NSR Query Results
Output year order : Descending NSR database version of May 10, 2024. Search: Author = W.Kanert Found 14 matches. 1993SU06 Nucl.Phys. A554, 223 (1993) A.S.Sudov, A.S.Botvina, A.S.Iljinov, Ye.S.Golubeva, V.G.Nedorezov, H.Daniel, T.von Egidy, F.J.Hartmann, P.Hofmann, W.Kanert, H.S.Plendl, G.Schmidt, C.A.Schug, G.Riepe Production of Light Particles After Antiproton-Nucleus Annihilation and Their Interpretation with Statistical Models NUCLEAR REACTIONS 6,7Li, Si, 40Ca, 58,64Ni, 70Ge, 98Mo, 165Ho, 208Pb, 232Th, 174Yb(p-bar, X), E at rest; measured proton, deuteron, triton spectra, yields; deduced reaction mechanism mass dependence features. Different models.
doi: 10.1016/0375-9474(93)90340-4
1993WY03 Nucl.Phys. A561, 607 (1993) S.Wycech, F.J.Hartmann, H.Daniel, W.Kanert, H.S.Plendl, T.von Egidy, J.J.Reidy, M.Nicholas, L.A.Redmond, H.Koch, A.Kreissl, H.Poth, D.Rohmann Antiprotonic Atoms with Heavy Nuclei NUCLEAR REACTIONS 126,130Te, 150,152Sm, 194,196Pt, 94,98Mo(p-bar, X), E=low; measured X-ray spectra; deduced optical potential features, atomic level widths, shifts. ATOMIC PHYSICS 126,130Te, 150,152Sm, 194,196Pt, 94,98Mo(p-bar, X), E=low; measured X-ray spectra; deduced optical potential features, atomic level widths, shifts.
doi: 10.1016/0375-9474(93)90068-9
1992MA32 Z.Phys. A343, 73 (1992) H.Machner, S.Jun, G.Riepe, D.Protic, H.Daniel, T.von Egidy, F.J.Hartmann, W.Kanert, W.Markiel, H.S.Plendl, K.Ziock, R.Marshall, J.J.Reidy Fission Fragment Distribution following Antiproton Absorption at Rest on 238U NUCLEAR REACTIONS 238U(p-bar, F), E at rest; measured fission fragment yields; deduced fission probability, product charge, mass distribution features. Off-line residual radioactivity measurement.
doi: 10.1007/BF01291600
1990HO11 Nucl.Phys. A512, 669 (1990) P.Hofmann, F.J.Hartmann, H.Daniel, T.von Egidy, W.Kanert, W.Markiel, H.S.Plendl, H.Machner, G.Riepe, D.Protic, K.Ziock, R.Marshall, J.J.Reidy Charged-Particle Spectra from Antiproton Annihilation at Rest in A = 12-238 Nuclei NUCLEAR REACTIONS 12C, 40Ca, 63Cu, 92,98Mo, 238U(p-bar, X), E at rest; measured spectra, yields of p, d, t; deduced emission processes, shape of spectra. Ge telescope, enriched targets.
doi: 10.1016/0375-9474(90)90229-F
1990VO03 Z.Phys. A335, 451 (1990) T.von Egidy, H.Daniel, F.J.Hartmann, W.Kanert, E.F.Moser, Ye.S.Golubeva, A.S.Iljinov, J.J.Reidy Yield of Residual Nuclei after Antiproton Annihilation in Ba NUCLEAR REACTIONS Ba(p-bar, X), E at rest; measured residual yields for 87Y-132Ce. Induced activity, Ba(NO3)2 target.
1989MO04 Z.Phys. A333, 89 (1989) E.F.Moser, H.Daniel, T.von Egidy, F.J.Hartmann, W.Kanert, G.Schmidt, Ye.S.Golubeva, A.S.Iljinov, M.Nicholas, J.J.Reidy Residual Nuclei After Antiproton Annihilation in Mo and Ho NUCLEAR REACTIONS 92,95,98Mo, 165Ho(p-bar, X), E at rest; measured residual yields for X=62Zn-159Tm; deduced annihilation mechanism. Induced radioactivity method.
1988KR04 Z.Phys. A329, 235 (1988) A.Kreissl, A.D.Hancock, H.Koch, Th.Kohler, H.Poth, U.Raich, D.Rohmann, A.Wolf, L.Tauscher, A.Nilsson, M.Suffert, M.Chardalas, S.Dedoussis, H.Daniel, T.von Egidy, F.J.Hartmann, W.Kanert, H.Plendl, G.Schmidt, J.J.Reidy First Direct Observation of Strong Interaction Spin-Orbit Effects in Antiprotonic Atoms ATOMIC PHYSICS 174Yb, 138Ba(p-bar, X), E not given; measured X-ray spectra; deduced strong interaction spin-orbit effects, energy shifts, widths.
1988MA44 Nucl.Phys. A485, 445 (1988) W.Markiel, H.Daniel, T.von Egidy, F.J.Hartmann, P.Hofmann, W.Kanert, H.S.Plendl, K.Ziock, R.Marshall, H.Machner, G.Riepe, J.J.Reidy Emission of Helium Ions after Antiproton Annihilation in Nuclei NUCLEAR REACTIONS 12C, 40Ca, 63Cu, 92,98Mo, 238U(p-bar, 3He), (p-bar, α), E at rest; measured spectra; deduced spectrum shape, yields. Si particle telescope, enriched targets.
doi: 10.1016/0375-9474(88)90547-7
1987DA10 Z.Phys. A326, 523 (1987) H.Daniel, F.J.Hartmann, W.Kanert, H.Plendl, T.von Egidy, J.J.Reidy, H.Koch, A.Kreissl, H.Poth, D.Rohmann Strong-Interaction Fine Structure Effects in Antiprotonic 148Nd NUCLEAR REACTIONS 146,148Nd(p-bar, X), E=300 MeV/c; measured X-ray spectra; deduced p-bar-nucleus potential. Enriched targets, Ge detectors.
