American Mineralogist, Volume 83, pages 1330-1334, 1998

Scandiobabingtonite,a new from the Bavenopegmatite, Piedmont, Italy

Ploro ORl.tNnIrr'* Ma,nco PasERorr and GrovlNNa Vn,zzllrNr2

rDipartimento di Scienzedella Terra, Universitd di Pisa, Via S. Maria 53,1-56126 Pisa, Italy '?Dipartimento di Scienzedella Terra, Universitd di Modena, Via S Eufemia 19, I-41 100 Modena, Italy

Ansrntcr Scandiobabingtonite,ideally Ca,(Fe,*,Mn)ScSi,O,o(OH) is the analogue of babingtonite; it was found in a pegmatitic cavity of the Baveno associatedwith , , , stilbite, and . Its optics are biaxial (+) with 2V : : ^v: 64(2)",ct 1.686(2),P: 1.694(3), 1.709(2).D-"." : 3.24(5)slcm3, D.",.:3.24 sl cm3, and Z : 2. Scandiobabingtoniteis colorless or pale gray-green, transparent,with vitreous luster. It occurs as submillimeter sized, short, tabular crystals, slightly elongated on [001],and characterizedby the associationof forms {010}, {001}, {110}, {110}, and {101}. It occurs also as a thin rim encrusting small crystals of babingtonite.The strongest lines in the X-ray powder pauern are at2.969 (S), 2.895 (S), 3.14 (mS), and 2.755 (mS) 4. fn" mineralis triclinic, ipu.. g.oup PT, with a : 7.536(2),b : 1L734(2),c : 6.t48(Z) A, : 91.10(2), : 93.86(2), : lO+.S:(2)'. Scandiobabingtoniteis isostructural " B r with babingtonite, with Sc replacing Fe3* in sixfold coordination, but no substitution of Fer* by Sc takes place. Due to the lack of a suitably large crystal of the new species, such a replacementhas been confirmed by refining the of a Sc-rich babingtonite (final R : O.O47)using single-crystal X-ray diffraction (XRD) data.

INrnolucrroN mica (probably zinnwaldite) on which scandiobabington- This paper describes the new mineral species scan- ite crystals were emplanted (Fig. 1). Platy crystals of diobabingtonite.Both the mineral and its name were ap- scandiobabingtonitewere also found in epitaxial inter- proved by the IMA Commission on New and growth as a thin rim around green-blackprismatic crys- Mineral Names. Scandiobabingtoniteis the sixth scandi- tals of babingtonite (Fig. 2). The few crystals of scan- um mineral found in nature after bazzite, cascandite,jer- diobabingtonite studied here came from one sample. visite, kolbeckite, and thortveitite. Two other Sc minerals Scandiobabingtoniteis transparent,with vitreous luster were recently discovered: the scandium-dominant ana- and pale gray-greencolor. Scandiobabingtoniteoccurs as logue of xenotime-(Y) (IMA no. 96-024) and the scan- submillimeter-sized, short, prismatic crystals, slightly dium-dominant analogue of overite and segelerite(IMA elongated on [001] and characterizedby the association no. 96-060) (Mandarino and Grice 1997). of theforms {010}, {001}, {110}, {110}, and{101}, as Baveno is the type locality for bazzite (Artini 1915), shown in Figure 3. The faces were indexed using a two- cascandite,and jervisite (Mellini et al. 1982). Recently circle optical goniometer,in conjunction with X-ray sin- thortveitite (Orlandi 1990) was found in this classic lo- gle-crystal study, to overcome problems associatedwith cality; therefore, the only scandiummineral not found to a slight distortion and opacity of the faces from a thin date at Baveno is kolbeckite. Due to this peculiarity, the crust of mica. pegmatiticgranite of Bavenois unique. Two small crystals used in the optical and chemical The type material is preserved in the Museo di Storia study showed a very small black core and a large gray- Naturale e del Territorio, University of Pisa.A small crys- green transparentrim. It appearsthat the two crystals of tal is also stored in the Royal Ontario Museum, Univer- scandiobabingtonitegrew starting from a green seedcrys- sity of Toronto. tal of babingtonite (Fig. 4). Babingtonite, normally as- sociated with minute lamellar crystals of , is a OccunnnNcE, pHysICAL, AND oprrcAI, pRopERTTES common mineral in the pegmatitic cavities of the Baveno Scandiobabingtonitewas found in the "Montecatini" granite. The color of scandiobabingtonite(light gray- granite quarry near Baveno (Novara, Piedmont, Italy), green) is however easily distinguishable from that of within a 10 x 10 x 20 cm cavity, associatedwith snow- babingtonite. like orthoclasecrystals, smoky qvafiz, light sky-blue al- Scandiobabingtoniteis brittle and shows {001} and bite, stilbite, fluorite, and light green-yellow rosettes of {110} perfect ;its hardnessis 6. The measured density, obtained by the heavy liquid method on a zoned * E-mail: [email protected] crystal, is 3.24(5) g/cm3;the calculatedvalue for the pure 0003-004x/98/1I l2-1330$05 00 | 1330 ORLANDI ET AL.: SCANDIOBABINGTONITE 1331

