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@ARTICLE{Gatta:281806,
author = {Gatta, G. Diego and Redhammer, Günther J. and Guastoni,
Alessandro and Guastella, Giorgio and Meven, Martin and
Pavese, Alessandro},
title = {{H}-bonding scheme and cation partitioning in axinite: a
single-crystal neutron diffraction and {M}össbauer
spectroscopic study},
journal = {Physics and chemistry of minerals},
volume = {43},
number = {5},
issn = {1432-2021},
address = {Berlin},
publisher = {Springer},
reportid = {FZJ-2016-01473},
pages = {341-352},
year = {2016},
abstract = {The crystal chemistry of a ferroaxinite from Colebrook
Hill, Rosebery district, Tasmania, Australia, was
investigated by electron microprobe analysis in
wavelength-dispersive mode, inductively coupled
plasma–atomic emission spectroscopy (ICP–AES), 57Fe
Mössbauer spectroscopy and single-crystal neutron
diffraction at 293K. The chemical formula obtained on the
basis of the ICP–AES data is the following: $X1,X2^Ca4.03$
$Y^(Mn0.42Mg0.23Fe2+1.39)_Σ2.04$
$Z1,Z2^(Fe3+0.15Al3.55Ti0.12)_Σ3.82$
$T1,T2,T3,T4^(Ti0.03Si7.97)_Σ8$ $T5^B1.96O30(OH)_2.18.The$
57Fe Mössbauer spectrum shows unambiguously the occurrence
of Fe2+ and Fe3+ in octahedral coordination only, with
Fe2+/Fe3+=9:1. The neutron structure refinement provides a
structure model in general agreement with the previous
experimental findings: the tetrahedral T1, T2, T3 and T4
sites are fully occupied by Si, whereas the T5 site is fully
occupied by B, with no evidence of Si at the T5, or Al or
Fe3+ at the T1–T5 sites. The structural and chemical data
of this study suggest that the amount of B in ferroaxinite
is that expected from the ideal stoichiometry: 2 a.p.f.u.
(for 32 O). The atomic distribution among the X1, X2, Y, Z1
and Z2 sites obtained by neutron structure refinement is in
good agreement with that based on the ICP–AES data. For
the first time, an unambiguous localization of the H site is
obtained, which forms a hydroxyl group with the oxygen atom
at the O16 site as donor. The H-bonding scheme in axinite
structure is now fully described: the O16–H distance
(corrected for riding motion effect) is 0.991(1)Å and an
asymmetric bifurcated bonding configuration occurs, with O5
and O13 as acceptors [i.e. with O16···O5=3.096(1)Å,
H···O5=2.450(1)Å and O16–H···O5=123.9(1)°;
O16···O13=2.777(1)Å, H···O13=1.914(1)Å and
O16–H···O13=146.9(1)°].},
cin = {JCNS (München) ; Jülich Centre for Neutron Science JCNS
(München) ; JCNS-FRM-II / JCNS-2},
ddc = {550},
cid = {I:(DE-Juel1)JCNS-FRM-II-20110218 /
I:(DE-Juel1)JCNS-2-20110106},
pnm = {6G4 - Jülich Centre for Neutron Research (JCNS) (POF3-623)
/ 6G15 - FRM II / MLZ (POF3-6G15)},
pid = {G:(DE-HGF)POF3-6G4 / G:(DE-HGF)POF3-6G15},
experiment = {EXP:(DE-MLZ)HEIDI-20140101},
typ = {PUB:(DE-HGF)16},
UT = {WOS:000377459200003},
doi = {10.1007/s00269-015-0798-x},
url = {https://juser.fz-juelich.de/record/281806},
}