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23<br />

SECTION IV. MAIN INJECTOR ERA<br />

With the Main Injector now well under construction, as can be seen in<br />

the <strong>Workbook</strong> cover photographs, much attention is turning to the physics<br />

opportunities that will become available upon completion of this 120/150 GeV<br />

high-intensity proton accelerator. Already one experiment using the Main<br />

Injector (E-803, neutrino oscillations - see Section VIII) has been approved,<br />

and planning for a proposed long-baseline neutrino oscillation experiment is<br />

well advanced.<br />

In this Section, we give some information on the expected Main Injector<br />

performance, and also preliminary estimates of some beam properties for<br />

experiments. Table 3 shows the number of 120 GeV protons/hour that can be<br />

expected from the Main Injector under various operating scenarios; the fast<br />

spill can be up to ....1 msec long, and slow spill will be one second. Figures 16,<br />

17, 18 show expected fluxes of some neutrino and secondary hadron beams<br />

using the Main Injector. Future editions of this <strong>Workbook</strong> will provide more<br />

information as it becomes available.<br />

It should be noted that there are some other future new experimental<br />

area possibilities under consideration at the present time. Examples are an<br />

experimental area to use 400 MeV protons from the Linac, and the use of the<br />

8 GeV Booster to produce a neutrino beam. Figure 19 gives a schematic<br />

illustration of some of these ideas.<br />

Of course, not to be overlooked is the major impetus for the Main<br />

Injector; it will increase the performance of the Tevatron, to luminosities of<br />

-lxI0 32 cm- 2 sec- 1 in the Collider mode, and to over 5xl013 protons per -20 sec<br />

spill every ....60 sec for fixed-target.

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