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Basalt or Not? Near-infrared Spectra, Surface Mineralogical Estimates, and Meteorite Analogs for 33 Vp-type Asteroids

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Published 2018 June 14 © 2018. The American Astronomical Society. All rights reserved.
, , Citation Paul S. Hardersen et al 2018 AJ 156 11 DOI 10.3847/1538-3881/aac3d2

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1538-3881/156/1/11

Abstract

Investigations of the main asteroid belt and efforts to constrain that population's physical characteristics involve the daunting task of studying hundreds of thousands of small bodies. Taxonomic systems are routinely employed to study the large-scale nature of the asteroid belt because they utilize common observational parameters, but asteroid taxonomies only define broadly observable properties and are not compositionally diagnostic. This work builds upon the results of work by Hardersen et al., which has the goal of constraining the abundance and distribution of basaltic asteroids throughout the main asteroid belt. We report on the near-infrared (NIR: 0.7 to 2.5 μm) reflectance spectra, surface mineralogical characterizations, analysis of spectral band parameters, and meteorite analogs for 33 Vp asteroids. NIR reflectance spectroscopy is an effective remote sensing technique to detect most pyroxene group minerals, which are spectrally distinct with two very broad spectral absorptions at ∼0.9 and ∼1.9 μm. Combined with the results from Hardersen et al., we identify basaltic asteroids for ∼95% (39/41) of our inner-belt Vp sample, but only ∼25% (2/8) of the outer-belt Vp sample. Inner-belt basaltic asteroids are most likely associated with (4) Vesta and represent impact fragments ejected from previous collisions. Outer-belt Vp asteroids exhibit disparate spectral, mineralogical, and meteorite analog characteristics and likely originate from diverse parent bodies. The discovery of two additional likely basaltic asteroids provides additional evidence for an outer-belt basaltic asteroid population.

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1. Introduction

Of the many currently unanswered questions in the field of asteroid science, one significant puzzle involves the initial formation, abundance, disruption, and resultant distribution of basaltic asteroids in the main asteroid belt (1.8 au < a < 3.4 au). Formed in the early epoch of the solar system in the chaotic regime of planetesimals, giant planet migration, and mass ejection from the solar system, the basaltic asteroids remaining in the main asteroid belt today inform us of the thermal, chemical, and temporal characteristics of the first tens of millions of years of the solar system (Cameron 1995; Keil 2000; Warren 2011).

Basalt is an extrusive, volcanic igneous rock type that forms from the high-temperature melting of rocks and their resulting recrystallization (Klein & Hurlbut 1977). This is a very common rock type on terrestrial bodies including Earth, Earth's Moon, Mercury, Venus, Mars, and asteroids (Burns 1993). How do we know there should be basaltic material in the asteroid belt? The relatively large abundance of grouped and ungrouped iron meteorite types strongly suggests that many protoplanets chemically differentiated at high temperatures (Wasson 1990; Keil 2000). Individual bodies subject to compositional zoning into canonical crust, mantle, and core components, whether partially or fully differentiated, were later disrupted via collisions and became constituents of the solar system. However, previous researchers have noted the dearth of mantle (i.e., olivine) and basaltic NIR spectral signatures on asteroids in the present era, which could be attributed to mass loss from the solar system (Burbine et al. 1996; Sanchez et al. 2014; Brasil et al. 2017).

The terrestrial collection of basaltic achondrites themselves provides direct evidence of basalt and derivation from partial or complete planetary-scale melting (Mittlefehdlt et al. 1998; Grady 2000). The identification of the 26Al radionuclide heating mechanism, and to a lesser extent the T Tauri induction heating method, provides pathways for this heating to planetary melting temperatures (Herbert et al. 1991; Grimm & McSween 1993). Other types of achondrites, such as anomalous basaltic achondrites, acapulcoites, lodranites, iron meteorites (grouped and ungrouped), and pallasites, also highlight even broader and more variable examples of melting processes (Mittlefehdlt et al. 1998). Most of these achondrites, the Howardite–Eucrite–Diogenite (HED) suite, are thought to derive from (4) Vesta. However, some of these achondrites, such as NWA 1240 and NWA 4587 (among others), are ungrouped and exhibit anomalous oxygen isotope ratios different from the HED meteorites, which suggest origins from parent bodies distinct from (4) Vesta (Mittlefehdlt et al. 1998; Barrat et al. 2003; Connolly et al. 2007).

The presence of (4) Vesta in the main asteroid belt as the sole remaining intact, large basaltic asteroid is additional direct evidence of that heating event in the early solar system. Remote investigations of Vesta across several decades and in situ spacecraft studies have confirmed Vesta's geological character and its uniqueness within the solar system volume that encompasses the hundreds of thousands of known main-belt asteroids (McCord et al. 1970; Gaffey 1997; Reddy et al. 2012c; Russell et al. 2012).

Evidence of the remaining basaltic asteroid population beyond (4) Vesta lies with the "Vestoids," which are posited as ejected fragments from Vesta's surface (Hardersen et al. 2014, and references therein). These Vestoids are defined using dynamical, taxonomic, mineralogical, and/or meteoritic lines of reasoning, although most potential Vestoids are still dynamically and taxonomically classified as V-type asteroids (Tholen 1984; Zappala et al. 1995; Bus & Binzel 2002; Hasselmann et al. 2012; Nesvorny 2015).

In the outer asteroid belt beyond 2.5 au, the only confirmed basaltic asteroid is (1459) Magnya, which has a semimajor axis of ∼3.14 au, is taxonomically classified as a V-type asteroid, and is thought to be too far from (4) Vesta to derive from that parent body (Lazzaro et al. 2000). This asteroid also exhibits NIR spectral and mineralogical features that are consistent with a basaltic surface (Hardersen et al. 2004).

Beyond this evidence, though, our knowledge of main-belt basaltic asteroids gets decidedly murkier. Recent work has been attempting to better define the basalt that resides throughout the main belt (Vilas et al. 2000; Burbine et al. 2001; Kelley et al. 2003; Cochran et al. 2004; Duffard et al. 2006; Moskovitz et al. 2008a; Nesvorny et al. 2008; Duffard & Roig 2009; Lim et al. 2011; Mayne et al. 2011; Reddy et al. 2011; Hardersen et al. 2014, 2015; Leith et al. 2017). A larger abundance of V-type asteroids has been identified and classified, which includes a tantalizing collection of possible non-Vesta-related basaltic asteroids (Hasselmann et al. 2012; Mainzer et al. 2012). Increasing numbers of Vestoids are being characterized that have analogs within the HED suite of basaltic achondrites (Hardersen et al. 2014, 2015, and references therein). However, no other outer-belt basaltic asteroids have yet been identified.

The present work builds upon, and expands, the near-infrared (NIR: 0.7 to 2.5 μm) spectral and mineralogical characterization of the Vp taxonomic class of asteroids (Carvano et al. 2010), which began with the work of Hardersen et al. (2014, 2015). The primary goals of this research are to: (1) identify those inner-belt Vp asteroids that have a significant likelihood of having a basaltic surface composition and deriving from (4) Vesta (as Vestoids), (2) better constrain the abundance and distribution of outer-belt basaltic asteroids, and (3) test the predictive ability of the Vp taxonomic class to accurately identify basaltic asteroids.

The above goals will be accomplished by: (1) visually inspecting asteroid NIR spectra and identifying those that are consistent with NIR spectra of HED meteorites, (2) using a three-tiered test to determine those Vp asteroids that exhibit NIR spectral and mineralogical properties consistent with a basaltic mineralogy and HED meteorite analogs, (3) constraining the surface mineralogy and potential meteorite analogs for the non-basaltic Vp asteroids, and (4) combining the results from Hardersen et al. (2014, 2015) with this work to estimate the success rate of the Vp taxonomy in predicting a basaltic surface mineralogy and composition.

Testing for a basaltic mineralogy involves comparing the derived ∼0.9 μm (Band I) and ∼1.9 μm (Band II) spectral absorption features with those of the HED meteorites, testing the consistency of the plots of Band I versus band area ratio (BAR) of the Vp asteroids with the basaltic achondrites (Gaffey et al. 1993, 2002), using existing laboratory calibrations for pyroxene and basaltic achondrites to estimate average surface pyroxene chemistries, and comparing the results with pyroxene mineral chemistries of the HED meteorites (Gaffey et al. 2002; Burbine et al. 2009; Reddy et al. 2012a).

For those Vp asteroids that exhibit Band I and Band II absorptions but are not classified as basaltic via the testing methods described above, efforts will be made to determine whether the asteroids belong to a different taxonomy (e.g., S-type, M-type, etc.) and have an average surface composition that is consistent with different meteorite types. Vp asteroids with featureless NIR spectra will be considered for taxonomic reclassification and efforts to constrain the potential range of meteorite types will be made.

