This is the author’s version of a work that was submitted/accepted for publication in the following source:
Frost, Ray L., Xi, Yunfei, Scholz, Ricardo, & Tazava, Edison
(2013)
Spectroscopic characterization of the phosphate mineral florencite-La –
LaAl3(PO4)2(OH, H2O)6, a potential tool in the REE mineral prospection.
Journal of Molecular Structure, 1037, pp. 148-153.
This file was downloaded from: https://eprints.qut.edu.au/61339/
c Copyright 2013 Elsevier B.V. All rights reserved.
This is the author’s version of a work that was accepted for publication in Journal of Molecular Structure. Changes resulting from the publishing process, such as peer review, editing,
corrections, structural formatting, and toher quality control mechanisms may not be reflected in this document. Changes may have been made to this work since it was submitted for publication. A definitive version was subsequently published in Journal of Molecular
Structure, [1037, (2013)] http://dx.doi.org/10.1016/j.molstruc.2012.12.045
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https://doi.org/10.1016/j.molstruc.2012.12.045
Spectroscopic
characterization
of
the
phosphate
mineral
florencite-La
–
LaAl 3 (PO 4 ) 2 (OH, H 2 O) 6 , a potential tool in the REE mineral prospection
Ray L. Frosta•, Yunfei Xia, Ricardo Scholzb, Edison Tazavab
a
School of Chemistry, Physics and Mechanical Engineering, Science and Engineering
Faculty, Queensland University of Technology, GPO Box 2434, Brisbane Queensland 4001,
Australia.
b
Geology Department, School of Mines, Federal University of Ouro Preto, Campus Morro do
Cruzeiro, Ouro Preto, MG, 35,400-00, Brazil
•
Author to whom correspondence should be addressed (r.frost@qut.edu.au)
P +61 7 3138 2407 F: +61 7 3138 1804
1
Abstract
We have studied bluish green crystals of the mineral florencite-(La) from Serra dos Carajás,
Pará, Brazil. Qualitative chemical analysis shows a La and Al phosphate with traces of Ce,
Nd and Pr in substitution for La. Two sharp Raman bands at 987 and 1021 cm-1 assigned to
the PO 4 3- and HPO 4 2- symmetric stretching modes. Raman bands at 1064, 1112 and 1221 cm1
are attributed to the PO 4 3- and HPO 4 2- antisymmetric stretching modes. Raman bands at
404, 464, 524 and 526 cm-1 are assigned to the PO 4 3- ν 4 bending modes; An intense Raman
band at 614 cm-1 with shoulder bands at 680 and 647 cm-1 are assigned to the PO 4 3- ν 2
bending modes.
A sharp Raman band observed at 3649 cm-1 is assigned to the stretching vibration of the OH
units. Raman bands at 2906, 2988, 3158 and 3440 cm-1 and infrared bands at 2808, 2956,
3117 and 3416 cm-1 are attributed to water stretching vibrations. The spectra in the OH
stretching region support the concept of both hydroxyl and water units in the structure of
florencite-La, thus confirming the formula as LaAl 3 (PO 4 ) 2 (OH, H 2 O) 6 .
Key words: florencite-La, Raman spectroscopy, infrared spectroscopy, phosphate, alunitejarosite group, molecular structure
2
Introduction
The most common minerals containing rare earth elements (REE) are related to the monazite,
bästnesite and alunite-jarosite groups (florencite subgroup). The REE are important chemical
elements in the high technology industry, with special application in ceramics, glasses, lasers,
electronics, aluminum alloys and nuclear batteries. Florencite-La is one of the members of
the homonymous subgroup that divide the alunite-jarosite group, which is composed by
sulphates, arsenates and phosphates of trigonal structure [1]. Other member in the florencite
subgroup include the Nd, Ce and Sm analogues of florencite-La, and a number of arsenates
such arsenoflorencite-(Ce), graulichite-(Ce) and arsenowaylandite.
The first report concerning “florencite” as a mineral was published by Hussak and Prior [2] in
sediments from Diamantina region, Brazil. Latter a number of occurrences where described
in the literature [3-6]. In a systematic study about florencites, Kato [7] has described the Ce,
La and Nd analogues. The type material for florencite-La was considered those described
from the Shituru mine, in the copper deposits of Katanga, Democratic Republic of Congo in
data published by Lefebvre and Gasparrini [8]. Florencites occur in different geological
environments. It can be found in hydrothermal deposits related to carbonatites [9], in lateritic
crusts and weathered rocks [10, 11] and as a diagenetic mineral in sediments [12]. In recent
years, due to the industrial and strategic importance of REE florencite subgroup minerals are
subject of a number of geological studies [13, 14].
