We reexamine a symmetry in nucleon-nucleus scattering that previously had been proclaimed to be dead. We show that this symmetry is the continuum analog of pseudospin symmetry, a relativistic symmetry which manifests itself in the spectra of nuclei. Using experimental data only, we show that pseudospin symmetry in nucleon-nucleus scattering is not dead but only modestly broken for 800 MeV proton scattering on nuclei. [S0031-9007(99)09284-4] PACS numbers: 25.40.Cm, 24.10.Ht, 24.10.Jv, 24.80. + y For nucleons moving in a relativistic mean field with scalar V S and vector potentials V V , an SU(2) symmetry exists for the case for which V S 2V V [1]. This symmetry manifests itself in nuclear spectra as a slightly broken symmetry [2-5] since j V S 1V V V S 2V V j is small for realistic mean fields [6-9] and QCD sum rules [10], and, in fact, gives rise to what has been called "pseudospin symmetry." The original observations that led to the coining of the term pseudospin symmetry were quasidegeneracies in spherical shell model orbitals with nonrelativistic quantum numbers ͑n r , ᐉ, j ᐉ 1 1͞2͒ and ͑n r 2 1, ᐉ 1 2, j ᐉ 1 3͞2͒, where n r , ᐉ, and j are the single-nucleon radial, orbital, and total angular momentum quantum numbers, respectively [11,12]. This doublet structure is expressed in terms of a "pseudo" orbital angular momentumᐉ ᐉ 1 1, the average of the orbital angular momentum of the two states in doublet, and pseudospin,s 1͞2. For example, ͓n r s 1͞2 , ͑n r 2 1͒d 3͞2 ͔ will haveᐉ 1; ͓n r p 3͞2 , ͑n r 2 1͒f 5͞2 ͔ will haveᐉ 2, etc. These doublets are almost degenerate with respect to pseudospin, since j ᐉ 6s for the two states in the doublet. Pseudospin "symmetry" was shown to exist in deformed nuclei as well [13,14] and has been used to explain features of deformed nuclei, including superdeformation [15] and identical bands [16,17]. However, the origin of pseudospin symmetry remained a mystery and "no deeper understanding of the origin of these (approximate) degeneracies" existed [18]. The source of pseudospin symmetry as a broken relativistic symmetry of the Dirac Hamiltonian with V S ഠ 2V V was pointed out [2][3][4][5]. For spherical nuclei, pseudo-orbital angular momentumᐉ is also conserved and physically is the "orbital angular momentum" of the lower component of the Dirac wave function.One consequence of this relativistic SU(2) pseudospin symmetry is that the spatial wave function for the lower component of the Dirac wave functions will be equal in shape and magnitude for the two states in the doublet. This has been shown to be approximately valid for realistic relativistic mean fields [3][4][5]9]. Recently this approximate equality has been applied to predicting relationships between magnetic dipole properties of the nucleus and between Gamow-Teller decays [19].For nuclear bound states the scalar and vector relativistic potentials are real. However, this symmetry exists for complex mean fields as well, that is, for the scattering of nucleons in the mean field of a nucleus. In fact, proton scattering on n...