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NSR database version of May 10, 2024.

Search: Author = C.Nithya

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2024NI02      Phys.Rev. C 109, 014612 (2024)

C.Nithya, K.P.Santhosh

Examination of the decay modes of ^293-295Og

doi: 10.1103/PhysRevC.109.014612
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2023NI09      Phys.Rev. C 108, 014606 (2023)

C.Nithya, K.P.Santhosh

Theoretical studies of the decay chain of the isotopes ^{298, 299}120

RADIOACTIVITY ^298,299120, ^294,295Og, ^290,291Lv, ^286,287Fl, ^282,283Cn, ^278,279Ds, ^274,275Hs, ^270,271Sg(α); calculated Q, T_1/2. ^298,299120(SF); calculated T_1/2. Coulomb and proximity potential model for deformed nuclei (CPPMDN) used for α-decay and shell-effect-dependent formula for spontaneous fission. Showed that the isotopes ²⁹⁸120 and ²⁹⁹120 decay via the 4α chain followed by spontaneous fission. Comparison to available experimental data.

doi: 10.1103/PhysRevC.108.014606
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2022NI01      Nucl.Phys. A1020, 122400 (2022)

C.Nithya, K.P.Santhosh

Studies on the decay modes of superheavy nuclei with Z = 120

RADIOACTIVITY ^{294,295,297,298,301,302,303,304,308}120(α), (SF); calculated T_1/2 using the modified generalized liquid drop model (MGLDM). Comparison with available data.

doi: 10.1016/j.nuclphysa.2022.122400
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2021SA34      Phys.Rev. C 104, 024617 (2021)

K.P.Santhosh, C.Nithya, T.A.Jose

Decay modes of superheavy nuclei using a modified generalized liquid drop model and a mass-inertia-dependent approach for spontaneous fission

RADIOACTIVITY ^{253,254,255,256,257,258,259,260,261,262,263,264,265,266,267,268}Rf, ^{258,259,260,261,262,263,264,265,266,267,268,269,270,271,272}Sg, ^{263,264,265,266,267,268,269,270,271,272,273,274,275,276,277}Hs, ^{267,268,269,270,271,272,273,274,275,276,277,278,279,280,281}Ds, ^{276,277,278,279,280,281,282,283,284,285}Cn, ^{284,285,286,287,288,289}Fl, ^{289,290,291,292,293}Lv, ^293,294,295Og(α), (SF); ^{255,256,257,258,259,260,261,262,263,264,265,266,267,268,269,270}Db, ^{260,261,262,263,264,265,266,267,268,269,270,271,272,273,274}Bh, ^{265,266,267,268,269,270,271,272,273,274,275,276,277,278,279}Mt, ^{272,273,274,275,276,277,278,279,280,281,282,283}Rg, ^{278,279,280,281,282,283,284,285,286,287}Nh, ^{287,288,289,290,291}Mc, ^{291,292,293,294}Ts(α), (SF); calculated α decay and SF decay T_1/2 of superheavy nuclei using modified generalized liquid drop model (MGLDM) with the proximity 77 parametrization for α decay, and a mass-inertia-dependent approach for spontaneous fission. Comparison with available experimental T_1/2.

doi: 10.1103/PhysRevC.104.024617
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2018SA08      Pramana 90, 35 (2018)

K.P.Santhosh, C.Nithya

Theoretical studies on the α-decay half-lives of hyper and normal isotopes of Po

RADIOACTIVITY ^{187,188,189,190,191,192,193,194,195,196,197,198,199,200,201,202,203,204,205,206,207,208,209,210,211,212,213,214,215,216,217,218,219,220,221,222,223,224}Po(α); calculated hypernuclei Q-value, T_1/2. Comparison with available data.

doi: 10.1007/s12043-018-1528-y
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2018SA12      At.Data Nucl.Data Tables 121-122, 216 (2018)

K.P.Santhosh, C.Nithya

Predictions on the modes of decay of odd Z superheavy isotopes within the range 105 ≤ Z ≤ 135

NUCLEAR STRUCTURE Z=105-135; calculated decay modes of 1051 odd Z superheavy nuclei, α-decay T_1/2 using the Coulomb and proximity potential model for deformed nuclei (CPPMDN). Comparison with available data.

doi: 10.1016/j.adt.2017.12.001
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2018SA15      Phys.Rev. C 97, 044615 (2018)