To the best knowledge of the authors, studies concerning the spectroscopic characterization
of phosphates of the florencite group are rare restricted to the database of the University of
Arizona (rruff.info), however no interpretation is given. However, in recent years, the
application of spectroscopic techniques to understand the structure of phosphates has been
increasing [15-17].
Farmer (1974) [18] divided the vibrational spectra of phosphates according to the presence,
or absence of water and hydroxyl units in the minerals. In aqueous systems, Raman spectra of
phosphate oxyanions show a symmetric stretching mode (ν 1 ) at 938 cm−1, the antisymmetric
stretching mode (ν 3 ) at 1017 cm−1, the symmetric bending mode (ν 2 ) at 420 cm−1 and the ν 4
mode at 567 cm−1. The value for the ν 1 symmetric stretching vibration of PO 4 units as
determined by infrared spectroscopy was also described [19-21]. The position of the
symmetric stretching vibration is mineral dependent and a function of the cation and crystal
3
structure. The fact that the symmetric stretching mode is observed in the infrared spectrum
affirms a reduction in symmetry of the PO 4 units.
The vibrational spectroscopic characterization of REE minerals can be an important tool
applied to the mineral exploration, where rocks and soils with potential of mineralization can
be easily submitted to IR or Raman study. In this work, samples of the REE phosphate
mineral florencite-La from the Igarapé Bahia mine, located in the municipality of
Parauapebas, Brazil has been carried out. Studies include spectroscopic characterization of
the structure with infrared and Raman. Chemical study via Scanning electron microscope
(SEM) was applied in the mineral characterization.
Experimental
Samples preparation and description
Bluish green florencite-(La) crystals from Serra dos Carajás, Pará were obtained from the
collection of the Geology Department of the Federal University of Ouro Preto, Minas Gerais,
Brazil, with sample code SAA-085. The sample is from the Igarapé Bahia mine, located in
the municipality of Parauapebas. The mine is an important Iron Oxide-Cu-Au (IOCG type
mineralization) ore deposit in the Carajás mineral district in Brazil, one of the most important
mineral provinces around the world. It is hosted by a low-grade metamorphosed volcanosedimentary sequence, the Igarapé Bahia Group of Archaean age [22]. The economically
extracted ore at Igarapé Bahia is largely developed as a supergene enrichment within the 150200 m thick oxide profile [23, 24]. The oxide zone is characterized by supergene enrichment
and hematite, goethite, gibbsite and quartz and has traces of secondary copper minerals and
REE-rich phosphates (florencite, crandalite, and rhabdophane) [25]. The original reserves of
oxidized gold ore were 15 Mt of high-grade ore (5 g/t Au) and 14 Mt of low-grade ore (1.4
g/t Au). To date, total production of gold is approximately 92 t, exclusively from supergeneenriched ore in the oxidized zone [25].
This is underlain by a transition zone that may be up to 50 m thick with enriched supergene
malachite, azurite, cuprite, native copper and goethite and minor amounts of digenite and
chalcocite. The primary copper-gold mineralization occurs below 200 m and consists mainly
of Fe chlorite, siderite, and magnetite rich breccias hydrothermally altered [22].
The total resource of primary ore is 219 Mt at 1.4 percent Cu and 0.86 g/t Au.
4
The 2575 ± 12 Ma SHRIMP age was obtained of hydrothermal monazite from the Igarapé
Bahia mineralization [22].
The sample was gently crushed in an agate mortar and to remove contaminate phases, with
the support of a Stereomicroscope Leica Model EZ4, florencite-La crystals were handily
selected from a sample in association with goethite and white clay. The florencite-La crystals
were phase analyzed by X-ray powder diffraction and Scanning electron microscopy in the
EDS mode (SEM/EDS).
Scanning electron microscopy (SEM)
Experiments and analyses involving electron microscopy were performed in the Center of
Microscopy of the Universidade Federal de Minas Gerais, Belo Horizonte, Minas Gerais,
Brazil (http://www.microscopia.ufmg.br).
Florencite-La sample was coated with a 5 nm layer of evaporated carbon. Secondary Electron
and Backscattering Electron images were obtained using a JEOL JSM-6360LV equipment.
Qualitative and semi-quantitative chemical analyses in the EDS mode were performed with a
ThermoNORAN spectrometer model Quest and was applied to support the mineral
characterization.
