of mechanically fragmented samples implies
some amount of fatigue or permanent defor-
mation in them.
We further mapped the nanoscale local
electrostatic surface potential of different
crystals using Kelvin probe force microscopy
(KPFM; Fig. 2, F to H) ( 16 ). Fresh 001ðÞ=ðÞ 00 1
faces created by fracturing crystals of 1 per-
pendicular to the needle axis showed large
remnant surface potentials; 4.7 V was the
highest average value observed in our scans
(Fig. 2H and figs. S11 to S13). Potential at the
fracture tip surface was either positive or neg-
ative for a particular fragment, confirming the
complementary nature of the charges on oppo-
site fragmented pieces (figs. S11 and S12). The
experiments at a crack junction on (100)/(010)
faces of imperfectly healed crystals also pro-
vided evidence for the residual opposite po-
tentials (e.g., ~0.2 V to–0.6 V; Fig. 2, F and G)
on either side of the crack line (fig. S14). Such
opposite surface potentials were also observed
at crack lines in piezoelectric ceramics ( 17 ).
The opposite surface charges on fracture
faces observed in KPFM experiments can be
understood from the piezoelectric nature of
the polar crystals.
324 16 JULY 2021•VOL 373 ISSUE 6552 sciencemag.org SCIENCE
Fig. 3. The mecha-
nism of generation of
surface charges
on fracture faces and
crystallographically
precise self-healing
in crystals of 1.
(A) Schematic depic-
tion of molecular
dipoles inside a pristine
crystal and generation
of opposite polarities
on freshly created
faces of 001ðÞ= 00 1