References quoted in the ENSDF dataset: 77KR ADOPTED LEVELS, GAMMAS

70 references found.

Clicking on a keynumber will list datasets that reference the given article.


1948WO07

Phys.Rev. 74, 761 (1948)

L.L.Woodward, D.A.McCown, M.L.Pool

Radioactive Kr Isotopes

doi: 10.1103/PhysRev.74.761


1955TH01

Arkiv Fysik 9, 137 (1955)

S.Thulin

Studies in Nuclear Spectroscopy with Electromagnetically Separated Gaseous Isotopes II - Disintegration of Some Krypton and Xenon Isotopes


1957BE46

Nuclear Phys. 2, 593 (1957)

J.Beydon, R.Chaminade, M.Crut, H.Faraggi, J.Olkowsky, A.Papineau

Etude de la Transmutation du Cuivre par la l'Azote et l'Oxygene

doi: 10.1016/0029-5582(57)90072-X


1960BU22

J.Inorg.Nuclear Chem. 16, 10 (1960); Erratum J.Inorg.Nuclear Chem. 17, 194 (1961)

F.D.S.Butement, G.G.J.Boswell

New Neutron Deficient Isotopes of Krypton

NUCLEAR STRUCTURE 76Br, 75Kr, 74Kr, 74Br; measured not abstracted; deduced nuclear properties.

doi: 10.1016/0022-1902(60)80079-6


1971BO30

Z.Phys. 244, 338 (1971)

I.Borchert

Der Zerfall des 77Kr

RADIOACTIVITY 77Kr; measured Eγ, Iγ, γγ-coin, T1/2; deduced log ft. 77Br deduced levels, J, π, γ-branching.


1973BA22

Izv.Akad.Nauk SSSR, Ser.Fiz. 37, 73 (1973); Bull.Acad.Sci.USSR, Phys.Ser. 37, No.1, 64 (1973)

K.A.Baskova, S.S.Vasilev, M.A.Mokhsen, T.V.Chugai, L.Y.Shavtvalov

The Decay of 77Kr

RADIOACTIVITY 77Kr; measured T1/2, Eγ, Iγ, Eβ, Iβ, βγ-, γγ-coin; deduced log ft. 77Br deduced levels, J, π.


1974HO37

Phys.Fenn. 9, 85 (1974)

A.Houdayer, S.K.Mark, J.E.Kitching, T.Paradellis

Levels of 77Br Populated in the Decay of 77Kr and a Unified Model Description of 77,79,81,83Br Isotopes

RADIOACTIVITY 77Kr [from 79Br(p, 3n), E=35 MeV]; measured Eγ, Iγ, I(ce). 77Br levels deduced J, π, log ft, multipolarity. Unified model calculation.


1975NO11

Z.Phys. A275, 33 (1975)

E.Nolte, P.Vogt

Rotational Bands in 77Kr

NUCLEAR REACTIONS 63Cu(16O, pnγ), E=42 MeV; measured γγ-coin, σ(Eγ, θ). 64Ni(16O, 3nγ), E=42, 47, 52, 57 MeV; measured Eγ, Iγ, recoil distance DSA. 64Zn(16O, n2pγ), 66Zn(16O, nαγ), E=44, 51, 58 MeV; measured Eγ, Iγ. 77Kr deduced levels, K, J, π, T1/2, B(λ).


1979DE39

Int.J.Appl.Radiat.Isotop. 30, 786 (1979)

D.de Jong, H.Kooiman, J.T.Veenboer

76Br and 77Br from Decay of Cyclotron Produced 76Kr Amd 77Kr

RADIOACTIVITY 76,77Kr; calculated maximal yields for 76,77Br.

NUCLEAR REACTIONS 79Br(p, xn), E=65 MeV; Se(3He, xn), E=40 MeV; measured production σ for 76,77Kr. Thick targets.

doi: 10.1016/0020-708X(79)90161-3


1979DI04

Phys.Rev. C19, 1753 (1979)

M.Diksic, J.-L.Galinier, H.Marshall, L.Yaffe

79Br and 81Br(p, xn) and (p, pxn) Excitation Functions in the Energy Range 10-85 MeV

NUCLEAR REACTIONS 79Br(p, n), (p, 3n), (p, 4n), (p, pn), (p, 2np), (p, 3np), (p, 4np), (p, 5np), 81Br(p, 3n), (p, 5n), (p, 6n), (p, pn), (p, 3np), (p, 4np), (p, 5np), (p, 6np), E=10-85 MeV; measured σ(E). Enriched target.

doi: 10.1103/PhysRevC.19.1753


1979KR12

Phys.Rev.Lett. 43, 1150 (1979)

A.J.Kreiner, M.A.J.Mariscotti

Coriolis-Distorted Bands of Common g9/2 Parentage in Odd and Doubly Odd N = 41 Nuclei

NUCLEAR STRUCTURE 77Kr, 76Br; calculated band structure. Two noninteracting quasiparticles-plus-rotor model.

doi: 10.1103/PhysRevLett.43.1150


1979NO07

Int.J.Appl.Radiat.Isotop. 30, 79 (1979)

T.Nozaki, M.Iwamoto, Y.Itoh

Production of 77Br by Various Nuclear Reactions

RADIOACTIVITY 77Kr [from 79Br(p, 3n), E < 50 MeV]; measured Iγ; deduced production σ for 77Br.

