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NSR database version of April 27, 2024.

Search: Author = H.Langhoff

Found 34 matches.

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1981EN03      Z.Phys. A302, 61 (1981)

G.Endres, H.Langhoff, W.Muckenheim, F.Wolf, P.Rullhusen, F.Smend, M.Schumacher

Resonance Fluorescence in 121Sb

NUCLEAR REACTIONS 121Sb(γ, γ), E=3.452 MeV; measured σ vs source velocity. 121Sb level deduced T1/2, J, π, γ-branching. 56Fe level deduced T1/2. Nuclear resonance fluorescence technique, Doppler shift analysis, 56Co source, high speed centrifuge.

doi: 10.1007/BF01425103
Citations: PlumX Metrics


1981MU05      Z.Phys. A300, 43 (1981)

W.Muckenheim, P.Rullhusen, F.Smend, M.Schumacher, G.Endres, H.Langhoff

Nuclear Resonance Fluorescence in 238U and a New Approach to Doppler-Shift-Attenuation using High Speed Rotation

NUCLEAR REACTIONS 238U(γ, γ'), E=resonance; measured Eγ, Iγ, γγ(θ), σ(θγ), resonance fluorescence yield. 238U deduced levels, J, π, γ-branching, T1/2, Γ. Cobalt-56 source.

RADIOACTIVITY 56Co; measured Doppler shift attenuation of emission line. 56Fe level deduced T1/2. High speed centrifuge.


1978EN01      Z.Phys. A285, 121 (1978)

G.Endres, H.Weiss, H.Langhoff

Nuclear Resonance Fluorescence from the 58 keV Level in 159Tb

NUCLEAR REACTIONS 159Tb(γ, γ'), E=58 keV; measured resonance absorption, Mossbauer spectra. 159Tb level deduced T1/2.

doi: 10.1007/BF01408738
Citations: PlumX Metrics


1972BO64      Z.Phys. 256, 441 (1972)

I.Borchert, M.Schumacher, F.Smend, H.Langhoff

The Perturbation of a γγ Directional Correlation of 75As in Gaseous H2 75Se Sources

RADIOACTIVITY 75Se; measured γγ(θ, pressure) in H2 Se sources; deduced attenuation coefficients.

doi: 10.1007/BF01386989
Citations: PlumX Metrics


1971SM07      Z.Phys. 248, 326 (1971)

F.Smend, I.Borchert, H.Langhoff

The Influence of the Chemical Environment on the Decay Constant of 90mNb

RADIOACTIVITY 90mNb; measured T1/2 in Zr, F complex; deduced chemical environment effects.

doi: 10.1007/BF01400546
Citations: PlumX Metrics


1970LA19      Nucl.Phys. A158, 657 (1970)

H.Langhoff

Lifetime Measurements in 131Xe and 129Xe

NUCLEAR REACTIONS 131Xe(γ, γ), Eγ=364 keV, 637 keV, 723 keV; 129Xe(γ, γ), Eγ=411 keV, 318 keV; measured σ(v), σ(θ). 129,131Xe levels deduced T1/2, γ-mixing, B(λ). Nuclear resonance fluorescence.

doi: 10.1016/0375-9474(70)90213-7
Citations: PlumX Metrics


1970WE01      Z.Phys. 230, 371 (1970)

J.Weiss, H.Langhoff, M.Schumacher

Die Anregungszustande des 79Br

RADIOACTIVITY 79Kr; measured Eγ, Iγ, γγ-coin; deduced log ft. 79Br deduced levels, J, π, T1/2, γ-mixing.

NUCLEAR REACTIONS 79Br(γ, γ'), E=0.2-0.9 MeV; measured nuclear resonance fluorescence. 79Br deduced levels, J, π, T1/2, γ-mixing. Ge(Li) detector.

doi: 10.1007/BF01403125
Citations: PlumX Metrics


1969GF01      Z.Physik 227, 45 (1969)

D.Gfoller, H.Langhoff, F.Smend, W.Weirauch, W.-D.Schmidt-Ott

Der Zerfall des 122Xe(T1/2=20, 1 h) und des 122J(T1/2=3, 6 min)

RADIOACTIVITY 122Xe [from 120Te(α, 2n)]; 122I [from 122Te(d, 2n)]; measured Eγ, Iγ, γγ-coin. 122I, 122Te deduced levels.


1969LA08      Nucl.Phys. A127, 379 (1969)

H.Langhoff, D.Gfoller

Nuclear Resonance Fluorescence from the 375 keV Level in 127I

NUCLEAR REACTIONS 127I(γ, γ), E=375 keV (127Xe source); measured σ(temperature, electric field strength). 127I level deduced T1/2. 127Xe deduced Q(EC).

doi: 10.1016/0375-9474(69)90578-8
Citations: PlumX Metrics


1968GF02      Z.Physik 211, 317 (1968)

D.Gfoller, H.Langhoff

Der Zerfall des J121(T1/2=2, 12 h)

NUCLEAR STRUCTURE 121I; measured not abstracted; deduced nuclear properties.