The predictive test of the Vp class is an important component of this work because this taxonomy uses an average five-color spectrum derived from Sloan Digital Sky Survey (SDSS) colors to define its asteroid taxonomic classes (Carvano et al. 2010). The connection between asteroid taxonomic classes, the parameters that define those classes, and the geological nature of asteroids is not direct nor guaranteed. Compositional suggestions from an asteroid taxonomy can only be made broadly and must be done with caution (Tholen 1984). Our sample of Vp asteroids also have NEOWISE-derived albedos that are broadly consistent with (4) Vesta (Tedesco et al. 2002; Masiero et al. 2011; Mainzer et al. 2016); together these provide the best indirect evidence of a likely basaltic nature for this taxonomic group of asteroids.

2. Vp Asteroid Taxonomy

The asteroid classification system of Carvano et al. (2010) is based on SDSS broadband filter observations of a relatively large number of asteroids (63,468), but with that useful and large number of taxonomic classifications come some unique characteristics. SDSS primarily obtains photometric data of stars, galaxies, and quasars, but the data have also been applied to study asteroids (Adelman-McCarthy et al. 2006). First, the five SDSS colors (u'g'r'i'z') are solar-corrected and used to create very low-resolution, five-element, visible wavelength spectra that are the primary criterion used to define the different asteroid taxonomic classes. Second, the median spectra that define a given taxonomic class (Figure 2 of Carvano et al. 2010) have associated limits on color gradient (i.e., spectral slope) that define the range of acceptability of observations that fit a given taxonomic class (Figure 1 of Carvano et al. 2010). The limits on color gradient are the largest for the Vp class for the (i – r) and (z – i) color indices (Carvano et al. 2010). In addition, the ranges of color gradient for the different classes exhibit some overlap, and Figure 2 from Carvano et al. (2010) shows that the Vp class overlaps with the Qp class and slightly with the Op class for the (z – i) color index.

Third, SDSS observations can be of poor quality and identified as such with low taxonomic probability scores or larger than average filter errors, single observations for an asteroid may be assigned to multiple taxonomic classes, and multiple observations of individual asteroids may potentially lead to the assignment of multiple classifications for the same asteroid (Carvano et al. 2010).

By comparison, the SDSS-based taxonomy of Roig & Gil-Hutton (2006) applied principal component analysis (PCA) to identify 499 V-type, and potentially basaltic, asteroids from the SDSS Moving Object Catalog. Roig & Gil-Hutton (2006) identify 17 V-type asteroids that were also classified in Hasselmann et al. (2012) and analyzed in Hardersen et al. (2014, 2015) and this work.

3. Connecting the Vp Taxonomy to Asteroid Basaltic Mineralogy

For the Vp taxonomy to be effective, there should be a direct connection between the primary measurable feature of the Vp taxonomy and that feature's ability to securely predict an asteroid with a primarily basaltic surface composition. In this case, the primary Vp taxonomic measurable is the deep absorption in the ∼0.9 μm spectral region based on the solar-corrected SDSS color magnitudes at the i' and z' filters, where the reflectance at the z' filter decreases more than in any other taxonomic class of Carvano et al. (2010). The median log reflectance spectrum of the Vp class is given in Figure 2 of Carvano et al. (2010), but it is not possible to strongly constrain the absolute depth (based on visual examination, we estimate a decrease in reflectance from the i' to z' filter of ∼20%). Also, the band minimum of this median absorption feature cannot be determined due to the long-wavelength cutoff of the central wavelength of the z' filter at 0.913 μm, although the z' band goes out to 1.123 μm (Fukujita et al. 1996; Carvano et al. 2010).

In addition, the absorption feature(s) for the Vp taxonomy should be caused by the major mafic silicate and spectrally active mineral(s) found in the HED and basaltic achondrite meteorites, which is low-Ca pyroxene (i.e., pigeonite) (Gaffey 1976; Rubin 1997; Mittlefehdlt et al. 1998). The other abundant mafic silicate mineral that is spectrally present in the ∼1 μm region is olivine (Burns 1993), as well as olivine–pyroxene mineral mixtures (Singer 1981; Cloutis et al. 1986; Gaffey et al. 1993). The presumption is that the Vp class with its very deep absorption is a proxy for the typically deep ∼0.9 μm low-Ca or orthopyroxene absorption seen in the NIR spectra of basaltic asteroids (Hardersen et al. 2014, 2015).

Another complication includes the inability of the low-resolution SDSS spectrum to capture the actual shape of an absorption feature in the ∼0.9 μm region. As different minerals and mineral mixtures may be spectrally present, the SDSS two-point spectrum at 0.763 and 0.913 μm (the i' and z' magnitudes) is unable to capture variations in band shape within this spectral interval and at wavelengths beyond the z' filter magnitude.

4. Data and Observations

The data set for this work includes 33 Vp asteroids that were observed between 2013 September and 2016 December. Table 1 lists orbital, physical, and albedo information for each asteroid in this work along with the 16 asteroids from Hardersen et al. (2014, 2015). Figure 1 plots the 49 Vp asteroids from this work and from Hardersen et al. (2014, 2015) as a function of orbital inclination versus semimajor axis (au). Twenty-five of the Vp asteroids in this work, and 41 Vp asteroids in Table 1, have semimajor axes <2.5 au, while eight Vp asteroids have semimajor axes >2.5 au. These two groups of Vp asteroids are called inner-belt and outer-belt basaltic asteroid candidates, respectively. All the asteroids in Table 1 have NEOWISE-derived effective diameters (Deff) < 11 km (Masiero et al. 2011; Mainzer et al. 2016) with a mean effective diameter of 4.872 km. Our target asteroids were also selected based on NEOWISE-derived geometric albedos (pv) that are generally consistent with (4) Vesta (pv = 0.4228, Tedesco et al. 2002), but span a range in pv from 0.178 to 0.554 with a mean value of 0.343.

Figure 1.

Figure 1. Orbital inclination of 49 Vp asteroids from this work and Hardersen et al. (2014, 2015) overlaid with the population of the main asteroid belt, plotted as a function of semimajor axis. Data on the main asteroid belt were obtained from the MPCORB data file at the IAU Minor Planet Center.

Standard image High-resolution image

Table 1.  Orbital Elements and Physical Data for 49 Vp Asteroids from This Work and Hardersen et al. (2014, 2015)