NUCLEAR REACTIONS Br, Se(p, xn), E < 50 MeV; 75As(α, xn), E=15-40 MeV; measured production σ for 76,77,82Br, 77,76Kr. Thick targets.

doi: 10.1016/0020-708X(79)90076-0


1981NO02

Int.J.Appl.Radiat.Isotop. 32, 73 (1981)

R.Nowotny

Calculation of Proton-Induced Radioisotope Production Yields with a Statistical-Model Based Code

NUCLEAR REACTIONS 75As, 79,81Br, 83,84,86Kr, 85,87Rb, 203,205Tl(p, 3n), E=20-50 MeV; 75As, 79Br, 84,86Kr, 85Rb, 203,205Tl(p, 4n), E=25-60 MeV; 81Br, 86Kr, 85,87Rb, 127I, 205Tl(p, 5n), E=35-70 MeV; 205Tl(p, 6n), E=40-70 MeV; 86Kr(p, 6n), E=55-70 MeV; calculated σ(E); deduced production yields for 72,73Se, 76,77Kr, 81,82m,83Rb, 81,82,83Sr, 200,201,203Pb.

doi: 10.1016/0020-708X(81)90136-8


1982BA33

Nucl.Phys. A384, 211 (1982)

J.Barreto, M.Langevin, C.Detraz

Formation and Deexcitation of the 79Rb Compound Nucleus

NUCLEAR REACTIONS 63Cu(16O, X), E=40-85 MeV; 45Sc(34S, X)77Kr/76Kr/75Kr/77Br/75Br/74Br/73Br/73Se/76Br/70As/71As/72As/69Ge, E=85-130 MeV; measured Eγ, Iγ; deduced production σ vs E for residuals. 79Rb deduced fusion barrier. Activation technique, enriched target. Statistical model.

doi: 10.1016/0375-9474(82)90314-1


1982BL24

J.Labelled Compd.Radiopharm. 19, 1431 (1982)

G.Blessing, K.Suzuki, He Youfeng, S.M.Qaim, G.Stocklin

Production of High-Purity 77Kr

NUCLEAR REACTIONS, ICPND 77Se(3He, 3n), E=22-36 MeV; measured production σ(E). Metallic target, activation technique.


1982CLZZ

Bull.Am.Phys.Soc. 27, No.4, 498, DYa5 (1982)

M.Clark, D.Brandt, S.Shafroth, J.Swenson, C.R.Gould, S.A.Wender

A Pulsed Beam Study of the 16O(63Cu, pn)77Kr Gamma Reaction

RADIOACTIVITY 77Kr [from 63Cu(16O, np), E=42 MeV]; measured I(K X-ray)/Iγ, T1/2. 77Kr levels deduced J, π, ICC. Thick Cu target, pulsed beam.


1982SU10

Int.J.Appl.Radiat.Isotop. 33, 1445 (1982)

K.Suzuki, G.Blessing, S.M.Qaim, G.Stocklin

Production of High-Purity 77Kr via the 77Se(3He, 3n)77Kr-Process

NUCLEAR REACTIONS 77Se(3He, 3n), E=22-36 MeV; measured residual production yield. Activation technique.

doi: 10.1016/0020-708X(82)90184-3


1982ZOZY

Program and Theses, Proc.32nd Ann.Conf.Nucl.Spectrosc.Struct.At.Nuclei, Kiev, p.69 (1982)

A.E.Zolov, I.Kh.Lemberg, A.A.Pasternak, B.I.Rzhanov

Life Times of Excited States of 77Kr

NUCLEAR REACTIONS 66Zn(14N, n2p), E=52 MeV; measured DSA, recoil. 77Kr levels deduced T1/2.


1983WE05

Int.J.Appl.Radiat.Isotop. 34, 1335 (1983)

R.Weinreich, J.Knieper

Production of 77Kr and 79Kr for Medical Applications via Proton Irradiation of Bromine: Excitation functions, yields and separation procedure

NUCLEAR REACTIONS, ICPND 79,81Br(p, xnyp)76Kr/77Kr/79Kr, E=45-32 MeV; measured residuals production σ(E), thick target yields.

doi: 10.1016/0020-708X(83)90024-8


1984SA36

Radiochim.Acta 37, 83 (1984)

K.Sakamoto, M.Nishio, M.Dohniwa, K.Okada, Y.Hamajima

Spallation Yields from Natural Rb, Sr and Y Irradiated with 100 MeV and 200 MeV Bremsstrahlung

NUCLEAR REACTIONS Rb(γ, X)86Rb/84Rb/84mRb/83Rb/82Rb/82mRb/81Rb/81mRb/87Kr/85Kr/85mKr/79Kr/77Kr/76Kr/84Br/83Br/82Br/80Br/80mBr/77Br/76Br/75Br/81Se/81mSe/75Se/73Se/72Se/78As/77As/76As/74As/73As/72As/71As, Sr(γ, X)87Sr/87mSr/85Sr/85mSr/83Sr/86Rb/84Rb/83Rb/82Rb/82mRb/81Rb/85Kr/85mKr/79Kr/77Kr/76Kr/83Br/82Br/80Br/80mBr/77Br/76Br/75Br/75Se/73Se/76As/74As/73As/72As/71As, 89Y(γ, X)88Y/87Y/87mY/86Y/86mY/85Y/85mY/84Y/87Sr/87mSr/85Sr/85mSr/83Sr/86Rb/84Rb/84mRb/83Rb/82Rb/82mRb/81Rb/81mRb/79Rb/85Kr/85mKr/79Kr/77Kr/76Kr/82Br/80Br/80mBr/77Br/76Br/75Br, E=100, 200 MeV bremsstrahlung; measured spallation yields; deduced isotopic, isobaric mass distributions, charge dispersions, isomeric ratios. Activation, radiochemical methods, 197Au(γ, n) standard.


1984WO10

Nucl.Phys. A431, 170 (1984)

B.Wormann, K.P.Lieb, R.Diller, L.Luhmann, J.Keinonen, L.Cleemann, J.Eberth

The Yrast Bands In 77Kr and 76Kr

NUCLEAR REACTIONS 63Cu(16O, 2np), (16O, pn), E=49-58 MeV; measured Eγ, I(Eγ), γ(θ), recoil distance Droppler shift, DSA, γγ-coin. 77Kr deduced levels, J, π, T1/2, (E2/M1) mixing ratio, B(E2), B(M1). 76Kr deduced T1/2, B(E2). Enriched target. Triaxial rotor plus quasiparticle model.

doi: 10.1016/0375-9474(84)90060-5


1985AH05

Nucl.Phys. A445, 1 (1985)

D.P.Ahalpara, A.Abzouzi, K.H.Bhatt

A Microscopic Decription of the Collective Bands in 75-77Kr

NUCLEAR STRUCTURE 75Kr; calculated levels. 77Kr calculated levels, B(E2). 76Kr; calculated levels. Microscopic model.

doi: 10.1016/0375-9474(85)90356-2


1985GUZZ

Bull.Am.Phys.Soc. 30, No.8, 1256, BB11 (1985)

J.H.Gundlach, J.A.Behr, G.Feldman, C.A.Gossett, K.A.Snover

Statistical Decay of the Giant Dipole Resonance in Highly Excited Nuclei in the Mass Region A = 70-90

NUCLEAR REACTIONS 60,61,64Ni(12C, X), 61,64Ni, 64Zn(16O, X), 72Ge(18O, X), E=40-52 MeV; measured Eγ, Iγ. 72,73,76Se, 77,80Kr, 80Sr, 90Zr deduced GDR decay characteristics.


