1 Introduction

In the field of mineral exploration, remote sensing has significant contribution in mapping of faults, fracture systems, host rocks and alteration/weathered zones indicative of mineral deposits [11, 16,17,18, 28,29,30,31, 48, 55]. High spectral resolution of hyperspectral sensors makes it an ideal complementary and confirming tool alongside traditional multi-spectral and field-based methods for mineral exploration [3]. Therefore, reflectance and emission spectroscopy in visible-to-near-infra-red and mid-infra-red have globally been used as an important tool for mineral characterization and exploration [8, 20, 22, 26, 32, 39, 44]. Data collected by imaging spectrometer using geometrically coherent spectral measurements facilitate quantitative and qualitative identification and mapping, thereby allowing a more detailed characterization of the spatial mineralogical heterogeneity using mixture analysis technique [21, 50,51,52,53].With the availability of more sophisticated and high-resolution spectrometers, the field of imaging spectroscopy from space, air or field has grown in terms of technical capability and application potential in geological mapping and mineral exploration [12, 13, 19, 27, 33, 35, 36, 43, 45, 54, 56].

Although hyperspectral remote sensing techniques are operational since last two decades, the application of the same in Indian sub-continent has rather been limited mainly due to unavailability of space- or air-borne hyperspectral data. Works dedicated to mineral exploration taking cues from satellite-based data are still scanty and therefore hold promise for their application in mineral potential areas, so far unexplored or inadequately explored [34, 35, 41, 46]. Such areas exist in the state of Rajasthan, which is one of the leading producers of metallic ores such as Pb–Zn, Cu and non-metallic ores like rock phosphate, gypsum, limestone, etc. Currently, 48 minerals are being mined out of 79 discovered minerals [10]. Therefore, considering the vast minerals potential of the state, the Government has recently proposed to increase its mining coverage from 0.4 to 1% by area [47]. Contemporary works around the globe also demand satellite-based studies to be incorporated to narrow down search for newer potential ore-rich zones. The present work, thus, aims at using space-based hyperspectral remote sensing data along with field-based spectroscopic data to address mineral exploration in Rajasthan.

The spectra derived from satellite image and field samples readily help to detect transitional element phases, viz. haematite, goethite and jarosite, which mainly show absorption dips because of electronic processes and alteration minerals containing hydroxyl ions and water like kaolinite, dickite, alunite and sericite that show absorption features due to vibrational characteristics [5, 6, 24, 37, 38]. Therefore, this fundamental property was used in both space-borne and ground-based spectral analysis to identify and classify the alteration zones based on abundance of diagnostic minerals. The study thus aims to identify and characterize the altered mineral phases associated with hydrothermal metallogenic process with the help of remote sensing data, especially in the VNIR wavelength range which may lead to zeroing in on potentially enriched, but relatively unexplored areas of or mineralization.

2 Geological setting of the area

The study area corresponds to vast north-eastern craton of India which preserves geological history from 3500 to 0.5 My in a suit of metamorphosed rocks that have undergone polyphase deformation. The study area, albeit, represents a smaller part of it, situated mainly around Udaipur town (N 24°37′ to 24°53′ and E 73°40′ to 73°48′). The basement represented by high-grade gneissic rocks of Archaean age is popularly known as Banded Gneissic Complex, which consists of composite Mangalwar–Sandmata complex and meta-volcanics of Hindoli Group [15, 40] (Fig. 1).

Fig. 1
figure 1

(modified after [40]

