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NSR database version of May 3, 2024.

Search: Author = H.Jungclas

Found 12 matches.

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1989KO03      Phys.Rev. C39, 687 (1989)

E.A.Koop, G.Feige, L.Schmidt, H.Jungclas, R.Brandt, G.Ingold, D.C.Hoffman

Direct Measurements of Neutron Emission in Complete and Incomplete 12C-Induced Fusion Reactions

NUCLEAR REACTIONS 197Au, 209Bi, 232Th, 238U(12C, X), (12C, F), E=120 MeV; measured neutron multiplicity following incomplete fusion, fission; deduced average neutron multiplicity, fission mechanism.

doi: 10.1103/PhysRevC.39.687
Citations: PlumX Metrics


1983FA03      Nucl.Instrum.Methods 206, 317 (1983)

R.Fass, P.Lemmertz, L.J.Alquist, H.Wollnik, D.Hirdes, H.Jungclas

On-Line Mass Determination of α-Active Products from the Reaction (nat)U + 208Pb with a Gas Jet Time-of-Flight Mass Spectrometer

NUCLEAR REACTIONS U, Ar(208Pb, αX)150Dy/151Dy/152Dy/151Ho/152Ho/152mHo/159Hf/155Yb/163W/159Ta/209At/207At/211At/217At/216At/215At/225Ac/192Bi/211Bi/212Bi/212mBi/218Po/217Po/216Po/211Po/211mPo/214Po/213Po/212Po/212mPo/221Fr/212Fr/211Fr/213Fr/219Fr/218Fr/226Th/225Th/223Th/213Ra/221Ra/224Ra/222Ra/214Ra/220Rn/217Rn/213Rn, E=7 MeV/nucleon; measured Eα, Iα, αγ-coin, α-recoil masses; deduced production σ ratios, masses for certain residuals. Gas jet Tof mass spectrometer, Ti window, Ar gas thermalization, natural U target.

doi: 10.1016/0167-5087(83)91275-9
Citations: PlumX Metrics


1981LU06      Z.Phys. A303, 115 (1981)

T.Lund, D.Hirdes, H.Jungclas, D.Molzahn, P.Vater, R.Brandt, P.Lemmertz, R.Fass, H.Wollnik, H.Gaggeler

Search for Production of Superheavy Elements via ' Fusion after Instantaneous Fission ' in the Reaction 238U + 208Pb

RADIOACTIVITY, Fission 254Cf(SF), 240,242m,244mAm(SF) [from 238U(208Pb, X), E=8 MeV/nucleon]; measured fragment distribution. Gas jet, fission track counting techniques.

NUCLEAR REACTIONS, Fission 238U(208Pb, X), E=8 MeV/nucleon; measured Eα, Iα, SF fragment distribution, α(fragment)-coin; deduced production yields for 240,242,244Cm, 254Cf, superheavy production σ. Radiochemical, gas jet, rotating wheel techniques, natural target.

doi: 10.1007/BF01420268
Citations: PlumX Metrics


1980LE27      Z.Phys. A298, 311 (1980)

P.Lemmertz, L.J.Alquist, R.Fass, H.Wollnik, D.Hirdes, H.Jungclas, R.Brandt, D.Schardt, J.Zylicz

Studies on Low Spin Yrast States in 212mPo

RADIOACTIVITY 212Bi [from U(208Pb, X), E=7 MeV/nucleon]; measured Eγ, Eα, αγ-coin; deduced log ft. 212Po deduced levels, T1/2, low-spin yrast band, configuration.

doi: 10.1007/BF01425163
Citations: PlumX Metrics


1978DE34      Nucl.Instrum.Methods 156, 355 (1978)

S.Della Negra, C.Deprun, H.Jungclas, H.Gauvin, J.P.Husson, Y.Le Beyec

The Time-of-Flight Mass Identification System Connected to the Alice He-Jet. 'On-Line' Experimental Results

NUCLEAR REACTIONS 121Sb, 118Sn(40Ar, xn), E not given; measured Eα. 152,153Er levels deduced T1/2. 103Rh, Ni, 27Al(12C, xn), E=67-92 MeV; measured β-recoil; deduced masses of mother, daughter isotopes. 64Zn, 60Ni, 28Si(32S, xn)E=100-190 MeV; measured β-recoil, T1/2; deduced evidence for 82Zr, 82Nb. Tof connected to He-jet technique.


