Abstract
AbstractThe photoproduction of $$^{95\mathrm m}$$
95
m
Nb on $${^\textrm{nat}\textrm{Mo}}$$
nat
Mo
was studied using the electron beam of the LUE-40 linac RDC ”Accelerator” NSC KIPT. Measurements were performed using activation and off-line $$\gamma $$
γ
-ray spectrometric techniques. The experimental flux-averaged cross-section $$\langle {\sigma (E_\mathrm{{\gamma max}})}\rangle _\mathrm{{m}}$$
⟨
σ
(
E
γ
max
)
⟩
m
for the $${^{\textrm{nat}}\textrm{Mo}}(\gamma ,x\mathrm np)^{95\mathrm m}$$
nat
Mo
(
γ
,
x
n
p
)
95
m
Nb reaction at the bremsstrahlung end-point energy range of 38–93 MeV has been first time obtained. The estimated values $$\langle {\sigma (E_\mathrm{{\gamma max}})}\rangle _\mathrm{{g}}$$
⟨
σ
(
E
γ
max
)
⟩
g
for the formation of $$^{95}$$
95
Nb in the ground state and total cross-sections $$\langle {\sigma (E_\mathrm{{\gamma max}})}\rangle _\mathrm{{tot}}$$
⟨
σ
(
E
γ
max
)
⟩
tot
for the studied reaction were determined. The theoretical values of the yields $$Y_\textrm{m,g,tot}(E_\mathrm{{\gamma max}})$$
Y
m,g,tot
(
E
γ
max
)
and flux-averaged cross-sections $$\langle {\sigma (E_\mathrm{{\gamma max}})}\rangle _\mathrm{{m,g,tot}}$$
⟨
σ
(
E
γ
max
)
⟩
m
,
g
,
tot
for the $${^{\textrm{nat}}\textrm{Mo}}(\gamma ,x\mathrm np)^{95\mathrm m,g,tot}$$
nat
Mo
(
γ
,
x
n
p
)
95
m
,
g
,
t
o
t
Nb reactions were calculated using the cross-sections $$\sigma (E)$$
σ
(
E
)
from the TALYS1.95 code for six different level density models. The comparison showed a significant excess of the experimental results over the theoretical $$\langle {\sigma (E_\mathrm{{\gamma max}})}\rangle _\mathrm{{m,g,tot}}$$
⟨
σ
(
E
γ
max
)
⟩
m
,
g
,
tot
values.
Funder
Slovak Academy of Sciences
Publisher
Springer Science and Business Media LLC
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