K.P.Santhosh, C.Nithya

α-decay chains of superheavy nuclei with Z=125

RADIOACTIVITY ^{310,311,312,313,314,315,316,317,318,319,320,323}125, ^{306,307,308,309,310,311,312,313,314,315,316,319}123, ^{302,303,304,305,306,307,308,309,310,311,312,315}121, ^{298,299,300,301,302,303,304,305,306,307,308,311}119, ^{294,295,296,297,298,299,300,301,302,303,304,307}Ts, ^{290,291,292,293,294,295,296,297,298,299,300,303}Mc, ^{286,287,288,289,290,291,292,293,294,295,296,299}Nh, ^{282,283,284,285,286,287,288,289,290,291,292,295}Rg, ^{278,279,280,281,282,283,284,285,286,287,288,291}Mt, ^{274,275,276,277,278,279,280,281,282,283,284,287}Bh(α), (SF); calculated Q(α) value using four different mass models, T_1/2(α) using Coulomb and proximity potential model for deformed nuclei (CPPMDN) with six different theoretical formalisms, and T_1/2(SF) using shell-effect-dependent formula. From a comparison of α-decay half-lives with spontaneous fission half-lives deduced that ^310,311125 decay by six α chains, ^{312,313,314,315,316,317,318}125 decay by five α chains, ^319,320125 by two α chains, and ³²³125 by one α chain, and that ^{321,322,324,325,326,327,328,329,330,331,332,333,334,335,336,337,338,339}125 decay by SF mode. ^{303,304,305,306,307,308,309}125; calculated S(p) and S(2p), possible decay by proton emission.

doi: 10.1103/PhysRevC.97.044615
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2018SA25      Phys.Rev. C 97, 064616 (2018)

