NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = M.Aggarwal Found 72 matches. 2024AG02 Nucl.Phys. A1044, 122843 (2024) Correlation between the shape coexistence and stability in Mo and Ru isotopes NUCLEAR STRUCTURE 78,79,80,81,82,83,84,85,86,87,88,89,90,91,92,93,94,95,96,97,98,99,100,101,102,103,104,105,106,107,108,109,110,111,112,113,114,115,116,117,118,119,120,121,122,123,124,125,126,127,128,129,130,131,132,133,134,135,136,137,138,139,140,141,142,143,144Mo, 83,84,85,86,87,88,89,90,91,92,93,94,95,96,97,98,99,100,101,102,103,104,105,106,107,108,109,110,111,112,113,114,115,116,117,118,119,120,121,122,123,124,125,126,127,128,129,130,131,132,133,134,135,136,137,138,139,140,141,142,143,144,145,146,147,148,149,150,151,152Ru; calculated deformation parameters, shell corrections, ground state shape and deformation within the microscopic theoretical framework using Nilsson Strutinsky Method and Relativistic Mean Field Model; deduced energy minima. Comparison with available data.
doi: 10.1016/j.nuclphysa.2024.122843
2023AG01 Nucl.Phys. A1032, 122619 (2023) Impact of the quenching of shell effects with excitation energy on nuclear level density NUCLEAR STRUCTURE Z=27-35; calculated impact of shell effects on nuclear level density (NLD) and particle emission probability as a function of temperature in a microscopic theoretical framework of Statistical Model; deduced the enhancement of LD parameter with the deformation and rotation and the fade out of enhancement with increasing excitations.
doi: 10.1016/j.nuclphysa.2023.122619
2023SA02 J.Phys.(London) G50, 015102 (2023) G.Saxena, M.Aggarwal, D.Singh, A.Jain, P.K.Sharma, H.L.Yadav Deformation dependence of 2p-radioactivity half-lives: probe with a new formula across the mass region with Z < 82 RADIOACTIVITY 6Be, 12O, 16Ne, 19Mg, 45Fe, 48Ni, 54Zn, 67Kr, 10N, 28Cl, 32K, 52Cu, 57Ga, 60,62As(2p); analyzed available data; deduced T1/2 by employing our newly proposed semi-empirical formula wherein the nuclear deformation has been incorporated in a phenomenological way.
doi: 10.1088/1361-6471/ac991d
2021AB12 Phys.Rev. C 104, L061901 (2021) M.S.Abdallah, B.E.Aboona, J.Adam, L.Adamczyk, J.R.Adams, J.K.Adkins, G.Agakishiev, I.Aggarwal, M.M.Aggarwal, Z.Ahammed, I.Alekseev, D.M.Anderson, A.Aparin, E.C.Aschenauer, M.U.Ashraf, F.G.Atetalla, A.Attri, G.S.Averichev, V.Bairathi, W.Baker, J.G.Ball Cap, K.Barish, A.Behera, R.Bellwied, P.Bhagat, A.Bhasin, J.Bielcik, J.Bielcikova, I.G.Bordyuzhin, J.D.Brandenburg, A.V.Brandin, I.Bunzarov, J.Butterworth, X.Z.Cai, H.Caines, M.Calderon de la Barca Sanchez, D.Cebra, I.Chakaberia, P.Chaloupka, B.K.Chan, F.