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論文

Population of nuclides with Z$$ge$$98 in multi-nucleon transfer reactions of $$^{48}$$Ca+$$^{248}$$Cm

Devaraja, H. M.*; Heinz, S.*; Beliuskina, O.*; Hofmann, S.*; Hornung, C.*; M$"u$nzenberg, G.*; Ackermann, D.*; Gupta, M.*; Gambhir, Y. K.*; Henderson, R. A.*; et al.

European Physical Journal A, 55(2), p.25_1 - 25_9, 2019/02

https://doi.org/10.1140/epja/i2019-12696-3
 被引用回数：13 パーセンタイル：75.55(Physics, Nuclear)

The results for nuclei above curium, produced in multi-nucleon transfer reactions of $$^{48}$$Ca+$$^{248}$$Cm at the velocity filter SHIP of GSI Darmstadt, are presented. Spontaneous fission and $$alpha$$ activities have been used to study the population of nuclei with lifetimes ranging from few milliseconds to several days. We observed several, relatively neutron-rich isotopes with atomic numbers Z $$ge$$ 98; among them a weak 224 millisecond activity which we tentatively attributed to $$^{260}$$No. The measured cross-sections of the observed nuclei give hope that multi-nucleon transfer reactions are a way to reach new neutron-rich heavy and superheavy nuclei, which are not accessible in other reactions. We compare our results with data from earlier experiments and discuss limitations and future perspectives of the method.

論文

Review of even element super-heavy nuclei and search for element 120

Hofmann, S.*; Heinz, S.*; Mann, R.*; Maurer, J.*; M$"u$nzenberg, G.*; Antalic, S.*; Barth, W.*; Burkhard, K. G.*; Dahl, L.*; Eberhardt, K.*; et al.

European Physical Journal A, 52(6), p.180_1 - 180_34, 2016/06

https://doi.org/10.1140/epja/i2016-16180-4
 被引用回数：192 パーセンタイル：93.94(Physics, Nuclear)

The reaction $$^{54}$$Cr+$$^{248}$$Cm was investigated at the velocity filter SHIP at GSI with the intention to study production and decay properties of isotopes of element 120. Three correlated signals were measured, which occurred within a period of 279 ms. The heights of the signals correspond with the expectations for a decay sequence starting with an isotope of element 120. However, a complete decay chain cannot be established, since a signal from the implantation of the evaporation residue cannot be identified unambiguously. Measured properties of the event chain are discussed in detail. The result is compared with theoretical predictions. Previously measured decay properties of even element super-heavy nuclei were compiled in order to find arguments for an assignment from the systematics of experimental data. In the course of this review, a few tentatively assigned data could be corrected. New interpretations are given for results which could not be assigned definitely in previous studies. The discussion revealed that the cross-section for production of element 120 could be high enough so that a successful experiment seems possible with presently available techniques. However, a continuation of the experiment at SHIP for a necessary confirmation of the results obtained in a relatively short irradiation of five weeks is not possible at GSI presently. In the summary and outlook section we also present concepts for the continuation of research in the field of super-heavy nuclei.

論文

Remarks on the fission barriers of super-heavy nuclei

Hofmann, S.*; Heinz, S.*; Mann, R.*; Maurer, J.*; M$"u$nzenberg, G.*; Antalic, S.*; Barth, W.*; Dahl, L.*; Eberhardt, K.*; Grzywacz, R.*; et al.