aa,/

o Frcunt 1. SEM photo of scandiobabingtonitecrystals on l- : micafrom Baveno,Piedmont, Italy. Scalebar 0 1 mrn. F

Sc and Fe3* end-membersis 3.22 and 3.29 glcm., respectively. Optically, scandiobabingtoniteis biaxial positive, shows a 2V(meas) of 64(2)' and a strong (r > Frcunn3. Drawingof a singlecrystal of scandiobabingtonite v); is strong with colors from pink (f') to green (a'). Refractive indices for Na light are: ct : r.686(2);p : r.694(3);1 : 1.7o9(2). voltage 15 kV, sample current 20 nA, beam size 15 pm. An evaluation of the optical orientation was done on a The elementsmeasured were Si, Sn, Sc, Fe, Ca, Mn, and thin plate cut perpendicularto [001] with a crystal section Na. All other elements,including REE and Y, were below delimitedby (110),(010), (110), (110), (010), and (110) detection limit. (for Fe and Mn), kaersutite faces,where an evidentcleavage (110) was also present; (for Ca, Na, Si), metallic Sn (for Sn), and synthetic an extinction angle of approximately 6'was measuredon NaScSirOu(for Sc) were used as standards. (Il0). Z:$ : -250, p = 47"; Y:$ : 146, p = 751'X:6 The crystal examined shows a sudden transition from : 42", p : 47'. Figure 5 shows the relationship between a core with a composition essentiallyequal to scandium- optical and crystallographic axes in scandiobabingtonite free babingtonite to a rim with a high and homogeneous from Baveno. scandium content and a composition typical of scandio- babingtonite. These data show that whenever the Fe con- CnnlrrcAr, nar.l tent is high the Sc content is low and vice-versa,whereas Electron microprobe analyses(Table 1) were collected the Mn content remains constant acrossthe two zones. using a wavelength dispersive ARL-SEMQ instrument The HrO content could not be directly determinedbe- under the following operating conditions: accelerating cause of the scarcity of material, but it was inferred to

Frcunn 2. Epitaxial growth of tabular scandiobabingtonite FrcunB 4. Thin section approximatelyon (001) of a submil- crystals on a shorl prismatic crystal of babingtonite SEM photo limeter sized crystal showing a gray core of babingtonite and a Scalebar : 0.1 mm. light rim of scandiobabingtonite. | -)-)L ORLANDI ET AL : SCANDIOBABINGTONITE

-t'lo Taele 1. Chemicaldata for scandiobabingtonite(average of 7'io,-' three analyses) ,.7 Weightpercent Range sio, 55 26 54.61-55.62 SnO, 12'l 1 09-1.34 xX Sc,O" 1132 1101-11 51 FeO. 893 7.74-9 91 , ,/, CaO 1733 17 14-17 69 t MnO 411 3 43-5 18 , I l0lO Naro 140 1 37-1 43 -l 2\ X H,Ot too 010 I xI I : 101 24 t l, " Total Fe: This was recalculatedas FeO 8.48 and Fe,O30.50. l, t :,:i I t Constrainedto give t hydroxylpfu

i'-.- -_--1- I y 1 is.

