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By Carl R. Green

After an actor is poisoned onstage and the physique disappears, different mysterious occasions recommend that the theater conceals both his ghost or a smart assassin.

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The set of all such k’s fills the first Brillouin zone of k-space (Ashcroft and Mermin 1976). An example of crystal electronic structure is shown in Fig. 1, which shows calculated bands of Ag along various directions within the first Brillouin zone (Moruzzi, Janak et al. 1978, Papaconstantopoulos 1986, Smith and Mattheiss 1974). Knowledge of the emission angle and energy equates to knowing the electron momentum after it has been emitted from the sample. Passing through the surface, the translational symmetry of the lattice is preserved in the surface plane, but not perpendicular to it, and likewise with the crystal momentum.

1–1 keV is commercially available these days. Surface sensitivity is largely enhanced with the low energy beam, especially when it is used in an ultrahigh vacuum. Low energy electron microscopy (LEEM), which uses projection optics of reflected electrons for imaging, has realized real-time imaging of atomic steps even at elevated temperatures. LEEM is now widely used for observation of growing surfaces of various materials (Bauer, 1994; Meyer zu Heringdorf, 2008). 8 References Bales G S and Zangwill A (1990) ‘Morphological instability of a terrace edge during step-flow growth’, Phys.

Phys. 44, 1039–1049. Finnie P and Homma Y (2000a) ‘Motion of atomic steps on ultraflat Si(111): constructive collisions’, J. Vac. Sci. Technol. A18, 1941–1945. Finnie P and Homma Y (2000b) ‘Nucleation and step flow on ultraflat silicon’, Phys. Rev. B 62, 8313–8317. Finnie P and Homma Y (2000c) ‘Stability–instability transitions in silicon crystal growth’, Phys. Rev. Lett. 85, 3237–3240. Florio J V and Robertson W D (1970) ‘Phase transformations of the Si(111) surface’, Surf. Sci. 22, 459–464. Hibino H, Sumitomo K, Fukuda T, Homma Y and Ogino T (1998) ‘Disordering of Si(111) at high temperatures’, Phys.

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