        NEOWISE NEOWISE NEOWISE
Asteroid a (au) e i (deg) Deff (km) pv pIR
(2168) Swope 2.452 0.154 4.745 8.205 ± 0.058 0.263 ± 0.011 0.459 ± 0.043
(3715) Stohl 2.315 0.099 5.935 4.913 ± 0.065 0.384 ± 0.068 0.509 ± 0.065
(3782) Celle 2.415 0.095 5.251 5.924 ± 0.23 0.503 ± 0.078 0.675 ± 0.141
(3849) Incidentia 2.475 0.048 5.775 5.798 ± 0.125 0.398 ± 0.041 0.475 ± 0.089
(4055) Magellan 1.820 0.326 23.344
(4900) Maymelou 2.378 0.130 5.932 4.654 ± 0.155 0.514 ± 0.046 0.772 ± 0.069
(5754) 1992 FR2 2.267 0.142 5.540 6.337 ± 0.078 0.277 ± 0.031 0.567 ± 0.093
(5952) Davemonet 2.270 0.112 4.064 4.861 ± 0.275 0.271 ± 0.055 0.812 ± 0.078
(7302) 1993 CQ 2.807 0.181 9.954 9.56 ± 0.51 0.262 ± 0.037 0.339 ± 0.038
(8271) Imai 2.410 0.209 10.413 5.783 ± 0.234 0.192 ± 0.028 0.288 ± 0.042
(9064) Johndavies 2.434 0.128 8.133 3.969 ± 0.33 0.407 ± 0.18 0.611 ± 0.145
(9223) Leifandersson 2.300 0.071 3.413 4.498 ± 0.176 0.381 ± 0.051 0.571 ± 0.077
(9368) Esashi 2.310 0.118 6.848 4.26 ± 0.164 0.466 ± 0.043 0.699 ± 0.065
(9531) Jean-Luc 2.235 0.187 5.816 4.176 ± 0.228 0.279 ± 0.05 0.418 ± 0.076
(10537) 1991 RY16 2.851 0.066 7.248 7.865 ± 0.269 0.313 ± 0.053 0.489 ± 0.039
(10666) Feldberg 2.223 0.058 5.919 3.978 ± 0.038 0.233 ± 0.02 0.35 ± 0.03
(11341) Babbage 2.381 0.056 7.358 4.404 ± 0.169 0.302 ± 0.044 0.452 ± 0.067
(11699) 1998 FL105 2.406 0.083 5.078 6.447 ± 0.172 0.245 ± 0.034 0.441 ± 0.045
(12073) Larimer 2.416 0.085 6.241 2.951 ± 0.227 0.456 ± 0.163 0.697 ± 0.242
(14390) 1990 QP10 3.243 0.108 6.583 10.767 ± 0.189 0.22 ± 0.057 0.33 ± 0.086
(15630) Disanti 2.326 0.115 5.461 3.548 ± 0.182 0.332 ± 0.027 0.546 ± 0.056
(16703) 1995 ER7 2.441 0.172 8.933 3.132 ± 0.729 0.544 ± 0.179 0.815 ± 0.268
(17035) Velichko 2.443 0.146 6.243 4.758 ± 0.314 0.283 ± 0.08 0.425 ± 0.12
(17480) 1991 PE10 2.788 0.177 8.685 4.301 ± 0.074 0.263 ± 0.065 0.394 ± 0.097
(19165) Nariyuki 2.291 0.074 7.791 3.464 ± 0.196 0.487 ± 0.099 0.731 ± 0.149
(19738) Callinger 2.282 0.185 7.736 3.272 ± 0.082 0.314 ± 0.056 0.472 ± 0.084
(20171) 1996 WC2 2.383 0.032 8.034 2.346 ± 0.602 0.508 ± 0.286 0.763 ± 0.249
(24014) 1999 RB118 2.560 0.190 11.967 6.513 ± 0.35 0.24 ± 0.053 0.36 ± 0.079
(25849) 2000 ET107 2.585 0.126 14.034 5.287 ± 0.171 0.276 ± 0.045 0.414 ± 0.067
(26417) Michaelgord 2.256 0.058 6.082 2.325 ± 0.557 0.472 ± 0.199 0.708 ± 0.237
(27025) 1998 QY77 2.292 0.058 6.307 2.007 ± 0.599 0.439 ± 0.159 0.658 ± 0.239
(34698) 2001 OD22 3.176 0.068 23.210 8.174 ± 0.23 0.383 ± 0.066 0.567 ± 0.122
(36118) 1999 RE135 2.709 0.035 4.797 4.998 ± 0.322 0.338 ± 0.077 0.508 ± 0.116
(3867) Shiretoko 2.351 0.107 6.275 5.345 ± 0.153 0.324 ± 0.058 0.487 ± 0.087
(5235) Jean-Loup 2.298 0.141 4.848 6.709 ± 0.109 0.36 ± 0.056 0.524 ± 0.164
(5560) Amytis 2.287 0.107 5.618 4.703 ± 0.041 0.29 ± 0.051 0.451 ± 0.09
(6331) 1992 FZ1 2.359 0.134 7.763 5.321 ± 0.101 0.473 ± 0.101 0.553 ± 0.115
(6976) Kanatsu 2.333 0.169 8.247 5.497 ± 0.116 0.307 ± 0.042 0.46 ± 0.064
(17469) 1991 BT 2.372 0.083 6.165 5.999 ± 0.173 0.258 ± 0.035 0.386 ± 0.052
(29796) 1999 CW77 2.344 0.075 7.868 4.851 ± 0.073 0.248 ± 0.062 0.392 ± 0.025
(30872) 1992 EM17 2.328 0.113 5.060 2.995 ± 0.102 0.455 ± 0.069 0.705 ± 0.108
(2011) Veteraniya 2.386 0.150 6.187 5.193 ± 0.646 0.463 ± 0.1 0.695 ± 0.15
(5875) Kuga 2.379 0.049 6.469 7.465 ± 0.144 0.381 ± 0.119 0.503 ± 0.084
(8149) Ruff 2.324 0.142 6.584 4.091 ± 0.132 0.554 ± 0.116 0.831 ± 0.133
(9147) Kourakuen 2.191 0.106 5.816 4.854 ± 0.166 0.248 ± 0.071 0.473 ± 0.084
(9553) Colas 2.199 0.117 1.920 3.791 ± 0.141 0.178 ± 0.029 0.266 ± 0.044
(15237) 1988 RL6 2.392 0.149 7.326 2.557 ± 0.52 0.47 ± 0.254 0.704 ± 0.19
(31414) Rotarysusa 2.260 0.153 5.376 2.547 ± 0.179 0.282 ± 0.056 0.423 ± 0.084
(32940) 1995 UW4 2.189 0.136 8.111 3.351 ± 0.07 0.273 ± 0.09 0.41 ± 0.135

Note.  Deff = effective diameter, pv = visible albedo, pIR = infrared albedo (Masiero et al. 2011). The first group of asteroids is from this work, the second and third groups from Hardersen et al. (2014, 2015), respectively.

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All observations and NIR spectra were obtained using the NASA Infrared Telescope Facility (IRTF) on Maunakea, Hawai'i, either on-site or remotely. Data were acquired with the SpeX medium-resolution spectrograph and imager using a consistent observational protocol and with consistent instrumental settings (Rayner et al. 2003, 2004). Remote observations with SpeX are identical to on-site observing using a VNC client for remote observers. Observations for each asteroid during a night include ∼10–20 spectra of the asteroid and 20 spectra of a late F-/G-type main-sequence extinction star that is near the asteroid (i.e., within ∼3°). The extinction star observations bracket the asteroid observations and encompass an airmass range greater than that of the asteroid. Extinction stars are primarily observed to perform spectral telluric corrections during data reduction. About 20–30 spectra of a single solar analog star are also obtained each night, which are used for spectral slope corrections. Flat field images and argon (Ar) spectra are obtained to correct for variations in array pixel sensitivity and spectral wavelength calibration. All SpeX data were obtained using the low-resolution (R ∼ 95) prism mode (0.7 to 2.5 μm) with a 0farcs8 wide slit and an open dichroic to obtain the largest spectral range of data possible.

Table 2 describes the respective observational circumstances for the 33 Vp asteroids in this paper. All Vp asteroids were observed with apparent magnitudes within the range from 16.0 to 18.0, cumulative integration times from 400 to 3000 s, and the total number of spectra acquired for each asteroid ranging from 4 to 20. Most observing runs experienced photometric, clear weather conditions or only the minor presence of cirrus clouds and low relative humidity. Exceptions include the observing runs of 2015 June 16 UT, which experienced cirrus across the sky during the entire night and moderate relative humidity of ∼54% late in the observing run; 2015 June 17 UT, which experienced moderate-to-high values of relative humidity from 48% to 74% and cirrus throughout the sky at the beginning of the night; and 2015 December 11 UT, which experienced poor atmospheric seeing (∼1farcs5 to 2farcs0).

Table 2.  Observational Circumstances for 33 Vp-type Asteroids in this Work

Asteroid Observation Date (UT) Apparent V Magnitude Phase Angle (deg) Total Integration Time (s) Total Spectra Extinction Star Solar Analog Star
(2168) Swope 2015 Jan 16 17.49 16.4 1600 8 BD+02 2405 SAO 120107
(2168) Swope 2015 Jan 17 17.47 16.2 1400 7 BD+02 2405 SAO 120107
(2168) Swope 2015 Jan 19 17.43 15.7 2400 12 BD+02 2405 SAO 120107
(3715) Stohl 2015 Jan 15 16.19 3.4 2000 10 HD 65523 SAO 120107
(3715) Stohl 2015 Jan 19 16.10 2.0 1600 8 HD 65523 SAO 120107
(3782) Celle 2015 Jan 15 17.16 25.2 800 4 HD 116667 SAO 120107
(3782) Celle 2015 Jun 16 16.45 24.7 2000 10 SAO 157732 SAO 120107
(3782) Celle 2015 Jun 22 16.55 25.7 2000 10 SAO 157732 SAO 120107
(3849) Incidentia 2015 Jan 16 17.15 21.8 1600 8 HD 104800 SAO 120107
(3849) Incidentia 2015 Jan 17 17.13 21.6 1800 9 HD 104800 SAO 120107
(4055) Magellan 2015 Jun 16 16.02 47.9 2000 10 SAO 69926 SAO 120107
(4900) Maymelou 2016 Jan 26 17.46 8.9 2000 10 HD 50060 SAO 93936
(5754) 1992 FR2 2015 Jan 19 16.47 11.5 1000 5 HIP 28216 SAO 120107
(5952) Davemonet 2015 Jun 16 16.74 17.9 3000 15 SAO 189480 SAO 120107
(7302) 1993 CQ 2016 Jan 26 16.48 19.2 2000 10 HD 30047 SAO 93936
(8271) Imai 2015 Jun 16 16.14 7.3 2000 10 SAO 141903 SAO 120107
(8271) Imai 2015 Jun 17 16.13 7.2 2000 10 SAO 141903 SAO 120107
(9064) Johndavies 2016 Jan 26 17.15 10.2 2400 12 HD 87776 SAO 93936
(9223) Leifandersson 2015 Jun 16 16.18 8.8 2000 10 SAO 162034 SAO 120107
(9223) Leifandersson 2015 Jun 17 16.15 8.3 2000 10 SAO 162034 SAO 120107
(9368) Esashi 2015 Jun 17 17.12 11.4 2000 10 HD 186163 SAO 120107
(9531) Jean-Luc 2016 Jan 26 17.09 6.3 2800 14 HD 62043 SAO 93936
(10537) 1991 RY16 2016 Dec 29 17.04 7.7 1600 8 SAO 76855 SAO 93936
(10666) Feldberg 2015 Jan 16 16.14 4.5 1600 8 HD 68017 SAO 120107
(10666) Feldberg 2015 Jan 19 16.14 4.5 1400 7 HD 68017 SAO 120107
(11341) Babbage 2016 Jan 26 16.70 13.5 2400 12 HD 93653 SAO 93936
(11699) 1998 FL105 2014 Sep 4 16.40 5.1 1200 10 SAO 128229 HD 28099
(12073) Larimer 2014 Sep 2 17.04 5.5 480 4 SAO 128164 HD 28099
(14390) 1990 QP10 2013 Sep 13 17.17 15.0 2400 20 SAO 189379 SAO 93936
(15630) Disanti 2016 Dec 29 16.45 5.7 2000 10 SAO 77406 SAO 93936
(16703) 1995 ER7 2015 Jun 16 16.91 18.9 1400 7 SAO 144197 SAO 120107
(17035) Velichko 2015 Jun 22 17.08 11.8 1600 8 SAO 159838 SAO 120107
(17480) 1991 PE10 2016 Jan 2 17.58 7.3 2600 13 SAO 58270
(19165) Nariyuki 2015 Jan 19 16.71 14.8 2000 10 BD+36 1276 SAO 120107
(19738) Callinger 2015 Jun 17 17.12 14.8 2400 12 SAO 188854 SAO 120107
(20171) 1996 WC2 2016 Jan 26 17.67 6.9 1600 8 HD 82069 SAO 93936
(24014) 1999 RB118 2015 Jun 17 17.35 8.2 2000 10 SAO 188103 SAO 120107
(25849) 2000 ET107 2016 Jan 2 17.48 13.7 2000 10 HD 27947
(26417) Michaelgord 2016 Dec 29 17.59 2.8 2800 14 SAO 78788 SAO 93936
(27025) 1998 QY77 2006 Dec 21 17.36 4.5 2800 14 HD 261730 SAO 93936
(34698) 2001 OD22 2015 Jan 15 17.34 10.3 2000 10 TYC 4894-595-1 SAO 120107
(34698) 2001 OD22 2015 Jan 16 17.32 10.0 1200 6 TYC 4894-595-1 SAO 120107
(36118) 1999 RE135 2015 Jan 15 17.43 9.9 1200 6 HD 82906B SAO 120107
(36118) 1999 RE135 2015 Jan 19 17.33 8.3 2000 10 HD 82906B SAO 120107