European Physical Journal A, 52(4), p.116_1 - 116_12, 2016/04

https://doi.org/10.1140/epja/i2016-16116-0
 被引用回数：31 パーセンタイル：87.77(Physics, Nuclear)

Shell-correction energies of super-heavy nuclei are approximated by using Q$$_{alpha}$$ values of measured decay chains. Five decay chains were analyzed, which start at the isotopes $$^{285}$$Fl, $$^{294}$$118, $$^{291}$$Lv, $$^{292}$$Lv and $$^{293}$$Lv. The data are compared with predictions of macroscopic-microscopic models. Fission barriers are estimated that can be used to eliminate uncertainties in partial fission half-lives and in calculations of evaporation-residue cross-sections. In that calculations, fission probability of the compound nucleus is a major factor contributing to the total cross-section. The data also provide constraints on the cross-sections of capture and quasi-fission in the entrance channel of the fusion reaction. Arguments are presented that fusion reactions for synthesis of isotopes of elements 118 and 120 may have higher cross-sections than assumed so far.

論文

Observation of new neutron-deficient isotopes with Z$$ge$$92 in multinucleon transfer reactions

Devaraja, H. M.*; Heinz, S.*; Beliuskina, O.*; Comas, V. F.*; Hofmann, S.*; Hornung, C.*; M$"u$nzenberg, G.*; 西尾 勝久; Ackermann, D.*; Gambhir, Y. K.*; et al.

Physics Letters B, 748, p.199 - 203, 2015/09

AA2015-0304.pdf:0.78MB

https://doi.org/10.1016/j.physletb.2015.07.006
 被引用回数：69 パーセンタイル：96.85(Astronomy & Astrophysics)

In deep inelastic multinucleon transfer reactions of $$^{48}$$Ca +$$^{248}$$Cm we observed about 100 residual nuclei with proton numbers between Z =82 and Z =100. Among them, there are five new neutron-deficient isotopes: $$^{216}$$U, $$^{219}$$Np, $$^{223}$$Am, $$^{229}$$Am and $$^{233}$$Bk. As separator for the transfer products we used the velocity filter SHIP of GSI while the isotope identification was performed via the $$alpha$$-decay chains of the nuclei. These first results reveal that multinucleon transfer reactions together with here applied fast and sensitive separation and detection techniques are promising for the synthesis of new isotopes in the region of heaviest nuclei.

論文

In-beam fissio study at JAEA for heavy element synthesis

西尾 勝久; 池添 博; Hofmann, S.*; Ackermann, D.*; 有友 嘉浩*; Comas, V. F.*; D$"u$llmann, Ch. E.*; Heinz, S.*; Heredia, J. A.*; He${ss}$berger, F. P.*; et al.

AIP Conference Proceedings 1524, p.68 - 72, 2013/04

https://doi.org/10.1063/1.4801679
 被引用回数：0 パーセンタイル：0.00(Physics, Nuclear)

Fission fragment mass and kinetic energies distributions were measured in the heavy-ion induced reactions using $$^{238}$$U target nucleus at the energies around the Coulomb barrier. We observed strong variation of the fragment mass distribution with incident energy, which was explained by an energy dependence of the probabilities for fusion and quasifission. A calculation based on a fluctuation-dissipation model was carried out to determine the fusion probability in the reactions of $$^{30}$$Si+$$^{238}$$U and $$^{34}$$S+$$^{238}$$U. The fusion probabilities were consistent with those determied from the evaporation residue cross sections for both reactions, showing that in-beam fission measurement and analysis can give a reasonable estimation for the cross sections to produce super-heavy nuclei. We also discss the results for in-beam fission measurement of $$^{48}$$Ca+$$^{238}$$U.

論文

The Reaction $$^{48}$$Ca + $$^{248}$$Cm $$rightarrow$$ $$^{296}$$116$$^{*}$$ studied at the GSI-SHIP

Hofmann, S.*; Heinz, S.*; Mann, R.*; Maurer, J.*; Khuyagbaatar, J.*; Ackermann, D.*; Antalic, S.*; Barth, B.*; Block, M.*; Burkhard, H. G.*; et al.

