2003; Morota et al., 2005; Le Feuvre and Wieczorek, 2008; Gallant et al., 2009). However, in the region investigated by our study, the effect of the apex-antapex cratering asymmetry on age determination is estimated to be less than 7% (Gallant et al., 2009), much smaller than the error due to statistical fluctuation. Therefore, we excluded the effect in this study.
Lunar geologic history is subdivided into five chronologic periods defined by impact events that formed the Nectaris basin, the Imbrium basin, the crater Eratosthenes, and the crater Copernicus. Various authors defined lunar chronologic systems in different ways (e.g., Neukum, 1983; Wilhelms, 1987; Neukum and Ivanov, 1994; Stöffler and Ryder, 2001). Estimates of the beginning of the Eratosthenian Period agree well among Neukum (1983), Wilhelms (1987), and Neukum and Ivanov (1994) at 3.2 Gyr, and Stöffler and Ryder (2001) at 3.15 Gyr. However, there are differences in the definitions for the beginnings of the Nectarian, Imbrian, and Copernican given in detail by Hiesinger et al. (2000, 2003) and Wagner et al. (2002). The cratering model ages for the major impact basins fall within the range of radiometric ages published by several investigators (see Neukum, 1983; Neukum and Ivanov, 1994; Hiesinger et al., 2000, 2003; Wagner et al., 2002). In this study, therefore, we adopt the chronologic system of Neukum (1983) and Neukum and Ivanov (1994), with Nectaris being 4.1±0.1 Gyr, the Imbrium basin being 3.91±0.1 Gyr old, and the Copernican Period beginning 1.5 Gyr ago.
3.1 Lacus Luxuriae
Mare deposit, Lacus Luxuriae is located at the center of the 600 km-diameter Freundlich-Sharonov basin (18.5°N, 175°E) and has a diameter of 50 km (Fig. 1). The mare deposit was previously mapped as Imbrian age (Stuart-Alexander, 1978).
Model ages of mare deposits.
Count area [km2]
N (1)a [km−2]
Model age [Ga]
(19° N, 176° E)
The CSFD for the northern unit also exhibits evidence of resurfacing events. For the lava flow exposed in the northern unit, the CSFD for D < 450 m gives a model age of ∼3.3 Ga, younger than that of the southern unit (Table 1). The result supports the interpretation that the higher albedo of the southern part is mainly due to impact mixing with highland materials. From the CSFD for D ∼ 650 m, the model age of the underlaid flow is estimated to be ∼3.7 Ga, which is equivalent to that of the flow under the southern unit. Therefore, we consider the lava flow under the northern unit to be the same as that under the southern unit. Furthermore, we note that the CSFD for 0.45 km ∼ D ∼ 0.6 km lies on the polynomial of 3.46 Ga, although the errors are significantly large. This result implies that the lava flow of 3.4–3.5 Ga exposed in the southern unit would spread under the northern unit. From the crater diameter-rim height relation (Pike, 1977), the thickness of the lava flow of ∼3.3 Ga is estimated to be 13–19 m, and that of 3.4–3.5 Ga is estimated to be 19–28 m.
Our results indicate that mare volcanism in Lacus Luxuriae began at least ∼3.7 Gyr ago and continued through the Late Imbrian Epoch, that is consistent with the previous mapping as Imbrian age (Stuart-Alexander, 1978).
Buys-Ballot, which lies just northwest of Lacus Luxuriae, is a 55 km-diameter Imbrian crater (Stuart-Alexander, 1978) or Nectarian crater (Wilhelms, 1987). The odd shape exhibits the distinctive signatures of a very low-angle impact: elongated pear-shaped plan (90 × 60 km), crater widening transverse to the inferred trajectory, and central peak ridge (Schultz et al., 1998) (Fig. 2). The floor of this crater is filled by mare basalt with iron content estimated to be 8–15 wt% and titanium content estimated to be 0–2 wt% from Clementine spectral data (Gillis and Spudis, 1998).
Campbell is a 220 km-diameter pre-Nectarian crater (Stuart-Alexander, 1978; Wilhelms, 1987). Mare basalt covers an area of 2400 km2 within the central western portion of the crater and was previously mapped as Imbrian age (Stuart-Alexander, 1978; Wilhelms, 1987). The basalt has low iron (10–14 wt% FeO) and low titanium (0.5–1.5 wt% TiO2) contents. Furthermore, the concentration of mafic material is constant and does not vary across the expanse of the mare (Gillis and Spudis, 1996, 1998).
Kohlschütter, which is located to the southeast of the Mare Moscoviense (Fig. 1), is a 53 km-diameter Nectarian crater (Stuart-Alexander, 1978; Wilhelms, 1987). The floor of the crater is partially covered by mare basalt. The mare deposit was previously classified as Imbrian in age (Stuart-Alexander, 1978).
4.1 Duration of mare volcanism in the FHT
The model ages of mare basalts investigated in our study range from 3.7 to 2.7 Gyr ago (i.e., from the Late Imbrian Epoch to the Eratosthenian Period). The oldest basalt was found in Lacus Luxuriae as a layer buried by later flows. In contrast, the youngest basalt occurs in Campbell. No evident correlations exist between the model ages and the topography, the gravity anomaly, and the sizes and ages of the craters or the basins filled by the mare basalts.