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5. Data Reduction

Production of average, normalized NIR reflectance spectra occurs using a combination of IDL-based Spextool software (Cushing et al. 2004) and Microsoft Excel. Spextool is specifically designed for IRTF SpeX data and is utilized in the first phase of the data reduction process. Tasks that are accomplished with Spextool include removal of the background sky signal, telluric corrections, channel shifting, flat field and wavelength calibrations, and spectral averaging routines. Successful background sky subtraction is linked to an observational approach that obtains spectra in an ABBAABBAAB... sequence at the two slit positions, A and B, which allows AB spectral pairs to be subtracted to efficiently remove the background sky flux contribution. Channel shifting is also important to ensure that all spectra properly overlay and cover the same pixels in each spectrum. Not performing this function introduces unwanted noise into the resulting average spectrum.

Telluric corrections are the most important part of the data reduction because correcting for the atmospheric water vapor absorptions at ∼1.4 and ∼1.9 μm is vital for producing high-quality, interpretable average spectra. This task is also linked to a specific observational strategy where the extinction star for a given asteroid is observed prior to, and after, the asteroid observations. This sequence is performed to ensure that the airmass range of the star exceeds and encompasses the airmass range of the asteroid, which allows effective empirical modeling of the night sky and removal of the telluric contribution.

Once background subtraction, telluric corrections, and channel shifting have been successfully accomplished, an averaging of the asteroid spectra relative to the extinction star is performed. The same process is then performed for the solar analog star. These two average spectra are then converted to text files and exported into Microsoft Excel. For the solar analog star spectrum relative to the extinction star, any remnant telluric features are removed and replaced by a smoothed spectrum. This is a standard procedure and is justified based on the lack of broad absorption features in stellar spectra. The resulting average unnormalized asteroid spectrum is described in the following qualitative equation:

Average Asteroid/Solar Analog is the final unnormalized average asteroid spectrum, (Asteroid/Ext. Star) is the average asteroid spectrum relative to the extinction star, and (Solar Analog/Ext. Star) is the average solar analog star spectrum relative to the extinction star. The average asteroid reflectance spectrum is then normalized to a flux of 1.0 at 1.5 μm, which is a wavelength position along the overall continuum and away from any spectral absorption features.

6. Data Analysis

The results of the data reduction effort are shown in Figure 2, which displays 44 average NIR spectra for the 33 Vp asteroids in this work. The asteroids are listed numerically based on their number designation and by the UT date of observation. Each asteroid has at least one average spectrum in Figure 2, but several asteroids were observed on multiple nights and the spectra from all nights are shown for comparison.

Figure 2.
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Figure 2.
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Figure 2.

Figure 2. Average NIR reflectance spectra for 33 Vp asteroids in this work.

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Determining whether a Vp-classified asteroid is likely to have a basaltic nature is evaluated initially on a visual examination of each asteroid's reflectance spectrum and later, as appropriate, by more rigorous analysis of spectral band parameters. Asteroids with an average reflectance spectrum that do not display spectral absorption features are identified as not being basaltic due to the lack of the two prominent and deep pyroxene spectral absorption bands at ∼0.9 and ∼1.9 μm present in NIR spectra of basaltic achondrites and the NIR spectrum of (4) Vesta (Gaffey 1997; Reddy 2011). Those asteroids that display spectral absorption features, but absorptions that are significantly different from those of pyroxene (i.e., weaker absorptions, differences in spectral band shapes, etc.) are flagged as potentially non-basaltic, but are subjected to analysis of band parameters. Finally, those asteroids displaying the canonical pyroxene absorptions are subjected to analysis of band parameters. For the latter two cases, the three-tiered test is applied to determine the basaltic affinity for each asteroid.

Analysis of spectral band parameters is a technique to extract, measure, and quantify the different absorption features of an NIR spectrum. This technique can potentially be applied to all asteroid NIR spectra with measurable spectral absorption features but is most useful for well-calibrated spectra dominated by pyroxene, olivine, or both (Burns 1993; Gaffey et al. 1993; Hardersen et al. 2014, 2015; Sanchez et al. 2014). Calibrations of laboratory pyroxene and basaltic achondrites are the most relevant calibrations for this work because pyroxene is the dominant mafic silicate component in basaltic achondrites and the HED clan (Mittlefehdlt et al. 1998).

It is also important to note that Type B pyroxenes (orthopyroxenes, low-Ca clinopyroxenes) are the relevant types of pyroxenes for basaltic achondrites and display both primary absorption features, unlike the high-Ca Type A pyroxenes (generally along the diopside–hedenbergite trend in the pyroxene quadrilateral) that often include only the ∼0.9 μm absorption (Adams 1974; Schade et al. 2004). A calibration of mineral chemistry does not exist for high-Ca Type A clinopyroxenes, although Schade et al. (2004) suggest that a possible association may exist between the 1.15 μm feature in the pyroxene M1 coordination site and Fe content.

The primary spectral band parameters that are quantified include absorption band centers, band areas, and BARs. An absorption band center is the minimum reflectance of a continuum-removed absorption feature. This is produced by creating a linear continuum across the absorption, meeting at the local maximum on each side of the absorption. A ratio of the linear continuum to the absorption feature produces the continuum-removed feature, which removes the effect of any positive or negative slope in this region of the NIR spectrum. The continuum-removed absorption can then be directly linked to pyroxene mineral chemistries (Burns 1993). Analysis of Type B pyroxenes with a range of mineral chemistries has shown that band centers systematically shift to longer wavelengths with higher Fe and Ca content (Adams 1974; Cloutis et al. 1986; Burns 1993).

Band areas are then calculated from the areas of individual, continuum-removed absorptions. The BAR is the ratio of the area of the ∼1.9 μm (i.e., Band II) feature to the area of the ∼0.9 μm (i.e., Band I) feature. A calibration of Band I versus BAR exists for olivine–orthopyroxene mixtures (Cloutis et al. 1986; Gaffey et al. 2002), where larger BAR values indicate a greater relative pyroxene abundance compared to olivine, with basaltic achondrites typically exhibiting BAR values >1.5 (Cloutis et al. 1986; Gaffey et al. 2002). Absorption band depth is another commonly measured spectral band parameter, which represents the percentage decrease in reflectance of an absorption relative to the isolated continuum (e.g., band depth (%) = 1 – X  = Y, where X is the relative reflectance value of the minimum reflectance of the absorption band and Y is the continuum-removed absorption band depth represented as a percentage). Band depths are not diagnostic of mineralogy and can vary based on the asteroid's phase angle during observations, space weathering on an asteroid's surface, or a surface metal component (Britt & Pieters 1988; Blewett et al. 2015; Cloutis et al. 1990, 2015; Sanchez et al. 2014).

Our analysis of band parameters utilizes a set of MATLAB routines (Reddy et al. 2012a) and the IDL-based Spectral Analysis Routine for Asteroids (SARA) (Lindsay et al. 2015). While both sets of code extract the same band parameters, the MATLAB method is semi-automated and the SARA method is completely automated. The only difference in the methods is that we used the SARA routines with the default Band II long-wavelength limit of 2.50 μm, while we manually chose the Band II long-wavelength limit in MATLAB for each asteroid based on the furthest extent of the measurable absorption.

