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lengths had not been implemented when these data were collected, so some residual asymmetry can be observed in the pro les. Later measurements at 527 nm show a further reduction in the relative piston phase offset errors (Fig. 5.36). 5.5.3.3 Second harmonic conversion of the phase-locked array The frequency doubler for the 100-J/pulse phase-locked laser system is a scaled version of that used for the 30-J/pulse 500-ns laser. The width of the 458 beam shaping prisms and the KD P doubler crystals was increased to accommodate the four phaselocked beams, side by side. A dichroic mirror outside of the laser enclosure is used to separate the unconverted 1053-nm light from the 527-nm beam. As shown in the optical layout of Fig. 5.27, the unconverted light is transmitted through the dichroic and emerges as a 25 100-mm2 array of four beamlets. The 527-nm output is reformatted to a square 50 50-mm2 array using a nal anamorphic beamreshaping telescope. This provides a circularly symmetric far eld central lobe for the array of four phased-locked 12 50-mm2 beamlets. A typical external conversion ef ciency of . 60% was obtained at up to 25 J/ pulse with 500-ns pulse durations. Figure 5.34 shows an external frequency conversion ef ciency curve measured for a single beamlet using one doubler crystal and two crystals in the alternating-Z geometry [41]. The measured ef ciency includes the re ective losses from the prism and KD P surfaces. Figure 5.35 shows a measured near- eld pro le at 527 nm, 50 J/pulse, and 3 Hz after reshaping by the nal anamorphic telescope. Slightly less energy is typically present in the outside

No matter how slowly this squeeze is carried out, motion near the unstable fixed points will fail to be adiabatic; for in the neighborhood of these points motion becomes arbitrarily slow in the static case Particles depart the stable area at the fixed points and stream out along the outgoing arms of the separatrix But the continuum in amplitudes of these outgoing particles leads to beam loss, since somewhere there has to be a device that is the start of the channel for departing particles The partition, or septum, between in and out particles must be as thin as possible in order to obtain high extraction efficiency At present, the thin septa are electrostatic.

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measured sagitta is z, the radius of curvature R of the surface is given by: (Cooke, 1964) z y2 17:2 R r 2 2z where r is the radius of curvature of the balls. The plus sign is used for concave surfaces, and the minus sign for convex surfaces. The precision of this instrument may be obtained by differentiating Eq. (17.2), as follows: dR 1 y2 DZ 2 2z2 to obtain: z y2 1 2 R 2 z 17:4 17:3

When the ultimate feature sizes of nanoscale objects are approximately a nanometer or so, one is dealing with dimensions an order of magnitude larger than the scale exploited by chemists for over a century. Synthetic chemists have manipulated the constituents, bonding, and stereochemistry of vast numbers of molecules on the angstrom scale, and physical and analytical chemists have examined the properties of these molecules. So what is so special about the nanoscale There are many answers to this question, possibly as many as there are people who call themselves nanoscientists or nanotechnologists. A particularly intriguing feature of the nanoscale is that this is the scale on which

They are not strong enough to fling particles out of the ring, but they can establish enough of a gap between in and out particles so that a second, stronger magnetic septum can direct particles into an exit channel The great virtue of the electrostatic septum is that the obstacle presented to the beam is very small, about 50 pm For a proton accelerator with conventional magnets, it is already important that the losses off the primary extraction septum be minimized: the buildup of radioactivity in the ring is a major concern for operation and maintenance For a proton accelerator using superconducting magnets, control of the septum loss is essential to avoid excessive energy deposition in the magnets with the attendant risk of superconducting to normal transition; that is, the extraction process brings with it the danger of a quench The third integer resonance can be used for slow extraction.

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