1968LA05      Nucl.Phys. A111, 225 (1968)

H.Langhoff, L.Frevert

Nuclear Resonance Fluorescence in 69Ga

NUCLEAR REACTIONS 69Ga(γ, γ), E=1107, 872, 574 keV; measured σ(E;θ). 69Ga levels deduced J, T1/2. 69Ge [from 69Ga(d, 2n)]; measured Eγ, Iγ, γγ-coin. 69Ga deduced levels. Natural target, Ge(Li) detector.

doi: 10.1016/S0375-9474(68)91026-9
Citations: PlumX Metrics


1968LA12      Proc.Conf.Electron Capture and Higher Order Processes in Nucl.Decays, Debrecen, Hungary, D.Berenyi, Ed., Eotvos Lorand Phys.Soc., Budapest, p.418(1968)

H.Langhoff

Nuclear Resonance Fluorescence After Electron Capture

NUCLEAR REACTIONS 69Ga, 127I(γ, γ), E = 375, 872, 1107 keV; measured nuclear resonance fluorescence at different temperatures. 127Xe deduced Q(EC).


1968SC14      Z.Physik 217, 282 (1968)

W.-D.Schmidt-Ott, W.Weirauch, F.Smend, H.Langhoff, D.Gfoller

Der Zerfall des 125mXe, des 127mXe und des 127gXe

NUCLEAR STRUCTURE 125Xe, 127Xe; measured not abstracted; deduced nuclear properties.

doi: 10.1007/BF01394102
Citations: PlumX Metrics


1967LA04      Bull.Am.Phys.Soc. 12, No.1, 129, HF7 (1967); Priv.Comm. (February 1967)

H.Langhoff, M.Schumacher

Lifetimes of the Levels at 265 and 280 keV in As75


1967LA07      Phys.Rev. 155, 1246 (1967)

H.Langhoff, M.Schumacher

Lifetimes of the Levels at 265 and 280 keV in As75

NUCLEAR STRUCTURE 75As; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRev.155.1246
Citations: PlumX Metrics


1967LA14      Z.Physik 205, 1 (1967)

H.Langhoff, R.Cesareo, A.Flammersfeld

Kernresonanzfluoreszenz in Mo94, Mo95 und Mo96

NUCLEAR REACTIONS 94,95,96Mo(γ, γ), E=600-1100 keV; measured resonance fluorescence, σ(Eγ, θ(γ)). 95Mo level deduced T1/2, J, γ-mixing.

doi: 10.1007/BF01326294
Citations: PlumX Metrics


1967LA15      Phys.Rev. 159, 1033 (1967)

H.Langhoff

Resonance Fluorescence in Re187

RADIOACTIVITY 187W; measured Eγ, Iγ. 187Re(γ, γ), E=512-880 keV; measured nuclear resonance fluorescence. 187Re levels deduced T1/2, B(M1). Ge(Li) detector.

doi: 10.1103/PhysRev.159.1033
Citations: PlumX Metrics


1967SC17      Z.Phys. 203, 443 (1967)

W.Schott, H.Langhoff, L.Frevert, A.Flammersfeld

Die Storung der Resonanzstreuung von γ-Strahlung einer Kr79-Quelle an Br79 durch Gaskinetische Stosse in der Quelle

NUCLEAR REACTIONS 79Br(γ, γ), E=300-800 keV; measured σ(Eγ), resonance scattering. 79Br levels deduced J, T1/2.


1967SC25      Phys.Rev. 162, 1153 (1967)

M.Schumacher, H.Langhoff

Nuclear-Resonance-Fluorescence and Gamma-Spectroscopic Studies in Ir191

RADIOACTIVITY 191Pt; measured Eγ, Iγ; deduced log ft.

NUCLEAR REACTIONS 191Ir(γ, γ'), E=539, 588 keV; measured nuclear resonance fluorescence. 191Ir deduced levels, J, π, T1/2, level width, γ-multipolarity. Ge(Li) detector.

doi: 10.1103/PhysRev.162.1153
Citations: PlumX Metrics


1966CE04      Z.Physik 197, 426 (1966)

R.Cesareo, H.Langhoff, A.Flammersfeld

Die γ-Spektren von Tc95, Tc95m und Tc96

NUCLEAR STRUCTURE 95Tc, 96Tc; measured not abstracted; deduced nuclear properties.

doi: 10.1007/BF01325909
Citations: PlumX Metrics


1966FR08      Z.Phys. 194, 248 (1966)