-H.Chang, Z.Chang, N.Chankova-Bunzarova, A.Chatterjee, S.Chattopadhyay, D.Chen, J.Chen, J.H.Chen, X.Chen, Z.Chen, J.Cheng, M.Chevalier, S.Choudhury, W.Christie, X.Chu, H.J.Crawford, M.Csanad, M.Daugherity, T.G.Dedovich, I.M.Deppner, A.A.Derevschikov, A.Dhamija, L.Di Carlo, L.Didenko, P.Dixit, X.Dong, J.L.Drachenberg, E.Duckworth, J.C.Dunlop, N.Elsey, J.Engelage, G.Eppley, S.Esumi, O.Evdokimov, A.Ewigleben, O.Eyser, R.Fatemi, F.M.Fawzi, S.Fazio, P.Federic, J.Fedorisin, C.J.Feng, Y.Feng, P.Filip, E.Finch, Y.Fisyak, A.Francisco, C.Fu, L.Fulek, C.A.Gagliardi, T.Galatyuk, F.Geurts, N.Ghimire, A.Gibson, K.Gopal, X.Gou, D.Grosnick, A.Gupta, W.Guryn, A.I.Hamad, A.Hamed, Y.Han, S.Harabasz, M.D.Harasty, J.W.Harris, H.Harrison, S.He, W.He, X.H.He, Y.He, S.Heppelmann, S.Heppelmann, N.Herrmann, E.Hoffman, L.Holub, Y.Hu, H.Huang, H.Z.Huang, S.L.Huang, T.Huang, X.Huang, Y.Huang, T.J.Humanic, G.Igo, D.Isenhower, W.W.Jacobs, C.Jena, A.Jentsch, Y.Ji, J.Jia, K.Jiang, X.Ju, E.G.Judd, S.Kabana, M.L.Kabir, S.Kagamaster, D.Kalinkin, K.Kang, D.Kapukchyan, K.Kauder, H.W.Ke, D.Keane, A.Kechechyan, M.Kelsey, Y.V.Khyzhniak, D.P.Kikola, C.Kim, B.Kimelman, D.Kincses, I.Kisel, A.Kiselev, A.G.Knospe, H.S.Ko, L.Kochenda, L.K.Kosarzewski, L.Kramarik, P.Kravtsov, L.Kumar, S.Kumar, R.Kunnawalkam Elayavalli, J.H.Kwasizur, R.Lacey, S.Lan, J.M.Landgraf, J.Lauret, A.Lebedev, R.Lednicky, J.H.Lee, Y.H.Leung, C.Li, C.Li, W.Li, X.Li, Y.Li, X.Liang, Y.Liang, R.Licenik, T.Lin, Y.Lin, M.A.Lisa, F.Liu, H.Liu, H.Liu, P.Liu, T.Liu, X.Liu, Y.Liu, Z.Liu, T.Ljubicic, W.J.Llope, R.S.Longacre, E.Loyd, N.S.Lukow, X.F.Luo, L.Ma, R.Ma, Y.G.Ma, N.Magdy, D.Mallick, S.Margetis, C.Markert, H.S.Matis, J.A.Mazer, N.G.Minaev, S.Mioduszewski, B.Mohanty, M.M.Mondal, I.Mooney, D.A.Morozov, A.Mukherjee, M.Nagy, J.D.Nam, Md.Nasim, K.Nayak, D.Neff, J.M.Nelson, D.B.Nemes, M.Nie, G.Nigmatkulov, T.Niida, R.Nishitani, L.V.Nogach, T.Nonaka, A.S.Nunes, G.Odyniec, A.Ogawa, S.Oh, V.A.Okorokov, B.S.Page, R.Pak, J.Pan, A.Pandav, A.K.Pandey, Y.Panebratsev, P.Parfenov, B.Pawlik, D.Pawlowska, H.Pei, C.Perkins, L.Pinsky, R.L.Pinter, J.Pluta, B.R.Pokhrel, G.Ponimatkin, J.Porter, M.Posik, V.Prozorova, N.K.Pruthi, M.Przybycien, J.Putschke, H.Qiu, A.Quintero, C.Racz, S.K.Radhakrishnan, N.Raha, R.L.Ray, R.Reed, H.G.Ritter, M.Robotkova, O.V.Rogachevskiy, J.L.Romero