European Physical Journal A, 48(5), p.62_1 - 62_23, 2012/05

https://doi.org/10.1140/epja/i2012-12062-1
 被引用回数：173 パーセンタイル：98.83(Physics, Nuclear)

The synthesis of element 116 in the reactions of $$^{48}$$Ca+$$^{248}$$Cm was studied at the GSI-SHIP. Four decay chains from the isotope $$^{292}$$116 and one decay $$^{293}$$116 were detected at the reaction leading to the excitation energy of 40.9 MeV. The cross sections were 3.4 and 0.9 pb, respectively. The decay character reproduced the reported data at FLNR, Russia. In the $$alpha$$ decay chain, we observed the higher $$alpha$$-particle energy in the decay of $$^{289}$$114, which suggested the population and the decay of a quasiparitcle state.

論文

Investigation of fission properties and evaporation residue measurement in the reactions using $$^{238}$$U target nucleus

西尾 勝久; 池添 博; Hofmann, S.*; Ackermann, D.*; Antalic, S.*; 有友 嘉浩; Comas, V. F.*; D$"u$llmann, Ch. E.*; Gorshkov, A.*; Graeger, R.*; et al.

EPJ Web of Conferences, 17, p.09005_1 - 09005_4, 2011/10

https://doi.org/10.1051/epjconf/20111709005
 被引用回数：1 パーセンタイル：47.05(Physics, Nuclear)

Fission fragment mass distributions after full momentum transfer of the projectile were measured in the reactions using a $$^{238}$$U target nucleus bombarded by $$^{30}$$Si, $$^{31}$$P, $$^{34,36}$$S, $$^{40}$$Ar, $$^{40,48}$$Ca projectiles. We observed a strong variation of the distribution as function of bombarding energy. The results were interpreted by the effects of nuclear deformation of the target nucleus on the competition between fusion and quasifission. The symmetric fission includes fusion-fission, wheres as the asymmetric fission represents quasifission. The fusion probabilities were determined with the help of fluctuation-dissipation model. The estimated evaporation residue cross sections ($$^{263,264}$$Sg and $$^{267,268}$$Hs) produced in $$^{30}$$Si + $$^{238}$$U and $$^{34}$$S+$$^{238}$$U reproduced the experimental data.

論文

Nuclear orientation in the reaction $$^{34}$$S+$$^{238}$$U and synthesis of the new isotope $$^{268}$$Hs

西尾 勝久; Hofmann, S.*; He${ss}$berger, F. P.*; Ackermann, D.*; Antalic, S.*; 有友 嘉浩; Comas, V. F.*; D$"u$llmann, Ch. E.*; Gorshkov, A.*; Graeger, R.*; et al.

Physical Review C, 82(2), p.024611_1 - 024611_9, 2010/08

https://doi.org/10.1103/PhysRevC.82.024611
 被引用回数：82 パーセンタイル：95.87(Physics, Nuclear)

Synthesis of isotopes of the element hassium was studied using the reaction $$^{34}$$S+$$^{238}$$U$$rightarrow$$$$^{272}$$Hs*. At a kinetic energy of 163.0 MeV in the center of mass system we observed one $$alpha$$-decay chain starting at the isotope $$^{267}$$Hs. The cross-section was 1.8$$^{+4.2}_{-1.5}$$pb. At 152.0 MeV one decay of the new isotope $$^{268}$$Hs was observed. It decays with a half-life of 0.38$$^{+1.8}_{-0.17}$$s by 9479$$pm$$16 keV $$alpha$$-particle emission. Spontaneous fission of the daughter nucleus $$^{264}$$Sg was confirmed. The measured cross-section was 0.54$$^{+1.3}_{-0.45}$$pb. In-beam measurements of fission fragment mass distributions were performed to obtain information on the fusion probability at various orientation of the deformed target nucleus. The distributions changed from symmetry to asymmetry when the beam energy was changed from above-barrier to sub-barrier values, indicating orientation effects on fusion and/or quasifission. It was found that the distribution of symmetric mass fragments originates not only from fusion-fission, but has a strong component from quasifission. This result significantly influences the interpretation of data obtained from measurements of symmetric mass distributions with respect to extracting evaporation residue cross-sections.