L.Frevert, W.Schott, H.Langhoff, A.Flammersfeld

Resonanzstreuung am 202, 8 Kev-Niveau im J127

NUCLEAR STRUCTURE 127I; measured not abstracted; deduced nuclear properties.

doi: 10.1007/BF01571249
Citations: PlumX Metrics


1966LA06      Nucl.Phys. 79, 145 (1966)

H.Langhoff, L.Frevert, W.Schott, A.Flammersfeld

The Excited Levels of 79Br

RADIOACTIVITY 79Kr [from 79Br(d, 2n)]; measured Iγ, γγ-coin. 79Br deduced ICC, γ-mixing. 79Br(γ, γ), Eγ = 307, 398, 526, 606, 834 keV; measured σ(E;θ). 79Br deduced levels, J, T1/2. Natural target.

doi: 10.1016/0029-5582(66)90397-X
Citations: PlumX Metrics


1965LA01      Nucl.Phys. 63, 425 (1965)

H.Langhoff

Properties of the 418 keV Level in I127

NUCLEAR REACTIONS 127I(γ, γ), E=418 keV; measured σ(ν source; Eγ, θ), polarization. 75As(γ, γ), E=265 keV; measured polarization. 127I deduced J, T1/2. 127Te[from 126Te(n, γ)]; measured γγ(θ). 127I deduced J, delta(E2/M1). Enriched target.

doi: 10.1016/0029-5582(65)90473-6
Citations: PlumX Metrics


1964LA01      Bull.Am.Phys.Soc.9, No.1, 9, AB9 (1964)

H.Langhoff

Resonance Fluorescence in Re187


1964LA02      Phys.Rev. 135, B1 (1964)

H.Langhoff

Resonance Fluorescence in Re187

NUCLEAR STRUCTURE 187Re; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRev.135.1
Citations: PlumX Metrics


1964LA18      Phys.Rev. 136, B1590 (1964)

H.Langhoff

Resonance Fluorescence in Ir191

NUCLEAR STRUCTURE 191Ir; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRev.136.B1590
Citations: PlumX Metrics


1963ME03      Bull.Am.Phys.Soc. 8, No.4, 332, J9 (1963)

F.R.Metzger, H.Langhoff

Resonance Fluorescence in Sb121

NUCLEAR STRUCTURE 121Te; measured not abstracted; deduced nuclear properties.


1963ME13      Phys.Rev. 132, 1753 (1963)

F.R.Metzger, H.Langhoff

Properties of Low-Lying Levels in Sb121

NUCLEAR STRUCTURE 121Sb; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRev.132.1753
Citations: PlumX Metrics


1962KI08      Z.Physik 169, 23 (1962)

P.Kilian, H.Langhoff, A.Flammersfeld

Der Zerfall von Nb94m

NUCLEAR STRUCTURE 94Nb; measured not abstracted; deduced nuclear properties.

doi: 10.1007/BF01378280
Citations: PlumX Metrics


1962KI11      Physik Verb. 13, 45 (1962)

P.Kilian, H.Langhoff, A.Flammersfeld

NUCLEAR STRUCTURE 94Nb; measured not abstracted; deduced nuclear properties.


1961LA07      Z.Phys. 164, 166 (1961)

H.Langhoff, H.H.Hennies

Zum experimentellen Nachweis von Zweiquantenzerfall beim 0+-0+-Ubergang des Zr90

NUCLEAR STRUCTURE 90Y; measured not abstracted; deduced nuclear properties.

doi: 10.1007/BF01377806
Citations: PlumX Metrics


1961LA15      Z.Physik 165, 387 (1961)

H.Langhoff, P.Kilian, A.Flammersfeld

Die Koeffizienten der Inneren Paarbildung bei Den γ Ubergangen nach Co60 → Ni60 und Pr142 → Nd142

NUCLEAR STRUCTURE 142Pr, 60Co; measured not abstracted; deduced nuclear properties.

doi: 10.1007/BF01381895
Citations: PlumX Metrics


1961LA16      Z.Phys. 165, 393 (1961)

H.Langhoff, P.Kilian, A.Flammersfeld

Das K/β+-Verhaltnis beim Zerfall J128 → Te128

NUCLEAR STRUCTURE 128I, 104Rh, 176Lu; measured not abstracted; deduced nuclear properties.

doi: 10.1007/BF01381896
Citations: PlumX Metrics


1960LA13      Z.Physik 160, 186 (1960)

H.Langhoff

Die Linearpolarisation der Vernichtungsstrahlung von Positronen

NUCLEAR STRUCTURE 22Na, 64Cu; measured not abstracted; deduced nuclear properties.

doi: 10.1007/BF01336980
Citations: PlumX Metrics


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