References from selected dataset

RADIOACTIVITY ⁷⁵Br[from ⁷⁶Se(p, 2n)]; measured Eγ, Iγ, Eβ, Iβ, γγ-, βγ-coin, T_1/2; deduced log ft. ⁷⁵Se deduced levels, T_1/2. Enriched ⁷⁶Se target; Ge(Li), Si(Li), NaI(Tl) detectors.

doi: 10.1016/0375-9474(69)90379-0

1969RE14

Phys.Rev. 188, 1771 (1969)

R.C.Reedy, M.J.Fluss, G.F.Herzog, L.Kowalski, J.M.Miller

Study of Protons and Alpha Particles Emitted from Br⁷⁵ Compound Nuclei With Differing Angular-Momentum Distributions

NUCLEAR REACTIONS ⁶⁴Zn(¹¹B, X), E=43, 89 MeV; ⁶³Cu(¹²C, X), E=55, 100 MeV; ⁵⁹Co(¹⁶O, X), E=58, 110 MeV; measured σ(Ep, Eα, θ(p), θ(α)). ⁷⁵Br deduced compound-nucleus angular momentum distribution effects.

doi: 10.1103/PhysRev.188.1771

1972CO06

Nucl.Phys. A182, 385 (1972)

A.Coban, J.C.Willmott, J.C.Lisle, G.Murray

A Study of the Energy Levels of ⁷⁵Se

RADIOACTIVITY ⁷⁵Br[from ⁶⁵Cu(¹²C, 2n)⁷⁵Br]; measured Eγ, Iγ, T_1/2, ICC, γγ-coin;γγ-delay; deduced log ft. ⁷⁵Se deduced levels, J, π, T_1/2, γ-multipolarity. Enriched target; Ge(Li), Si(Li) detectors.

doi: 10.1016/0375-9474(72)90285-0

1974RO11

Z.Phys. 266, 65 (1974)

E.Roeckl, D.Lode, K.Bachmann, B.Neidhart, G.K.Wolf, W.Lauppe, N.Kaffrell, P.Patzelt

Decay Properties of Neutron Deficient Kr Isotopes

RADIOACTIVITY ^{73,74,75,76,77}Kr, ^73,74,75,76Br; measured T_1/2, Eβ, βγ-coin. Deduced Q. ^73,74Kr measured Eγ, Iγ.

1974RO12

Z.Phys. 266, 123 (1974)

E.Roeckl, D.Lode, W.Pessara

The Decay of ⁷⁵Kr

RADIOACTIVITY ⁷⁵Kr; measured Eγ, Iγ, γγ-coin, T_1/2, I(ce), γγ(t), Eβ. Deduced ICC, log ft, Q. ⁷⁵Br deduced levels, J, π, T_1/2, γ-mixing.

1976LA11

Phys.Rev. C14, 152 (1976)

M.Langevin, J.Barreto, C.Detraz

Complete Fusion Mechanism in the ¹⁶O + ⁶³Cu Reaction

NUCLEAR REACTIONS ⁶³Cu(¹⁶O, 2n), (¹⁶O, np), (¹⁶O, 2np), (¹⁶O, 3np), ⁶³Cu(¹⁶O, 2p), (¹⁶O, n2p), (¹⁶O, 2n2p), (¹⁶O, nα), (¹⁶O, 2nα), (¹⁶O, npα), (¹⁶O, n2pα), (¹⁶O, 2α), (¹⁶O, n2α), (¹⁶O, np2α), E=40-85 MeV; measured σ(E); deduced critical angular momentum. Enriched target.

doi: 10.1103/PhysRevC.14.152

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

1980EK02

Phys.Scr. 22, 344 (1980)

C.Ekstrom, L.Robertsson

Nuclear Spins of the Bromine Isotopes ^{74m,75,77m,78}Br

NUCLEAR MOMENTS ^74,75,77,78Br [from Nb(p, x), E=660 MeV]; measured J, hfs. Atomic-beam magnetic resonance technique. Strong coupling model.