1985NA02

Nucl.Phys. A435, 397 (1985)

W.Nazarewicz, J.Dudek, R.Bengtsson, T.Bengtsson, I.Ragnarsson

Microscopic Study of the High-Spin Behaviour in Selected A = 80 Nuclei

NUCLEAR STRUCTURE 84,82,80,78,76,74Sr; calculated total energy vs β2. 72,74,76,78Kr, 82,84,74,76,78,80,82,84Sr, 78,80,82,84,86Zr; calculated oblate, protate β2, quadrupole moment. 74,76,78,80,82,84Sr; calculated total energy surfaces, yrast levels. 75,77,79,81Kr, 77,79,81Rb, 77,79,81,83Sr, 83Y; calculated levels, β2. 80,82Kr; calculated low energy levels, band structure. Shell correction, microscopic model.

doi: 10.1016/0375-9474(85)90471-3


1985SA23

Int.J.Appl.Radiat.Isotop. 36, 481 (1985)

K.Sakamoto, M.Dohniwa, K.Okada

Excitation Function for (p, xn) and (p, pxn) Reactions on Natural 79+81Br, 85+87Rb, 127I and 133Cs upto E(p) = 52 MeV

NUCLEAR REACTIONS, ICPND 79,81Br(p, xn), (p, xnp)79Kr/77Kr/76Kr/77Br/76Br, E=threshold-52 MeV; 85,87Rb(p, xn), (p, xnp)87Sr/87mSr/85Sr/85mSr/83Sr/86Rb/84Rb, E=threshold-52 MeV; 127I(p, xn), (p, xnp)127Xe/125Xe/123Xe/126I/124I, E=threshold-52 MeV; 133Cs(p, xn), (p, xnp)133Ba/133mBa/131Ba/131mBa/129Ba/132Cs/130Cs, E=threshold-52 MeV; measured residuals production σ(E). Activation technique, preequilibrium decay.

doi: 10.1016/0020-708X(85)90213-3


1986BAYU

Program and Theses, Proc.36th Ann.Conf.Nucl.Spectrosc.Struct.At.Nuclei, Kharkov, p.364 (1986)

V.G.Baty, Yu.V.Vladimirov, Yu.N.Rakivnenko, Yu.N.Ranyuk, O.A.Rastrepin, E.A.Skakun

Electro- and Photodisintegration of Y, Zr, Nb, Mo, 113In, 115In Nuclei by Electrons of 275 MeV Energy

NUCLEAR REACTIONS 89Y(e, X), (γ, X)77Kr/81Rb/83Sr/84Y/86Y/86mY/87Y/87mY/88Y, E=275 MeV; Mo(e, X), (γ, X)87Y/87mY/91Y/91mY/86Zr/89Zr/89Nb/96Nb/97Nb/90Mo/99Mo, E=275 MeV; 113,115In(e, X), (γ, X)104Ag/111Cd/111mCd/108In/108mIn/109In/110In/110mIn/111In/112In/112mIn/113In/113mIn/114In/114mIn/115In/115mIn, E=275 MeV; measured residuals production σ. Cascade evaporation model.


1986BU24

Yad.Fiz. 44, 425 (1986); Sov.J.Nucl.Phys. 44, 271 (1986)

V.S.Buttsev, G.L.Buttseva, V.Ya.Kostin, V.Ya.Migalenya

Interaction of 7.3-GeV Deuterons with 93Nb, 159Tb, (Nat 207.2)Pb, and 209Bi

NUCLEAR REACTIONS 93Nb, 159Tb, Pb, 209Bi(d, X)117Te/116In/116mIn/119I/120I/121I/131La/132La/132Ce/133Ce/24Na/28Mg/41Ar/67Cu/71As/72As/72Zn/73Se/75Br/76Br/77Br/81Rb/82Rb/82mRb/84Y/86Y/86mY/87Y/87mY/86Zr/89Zr/77Kr/85Kr/85mKr/90Nb/92Nb/92mNb/34Cl/34mCl/93Tc/93mTc/94Tc/94mTc/104Ag/104mAg/138Pr/138mPr/157Dy/198Tl/198mTl/198Pb/199Pb/201Pb/202Pb/202mPb/203Pb/204Pb/204mPb/204Bi/206Bi/203Bi/202Bi/200Tl/132La/95Tc/93Mo/93mMo/90Mo/90Nb/56Mn, E=7.3 GeV; measured residue T1/2, Eγ, σ. 87,88Y, 93,94Tc, 133Ce, 104Ag, 198Tl, 196,198Au, 186Ir deduced isomeric ratios. Ge(Li) detector.


1986MA64

Int.J.Appl.Radiat.Isotop. 37, 703 (1986)

B.Maziere, C.Loch

Radiopharmaceuticals Labelled with Bromine Isotopes

NUCLEAR REACTIONS, ICPND 75As(3He, 3n), E=25-36 MeV; 76Se(p, 2n), E=21.5-28 MeV; 78Kr(p, α), E=12-15 MeV; 75As(3He, 2n), E=10-30 MeV; Br(d, xn)76Kr, Br(p, xn)76Kr, E=50-90 MeV; 76Se(3He, 3n), E=30-36 MeV; 75As(α, 2n), E=14-28 MeV; 77Se(p, n), E=12 MeV; 78Se(p, 2n), E=20-26 MeV; Mo(p, F), E=800 MeV; Br(d, xn)77Kr, E=25-50 MeV; 79Br(p, 3n), E=45, 65 MeV; compiled 75,76,77Br yields. Direct, indirect methods.