Previous studies of dark haloed craters and light plains revealed the presence of cryptomaria (i.e., maria that were buried by ejecta from large craters or basins) and interpreted them as evidence for ancient mare volcanism (e.g., Schultz and Spudis, 1978, 1983; Hawke and Bell, 1981; Bell and Hawke, 1984; Antonenko et al., 1995). Such ancient mare volcanism has been supported by radiometric analyses of rock samples returned from the lunar nearside (e.g., Taylor et al., 1983; Dasch et al., 1987; Nyquist et al., 2001) and lunar meteorites (Terada et al., 2007), which indicate ages of 4.2–4.35 Gyr for their basalt clasts. In the central northern region of the farside, the onset of mare volcanism is not well understood, even though our results indicate that mare volcanism began at least as early as 3.9 Gyr ago, for a total duration of ∼1.3 Gyr. However, the total duration in the region might be expanded to ∼1.7 Gyr, if the light plains that can be found as small patches in the FHT (Howard et al., 1974) are associated with cryptomaria.
4.2 Comparison with the SPA basin and the nearside
Figures 9(B) and 9(C) present histograms of model ages for mare deposits in the SPA basin (Haruyama et al., 2009) and on the nearside (Hiesinger et al., 2000, 2003, 2006) for comparison. We found that the shape of the frequency distribution of mare basalts in the FHT is very similar to that in the SPA basin; the histograms have a peak at ∼3.5 Gyr, and expand to ∼2.5 Gyr. However, it must be noted that some cryptomaria exist within the SPA basin (e.g., Pieters et al., 2001), implying that mare volcanism in the SPA basin may have started prior to that in the FHT, though the volumes of the cryptomare deposits are not so large.
The effects of large impacts on the thermal evolution of the mantle have been proposed as one mechanism for the formation of lunar basalts (e.g., Arkani-Hamed, 1973, 1974; Elkins-Tanton et al., 2004; Ghods and Arkani-Hamed, 2007). A recent version of the mechanism, related to the mantle convection triggered by impact-induced thermal perturbations (Ghods and Arkani-Hamed, 2004, 2007), requires that the SPA basin formation impact generates a substantial amount of melting in the mantle, which does not seem to be compatible with the minor amount of mare and cryptomare deposits filling this basin. Furthermore, the impact-induced convection model requires a long duration of mare volcanism for the SPA basin (Ghods and Arkani-Hamed, 2007). This is also incompatible with our result, which indicates no difference in the timing and the duration of mare volcanism within and outside the SPA basin. Thus, we concluded that the SPA basin formation impact had a minor effect on the formation of mare basalts in the region. It is probable that the basin simply provided a depression for magma generated by internal heating in early history to pond.
As presented by Haruyama et al. (2009), comparing model ages of mare basalts on the farside and those on the nearside indicates that the timing of the termination of mare volcanism differed between the farside (∼2.5 Ga) and the nearside (∼1.2 Ga). This difference might be related to the thicker crust (e.g., Head and Wilson, 1992) and/or a deficiency of heat-producing radioactive elements on the far-side (e.g., Jolliff et al., 2000). However, a more solid interpretation of the causes for the nearside-farside dichotomy in mare volcanism requires a clearer understanding of the ages, volumes, compositions of mare basalts, and relation to crustal structure. Such clarification will be possible with SELENE multispectral (Matsunaga et al., 2008; Ohtake et al., 2009), topography (Araki et al., 2009), and gravity (Namiki et al., 2009) data sets.
The new high-resolution images obtained by SELENE TC enable us to perform accurate crater size-frequency measurements in the mare deposits in the central region of the northern farside, which were previously undated. Our results indicated that the mare deposits in the region formed from 3.7 to 2.7 Gyr ago. From model ages for all mare deposits in the region investigated by both our study and previous studies (Haruyama et al., 2009; Morota et al., 2009), we found that mare volcanism in this region began at least as early as 3.9 Gyr ago, and continued until ∼2.6 Gyr ago. The comparison of model ages in the region and the SPA basin indicates the simultaneity of the mare volcanism in these regions. Therefore, we concluded that the SPA basin formation impact simply provided a depression for magma generated by internal heating in early history to pond rather than affecting the formation of mare basalts in the region.
We thank all the contributors to the SELENE (Kaguya) project and Lunar Imager/Spectrometer (LISM) working group for their efforts in development, operation, and data processing of SELENE and LISM. We are grateful to C. R. Chapman and R. Wagner for thoughtful and constructive comments in their review of this paper. We also thank J. Oberst for his helpful comments. This work was supported by the Japan Society for the Promotion of Science under a Grant-in-Aid for JSPS Fellows (20·9211: T. Morota), a Grant-in-Aid for Scientific Research (C) (20540416: J. Haruyama), and a Grant-in-Aid for Scientific Research (A) (19204045: H. Demura).
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