Imaging Spectrometry and Metamorphic Processes

Edward F. Duke and Patrick K. Kozak
Presented at the Ninth AVIRIS Earth Science and Applications Workshop, February 23-25, 2000,
Jet Propulsion Laboratory, Pasadena, CA

Introduction

Metamorphism of rocks in the earth's crust is characterized by progressive changes in mineral assemblages, mineral proportions, and mineral chemistry in response to changes in temperature, pressure, or composition of coexisting fluids. Spectral features in the 0.4-2.5 mm wavelength range of modern imaging spectrometers serve to distinguish among important metamorphic minerals and, in some cases, to record the extent of temperature-sensitive cation exchange reactions. It is possible, therefore, to apply imaging spectrometer data to map the zonation of metamorphic minerals as a function of past thermal and compositional gradients in the crust.

The present study is part of a broader investigation, which examines the use of laboratory, field, airborne, and spaceborne spectroscopic measurements to achieve a better understanding of metamorphic conditions and metamorphic fluid flow. The emphasis is on field and laboratory visible and near infrared reflectance spectra, combined with high spectral resolution remote sensing imagery from NASA's Airborne Visible and Infrared Imaging Spectrometer (AVIRIS) and other imaging spectrometer data. In order to illustrate these applications, this paper presents AVIRIS images which delineate metamorphic zones resulting from contact metamorphism of siliceous dolomite near Ubehebe Peak, Death Valley National Park, California.

Geology and Metamorphism

The Ubehebe Peak contact aureole is located in Death Valley National Park, California, at the southern end of the Last Chance Mountains. Figure 1 shows the location of the Ubehebe Peak contact aureole on a Landsat Thematic Mapper satellite image and on a generalized geologic map (Streitz and Stinson, 1977). The ground track of NASA's Airborne Visible and Infrared Imaging Spectrometer (AVIRIS) flight f96050t01p02_r04 is shown by dotted yellow lines on the satellite image with the rectangular box outlining the specific AVIRIS scene used in this study.

Figure 1. Regional setting.
Figure 1. Regional setting. - click on figure for larger image

 

Figure 2 is a more detailed geologic map of the Ubehebe Peak contact aureole. Intrusion of Middle Jurassic (173 Ma) quartz monzonite into steeply dipping siliceous dolomites produced a zone of contact metamorphism that is well exposed for a distance of at least 2.5 km north of the intrusive (Roselle, 1997; Roselle et al., 1999). Metamorphic effects are most pronounced in the Silurian Hidden Valley dolomite and Devonian Lost Burro formation, which are predominantly quartz-poor dolomite, with subordinate dolomitic sandstone and limestone layers. Approximately 5 km north of the intrusive body at Ubehebe Peak (see Fig. 1), another intrusive is exposed. Although no detailed study of metamorphism has been conducted in that area, the intrusive is known to have caused local contact metamorphic effects and mineralization (McAllister, 1955, 1956; Burchfiel, 1969). AVIRIS imagery in subsequent figures covers most of the area of Figure 2, with the exception of the western margin of map, but the AVIRIS imagery extends roughly 3 km further north.

Figure 2. Geologic map of the Ubehebe Peak contact aureole showing isograds
Figure 2. Geologic map of the Ubehebe Peak contact aureole showing isograds (Roselle et al., 1999). - click on figure for larger image

 

Metamorphic phase relations in the siliceous dolomites in the Ubehebe Peak aureole can be approximated by the simple CaO-MgO-SiO2 (H2O-CO2) compositional system. Roselle (1997) divided the aureole into an unmetamorphosed zone followed sequentially by tremolite, forsterite, and periclase zones toward the intrusive contact. A restricted wollastonite zone was mapped in calcitic marbles in the southwestern part of the aureole (Fig. 2), but not discussed further here. Prograde reactions at the tremolite, forsterite, and periclase isograds can be approximated as follows (see Table 1 for mineral compositions and abbreviations):

5 Dol + 8 Qtz + H2O = Tr + 3 Cal + 7 CO2                        (1)
Tr + 11 Dol = 8 Fo + 13 Cal + 9 CO2 + H2O                      (2)
Dol = Per + Cal + CO2                                                    (3)

Retrograde effects are significant, including partial alteration of forsterite to serpentine and complete replacement of periclase by brucite according to the following reactions:

Fo + Cal + 2 H2O + CO2 = Srp + Dol                                (4)
Per + H2O = Brc                                                             (5)

Roselle et al. (1999) estimated the pressure of metamorphism at 1.4-1.7 kbar based on stratigraphic reconstructions. Temperatures of metamorphism, based on calcite-dolomite geothermometry, ranged from <300°C in the unmetamorphosed rocks to 665°C at the periclase isograd.