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


1987ME09

Z.Phys. A327, 393 (1987)

R.A.Meyer, E.Monnand, J.A.Pinston, F.Schussler, B.Pfeiffer, V.Paar

Pseudobands in Non-SU(3) Odd-Mass Nuclei and Coherent State Structures of Quadrupole Phonons

NUCLEAR STRUCTURE 99Y, 75Se, 75,77Kr; calculated levels, J. Quadrupole phonon model.


1987MO06

Phys.Rev. C35, 1275 (1987)

D.M.Moltz, A.C.Betker, J.P.Sullivan, R.H.Burch, C.A.Gagliardi, R.E.Tribble, K.S.Toth, F.T.Avignone III

Masses of 77Kr and 75Kr

NUCLEAR REACTIONS 78,80Kr(3He, 6He), E=70 MeV; 78Kr(d, t), E=29.1 MeV; measured σ(E(6He)), σ(Et), Q. 75,77Kr deduced masses. Enriched gas targets.

doi: 10.1103/PhysRevC.35.1275


1988KIZR

RIKEN-87, p.191 (1988)

K.Kitao, A.Hashizume, Y.Tendow, Y.Ohkubo, K.Sueki

On the Cross Sections for 77Br Production Reactions

NUCLEAR REACTIONS, ICPND 75As(α, 2n), E ≈ 15-50 MeV; 79Br(p, 3n), 81Br(p, 5n), E ≈ threshold-80 MeV; 79Br(p, 3n), E ≈ 25-50 MeV; 81Br(p, 4np), (p, 5n), 79Br(p, 2np), (p, 3n), E ≈ threshold-90 MeV; analyzed residual production σ(E).


1988TAZR

Proc.Intern.Workshop Nucl.Struct.of the Zirconium Region, Bad Honnef, Germany, p.303 (1988)

S.L.Tabor, P.D.Cottle, C.J.Gross, D.M.Headly, U.J.Huttmeier, E.F.Moore, W.Nazarewicz

Core Polarization Effects in Odd A ≈ 80 Nuclei

NUCLEAR STRUCTURE 81Sr, 77Kr, 79,77,87Rb; analyzed levels, dynamic moment of inertia, quadrupole moments type of data; deduced shape, core polarization role.


1989HE10

J.Radioanal.Nucl.Chem. 136, 95 (1989)

F.Helus, S.Zeisler, H.Gasper, S.McQuarrie, W.Maier-Borst

A Feasibility Study of 75Br and 77Br Production from Enriched Krypton

NUCLEAR REACTIONS, ICPND 78Kr(p, np), (p, α), 80Kr(p, α), E < 30 MeV; calculated thick target yields. Enriched targets. Kr(p, xnypzα)75Br/77Br, E=20.5 MeV; measured residuals production rate.


1989SKZW

Program and Thesis, Proc.39th Ann.Conf.Nucl.Spectrosc.Struct.At.Nuclei, Tashkent, p.323 (1989)

E.A.Skakun, O.A.Rastrepin, V.G.Baty, Yu.N.Rakivnenko, Yu.N.Ranyuk, E.O.Babichev

Production Cross-Sections of Radioactive Nuclei in Deep Disintegration Reactions of 89Y by Electrons and Protons

NUCLEAR REACTIONS 89Y(e, X), (γ, X)71As/73Se/75Br/77Kr/79Kr/85mKr/81Rb/84Rb/89Sr/84Y/85Y/85mY/86Y/86mY/87Y/87mY/88Y, E=700, 1200 MeV; measured cumulative, independent residuals yields vs E; deduced 85,86,87Y isomeric σ ratios.


1990CA27

Phys.Rev. C42, 591 (1990)

M.A.Cardona, G.Garcia Bermudez, A.Filevich, E.Achterberg

Lifetime Measuremens in 75Kr and Systematic Study of Krypton Isotopes

NUCLEAR REACTIONS 54Fe(24Mg, n2p), E=75 MeV; measured Eγ, Iγ, recoil distance Doppler shift. 75Kr levels deduced T1/2, B(E2). Enriched target. Triaxial rotor-plus-quasiparticle model.

NUCLEAR STRUCTURE 75,77,79Kr; calculated levels, B(λ). Triaxial rotor-plus-quasiparticle model.

doi: 10.1103/PhysRevC.42.591


1990JO07

Phys.Rev. C42, 2418 (1990)

T.D.Johnson, J.W.Holcomb, P.C.Womble, P.D.Cottle, S.L.Tabor, F.E.Durham, S.G.Buccino, M.Matsuzaki

Transition Strengths and Deformation in 77Kr

NUCLEAR REACTIONS 48Ti(32S, n2p), E=106 MeV; measured γγ-coin spectra, DCO ratios, DSA, line shapes. 77Kr deduced levels, J, π, T1/2, B(λ).

doi: 10.1103/PhysRevC.42.2418


1991HE08

J.Radioanal.Nucl.Chem. 153, 417 (1991)

F.Helus, St.Zeisler, G.Gschwandtner, H.Marx, W.Maier-Borst

Production of 75Br and 77Br from Enriched Krypton: Excitation Functions

NUCLEAR REACTIONS, ICPND 78Kr(p, α), (p, np), (p, 2n), 80Kr(p, α), (p, nα), (p, 2n), E=threshold-30 MeV; measured residuals production σ(E).


1991ST02

Appl.Radiat.Isot. 42, 361 (1991)

G.F.Steyn, S.J.Mills, F.M.Nortier, F.J.Haasbroek

Integral Excitation Functions for (nat)Kr + p up to 116 MeV and Optimization of the Production of 81Rb for 81mKr Generators

NUCLEAR REACTIONS, ICPND Kr(p, X)79Rb/81Rb/81mRb/82Rb/82mRb/83Rb/84Rb/84mRb/86Rb/77Kr/79Kr/85Kr/85mKr/77Br/82Br, E=threshold-116 MeV; measured thick target production rates, σ(E). Geometry dependent hybrid model.