Raman microprobe spectroscopy
Crystals of florencite-La were placed on a polished metal surface on the stage of an Olympus
BHSM microscope, which is equipped with 10x, 20x, and 50x objectives. The microscope is
part of a Renishaw 1000 Raman microscope system, which also includes a monochromator, a
filter system and a CCD detector (1024 pixels). The Raman spectra were excited by a
Spectra-Physics model 127 He-Ne laser producing highly polarized light at 633 nm and
collected at a nominal resolution of 2 cm-1 and a precision of ± 1 cm-1 in the range between
200 and 4000 cm-1. Repeated acquisitions on the crystals using the highest magnification
(50x) were accumulated to improve the signal to noise ratio of the spectra. Raman Spectra
were calibrated using the 520.5 cm-1 line of a silicon wafer. The Raman spectrum of at least
10 crystals was collected to ensure the consistency of the spectra.
Infrared spectroscopy
5
Infrared spectra were obtained using a Nicolet Nexus 870 FTIR spectrometer with a smart
endurance single bounce diamond ATR cell. Spectra over the 4000−525 cm-1 range were
obtained by the co-addition of 128 scans with a resolution of 4 cm-1 and a mirror velocity of
0.6329 cm/s. Spectra were co-added to improve the signal to noise ratio. The infrared spectra
are given in the supplementary information.
Spectral manipulation such as baseline correction/adjustment and smoothing were performed
using the Spectracalc software package GRAMS (Galactic Industries Corporation, NH,
USA). Band component analysis was undertaken using the Jandel ‘Peakfit’ software package
that enabled the type of fitting function to be selected and allows specific parameters to be
fixed or varied accordingly. Band fitting was done using a Lorentzian-Gaussian cross-product
function with the minimum number of component bands used for the fitting process. The
Gaussian-Lorentzian ratio was maintained at values greater than 0.7 and fitting was
undertaken until reproducible results were obtained with squared correlations of r2 greater
than 0.995.
Results and discussion
Chemical characterization
The SEM image of florencite-La sample studied in this work is shown in Figure 1. The
fragment shows an aggregate of crystals up to 10 µm with rhombohedra form. The EDS
spectra are shown in Figure 2. Qualitative chemical analysis shows a La and Al phosphate.
Traces of Ce, Nd and Pr were also observed in substitution to La. Due to the presence of
goethite in association with florencite-La, an intense pick of Fe was also found.
Spectroscopy
The Raman spectrum of florencite in the 100 to 4000 cm-1 spectral range is displayed in
Figure 3a. This figure shows the position of the peaks and the relative intensities of the
Raman bands. The spectrum in the 2600 to 3800 cm-1 displays lower intensity than the
phosphate spectral region around 1000 cm-1. Clearly, there are parts of the spectrum where
no intensity is observed. Thus, the Raman spectrum is divided into subsections depending
upon the type of vibrations being observed. In comparison, the infrared spectrum as shown in
Figure 3b shows significantly more intensity in the 2500 to 3600 cm-1 spectral range. Again
6
there are parts of the spectrum where no intensity is found, and as a consequence the
spectrum is divided into sections for further analysis.
The Raman spectrum of florencite-la in the 800 to 1400 cm-1 region is illustrated in Figure
4a. The Raman spectrum is dominated by an intense sharp band at 987 cm-1 with a second
band at 1021 cm-1. These bands are assigned to the PO 4 3- and HPO 4 2- symmetric stretching
modes. The Raman bands at 1064, 1112 and 1221 cm-1 are attributed to the PO 4 3- and HPO 4 2antisymmetric stretching modes.
The Raman band at 846 cm-1 is likely to be a water
librational mode.
The infrared spectrum of florencite-La in the 500 to 1300 cm-1 spectral region is reported in
Figure 4b. The spectrum shows complexity especially when compared with the Raman
spectrum which shows clearly resolved bands. The spectrum may be resolved into component
bands. An intense band is observed at 1026 cm-1 which is the infrared equivalent of the
Raman band at 1021 cm-1. The resolved infrared band at 975 cm-1 is likely to be the
equivalent of the Raman band at 987 cm-1. The infrared bands at 1075, 1123 and 1214 cm-1
are assigned to the PO 4 3- and HPO 4 2- antisymmetric stretching modes.
The Raman spectrum of florencite-La in the 300 to 800 and in the 100 to 300 cm-1 spectral
ranges are illustrated in Figures 5a and 5b. The first figure displays the region where the
phosphate bending modes are to be found. The bands are found at 404, 464, 524 and 526
cm-1 are assigned to the PO 4 3- ν 4 bending modes. An intense Raman band is observed at 614
cm-1 with shoulder bands at 680 and 647 cm-1.
These bands are assigned to the PO 4 3- ν 2
bending modes. The observation of multiple bands in the ν 2 and ν 4 regions proves the
symmetry of the phosphate anion is reduced to C 3v or C 2v . The broad band at 310 cm-1 is a
metal (La)-oxygen stretching vibration. The two bands at 699 and 716 cm-1 are thought to be
related to the OH deformation modes. The Raman bands in the far low wavenumber region at
202, 255 and 270 cm-1 are simply referred to as lattice vibrations.