1987PO05 Nucl.Phys. A466, 667 (1987) H.Poth, H.Barth, G.Buche, A.D.Hancock, H.Koch, Th.Kohler, A.Kreissl, U.Raich, D.Rohmann, A.Wolf, L.Tauscher, A.Nilsson, M.Suffert, M.Chardalas, S.Dedoussis, H.Daniel, T.von Egidy, F.J.Hartmann, W.Kanert, H.S.Plendl, G.Schmidt, J.J.Reidy Measurement of Strong-Interaction Effects in Light Antiprotonic Atoms ATOMIC PHYSICS 6,7Li, 14N, 19F, 23Na(p-bar, X), E at 300 MeV/c; measured X-ray spectra. 7,6Li, 14N, 19F, 23Na deduced antiprotonic strong interaction level shifts, widths.
doi: 10.1016/0375-9474(87)90462-3
1986KA08 Phys.Rev.Lett. 56, 2368 (1986) W.Kanert, F.J.Hartmann, H.Daniel, E.Moser, G.Schmidt, T.von Egidy, J.J.Reidy, M.Nicholas, M.Leon, H.Poth, G.Buche, A.D.Hancock, H.Koch, Th.Kohler, A.Kreissl, U.Raich, D.Rohmann, M.Chardalas, S.Dedoussis, M.Suffert, A.Nilsson First Observation of the E2 Nuclear-Resonance Effect in Antiprotonic Atoms ATOMIC PHYSICS 92,94,95,98,100Mo(p-bar, X), E at 200, 300 MeV/c; measured antiprotonic X-ray spectra; deduced strong interaction widths, shifts, effective (p-bar)-nucleon scattering length, E2 nuclear resonance effect.
doi: 10.1103/PhysRevLett.56.2368
1986KO22 Phys.Lett. 176B, 327 (1986) Th.Kohler, P.Blum, G.Buche, A.D.Hancock, H.Koch, A.Kreissl, H.Poth, U.Raich, D.Rohmann, G.Backenstoss, Ch.Findeisen, J.Repond, L.Tauscher, A.Nilsson, S.Carius, M.Suffert, S.Charalambus, M.Chardalas, S.Dedoussis, H.Daniel, T.von Egidy, F.J.Hartmann, W.Kanert, G.Schmidt, J.J.Reidy, M.Nicholas, A.Wolf Precision Measurement of Strong Interaction Isotope Effects in Antiprotonic 16O, 17O, and 18O Atoms NUCLEAR REACTIONS 16,17,18O(p-bar, X), E=low; measured antiprotonic X-rays. ATOMIC PHYSICS 16,17,18O(p-bar, X), E=low; measured antiprotonic X-rays; deduced strong interaction shifts, widths.
doi: 10.1016/0370-2693(86)90173-5
1986MO20 Phys.Lett. 179B, 25 (1986) E.F.Moser, H.Daniel, T.von Egidy, F.J.Hartmann, W.Kanert, G.Schmidt, M.Nicholas, J.J.Reidy Yields of Residual Nuclei after Antiproton Annihilation in 95Mo and 98Mo NUCLEAR REACTIONS 95,98Mo(p-bar, X)93Mo/90Mo/97Nb/96Nb/95Nb/92Nb/90Nb/89Nb/95Zr/89Zr/88Zr/86Zr/90Y/88Y/87Y/86Y/85Y/84Y/85Sr/83Sr/81Sr/84Rb/83Rb/82Rb/81Rb/79Rb/79Kr/77Kr/76Kr/80Br/77Br/76Br/75Br/74Br/75Se/73Se/72Se/74As/72As/71As/69Ge/67Ga/66Ga, E=200 MeV; measured residual nuclei absolute yields. Activation method.
doi: 10.1016/0370-2693(86)90429-6
1986RO23 Z.Phys. A325, 261 (1986) D.Rohmann, H.Barth, A.D.Hancock, H.Koch, Th.Kohler, A.Kreissl, H.Poth, U.Raich, A.Wolf, L.Tauscher, M.Suffert, M.Chardalas, S.Dedoussis, A.Nilsson, W.Kanert, T.von Egidy, F.J.Hartmann, G.Schmidt, J.J.Reidy Measurement of the 4f Strong Interaction Level Width in Light Antiprotonic Atoms NUCLEAR REACTIONS 14N, 16,17,18O, 19F, 23Na(p-bar, X), E=200, 300 MeV/c; measured antiprotomic X-ray spectra; deduced target atomic 4f level Γ; calculated antiprotonic transition intensities. Scintillation counters. Cascade model. ATOMIC PHYSICS 14N, 16,17,18O, 19F, 23Na(p-bar, X), E=200, 300 MeV/c; measured antiprotonic X-ray spectra. 14N, 16,17,18O, 19F, 23Na deduced 4f level Γ; calculated antiprotonic transition intensities. Scintillator counters. Cascade model.
Back to query form |