1991ZA02

Radiochim.Acta 54, 57 (1991)

N.G.Zaitseva, C.Deptula, O.Knotek, S.K.Kim, S.Mikolaevsky, P.Mikecz, E.Rurarz, V.A.Khalkin, V.A.Konov, L.M.Popinenkova

Cross Sections for the 100 MeV Proton-Induced Nuclear Reactions and Yields of Some Radionuclides Used in Nuclear Medicine

NUCLEAR REACTIONS, ICPND 55Mn(p, xn)53Fe/55Fe/52Fe, E=36-100 MeV; 59Co(p, xnyp)57Co/56Co/58Co/57Ni/52Fe/59Ni, E=64-100 MeV; Br(p, xn)77Kr/76Kr/79Kr, E=24-100 MeV; Rb(p, xn)82Sr, 85Rb(p, xn)82Sr/83Sr/81Sr, 87Rb(p, xn)83Sr/82Sr/85Sr, E=36-100 MeV; 127I(p, xn)123Xe/125Xe, E=48-100 MeV; 133Cs(p, xn)128Ba/129Ba/131Ba, 133Cs(p, xnp)127Cs/128Cs/129Cs/130Cs/131Cs/132Cs, E=43-100 MeV; 206Pb(p, xn)199Bi/200Bi/201Bi/202Bi/202mBi/204Bi/205Bi, 206Pb(p, xnp)199Pb/200Pb/201Pb/202Pb/203Pb/205Pb, E=49-57 MeV; 207Pb(p, xn)200Bi/201Bi/202Bi/202mBi/203Bi/204Bi/205Bi/206Bi, 207Pb(p, xnp)200Pb/201Pb/202Pb/203Pb/205Pb, E=57-68 MeV; 208Pb(p, xn)200Bi/201Bi/202Bi/204Bi/205Bi/206Bi/207Bi, 208Pb(p, xnp)201Pb/202Pb/203Pb/205Pb, E=68-76 MeV; measured residue production σ(E), thick target yields. Model comparison.


1992DOZV

Proc.Int.Conf.Nuclear Structure and Nuclear Reactions at Low and Intermediate Energies, Dubna, p.17 (1992); JINR E4-92-293 (1992)

D.N.Doinikov, V.M.Mikhailov

J-2 - Anomaly in Nuclear Spectra with N = 41

NUCLEAR STRUCTURE 75Se, 77Kr, 83Rb; analyzed level data; deduced j-2-anomaly. Interacting boson approximation.


1992LI24

Hyperfine Interactions 74, 3 (1992)

P.Lievens, and the ISOLDE Collaboration

Towards Higher Sensitivity and Lighter Elements by Collinear Laser Spectroscopy at ISOLDE

NUCLEAR STRUCTURE 40,42,44,46,45,48,50Ca, 79,81,83,85,87,89,91,93,95,99Sr, 72,74,75,76,77,78,79,80,81,82,83,84,85,86,87,88,89,90,91,92,93,94,95,96Kr; compiled, reviewed charge rms radii data. Isomers included.

RADIOACTIVITY 9,11Li(β-); measured β NMR asymmetry; deduced quadrupole moment raio.


1992NE09

Hyperfine Interactions 75, 339 (1992)

R.Neugart

Laser Spectroscopy - Recent Results and Prospects for Lighter Nuclei

COMPILATION 161,162,163,164,165,166,167,168,169,170,171,172,173,174,175,176,177,178,179,180Lu; compiled, reviewed μ, quadrupole moment, rms charge radii, J. 77,78,79,80,81,82,83,84,85,86,87,88,89,90,91,92,93,94,95,96,97,98,99,100Sr; 72,74,75,76,77,78,79,80,81,82,83,84,85,86,87,88,89,90,91,92,93,94,95,96Kr; 40,41,42,43,44,45,48,50Ca; compiled, reviewed rms charge radii changes. 9,11Li; compiled, reviewed NMR quadrupole splitting. New techniques based on collinear laser spectroscopy.


1992TA01

Phys.Rev. C45, 242 (1992)

S.L.Tabor

Convergence of the Moments of Inertia in f-p-g Shell Nuclei

NUCLEAR STRUCTURE 76,78Rb, 74,76Br; calculated kinematic moments of inertia vs rotational frequency, level energy differences. 71,73,75Se, 73,75,77,79Br, 75,77,79Kr, 77,79,81Rb, 79,81,83Sr, 81,83,85Y, 83Zr; calculated kinematic moments of inertia vs rotational frequency.

doi: 10.1103/PhysRevC.45.242


1993ARZW

Proc.6th Intern.Conf.on Nuclei Far from Stability + 9th Intern.Conf.on Atomic Masses and Fundamental Constants, Bernkastel-Kues, Germany, 19-24 July, 1992, R.Neugart, A.Wohr, Eds., p.197 (1993)

E.Arnold, W.Borchers, U.Georg, M.Keim, A.Klein, P.Lievens, R.Neugart, R.E.Silverans, L.Vermeeren

Laser Spectroscopy Measurements of 72-96Kr Moments and Charge Radii

NUCLEAR MOMENTS 78,80,82,83,84,86Kr; measured hfs, isotope shifts; deduced μ, quadrupole moment, mean square charge radii. Collinear fast beam laser spectroscopy. Comparison with data on other nuclei.

RADIOACTIVITY 74,75,77,79,72Kr(β+), (EC); 81,77Kr(EC); 85,87,89,90,91,92,93,94,95,96Kr(β-); measured hfs, isotope shifts; deduced μ, quadrupole moment, mean square charge radii. Collinear fast beam laser spectroscopy. Comparision with data on other nuclei.


1993DO10

Bull.Rus.Acad.Sci.Phys. 57, 74 (1993)

D.N.Doinikov, V.M.Mikhailov

Effective Hamiltonian of Quadrupole Bosons Interacting with Quasiparticles

NUCLEAR STRUCTURE 77,79Se, 77Kr; calculated levels. Microscopic approach.


1993DO17

Bull.Rus.Acad.Sci.Phys. 57, 1630 (1993)

D.N.Doinikov, V.M.Mikhailov

Electromagnetic Transitions in Fermion-Boson System

NUCLEAR STRUCTURE 77,79Se, 77Kr; calculated levels, B(λ). Effective operator, quadrupole bosons, fermions system.