Table 3 displays the MATLAB, SARA, and average MATLAB/SARA-derived and temperature-corrected band centers. To determine band centers, polynomial fits with different orders were used to measure the lower region of each absorption feature. The semi-automated MATLAB routines (Hardersen et al. 2014, 2015, and references therein) utilize third- and fourth-order polynomials to obtain at least 20 measurements of the lower third of each absorption feature. The results for both orders were consistent across our set of measurements. The automated SARA routines produce third-, fourth-, and fifth-order polynomial fits, but we only used the fourth- and fifth-order fits because the third-order fits often fit the data poorly and were not consistent with the higher-order fits. Multiple runs of each NIR spectrum through SARA were also conducted to ensure consistency of derived band centers and BARs. The results in Table 3 show that the Band I averages derived from the MATLAB and SARA routines are very consistent. The results for the Band II averages show larger deviations, which is primarily attributable to greater scatter in the data in this spectral region due to an inherently lower signal-to-noise ratio (SNR) at longer wavelengths in the NIR spectra.

Table 3.  Absorption Band Centers for the Vp Asteroids in This Work That Exhibit Absorptions Across the Spectral Range 0.7 to 2.5 μm

  MATLAB MATLAB SARA SARA Average Average
  (μm) (μm) (μm) (μm) (μm) (μm)
Asteroid Band I center Band II center Band I center Band II center Band I center Band II center
(2168) Swope 0.947 ± 0.003 1.953 ± 0.006 0.943 1.960 0.945 ± 0.003 1.957 ± 0.006
(2168) Swope 0.948 ± 0.003 1.973 ± 0.009 0.943 1.976 0.946 ± 0.003 1.973 ± 0.009
(2168) Swope 0.942 ± 0.003 1.953 ± 0.010 0.939 1.957 0.941 ± 0.003 1.955 ± 0.010
(3715) Stohl 0.943 ± 0.003 1.973 ± 0.004 0.942 1.982 0.943 ± 0.003 1.978 ± 0.005
(3715) Stohl 0.940 ± 0.003 1.973 ± 0.008 0.931 1.978 0.940 ± 0.003 1.976 ± 0.008
(3782) Celle 0.935 ± 0.003 1.966 ± 0.012 0.935 1.959 0.935 ± 0.003 1.963 ± 0.012
(3782) Celle 0.934 ± 0.003 1.974 ± 0.009 0.933 1.963 0.934 ± 0.003 1.968 ± 0.009
(3782) Celle 0.936 ± 0.003 1.956 ± 0.006 0.933 1.972 0.935 ± 0.003 1.963 ± 0.008
(3782) Celle (Moskovitz) 0.939 ± 0.003 1.930 ± 0.010 0.939 ± 0.003 1.930 ± 0.010
(3782) Celle (Moskovitz) 0.944 ± 0.003 1.952 ± 0.004 0.944 ± 0.003 1.952 ± 0.004
(3849) Incidentia 0.951 ± 0.003 1.992 ± 0.007 0.947 2.006 0.949 ± 0.003 1.999 ± 0.007
(3849) Incidentia 0.951 ± 0.003 1.987 ± 0.009 0.949 2.003 0.950 ± 0.003 1.995 ± 0.009
(4055) Magellan 0.929 ± 0.003 1.935 ± 0.004 0.936 1.950 0.933 ± 0.003 1.943 ± 0.008
(4900) Maymelou 0.942 ± 0.003 1.975 ± 0.008 0.940 1.984 0.941 ± 0.003 1.980 ± 0.008
(5754) 1992 FR2 0.934 ± 0.003 1.951 ± 0.005 0.934 1.964 0.934 ± 0.003 1.958 ± 0.007
(5952) Davemonet 0.941 ± 0.003 1.978 ± 0.007 0.940 1.987 0.941 ± 0.003 1.983 ± 0.007
(7302) 1993 CQ 0.963 ± 0.005 1.930 ± 0.012 0.964 1.940 0.964 ± 0.003 1.935 ± 0.012
(8271) Imai 0.937 ± 0.003 1.944 ± 0.008 0.935 1.953 0.936 ± 0.003 1.949 ± 0.008
(8271) Imai 0.938 ± 0.003 1.947 ± 0.006 0.936 1.950 0.937 ± 0.003 1.949 ± 0.006
(9064) Johndavies 0.953 ± 0.003 2.005 ± 0.013 0.947 2.035 0.950 ± 0.003 2.020 ± 0.015
(9223) Leifandersson 0.944 ± 0.003 1.980 ± 0.005 0.943 2.004 0.944 ± 0.003 1.992 ± 0.012
(9223) Leifandersson 0.950 ± 0.003 1.970 ± 0.003 0.949 1.989 0.950 ± 0.003 1.980 ± 0.010
(9368) Esashi 0.956 ± 0.003 2.013 ± 0.011 0.954 2.014 0.955 ± 0.003 2.014 ± 0.011
(9531) Jean-Luc 0.949 ± 0.004 1.953 ± 0.008 0.942 1.972 0.946 ± 0.004 1.963 ± 0.010
(10537) 1991 RY16 0.959 ± 0.003 1.945 ± 0.020 0.984 1.981 0.976 ± 0.009 1.961 ± 0.020
(10537) 1991 RY16 (Moskovitz) 0.960 ± 0.002 1.933 ± 0.005 0.960 ± 0.002 1.933 ± 0.005
(10666) Feldberg 0.939 ± 0.003 1.955 ± 0.007 0.937 1.963 0.938 ± 0.003 1.959 ± 0.007
(10666) Feldberg 0.941 ± 0.003 1.956 ± 0.007 0.937 1.970 0.939 ± 0.003 1.963 ± 0.007
(11341) Babbage 0.947 ± 0.003 2.002 ± 0.008 0.944 2.009 0.946 ± 0.003 2.006 ± 0.008
(11699) 1998 FL105
(12073) Larimer 0.927 ± 0.003 1.940 ± 0.010 0.925 1.969 0.926 ± 0.003 1.955 ± 0.015
(14390) 1990 QP10 0.962 ± 0.003 1.984 ± 0.018 0.969 1.977 0.966 ± 0.004 1.981 ± 0.018
(15630) Disanti 0.939 ± 0.003 1.988 ± 0.007 0.936 1.991 0.938 ± 0.003 1.990 ± 0.007
(16703) 1995 ER7 0.943 ± 0.003 1.981 ± 0.020 0.941 1.987 0.942 ± 0.003 1.984 ± 0.020
(17480) 1991 PE10 0.948 ± 0.006 0.940 1.941 0.944 ± 0.006 1.941
(17035) Velichko 0.933 ± 0.003 1.925 ± 0.010 0.933 1.946 0.933 ± 0.003 1.936 ± 0.011
(19165) Nariyuki 0.945 ± 0.003 1.983 ± 0.007 0.941 1.988 0.943 ± 0.003 1.986 ± 0.007
(19738) Callinger 0.942 ± 0.003 2.006 ± 0.013 0.938 2.051 0.940 ± 0.003 2.029 ± 0.023
(20171) 1996 WC2 0.939 ± 0.003 1.978 ± 0.018 0.937 1.975 0.938 ± 0.003 1.977 ± 0.018
(24014) 1999 RB118 0.998 ± 0.005 1.037 1.018 ± 0.020
(25849) 2000 ET107 0.913 ± 0.015 0.913 ± 0.015
(26417) Michaelgord
(27025) 1998 QY77 0.922 ± 0.003 1.906 ± 0.017 0.926 1.892 0.924 ± 0.003 1.899 ± 0.017
(34698) 2001 OD22 0.928 ± 0.003 1.910 ± 0.010 0.923 1.940 0.926 ± 0.003 1.925 ± 0.015
(34698) 2001 OD22 0.933 ± 0.004 1.907 ± 0.008 0.928 1.921 0.931 ± 0.004 1.914 ± 0.010
(36118) 1999 RE135 0.955 ± 0.003 1.946 ± 0.014 0.954 1.969 0.955 ± 0.003 1.958 ± 0.012
(36118) 1999 RE135 0.950 ± 0.003 1.950 ± 0.011 0.948 1.952 0.949 ± 0.003 1.951 ± 0.011

Note. Band centers are temperature-corrected and display the MATLAB, SARA, and average results. MATLAB results for NIR spectra of (3782) Celle and (10537) 1991 RY16 from Moskovitz et al. (2008b, 2010), Moskovitz (2011) are shown for comparison.

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The HED band center data in Figures 3 and 4 were measured using the same approach as in this work (and Hardersen et al. 2014, 2015) while also using very similar routines. Reddy et al. (2012b) used a Python code to measure the HED band center data that is very similar to the MATLAB code used by this work, but is more automated than the MATLAB code.

Figure 3.

Figure 3. Band I vs. Band II center plot for the inner-belt Vp asteroids in this work. The 16 Group 1 asteroids plot directly on the HED meteorite data in the plot while the eight Group 2 asteroids plot slightly above the data for the HED meteorites. Both groups of asteroids exhibit average surface pyroxene chemistries consistent with the HED meteorites.