論文

Decay studies of K isomer in $$^{254}$$No

He${ss}$berger, F. P.*; Antalic, S.*; Sulignano, B.*; Ackermann, D.*; Heinz, S.*; Hofmann, S.*; Kindler, B.*; Khuyagbaatar, J.*; Kojouharov, I.*; Kuusiniemi, P.*; et al.

European Physical Journal A, 43(1), p.55 - 66, 2010/01

https://doi.org/10.1140/epja/i2009-10899-9
 被引用回数：74 パーセンタイル：95.32(Physics, Nuclear)

$$gamma$$-rays decay study of two K isomers in $$^{254}$$No was performed. Two new transitions of 778 and 856 keV could be attributed to the decay pattern of $$^{254m1}$$No (T$$_{1/2}$$=275 ms). The population of an excited band built up on this isomer ($$K$$$$^{pi}$$=8$$^{-}$$) by the decay of $$^{252m2}$$No (198 $$mu$$s) could be proven. A spontaneous fission branch of 2.0$$times$$10$$^{-4}$$ was measured for $$^{252m1}$$No, and upper limit of 1.2$$times$$10$$^{-4}$$ was estimated for $$^{252m2}$$No. These values demonstrate the high stability of multi-quasiparticle configuration against spontaneous fission.

論文

Orientation effects of deformed $$^{238}$$U target nuclei on the fusion probability for the heavy element synthesis

西尾 勝久; Hofmann, S.*; 池添 博; He${ss}$berger, F. P.*; Ackermann, D.*; Antalic, S.*; Comas, V. F.*; Gan, Z.*; Heinz, S.*; Heredia, J. A.*; et al.

Nuclear Physics A, 805(1-4), p.516 - 518, 2008/06

The effects of the orientation of the deformed $$^{238}$$U target nuclei were investigated in the reaction of $$^{30}$$Si+$$^{238}$$U. The cross-sections of the system to overcome the Coulomb barrier were determined by measuring the fission cross-sections at JAEA-tandem accelerator, from which the Coulomb barrier height for the collision of $$^{30}$$Si to the polar side and the equatorial side of $$^{238}$$U were determined. The evaporation residue (ER) cross-sections were determined at the velocity filter SHIP of GSI. Significant enhancement of the cross-sections of $$^{264}$$Sg(4n) in the sub-barrier energy indicates the lowering of the Coulomb barrier at the Polar collisions. However, competition between fusion and quasifission was implied. The cross-sections for $$^{263}$$Sg(5n) measured at the above barrier energy indicated that there is no significant fusion hindrance at the equatorial collisions. In this contribution, the systematic behavior of the orientation effects of $$^{238}$$U is discussed by using additionally the data of $$^{16}$$O+$$^{238}$$U and $$^{48}$$Ca+$$^{238}$$U.

論文

Measurement of evaporation residue and fission cross sections of the reaction $$^{30}$$Si + $$^{238}$$U at subbarrier energies

西尾 勝久; Hofmann, S.*; 池添 博; He${ss}$berger, F. P.*; Ackermann, D.*; Antalic, S.*; Comas, V. F.*; Gan, Z.*; Heinz, S.*; Heredia, J. A.*; et al.

Journal of Nuclear and Radiochemical Sciences, 8(2), p.73 - 78, 2007/10

https://doi.org/10.14494/jnrs2000.8.73

Effects of the prolate deformation of $$^{238}$$U on fusion were studied in the reaction $$^{30}$$Si + $$^{238}$$U at bombarding energies close to the Coulomb barrier. The fission cross section was measured at JAEA tandem accelerator to see the enhancement of the cross section in the subbarrier energy due to the lowering of the Coulomb barrier at the collision of the projectile to polar side of $$^{238}$$U. Evaporation residue cross sections were measured at UNILAC of GSI by using the velocity filter SHIP to determine the fusion probability. In the subbarrier region, we could produce isotope $$^{264}$$Sg by 4n channel, but fusion hindrance was implied in the analysis. At above barrier energies, we produced $$^{263}$$Sg by 5n channel. The analysis suggests that there is no fusion hindrance at the equatorial collisions.