, D.Roy, L.Ruan, J.Rusnak, N.R.Sahoo, H.Sako, S.Salur, J.Sandweiss, S.Sato, W.B.Schmidke, N.Schmitz, B.R.Schweid, F.Seck, J.Seger, M.Sergeeva, R.Seto, P.Seyboth, N.Shah, E.Shahaliev, P.V.Shanmuganathan, M.Shao, T.Shao, A.I.Sheikh, D.Shen, S.S.Shi, Y.Shi, Q.Y.Shou, E.P.Sichtermann, R.Sikora, M.Simko, J.Singh, S.Singha, M.J.Skoby, N.Smirnov, Y.Sohngen, W.Solyst, P.Sorensen, H.M.Spinka, B.Srivastava, T.D.S.Stanislaus, M.Stefaniak, D.J.Stewart, M.Strikhanov, B.Stringfellow, A.A.P.Suaide, M.Sumbera, B.Summa, X.M.Sun, X.Sun, Y.Sun, Y.Sun, B.Surrow, D.N.Svirida, Z.W.Sweger, P.Szymanski, A.H.Tang, Z.Tang, A.Taranenko, T.Tarnowsky, J.H.Thomas, A.R.Timmins, D.Tlusty, T.Todoroki, M.Tokarev, C.A.Tomkiel, S.Trentalange, R.E.Tribble, P.Tribedy, S.K.Tripathy, T.Truhlar, B.A.Trzeciak, O.D.Tsai, Z.Tu, T.Ullrich, D.G.Underwood, I.Upsal, G.Van Buren, J.Vanek, A.N.Vasiliev, I.Vassiliev, V.Verkest, F.Videbaek, S.Vokal, S.A.Voloshin, F.Wang, G.Wang, J.S.Wang, P.Wang, Y.Wang, Y.Wang, Z.Wang, J.C.Webb, P.C.Weidenkaff, L.Wen, G.D.Westfall, H.Wieman, S.W.Wissink, J.Wu, Y.Wu, B.Xi, Z.G.Xiao, G.Xie, W.Xie, H.Xu, N.Xu, Q.H.Xu, Y.Xu, Z.Xu, Z.Xu, C.Yang, Q.Yang, S.Yang, Y.Yang, Z.Ye, Z.Ye, L.Yi, K.Yip, Y.Yu, H.Zbroszczyk, W.Zha, C.Zhang, D.Zhang, J.Zhang, S.Zhang, S.Zhang, X.P.Zhang, Y.Zhang, Y.Zhang, Y.Zhang, Z.J.Zhang, Z.Zhang, Z.Zhang, J.Zhao, C.Zhou, X.Zhu, M.Zurek, M.Zyzak Global Λ-hyperon polarization in Au+Au collisions at √ sNN = 3 GeV
doi: 10.1103/PhysRevC.104.L061901
2021RO07 Phys.Rev. C 103, 024602 (2021) P.Roy, S.Mukhopadhyay, M.Aggarwal, D.Pandit, T.K.Rana, S.Kundu, T.K.Ghosh, K.Banerjee, G.Mukherjee, S.Manna, A.Sen, R.Pandey, D.Mondal, S.Pal, D.Paul, K.Atreya, C.Bhattacharya Excitation energy and angular momentum dependence of the nuclear level density parameter around A ≈ 110 NUCLEAR REACTIONS 93Nb(16O, X), E=116, 142, 160 MeV; 93Nb(20Ne, X), E=145, 180 MeV; measured E(n), I(n), Eγ, Iγ, nγ-coin, n(θ), time-of-flight using eight liquid-scintillator-based neutron detectors, and 50-element BaF2 detector array for γ detection at the K130 cyclotron facility of VECC, Kolkata; deduced differential σ(E, θ), multiplicity of low-energy γ rays, excitation energy and temperature dependence of the inverse nuclear level density parameter, average angular momenta in the residual nuclei and inverse nuclear level density parameters. 104Ag, 107,108In, 111,112Sb; deduced nuclear density parameters, and compared with microscopic statistical-model calculations.