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Figure 4.

Figure 4. Band I vs. Band II plot for the outer-belt basaltic asteroid candidates in this work. Also included is a plot of band center-derived data from an NIR spectrum of (10537) 1991 RY16 from Moskovitz et al. (2008a).

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Temperature corrections from Reddy et al. (2012b) are applied to both the Band I and Band II centers, with the largest corrections applied to the latter. MATLAB band centers are averages of ∼40 measurements and SARA results are averages of three runs to ensure repeatability and consistency of the results. Band center errors encompass the largest deviations that exist among the MATLAB- and SARA-derived values and exceed the 1σ standard deviations of both the individual average MATLAB and SARA results.

Table 4 displays the resulting average asteroid surface pyroxene chemistries using those of Gaffey et al. (2002) and Burbine et al. (2009), and the average chemistries derived from both calibrations. Table 4 also includes the average BAR values obtained from an average of the MATLAB and SARA results.

Table 4.  Band Area Ratios and Average Surface Pyroxene Chemistries for Pyroxene-bearing Asteroids in this Paper

  Gaffey et al. (2002) Burbine et al. (2009) Overall Average Surface  
Asteroid Avg. Pyroxene Chemistry Avg. Pyroxene Chemistry Pyroxene Chemistry BAR
(2168) Swope Wo15Fs40 Wo11Fs46 Wo13Fs43 2.402 ± 0.245
(2168) Swope Wo15Fs41 Wo12Fs48 Wo14Fs44 2.253 ± 0.107
(2168) Swope Wo13Fs40 Wo10Fs44 Wo12Fs42 2.406 ± 0.146
(3715) Stohl Wo14Fs41 Wo12Fs47 Wo13Fs44 2.414 ± 0.101
(3715) Stohl Wo13Fs41 Wo11Fs45 Wo12Fs43 2.252 ± 0.132
(3782) Celle Wo11Fs43 Wo10Fs41 Wo11Fs42 2.117 ± 0.020
(3782) Celle Wo10Fs44 Wo9Fs42 Wo10Fs43 2.402 ± 0.240
(3782) Celle Wo11Fs43 Wo10Fs41 Wo11Fs42 2.318 ± 0.034
(3782) Celle (Moskovitz) Wo12Fs38 Wo8Fs40 Wo10Fs39 3.350 ± 0.062
(3782) Celle (Moskovitz) Wo15Fs40 Wo10Fs45 Wo13Fs43 3.040 ± 0.076
(3849) Incidentia Wo17Fs42 Wo13Fs52 Wo15Fs47 2.029 ± 0.117
(3849) Incidentia Wo17Fs42 Wo14Fs52 Wo16Fs47 2.079 ± 0.088
(4055) Magellan Wo10Fs37 Wo8Fs39 Wo9Fs38 2.135 ± 0.014
(4900) Maymelou Wo13Fs41 Wo11Fs46 Wo12Fs44 2.450 ± 0.117
(5754) 1992 FR2 Wo10Fs41 Wo9Fs41 Wo10Fs41 2.346 ± 0.091
(5952) Davemonet Wo13Fs41 Wo11Fs47 Wo12Fs44 2.491 ± 0.309
(7302) 1993 CQ 0.859 ± 0.140
(8271) Imai Wo11Fs39 Wo9Fs41 Wo10Fs40 2.558 ± 0.088
(8271) Imai Wo12Fs39 Wo9Fs41 Wo11Fs40 2.246 ± 0.059
(9064) Johndavies Wo17Fs43 Wo15Fs55 Wo16Fs49 2.122 ± 0.122
(9223) Leifandersson Wo15Fs42 Wo12Fs49 Wo14Fs46 2.205 ± 0.197
(9223) Leifandersson Wo17Fs41 Wo13Fs51 Wo15Fs46 2.075 ± 0.075
(9368) Esashi Wo19Fs43 Wo16Fs57 Wo18Fs49 1.990 ± 0.017
(9531) Jean-Luc Wo15Fs40 Wo12Fs47 Wo14Fs44 2.025 ± 0.031
(10537) 1991 RY16 0.992 ± 0.017
(10537) 1991 RY16 (Moskovitz) 1.020 ± 0.033
(10666) Feldberg Wo12Fs40 Wo10Fs43 Wo11Fs42 2.205 ± 0.105
(10666) Feldberg Wo12Fs40 Wo10Fs44 Wo11Fs42 2.137 ± 0.105
(11341) Babbage Wo15Fs43 Wo13Fs52 Wo14Fs48 2.137 ± 0.089
(11699) 1998 FL105
(12073) Larimer Wo7Fs41 Wo7Fs36 Wo7Fs39 2.897 ± 0.163
(14390) 1990 QP10 0.895 ± 0.015
(15630) Disanti Wo12Fs42 Wo11Fs46 Wo12Fs44 2.468 ± 0.092
(16703) 1995 ER7 Wo14Fs41 Wo12Fs47 Wo13Fs44 2.715 ± 0.465
(17480) 1991 PE10 0.397 ± NA
(17035) Velichko Wo10Fs36 Wo8Fs38 Wo9Fs37 2.731 ± 0.401
(19165) Nariyuki Wo14Fs41 Wo12Fs48 Wo13Fs45 2.144 ± 0.128
(19738) Callinger Wo13Fs44 Wo13Fs51 Wo13Fs48 2.286 ± 0.031
(20171) 1996 WC2 Wo12Fs41 Wo11Fs45 Wo12Fs43 3.069 ± 0.459
(24014) 1999 RB118 1.267 ± 0.009
(25849) 2000 ET107 1.783 ± 0.135
(26417) Michaelgord
(27025) 1998 QY77 Wo6Fs26 Wo4Fs30 Wo5Fs28 2.530 ± 0.050
(34698) 2001 OD22 Wo7Fs33 Wo6Fs33 Wo7Fs33 1.742 ± 0.192
(34698) 2001 OD22 Wo9Fs30 Wo7Fs35 Wo8Fs33 1.363 ± 0.205
(36118) 1999 RE135 Wo19Fs40 Wo15Fs39 Wo17Fs40 2.251 ± 0.581
(36118) 1999 RE135 Wo13Fs52 Wo12Fs46 Wo13Fs49 1.539 ± 0.109

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7. Interpretations and Results

Of the 33 Vp asteroids in this work, 25 asteroids reside in the inner main belt with a < 2.5 au while eight asteroids have a > 2.5 au. Two of the inner-belt Vp asteroids, (11699) 1998 FL105 and (26417) Michaelgord, are potentially not basaltic asteroids and do not have analogs with the HED meteorites. The remaining 23 inner-belt Vp asteroids are consistent with a basaltic composition and have likely analogs with the HED meteorites.

The eight outer-belt Vp asteroids include two asteroids, (34698) 2001 OD22 and (36118) 1999 RE135, that have a likely basaltic composition. The other six Vp asteroids are not consistent with a basaltic composition and display significant spectral variability and likely surface compositional and meteorite analog diversity.

8. Inner-belt Vp Asteroids

The group of inner-belt Vp asteroids in this work are mostly consistent with a basaltic composition and associations with specific HED meteorite analogs. We distinguish three subgroups among these inner-belt Vp asteroids: (1) those asteroids that display uniformly consistent spectral and mineralogical evidence in support of a basaltic surface composition and association with an HED meteorite type, (2) those asteroids also exhibiting consistent evidence for a basaltic composition and HED meteorite analogs with the exception of a difference in Band I versus Band II positions in Figure 3, and (3) those asteroids that are spectrally and mineralogically inconsistent with a basaltic composition. The second group of asteroids is consistent with other Vp asteroids from Hardersen et al. (2014, 2015) that also lie just off the Band I versus Band II plot, but still exhibit an HED meteorite analog.

8.1. Group 1

Fifteen of the Vp asteroids in our sample exhibit spectral, band parameter, and mineralogical evidence that these asteroids have a basaltic surface composition. Spectrally, Figure 2 displays the NIR spectra of these asteroids that exhibit the two deep pyroxene absorptions at ∼0.9 and ∼1.9 μm with continuum-removed Band I and Band II depths that range from 35%–52% and 32%–55%, respectively. Plotting the continuum-removed Band I and Band II centers in Figure 3 places all the inner-belt Vp asteroids on the plot with the data for the HED meteorite suite of howardites, diogenites, and eucrites. Figure 4 is a band–band plot for the outer-belt Vp asteroids in this work. Figure 5 shows that all Group 1 asteroids lie on the Band I versus BAR plot in the rectangular region designated for basaltic achondrites or with larger BAR values that are beyond the bounds of that region.

Figure 5.

Figure 5. Plot of Band I center vs. BAR for the Vp asteroids in this work. The rectangular region encloses band parameter space for basaltic achondrites (BA) and represents asteroids with surfaces that are dominated by pyroxene group minerals and are consistent with a basaltic composition. The labels S(I) through S(VII) are taken from Gaffey et al. (1993).