K.P.Santhosh, C.Nithya

Systematic studies of α and heavy-cluster emissions from superheavy nuclei

RADIOACTIVITY ²⁹⁴Og, ^293,294Ts, ^{290,291,292,293}Lv, ^{287,288,289,290}Mc, ^{285,287,288,289}Fl, ^{282,283,284,285,286}Nh, ^{281,282,283,285}Cn, ^278,279,280Rg, ²⁷⁷Ds, ^{274,275,276,278}Mt, ^273,275Hs, ^{270,271,272,274}Bh(α); ²⁵²Fm(⁴⁸Ca); ²⁷⁸Hs(⁷²Ni); ²⁸²Ds(⁷⁴Ni); ²⁸²Cn(⁷⁴Zn); ²⁸⁴Cn(⁷⁶Zn); ²⁸⁴Fl(⁷⁸Ge); ^286,288Fl(⁸⁰Ge); ^290,294Fl(⁸²Ge); ²⁹²Lv(⁸⁴Se); ²⁹⁴Og(⁸⁶Kr); ³⁰⁰120(⁹²Sr), (⁹⁴Sr); ²⁶⁵Rf(⁵⁵Ti); ²⁶⁷Rf(⁶¹Cr); ²⁶⁹Sg(⁶⁴Fe); ²⁷¹Sg(⁶⁵Fe); ²⁷³Hs(⁶⁸Ni); ²⁷⁵Hs(⁷⁰Ni); ²⁷⁷Hs, ²⁷⁹Ds(⁷¹Ni); ²⁸¹Ds(⁷²Ni); ²⁸¹Cn(⁷⁴Zn); ²⁸³Cn(⁷⁶Zn); ²⁸⁵Cn(⁷⁷Zn); ²⁸⁷Fl(⁸⁰Ge); ²⁸⁹Fl(⁸¹Ge); ²⁹¹Lv(⁸⁴Se); ²⁹³Lv(⁸⁵Se); ²⁹⁵Og(⁸⁷Kr); ²⁹⁹120(⁹¹Sr); ³⁰¹120(⁹³Sr); ²⁵³Es(⁴⁶Ar); ²⁸⁷Nh(⁷⁹Ga); ²⁹⁷119(⁸⁹Rb); ²⁹⁹119(⁹¹Rb); ²⁷⁸Bh(⁷³Ni); ²⁸²Mt(⁷¹Co); ²⁸⁶Rg(⁷⁸Cu); ²⁹⁰Nh(⁸¹Ga); ³⁰⁰119(⁹²Rb); ²⁵⁸Fm(α), (⁵⁰Ar); ²⁶⁰Fm(α), (⁵²Ar); ²⁶²Rf(α), (⁵⁴Ti); ²⁶⁶Sg(α), (⁵⁸Cr); ²⁶⁸Sg(α), (⁶⁰Cr); ²⁷⁰Hs(α), (⁶²Fe); ²⁷²Hs(α), (⁶⁴Fe); ²⁷⁴Hs(α), (⁶⁶Fe); ²⁷⁴Ds(α), (⁶⁶Ni); ²⁷⁶Ds(α), (⁶⁸Ni); ²⁷⁸Ds(α), (⁷⁰Ni); ²⁸⁰Ds(α), (⁷²Ni); ²⁸²Ds(α), (⁷⁴Ni); ²⁸⁴Ds(α), (⁷⁶Ni); ²⁸⁶Ds(α), (⁷⁸Ni); ²⁸²Cn(α), (⁷⁴Zn); ²⁸⁴Cn(α), (⁷⁶Zn); ²⁸⁶Cn(α), (⁷⁸Zn); ²⁸⁸Cn(α), (⁸⁰Zn); ²⁹⁰Cn(α), (⁸²Zn); ²⁸⁶Fl(α), (⁷⁸Ge); ²⁸⁸Fl(α), (⁸⁰Ge); ²⁹⁰Fl(α), (⁸²Ge); ²⁹²Fl(α), (⁸⁴Ge); ²⁹⁴Fl(α), (⁸⁶Ge); ²⁹⁶Fl(α), (⁸⁸Ge); ²⁹⁰Lv(α), (⁸²Se); ²⁹²Lv(α), (⁸⁴Se); ²⁹⁴Lv(α), (⁸⁶Se); ²⁹⁶Lv(α), (⁸⁸Se); ²⁹⁸Lv(α), (⁹⁰Se); ²⁹⁴Og(α), (⁸⁶Kr); ²⁹⁶Og(α), (⁸⁸Kr); ²⁹⁸Og(α), (⁹⁰Kr); ³⁰⁰Og(α), (⁹²Kr); ³⁰²Og(α), (⁹⁴Kr); ³⁰⁴Og(α), (⁹⁶Kr); ³⁰⁶Og(α), (⁹⁸Kr); ³⁰⁸Og(α), (¹⁰⁰Kr); ²⁹⁶120(α), (⁸⁸Sr); ²⁹⁸120(α), (⁹⁰Sr); ³⁰⁰120(α), (⁹²Sr); ³⁰²120(α), (⁹⁴Sr); ³⁰⁴120(α), (⁹⁶Sr); ³⁰⁶120(α), (⁹⁸Sr); ³⁰⁸120(α), (¹⁰⁰Sr); ³¹⁰120(α), (¹⁰²Sr); ³¹²120(α), (¹⁰⁴Sr); ²⁶¹Rf(α), (⁵³Ti); ²⁶⁷Sg(α), (⁵⁹Cr); ²⁷⁹Ds(α), (⁷¹Ni); ²⁸¹Ds(α), (⁷³Ni); ²⁸³Ds(α), (⁷⁵Ni); ²⁸⁵Ds(α), (⁷⁷Ni); ²⁸⁵Cn(α), (⁷⁷Zn); ²⁸⁷Cn(α), (⁷⁹Zn); ²⁸⁹Cn(α), (⁸¹Zn); ²⁹¹Fl(α), (⁸³Ge); ²⁹⁵Fl(α), (⁸⁷Ge); ²⁹³Lv(α), (⁸⁵Se); ²⁹⁵Lv(α), (⁸⁷Se); ²⁹⁷Lv(α), (⁸⁹Se); ²⁹⁵Og(α), (⁸⁷Kr); ²⁹⁷Og(α), (⁸⁹Kr); ²⁹⁹Og(α), (⁹¹Kr); ²⁹⁷120(α), (⁸⁹Sr); ³⁰¹120(α), (⁹³Sr); ³⁰³120(α), (⁹⁵Sr); ³¹³120(α), (¹⁰⁵Sr); ²⁸²Rg(α), (⁷⁴Cu); ²⁸⁴Rg(α), (⁷⁶Cu); ²⁸⁶Rg(α), (⁷⁸Cu); ²⁸⁸Rg(α), (⁸⁰Cu); ²⁸⁶Nh(α), (⁷⁸Ga); ²⁸⁸Nh(α), (⁸⁰Ga); ²⁹⁰Nh(α), (⁸²Ga); ²⁸⁸Mc(α), (⁸⁰As); ²⁹²Mc(α), (⁸⁴As); ²⁹⁴Mc(α), (⁸⁶As); ²⁹⁶Mc(α), (⁸⁸As); ²⁹⁴Ts(α), (⁸⁶Br); ²⁹⁶Ts(α), (⁸⁸Br); ²⁹⁸Ts(α), (⁹⁰Br); ³⁰⁰Ts(α), (⁹²Br); ²⁹⁸119(α), (⁹⁰Rb); ³⁰⁰119(α), (⁹²Rb); ³⁰²119(α), (⁹⁴Rb); ³⁰⁴119(α), (⁹⁶Rb); ³⁰⁶119(α), (⁹⁸Rb); ³⁰⁸119(α), (¹⁰⁰Rb); ³¹⁰119(α), (¹⁰²Rb); ²⁷¹Mt(α), (⁶³Co); ²⁷³Mt(α), (⁶⁵Co); ²⁷⁹Mt(α), (⁷¹Co); ²⁸¹Mt(α), (⁷³Co); ²⁸³Mt(α), (⁷⁵Co); ²⁸¹Rg(α), (⁷³Cu); ²⁸³Rg(α), (⁷⁵Cu); ²⁸⁵Rg(α), (⁷⁷Cu); ²⁸⁷Rg(α), (⁷⁹Cu); ²⁸³Nh(α), (⁷⁵Ga); ²⁸⁵Nh(α), (⁷⁷Ga); ²⁸⁷Nh(α), (⁷⁹Ga); ²⁸⁹Nh(α), (⁸¹Ga); ²⁹¹Nh(α), (⁸³Ga); ²⁸⁷Mc(α), (⁷⁹As); ²⁸⁹Mc(α), (⁸¹As); ²⁹¹Mc(α), (⁸³As); ²⁹³Mc(α), (⁸⁵As); ²⁹⁵Mc(α), (⁸⁷As); ²⁹⁷Mc(α), (⁸⁹As); ²⁹³Ts(α), (⁸⁵Br); ²⁹⁵Ts(α), (⁸⁷Br); ²⁹⁷Ts(α), (⁸⁹Br); ²⁹⁹Ts(α), (⁹¹Br); ³⁰¹Ts(α), (⁹³Br); ²⁹⁷119(α), (⁸⁹Rb); ²⁹⁹119(α), (⁹¹Rb); ³⁰¹119(α), (⁹³Rb); ³⁰³119(α), (⁹⁵Rb); ³⁰⁵119(α), (⁹⁷Rb); ³⁰⁷119(α), (⁹⁹Rb); ³⁰⁹119(α), (¹⁰¹Rb); calculated Q values, T_1/2, and branching ratio relative to α-decay for cluster decays. Comparison with available experimental values, and with predictions of analytical super-asymmetric fission (ASAF) model calculations, when possible. Relevance to decays of superheavy nuclei (SHN).