doi: 10.1103/PhysRevC.103.024602
2021SA57 J.Phys.(London) G48, 125102 (2021) G.Saxena, M.Kumawat, R.Sharma, M.Aggarwal Collapse of N = 28 magicity in exotic 40Mg-probe of deformed halo and 2n-radioactivity at Mg neutron drip-line NUCLEAR STRUCTURE 40,42,44Mg; calculated neutron separation energies, single particle energies, neutron and proton pairing energy contributions, shell gaps, radial moments, radial density distributions, neutron skin thickness. 40Mg; deduced neutron halo, dineutron correlations.
doi: 10.1088/1361-6471/ac288b
2020KU26 Int.J.Mod.Phys. E29, 2050068 (2020) M.Kumawat, G.Saxena, M.Kaushik, S.K.Jain, J.K.Deegwal, M.Aggarwal Novel feature of doubly bubble nuclei in 50 ≤ Z(N) ≤ 82 region along with magicity and weakly bound structure NUCLEAR STRUCTURE Z=50-82; calculated the separation energies, s.p. energies, pairing energies, proton and neutron density profiles along with deformations of even-even nuclei using the Relativistic Mean-Field (RMF) approach; deduced central density depletion in both proton and neutron named as doubly bubble nuclei.
doi: 10.1142/S0218301320500688
2019AG04 Nucl.Phys. A983, 166 (2019) Dependence of spin induced structural transitions on level density and neutron emission spectra NUCLEAR STRUCTURE 112Ru, 113Rh, 114Pd, 115Ag, 116Cd, 117In, 118Sn, 119Sb, 120Te, 121I, 122Xe, 123Cs; calculated (inverse of) level density parameter, its dependence on spin, shape (γ) and deformation (β) at excitation energy close to 31 MeV within the framework of statistical theory of superfluid nuclei, rotational energy vs spin, level density vs rotational energy, level density vs internal excitation energy of residual nucleus after the neutron emission, neutron evaporation spectra for 119Sb at E*≈ 31 MeV; deduced impact of shape transition in 112Ru from 14 to 16 h-bar, inverse level density parameter increases with spin for all studied systems, but it decreases with deformation or shape transition form oblate to (uncommon) prolate non-collective at approaching sphericity. Neutron spectra compared to data.
doi: 10.1016/j.nuclphysa.2018.12.010
2019AG14 Int.J.Mod.Phys. E28, 1950099 (2019) M.Aggarwal, M.Kaushik, G.Saxena High spin states of Zr isotopes around A=80 mass region- study on cold and hot rotating nuclei NUCLEAR STRUCTURE 76,77,78,79,80,81,82,83,84,85,86,87,88,89,90,91,92,93,94,95,96,97,98,99,100,101,102,103,104,105,106,107,108,109,110,111,112,113,114,115,116,117,118,119,120,121,122,123,124Zr; calculated ground state quadrupole deformation, parameters, high-spin states, proton and neutron pairing gaps, moments of inertia.