1981KR10

Phys.Rev. C24, 148 (1981)

A.J.Kreiner, M.A.J.Mariscotti, C.Baktash, E.der Mateosian, P.Thieberger

High Spin Structure of ⁷⁵Br and the (N, Z) Dependence of the Nuclear Deformation in the Br Region

NUCLEAR REACTIONS ⁶²Ni(¹⁶O, 2np), E=45-70 MeV; measured Eγ, Iγ, T_1/2, γγ-coin. ⁷⁵Br deduced levels, J, π. Enriched target, Ge(Li) detector. Particle plus rotor model.

doi: 10.1103/PhysRevC.24.148

1981WI05

Nucl.Phys. A367, 95 (1981)

G.Winter, J.Doring, W.D.Fromm, L.Funke, P.Kemnitz, H.Prade, E.Will

Evidence for Deformed States in ⁷⁵Br

NUCLEAR REACTIONS ⁷⁴Se(³He, pn), E=28, 32 MeV; measured Eγ, σ(E, Eγ, θ), γγ-coin; ⁷⁴Se(p, γ), E=6.7 MeV; measured Eγ, σ(Eγ, θ), γγ-coin, pγ(t); ⁷⁴Se(d, n), E=12, 13.5 MeV; measured Eγ, σ(E, Eγ), γγ-coin, dγ(t); ⁷⁴Se(α, 2np), E=51-59 MeV; measured Eγ, σ(Eγ), γγ-coin. ⁷⁵Br deduced levels, J, π, T_1/2. Enriched target, Ge detectors.

doi: 10.1016/0375-9474(81)90279-7

1982AL20

Radiochim.Acta 30, 67 (1982)

Z.B.Alfassi, R.Weinreich

The Production of Positron Emitters ⁷⁵Br and ⁷⁶Br: Excitation Functions and Yields for ³He and α-Particle Induced Nuclear Reactions on Arsenic

NUCLEAR REACTIONS ⁷⁵As(³He, xn), E=threshold - 70 MeV; ⁷⁵As(α, xn)⁷⁷Br/⁷⁶Br/⁷⁵Br/⁷⁴Br, E=threshold -140 MeV; measured production σ(E) for ^77,76,75,74mBr; deduced thick target yields. Activation technique.

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

1982BL07

Int.J.Appl.Radiat.Isotop. 33, 333 (1982)

G.Blessing, R.Weinreich, S.M.Qaim, G.Stocklin

Production of ⁷⁵Br and ⁷⁷Br via the ⁷⁵As(³He, 3n)⁷⁵Br and ⁷⁵As(α, 2n)⁷⁷Br Reactions using Cu₃As-alloy as a High-Current Target Material

NUCLEAR REACTIONS, ICPND ⁷⁵As(³He, 3n), E=25-36 MeV; ⁷⁵As(α, 2n), E=14-28 MeV; measured thick target yields of ^75,77Br. High current Cu₃As alloy target.

doi: 10.1016/0020-708X(82)90145-4

1982FR18

J.Labelled Compd.Radiopharm. 19, 1427 (1982)

A.M.Friedman, O.J.DeJesus, P.Harper, C.Armstrong

Preparation of ⁷⁵Br by the ⁷⁸Kr(p, α)⁷⁵Br Reaction

NUCLEAR REACTIONS, ICPND ⁷⁸Kr(p, α), E=12-15 MeV; measured residual production σ(E). Activation technique.

1982MI07

Izv.Akad.Nauk SSSR, Ser.Fiz. 46, 877 (1982)

V.E.Mitroshin, B.A.Nemashkalo, V.K.Chirt

Structure of the Excited States of the Odd Isotopes ^{75,77,79,81,83}Br

NUCLEAR STRUCTURE ^{75,77,79,81,83}Br; calculated levels, B(λ), quadrupole moment, μ, γ-branching.