The Raman spectrum and infrared spectrum of florencite-La in the 2600 to 3800 cm-1 spectral
range is reported in Figures 6a and 6b.
The formula of the mineral is written as
LaAl3 (PO 4 ) 2 (OH, H 2 O) 6 and as such has both hydroxyl units and water molecules in the
structure. The spectra of these units should be readily observed in the spectra of the OH
stretching region. A sharp Raman band observed at 3649 cm-1 is assigned to the stretching
7
vibration of the OH units. This band is not observed in the infrared spectrum. Raman bands
found at 2906, 2988, 3158 and 3440 cm-1 are attributed to water stretching vibrations. In the
infrared spectrum broad bands at 2808, 2956, 3117 and 3416 cm-1 are attributed to water
stretching vibrations. The position of these bands is indicative of a range of hydrogen
bonding. The bands at the lower wavenumbers are assigned to very strong hydrogen bonded
water molecules.
The Raman spectrum of florencite-La in the 1300 to 2000 cm-1 spectral range is illustrated in
Figure 7a, whilst the infrared spectrum over the 1300 to 1800 cm-1 region is reported in
Figure 7b. This concept is affirmed by the bending modes of water at 1655 cm-1 (Raman) and
1667 cm-1 (infrared).
Conclusions
The most common minerals containing rare earth elements (REE) are related to the monazite,
bästnesite and alunite-jarosite groups (florencite subgroup). The REE are important chemical
elements in the high technology industry, with special application in ceramics, glasses, lasers,
electronics, aluminum alloys and nuclear batteries. Florencite-La is one of the members of
the homonymous subgroup that divide the alunite-jarosite group, which is composed by
sulphates, arsenates and phosphates of trigonal structure.
Qualitative chemical analysis shows a La and Al phosphate with traces of Ce, Nd and Pr in
substitution for La. Due to the presence of goethite in association with florencite-La, an
intense pick of Fe was also found.
Raman spectroscopy complimented with infrared spectroscopy identified the presence of
phosphate, hydroxyl units and water in the structure of florencite-La
Acknowledgements
The financial and infra-structure support of the Discipline of Nanotechnology and Molecular
Science, Science and Engineering Faculty of the Queensland University of Technology, is
gratefully acknowledged. The Australian Research Council (ARC) is thanked for funding the
instrumentation. The authors would like to acknowledge the Center of Microscopy at the
Universidade Federal de Minas Gerais (http://www.microscopia.ufmg.br) for providing the
8
equipment and technical support for experiments involving electron microscopy. R. Scholz
thanks to FAPEMIG – Fundação de Amparo à Pesquisa do estado de Minas Gerais, (grant
No. CRA - APQ-03998-10).
9
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Karfunkel, J. Schnellrath, R. Scholz, Amer. Min.,96 (2011) 42-52.
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[21] R.L. Frost, W.N. Martens, T. Kloprogge, P.A. Williams, Neues Jahrb.Min. Mon., (2002)
481-496.
[22] E. Tazava, C.G.d. Oliveira, Igarape Bahia Au-Cu-(REE-U) deposit, Carajas Mineral
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11
List of figures
Figure 1 - Backscattered electron image (BSI) of a florencite-La.
Figure 2 - EDS spectra of florencite-La.
Figure 3 (a) Raman spectrum of florencite-La over the 100 to 4000 cm-1 spectral range
(b) Infrared spectrum of florencite-La over the 500 to 4000 cm-1 spectral range
Figure 4 (a) Raman spectrum of florencite-La over the 800 to 1400 cm-1 spectral range
(b) Infrared spectrum of florencite-La over the 500 to 1300 cm-1 spectral range
Figure 5 (a) Raman spectrum of florencite-La over the 300 to 800 cm-1 spectral range
(b) Raman spectrum of florencite-La over the 100 to 300 cm-1 spectral range
Figure 6 (a) Raman spectrum of florencite-La over the 2600 to 4000 cm-1 spectral range
(b) Infrared spectrum of florencite-La over the 2600 to 4000 cm-1 spectral range
Figure 7 (a) Raman spectrum of florencite-La over the 1300 to 1800 cm-1 spectral range
(b) Infrared spectrum of florencite-La over the 1300 to 1800 cm-1 spectral range
12
Figure 1 - Backscattered electron image (BSI) of a florencite-La.
Figure 2 - EDS spectra of florencite-La.
13
Figure 3a
Figure 3b
14
Figure 4a
Figure 4b
15
Figure 5a
Figure 5b
16
Figure 6a
Figure 6b
17
Figure 7a
Figure 7b
18