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941.
A. N. Aleev N. S. Amaglobeli V. P. Balandin O. V. Bulekov I. M. Geshkov T. S. Grigalashvili E. A. Goudzovski D. K. Guriev D. D. Emelianov S. V. Eremin A. I. Zinchenko Z. M. Ivanchenko I. M. Ivanchenko M. N. Kapishin A. A. Loktionov V. D. Kekelidze Z. I. Kozhenkova V. V. Korenkov I. G. Kosarev N. A. Kuzmin A. L. Ljubimov D. T. Madigozhin V. G. Maznyj A. S. Mestvirishvili N. A. Molokanova A. N. Morozov R. E. Pismenyj V. D. Poze I. A. Polenkevich A. K. Ponosov T. Ponta Yu. K. Potrebenikov F. M. Sergeev L. A. Slepets V. N. Spaskov 《Physics of Atomic Nuclei》2004,67(8):1513-1522
The features of the associated production of φ mesons with Λ0 hyperons in neutron-carbon interactions were investigated. The experiment was performed with the aid of the EXCHARM spectrometer at the Serpukhov accelerator in a neutron beam of energy in the interval 20–70 GeV. The differential cross section for inclusive associated φΛ0 production was measured. 相似文献
942.
M. L. Bonardi C. Birattari F. Groppi L. Gini H. S. C. Mainardi 《Journal of Radioanalytical and Nuclear Chemistry》2004,259(3):415-419
Radionuclides of very high specific activity A
S(t) have great relevance for applications in the life sciences. Updated definitions of A
S are given. The real A
S(t) must be measured by analytical and radioanalytical techniques. No-carrier-added (NCA) radionuclides have A
S(NCA) sometimes close to the carrier-free (CF) value A
S(CF). The accurate knowledge of excitation functions of nuclear reactions vs. ion beam energy is mandatory to maximize A
S(NCA); the minimization of isotopic dilution factor IDF(t) has been achieved too. A range of accelerator production and radioanalytical QC methods for A
S(NCA) optimization and determination is presented.
This revised version was published online in August 2006 with corrections to the Cover Date. 相似文献
943.
S. Akin S. Isikli F. Korkusuz M. Ungan A. Senkoylu 《Journal of Radioanalytical and Nuclear Chemistry》2004,259(2):361-364
The aim of this study was to investigate the relationship between BMD and age at lumbar spine and proximal femur in Turkish
males. Two hundred ninety healthy males (aged 20-59 years) were investigated. BMD of the lumbar spine had its peak at ages
30-39, however, the peak for the proximal femur was between the ages of 20 and 29. There was a significant decrease in BMD
at proximal femur after these peak values with increasing age. In conclusion, there was a significant correlation between
age and the proximal femoral BMD in males and age has a strong predictive power on proximal femur BMD score.
This revised version was published online in August 2006 with corrections to the Cover Date. 相似文献
944.
945.
946.
We introduce a generalized notion of semiring and prove that all known properties that semirings have according to the old definition are preserved. 相似文献
947.
F. v. Arlt 《Monatshefte für Chemie / Chemical Monthly》1901,20(5):425-449
Ohne ZusammenfassungEs sei mir gestattet, auch an dieser Stelle meinem hochverehrten Lehrer, Herrn Prof. Dr. Zd. H. Skraup, für das während meiner ganzen Studienzeit mir entgegengebrachte Interesse und Wohlwollen, sowie ganz besonders für die Unterstützung und Förderung bei Ausarbeitung der vorliegenden Dissertation herzlich und aufrichtig zu danken. 相似文献
948.
949.
950.
The π? p→e + e ? n and π+ n→e + e ? p reaction cross sections are calculated below and in the vicinity of the vector-meson (?0,ω) production threshold. These processes are largely responsible for the emission of e +e? pairs in pion-nucleus reactions and contribute to the dilepton spectra observed in relativistic heavy ion collisions. They are dominated by the decay of low-lying baryon resonances into vector-meson-nucleon channels. The vector mesons materialize subsequently into e + e? pairs. Using πN→?0 N and πN→ωN, amplitudes calculated in the center of mass energy interval 1.4 < √s<1.8 GeV, we compute the π? p→e + e ? n and π+ n→e + e ? p reaction cross sections in these kinematics. Below the vector-meson production threshold, the π0?ω interference in the e + e? channel appears largely destructive for the π? p→e + e ? n cross section and constructive for the π+ n→e + e ? p cross section. The pion beam and the HADES detector at GSI offer a unique possibility to measure these effects. Such data would provide strong constraints on the coupling of vector-meson-nucleon channels to low-lying baryon resonances. 相似文献