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A set of four two-dimensional plots containing the same data as in Figure 1: (a) band depth versus continuum ratio, (b) continuum ratio versus albedo, (c) albedo versus band depth, and (d) same as Figure 2c but with axes interchanged and data in the y axis reversed. This set of four plots will be the standard way maturity variations are displayed in this paper.

A set of four two-dimensional plots containing the same data as in Figure 1: (a) band depth versus continuum ratio, (b) continuum ratio versus albedo, (c) albedo versus band depth, and (d) same as Figure 2c but with axes interchanged and data in the y axis reversed. This set of four plots will be the standard way maturity variations are displayed in this paper.

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High spectral and spatial resolution data from the Moon Mineralogy Mapper (M3) instrument on Chandrayaan-1 are used to investigate in detail changes in the optical properties of lunar materials accompanying space weathering. Three spectral parameters were developed and used to quantify spectral effects commonly thought to be associated with increas...

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... craters are shown to show that results are con- sistent. Plots are the same configuration as in Figure 2. ...
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... of the difficulties associated with clearly depicting a three-dimensional data space in a two-dimensional plot, the combination of Figures 2a-2d will be used throughout the paper as a standard way to show maturity variations. Figure 2a plots band depth versus continuum ratio. Le Mouélic et al. [2002] used a plot similar to this to determine maturity trends for a region surrounding Tycho Crater. ...
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... soils should, in general, show significant variations in this type plot. Highland soils, however, should show significant variations in Figure 2b, which plots the continuum ratio versus albedo. Figure 2c is a plot of albedo versus band depth. ...
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... soils, however, should show significant variations in Figure 2b, which plots the continuum ratio versus albedo. Figure 2c is a plot of albedo versus band depth. Scatterplots of these two spectral properties are perhaps most familiar since they form the basis for the OMAT parameter defined by Lucey et al. [1995]. ...
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... our formulation is a summation of band strength relative to a continuum and the Clementine formulation is a ratio, higher numbers in our parameter indicate greater band depths, while in the Clementine ratio, lower numbers suggest stronger band depths in the Clementine ratio. Figures 2d is the same as Figure 2c but with the axes exchanged and the data in the y axis reversed to allow a more ready comparison to previous results such as those from analyses of Clem- entine UVVIS data [e.g., Lucey et al., 2000b]. ...
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... our formulation is a summation of band strength relative to a continuum and the Clementine formulation is a ratio, higher numbers in our parameter indicate greater band depths, while in the Clementine ratio, lower numbers suggest stronger band depths in the Clementine ratio. Figures 2d is the same as Figure 2c but with the axes exchanged and the data in the y axis reversed to allow a more ready comparison to previous results such as those from analyses of Clem- entine UVVIS data [e.g., Lucey et al., 2000b]. ...
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... Figure 3 shows the location of a Mare Serenitatis Crater plotted in Figure 2, along with a radial transect of representative spectra. A similar transect for South Ray Crater, the highlands crater whose maturity trends are illustrated in Figures 1 and 2, is shown in Figure 4. From inspection of Figures 3 and 4, the relation of trends shown in Figure 2 becomes clear. ...
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... Figure 3 shows the location of a Mare Serenitatis Crater plotted in Figure 2, along with a radial transect of representative spectra. A similar transect for South Ray Crater, the highlands crater whose maturity trends are illustrated in Figures 1 and 2, is shown in Figure 4. From inspection of Figures 3 and 4, the relation of trends shown in Figure 2 becomes clear. The trend for Mare Serenitatis, based on the behavior of this small, fresh crater, is that much of the variation in the three-parameter space is in the 1 mm band depth and the continuum, while the albedo variation is less significant. ...
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... Figures 5 and 6, data from two fresh craters are plotted to show that the data from different craters in the same region are consistent. The general similarity between trends in Figures 5 and 6 and those shown for Mare Serenitatis in Figure 2 confirms that optical maturity systematics expected of mare units are being captured by the M 3 data with the three parameters employed. ...
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... craters plotted in Figures 7 and 8 were taken from an area in the western farside high- lands surrounding Crater Timiryazev (147°W, 5°S). Craters containing relatively feldspathic material are plotted in Figure 7, whereas craters with more mafic regolith are plotted in Figure 8. Highlands materials with relatively feldspathic compositions, similar to those of South Ray Crater ejecta shown in Figure 2, exhibit little variation in band depth but significant variation in albedo. Continuum ratio variation is small in these craters but larger in mafic highlands craters (Figure 8). ...
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... these parameter spaces are appropriate for defining overall differences in maturity across a given ter- rain, our analysis of M 3 data shows that the use of simple parameter spaces often masks subtleties in maturity varia- tion that are revealed when three parameters are used to describe maturity variations. In Figure 2, trends for Mare Serenitatis appear essentially linear in albedo versus band depth space (Figure 2c), but the trend is shown to have a slightly curvilinear relationship in band depth versus con- tinuum ratio space (Figure 2a). Maturity trends for the Mare Humorum Crater ejecta show similar behavior in Figure 6, though to a lesser degree. ...
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... these parameter spaces are appropriate for defining overall differences in maturity across a given ter- rain, our analysis of M 3 data shows that the use of simple parameter spaces often masks subtleties in maturity varia- tion that are revealed when three parameters are used to describe maturity variations. In Figure 2, trends for Mare Serenitatis appear essentially linear in albedo versus band depth space (Figure 2c), but the trend is shown to have a slightly curvilinear relationship in band depth versus con- tinuum ratio space (Figure 2a). Maturity trends for the Mare Humorum Crater ejecta show similar behavior in Figure 6, though to a lesser degree. ...
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... these parameter spaces are appropriate for defining overall differences in maturity across a given ter- rain, our analysis of M 3 data shows that the use of simple parameter spaces often masks subtleties in maturity varia- tion that are revealed when three parameters are used to describe maturity variations. In Figure 2, trends for Mare Serenitatis appear essentially linear in albedo versus band depth space (Figure 2c), but the trend is shown to have a slightly curvilinear relationship in band depth versus con- tinuum ratio space (Figure 2a). Maturity trends for the Mare Humorum Crater ejecta show similar behavior in Figure 6, though to a lesser degree. ...
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... Another challenge that absolute maturity indices must overcome is that the spectral properties they are based on are Figure 8. Fresh crater data for three fresh craters in same region as in Figure 6 but for craters that have mafic absorption bands (i.e., are noritic). Plots are the same configuration as in Figure 2. often affected by factors other than maturity differences, most notably differences in composition. ...