Table 1. Mineral abbreviations and chemical formulae
Dol = dolomite, CaMg(CO3)2
Cal = calcite, CaCO3
Qtz = quartz, SiO2
Tr = tremolite, Ca2Mg5Si8O22(OH)2
Fo = forsterite, Mg2SiO4
Per = periclase, MgO
Srp = serpentine, Mg3Si2O5(OH)4
Brc = brucite, Mg(OH)2

Figure 3 shows visible and near infrared reflectance spectra of important minerals in the CaO-MgO-SiO2 (H2O-CO2) compositional system along with the metamorphic reactions that explain the prograde or retrograde production of these minerals. Mineral spectra in Figure 3 are from the U.S. Geological Survey spectral library (Clark et al., 1993).

Figure 3. General spectral features of minerals in metamorphosed siliceous dolomites.
Figure 3. General spectral features of minerals in metamorphosed siliceous dolomites.  - click on figure for larger image

 

Remote Sensing Data and Processing Methods

Airborne Visible and Infrared Imaging Spectrometer (AVIRIS) data used in this study were acquired May 3, 1996 (flight f96050t01p02_r04) and obtained for this project from NASA's Jet Propulsion Laboratory. The AVIRIS instrument is flown on an ER-2 at an altitude of 60,000 feet giving a spatial resolution of 20 m. The spectral data comprise 224 contiguous bands covering the wavelength range from 0.37 to 2.51 mm with bandwidth varying between approximately 8.5 and 11 nm. AVIRIS calibrated radiance values were corrected for atmospheric effects and converted to apparent reflectance using the ATREM procedure (Gao and Goetz, 1990). Additional surface calibration of ATREM reflectance values was performed using an Empirical Line calibration method; field and laboratory reflectance spectra from sites within the image were used to determine gains and offsets for the image spectra (Kruse et al., 1990). In this study, laboratory spectra of samples from the quartz monzonite and the Racetrack Playa were used to set the dark and bright signals, respectively.

AVIRIS apparent surface reflectance images were analyzed using ENVI software. A Minimum Noise Fraction transformation was employed to determine a reduced set of noise-free spectral bands. Using the reduced set of bands, the Pixel Purity Index (Boardman et al., 1995) was used to identify spectrally pure pixels in the image. Spectra from these pixels were compared with field and laboratory spectra and with spectra from the U.S. Geological Survey spectral library (Clark et al., 1993) to derive a set of image-based spectral endmembers. Based on these endmembers, mineral maps of the distribution and relative abundance of important metamorphic minerals were generated using four different algorithms: Spectral Angle Mapper (SAM, Boardman and Kruse, 1994), Mixture Tuned Matched Filtering (MTMF, Boardman et al., 1995), Spectral Feature Fitting (Clark et al., 1990), and Linear Spectral Unmixing (LSU, Boardman, 1989). Examples of MTMF, LSU, and SAM results are presented in this paper.

In order to establish ground-truth data, over 1000 field and laboratory reflectance measurements in the spectral range 0.35-2.5 mm were acquired from the Ubehebe Peak contact aureole using a FieldSpec FR spectroradiometer from Analytical Spectral Devices (Boulder, CO). Mineral assemblages indicated by spectroscopic methods were evaluated by comparison with reference spectral libraries and validated using standard laboratory techniques including optical microscopy, scanning electron microscopy and energy-dispersive X-ray microanalysis, and X-ray diffraction.