doi: 10.1103/PhysRevC.97.064616
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2018SA41      Phys.Rev. C 98, 024625 (2018)

K.P.Santhosh, C.Nithya, H.Hassanabadi, D.T.Akrawy

α-decay half-lives of superheavy nuclei from a modified generalized liquid-drop model

RADIOACTIVITY ^{257,268,269,271}Sg, ^{262,263,270,271,272,274}Bh, ^{261,262,273,275}Hs, ^{266,267,275,276,278}Mt, ^{265,266,277,279,281}Ds, ^{272,274,278,279,280,281,282}Rg, ^{271,279,281,283,285}Cn, ^{279,281,282,283,284,285,286}Nh, ^{283,284,285,286,287,288,289}Fl, ^{286,292,287,288,289,290}Mc, ^{287,288,290,291,292,293}Lv, ^{290,292,293,294}Ts, ^291,292,294Og(α); ^296,297119, ^295,300120, ^304,306121, ^301,306122, ^310,312123, ^307,312124, ^316,318125, ^313,320126, ^320,322127, ^319,320128, ^326,327129, ^324,325130, ^334,336131, ^331,332132, ^329,330133, ^333,334134(α); calculated half-lives using the generalized liquid-drop model (GLDM) with 1977 nuclear proximity potential proposed by Blocki et al. Comparison with available experimental values, and with half-lives using GLDM model of Royer et al.

doi: 10.1103/PhysRevC.98.024625
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2017SA29      Phys.Rev. C 95, 054621 (2017)

K.P.Santhosh, C.Nithya

α-decay chains of the superheavy nuclei ^255-350Rg

NUCLEAR STRUCTURE ^{255,256,257,258,259,260,261,262,263,264,265,266,267,268,269,270,271,273}Rg; calculated S(p), S(2p); deduced negative S(p), thus decay through proton emission.