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The Moon serves as an attic to the Earth’s treasure by preserving the volatile repository from the harsh space environment. The exposure of the lunar surface to the solar wind plasma results in the implantation of potential 3He into the top 1 mm of the regolith. The retention of the 3He primarily depends on the regional ilmenite content and maturation subject to the solar wind plasma supply. In the present research, an attempt is made to explore the influence of petrophysical properties of the regolith on the retained 3He using multisensor approach. The retention framework is improved by incorporating the associated effects of space weathering on the regolith materials, which are represented by spectral parameters. The integration of the spectral parameters, plasma flux, and ilmenite content leads to a novel hybrid variable that is directly compared with the in-situ 3He measurements at the Apollo and Luna landing sites. Considering the independence of the space weathering processes, the correlation analysis suggests that the predicted 3He contents are in close agreement with the actual abundance. However, all the weathering processes lead to the reduction of Fe2+ into the nanophase metallic iron particles, thereby interrelating to each other. The applicability of the weighted average linear combination is utilized to model the unknown inherent relationship between the weathering trends. Upon comparing with the in-situ 3He, the RMSE reduces to 1.17 ppb compared to the independent approach. The empirical relationship is applied to the Vallis Schroteri region, wherein the high 3He abundant regions emerge out to be pyroclastic deposits and localized hotspots near the primary rille and Agricola Mountains. It is also observed that the two dominant processes governing the abundance are attenuation of the mafic absorption band depths and reddening of the soil. However, a different scenario all together appears for the 3He abundance per unit area, wherein the soil chemistry proves to be a deciding factor. The spatial variability of the 3He abundant regolith is found to be aligned with the episodic space weathering events over the geological timescale, clearly indicated by the cyclic behaviour of the variogram trends. Moreover, the highly retained 3He content may be oriented at around 135º relative to other directions. The lower cutoff and width increases the spatial variability of the deposition. The retention of the 3He is found to be associated with the petrophysical properties of the soil. This is clearly illustrated by comparing the retrieved scattering mechanisms, dielectric content, and geotechnical variations. In the research, the utility of the radar backscatter is modelled as a function of incidence angle, dielectric constant and surface roughness. The sensitivity analysis is performed, which provides the bounding limits of the realistic surface parameters and radar configuration. This is fed into the multilayer perceptron neural network for performing the inversion based on multivariate regression. The inverted dielectric constant shows an RMSE of 0.26. The retrieval process is applied to the monostatic data of the landing sites, wherein the inverted values are in close agreement with the actual values. Upon testing the study site, the pyroclastic regoliths are associated with high dielectric constant and increased surface scattering mechanisms. The regolith is also characterized by lower void spaces between the grains and higher relative density. Due to the freshly formed microcraters, the excavation of the rocks from the interior lowers the penetration of the radar wave, thereby increasing the granular packing of the gardened regolith. As the dielectric contrast increases, the retention of the lower 3He ejecta regolith increases, attributing to the roughness variations. The observation is also aligned with the CPR. Moreover, the abundance is negatively correlated with the void ratio for shorter lag distances. On the contrary, the higher abundant pyroclastic regolith relates well with the surface scattering mechanisms associated with cyclicity. An opposition is also observed in this to the bistatic angle with a more significant exponential depth profile. Furthermore, retention modelling provides new insights into the potential mining operations for the lunar outposts. The study recommends deeper exploration of the pyroclastic regoliths, thereby contributing to the lunar mining and remote sensing paradigms.