1984BL16

Int.J.Appl.Radiat.Isotop. 35, 927 (1984)

G.Blessing, S.M.Qaim

An Improved Internal Cu₃As-Alloy Cyclotron Target for the Production of ⁷⁵Br and ⁷⁷Br and Separation of the By-Product ⁶⁷Ga from the Matrix Activity

NUCLEAR REACTIONS, ICPND ⁷⁵As(³He, 3n), E=25-36 MeV; ⁷⁵As(α, n), E=14-28 MeV; measured residuals thick target yields vs E. ⁶⁵Cu(α, 2n), E=28 MeV; measured residual thick target yield. Internal target system, high current Cu₃As alloy.

doi: 10.1016/0020-708X(84)90204-7

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.

1985HU06

Hyperfine Interactions 22, 439 (1985)

M.Huyse, G.Brijs, P.De Bisschop, J.Gentens, E.Coenen, K.Deneffe, P.Van Duppen

Recent Developments at the Leuven Isotope Separator On Line

RADIOACTIVITY ^104,105Sn(β⁺), (EC) [from ⁹²Mo(²⁰Ne, X), E=210 MeV]; measured Eγ, Iγ, E X-ray, I X-ray, γγ(t), γ(X-ray)(t). ^104,105In deduced levels, γ-branching.

NUCLEAR REACTIONS Ni(³²S, X)⁸⁴Sr/⁸³Sr/⁸¹Sr/⁸⁴Rb/⁸¹Rb/⁸⁰Rb/⁷⁹Rb/⁷⁸Rb/^78mRb/⁷⁷Rb/⁷⁶Rb/⁷⁵Rb/⁸¹Kr/^81mKr/⁷⁸Kr/⁷⁵Kr/⁷³Kr/⁷⁷Br/^77mBr/⁷⁵Br/^74mBr/⁷⁴Br/⁷³Br/⁷²Br, E=280 MeV; ⁹²Mo(²⁰Ne, X)¹⁰⁷In/¹⁰⁶In/¹⁰⁵In/¹⁰⁴In/¹⁰³In/¹⁰²In/¹⁰³Cd/¹⁰²Cd/¹⁰³Ag/¹⁰²Ag, E=180 MeV; Re(¹⁶O, X)¹⁹⁶Bi/¹⁹⁵Bi/¹⁹⁴Bi/¹⁹³Bi/¹⁹²Bi/¹⁹⁵Pb/¹⁹⁴Pb/¹⁹³Pb/¹⁹²Pb/¹⁹¹Pb/¹⁹⁴Tl/¹⁹³Tl/¹⁹²Tl/¹⁹¹Tl, E=210 MeV; measured residual yields. Activation technique.

1985KO25

Int.J.Appl.Radiat.Isotop. 36, 635 (1985)

Z.Kovacs, G.Blessing, S.M.Qaim, G.Stocklin

Production of ⁷⁵Br via the ⁷⁶Se(p, 2n)⁷⁵Br Reaction at a Compact Cyclotron

NUCLEAR REACTIONS, ICPND ⁷⁶Se(p, n), E ≈ 7-40 MeV; ⁷⁶Se(p, 2n), E ≈ 15.5-40 MeV; ⁷⁶Se(p, 3n), E ≈ 32-40 MeV; ⁷⁶Se(p, α), E=10-40 MeV; ⁷⁶Se(p, nα), E=20-40 MeV; ⁷⁶Se(p, 2nα), E=30-40 MeV; ⁷⁶Se(p, np), E=13-40 MeV; measured reaction σ(E). ⁷⁶Se(p, ³He), (p, n2p), (p, pd), E ≈ 29-40 MeV; measured summed reaction σ(E). ⁷⁶Se(p, xn)⁷⁶Br/⁷⁵Br/^74mBr, E=threshold-40 MeV; calculated cumulative thick target yield vs E. Activation technique.