論文

Identification of a K isomer in $$^{252}$$No

Sulignano, B.*; Heinz, S.*; He${ss}$berger, F. P.*; Hofmann, S.*; Ackermann, D.*; Antalic, S.*; Kindler, B.*; Kojouharov, I.*; Kuusiniemi, P.*; Lommel, B.*; et al.

European Physical Journal A, 33(4), p.327 - 331, 2007/09

https://doi.org/10.1140/epja/i2007-10469-3
 被引用回数：81 パーセンタイル：96.16(Physics, Nuclear)

The $$K$$-isomer with a half-life of 100 ms has been discovered in the nucleus $$^{252}$$No. The nucleus was produced in the fusion-evaporation reacion $$^{206}$$Pb($$^{48}$$Ca,2n)$$^{252}$$No. The experiment was carried out at the velocity filter SHIP of GSI. The isomeric state is located at an excitation energy of 1254 keV and is interpreted as a two quasi-neutron state with $$K$$=8$$^{-}$$. The isomeric state has direct connection to the rotational states of 8$$^{+}$$ in $$^{252}$$No. Also the rotational states of 6$$^{+}$$ and 4$$^{+}$$ was feeded via the octupole band with $$K$$=2$$^{-}$$. The isomeric state and the ground state was populated with the equal intensity in the fusion-evaporation reaction.

論文

The Reaction $$^{48}$$Ca+$$^{238}$$U $$rightarrow$$ $$^{286}$$112$$^{*}$$ studied at the GSI-SHIP

Hofmann, S.*; Ackermann, D.*; Antalic, S.*; Burkhard, H. G.*; Comas, V. F.*; Dressler, R.*; Gan, Z.*; Heinz, S.*; Heredia, J. A.*; He${ss}$berger, F. P.*; et al.

European Physical Journal A, 32(3), p.251 - 260, 2007/06

https://doi.org/10.1140/epja/i2007-10373-x
 被引用回数：268 パーセンタイル：99.69(Physics, Nuclear)

The fusion reaction of $$^{48}$$Ca projectiles with$$^{238}$$U target nuclei was studied at the velocity filter SHIP of GSI. Two decay chains were measured, which fully confirm data that were previously assigned to the isotope $$^{283}$$112 in experiments at the Flerov Laboratory in Dubna. Two other events are consistent with a 50% spontaneous fission (SF) branch of this isotope. The mean value obtained for the half-life of $$^{283}$$112 is (6.9$$^{+6.9}_{-2.3}$$) s, the $$alpha$$ energy is (9.520$$pm$$0.015) MeV, and the total kinetic energy (TKE) of SF is (238$$pm$$14) MeV. The half-life of the $$alpha$$ decay daughter nucleus $$^{279}$$Ds is (0.18$$^{+0.32}_{-0.07}$$) s, and the TKE of SF is (210$$^{+32}_{-11}$$) MeV. The cross-section deduced from all four events is (0.72$$^{+0.58}_{-0.35}$$) pb, measured at an excitation energy of 34.6 MeV of the compound nucleus $$^{286}$$112.

論文

Measurement of evaporation residue cross-sections of the reaction $$^{30}$$Si + $$^{238}$$U at subbarrier energies

西尾 勝久; Hofmann, S.*; He${ss}$berger, F. P.*; Ackermann, D.*; Antalic, S.*; Comas, V. F.*; Gan, Z.*; Heinz, S.*; Heredia, J. A.*; 池添 博; et al.