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Using the band center data in the laboratory pyroxene calibration of Gaffey et al. (2002) and the laboratory HED meteorite calibration of Burbine et al. (2009), and averaging the results, each asteroid was tested to determine whether it had an association with a specific type of HED meteorite. Three Vp asteroids [(9064) Johndavies, (11341) Babbage, (19738) Callinger] produced average surface pyroxene chemistries consistent with the eucrites. Only one asteroid, (27025) 1998 QY77, has a surface mineralogy consistent with the diogenites. Three asteroids [(4055) Magellan, (5754) 1992 FR2, (12073) Larimer] are consistent with a howardite interpretation. One asteroid, (17035) Velichko, has a likely howardite composition that may be enriched in a diogenite component while seven asteroids [(3782) Celle, (4900) Maymelou, (5952) Davemonet, (15630) Disanti, (16703) 1995 ER7, (19165) Nariyuki, (20171) 1996 WC2) are consistent with a howardite interpretation with a possible eucrite enrichment.

8.2. Group 2

This group of asteroids is very similar to the Group 1 asteroids with the sole difference being that these asteroids lie just above the Band I versus Band II HED meteorite data in Figure 3. This slight offset in position in Figure 3, however, does not affect the resulting interpretations for these asteroids. The HED data in Figure 3 do not encompass the entire range of measured HED band center data, which extend out to ∼0.98 μm for Band I (Figure 4, Cloutis et al. 2013). The asteroid Band I positions may also suggest a slight enrichment in an olivine or high-Ca clinopyroxene component to the average surface composition (Hardersen et al. 2014), but not enough of an enrichment to lead to a significant non-basaltic surface composition.

For this group, three asteroids exhibit average surface pyroxene chemistries consistent with eucrites [(3849) Incidentia, (9223) Leifandersson, (9368) Esashi]; one asteroid, (8271) Imai, is consistent with a howardite interpretation; and four asteroids are consistent with a howardite interpretation with a possibly enhanced eucrite component [(2168) Swope, (3715) Stohl, (9531) Jean-Luc, (10666) Feldberg].

8.3. Group 3

Only two inner-belt Vp asteroids are completely inconsistent with a basaltic surface composition: (11699) 1998 FL105 and (26417) Michaelgord. Both asteroids display a featureless NIR spectrum in Figure 2 with (11699) 1998 FL105 displaying a relatively steep, spectrally red slope with increasing reflectance from ∼0.7 to 1.8 μm, followed by a flattening of the spectrum beyond 1.8 μm. The weak absorptions at ∼1.4 and ∼1.9 μm in the NIR spectrum of (11699) 1998 FL105 are likely telluric. (26417) Michaelgord displays a much shallower increase in reflectance across the same spectral range but is also spectrally featureless. However, Jasmin et al. (2013) report an NIR spectrum and analysis for (11699) 1998 FL105 that are consistent with a basaltic surface composition. Verification of the basaltic nature of (11699) 1998 FL105 will require additional observations, but our results should be taken as provisional, pending verification of the presence of rotational variations in the asteroid's NIR spectra.

Both asteroids are members of the Vesta dynamical family (Zappala et al. 1995; Nesvorny 2015) and are classified as Vp asteroids with no variability in classification (Carvano et al. 2010). (11699) 1998 FL105 has a Vp classification based on one SDSS observation, a classification probability score of 89%, and an SDSS z' filter mean error (0.008) that is below the average error at the z' filter for all SDSS z' filter observations for the asteroids in this work (0.015). The NEOWISE geometric albedo, pv, for this asteroid is 0.245 ± 0.034 (Masiero et al. 2011). Additional NIR spectra of (11699) 1998 FL105 should be obtained to confirm our results.

For (26417) Michaelgord, there are two SDSS observations, both with Vp classifications, probability scores of 11% and 64%, and with both observations being flagged as "BAD." From Hasselmann et al. (2012), a "BAD" flag defines at least one derived magnitude having an uncertainty above the third quartile for the observation associated with the assigned classification. The mean SDSS z' filter errors for the two observations for (26417) Michaelgord are 0.024 and 0.014, which are near, or larger than, the mean SDSS z' filter error for all the asteroids in this work (0.015). The NEOWISE geometric albedo, pv, for (26417) Michaelgord is 0.472 ± 0.199. Additional NIR spectra of this asteroid should also be obtained to confirm our findings.

9. Outer-belt Vp Asteroids

Eight of the asteroids in this work have semimajor axes that place them beyond the mean motion resonance at 2.5 au and are considered "outer main belt" asteroids unlikely to be fragments from (4) Vesta (Lazzaro et al. 2000). Their semimajor axes are quite disparate and range from ∼2.56 au for (24014) 1999 RB118 to ∼3.24 au for (14390) 1990 QP10. For reference, the only previously identified basaltic asteroid in the outer main belt, (1459) Magnya, has a semimajor axis of ∼3.14 au. Three asteroids have been classified into different families: (17480) 1991 PE10 is a member of the Ceres dynamical family (Zappala et al. 1995), (25849) 2000 ET107 is a member of the Maria or Maria/Renate family (Nesvorny 2015; Mothe'-Diniz et al. 2012), and (34698) 2001 OD22 is a member of the Alauda family (Nesvorny 2015) and a member of the C4 high-inclination asteroid family (i ∼ 23fdg2, Gil-Hutton 2007). The remaining outer-belt Vp asteroids, (7302) 1993 CQ, (10537) 1991 RY16, (14390) 1990 QP10, (24014) 1999 RB118, and (36118) 1999 RE135, have not been assigned to any family thus far. This evidence suggests that these asteroids are probably unrelated to each other and derive from different parent bodies.

Six of these asteroids are classified as Vp asteroids, but two are classified as SV asteroids [(17480) 1991 PE10, (25849) 2000 ET107] (Hasselmann et al. 2012). Both latter asteroids are based on one SDSS observation and both have a "BAD" flag associated with the taxonomic classification. (17480) 1991 PE10 has a taxonomic probability score of 10% and (25849) 2000 ET107 has a taxonomic probability score of 8% (Hasselmann et al. 2012). (10537) 1991 RY16 has taxonomic probability scores of 47% and 89% based on two SDSS observations, but no "BAD" flag designations (Hasselmann et al. 2012). (14390) 1990 QP10 has a Vp classification based on two SDSS observations with taxonomic probability scores of 8% and 6%, respectively, both with "BAD" flag markers (Hasselmann et al. 2012). The Vp classification for (34698) 2001 OD22 is based on one SDSS observation with a taxonomic probability score of 14% and marked as "BAD" (Hasselmann et al. 2012). Finally, the Vp classification for (36118) 1999 RE135 is based on one SDSS observation, and has a taxonomic probability score of 11% and a "BAD" flag rating (Hasselmann et al. 2012).

Visually, the NIR spectra of most outer-belt basaltic asteroid candidates are markedly different from the NIR spectra of asteroids that are consistent with a basaltic surface composition. The absorption features of the ∼0.9 and ∼1.9 μm absorptions for these asteroids, if they are present, exhibit different spectral band shapes and depths that indicate differences from primary pyroxene absorption features. While the Band I and Band II continuum-removed absorption band depths for likely basaltic asteroids range from 31% to 52% and 31% to 46%, respectively, the band depths for the outer-belt Vp asteroids range from 11% to 53% and 9% to 30%, respectively. A Band II depth for (17480) 1991 PE10 could not be measured due to the weakness of the feature and the noisiness of that region of the spectrum.8

(34698) 2001 OD22 and (36118) 1999 RE135 are the only two outer-belt Vp asteroids in our sample that are both spectrally similar to, and consistent with, a basaltic surface composition. For (34698) 2001 OD22, Band I and II centers lie on or slightly above the plot in Figure 3, and the derived average surface pyroxene chemistries suggest that this asteroid has a howardite-like composition (Wo8Fs33) possibly enriched with a diogenite component. While the BAR (1.742) for one NIR spectrum is consistent with a basaltic achondrite analog, the other BAR (1.363) is more consistent with the S(VI) asteroids (Gaffey et al. 1993). Potential meteorite analogs for the S(VI) group include lodranites, winonanites/IAB irons, and siderophyres (Gaffey et al. 1993). The BAR variations suggest the intriguing possibility of surface compositional variations with rotation but require further observations for confirmation.

For (36118) 1999 RE135, plots of Band I and Band II for both nights of data are marginally above the HED trend line in Figure 4. BAR values ranging from ∼1.5 to ∼2.25, along with the range of average surface pyroxene chemistries (∼Fs40–49), are consistent with a howardite or eucrite interpretation. As discussed with the Group 2 asteroids, band data that lie only marginally above the HED trend line may have some additional olivine or clinopyroxene within the overall surface composition, but can still be consistent with an HED meteorite analog.

