Figure 3
(a) STM image of Cu(110) covered with multilayer water and subsequently heated to 120 K
. The image was obtained at 0.03 nA and 0.5 V. The multilayer disappears, and the 2D overlayer and chains coexist on the surface. The 2D overlayer shows a periodic structure of
along
. (b) STM image of the 2D island
. The image was obtained at 0.05 nA and 0.2 V. The 2D overlayer is composed of the 1D chains which are broken and disordered along the chains. (c) LEED pattern for the 2D overlayer, where
order spots are observed near the
spots in the
direction. (d) STM image after heated to 140 K
. The image was obtained at 0.1 nA and 0.3 V. Parallel chains at nearly regular intervals are observed. (e) Histogram of the distances between two adjacent chains at arbitrary 280 positions. The data were collected from five images acquired under the same condition as (d). The distances are measured between the centers of the chains. Two parallel chains are hardly observed within
. The arrow indicates the interchain distance in the 2D overlayer. (f) A simple model to roughly estimate the dipole repulsion between long water chains (inset). The model consists of an ensemble of chains of
length at regular intervals of
. We displace a chain in the direction perpendicular to the chains (arrow), and the dipole interaction energy between the displaced chain and the others is calculated as a function of the displacement (solid curve). The energies required to displace a chain by
and
are 10 and 40 meV, respectively. The result qualitatively indicates that the dipole repulsion is strong enough to arrange the chains at nearly regular intervals.
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