doi: 10.1142/S021830131950099X
2019SA02 Phys.Lett. B 788, 1 (2019) G.Saxena, M.Kumawat, M.Kaushik, S.K.Jain, M.Aggarwal Bubble structure in magic nuclei NUCLEAR STRUCTURE 12,13,14,15,16,17,18,19,20,21,22,23,24O, 34,35,36,37,38,39,40,41,42,43,44,45,46,47,48,49,50,51,52,53,54,55,56,57,58,59,60,61,62,63,64,65,66,67,68,69,70Ca, 48,49,50,51,52,53,54,55,56,57,58,59,60,61,62,63,64,65,66,67,68,69,70,71,72,73,74,75,76,77,78,79,80,81,82,83,84,85,86,87,88,89,90,91,92,93,94,95,96,97,98Ni, 80,81,82,83,84,85,86,87,88,89,90,91,92,93,94,95,96,97,98,99,100,101,102,103,104,105,106,107,108,109,110,111,112,113,114,115,116,117,118,119,120,121,122,123,124,125,126,127,128,129,130,131,132,133,134,135,136,137,138,139,140,141,142,143,144,145,146,147,148,149,150Zr, 78,79,80,81,82,83,84,85,86,87,88,89,90,91,92,93,94,95,96,97,98,99,100,101,102,103,104,105,106,107,108,109,110,111,112,113,114,115,116,117,118,119,120,121,122,123,124,125,126Sn, 178,179,180,181,182,183,184,185,186,187,188,189,190,191,192,193,194,195,196,197,198,199,200,201,202,203,204,205,206,207,208,209,210,211,212,213,214,215,216,217,218,219,220,221,222,223,224,225,226,227,228,229,230,231,232,233,234,235,236,237,238,239,240,241,242,243,244,245,246,247,248,249,250,251,252,253,254,255,256,257,258,259,260,261,262Pb, 251Fr, 299Mc, 302Og, 22Si, 34Si, 46Ar, 56S, 58Ar, 184Ce, 347119, 292120, 341Nh; calculated charge and matter densities, single particle levels and depletion fraction (DF) across the periodic chart; deduced that the central depletion is correlated to shell structure and occurs due to unoccupancy in s-orbit (2s, 3s, 4s) and inversion of (2s, 1d) and (3s, 1h) states in nuclei upto Z less or equal to 82. Bubble effect in superheavy region is a signature of the interplay between the Coulomb and nn-interaction where the depletion fraction is found to increase with Z (Coulomb repulsion) and decrease with isospin.
doi: 10.1016/j.physletb.2018.08.076
2019SA08 Phys.Lett. B 789, 323 (2019) G.Saxena, M.Kumawat, B.K.Agrawal, M.Aggarwal Anti-bubble effect of temperature and deformation: A systematic study for nuclei across all mass regions between A=20-300 NUCLEAR STRUCTURE 22,34Si, 46,58Ar, 56S, 184Ce, 294,302Og, 292120, 22O, 34Ca, 24Ne, 40Mg, 44S, 32Ar; calculated charge and neutron densities as function of temperatures, proton single-particle energies, nuclear charge form factors, depletion fractions, quadrupole deformation parameters, occupation probabilities.
doi: 10.1016/j.physletb.2018.10.062
2019SA25 Int.J.Mod.Phys. E28, 1950008 (2019) G.Saxena, M.Kumawat, S.Somorendro Singh, M.Aggarwal Structural properties and decay modes of Z = 122, 120 and 118 superheavy nuclei NUCLEAR STRUCTURE 284,285,286,287,288,289,290,291,292,293,294,295,296,297,298,299Og, 290,291,292,293,294,295,296,297,298,299,300,301,302,303,304,305120, 298,299,300,301,302,303,304,305,306,307,308,309,310,311,312,313,314122; calculated neutron and charge densities, ground state properties viz. binding energies, charge, proton, neutron, matter radii. RADIOACTIVITY 272,273,274,275,276,277,278,279,280,281,282,283,284,285,286,287,288Cn, 276,277,278,279,280,281,282,283,284,285,286,287,288,289,290,291,292Fl, 280,281,282,283,284,285,286,287,288,289,290,291,292,293,294,295,296Lv, 284,285,286,287,288,289,290,291,292,293,294,295,296,297,298,299,300Og, 288,289,290,291,292,293,294,295,296,297,298,299,300,301,302,303,304120, 292,293,294,295,296,297,298,299,300,301,302,303,304,305,306,307,308122(α); calculated T1/2. Comparison with available data.
doi: 10.1142/S0218301319500083
2019SA45 J.Phys.(London) G46, 065105 (2019) G.Saxena, M.Kumawat, B.K.Agrawal, M.Aggarwal A systematic study of the factors affecting central depletion in nuclei NUCLEAR STRUCTURE 30Ne, 32Mg, 34Si, 46Ar, 56S, 58Ar; calculated bubble parameters, proton single-particle energies, binding energies.