Figure 4. Collection of field spectra at Ubehebe Peak (Racetrack Playa in background).
Figure 4. Collection of field spectra at Ubehebe Peak (Racetrack Playa in background). - click on figure for larger image

 

Results

General. Field and laboratory spectra of samples from the Ubehebe Peak contact aureole are consistent with mixtures of the key CaO-MgO-SiO2 (H2O-CO2) minerals listed in Table 1. Spectral features of calcite and/or dolomite dominate in most samples and features of tremolite and brucite are prominent locally. Quartz cannot be identified spectrally in the visible-near infrared, and the presence (or former presence) of forsterite is implied by strong spectral features of serpentine, which is a ubiquitous retrograde alteration product of forsterite. Other minerals recorded in spectra from the area include phlogopite (KMg3AlSi3O10(OH)2), which indicates some deviation from the simple CaO-MgO-SiO2 (H2O-CO2) system, and scapolite (~Ca4Al6Si6O24(CO3)) and chondrodite (Mg5(SiO4)2(F,OH)2), which indicate local metasomatism by igneous fluids. Grossular, epidote, malachite, and azurite were also spectrally identified in some samples.

Image endmembers. The AVIRIS apparent reflectance spectra generally show excellent correlation with the field and laboratory data. Image-derived spectral endmembers are shown in Figure 5, which contains both the full spectral range (left) and an expanded view of the 2.0-2.5 mm range (right). The spectral regions near 1.4 and 1.9 mm are excluded because of absorption effects by atmospheric water vapor.

Figure 5. Endmember spectra derived from AVIRIS imagery.
Figure 5. Endmember spectra derived from AVIRIS imagery. - click on figure for larger image

 

The endmembers features can be correlated with spectral features of calcite (2.335 mm), dolomite (2.315 mm), tremolite (2.380 mm), and serpentine (2.216 mm). A satisfactory image endmember for brucite is difficult to determine for two reasons. First, the main spectral features of brucite are centered in the water-vapor absorption regions near 1.4 and 1.9 mm. Second, the periclase zone where brucite occurs is very limited in extent and generally less than 100 m wide (Fig. 2). Despite these problems, a distinct image endmember was derived, which contains a very minor feature at 0.956 mm, the wavelength of a second-order OH absorption in brucite. Although not discussed here, additional image endmembers were derived including Eureka quartzite and the quartz monzonite intrusive.

Tremolite zone. Figure 6 shows tremolite distribution maps based on the LSU and MTMF algorithms. Higher abundances are shown by brighter pixels. The first indication of significant amounts of tremolite corresponds very closely with the position of the tremolite-in isograd mapped by Roselle (1997) on the basis of field studies and petrographic analysis. Furthermore, the tremolite maps show that the distribution is highly irregular within the zone and probably related to stratigraphic variations in bulk composition of the dolomites. Most notably, tremolite is preferentially developed at a stratigraphic horizon representing the contact between the Hidden Valley dolomite and the Lost Burro formation. This so-called "gray layer" is a sandy dolomite with 5-10% quartz; it was the focus of much of the sampling and petrologic analysis by Roselle (1997) because the bulk composition resulted in the most complete sequence of the metamorphic reactions in the CaO-MgO-SiO2 (H2O-CO2) system. Baumgartner et al. (1996) suggested also that fracture-controlled infiltration of H2O-rich fluids may have been focused selectively along beds in this layer.

Figure 6. Tremolite distribution maps based on Linear Spectral Unmixing (left) and Mixture Tuned Matched Filtering (right) algorithms.
Figure 6. Tremolite distribution maps based on Linear Spectral Unmixing (left) and Mixture Tuned Matched Filtering (right) algorithms. - click on figure for larger image

 

The detailed mapping and petrologic interpretation by Roselle (1997) was restricted to the southern half of the area covered by the AVIRIS imagery. The results of the hyperspectral analysis presented here show a previously undefined tremolite zone in the northern part of Figure 6 that is spatially associated with a poorly exposed granitic intrusive (McAllister, 1956; Burchfiel, 1969). The distribution of tremolite in those images suggests that it is developed primarily in the Pognip limestone, and that the isograd may extend as far as 1-2 km from the closest exposure of the intrusive.

