Abstract

A new type of nuclear spectroscopy to study hadron-nucleus bound states is described. The first successful experiment was to search for deeply bound π − states in heavy nuclei using the 208Pb(d, 3He) reaction at GSI, in which a narrow peak arising from the 2p π − orbital coupled with the neutron-hole states was observed at 135 MeV excitation energy. An improved experiment has just been carried out to separately identify the 1s and 2p π − states. These experiments provide important information on the local potential strength, from which the effective mass of π − is deduced to be 20 MeV. This method will be extended to search for η and ω bound states as well as for K − bound states. The advantage of the bound-state spectroscopy versus invariant mass spectroscopy is emphasized.

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