AIP Conference Proceedings 891, p.71 - 79, 2007/03

https://doi.org/10.1063/1.2713502

重イオン融合反応$$^{30}$$Si+$$^{238}$$UによりSg同位体を合成し、この生成断面積を調べた。実験は、ドイツ重イオン研究所(GSI)で行った。反応エネルギーE$$_{c.m.}$$=144MeVにおいて、$$^{263}$$Sgから始まる3つの$$alpha$$崩壊連鎖を観測し、断面積67pbを得た。サブバリヤエネルギーE$$_{c.m.}$$=133MeVで、新同位体$$^{264}$$Sgを3つ合成し、断面積10pbを得た。これは自発核分裂で崩壊し、半減期は120msであった。これら断面積を統計モデル計算と比較した。融合過程においては、$$^{238}$$Uの変形を取り入れたチャンネル結合法で捕獲断面積を決定した。この値は、原子力機構のタンデム加速器を用いて行った$$^{30}$$Si+$$^{238}$$Uの核分裂断面積とよく一致した。E$$_{c.m.}$$=133MeVでの断面積の値は、一次元モデルに比べて10$$^{4}$$倍大きな値であり、ウランの変形によって断面積が増加することがわかった。しかし、計算との不一致から、準核分裂が何割か存在することが示唆された。クーロン障壁より高いエネルギーE$$_{c.m.}$$=144MeVでは$$^{30}$$Siは$$^{238}$$Uの赤道面と接触できる。$$^{263}$$Sgの生成断面積67pbは、統計モデル計算値によく一致し、融合に阻害がなかった。これは、赤道面衝突が融合に有利であることを示唆している。

論文

Alpha-$$gamma$$ decay studies of $$^{255}$$Rf, $$^{251}$$No and $$^{247}$$Fm

He${ss}$berger, F. P.*; Hofmann, S.*; Ackermann, D.*; Antalic, S.*; Kindler, B.*; Kojouharov, I.*; Kuusiniemi, P.*; Leino, M.*; Lommel, B.*; Mann, R.*; et al.

European Physical Journal A, 30(3), p.561 - 569, 2006/12

https://doi.org/10.1140/epja/i2006-10137-2
 被引用回数：53 パーセンタイル：91.59(Physics, Nuclear)

$$^{255}$$Rf, $$^{251}$$No及び$$^{247}$$Fmについて、$$alpha$$線と$$gamma$$線の検出による崩壊核分光実験を行った。実験は、ドイツ重イオン研究所の線形加速器施設UNILACにおける反跳生成核分離装置SHIPを用いて行った。SHIPで分離された蒸発残留核を焦点に設置したシリコン検出器に打ち込んだ。この検出器で$$alpha$$崩壊を検出し、また近くに設けたGe検出器で$$gamma$$線を検出した。これら同位体は、$$^{207}$$Pb($$^{50}$$Ti,2n)$$^{255}$$Rf及びこの$$^{255}$$Rfの$$alpha$$崩壊核種として生成し、さらに$$^{206}$$Pb($$^{48}$$Ca,3n)$$^{251}$$No反応及びこの$$^{251}$$Noの$$alpha$$崩壊核種として生成した。解析から次のことがわかった。(1)$$^{251}$$Noには半減期1.0秒のアイソマがあることがわかっていたが、このエネルギー準位が106keVであることがわかった。(2)また、$$^{251}$$Noには2$$mu$$sの半減期を持つ第2のアイソマがあり、$$^{206}$$Pb($$^{48}$$Ca,3n)$$^{251}$$No反応で直接生成されることがわかった。このアイソマは、2本の$$gamma$$線とコインシデンスし、解析から励起エネルギーが1700keV以上の準位にあることが示唆された。この2本の$$gamma$$線は、$$^{255}$$Rfの$$alpha$$崩壊につづく$$gamma$$遷移と一致した。

論文

Doubly magic nucleus $$^{270}_{108}$$Hs$$_{162}$$

Dvorak, J.*; Br$"u$chle, W.*; Chelnokov, M.*; Dressler, R.*; D$"u$llmann, Ch. E.*; Eberhardt, K.*; Gorshkov, V.*; J$"a$ger, E.*; Kr$"u$cken, R.*; Kuznetsov, A.*; et al.