RADIOACTIVITY ^{272,274,275,276,277,278,279,280,281,282}Rg, ^{268,270,271,272,273,274,275,276,277,278}Mt, ^{264,266,267,268,269,270,271,272,273,274}Bh, ^{260,262,263,264,265,266,267,268,269,270}Db, ^{256,258,260,261,262,263,264,265,266}Lr, ^{252,254,255,256,257,258,259,260,261,262}Md, ^{248,250,251,252,253,254,255,256,257,258}Es, ^{244,246,247,248,249,250,251,252,253,254}Bk, ^{240,242,243,244,245,246,247,248,249,250}Am(α), (SF); calculated half-lives for α and SF decays using Coulomb and proximity potential model for deformed nuclei (CPPMDN). Comparison with other theoretical and empirical calculations, and with available experimental data. A=283-345, Z=111; decay by SF mode. A=346-350, Z=111; stable against α decay.

doi: 10.1103/PhysRevC.95.054621
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2017SA57      Eur.Phys.J. A 53, 189 (2017)

K.P.Santhosh, C.Nithya

Decay properties of ^256-339Ds superheavy nuclei

RADIOACTIVITY ^{256,257,258,259,260,262,262}Ds(α), (p), (SF); calculated p-decay T_1/2 using 5 different models (CPPMDN (Coulomb and Proximity Potential Model for Deformed Nuclei), CPPM (Coulomb and Proximity Potential), Gamow-like approach, Hatsukawa semi-empirical relation, Ni approach), α-decay T_1/2 using 6 different models, spontaneous fission T_1/2. Compared with available data.

doi: 10.1140/epja/i2017-12379-1
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2017SA63      Phys.Rev. C 96, 044613 (2017)

K.P.Santhosh, C.Nithya

α-decay chains of superheavy ^265-279Mt isotopes

RADIOACTIVITY ^{266,268,270,274,275,276,277,278}Mt, ^{262,264,266,270,271,272,274}Bh, ^{258,260,262,266,267,268,270}Db, ^256,258Lr, ²⁵⁴Md(α), (SF); ^{265,266,267,268,269,270,271,272,273,274,275,276,277,278}Mt, ^{261,262,263,264,265,266,267,268,269,270,271,272,273,274}Bh, ^{257,258,259,260,261,262,263,264,265,266,267,268,269,270}Db, ^{253,254,255,256,257,258,259,260,261,262,263,264,265,266}Lr, ^{249,250,251,252,253,254,255,256,257,258,259,260,261,262}Md, ^{245,246,247,248,249,250,251,252,253,254,255,256,257,258}Es, ^{241,242,243,244,245,246,247,248,249,250,251,252,253,254}Bk, ^{237,238,239,240,241,242,243,244,245,246,247,248,249,250}Am, ^{233,234,235,236,237,238,239,240,241,242,243,244,245,246}Np, ^{229,230,231,232,233,234,235,236,237,238,239,240,241,242}Pa, ^{225,226,227,228,229,230,231,232,233,234,235,236,237,238}Ac(α), (SF); calculated half-lives for α and SF decays using Coulomb and proximity potential model for deformed nuclei (CPPMDN) for α decays and shell-effect-dependent formula for SF half-lives. Comparison with available experimental values, and with several other theoretical calculations.

doi: 10.1103/PhysRevC.96.044613
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2017SA65      At.Data Nucl.Data Tables 119, 33 (2017)

K.P.Santhosh, C.Nithya

Predictions on the modes of decay of even Z superheavy isotopes within the range 104 ≤ Z ≤ 136

NUCLEAR STRUCTURE Z=104-136; calculated decay modes and T_1/2, Q-values. Comparison with available data.

doi: 10.1016/j.adt.2017.03.003
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2016SA18      Nucl.Phys. A951, 116 (2016)

K.P.Santhosh, A.Augustine, C.Nithya, B.Priyanka

Predictions on the alpha decay half lives of superheavy nuclei with Z = 113 in the range 255 ≤ A ≤ 314