1978JU03      Phys.Lett. 79B, 58 (1978)

H.Jungclas, D.Hirdes, R.Brandt, P.Lemmertz, E.Georg, H.Wollnik

Search for Superheavy Elements in the Interaction of 136Xe and 238U with (nat)U Using the Gas Jet Transport Technique

NUCLEAR REACTIONS U(136Xe, X), U(238U, X), E not given; measured σ for production of SF nuclides; deduced upper limits for production of superheavy elements. Gas jet collection.

doi: 10.1016/0370-2693(78)90435-5
Citations: PlumX Metrics


1978SC26      Z.Phys. A288, 189 (1978)

U.J.Schrewe, W.-D.Schmidt-Ott, R.-D.v.Dincklage, E.Georg, P.Lemmertz, H.Jungclas, D.Hirdes

Evidence of New Isotopes: 169,170Ir, 166,167,168Re

RADIOACTIVITY 172,171,170,169Ir, 168,167,166Re, 171,170,169,168Os; measured Eα, T1/2; deduced α-branching.

doi: 10.1007/BF01408649
Citations: PlumX Metrics


1977DE18      Z.Phys. A282, 65 (1977)

S.Della Negra, H.Gauvin, H.Jungclas, Y.Le Beyec, M.Lefort

Mechanism of Formation and Decay of the Compound Nuclei 150Gd Produced By Two Entrance Channels (16O + 134Ba) and (40Ar + 110Pd)

NUCLEAR REACTIONS 134Ba(16O, X), E=60-120 MeV; 110Pd(40Ar, X), E=140-230 MeV; measured complete fusion σ(E), σ(E) for production of 145,146,147Gd, 145,146,147Eu, 141mSm, 143mSm, 140mPm, 139mNd.

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetB0129.


1977DE19      Z.Phys. A282, 75 (1977)

S.Della Negra, H.Gauvin, H.Jungclas, Y.Le Beyec, M.Lefort

Comparison between Experimental Decay of the Compound Nuclei 150Gd and Evaporation Calculations

NUCLEAR REACTIONS 134Ba(16O, X), E=60-120 MeV; 110Pd(40Ar, X), E=140-230 MeV; analyzed data, calculated σ.

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetB0129.


1976AG01      Z.Phys. A278, 265 (1976)

S.Agarwal, H.Gauvin, D.Guerreau, H.Jungclas, Y.Le Beyec, M.Lefort, X.Tarrago

Evaporation Residue Cross Sections in Complete Fusion Reactions between 52Cr-56Fe, 63Cu-Ni and 63Cu-Ag

NUCLEAR REACTIONS 107,109Ag, 58,60Ni(63Cu, X), E=347 MeV; 56Fe(52Cr, X), E=207, 264 MeV; measured evaporation residue σ.

doi: 10.1007/BF01409177
Citations: PlumX Metrics


1976JU05      Radiochim.Acta 23, 38 (1976)

H.Jungclas, R.Brandt

Search for Eca-Gold and Eca-Lead in Nature Using the Spinner-Technique

RADIOACTIVITY Z=111, Z=114; measured no activity from natural samples.


1975JU04      Phys.Rev. C12, 1834 (1975)

H.Jungclas, R.Brandt, G.Stark

Recoil Properties of 232Th(γ, xn) Evaporation Products

NUCLEAR REACTIONS 232Th(γ, xn), E ≤ 55 MeV; measured ranges (X=5, 6), forward-backward recoil ratios (X=4, 5, 6) compared with estimations based on compound nucleus model.

doi: 10.1103/PhysRevC.12.1834
Citations: PlumX Metrics


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