Physical Review Letters, 97(24), p.242501_1 - 242501_4, 2006/12

https://doi.org/10.1103/PhysRevLett.97.242501
 被引用回数：157 パーセンタイル：96.00(Physics, Multidisciplinary)

超重核領域で理論的に予想されていた変形した二重魔法核$$^{270}_{108}$$Hs$$_{162}$$を初めて実験的に確認した。実験はドイツ重イオン研究所(GSI)で行った。$$^{248}$$Cm+$$^{26}$$Mg反応で合成されたHs同位体を、迅速気相化学分離法で選択に分離し、$$alpha$$壊変エネルギーとそれに伴う15事象の壊変連鎖から$$^{270}_{108}$$Hsを同定した。また$$alpha$$壊変エネルギーから$$Q_{alpha}$$値を$$9.02 pm 0.03$$と決定した。$$^{270}_{108}$$Hsの生成断面積は約3pbであった。

論文

Measurement of evaporation residue cross-sections of the reaction $$^{30}$$Si+$$^{238}$$U at subbarrier energies

西尾 勝久; Hofmann, S.*; He${ss}$berger, F. P.*; Ackermann, D.*; Antalic, S.*; Comas, V. F.*; Gan, Z.*; Heinz, S.*; Heredia, J. A.*; 池添 博; et al.

European Physical Journal A, 29(3), p.281 - 287, 2006/09

https://doi.org/10.1140/epja/i2006-10091-y
 被引用回数：66 パーセンタイル：93.85(Physics, Nuclear)

重イオン融合反応$$^{30}$$Si+$$^{238}$$UによりSg同位体を合成し、この生成断面積を調べた。実験は、ドイツ重イオン研究所(GSI)で行った。反応エネルギーE$$_{c.m.}$$=144MeVにおいて、$$^{263}$$Sgから始まる3つの$$alpha$$崩壊連鎖を観測した。断面積は、67pbであった。サブバリヤエネルギーE$$_{c.m.}$$=133MeVで、新同位体$$^{264}$$Sgを3つ合成し断面積10pbを得た。これは自発核分裂で崩壊し、半減期は120msであった。これら断面積を統計モデル計算と比較した。融合過程においては、$$^{238}$$Uの変形を取り入れたチャンネル結合法で捕獲断面積を決定した。この値は、原子力機構のタンデム加速器を用いて行った$$^{30}$$Si+$$^{238}$$Uの核分裂断面積とよく一致した。E$$_{c.m.}$$=133MeVでの断面積の値は、一次元モデルに比べて10$$^{4}$$倍大きな値であり、ウランの変形によるサブバリヤでの断面積の増加で説明できた。しかし、計算との不一致から、準核分裂が何割か存在することが示唆された。クーロン障壁より高いエネルギーE$$_{c.m.}$$=144MeVでは$$^{30}$$Siは$$^{238}$$Uの赤道面と接触できる。$$^{263}$$Sgの生成断面積65pbは、統計モデル計算値によく一致し、融合に阻害がなかった。これは、赤道面衝突が融合に有利であることを示唆している。

論文

Alpha-$$gamma$$ decay studies of $$^{255}$$No

He${ss}$berger, F. P.*; Hofmann, S.*; Ackermann, D.*; Antalic, S.*; Kindler, B.*; Kojouharov, I.*; Kuusiniemi, P.*; Leino, M.*; Lommel, B.*; Mann, R.*; et al.

