A search for nuclear-bound states of the 77 meson has been carried out. Targets of lithium, carbon, oxygen, and aluminum were placed in a /r"^ beam at 800 MeV/c. A predicted T] bound state in ^^O* {Ex « 540 MeV) with a width of « 9 MeV was not observed. A bound state of a size j of the predicted cross section would have been seen in this experiment at a confidence level of 3CT {P> 0.9987).PACS numbers: 25.80.-e, 21.90.+f, 27.20.+n This Letter describes a search for a novel nuclear excitation involving the creation of a bound r] meson in the nuclear medium. The concept is similar in spirit to a number of ideas which have recently been vigorously pursued. Some familiar examples are A hypernuclear states, Z hypernuclear states, antiprotonic nuclear states, and various dibaryon resonances. In each case an attractive particle-nucleus potential is required together with some mechanism to inhibit the decay process, such as strangeness conservation in the case of the A.Several suggestions of the existence of bound states of the 7] meson in a wide range of nuclei have recently been published. ^"^ The suggestions of this novel nuclear excitation are based on bound-state formation through the attractive N-T] channel of the TV* (1535), where A^*(1535) is the {KN) resonance with (/,/'') = (T, y") and mass 1535 MeV/c^. This resonance dominates 77 production near threshold. Bhalerao and Liu'* have shown, by a coupled-channels analysis, that the lowenergy rfN interaction is attractive with a scattering length of 0.28 + 0.202/ fm. The attractive interaction is a consequence of the threshold being below the A^*(1535) resonance.Liu and his collaborators have examined the consequences of this attractive interaction in the formation of a bound-77 state as a function of mass number. Their study indicates that nuclear bound states could exist for mass numbers larger than A^\Q. At low mass numbers, only 5-state bound r/'s are predicted. At larger mass numbers, p and d states could become bound. Both binding energies and widths increase with A. The optimum case, in their analysis, is \^0, formed from the in^.p) reaction on *^0 at a momentum near 740 MeV/c. ^ At an angle near 15°, the momentum transfer is favorable for the transition involving the conversion of a p-shell neutron to an ^-shell ry. For higher mass numbers, the increase in predicted width would make this excitation more difficult to see over the continuum {K^,p) background which is present.An experiment to test these predictions was devised with the positive pion beam available at the low-energy separated beam I at the Brookhaven alternating-gradient synchrotron (AGS), and the Moby Dick spectrometer. The experimental arrangement is virtually identical with that used for the production and measurement of hypernuclei, and it has been described in detail in a number of publications (see Milner et al.^ and related references). The only differences involve the selection of pions, rather

Data obtained by the associated production of A hypernuclei through the (n + ,K + ) reaction are presented for a wide range of mass numbers. The special features which make this reaction useful are pointed out. The reaction is shown to be an excellent probe of A single-particle states, as demonstrated by the excitation of deeply bound states which are interpreted as the weak coupling of a A to neutronhole states of the core. The A binding energies and ground-state production cross sections for JvBe, 'AC, '&>, 2 2Si, ^Ca, 5 A V, and ^Y are presented.

A search for S hypernuclear states in p-shell hypernuclei has been performed with the Moby Dick spectrometer and the low energy separated beam (LESB-2) at the Brookhaven Alternating Gradient Synchrotron (BNL AGS). Unlike some previously published reports, no narrow states have been observed for targets of 6 Li and 9 Be in ͑K 2 , p 6 ͒ reactions, either for bound state or continuum regions. Together with the previously reported J 0, T 1͞2 bound state in 4 S He, these results demonstrate the crucial role of isospin in S hypernuclei.

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Results from I(, +elastic and inelastic scattering from ' C and Ca are reported. The data were all taken at an incident momentum of 800 MeV/c over an angular range from 2' to 38'. The elastic data are compared to first-order optical model calculations in coordinate and momentum space; good qualitative agreement is obtained. The inelastic data (from ' C only) are compared to distorted-wave Born approximation calculations, and good agreement is found if "realistic" inelastic transition densities are used. Although a first-order optical potential description does not describe the data fully, there are strong indications of the increased penetrability of K+ over E in this energy range. NUCLEAR REACTIONS ' C(E -E )' C Ca(-E , IC )Ca, F--=442 MeV (800 MeV/c), measured o. (I9) for elastic and inelastic scattering, compared to optical model and DWBA calculations, deduced optical potential parameters; 8=2' -38', 68= 1'.

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A 8 O, excited by 800-MeV/c kaons in the (K" 9 n~) reaction, have been observed at the Brookhaven alternating-gradient synchrotron. Data were recorded for scattering angles from 0° to 25°, corresponding to momentum transfers from 50 to 330 MeV/c. The levels are interpreted in terms of a A hyperon coupled to a strangeness-zero nuclear core. The results provide insights into the properties of the A-nucleon and A-nucleus interactions.