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Synthesis and characterisation of the quaternary nitride-fluoride
Ce
2
MnN
3
F
2-d
David A. Headspith,
a
Eirin Sullivan,
b
Colin Greaves
b
and M. Grazia Francesconi*
a
Received 30th April 2009, Accepted 19th August 2009
First published as an Advance Article on the web 4th September 2009
DOI: 10.1039/b908591b
Ce
2
MnN
3
F
2-d
has been synthesised via low-temperature fluorination of the ternary nitride Ce
2
MnN
3
.
To the best of our knowledge, Ce
2
MnN
3
F
2-d
is the first quaternary nitride-fluoride to be reported. The
reaction of Ce
2
MnN
3
with 10% F
2
/N
2
at 95–115
◦
C yields the fluorinated phase Ce
2
MnN
3
F
2-d
, with
tetragonal symmetry (P4/nmm a = 3.8554(4) A
˚
and c = 13.088(4) A
˚
based on neutron powder
diffraction), accompanied by starting material. Rietveld refinement supports a staged fluorine insertion
reaction (into alternate rocksalt layers) to give a product with stoichiometry Ce
2
MnN
3
F
2-d
.A
comparison with the formation of Sr
2
TiO
3
F
2
and the isostructural LaSrMnO
4
F indicates that two
F
-
anions are inserted but no F
-
/N
3-
substitution takes place. Magnetic susceptibility measurements
show a transition from Pauli paramagnetic behaviour, in Ce
2
MnN
3
, to paramagnetic behaviour upon
fluorination. The effective magnetic moment in Ce
2
MnN
3
F
2-d
, m
eff
= 5.38 m
B
, is consistent with an
intermediate value between that of Mn
3+
(4.9 m
B
) and Mn
2+
(5.9 m
B
) supporting the proposed
stoichiometry, Ce
2
MnN
3
F
2-d
.
1. Introduction
An important goal of solid-state chemists is the synthesis and
characterisation of new compounds followed by chemical manip-
ulation to induce valuable physical properties for technological
exploitation. Cationic substitutions and high pressure offer two
powerful ways to tune physical properties by manipulating the
chemical formula of solids; these methods can provide modified
structures, mixed oxidation states and, in general, different elec-
tronic configurations of metals. Anionic substitutions provide a
lesser utilised alternative via complete or partial substitution of
anions. Partial substitution leads to mixed-anion compounds, a
category of compounds that has received less attention than its
single-anion counterparts. However, chemists are now starting to
understand the potential of anionic substitutions for the tuning
of physical properties of materials. For example, any colour
in the range from light yellow to deep red can be tailored
by adjustment of the O
2-
/N
3-
ratio in the perovskite series
Ca
(1-x)
La
x
TaO
(2-x)
N
(1+x)
.
1
In 1994 the first superconducting oxide-
fluoride, Sr
2
CuO
2
F
2+d
was initially synthesised by Al-Mamouri
et al. from the direct fluorination of Sr
2
CuO
3
with fluorine gas
at 210
◦
C.
2
Sr
2
CuO
3
shows an anion deficient La
2
CuO
4
structure,
with Cu
2+
cations coordinated by oxide anions in a square-planar
fashion. The Cu-O squares join corners to form one-dimensional
chains along the b axis. The fluorination process causes the
substitution of one oxide anion with two fluoride anions and the
consequent expansion of the copper coordination from square
planar to octahedral and filling of the anion vacancies, giving rise
to a La
2
CuO
4
-structure. Extra fluoride is also inserted between
the Sr-O layers of the structure, causing an imbalance in negative
charge, which forces partial oxidation of the copper cation and
a
The Chemistry Department, The University of Hull, Hull, England.
E-mail: M.G.Francesconi@hull.ac.uk
b
School of Chemistry, University of Birmingham, Birmingham, England
induces superconductivity for a range of fluorine contents. This
insertion occurs in a similar way to fluorination of La
2
CuO
4
to
give La
2
CuO
4
F
d
.
3
Fluorination of other oxides isostructural with Sr
2
CuO
3
, in par-
ticular Ca
2
CuO
3
4
and Ba
2-x
Sr
x
PdO
3
(0 ≤ x ≤ 1),
5–7
produced a simi-
lar structural rearrangement: the formation of the oxide-fluorides,
Ca
2
CuO
2
F
2+d
and Ba
2-x
Sr
x
PdO
2
F
2
, occurs as a consequence of sub-
stitution of one oxide with two fluoride anions. However, for these
oxides there is no change in the copper/palladium coordination,
which remains square planar, because of size effects and cationic
preference. Whereas Sr
2
CuO
2
F
2+d
has an orthorhombic La
2
CuO
4
-
type unit cell, Ca
2
CuO
2
F
2+d
and Ba
2-x
Sr
x
PdO
2
F
2
have tetragonal
structures derived from a Nd
2
CuO
4
-type unit cell.
Only a small number of ternary nitrides are isostructural with
Sr
2
CuO
3
. Early examples, from the radioactive metals thorium
and uranium, Th
2
MN
3
and U
2
MN
3
(M = Mn, Cr), were prepared
over 30 years ago and found to be very similar in structure,
with an orthorhombic anion deficient La
2
CuO
4
-type structure.
8
Cerium has been investigated as an alternative to radioactive
uranium, and Niewa et al. showed that Ce
2
MnN
3
is isostructural to
U
2
MN
3
.
9,10
The structure of Ce
2
MnN
3
comprises corner linked chains of
MnN
4
units along [100], with Mn in approximately square planar
geometry.
10
These units resemble the CuO
4
squares in Sr
2
CuO
3
.
The bonds between nitride anions and manganese differ slightly,
altering the square shape. In particular the Mn-N
bridging
bonds are
shorter than the Mn-N
terminal
bonds. The structure is described
as an anion deficient T-type structure, isostructural to Sr
2
CuO
3
,
where Ce replaces Sr and Mn substitutes for Cu. The coordination
environment of cerium is considered by Landrum et al. to
include seven other cerium cations, seven nitride anions and
four manganese cations.
11
The two crystallographically different
nitrogen anions are coordinated in a distorted octahedral fashion,
one by four cerium and two manganese cations, the other by five
cerium and one manganese cations.
10
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