<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mi>α</mml:mi></mml:math>-particle induced reactions on yttrium and terbium

Mukherjee, S. N.; Kumar, B Bindu; Rashid, M. H.; Chintalapudi, S. N.

doi:10.1103/physrevc.55.2556

Cited by 19 publications

(19 citation statements)

References 38 publications

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“…3 together with the experimental data [13][14][15][16] and data from the TENDL-2013 library [20]. The present data are in general agreement with the data reported by Mukherjee et al [13] and Levkovskij et al [15] but are higher than those measured by Singh et al [14] and Smend et al [16]. The overall shape of the excitation curve looks similar to that of the theoretical data obtained from the TENDL-2013 library [20].…”

Section: Y(a3n) 90 Nb Reactionsupporting

confidence: 95%

“…5 together with data from the literature [13,15] and from the TENDL-2013 library [20] based on the TALYS 1.6 code [21]. The measured cross-sections below 35 MeV regions are lower than those obtained by Mukherjee et al [13]. The present excitation function showed similar tendency with data extracted from the TENDL-2013 library.…”

Section: Y(an) 92m Nb Reactionsupporting

confidence: 85%

“…The measured cross-sections for the 92m Nb production are presented in Fig. 5 together with data from the literature [13,15] and from the TENDL-2013 library [20] based on the TALYS 1.6 code [21]. The measured cross-sections below 35 MeV regions are lower than those obtained by Mukherjee et al [13].…”

Section: Y(an) 92m Nb Reactionmentioning

confidence: 83%

“…The emission of b + (E mean = 0.66 MeV and E max = 1.5 MeV) from 90 Nb makes it especially promising for the immuno-PET and clinical applications [11,12]. Only limited excitation functions for the alpha-induced reactions on 89 Y are available in the various energy ranges [13][14][15][16][17][18][19]. In the present work, we measured the excitation functions of 89g,m Nb, 90 Nb, 91m Nb, 92m Nb, 88 Zr, 89 Zr, 87g,m Y, 88 Y, 90m Y, and 91m Y in the 89 Y(a,x) reactions by the stacked-foil activation and off-line c-ray spectrometric technique in the energy range between their respective reaction threshold and 45 MeV at the MC-50 cyclotron of the Korean Institute of Radiological and Medical Sciences (KIRAMS), Korea.…”

Section: Introductionmentioning

confidence: 98%

“…In the present work, we measured the excitation functions of 89g,m Nb, 90 Nb, 91m Nb, 92m Nb, 88 Zr, 89 Zr, 87g,m Y, 88 Y, 90m Y, and 91m Y in the 89 Y(a,x) reactions by the stacked-foil activation and off-line c-ray spectrometric technique in the energy range between their respective reaction threshold and 45 MeV at the MC-50 cyclotron of the Korean Institute of Radiological and Medical Sciences (KIRAMS), Korea. The experimental results measured in this work were compared with the literature data [13][14][15][16] and also theoretical values obtained from TENDL-2013 library [20] based on the computer code TALYS-1.6 [21]. The integral yields for thick target of the investigated radioisotopes were calculated from the excitation function and the electronic stopping power.…”

Section: Introductionmentioning

confidence: 99%

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Measurement of excitation functions in alpha-induced reactions on yttrium

Shahid

Kim

Naik

et al. 2015

Nuclear Instruments and Methods in Physics Research Section B:

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Y(a,x) reactions MC-50 cyclotron Stacked-foil activation technique Excitation functionOff line c-ray spectrometry a b s t r a c tThe excitation functions of 89g,m,90,91m,92m Nb, 88,89 Zr, and 87g,m,88,90m,91m Y from alpha-induced reactions on 89 Y were measured from their respective threshold to 45 MeV by using a stacked-foil activation technique at the MC-50 cyclotron of the Korean Institute of Radiological and Medical Sciences. The results were compared with the earlier reported data as well as with the theoretical values obtained from the TENDL-2013 library based on the TALYS1.6 code. Our measurements in the energy region from the threshold energy to 45 MeV are in general good agreement with the other experimental data and calculated results. The integral yields for thick target of the produced radionuclides were also deduced from their measured cross sections and the stopping power of 89 Y. The measured excitation functions find importance in various practical applications including nuclear medicine and improvement of nuclear model calculations.