doi: 10.1088/1361-6471/ab0853
2019SA49 Hyperfine Interactions 240, 106 (2019) Authors: G.Saxena, M.Kumawat, B.K.Agrawal, M.Aggarwal Correction to: Effect of quadrupole deformation and temperature on bubble structure in N = 14 nuclei
doi: 10.1007/s10751-019-1647-y
2019SA50 Hyperfine Interactions 240, 74 (2019) G.Saxena, M.Kumawat, B.K.Agrawal, M.Aggarwal Effect of quadrupole deformation and temperature on bubble structure in N=14 nuclei NUCLEAR STRUCTURE 24Ne, 32Ar; calculated quadrupole deformation parameters, proton occupation probability using the relativistic mean-field plus BCS approach using NL3* and PK1 parameters.
doi: 10.1007/s10751-019-1620-9
2019SA58 Int.J.Mod.Phys. E28, 1950101 (2019) G.Saxena, M.Kumawat, M.Aggarwal Search for exotic features in the ground state light nuclei with 10≤Z≤18 from stable valley to drip lines NUCLEAR STRUCTURE 16,18,20,22,24,26,28,30,32,34,36,38,40,42,44,46,48,50,52Ne, 18,20,22,24,26,28,30,32,34,36,38,40,42,44,46,48,50,52,54Mg, 20,22,24,26,28,30,32,34,36,38,40,42,44,46,48,50,52,54,56Si, 22,24,26,28,30,32,34,36,38,40,42,44,46,48,50,52,54,56,58S, 24,26,28,30,32,34,36,38,40,42,44,46,48,50,52,54,56,58,60Ar; calculated two neutron separation energy, charge and neutron radii, neutron density and skin, charge form factor, deformation parameters, potential energy surface as a function of the deformation parameter, ground state properties.
doi: 10.1142/S0218301319501015
2018AG06 Int.J.Mod.Phys. E27, 1850062 (2018) Persistence of magicity in neutron-rich exotic 78Ni in ground as well as excited states NUCLEAR STRUCTURE 70Ca, 72Ti, 74Cr, 76Fe, 78Ni; calculated charge distribution along with radius, pairing energy contributions from protons and neutrons, neutron and proton single-particle energies for Ni isotopes, two-neutron shell gaps, level density parameter versus mass number A for Ni isotopes at different temperatures, entropy versus mass number A for Ni isotopes at different temperatures, rotational states. Comparison with available data.
doi: 10.1142/S0218301318500623
2018SA44 Int.J.Mod.Phys. E27, 1850074 (2018) G.Saxena, U.K.Singh, M.Kumawat, M.Kaushik, S.K.Jain, M.Aggarwal Distinct ground state features and the decay chains of Z=121 superheavy nuclei NUCLEAR STRUCTURE Z=121; calculated separation energies, shell corrections, deformation parameters, radial variation of charge density and neutron density using RMF+BCS approach. RADIOACTIVITY 293,294,295,296,297,298,299,300,301,302,303,304,305,306,307,308,309,310,311,312121(α); calculated Q-values, T1/2. Comparison with available data.
doi: 10.1142/S021830131850074X
2017SA69 Int.J.Mod.Phys. E26, 1750072 (2017) G.Saxena, M.Kumawat, M.Kaushik, U.K.Singh, S.K.Jain, S.Somorendro Singh, M.Aggarwal Implications of occupancy of 2s1/2 state in sd-shell within RMF+BCS approach NUCLEAR STRUCTURE 22C, 22,24O, 34,36Ca, 26S, 36S, 56S, 22,34,48Si; calculated quadrupole deformation parameters, neutron single particle states, neutron density. Comparison with available data.
doi: 10.1142/S0218301317500720
2017SA70 Phys.Lett. B 775, 126 (2017) G.Saxena, M.Kumawat, M.Kaushik, S.K.Jain, M.Aggarwal Two-proton radioactivity with 2p halo in light mass nuclei A = 18-34 NUCLEAR STRUCTURE 19Mg, 22Si, 26S, 30Ar, 34Ca; calculated variation of charge density, charge radii, RMF potential energy, centrifugal barrier energy for proton resonant states; deduced 2-proton halo.
