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3.2 Performance at Dane .

 

To predict how good the tests could be at Dane , we consider an experiment lasting one year with 30% efficiency, (i.e. effective duration 10 s.) at the luminosity cms. The integrated luminosity is 10 000 pb. In that time, neutral-kaon pairs are expected to be produced.

For both kaons decaying into , using the kaon data of Ref. [7], we compute

  

We assume the background due to misidentified events in the sample to be no more than what can be tolerated in a measurement of , i.e. let us say 10 of the rate into . To that we add the -background and yet another contribution, equivalent to background, due to the measurement error on the vertex positions of the two kaon decays. The latter effect generates uncertainties and in the determinations of the proper times and , thus in z, and populates the region around z = 0. We will assume that the sample of events can be limited to events where the vertex uncertainty is 1 mm in average. Then the uncertainty in z is .

Assuming that the contribution of these backgrounds is known within 10% and can be subtracted off with that 10% uncertainty, we find, in the case of no violation, that the systematic error is about equal to the statistical error, given by Eqs. (18) and (20).

It follows that this test would explore possible values of as small as one or two 10. This value is better than the one given in Ref. [6] in the context of neutron interferometry. Even smaller values of can be detected if the vertex accuracy can be improved.

A similar calculation can be made for the case where both kaons decay into or both into . Predictions of the performance at Dane are less reliable than for the --decays because the background due to misidentified events is more difficult to estimate at this point in time. The background contributes to for much less than because of the limited acceptance of the detector for -decays. That background is totally negligible. Assuming that, as for the --mode, the background is dominated by the effect of the vertex position uncertainty, we get

 

for each of the two modes and . This value of would permit exploring values of and of comparable to the value estimated for the --mode, i.e. a few 10. Of course, if a violation is found, questions will be raised about the rule that was assumed to justify the test with leptons in the final state. However studies of correlations between regions of the --Dalitz plot will permit us to distinguish a violation of quantum mechanics from a violation of the rule.



next up previous contents
Next: 3.3 events Up: 3 Two-Kaon Systems. Previous: 3.1 Predictions and Errors.



Carlos E.Piedrafita