Five of the asteroids [(7302), (10537), (14390), (17480), (24014)] exhibit Band I and Band II absorptions, but only one asteroid, (17480) 1991 PE10, has a potential meteorite analog. Band parameters for (17480) 1991 PE10 suggest a possible H/L-chondrite analog from the ordinary chondrite calibration of Dunn et al. (2010); however, the ordinary chondrite calibration of Gaffey et al. (2002) fails for all three ordinary chondrite types. The remaining asteroids with Band I and II absorptions fail the ordinary chondrite calibration tests of both Gaffey et al. (2002) and Dunn et al. (2010). Regardless, it is very likely that these asteroids exhibit some combination of mafic silicate minerals on their surfaces (i.e., olivine, low- and/or high-Ca pyroxene) based on the presence of these absorption features and their Band I and Band II center values. Those asteroids that lie above the olivine–orthopyroxene trend line in Figure 4, with the exception of (36118) 1999 RE135, have relatively large amounts of olivine or clinopyroxene present on their surfaces, which excludes them from classification as likely basaltic asteroids.

Jasmin et al. (2013) reported an NIR spectrum for (7302) 1993 CQ that is very similar to our spectrum in Figure 2. Their reported band parameters (Band I: 0.958 μm; Band II: 1.914 μm; BAR: 0.566) are broadly consistent with our results, although our reported band centers and BAR values are marginally larger. Jasmin et al. (2013) suggested an ordinary chondrite meteorite analog for (7302) 1993 CQ. Our two results are consistent in that (7302) 1993 CQ is inconsistent with a basaltic surface composition.

(25849) 2000 ET107 is spectrally unique among these Vp asteroids because only weak Band I and (possibly) Band II absorption features are present in the NIR spectrum. The Band I center at ∼0.91 μm is consistent with a surface dominated by low-Fe orthopyroxenes and possibly metal due to the overall redness of the spectrum. These spectral and band parameter characteristics are consistent with many of the M-/X-type asteroids analyzed by Hardersen et al. (2011). Interpretations suggested by Hardersen et al. (2011) for asteroids with similar spectral features include residual mantle material overlying disrupted Fe cores of differentiated parent bodies, analogs to the CB-/CH-chondrites, mesosiderites, and silicate-bearing iron meteorites.

10. Investigating Vp Taxonomic Misclassifications

To further attempt to understand the reasons for the apparent misclassifications of some of the Vp asteroids in our sample, we compared the positions of the SDSS i' and z' filter wavelengths (0.763 and 0.913 μm, respectively: Fukujita et al. 1996; Carvano et al. 2010) on the NIR spectra of the asteroids from this work that display the ∼0.9 μm absorption feature. For the Vp asteroids identified as basaltic, the i' filter wavelength was uniformly positioned at or near the short-wavelength local reflectance maximum of the ∼0.9 μm absorption. The SDSS z' filter wavelength was also uniformly positioned at or near the minimum absorption of the ∼0.9 μm feature.

For the asteroids in this work identified as non-basaltic and having a ∼0.9 μm absorption, the positions of the SDSS i' and z' filter wavelengths also reasonably mirrored the results for the basaltic asteroids above. Exceptions include (14390) 1990 QP10, where the absorption extends to shorter wavelengths than the i' filter wavelength, and (24014) 1999 RB118, where the position of the SDSS z' filter wavelength is somewhat shortward of the band minimum position.

Overall, the choice of central wavelength positions for the SDSS i' and z' filters seems very well suited to capture the short-wavelength local reflectance band maximum and band minimum for asteroids with a primarily surface pyroxene mineral signature. Asteroids with weaker Band I depths and with different surface mineral abundances are also captured in the Vp taxonomy with this method, which may be due to larger than average SDSS filter noise and errors, as well as the relatively large ranges in (i – r) and (z – i) color gradients for the Vp asteroids. The cause of the apparent misclassifications for (11699) 1998 FL105 and (26417) Michaelgord is unknown but should be pursued with additional NIR spectral observations.

11. Conclusions

Based on the results from this work and the work of Hardersen et al. (2014, 2015) for 49 potentially basaltic asteroids, we can conclude the following:

  • 1.  
    For the 41 inner-belt Vp asteroids in our sample, 39 of them exhibit NIR spectra, absorption features, derived spectral band parameters (band centers, BAR, band depths), and derived average surface mineralogies that are consistent with a basaltic interpretation with likely HED meteorite analogs. This represents an ∼95% success rate of the Vp taxonomy in predicting a basaltic surface composition.
  • 2.  
    The two inner-belt Vp asteroids that are potentially not basaltic, (11699) 1998 FL105 and (26417) Michaelgord, are spectrally featureless in the NIR. There is no evidence from Hasselmann et al. (2012) and the SDSS data (Carvano et al. 2010) of excessive noise or errors in the data used to determine the Vp classification for (11699) 1998 FL105. By comparison, (26417) Michaelgord does exhibit the presence of noisy SDSS z' filter data that may have contributed to the misclassification. Jasmin et al. (2013) report a basaltic NIR spectrum and analysis for (1699) 1998 FL105 that suggests a basaltic surface composition. Additional NIR spectra for this asteroid are necessary to confirm our result or to provide evidence for rotational spectral variations.
  • 3.  
    Only two outer-belt Vp asteroids in our sample, (34698) 2001 OD22 and (36118) 1999 RE135, are suggestive of basaltic surface compositions and an HED meteorite analog. Variations in the derived BAR values for (34698) 2001 OD22 suggest the possibility of surface compositional variability, which requires confirmation via additional observations.
  • 4.  
    Two outer-belt asteroids with an SV classification, (17480) 1991 PE10 and (25849) 2000 ET107, do not have a basaltic surface composition, and exhibit relatively high SDSS z' filter magnitude errors and taxonomic classifications with low probability. (17480) 1991 PE10 has a potential H- or L-chondrite meteorite analog. (25849) 2000 ET107 has a weak Band I feature suggestive of the presence of low-Fe orthopyroxene.
  • 5.  
    The remaining four outer-belt Vp asteroids display NIR absorption features of varying shapes and band depths indicative of the presence of one or more mafic silicate surface minerals and possibly metal. However, no meteorite analogs have yet been identified for these asteroids.
  • 6.  
    Results from Leith et al. (2017) identify (10537) 1991 RY16 and (14390) 1990 QP10 as Unclassified Objects (their Table 6) and different from the V-type asteroids in this work, which is consistent with our results.
  • 7.  
    Thus far, the Vp taxonomy has predicted a basaltic surface composition for only two out of eight asteroids (∼25%). The sample of outer-belt asteroids generally exhibit greater classification uncertainties via their low taxonomic probability scores, the presence of "BAD" flags indicating larger SDSS magnitude uncertainties, and generally larger SDSS z' filter errors compared to the average for all the asteroids in this work.
  • 8.  
    Fourteen Vp asteroids with likely basaltic surface compositions and identified HED meteorite analogs from this work and Hardersen et al. (2014, 2015) display either a low taxonomic probability score or a "BAD" flag indication. These indications of potentially noisy or low-quality data did not translate into a non-basaltic composition for these asteroids. By comparison, there are two Vp asteroids [(7302) 1993 CQ, (11699) 1998 FL105] that were not identified with a basaltic surface composition, but also did not display any indications of low-quality or noisy data.
  • 9.  
    Among the outer-belt basaltic asteroid candidates, seven of the eight asteroids displayed the "BAD" flag, had low taxonomic probability scores, or had relatively high SDSS z' filter errors. Thirteen of the 41 inner-belt basaltic asteroid candidates displayed similar indications of low-quality data, but this did not translate into interpretations of a non-basaltic surface composition. One reason for this is that many of the asteroids were observed multiple times, with most of the observations indicating good quality data. Regardless, a smaller percentage of inner-belt asteroids in our sample of Vp asteroids displayed questionable data as compared to the outer-belt asteroid sample.
  • 10.  
    While our results suggest that many outer-belt Vp asteroids may be misclassified and do not typically indicate the presence of basaltic material, the identification of two additional likely basaltic asteroids in the outer main belt indicates that a larger basaltic population likely exists and should be characterized. Accurately characterizing this population could affect the nature, extent, and distribution of the heating event in the early solar system (Herbert et al. 1991; Grimm & McSween 1993).

The authors acknowledge and thank the leadership, staff, and telescope operators at the NASA Infrared Telescope Facility (IRTF), as well as the program officers and scientists at NASA Headquarters, for giving us the opportunity to conduct this research program and observe at the IRTF with the SpeX instrument, both on-site and remotely.

The authors thank Tom Burbine for the valuable and insightful comments that improved this manuscript.

P.S.H. thanks Sean Lindsay for access to the SARA software, and guidance on operation of the program, for a portion of our data analysis work. P.S.H. also thanks the co-authors of this paper for their contributions.

P.S.H. also sincerely thanks everyone who has been genuinely supportive of his personal and professional journey and transition away from the Upper Midwest to the warmer, more enjoyable and productive environs of Arizona. May fortune favor the foolish.

Work by P.S.H. and V.R. is supported by NASA Planetary Astronomy Program Grant NNX14AJ37G (PI: Hardersen).

Footnotes

  • Note that the Band II depth of ∼22% for (31414) Rotarysusa in Hardersen et al. (2015) is incorrect and is more accurately shown to be ∼42%.

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10.3847/1538-3881/aac3d2