1993TA15

Appl.Radiat.Isot. 44, 1105 (1993)

F.Tarkanyi, Z.Kovacs, S.M.Qaim

Excitation Functions of Proton Induced Nuclear Reactions on Highly Enriched 78Kr: Relevance to the Production of 75Br and 77Br at a Small Cyclotron

NUCLEAR REACTIONS, ICPND 78Kr(p, np), (p, α), (p, 2p), E=threshold-19.62 MeV; measured residual production σ(E), thick target yields. Activation technique.

doi: 10.1016/0969-8043(93)90114-P


1994VO09

Yad.Fiz. 57, No 4, 582 (1994); Phys.Atomic Nuclei 57, 618 (1994)

D.A.Volkov, I.B.Kovgar, A.I.Levon, A.A.Pasternak

Conflicting Coupling in Odd-Odd Nucleus 76Br

NUCLEAR STRUCTURE 77,76Kr; calculated levels. 76Br; calculated levels, B(λ); deduced M1 transitions behavior explanation.


1995KE04

Nucl.Phys. A586, 219 (1995)

M.Keim, E.Arnold, W.Borchers, U.Georg, A.Klein, R.Neugart, L.Vermeeren, R.E.Silverans, P.Lievens

Laser-Spectroscopy Measurements of 72-96Kr Spins, Moments and Charge Radii

NUCLEAR MOMENTS 78,80,82,83,84,86Kr; measured isotope shifts, hfs; deduced hyperfine constants, J, μ, electric quadrupole moments, mean square charge radii. Collinear fast beam laser spectroscopy, collisional ionization detection.

RADIOACTIVITY 72,74,75,77,79Kr(EC), (β+); 81,76Kr(EC); 80m,83m,85mKr(IT); 85,87,88,89,90,91,92,93,94,95,96Kr(β-); measured isotope shifts, hfs; deduced hyperfine constants, J, μ, electric quadrupole moments, mean square charge radii. Collinear fast beam laser spectroscopy, collisional ionization detection.

doi: 10.1016/0375-9474(94)00786-M


1996LI25

Europhys.Lett. 33, 11 (1996)

P.Lievens, E.Arnold, W.Borchers, U.Georg, M.Keim, A.Klein, R.Neugart, L.Vermeeren, R.E.Silverans

On the Odd-Even Staggering of Mean-Square Charge Radii in the Light Krypton and Strontium Region

NUCLEAR MOMENTS 75,76,77,78,79,80,81,82,83,84,85,86,87,88,89,90,91,92,93,94,96Kr, 78,79,80,82,83,84,85,86,87,88,89,90,91,92,93,94,95,96,97,98,99,100Sr; analyzed rms charge radii differential changes; deduced odd-even staggering related features.

doi: 10.1209/epl/i1996-00296-0


1997SY01

Phys.Rev. C56, 772 (1997)

G.N.Sylvan, J.Doring, G.D.Johns, S.L.Tabor, C.J.Gross, C.Baktash, H.-Q.Jin, D.W.Stracener, P.F.Hua, M.Korolija, D.R.LaFosse, D.Sarantites, F.Cristancho, E.Landulfo, J.X.Saladin, B.Cederwall, I.Y.Lee, A.O.Macchiavelli, W.Rathbun, A.Vander Molen

Deformation Driving Intruder Orbitals in 77Kr

NUCLEAR REACTIONS 58Ni(29Si, 2p2α), E=128 MeV; measured Eγ, Iγ, γγγ-, (charged particle)γ-coin, DCO ratios. 77Kr deduced high-spin levels, J, π, configurations. CSM, TRS calculations.

doi: 10.1103/PhysRevC.56.772


1998DAZV

Program and Thesis, Proc.48th Conf.Ann.Nucl.Spectrosc.Struct.At.Nuclei, Moscow, p.219 (1998)

A.S.Danagulyan, L.G.Martirosyan, J.Adam, A.R.Balabekyan, V.G.Kalinnikov, V.I.Stegailov, A.N.Priemyshev, V.S.Pronskikh, V.M.Tsupko-Sitnikov, Ya.Frana

The Energy Dependence of Cross-Sections of Formation of Production-Nuclei with the Intermediate Mass Number on the Reactions of Protons with Separated Tin Isotopes

NUCLEAR REACTIONS 112,118,120,124Sn(p, X)90Mo/86Zr/88Zr/89Zr/84mY/85Y/86Y/88Y/82Sr/83Sr/85Sr/81Rb/82mRb/83Rb/75Br/76Br/73Se/75Se/77Kr/70As/71As/74As/67Ge/69Ge/67Ga/69Zn/59Fe/56Co/57Co/58Co/52Mn/54Mn/56Mn/49Cr/51Cr/48V/43Sc/44Sc/46Sc/48Sc/42K/43K, E=1, 8.1 GeV; measured productionσ. HpGe detectors.


1999ALZR

JINR-P15-99-268 (1999)

V.Alexandryan, J.Adam, A.Balabekyan, A.Danagulyan, V.G.Kalinnikov, Zh.Musulmanbecov, V.K.Rodionov, V.I.Stegailov, Yar.Frana

Formation of Residual Nuclei with Medium Mass Number in the Reaction of Protons with Separated Tin Isotopes

NUCLEAR REACTIONS 112,118,120,124Sn(p, X)81Sr/81Rb/79Kr/77Kr/76Kr/77Br/76Br/75Br/74Br/75Se/73Se/72Se/76As/74As/72As/71As/70As/69Ge/67Ge/72Ga/67Ga/67Cu/69Zn/59Fe/58Co/57Co/56Co/56Mn/54Mn/52Mn/51Cr/49Cr/48V/48Sc/46Sc/44Sc/43Sc/43K/42K, E=0.66, 1.0, 8.1 GeV; measured Eγ, Iγ; deduced production σ. Comparison with cascade-evaporation model, statistical multifragmentation model. HPGe detector, enriched targets, activation method, accelerator.