Serpentine (forsterite zone). Figure 7 shows tremolite distribution maps based on the LSU and MTMF algorithms. The serpentine images are considered to approximate the extent of prograde forsterite, because most forsterite is partially or completely retrograded to serpentine by reactions such as (4), above. The maps indicate that serpentine is widely distributed within a zone extending roughly 800 meters from the intrusive contact, in close agreement with the position of the forsterite isograd as located by Roselle (1997). As in the case of tremolite, a previously unrecognized forsterite zone is also indicated adjacent to the intrusive in the northern part of the images. Reconnaissance sampling and laboratory spectral analysis showed that serpentine is indeed a major constituent of many rocks in that area. As in the southern part of the images, the serpentine in the north is in closer proximity to the intrusive than tremolite (mostly within 600 meters). The geology near the northern intrusive is more complicated than in the Ubehebe Peak aureole, and it appears that the development of serpentine is most pervasive in the Ordovician Ely Springs formation and Silurian Hidden Valley dolomite.

Figure 7. Serpentine distribution maps based on Linear Spectral Unmixing (left) and Mixture Tuned Matched Filtering (right) algorithms.
Figure 7. Serpentine distribution maps based on Linear Spectral Unmixing (left) and Mixture Tuned Matched Filtering (right) algorithms. - click on figure for larger image

 

Roselle et al. (1999) cited several lines of evidence for limited and spatially heterogeneous infiltration of H2O-rich fluid in the contact aureole at Ubehebe Peak. Stable isotope depletions in calcite and dolomite (d13C as low as -9.1‰ and d18O as low as 11.1‰) were interpreted as one consequence of interaction with magmatic fluids. Isotopic depletions occur only in a zone 850 meters from contact, and within that zone only about one quarter of the samples showed evidence of isotopic exchange. This distribution coincides approximately with that of the forsterite zone as delineated from the AVIRIS data. Although a theoretical or mechanistic basis for this apparent correspondence is not proposed here, it is possible that imaging spectrometer data may serve to outline zones of focused fluid flow and provide guidance for detailed field work and sampling for isotopic analysis.

Brucite (periclase zone). Figure 8 shows brucite distribution maps based on the LSU and MTMF algorithms. In general brighter pixels indicate a closer spectral fit with brucite; however, only pixels with maximum values are considered to actually contain brucite and these are highlighted in red. The brucite images are considered to represent the extent of prograde periclase, because periclase is completely retrograded to brucite by reaction (5), above. The brucite distribution maps are based on an extremely minor spectral feature near 0.956 mm in combination with a larger feature at 2.318 mm. In addition to being small, the 0.956 mm feature is also in a region of potential interference by atmospheric water vapor. For these reasons, the reliability of this endmember is still being evaluated. Despite these reservations, the distribution of the brucite in the AVIRIS scene corresponds very well with the distribution of brucite (after periclase) as determined by Roselle (1997). Both the LSU and the MTMF images accurately mark a prominent but discontinuous brucite-bearing zone within approximately 200 meters of the intrusive contact. Field and laboratory spectra from that zone display near textbook examples of brucite absorption features. The LSU image appears to include significantly more spurious pixels (e.g., in the tremolite and unmetamorphosed zones) than does the MTMF image. Also the MTMF image maps widespread brucite in screens and inliers of metamorphic country rock within the intrusive in accordance with Roselle (1997). As in the case of tremolite and serpentine, a previously unrecognized brucite (periclase) zone is indicated adjacent to the intrusive in the northern part of the images.

Figure 8. Brucite distribution maps based on Linear Spectral Unmixing (left) and Mixture Tuned Matched Filtering (right) algorithms.
Figure 8. Brucite distribution maps based on Linear Spectral Unmixing (left) and Mixture Tuned Matched Filtering (right) algorithms. - click on figure for larger image

 

Calcite/dolomite ratio. Spatial variability in the calcite/dolomite ratio within the AVIRIS scene is evident based on a shift of the main CO3 band between the endmember wavelengths of 2.335 mm for calcite and 2.315 mm for dolomite (see Figs. 3 and 5). Variation in the ratio may reflect a combination of initial sedimentological differences and the effects of the prograde metamorphic reactions (e.g., 1-3, above), all of which consume dolomite and produce calcite. Laboratory mixtures of pure calcite and dolomite (Fig. 9) indicate that this shift is not strictly linear with respect to the weight percentages but that it can be used to extract calcite/dolomite ratios with an accuracy of on the order of ±10 percent. It should be cautioned, however, that tremolite, serpentine, and brucite have features between 2.297 and 2.324 mm, close to the main dolomite band. Therefore, it may not be possible to use the CO3 band shift to determine calcite/dolomite ratios in samples that contain abundant Mg-silicates or brucite.

