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You may consider adding a few environment variables to your .bashrc file. These can help make working with the shell more efficient and effective: TMOUT Sets how long the shell can be inactive before bash automatically exits. The value is the number of seconds for which the shell has not received input. This can be a nice security feature, in case you leave your desk while you are still logged in to Linux. So as not to be logged off while you are working, you may want to set the value to something like TMOUT=1800 (to allow 30 minutes of idle time). PATH As described earlier, the PATH variable sets the directories that are searched for commands you use. If you often use directories of commands that are not in your PATH, you can permanently add them. To do this, add a PATH variable to your .bashrc file. For example, to add a directory called /getstuff/bin, add the following:

an alkali halide or more recently, carbon clusters, to which charged reaction product recoils attach themselves via van der Waals forces The helium gas (and the aerosol particles) escapes through a small ori ce to a vacuum chamber, with the gas achieving sonic velocity The gas and aerosol can be transported for substantial distances in thin capillary tubes The aerosol particles (and the attached atoms) are collected by allowing the gas stream to strike a collector surface The resulting deposit can be counted directly or dissolved for further chemical processing The aerosol loaded gas stream (jet) can also be used to transport the atoms through a thin capillary a distance of several meters in a few seconds If the aerosol particles are carbon clusters, they can be burned in oxygen, freeing the transportal activity.

If the carrier gas is extremely pure helium gas, then the residues will remain ionized and can be collected using electrostatic devices A number of systems have been developed and used to collect reaction products as ions without involving aerosols in the carrier gas The principal limitation of the isolation devices discussed previously (tapes, jets, etc) is that the reaction product must be stopped and mechanically transported to radiation detectors before product identi cation can occur This restricts their use to studies of nuclei whose t1 1 ms For detection and identi cation of species 2 whose t1 , 1 ms, one employs instruments based upon direct magnetic and/or elec2 trostatic de ection of target recoils The most spectacularly successful of these devices is the velocity lter SHIP (Fig 157).

Within each area, every PE router has an RSVP-TE LSP created to the ABR. LDP is enabled in all the PE s router interfaces and the ABR s router interfaces. With LDPoRSVP in the network, PE routers in different areas (PE1 and PE2 at the right in Figure 8.8) use three RSVP-TE LSPs to carry traffic end-to-end: Intra-area RSVP-TE LSP in PE1 s area RSVP-TE LSP in the backbone area between two ABRs Intra-area RSVP-TE LSP in PE2 s area These three RSVP-TE LSPs are stitched together by the LDPoRSVP and form an end-to-end LDP-LSP. With such an LDPoRSVP implementation, the overall number of RSVP-TE LSPs in the entire network drops significantly: Within each area, every PE router still requires 38 (2 * 19) intra-area LSPs to connect to all PE routers in its area. Every PE router also requires one pair of LSPs connected to the ABR. LSP is unidirectional; two routers require two LSPs, one at each direction to pass traffic between them.

Evaporation residues produced in compound nucleus reactions emerge from the target and pass through a thin carbon foil that has the effect of equilibrating the ionic charge distribution of the residues The ions then pass through two lter stages consisting of electric de ectors, dipole magnets, and a quadruple triplet for focusing The solid angle of acceptance of the separator is 27 msr with a separation time for the reaction products of 2 ms with a total ef ciency of collecting evaporation residues of 20% for Aproj 40 Since complete fusion evaporation residues have very different velocities and angular distributions than targetlike transfer and deep-inelastic products (a factor of 2 difference in velocity between transfer products and evaporation residues) and beam nuclei, the separator with its +5% velocity acceptance range and narrow angular acceptance very effectively separates the evaporation residues from the other reaction products and the beam.