\i Sc-rich crystals were unsuitable for a structural study. \l Therefore, a zoned crystal was used. ilj, ro Operating conditions were: 48 kV 28 mA, graphite- rioX monochromatedMoKa radiation (I : 0.71069A;. Ze-*

Frcunn 5. Stereographicprojection of the optical(X, Y, D with respect to the crystallographic(x, y, z) axes tn Taele 2. X-raypowder diffraction pattern for scandiobabingtonite. scandiobabingtonite

-t1 possessone (OH) group per 14 O, as in the chemical m 37 1134 010 formula of babingtonite. Fe was recalculatedas FeO and MW 696 698 110 666 672 001 FerO. basedon stoichiometry. On these grounds,the em- 509 515 120 pirical formula of scandiobabingtonite,recalculated on 514 101 the basis of a total of 15 O, is (Ca,,,Naorr)r,nu(Fefr{, 474 4 to 101 474 111 Mnor)ro r, (Scon,Sno ooFefij.)>o nrsi, .nO,o -(OH), oo.The sim- 444 445 111 plified formula is: Ca.(Fe,*,Mn)ScSi,O,"(OH),and thus MW 411 411 121 scandiobabingtonite is the scandium analogue 374 375 210 of m 348 349 220 babingtonite. 329 3.30 131 mS 3.14 J. tc 102 X-nay cRysrALLocRApHy m 3.03 3.04 221 S 2.969 2.974 112 Preliminary X-ray single-crystalWeissenberg measure- J 2 895 2.903 140 ments indicate that scandiobabingtonite,similarly to ba- mS 2.755 2.760 220 2 680 2 684 141 bingtonite, is triclinic with space group Pl or pl. The 2.679 122 unit-cell parameters, refined at the four-circle z 056 2 648 141 diffractometer,are'. a:7.536(2) A, U : 11.734(2),c : 2 579 I CAI 212 : 2 483 2 484 122 6.148(2),a 9r.70(2)", I : 93.86(2),1 : 104.53(2). 2 458 2 467 320 The X-ray powder pattern (Table 2), collected with Gan- 2 286 2296 311 2 244 2 247 141 dolfi camera and FeKct radiation on a small frasment se- 2 216 2.219 013 lected from the rim of a zoned crystal, is almosiidentical 2 184 2 191 250 to that of babingtonite. 2 190 103 z tJo 2.158 231 Chemical dishomogeneityand rhe evident distortion of 2.120 2.120 023 some crystals, displayed also by a light curvature of the mw 2.O84 2.089 311 faces of the crystals, caused 2.083 251 all diffracted reflections of 2.040 2 046 322 the single crystal to be rather broad. 1 900 1 899 t?1 1 898 302 Srnucrunn ANALySIS 1 863 1 872 133 1 813 1 814 'l Collection of intensity data were carried out using a 722 1 726 160 small crystal (0.3 x 0.2 x 0.15 mm) on an Ital Structures 1 669 1 673 332 1 648 1 648 161 four-circle automatic diffractometer. The choice of the 1 630 I oJo 450 most suitable crystal for the XRD study representeda 1 633 024 compromise between chemical composition and quality. 1 608 totS 062 Severalcrystals were testedby Weissenbergphotographs Nofej Gandolficamera, FeKo radiationwere used, d are in angstroms and semiquantitative SEM-EDS chemical analyses.All Eightadditional lines were seen ORLANDI ET AL.: SCANDIOBABINGTONITE

