The MINOS CollaborationArgonne -Athens -Caltech -Chicago -Dubna -Fermilab -Harvard IHEP-Beijing -Indiana -ITEP-Moscow -Lebedev Livermore VCL-London Minnesota -Oxford -Pittsburgh -Protvino -Rutherford -Stanford -SussexTexas A&M -Texas-Austin -Tufts -Western Washington - Executive summaryThe MINOS (Main Injector Neutrino Oscillation Search) experiment is designed to search for neutrino oscillations with a sensitivity significantly greater than has been achieved to date. The phenomenon of neutrino oscillations, whose existence has not been proven convincingly so far, allows neutrinos of one "flavor" (type) to slowly transform themselves into another flavor, and then back again to the original flavor, as they propagate through space or matter.The MINOS experiment is optimized to explore the region of neutrino oscillation "para meter space" (values of the !:l.m 2 and sin 2 29 parameters) suggested by previous investigations of atmospheric neutrinos: the Kamiokande, 1MB, Super-Kamiokande and Soudan 2 experi ments. The study of oscillations in this region with a neutrino beam from the Main Injector requires measurements of the beam after a very long flight path. This in turn requires an intense neutrino beam and a massive detector in order to have an adequate event rate at a great distance from the source.We propose to enhance significantly the physics capabilities of the MINOS experiment by the addition of a Hybrid Emulsion Detector at Soudan, capable of unambigous identification of the neutrino flavor. Recent developments in emulsion experiments make such a detector possible, although significant technological challenges must be overcome. We propose to initiate an R&D effort to identify major potential problems and to develop practical solutions to them.In addition to this primary motivation for this R&D work, we note that the strong and growing interest in studies of neutrino oscillations using neutrino beams from future muon storage rings provides another potential application. These beams will offer significantly higher intensities, albeit of mixed 1I1J-and lie, beams. In order to take full advantage of these beams for neutrino oscillation studies it will be necessary that the detector be capable of determination of the flavor of the final state lepton, and the lepton's charge in a significant fraction of the interactions. At present, an emulsion detector in an external magnetic field appears best suited to offer such capabilities. The R&D effort discussed here will be an important step towards a design of such a future detector. This document is organized as follows:• Chapter 1 summarizes the physics motivation for the proposed emulsion detector,• Chapter 2 briefly reviews the status of the emulsion technology and its aplication to particle physics experiments,• Chapter 3 discusses design considerations for an emulsion detector,• Chapter 4 describes some of the details of a possible detector as well as results from the work up to date,• Chapter 5 outlines the proposed R&D program and summarizes the resources req...
Elastic scattering of hadrons on protons has been measured at momenta of 50, 100, and 200 GeV/c. The meson-proton scattering is found to be independent of momentum and meson type fort > 0.8 (GeV/c)'.The momentum dependence of the pp dip att = 1.4 (GeV/c)' was investigated. Slope parameters are given.
PHYSICAL REVIEW LETTERS 22 SEPTEMBER 1975 X Y 0 Akimov et al., "Proton-Deuteron Elastic Scattering at Small Momentum Transfer from 50 to 400 GeV/c" (to be published). 2 Y. Akimov et al 0i preceding Letter [Phys. Rev. Lett. 3J5, 763 (1975)]. 3 This is justified by the near factorization of the form factor in elastic scattering (Ref. 1) and by the factorization of the diffractive vertex in the low-mass region (Ref. 2). In a fit of our inelastic data where c was treated as a free parameter, we obtained c = 64 0 3± 11.4 (GeV/c)~4 in agreement with the (more accurate) value of 62.3 ± 1.1 given by the deuteron form factor.
3~o t hMonte Carlo-generated events for particular reactions a s well a s the real data, where it is possible to check this, indicate that there is little difference, generally less than 0.5 units, between 17 and the real longitudinal rapidity y = 4 ln[(E +p , , ) / ( E -prl)l.2"he different shapes of the data near v = 0 and near v = -6 result from the use of the pseudorapidity and the angle errors on the fast forward tracks.Measurements of ntp, K*p, pp, andpp elastic scattering a r e presented for incident momenta of 3, 3.65, 5, and 6 GeV/c and momentum transfers typically 0.03 to 1.8 Gev2. The q l e and momentum of the scattered particle were measured with the Argonne Effective Mass Spectrometer for 300 000 events, yielding 930 cross-section values with an uncertainty in absolute normalization of k4 %. Only the K + and proton data show any significant change in slope of the forward diffraction peak with incident momentum. The particle-antiparticle crossover positions are consistent with no energy dependence, average values being 0.14 10.03, 0.19010.006, and 0.162 +0.004 G~V ' for n's, K ' s , and protons, respectively; these e r r o r s reflect both statistics and the *1.5 % uncertainty in particle-antiparticle relative normalization. Differences between particle and antiparticle cross sections isolate interference terms between amplitudes of opposite C parity in the t channel; these differences indicate that the imaginary part of the odd-C nonflip-helicity amplitude has a ~~(r(-t)"') structure for -t ~0 . 8 Gev2, as predicted by strong absorption models. The cross-section differences for K * and proton-antiproton a r e in qualitative agreement with the predictions of w universality, the agreement improving with increasing energy. The corresponding quark-model predictions relating the n* and K* differences failed by more than a factor of 2. We have combined our r * cross sections with other data to better determine the nN amplitudes in a model-independent way; results of this analysis a r e presented.
A search for GUT magnetic monopoles has been conducted using the Soudan i-,.. 2 nucleon decay detector. This detector is a fine-grained tracking calorimeter. Monopole candidates were selected on the basis of significantly higher ionization .. than throughgoin9 cosmic ray muons. Preliminary results, using data taken over " approzimately one year with no monopoles observed, correspond to a flux limit of 2.4 10-14cm-28r-ls-1 over a velocity range of 10-3 3 < 0.95.
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