ARTICLE IN PRESS
J. Ann Aitken et al. / Journal of Solid State Chemistry 178 (2005) 970–975
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(3 equivalents of phosphorus) than for CuI (15
equivalents of phosphorus).
It has been reported that Cu3P has a moderate range
of homogeneity that can depend on the synthetic
conditions used. In a study undertaken by Olofsson it
was demonstrated that at 700 1C the homogeneity range
lies approximately between Cu2.82P and Cu2.73P. It was
also found that by changing the reaction temperature
from 400 to 800 to 850 1C a change in lattice parameters
can be observed, where at higher temperature smaller
lattice parameters were obtained, suggesting a larger
extent of Cu vacancies. Our experiments also show that
Cu3P displays a homogeneity range, since we obtained
slightly different ratios of Cu:P for nearly every
sample obtained, while the powder diffraction patterns
looked nearly identical. Under all solvothermal condi-
tions essayed, a slightly copper deficient material was
obtained, as determined by EDS, which could be
attributed to either intrinsicdefetc formation in the
copper phosphide materials as postulated by Olofsson,
or to the presence of amorphous phosphorus.
For the reaction of copper (II) chloride plus red
phosphorus in H2O at 200 1C the best ratio is 1:5, similar
to the case of CuI. Increased copper (II) chloride
amounts produced CuCl as a byproduct, whereas
increased amounts of phosphorous resulted in a
significant amorphous background in the powder
diffraction pattern, which we attribute to red phos-
phorus.
While our results show that an excess of phosphorus
is always necessary to form pure Cu3P, the excess is not
nearly as much as was reported by Qian and coworkers.
Their reactions required 22 mol of phosphorus (66
equivalents) for every 1 mol of CuCl2 Á 2H2O while our
greatest excess of phosphorus was 10 mol (30 equiva-
lents) for every 1 mol of copper metal. The reaction of
copper (I) chloride with red phosphorus requires the
least amount of excess phosphorus, only two additional
equivalents (i.e. Cu:P 1:1). The finding that less
phosphorus can be used than originally proposed makes
the formation of Cu3P under solvothermal conditions
much more atom efficient. Additionally, despite being
less reactive, red phosphorus can be employed success-
fully in lieu of yellow phosphorus.
3.3. Physical properties
Optical diffuse reflectance measurements were per-
formed for powdered samples of Cu3P. Analyses of
several Cu3P products obtained from different reaction
conditions all showed an optical absorption edge of
approximately 0.8 eV, indicating that Cu3P is a relatively
narrow gap semiconductor, consistent with the black
color of the material (Fig. 3).
Differential thermal analyses were performed for
several samples of Cu3P obtained under different
reaction conditions. The expected thermal behavior
was obtained for a sample obtained from the reaction
of CuI and P in a 1:5 molar ratio heated to 200 1C for 1
3.2. Structure and X-ray diffraction
Cu3P is a very interesting material since both its
composition and structure have been the center of some
controversy. The structure of Cu3P was originally
proposed to be a member of the anti-LaF3 structure-
type, along with many alkali metal pnictide 3:1 phases,
¯
crystallizing in space group P3C [12,13]. The structure
¯
was later solved in space group P3m [14]. Finally, in
day in H2O to yield a material of stoichiometry Cu2.87P
(Fig. 4). The DTA diagram shows an endothermicpeak
1972 Olofsson proposed that the space group P63cm was
correct [15]. Indeed, we calculated the powder X-ray
¯
diffraction pattern based on the P3C model and that of
the P63cm model to find that there were no differences in
the number of observed peaks and little difference in
intensities. Our diffraction data fits with the Olofsson
model and therefore that is the structure we based our
indexing upon (Fig. 2).
The structure of Cu3P contains both P and Cu with
high coordination numbers. Each P atom is surrounded
by eleven Cu atoms. The coordination sphere is quite
distorted but can be best described as a trigonal prism
with additional capping atoms on each of the three
rectangular faces and the two triangular faces. The
trigonal prisms are connected in the ab-plane to form
‘‘layers’’ that stack along the c-axis (Fig. 1). The
coordination of Cu is also irregular. Each Cu has either
three or four phosphorus atoms as neighbors with
distorted trigonal pyramidal and tetrahedral coordina-
tion spheres, respectively. In addition, each Cu atom has
nine Cu neighbors.
Fig. 3. Optical diffuse reflectance spectrum converted to absorption
for a powdered sample of Cu3P (CuCl+red P, 1:1 molar ratio, 200 1C,
24 h).