Geological map of the area

The basement sequence is referred as Bhilwara Supergroup [14]. Towards eastern side of Udaipur town, sporadic occurrence of granite intrusion, viz. Untala Granite 2900 My [9], into the basement complex is observed. The Proterozoic supra-crustals, lying above Archaean basement, are represented by fold belts of Lower-to-Middle Proterozoic Aravalli Supergroup (aka. Aravalli Fold Belt, AFB) and Middle-to-Upper Proterozoic Delhi Supergroup (aka. Delhi Fold Belt, DFB). Two major stratigraphic divisions have been proposed for AFB, i.e. a shelf facies with basic lavas and coarse clastics at the base (Delwara and Debari Groups) exposed in the west and deep sea turbidite facies (Jharol Group) with Ultramafic intercalations in the east of the study area [25]. The contact between two facies, at places, is marked by a suture known as Rakhabdev Lineament [40]. Towards the eastern side of the study area, there occurs a prominent end-Archaean plutonic horizon known as Berach Granite in the vicinity of Chittorgarh. Towards further east, the Great Boundary Fault (GBF) occurs in close association with Berach Granite, delineated by an important zone of dislocation marked by a reverse fault which separates younger Vindhyan sedimentary sequence from older Pre-Vindhyan sequence [40]. Higher in the stratigraphy, the southern part of DBF is exposed towards the west of Udaipur, separated by a sheared and thrusted contact with AFB. The litho-sequence of the area, thus, is bounded between AFB-DFB thrusted contact in the west and GBF in the east. The recent alluvium mainly consists of weathered derivatives of gneiss, schist, phyllite, felsic and basic volcanics, dolomite and quartzite. The area is rich in several metallic and non-metallic mineral deposits, viz. lead, zinc, copper, rock phosphate, soapstone, limestone, dolomite, etc. [10], and there is an urgent need to explore further potential economic mineral deposits.

3 Materials and methods

The Earth Observation-1 (EO-1) Hyperion data of 19 January 2004 study (Scene Id: PO1H11480432004019110PZ) (Row/Pass: 143/43) was used for the present study. Additionally, a false colour composite subset ASTER image of Hyperion coverage area with sample location shows the study area (Fig. 2). The Hyperion sensor measures reflected solar radiation in 242 spectral bands covering the 400–2500 nm range of electromagnetic spectrum. However, only 169 bands were used for further processing as the bands were uncalibrated and noisy. The radiometric corrections were applied on the data to remove the noise such as line drops and bad columns.

Fig. 2
figure 2

Standard FCC of ASTER image (subset to area covered by Hyperion image) (RGB: 321) showing sample collection points

The bad columns were corrected by averaging the neighbouring columns. After the pre-processing, atmospheric correction of image was done using Fast Line-of-Sight Analysis of Spectral Hypercubes (FLAASH) technique to convert radiance into apparent reflectance values as well as to suppress atmospheric effects with cloud percentage > 10% (Fig. 3, Table 1).

Fig. 3
figure 3

Atmospheric correction of Hyperion image (X-axis is rescaled)

Table 1 Parameters used for atmospheric corrections (FLAASH)

The MNF rotation was performed on atmospherically corrected image to determine the inherent dimensionality of image data. It also segregates the noise in the data and reduces the computational requirements for subsequent processing [2]. Pixel Purity Index (PPI) is used to find the most spectrally pure pixels in image. The Pixel Purity Index is computed by repeatedly projecting n-dimensional scatterplots onto a random unit vector. The extreme pixels in each projection are recorded, and the total number of times each pixel is marked as extreme is noted. The final endmembers present in the area are selected from the pure pixels identified by PPI which are used as the training sets for classification (Fig. 4). The image was classified using spectral angle mapper (SAM) algorithm [23]. SAM expresses the similarity between the two spectra, which is derived by calculating the angle between the vectors representing the endmember spectra in the n-dimensional space. This method is independent of illumination (i.e. topographic shading) and widely used for spectral matching.

Fig. 4
figure 4

SAM-classified mineral map of the area showing pure pixels of minerals

Representative rock samples were collected during field survey and analysed in laboratory for derivation of spectral signature using Analytical System Device (ASD) FieldSpec 4 operating in wavelength range of 350–2500 nm at a sampling interval of 1.4 nm @350–1050 nm and 2 nm @1000–2500 nm. A contact probe was used to nullify the effect of atmosphere. These spectral profiles of rocks were compared with USGS (resampled to Hyperion bands) mineral spectral library in ENVI 5 to detect major or spectrally dominant minerals (Fig. 5). Similarly, selected endmembers derived from the image were compared with laboratory spectra followed by their validation with published lithological map.

