Excitation functions and isomeric cross section ratio of the<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mrow><mml:mmultiscripts><mml:mrow><mml:mi mathvariant="normal">Ni</mml:mi></mml:mrow><mml:mprescripts /><mml:mrow /><mml:mrow><mml:mn>58</mml:mn></mml:mrow><mml:mrow /><mml:mrow /></mml:mmultiscripts></mml:mrow></mml:math>(<i>n</i>,<i>p</i><mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mrow><mml:msup><mml:mrow><mml:mo>)</mml:mo></mml:mrow

Buczkó, Cs. M.; Csikai, J.; Sudár, S.; Grallert, Ágnes; Jonah, S.A.; Jimba, B.W.; Chimoye, T.; Wagner, M.

doi:10.1103/physrevc.52.1940

Cited by 21 publications

(5 citation statements)

References 25 publications

(10 reference statements)

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“…Though the proton-and deuteron-induced reactions are most accessible to the majority of modern cyclotrons, there are alternative routes utilizing helium-4 ions, neutrons, or helium-3 nucleus with comparable cross sections [75][76][77]. Alpha beams afford a particularly attractive reaction route using monoisotopic manganese targets via 55 Mn(α,n) 58m Co.…”

Section: Cobalt-58m: Mn Targetsmentioning

confidence: 99%

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Production, Purification, and Applications of a Potential Theranostic Pair: Cobalt-55 and Cobalt-58m

et al. 2021

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The emerging success of [68Ga/177Lu]Ga/Lu-DOTATATE as a theranostic pair has spurred interest in other isotopes as potential theranostic combinations. Here, we review cobalt-55 and cobalt-58m as a potential theranostic pair. Radionuclidically pure cobalt-55 and cobalt-58m have been produced on small cyclotrons with high molar activity. In vitro, DOTATOC labeled with cobalt has shown greater affinity for SSTR2 than DOTATOC labeled with gallium and yttrium. Similarly, [58mCo]Co-DOTATATE has shown improved cell-killing capabilities as compared to DOTATATE labeled with either indium-111 or lutetium-177. Finally, PET imaging with an isotope such as cobalt-55 allows for image acquisition at much later timepoints than gallium, allowing for an increased degree of biological clearance of non-bound radiotracer. We discuss the accelerator targetry and radiochemistry used to produce cobalt-55,58m, emphasizing the implications of these techniques to downstream radiotracers being developed for imaging and therapy.

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Section: Cobalt-58m: Mn Targetsmentioning

confidence: 99%

“…Quasi-monoenergetic neutrons can be produced via 2 H(d,n) 3 He reaction on hydrogen-2 gas targets. The neutrons bombard nickel or cobalt induce the 58 Ni(n,p) 58m Co and 59 Co(n,2n) 58m Co reactions [29,75]. Tritons can be generated via the 6 Li(n,α) 3 H reaction within a nuclear reactor with an energy of 2.736 MeV.…”

Section: Cobalt-58m: Mn Targetsmentioning

confidence: 99%

Production, Purification, and Applications of a Potential Theranostic Pair: Cobalt-55 and Cobalt-58m

et al. 2021

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“…This value is close to our result. From the interpolation of values of Buczko et al [21] and Huang et al [25], the values 543 mb and 531 mb are predicted, respectively. Also the value predicted from the data of Tagesen et al [41] is 546 mb (for 5.45 MeV neutron energy).…”

Section: Thresholdmentioning

confidence: 99%

Measurement of cross sections of threshold detectors with spectrum average technique

Ağuş¹,

Çelenk²,

Özmen³

2004

Radiochimica Acta

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Sc were measured with average neutron energies above effective threshold by using the activation method through usage of spectrum average technique in an irradiation system where there are three equivalent Am/Be sources, each of which has 592 GBq activity. The cross sections were determined with reference to the fast neutron fission cross section of 238 U. The measured values and published values are generally in agreement.

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“…Such predictions can guide the design of the target/blanket configurations and can reduce engineering over design costs. Nickel (Ni) is an important structural material in fusion and also fission reactor technologies as well as for fast neutron dosimetry [5,6]. Precise knowledge of reaction cross sections and isotopic effects in the (n,p), (p,n), (p,p), (p,a) reaction cross-sections on Nickel isotopes are very important on the selection of fusion structural materials [6].…”

Section: Introductionmentioning

confidence: 99%

Neutron, Proton and Alpha Emission Spectra of Nickel Isotopes for Proton Induced Reactions

Tel

Kara

2011

J Fusion Energ

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The fusion energy is attractive as an energy source because the fusion will not produce CO 2 or SO 2 and so fusion will not contribute to environmental problems, such as particulate pollution and excessive CO 2 in the atmosphere. The fusion reaction does not produce radioactive nuclides and it is not self-sustaining, as is a fission reaction when a critical mass of fissionable material is assembled. Since the fusion reaction is easily and quickly quenched the primary sources of heat to drive such an accident are heat from radioactive decay and heat from chemical reactions. Both the magnitude and time dependence of the generation of heat from radioactive decay can be controlled by proper selection and design of materials.

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Excitation functions and isomeric cross section ratio of theNi58(n,p)

Cited by 21 publications

References 25 publications

Production, Purification, and Applications of a Potential Theranostic Pair: Cobalt-55 and Cobalt-58m

Production, Purification, and Applications of a Potential Theranostic Pair: Cobalt-55 and Cobalt-58m

Measurement of cross sections of threshold detectors with spectrum average technique

Neutron, Proton and Alpha Emission Spectra of Nickel Isotopes for Proton Induced Reactions

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