doi: 10.1016/0020-708X(85)90004-3

1985SK04

Izv.Akad.Nauk SSSR, Ser.Fiz. 49, 2252 (1985); Bull.Acad.Sci.USSR, Phys.Ser. 49, No.11, 160 (1985)

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

Electro- and Photodisintegration of ⁹³Nb in the 0.1-1.2 GeV Energy Range

NUCLEAR REACTIONS ⁹³Nb(e, X), (γ, X)⁹²Nb/^92mNb/⁸⁹Nb/⁸⁹Zr/⁸⁶Zr/⁸⁶Y/⁹¹Y/^91mY/⁹⁰Y/^90mY/⁸⁷Y/^87mY/⁸⁶Y/^86mY/⁸⁵Y/⁹⁰Nb/⁸⁷Zr/⁸⁴Y/⁸³Sr/⁸¹Rb/⁷⁶Br/⁷⁵Br/⁷³Se/⁷²As/⁷¹As, E=0.1-1.2 GeV; measured independent, cumulative yields following electro-, photodisintegration.

1985VA19

Int.J.Appl.Radiat.Isotop. 36, 961 (1985)

W.Vaalburg, A.M.J.Paans, J.W.Terpstra, T.Wiegman, K.Dekens, A.Rijskamp, M.G.Woldring

Fast Recovery by Dry Distillation of ⁷⁵Br Induced in Reusable Metal Selenide Targets via the ⁷⁶Se(p, 2n)⁷⁵Br Reaction

NUCLEAR REACTIONS, ICPND ⁷⁶Se(p, 2n), E=22-28 MeV; measured residual yield. Metallic selenide targets.

doi: 10.1016/0020-708X(85)90256-X

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 T_1/2, 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

1986QA05

Int.J.Appl.Radiat.Isotop. 37, 803 (1986)

S.M.Qaim

Recent Developments in the Production of ¹⁸F, ^75,76,77Br and ¹²³I

NUCLEAR REACTIONS, ICPND ¹⁸O(p, n), E=3-16 MeV; ²⁰Ne(d, α), E=2-14 MeV; ⁷⁶Se(p, 2n), E=16-35 MeV; ⁷⁵As(³He, 3n), E=17-35 MeV; Br(d, xn), (p, xn)⁷⁶Kr, E=50-80 MeV; ⁷⁶Se(³He, 3n), E=30-36 MeV; ^76,77Se(p, n), E=10-25 MeV; ⁷⁵As(³He, 2n), E=10-18 MeV; compiled thick target yields of ¹⁸F, ^75,76Br; ¹²³Xe(p, 2n), (p, np), E=14-30 MeV; compiled σ(E).

1988DE24

Appl.Radiat.Isot. 39, 709 (1988)

O.T.De Jesus, A.M.Friedman

Production of ⁷⁵Br via the ⁷⁸Kr(d, nα)⁷⁵Br Reaction

NUCLEAR REACTIONS, ICPND ⁷⁸Kr(d, nα), E=21.5 MeV; measured residual production yield.

1988GR26

Hyperfine Interactions 43, 481 (1988)

A.G.Griffiths, C.J.Ashworth, I.S.Grant, J.Rikovska, N.J.Stone, P.M.Walker, W.B.Walters, J.P.White

Deformation in the Light Br Isotopes

RADIOACTIVITY ^{72,74m,75,76,77}Br [from ⁵⁴Fe(²⁸Si, X), E=150 MeV]; measured γ(θ), oriented nuclei. ^{72,72m,74m,75,77}Br deduced μ. ⁷³Br deduced μ, J.