European Physical Journal A, 29(2), p.165 - 173, 2006/08

https://doi.org/10.1140/epja/i2006-10083-y
 被引用回数：43 パーセンタイル：88.46(Physics, Nuclear)

The decay of $$^{255}$$No was investigated by means of $$alpha$$-$$gamma$$ spectroscopy. The experiment was carried out by using the velocity filter SHIP at GSI. The isotope was produced in the reactions $$^{208}$$Pb($$^{48}$$Ca,n)$$^{255}$$No, $$^{209}$$Bi($$^{48}$$Ca,2n)$$^{255}$$Lr (EC)-$$>$$ $$^{255}$$No, and $$^{238}$$U($$^{22}$$Ne,5n)$$^{255}$$No. Decay data for $$alpha$$-$$gamma$$ coincidence measurements were obtained, and the level structures of the daughter nucleus $$^{251}$$Fm were obtained, including the tentative assignment of (1) 9/2$$^{-}$$ for ground state and (2) 5/2$$^{+}$$ for the 200 keV isomeric state with $$T_{1/2}$$=21 $$mu$$s.

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$$^{34}$$S+$$^{238}$$Uのサブバリヤエネルギー融合反応による新同位体$$^{268}$$Hsの合成

西尾 勝久; Hofmann, S.*; He${ss}$berger, F. P.*; Ackermann, D.*; Antalic, S.*; Comas, V. F.*; D$"u$llmann, Ch. E.*; Gorshkov, A.*; Graeger, R.*; Heinz, S.*; et al.

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$$^{34}$$S+$$^{238}$$Uのサブバリヤエネルギー融合反応により、超重元素(Z=108)の新同位体$$^{268}$$Hsを合成した。実験に先立ち、原子力機構タンデム加速器においてこの反応の核分裂断面積の励起関数を測定するとともに、核分裂片の質量数分布を測定した。モデル計算により、サブバリヤ領域でも融合反応確率が存在することを予測した。$$^{268}$$Hsの合成実験は、ドイツGSIの線形加速器UNILACに設置された反跳生成核分離装置SHIPを用いて行った。合成に成功し、断面積として0.54pbを得た。$$^{268}$$Hsは$$alpha$$崩壊核種で、半減期0.38 sであることがわかった。

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融合反応$$^{30}$$Si+$$^{238}$$UによるSgの合成

西尾 勝久; 光岡 真一; 池添 博; Hofmann, S.*; He${ss}$berger, F. P.*; Ackermann, D.*; Antalic, S.*; Comas, V. F.*; Gan, Z.*; Heinz, S.*; et al.

no journal, , 

重イオン融合反応$$^{30}$$Si+$$^{238}$$UによりSg同位体を合成し、この生成断面積を調べた。実験は、ドイツ重イオン研究所(GSI)で行った。反応エネルギーE$$_{c.m.}$$=144MeVにおいて、$$^{263}$$Sgから始まる3つの$$alpha$$崩壊連鎖を観測した。断面積は、67pbであった。サブバリヤエネルギーE$$_{c.m.}$$=133MeVで新同位体$$^{264}$$Sgを3つ合成し、断面積10pbを得た。これは自発核分裂で崩壊し、半減期は120msであった。これら断面積を統計モデル計算と比較した。融合過程においては、$$^{238}$$Uの変形を取り入れたチャンネル結合法で捕獲断面積を決定した。この値は、原子力機構のタンデム加速器を用いて行った$$^{30}$$Si+$$^{238}$$Uの核分裂断面積とよく一致した。E$$_{c.m.}$$=133MeVでの断面積の値は、一次元モデルに比べて10$$^{4}$$倍大きな値であり、ウランの変形によってサブバリヤで断面積が増加していることを明らかにした。しかし、計算との不一致から、準核分裂が何割か存在することが示唆された。クーロン障壁より高いエネルギーE$$_{c.m.}$$=144MeVでは$$^{30}$$Siは$$^{238}$$Uの赤道面と接触できる。$$^{263}$$Sgの生成断面積67pbは、統計モデル計算値によく一致し、融合に阻害がなかった。これは、赤道面衝突が融合に有利であることを示唆している。

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