Fig. 5
figure 5

Spectral responses of selected endmembers (line colours Red, Blue and Black show USGS library, image and field spectra, respectively)

XRD investigation was employed to confirm the mineralogical outputs. XRD is one of the key methods to characterize phyllosilicates. The air-dried, powdered samples were scanned on a Rigaku Geigerflex X-ray diffractometer from 3° to 60° 2θ at 1° 2θ/min scan speed, using nickel-filtered copper Kα radiation (40 kV and 30 mA). Subsequently, the samples were scanned after treating with ethylene glycol (100 °C for 1 h) and were finally scanned after heating at 490 °C for 2 h under the same instrumental settings. The clay and mica phase minerals were identified by their characteristic basal X-ray diffraction maxima.

4 Results

The endmember minerals were derived after analysis of atmospherically corrected image using MNF and PPI. MNF resulted in selection of 14 bands of high eigenvalues out of 242 bands as they contained the maximum information. These 14 bands were used as an input for PPI which provided 5 endmembers. The endmembers were further classified using SAM algorithm. Subsequently, the endmembers were validated with field spectra which consist mainly of carbonate and silicate phases in the study area (Figs. 4, 5).

The extent of spectral match decreased significantly when the mutual similarity became less than 0.75 in spectral analyst operation of ENVI software. The pixels of the particular class classified using the SAM algorithm were matched with the field spectra, respectively. In addition to that, tie points generated on the image and the spectra of these points were also matched with the assigned class. Any deviation of this method will be considered under error of commission and omission. Confusion matrix, subsequently, was used to assess the accuracy of the final mineralogical classification of the area. The overall accuracy and Kappa coefficient of mineral map thus obtained from SAM are 0.71 and 0.54, respectively. Endmember minerals were further analysed by X-ray diffraction studies of the collected samples from the key horizons (Fig. 6). The endmember of the classified image represents mineral paragenesis having phlogopite, montmorillonite, lizardite, dolomite and clinochlore which are indicative of hydrothermally altered suite. Spectral analysis revealed that the laboratory spectra have always remained smooth as compared to image spectra. This smoothness is attributed to uniform grain size, absence of atmosphere and exposure available at laboratory-scale samples. In the present study, except for lizardite and clinochlore, laboratory spectra of all other phases show closer match with USGS spectra compared to image spectra. As a whole, considering spectral response of both laboratory and image spectra, montmorillonite and phlogopite show maximum similarity with USGS spectra of the respective minerals. Holistically, all the image and laboratory-derived spectra of silicate phases bear signatures of Mg-OH molecules at 2.3 μm. The paragenesis of the altered zone minerals reflects dominance of Ca-, Na- and Mg-rich phases, with very little or no K-bearing minerals. Considering the ubiquitous metallogeny of hydrothermal origin for different ores in this study area, the diagnostic minerals are interpreted to indicate an outer part of the thermal metasomatic zone.

Fig. 6
figure 6

X-ray diffractograms of five endmembers and associated minerals (abbreviations used: Clc: Clinochlore, Lz: Lizardite, Dol: Dolomite, Phl: Phlogopite, Mnt: Montmorillonite, Qtz: Quartz, Ill: Illite)