Figure 9. Shift of wavelength of CO3 bandcenter in laboratory mixtures of calcite and dolomite.
Figure 9. Shift of wavelength of CO3 bandcenter in laboratory mixtures of calcite and dolomite. - click on figure for larger image

 

The calcite maps (Fig. 10) show an increase in the abundance of calcite southward toward the intrusive contact, with the increase particularly evident above the forsterite isograd. Dolomite maps (not shown here) show a corresponding decrease in the abundance of dolomite with increasing metamorphic grade. A comparable zone of high calcite and low dolomite is also indicated adjacent to the intrusive body 5 km north of the Ubehebe Peak contact, although the distribution of isograds around the northern pluton has not been established by field studies.

Figure 10. Calcite distribution maps based on Linear Spectral Unmixing (left) and Mixture Tuned Matched Filtering (right) algorithms.
Figure 10. Calcite distribution maps based on Linear Spectral Unmixing (left) and Mixture Tuned Matched Filtering (right) algorithms. - click on figure for larger image

 

Increase in the calcite/dolomite ratio with proximity to the two intrusives is further highlighted in Figures 11 and 12 (Kozak and Duke, 2000). Figure 11 compares the Spectral Angle Mapper rule images for dolomite and calcite and an image that represents the ratio of the calcite rule value divided by the dolomite rule value. Using this presentation, a major increase in the calcite/dolomite ratio is indicated near the Ubehebe Peak pluton in the south and the unnamed intrusive in the north. Figure 12 shows a transect of SAM rule values southward through the Ubehebe Peak aureole, from the unmetamorphosed zone to the contact, along the lines shown in Figure 11. Calcite and dolomite rule values are relatively constant and positively correlated through the unmetamorphosed zone and tremolite zone. At the forsterite isograd, the two trends diverge: calcite increases and dolomite decreases at the same point that serpentine (after forsterite) increases. Calcite appears to increase through the forsterite zone, but very close to the contact, approximately coincident with the periclase isograd, the trends appear to reverse with an apparent increase in dolomite. This may reflect the fact that brucite (after periclase) has a spectral feature located at approximately the same wavelength as that of dolomite; if that is the case, the SAM values would no longer provide accurate estimates of the relative ratio of calcite and dolomite.

Figure 11. Spectral Angle Mapper rule images for dolomite (left), calcite (center), and calcite/dolomite ratio (right).
Figure 11. Spectral Angle Mapper rule images for dolomite (left), calcite (center), and calcite/dolomite ratio (right). - click on figure for larger image

Figure 12. Variation of Spectral Angle Mapper rule values for dolomite, calcite, and serpentine along north to south transect through Ubehebe Peak aureole. Transect location shown in Fig. 11.
Figure 12. Variation of Spectral Angle Mapper rule values for dolomite, calcite, and serpentine along north to south transect through Ubehebe Peak aureole. Transect location shown in Fig. 11. - click on figure for larger image

 

Preliminary Evaluation HyMap Imagery

HyMap imagery of the study area was acquired September 10, 1999, during the AIG/HyVista North American Group Shoot, under a cooperative agreement with Analytical Imaging and Geophysics, LLC (AIG, Boulder, CO) and HyVista Corporation (Sydney, Australia) (Kruse et al., 1999). The instrument was flown at low altitude on a Cesna 402, which resulted in a spatial resolution of 3.5 m. The HyMap spectral data consist of 126 bands covering the wavelength range from 0.45 to 1.35, 1.40 to 1.80, and 1.95 to 2.48 mm with bandwidth varying between approximately 15 and 20 nm (Cocks et al., 1998). Figure 13 compares decorrelation stretch images of the AVIRIS and HyMap data that cover the main part of the Ubehebe Peak contact aureole. The higher spatial resolution of the HyMap image results in much improved discrimination of stratigraphic and metamorphic variability in the aureole.

