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The advent in the 1970s of synchrotrons that were capable of delivering beams of all elements with very high energies allowed the production of the same exotic nuclei observed as target residues with suf cient kinetic energies to allow rapid physical separation and identi cation This technique is usually called the projectile fragmentation technique but more correctly might be referred to as in- ight separation since other reaction mechanisms besides projectile fragmentation can be used to produce the nuclei (Fig 1413) The beams of exotic nuclei are not stopped in this technique, and even very short-lived nuclei can be studied and used to induce secondary reactions In the mid-1970s it was shown that up to 1% of a primary 12C beam could be converted into 11C ions and separated for implantation into biomedical samples.

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Nuclear physics experiments to produce exotic nuclei and calibrate space- ight instruments using similar techniques based on magnetic rigidity were also pioneered with beam-line elements at LBL (Berkeley, California) and then dramatically extended by using degraders (the LISE spectrometer at GANIL (Caen, France)) This technique has been further extended in four second-generation devices distributed around the world and third-generation devices at the NSCL (Michigan State) and at RIKEN (Japan) Fast-ion beams of exotic nuclei are separated from the primary beam and from the other reaction products by a combination of separated function magnetic bending dipoles and focusing quadrupole doublets acting on the distribution of ions emerging from the target at high velocities (b 05c) Achromatic magnetic systems are used, where achromatic means that the position and angle of ions at the end of the device (called the focal plane) does not depend on the ion s momentum.

Such achromatic magnetic systems are generally most useful for ef cient.

The text wraps oddly because of this book s formatting constraints. You can also feed readkey.c input from stdin using the cat command:

Using the beta function property [36, Eq. (8.384.1), p. 959] B(l, L l + 1) = (l) (L l + 1) (l 1)!(L l)! = (L + 1) L! (9E.6)

for JNDI-provider classes you can check Sun s listing at http://java.sun.com/ products/jndi/serviceproviders.html. This section covers the following JNDI service providers: File systems COS naming for CORBA Network Information System (NIS) Directory Services Markup Language (DSML) Application-server providers

For the countercurrent configuration the optimal heat capacity ratio converges asymptotically to h = 1 with increasing NTU values. Even for an ideal heat exchanger ), small deviations from the optimal heat capacity ratio cause significant (NTU heat losses. On the other hand, heat losses could be minimized with decreasing heat capacity ratio and increasing NTU values for the counter-cocurrent configuration. In this case the heat recovery becomes complete for an ideal heat exchanger ) independent of the heat capacity ratio h. (NTU

which agrees with the expression attributed to Barrow [34] and later reported by Wojnar [22, Eq. (2.38)] and Crepeau [35, Eq. (B1)]. For DQPSK, the average BEP is evaluated from (8.205) as Pb (E) = 1 2 m m + 2

Another approach is the three-tier architecture, which is discussed in greater detail later. While some of its benefits were already explained, this approach solves what might be the applet s biggest problem. Eventually, the applet makes a connection to the third tier and requests or calls an action on a particular object. This request should trigger a conversation between the third tier and the database management system. In this case, connection information like database identification may be excluded from the applet s code. Figure 4-5 depicts such a three-tiered architecture.

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