TeeLe3. Final{ractional coordinates and equivalentisotropic displacementparameters for scandianbabingtonite Site B (A') Ca1 0.7858(2) 0 s42e(1) o 1445(2) 0.s8(3) o 2344(2\ 0.5223(1) 0 2999(2) 1.02(3) Fe'?* 0 ss1s(1 ) 0 6448(1) 0 0615(1) o 71(2) M-0 Fe3*/Sc 0 0457(1) 0 2355(1) 0 1871(1) 0 60(2) {A} si1 0 2906(2) 0 0538(1) 0 3408(2) 0 66(4) si2 0.463s(2) 0 sl55(1) 0.4261(2\ 0.60(4) si3 0.8070(2) o 4473(1\ 0.2129(3) 0 61(3) si4 0.s8e0(2) 0.7148(1) 0.3071(3) 0.58(4) 5r5 0 3292(2\ 0.8386(1) 0 1074(3) 0.66(4) o1 0 1es3(6) 0 9898(4) o 5342(7) 1.28(12) 02 0 1315(6) o.0773(4) 0 1836(7) 0.93(1o) Q3 0 4346(6) 0 1733(4) o 4321(7) 0.90(11) o4 0 3230(6) 0 3416(4) 0.2478(7) 0.80(10) U5 o 5474(6) o 6223(4) 0 3618(6) 0.84(10) %$c Ub 0 6807(6) 0 3733(4) 0 3764(6) 0 85(10) 0.9670(6) 0 3864(4) 0.1589(7) 0 86(10) Frcunr 6. Occupancyat the Fe3*-Scoctahedral site vs. av- o8 0.6767(6) o 4744(4\ 0.0311(7) 0 se(11) erageM-O distance.The experimental valuefor scan- o9 0.9259(6) 0.5710(4) 0.3367(6) 0.80(10) dianbabingtonite is 2.092 A tthisstudy). The bold line gives the 010 0 86e4(6) 0.7534(4',) o 1242(6) 0.84(10) 01 1 0.01e5(6) 0.2184(4) o 4843(7) 1.01(1 1) averageM-O distancefor any substitutionof Fe by Sc basedon 012 0 2034(6) 0.7395(4) o 2464(6\ 0.84(e) the valuesof the ionic radii by Shannon(1976). The thin line 013 0 5106(6) 0 8003(4) o.0577(7) 1 00(11) hasthe samesignificance, but it startsfrom theobserved distance(2.048 A) foundin babingtonite(Araki andZoltai 01s 0 3s77(6) (4) 0.9681 o 2311(7\ 1 08(11) r972)