2001SA67

Phys.Rev. C64, 064306 (2001)

P.Sarriguren, E.Moya de Guerra, A.Escuderos

β Decay in Odd-A and Even-Even Proton-Rich Kr Isotopes

RADIOACTIVITY 69,70,71,72,73,74,75,76,77Kr(EC), (β+); calculated Gamow-Teller strength distributions, Q(EC), T1/2, deformation dependence. Self-consistent Hartree-Fock approach, comparisons with data.

doi: 10.1103/PhysRevC.64.064306


2002DE56

Appl.Radiat.Isot. 57, 907 (2002)

D.de Villiers, M.Nortier, W.Richter

Experimental and theoretical excitation functions for natBr(p, x) reactions

NUCLEAR REACTIONS Br(p, X)75Br/77Br/80mBr/76Kr/77Kr/79Kr/72Se/73Se/75Se/71As/74As, E ≈ 10-100 MeV; measured σ; deduced excitation functions. Stacked-foil activation technique, comparison with model predictions.

doi: 10.1016/S0969-8043(02)00234-8


2002HE23

Eur.Phys.J. A 15, 17 (2002)

F.Herfurth, A.Kellerbauer, F.Ames, G.Audi, D.Beck, K.Blaum, G.Bollen, O.Engels, H.J.Kluge, D.Lunney, R.B.Moore, M.Oinonen, E.Sauvan, C.Scheidenberger, S.Schwarz, G.Sikler, C.Weber, and the ISOLDE Collaboration

Accurate mass measurements of very short-lived nuclei: Prerequisites for high-accuracy investigations of superallowed β-decays

ATOMIC MASSES 34,36,38Ar, 41K, 74,76Rb, 73,74,75,76,77,78,80,82Kr; measured masses. Penning-trap mass spectrometer.

doi: 10.1140/epja/i2001-10216-x


2005IS09

Yad.Fiz. 68, 1407 (2005); Phys.Atomic Nuclei 68, 1352 (2005)

B.S.Ishkhanov, V.N.Orlin

Employing Spheroidal Global Potential to Estimate the Quadrupole Deformation of Nuclei

NUCLEAR STRUCTURE A=11-241; Z=5-95; analyzed quadrupole moments, deformation. 25Na, 25Mg, 77Kr, 153,165Ho, 229Ra; calculated single-particle level energies vs deformation. Spheroidal global potential.

doi: 10.1134/1.2011495


2006RO11

Nucl.Phys. A769, 1 (2006)

D.Rodriguez, G.Audi, J.Aysto, D.Beck, K.Blaum, G.Bollen, F.Herfurth, A.Jokinen, A.Kellerbauer, H.-J.Kluge, V.S.Kolhinen, M.Oinonen, E.Sauvan, S.Schwarz

Accurate mass measurements on neutron-deficient krypton isotopes

ATOMIC MASSES 72,73,74,75,76,77,78,80,82,86Kr; measured masses. Penning trap mass spectrometer.

doi: 10.1016/j.nuclphysa.2006.02.001


2006TR04

Pramana 66, 389 (2006)

K.C.Tripathy, R.Sahu, S.Mishra

Microscopic study of low-lying collective bands in 77Kr

NUCLEAR STRUCTURE 77Kr; calculated levels, J, π, configurations, rotational bands, B(M1), B(E2). Deformed shell model.


2007NA31

Phys.Rev. C 76, 064609 (2007)

P.Napolitani, K.-H.Schmidt, L.Tassan-Got, P.Armbruster, T.Enqvist, A.Heinz, V.Henzl, D.Henzlova, A.Kelic, R.Pleskac, M.V.Ricciardi, C.Schmitt, O.Yordanov, L.Audouin, M.Bernas, A.Lafriaskh, F.Rejmund, C.Stephan, J.Benlliure, E.Casarejos, M.Fernandez-Ordonez, J.Pereira, A.Boudard, B.Fernandez, S.Leray, C.Villagrasa, C.Volant

Measurement of the complete nuclide production and kinetic energies of the system 136Xe+hydrogen at 1 GeV per nucleon

NUCLEAR REACTIONS 136Xe(p, X), E=1 GeV/nucleon; measured isotopic cross sections, kinetic energies. 6,7,8Li, 9,10,11,12Be, 10,11,12,13B, 11,12,13,14,15C, 13,14,15,16,17N, 15,16,17,18,19O, 17,18,19,20,21F, 19,20,21,22,23Ne, 22,23,24,25Na, 23,24,25,26,27Mg, 25,26,27,28,29,30Al, 28,29,30,31,32Si, 30,31,32,33,34P, 32,33,34,35,36,37,38S, 34,35,36,37,38,39,40Cl, 36,37,38,39,40,41,42,43Ar, 39,40,41,42,43,44,45K, 41,42,43,44,45,46,47Ca, 43,44,45,46,47,48,49,50Sc, 45,46,47,48,49,50,51,52Ti, 46,47,48,49,50,51,52,53,54,55V, 49,50,51,52,53,54,55,56,57Cr, 50,51,52,53,54,55,56,57,58,59,60Mn, 55,56,57,58,59,60,61,62Fe, 57,58,59,60,61,62,63,64,65Co, 59,60,61,62,63,64,65,66,67Ni, 60,61,62,63,64,65,66,67,68,69,70Cu, 62,63,64,65,66,67,68,69,70,71,72Zn, 66,67,68,69,70,71,72,73,74,75Ga, 68,69,70,71,72,73,74,75,76,77Ge, 70,71,72,73,74,75,76,77,78,79,80,81As, 72,73,74,75,76,77,78,79,80,81,82,83Se, 74,75,76,77,78,79,80,81,82,83,84,85Br, 76,77,78,79,80,81,82,83,84,85,86,87,88Kr; measured cross sections.

NUCLEAR REACTIONS 136Xe(p, X), E=1 GeV/nucleon; measured isotopic cross sections, kinetic energies. 79,80,81,82,83,84,85,86,87,88,89,90Rb, 81,82,83,84,85,86,87,88,89,90,91,92,93Sr, 84,85,86,87,88,89,90,91,92,93,94,95,96Y, 86,87,88,89,90,91,92,93,94,95,96,97,98,99Zr, 87,88,89,90,91,92,93,94,95,96,97,98,99,100Nb, 90,91,92,93,94,95,96,97,98,99,100,101,102,103,104Mo, 92,93,94,95,96,97,98,99,100,101,102,103,104,105,106Tc, 95,96,97,98,99,100,101,102,103,104,105,106,107,108,109Ru, 97,98,99,100,101,102,103,104,105,106,107,108,109,110,111Rh, 99,100,101,102,103,104,105,106,107,108,109,110,111,112,113,114,115Pd, 101,102,103,104,105,106,107,108,109,110,111,112,113,114,115,116,117,118,119,120,121,122Ag, 104,105,106,107,108,109,110,111,112,113,114,115,116,117,118,119,120,121,122,123,124,125Cd, 105,106,107,108,109,110,111,112,113,114,115,116,117,118,119,120,121,122,123,124,125,126,127In, 108,109,110,111,112,113,114,115,116,117,118,119,120,121,122,123,124,125,126,127,128,129,130Sn, 110,111,112,113,114,115,116,117,118,119,120,121,122,123,124,125,126,127,128,129,130,131,132Sb, 111,112,113,114,115,116,117,118,119,120,121,122,123,124,125,126,127,128,129,130,131,132,133,134Te, 113,114,115,116,117,118,119,120,121,122,123,124,125,126,127,128,129,130,131,132,133,134,135I, 116,117,118,119,120,121,122,123,124,125,126,127,128,129,130,131,132,133,134,135Xe, 122,123,124,125,126,127,128,129,130,131,132,133,134,135,136Cs, 127,128,129,130,131,132Ba; measured cross sections.