1988TO08

Phys.Rev. C38, 267 (1988)

M.J.Tobin, P.J.Karol

Unexpected Recoil Systematics of Intermediate Energy Spallation Products

NUCLEAR REACTIONS ⁸⁹Y(p, X)⁶⁵Ga/⁶⁶Ga/⁶⁷Ge/⁶⁷Ga/⁶⁸Ga/⁶⁹As/⁶⁹Ge/⁷⁰As/⁷⁰Ga/⁷¹As/⁷²As/⁷²Ga/⁷³Ga/⁷⁴Br/⁷⁴As/⁷⁴Ga/⁷⁵Br/⁷⁵Ge/⁷⁶Br/⁷⁶As/⁷⁷Br/⁷⁷Ge/⁷⁸Br/⁸⁰Br/⁸²Br, E=800 MeV; measured residual production, recoil properties. Activation technique.

doi: 10.1103/PhysRevC.38.267

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.

1989LO03

J.Labelled Compd.Radiopharm. 26, 169 (1989)

C.Loch, B.Maziere

⁷⁵Br Production: Electrochemical preparation of an As-Cu target

NUCLEAR REACTIONS Cu, As(³He, X)⁷⁵Br, E=28 MeV; measured residual yield.

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).

1992BA68

Hyperfine Interactions 75, 433 (1992)

C.G.Barham, S.S.Al-Ghamdi, A.Bhagwat, M.Booth, I.S.Grant, M.Lindroos, J.Rikovska, B.D.D.Singleton, N.J.Stone, P.M.Walker

On-Line Orientation of Bromine Isotope

RADIOACTIVITY ^74mBr(β⁺), (EC); ⁷²Br(β⁺); measured γ-anisotropy. ⁷²Br level deduced μ limits. ⁷⁵Br(β⁺), (EC); measured β-asymmetry; deduced level configuration. On-line orientation.

1992GR20

Phys.Rev. C46, 2228 (1992)

A.G.Griffiths, C.J.Ashworth, J.Rikovska, N.J.Stone, J.P.White, I.S.Grant, P.M.Walker, W.B.Walters

Magnetic Moments and Shape Coexistence in the Light Br Isotopes

RADIOACTIVITY ^{72g,72m,73,74m,75,76g,77}Br; measured γ(θ, H, T), oriented nuclei implanted into Fe. ⁷³Br level deduced J. ^{72,74,75,76,77}Br levels deduced μ. Model comparison.

doi: 10.1103/PhysRevC.46.2228

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

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

1994LU02

Chin.Phys.Lett. 11, 65 (1994)

Q.Luo, G.Dai

Mass-Asymmetric Breakup in the Extended Finite-Range Macroscopic Model

NUCLEAR REACTIONS, ICPND ¹⁸¹Ta(¹²C, F), E=46.7 MeV/nucleon; calculated fission fragment yield vs mass. Extended finite-range macroscopic model.

NUCLEAR STRUCTURE ^110,112In, ¹⁵⁹Tb, ²⁰⁹Bi, ⁷⁵Br; calculated fission barrier vs mass asymmetry. Extended finite-range macroscopic model.

1994SC47

J.Labelled Compd.Radiopharm. 35, 260 (1994)

D.J.Schlyer, S.Tischer, M.Firouzbakht

Production and Processing of Bromine-75 from the ⁷⁵As(³He, 3n)⁷⁵Br Reaction

NUCLEAR REACTIONS ⁷⁵As(³He, 3n), E=38 MeV; measured residual yield; deduced ⁷⁶Br % impurity.

1995MA97

Nucl.Instrum.Methods Phys.Res. B99, 645 (1995)

J.G.Marques, J.G.Correia, A.A.Melo, M.F.da Silva, J.C.Soares, and the ISOLDE-CERN Isotope Separator Collaboration

Nuclear Structure Studies with (p, n) Reactions at Intermediate Energies

RADIOACTIVITY ⁷³As(EC); ⁷⁵Br(EC), (β⁺); ^111mCd(IT); compiled, reviewed γ(e^-)(θ, H) data. ^197mHg(IT), (EC); ^199mHg(IT); measured γ(e^-)(θ, H, t); deduced magnetic hyperfine field, electric field gradient in Co. Four detector γ(e^-) spectrometer, ISOLDE isotope separator.

