Using
first-principles structure searching with density-functional
theory (DFT), we identify a novel
Fm
3̅
m
phase of Cu
2
P and two low-lying metastable
structures, an
I
4̅3
d
–Cu
3
P phase and a
Cm
–Cu
3
P
11
phase. The computed pair distribution function of the novel
Cm
–Cu
3
P
11
phase shows its structural
similarity to the experimentally identified
Cm
–Cu
2
P
7
phase. The relative stability of all Cu–P phases at finite
temperatures is determined by calculating the Gibbs free energy using
vibrational effects from phonon modes at 0 K. From this, a finite-temperature
convex hull is created, on which
Fm
3̅
m
–Cu
2
P is dynamically stable and the Cu
3–
x
P (
x
< 1) defect
phase
Cmc
2
1
–Cu
8
P
3
remains metastable (within 20 meV/atom of the convex hull)
across a temperature range from 0 to 600 K. Both CuP
2
and
Cu
3
P exhibit theoretical gravimetric capacities higher
than contemporary graphite anodes for Li-ion batteries; the predicted
Cu
2
P phase has a theoretical gravimetric capacity of 508
mAh/g as a Li-ion battery electrode, greater than both Cu
3
P (363 mAh/g) and graphite (372 mAh/g). Cu
2
P is also predicted
to be both nonmagnetic and metallic, which should promote efficient
electron transfer in the anode. Cu
2
P’s favorable
properties as a metallic, high-capacity material suggest its use as
a future conversion anode for Li-ion batteries; with a volume expansion
of 99% during complete cycling, Cu
2
P anodes could be more
durable than other conversion anodes in the Cu–P system, with
volume expansions greater than 150%. The structures and figures presented
in this paper, and the code used to generate them, can be interactively
explored online using
.