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137<br />

E-815 (Bernstein / Shaevitz) Precision Measurements ofNeutrino Neutral<br />

CmTent Interactions Using a Sign-SelectedBeam<br />

Adelphi, Cincinnati, Columbia, Fermilab,<br />

Kansas State, Oregon, Rochester, Xavier<br />

IStatus: No Data YetI<br />

A major physics goal of the 1990's will be precision tests of the<br />

electroweak sector of the Standard Model. The Standard Model makes definite<br />

predictions which can be confirmed or refuted with sufficiently precise<br />

measurements. Comparing the value of sin 2 9w measured in e+e- collisions at<br />

the ZO pole, at hadron colliders, and in deep-inelastic neutrino-nucleon<br />

scattering tests the radiative corrections to the Standard Model and allows us<br />

to search for physics beyond it.<br />

E-815 (NuTeV) will exploit the full power of the high-energy, highintensity<br />

Tevatron neutrino beam to significantly improve the precision of the<br />

measurements of the electroweak parameters. The new sign-selected beam<br />

will enable us to measure neutrino and anti-neutrino interactions separately.<br />

This has two significant advantages: (1) previously limiting systematic errors<br />

can be eliminated or reduced, and (2) sign-selection will provide the first<br />

precision measurement of p. The value of p, the ratio of neutral-to-charged<br />

current coupling strengths, reflects the structure of the Higgs sector so a<br />

precise determination of p is a powerful probe of the nature of electroweak<br />

unification. Furthermore, both p and sin 29w are radiatively corrected by mt in<br />

a known way. Hence before the discovery of the top quark, the electroweak<br />

measurements can predict its mass; after mt has been directly measured,<br />

requiring consistency between the predicted and measured values is a<br />

stringent test ofthe Standard Model.<br />

NuTeV will yield a measurement of (1) sin 29w with an expected error of<br />

o(sin 29w) = ±0.0025 (statistical and systematic errors combined), and (2) p with<br />

an error of ±0.0054, a factor of six improvement over existing data. These<br />

errors can be compared to measurements of mt or Mw; the corresponding<br />

error on mt is 30 GeV/c 2 and only 130 MeV/c 2 on Mw, competitive with the<br />

expectations from the collider measurements. The vN measurements have a<br />

unique dependence on the radiative corrections and are the only<br />

measurements which directly determine both sin 29w and p.<br />

Neutrino-nucleon scattering has always been a rich source of<br />

information on the structure of nucleons and tests of QeD and NuTeV will<br />

build on that tradition. We will use our experience from E-744/E-770 to reduce<br />

the systematic errors on as and AQCD through the use of an extensive test beam<br />

program for calibrating the apparatus. E-744/E-770 has already provided the<br />

best measurement of as(Mz); NuTeV can reduce that error by nearly a factor of<br />

two. In addition, the sign-selected beam will allow us to make more precise

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