NUCLEAR STRUCTURE Z=113; calculated α-decay T_1/2 for 255≤A≤314 using CPPMDN (Coulomb and Proximity Potential Model for Deformed Nuclei) and also compared with more simple calculations (CPPM, VSS, Univ and Royer) and also with published results for spontaneous fission; deduced fission mode for individual isotopes of Z=113. Calculated also 4α and 6α decay chains. Compared to available data.

doi: 10.1016/j.nuclphysa.2016.03.041
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2016SA32      Nucl.Phys. A955, 156 (2016)

K.P.Santhosh, B.Priyanka, C.Nithya

Feasibility of observing the α decay chains from isotopes of SHN with Z = 128, Z = 126, Z = 124 and Z = 122

RADIOACTIVITY ^{298,299,300,301,302,303,304,305,306,307,309,310,311,312,313,314,315,316,317,318}122, ^{305,306,307,308,313,314,315,316,317,318,319,320,321,322,323}124, ^{317,318,319,320,323,324,325,326,327,328,329,330,331}126, ^{321,322,323,324,328,329,330,331,332,333}128(SF), (α); calculated T_1/2 of superheavy nuclei α-decay and fission (and also for their daughters Hs, Ds, Cn, Fe, Lv, Z=118) using CPPM (Coulomb and Proximity Potential Model), CPPMDN (CPPM for Deformed Nuclei) and VSS, UNIV and Royer formulae.

doi: 10.1016/j.nuclphysa.2016.06.010
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2016SA49      Int.J.Mod.Phys. E25, 1650079 (2016)

K.P.Santhosh, C.Nithya

Predictions on the alpha decay chains of superheavy nuclei with Z=121 within the range 290 ≤ A ≤ 339

RADIOACTIVITY ^{309,310,311,312,313,314}121, ^{305,306,307,308,309,310}119, ^{301,302,303,304}Ts, ²⁹⁸Mc(α); calculated T_1/2. Comparison with available data.

doi: 10.1142/S0218301316500798
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2016SA53      Phys.Rev. C 94, 054621 (2016)

K.P.Santhosh, C.Nithya

Theoretical studies on the modes of decay of superheavy nuclei

RADIOACTIVITY ²³²Th, ^234,236,238U, ^{236,238,240,242,244,246}Pu, ^{240,242,244,246,248,250}Cm, ^{242,244,246,248,250,252}Cf, ^{246,248,250,252,254,256}Fm, ^252,254,256No, ^{254,256,258,260,262}Rf, ^{258,260,262,264,266}Sg, ^{258,260,262,264,266,268,270,272,274,276,278,280}Hs, ^{264,266,268,270,272,274,276,278,280,282,284}Ds, ^{270,272,274,276,278,280,282,284,286}Cn, ^{274,276,278,280,282,284,286,288}Fl, ^{284,286,288,290,292,294,296,298,300,302,304}Lv, ^{288,290,292,294,296,298,300,302,304}Og, ^{292,294,296,298,300,302,304,306}120(SF); calculated half-lives. ^265,267Rf, ^{266,267,268,270}Db, ^269,271Sg, ^{270,271,272,274}Bh, ^273,275,277Hs, ^{274,275,276,277,278}Mt, ^277,278,281Ds, ^{278,279,280,281,282}Rg, ^{281,282,283,284,285}Cn, ^{282,283,284,285,286}Nh, ^{285,286,287,288,289}Fl, ^{287,288,289,290}Mc, ^{290,291,292,293}Lv, ^293,294Ts, ²⁹⁴Og(α), (SF); calculated half-lives and predicted dominant decay mode. Coulomb and proximity potential model for deformed nuclei (CPPMDN). Comparison with several other theoretical calculations, and available experimental values.

doi: 10.1103/PhysRevC.94.054621
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2016SA56      Eur.Phys.J. A 52, 371 (2016)

K.P.Santhosh, C.Nithya

Theoretical predictions on the decay properties of superheavy nuclei Z = 123 in the region 297 ≤ A ≤ 307

RADIOACTIVITY Z=123(α), (SF); calculated T_1/2 for masses from 297 to 307 and their α-decay daughter nuclei using CPPMDN (Coulomb and Proximity Potential model for Deformed Nuclei); deduced model parameters. Compared with other calculations.

doi: 10.1140/epja/i2016-16371-y
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