demonstratesthat all scandium concentratesin one only -+ = 60', scanwidth (0.8 + 0.15 tan 0)'symmetricalwith of the two independent octahedral sites: The average respect to the Bragg value, slowest scan speed 2./min, (Fe2*-O) distanceof 2.169 A in babinstoniteand 2.165 proportionally raised (up to 25'lmin) on the basis of the A in scandian babingtonite excludes aiy -scandium intensityof the peaks,0 < h I0, -16 < k -< 15, -9 = I substitution at this site. =9. The averagevalue of the cation--oxygendistance in the A set of 2442 independentstructure factors were used [(Fe3*-Sc)Ou]octahedron, 2.092 A. suggestsa site occu- for the refinement, after correction for Lorentz and po- pancy of Sco'Feo.,n,based on linear regressionusing the larization effects. The least-squaresrefinement program ionic radii given by Shannon,1976\:0.645 A for t6rFe3*, SHELXT6 was used (Sheldrick 1976). The absorptionef- 0.145 A for I6rSc,and 1.366A for O, for which a coor- fects were taken into account by means of DIFABS pro- dination number of 3.33 (equal to the averagecoordina- gram (Walker and Stuart 1983; correction factors on {'s tion for the six O atoms belonging to the octahedron)was in the range0.87-1.30). The structurewas refined,using assumed.However, considerationof the difference in ion- the fractional coordinatesof babingtonite (Araki andZol- ic radii between iron and scandium (0.10 A) and the pro- tai 1972) as starting point, to a conventional R factor of portional increase in the average distance with 0.041, and a weighted R* = 0.049 (w = kl[o,(F") + respect to the almost pure Fe3* crystal of babingtonite 0.00046 F3). refined by Araki and Zoltai (1912), implies an alternate The basic crystal-chemical features of scandiobabing- occupancyof ScorfeoruGig. 6). Both of theseanalyses, tonite are identical with babingtonite (Araki and Zoltai together with the uncertainty in X-ray data deriving from 1972), md therefore will not be consideredin detail. For the number of electrons of iron and scandium,which are sake of comparison, only the final fractional coordinates not too different, suggestthat the actual content of scan- of scandiobabingtoniteare reported in Table 3. dium in our scandian babingtonite may be somewhat The only major difference with respect to babingtonite higher than 27Vo,as is also indicated by semiquantitative lies in the peculiar chemical composition of scandioba- SEM-EDS data. bingtonite, which causesan increasein the dimensionsof The crystal structure of babingtonite also has been in- the Fe3*- (and Sc-) centered octahedron:The dependentlyrefined in the spacegroup Pl (Kosoi 1976). distanceis 2.048 A in babingtonitebut 2.092 A in scan- Therefore, refinement of the structure of scandian ba- diobabingtonite. To account for this, during the refine- bingtonite in this non-centric space group was also at- ment the occupancyof Fe3* and Sc was allowed to vary, tempted. Such a procedure implied the doubling of all by setting Fe3" + Sc : 1.0 in the site occupied by Fe3* atomic sites. In our case, such a trial could be substanti- only in babingtonite.The refinementconverged to the oc- possible '73Vo ated by the ordering of scandium and trivalent cupancy of Fe3* + 27Vo Sc. This result shows that iron in two different sites. However, the occurrence of the crystal used for the structural study is not, strictly very high correlation coefficients between positional pa- speaking, a crystal of scandiobabingtonite,but a Sc-rich rametersrelated to eachother by pseudo-inversioncenters variety of babingtonite. However, the structural study led us to deny any reliability to such refinement (e.g., t334 ORLANDI ET AL.: SCANDIOBABINGTONITE some non-positive definite atomic displacementparame- Kosoi, A (1976) The structure of babingtonite.Soviet Physics Crystal- ters are obtained). Therefore, the slight observed devia- lography,20,446-451. Mandarino, J.A. and Grice, J D (1997) New minerals recently approved tion from equivalent occupancy of scandium and iron in by the Commissionon New Minerals and Mineral Names-International sites related by a pseudo-inversioncenter was considered Mineralogical Association CanadianMineralogist, 35, 78'7 195 as negligible. Mellini, M, Merlino, S, Orlandi,P, and Rinaldi, R. (1982)Cascandite and jervisite, two new scandiumsilicates from Baveno,Italy. American AcrNowr-nrcMENTS Mineralogist, 67, 599-603 Orlandi, P (1990) Zibaldone di mineralogiaitaliana Rivista Mineralogica We thank S Merlino for his encouragementin the study of the minerals Italiana. 3/1990. 137-144 from Baveno, and the mineral collector G Nova, who supplied us with Shannon,R D (1976) Revisedeffective ionic radii and systematicstudies the scandiobabingtonitesamples D Sturman and M. Franzini provided of interatomic distancesin halides and chalcogenidesActa Crystallo- helpful assistancewith the optical measurements.Reviews by C.M Gra- graphica, A32, 75l-7 67. maccioli and S Graeserimproved the paper Sheldrick, GM (1976) SHELX. Program for crystal strxcture determi- nation University of Cambridge,England. RBpnnnNcns crrED Waiker, N. and Stuart, D ( 1983) An empirical method for correcting dif- fractometer data for absorption effects. Acta Crystallographica,A39, Araki, T and Zoltat,T. (19'72)Crystal structureof babingtonite Zeitschrift rs8-166 ftur Kristallographie, 135, 355 313 Artini, E (1915) Due minerali di Baveno contenentiterre rare: weibyite MeNuscnrrr REcETVEDFsenuenv 10. 1998 e bazzite. Rendiconti dell'Accademia Nazionale dei Lincei. 24.313- M,qNuscnrmAccEPTED JUI-y 4, 1998 319 Pepenslnorgo sv Gneenro Annort