doi: 10.1016/0168-583X(94)00591-5

1995RA07

Phys.Rev. C51, 2833 (1995)

G.V.Ravi Prasad, V.S.Ramamurthy, R.T.Yadav

Simple Formula for Conditional Fission Barriers of Rotating Nuclei

NUCLEAR STRUCTURE ⁷⁵Br, ¹¹⁰In, ⁵⁵Co; calculated fission barrier vs fragment charge. ²⁴⁴Cm; calculated fission fragment yield vs charge. Extended Swiatecki's fusion model.

doi: 10.1103/PhysRevC.51.2833

1995RO10

Phys.Rev. C51, 2813 (1995)

G.Royer, F.Haddad

Asymmetric Fission Barriers and Total Kinetic Energies for ¹⁹⁴Hg, ¹⁴⁹Tb, ¹¹⁰^-¹¹²In, ⁹⁴Mo, and ⁷⁵Br

NUCLEAR STRUCTURE ¹⁴⁹Tb, ⁷⁵Br, ⁹⁴Mo, ⁵²Fe, ^110,111,112In, ¹⁹⁴Hg; calculated total kinetic energy, fission barrier heights vs fragment charge.

doi: 10.1103/PhysRevC.51.2813

1999SO10

Phys.Rev. C59, 1339 (1999)

G.Z.Solomon, G.D.Johns, R.A.Kaye, S.L.Tabor

Shape Competition and Shape Coexistence in ⁷⁵Br

NUCLEAR REACTIONS ⁴⁸Ti(³⁰Si, 2np), E=90 MeV; measured Eγ, Iγ, γγ-coin. ⁷⁵Br deduced high-spin levels, J, π, configurations, deformation. Cranked shell model, particle-rotor model calculations.

doi: 10.1103/PhysRevC.59.1339

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

2009MU16

Nucl.Phys. A829, 137 (2009)

G.Mukherjee, P.Joshi, R.K.Bhowmik, S.N.Roy, S.Dutta, S.Muralithar, R.P.Singh

Effect of πg_9/2 and νg_9/2 alignments in the shape of ⁷⁵Br from lifetime measurement

NUCLEAR REACTIONS ⁵¹V(²⁸Si, 2n2p), E=115 MeV; measured Eγ, Iγ, γγ-coin with HPGe detectors. ⁷⁵Br; deduced high spin states T_1/2, B(E2), band configurations using DSA, transition quadrupole moments and deformation parameters. Comparison with cranking model and total Routhian surface calculations.

doi: 10.1016/j.nuclphysa.2009.07.016

2011HE10

Eur.Phys.J. A 47, 75 (2011)

F.Herfurth, G.Audi, D.Beck, K.Blaum, G.Bollen, P.Delahaye, M.Dworschak, S.George, C.Guenaut, A.Kellerbauer, D.Lunney, M.Mukherjee, S.Rahaman, S.Schwarz, L.Schweikhard, C.Weber, C.Yazidjian

New mass data for the rp-process above Z = 32

ATOMIC MASSES ^{70,71,72,73,74}Se, ^72,73,74,75Br; measured mass excess from Zr(p, X), E=1.4 GeV using thick target with ISOLTRAP.

doi: 10.1140/epja/i2011-11075-6

2011STZZ

INDC(NDS)-0594 (2011)

N.J.Stone

Table of nuclear magnetic dipole and electric quadrupole moments

COMPILATION Z=1-99, N=1-254; compiled experimental data on nuclear magnetic and electrical quadrupole moments.

2012WA38

Chin.Phys.C 36, 1603 (2012)

M.Wang, G.Audi, A.H.Wapstra, F.G.Kondev, M.MacCormick, X.Xu, B.Pfeiffer

The AME2012 atomic mass evaluation (II). Tables, graphs and references

COMPILATION A=1-295; compiled, evaluated atomic mass data.