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Section: Y(a3n) 90 Nb Reactionsupporting

confidence: 95%

Section: Y(an) 92m Nb Reactionsupporting

confidence: 85%

Section: Y(an) 92m Nb Reactionmentioning

confidence: 83%

Section: Introductionmentioning

confidence: 98%

Section: Introductionmentioning

confidence: 99%

See 3 more Smart Citations

Measurement of excitation functions in alpha-induced reactions on yttrium

Shahid

Kim

Naik

et al. 2015

Nuclear Instruments and Methods in Physics Research Section B:

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Investigation of production routes for the 161Ho Auger-electron emitting radiolanthanide, a candidate for therapy

Tárkányi

Ditrói

Hermanne

et al. 2013

J Radioanal Nucl Chem

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The radiolanthanide 161 Ho (2.48 h) is a promising Auger-electron emitter for internal radiotherapy that can be produced with particle accelerators. The excitation functions of the nat Dy(p,xn) 161 Ho and nat Dy(d,x) 161 Ho reactions were measured up to 40 and 50 MeV respectively by using the stacked foil activation method and -ray spectrometry. The experimental data were compared with results of the TALYS code available in the TENDL 2011 library [1]. The main parameters of different production routes are discussed.Keywords medical radioisotopes · therapeutical isotopes · proton and deuteron irradiation · 161 Ho · 162m Ho arXiv:1301.7176v1 [nucl-ex]

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Recommended nuclear data for medical radioisotope production: diagnostic positron emitters

Tárkányi

Ignatyuk

Hermanne

et al. 2019

J Radioanal Nucl Chem

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An IAEA coordinated research project that began in 2012 and ended in 2016 was primarily dedicated to the compilation, evaluation and recommendation of cross-section data for the production of medical radionuclides. One significant part of this work focused on diagnostic positron emitters. These particular studies consist of 69 reactions for direct and indirect or generator production of 44 Sc(44 Ti), 52m Mn(52 Fe), 52g Mn, 55 Co, 61 Cu, 62 Cu(62 Zn), 66 Ga, 68 Ga(68 Ge), 72 As(72 Se), 73 Se, 76 Br, 82 Rb(82 Sr), 82m Rb, 86 Y, 89 Zr, 90 Nb, 94m Tc, 110m In(110 Sn), 118 Sb(118 Te), 120 I, 122 I(122 Xe), 128 Cs(128 Ba), and 140 Pr(140 Nd) medical radionuclides. The resulting reference cross-section data were obtained from Padé fits to selected and corrected experimental data, and integral thick target yields were subsequently deduced. Uncertainties in the fitted results were estimated via a Padé least-squares method with the addition of a 4% assessed systematic uncertainty. Experimental data were also compared with theoretical predictions available from the TENDL-2015 and TENDL-2017 libraries. All of the numerical reference cross-section data with their corresponding uncertainties and deduced integral thick target yields are available on-line at the IAEA-NDS medical portal www-nds.iaea.org/medic alpor tal and also at the IAEA-NDS web page www-nds.iaea.org/ medic al/posit ron_emitt ers.html.

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α-particle induced reactions on yttrium and terbium

Cited by 19 publications

References 38 publications

Measurement of excitation functions in alpha-induced reactions on yttrium

Measurement of excitation functions in alpha-induced reactions on yttrium

Investigation of production routes for the 161Ho Auger-electron emitting radiolanthanide, a candidate for therapy

Recommended nuclear data for medical radioisotope production: diagnostic positron emitters

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