5 Discussions

Dominant carbonate phase present in the field is mainly dolomite with negligible calcite and their ferroan counterparts. However, only dolomites have been revealed in the classified endmember map which shows less-pronounced absorption at 2.31 μm compared to USGS spectra. This is attributed to impurity in carbonates in this region. Local mine tailings also indicate dominance of ubiquitous ferroan intercalation in dolomite. The relative flatness, specially in the visible region of laboratory spectra, indicates concentration of impinging energy on rather large pure euhedral dolomite grains as compared to image. The silicate phase present in the area is exemplified mainly by mica and clay minerals, viz. montmorillonite, phlogopite and chlorite. The image and laboratory spectral plots of montmorillonite show the typical absorption feature at 1.395 and 1.415 μm caused by (OH) overtone stretch and 1.95 to 2.208 μm for the combination of H–O–H bend plus (OH) stretch. Simultaneous occurrence of both these absorptions indicates a mineral having both (OH) and H2O [1, 7]. The stronger absorption at 1.9 to 2 μm also indicates predominance of water in the mineral over hydroxyl ion. However, it is most intriguing to note the conspicuous absorption due to the combination of metal (Al, Mg)–OH bend plus OH stretch, approximating 2.2 to 2.3 μm, which is evident both in image-derived and field spectra. Similarly, the diagnostic absorption feature of phlogopite at 2.3 μm is caused by Mg-OH bond and OH stretch. A small trough has also been recorded near 0.7 μm in image spectra indicating probable replacement of Mg by Fe2+ in octahedral site. The occurrence of phlogopite pixels in the vicinity of meta-basics further geologically strengthens the potential ferric iron enrichment in phlogopite lattice. However, this small dip gets diminished and spectra become rather flat in the case of laboratory-scale samples. But in the NIR region, an almost perfect match between laboratory and image spectra was observed which varies from USGS spectra in terms of spectral slope in 2.2 to 2.4 μm region. This results in a minor shift of the characteristic 2.3 μm dip towards lower wavelength region in the case of laboratory sample. The image spectra of the least-abundant phyllosilicate, i.e. Chlorite (aka. Clinochlore), are noticed to show almost near-perfect match with USGS spectra except slight offset in dips occurring at 0.9 and 1.4 μm. Spectral similarity with phlogopite and characteristic dip at 2.3 μm indicates that this variety of chlorite is also rich in Mg2+, thus interpreted as a clinochlore [43, 49]. However, a less-pronounced absorption at 0.7 μm cannot altogether rule out the presence of minor Fe2+. Therefore, Fe-bearing clinochlore is concluded to be more appropriate for this phase. The spectral plots of serpentine (aka. Lizardite) confirmed its presence owing to its diagnostic absorption at about 2.325 μm caused by Mg–OH molecules [4249]. A similar feature is also observed in the USGS spectra. As this phase is hydrous, it typically shows overtone absorptions due to the presence of (OH) ions in the visible and near-infra-red regions. It has been revealed that dips at 1.4 μm gets reduced in both image and laboratory spectra which are indicative of relatively (OH) poor variant of serpentine group of minerals. But, it is very interesting to note the relatively stronger presence of 1.9 μm absorption which corroborates the presence of water. This indicates the further progression of serpentine minerals in the serpentine–kaolinite solid solution series and development of neomorphic phase with little more dominance of H2O compared to serpentine. Brindely and Wann [4] reported the structural effect of transitional elements like Ni and Fe2+ in solid solution solutions related to serpentine group of minerals. In this study also, serpentines showing the presence of a broad absorption at 1 μm due to crystal field effect is believed to be due to the presence of Fe2+ and Ni in the lattice. The diagnostic mineral assemblage, thus obtained, is indicative of distal portion of thermal metasomatic zone.

6 Conclusions

This study reveals how effectively high-resolution hyperspectral data can be utilized for detection and characterization of altered minerals in a potentially mineralized area. As for the main ore formation process, a hydrothermal origin can be concluded based on the rock types, structure and characteristic altered mineral paragenesis represented by species like phlogopite, montmorillonite, lizardite, dolomite and clinochlore. Integration of satellite image-based and ground-borne spectral analysis with geochemical validation confirmed the abundance of phases rich in Ca, Na and Mg with a less K-bearing assemblage, which clearly is indicative of argillic or advanced argillic zone of hydrothermal alternation. This kind of mineralogical setup ideally follows a distal development of altered minerals away from the zone of intrusion. However, other complementary and field-based information is crucial to detect the particular zone or subzone of alteration. However, mainly employing satellite-based data and spectroscopy, an obvious lack of K-metasomatism or sericitization in altered rock has been disclosed. Abundance of carbonate phases like dolomite also beseeches for the outer part of the thermal aureole of metasomatically altered zone system.