Figure 13. Comparison of AVIRIS (20 m) and HyMap (3.8 m) spatial resolution. Label images (AVIRIS, HyMap)
Figure 13. Comparison of  HyMap (3.8 m) (left) and AVIRIS (20 m) (right) spatial resolution.  - click on figure for larger image

 

Figure 14 compares tremolite distribution maps based on Linear Spectral Unmixing of the AVIRIS and HyMap images. Figure 15 compares image-derived spectra from corresponding pixels in the AVIRIS and HyMap image. Symbols indicate the bandcenters and sampling intervals of each spectrometer. It can be seen that the spectral resolution of the HyMap data is slightly poorer than that of AVIRIS, which could diminish the capability to discriminate overlapping absorption features such as those of calcite and dolomite, which are separated by only 20 nm (Fig 15).

Figure 14. Tremolite distribution maps based on Linear Spectral Unmixing of AVIRIS (left) and HyMap (right) images.
Figure 14. Tremolite distribution maps based on Linear Spectral Unmixing of AVIRIS (left) and HyMap (right) images. - click on figure for larger image

Figure 15. AVIRIS and HyMap spectral resolution between 2.1 and 2.4 mm.
Figure 15. AVIRIS and HyMap spectral resolution between 2.1 and 2.4 mm. - click on figure for larger image

 

Summary and Conclusions

This work establishes the utility of imaging spectrometry as method for studying the metamorphism of impure carbonate rocks. A critical step in such studies is determining the spatial distribution of key metamorphic minerals as well as variations in their relative abundance. With the exception of tremolite, most of the metamorphic minerals mapped here using the remotely sensed data present challenges for conventional field mapping. For example, brucite and serpentine are difficult to identify, and distinguishing ratios of calcite and dolomite in mixed carbonates requires laboratory methods.

Important new accomplishments of this study include the following:

  • The distribution of key metamorphic minerals in the CaO-MgO-SiO2 (H2O-CO2) compositional system has been mapped based on imaging spectrometer data with spatial resolutions of 20 m (AVIRIS) and 3.8 m (HyMap). The isograd pattern determined from the remotely sensed data is in excellent agreement with that of previous workers and with phase relations in metamorphosed siliceous dolomites.
  • The continuous production of calcite at the expense of dolomite accompanying metamorphic reactions has been monitored by remote sensing methods.
  • The imaging spectrometer data highlights uniquely the irregular distribution of metamorphic minerals resulting from sedimentary compositional layering and spatial variability of metamorphic fluid flow.
  • Spectral endmembers derived using the Ubehebe Peak aureole have been applied to map metamorphic mineral zonation in a previously undefined contact aureole 5 km north of Ubehebe Peak and, although not discussed here, a third contact aureole is indicated, located on the east side of Racetrack Valley.

This work also shows that several significant challenges remain in applying imaging spectrometer data in the Ubehebe Peak contact aureole and related geological settings:

  • Minor amounts of reduced carbon (<0.1 wt.%) can dramatically reduce reflectance and make spectral mineral mapping difficult or impossible.
  • Minerals that occur in metamorphosed carbonate rocks but which do not contain OH, H2O, and CO3 (e.g., quartz, wollastonite, diopside, forsterite) are difficult to detect using visible and near infrared wavelengths.
  • Reliable mapping of narrow metamorphic zones (e.g., periclase zone at Ubehebe Peak) requires high spatial resolution imagery (<5 m pixel size).
  • Reliable identification of minerals in mixtures, estimates of mineral ratios, and quantification of compositional shifts within mineral series require high spectral resolution (<10 nm) and would be aided by closer spectral sampling (<5 nm?) than currently available with either AVIRIS or HyMap.

In near the future, satellite-based imaging spectrometers (e.g., Hyperion, NEMO, Warfighter, ARIES) will provide metamorphic petrologists with the opportunity to conduct this type of analysis on a global basis, and result in unprecedented insights into thermal, structural, and fluid evolution processes in contact aureoles.

Acknowledgments

Research on spectroscopic methods for mapping metamorphic rocks is supported by National Science Foundation grant EAR-9706629. AVIRIS data for graduate research was provided to PKK by NASA's Jet Propulsion Laboratory. The cooperation of the U.S. Park Service, Death Valley National Park, is gratefully acknowledged. The authors also thank G.T. Roselle and L.P. Baumgartner for information on the Ubehebe Peak contact aureole.

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