doi: 10.1103/PhysRevC.76.064609


2007ST28

Eur.Phys.J. A 33, 303 (2007)

T.Steinhardt, J.Eberth, I.Ragnarsson

Stable collective triaxial rotation in 77Kr

NUCLEAR STRUCTURE 77Kr; calculated level energies and deformation parameters using configuration-dependent cranked Nilsson-Strutinsky model.

doi: 10.1140/epja/i2006-10456-2


2008KI07

Nucl.Instrum.Methods Phys.Res. A589, 202 (2008)

T.Kibedi, T.W.Burrows, M.B.Trzhaskovskaya, P.M.Davidson, C.W.Nestor, Jr.

Evaluation of theoretical conversion coefficients using BrIcc

COMPILATION Z=5-110; compiled and evaluated ICC data. BrICC database.

doi: 10.1016/j.nima.2008.02.051


2008SI09

Int.J.Mod.Phys. E17, 549 (2008)

P.P.Singh, B.P.Singh, B.Sharma, Unnati, M.K.Sharma, R.Prasad, R.Kumar, H.D.Bhardwaj

Production of fission-like events after complete and/or incomplete fusion of 16O with 159Tb and 169Tm at E/A ≈ MeV

NUCLEAR REACTIONS 159Tb(16O, X), E=5.6 MeV/nucleon; measured Eγ, Iγ. 77Kr, 84mY, 80Sr, 75Br, 104Tc, 83Y, 85Y, 87mY, 81Sr, 83Sr, 85mSr, 74mBr, 83Kr, 88Kr, 94Ru, 102Ag, 95Ru, 79Rb, 87Zr, 110In, 78As, 112Ag; deduced σ of fission like events after complete and/or incomplete fusion. Recoil-catcher technique, γ-spectroscopy.

NUCLEAR REACTIONS 169Tm(16O, X), E=5.9 MeV/nucleon; measured Eγ, Iγ. 107In;66Ge;88Nb;95Y;83Se;99mTc;109Sn;101Tc;79As;105In;108mRh;95Ru;92Y;98mNb;87Kr;92Sr;105Tc;78Ge;110In;104Tc;115Ag;70As;115Ag;70As;112Ag;108In; deduced σ of fission like events after complete and/or incomplete fusion. Recoil-catcher technique, γ-spectroscopy.

doi: 10.1142/S0218301308009902


2009ST04

Phys.Rev. C 79, 015803 (2009)

J.B.Stoker, P.F.Mantica, D.Bazin, A.Becerril, J.S.Berryman, H.L.Crawford, A.Estrade, C.J.Guess, G.W.Hitt, G.Lorusso, M.Matos, K.Minamisono, F.Montes, J.Pereira, G.Perdikakis, H.Schatz, K.Smith, R.G.T.Zegers

β-decay half-life of the rp-process waiting-point nuclide 84Mo

RADIOACTIVITY 80Y, 81Zr, 83,84Nb, 84Mo(EC), (β+) [from 9Be(124Xe, X), E=140 MeV/nucleon]; measured Eγ, (particle)-γ coin, (particle)-β coin, half-life. 64Ge, 68Se, 72Kr, 76Sr, 80Zr, 84Mo, 88Ru;systematics of half-lives and yrast states. Comparisons with QRPA predictions.

NUCLEAR REACTIONS 9Be(124Xe, X)73As/74Se/76Br/77Kr/78Rb/79Sr/80Y/81,82Zr/83Nb/84Nb/84Mo, E=140 MeV/nucleon; measured yields.

doi: 10.1103/PhysRevC.79.015803


2013AN02

At.Data Nucl.Data Tables 99, 69 (2013)

I.Angeli, K.P.Marinova

Table of experimental nuclear ground state charge radii: An update

COMPILATION Z=0-96; compiled nuclear radii, rms nuclear charge radii.

doi: 10.1016/j.adt.2011.12.006


2016ST14

At.Data Nucl.Data Tables 111-112, 1 (2016)

N.J.Stone

Table of nuclear electric quadrupole moments

COMPILATION Z=1-99; compiled experimental values of nuclear electric quadrupole moments.

doi: 10.1016/j.adt.2015.12.002


2017WA10

Chin.Phys.C 41, 030003 (2017)

M.Wang, G.Audi, F.G.Kondev, W.J.Huang, S.Naimi, X.Xu

The AME2016 atomic mass evaluation (II). Tables, graphs and references

ATOMIC MASSES A=1-295; compiled, evaluated atomic masses data.

doi: 10.1088/1674-1137/41/3/030003


2019STZV

INDC(NDS)-0794 (2019)

N.J.Stone

Table of Recommended Nuclear Magnetic Dipole Moments: Part I - Long-lived States

COMPILATION Z=0-99; compiled experimental values of nuclear magnetic moments.


2019ZE02

Appl.Radiat.Isot. 152, 101 (2019)

J.Zeng, Y.Gong, X.Guo, Q.Xiang, F.Hao, Y.Xiang, C.Zhang

Half-life determination of 77Kr using the reference source method

RADIOACTIVITY 77Kr(EC) [from 78Kr(n, 2n), E<14 MeV]; measured decay products, Eγ, Iγ; deduced γ-ray energies, T1/2. Comparison with available data, ENSDF library.

doi: 10.1016/j.apradiso.2019.06.033