doi: 10.1016/j.physletb.2017.10.055
2015SH06 Phys.Rev. C 91, 024909 (2015) B.Sharma, M.M.Aggarwal, N.R.Sahoo, T.K.Nayak Dynamical charge fluctuations in the hadronic medium
doi: 10.1103/PhysRevC.91.024909
2014AG01 Phys.Rev. C 89, 024325 (2014) Coexisting shapes with rapid transitions in odd-Z rare-earth proton emitters NUCLEAR STRUCTURE 103,104,105,106,107,108Sb, 108,109,110,111,112,113,114,115I, 112,113,114,115,116,117,118Cs, 117,118,119,120,121,122,123La, 121,122,123,124,125,126,127,128Pr, 126,127,128,129,130,131,132,133Pm, 131,132,133,134,135,136,137Eu, 134,135,136,137,138,139,140,141,142Tb, 140,141,142,143,144,145,146,147Ho, 144,145,146,147,148,149,150Tm, 150,151,152,153,154,155,156,157,158,159Lu, 153,154,155,156,157,158,159,160,161,162,163Ta, 164Re; calculated position of proton drip line, S(p), β and γ deformation parameters. Shape coexistence and rapid shape phase transitions. 112,113,114,115Cs, 117,118La; calculated energy minimization curves as function of β and γ deformation. Triaxially deformed Nilsson potential and Strutinsky's prescription for shell correction. Comparison with experimental data.
doi: 10.1103/PhysRevC.89.024325
2014AG19 Phys.Rev. C 90, 064322 (2014) Shape coexistence in excited odd-Z proton emitters 131-136Eu NUCLEAR STRUCTURE 131,133,134,135,136Eu; calculated equilibrium deformation β versus angular momentum at different temperatures, free energy minimization curves as a function of deformation parameters (β, γ), occupation probability versus single particle energies for neutrons. Search for shape coexistence and shape phase transitions in odd-Z proton emitters as potential candidates for GDR probes nuclear shape. Calculations based on mean-field approximation for the rotating nucleus.
doi: 10.1103/PhysRevC.90.064322
2013AG03 Nucl.Phys. A898, 14 (2013) M.M.Aggarwal, Z.Ahammed, A.L.S.Angelis, V.Antonenko, V.Arefiev, V.Astakhov, V.Avdeitchikov, T.C.Awes, P.V.K.S.Baba, S.K.Badyal, S.Bathe, B.Batiounia, C.Baumann, T.Bernier, K.B.Bhalla, V.S.Bhatia, C.Blume, D.Bucher, H.Busching, L.Carlen, S.Chattopadhyay, M.P.Decowski, H.Delagrange, P.Donni, M.R.Dutta Majumdar, K.El Chenawi, A.K.Dubey, K.Enosawa, S.Fokin, V.Frolov, M.S.Ganti, S.Garpman, O.Gavrishchuk, F.J.M.Geurts, T.K.Ghosh, R.Glasow, B.Guskov, H.A.Gustafsson, H.H.Gutbrod, I.Hrivnacova, M.Ippolitov, H.Kalechofsky, R.Kamermans, K.Karadjev, K.Karpio, B.W.Kolb, I.Kosarev, I.Koutcheryaev, A.Kugler, P.Kulinich, M.Kurata, A.Lebedev, H.Lohner, L.Luquin, D.P.Mahapatra, V.Manko, M.Martin, G.Martinez, A.Maximov, Y.Miake, G.C.Mishra, B.Mohanty, M.-J.Mora, D.Morrison, T.Mukhanova, D.S.Mukhopadhyay, H.Naef, B.K.Nandi, S.K.Nayak, T.K.Nayak, A.Nianine, V.Nikitine, S.Nikolaev, P.Nilsson, S.Nishimura, P.Nomokonov, J.Nystrand, A.Oskarsson, I.Otterlund, S.Pavliouk, T.Peitzmann, D.Peressounko, V.Petracek, S.C.Phatak, W.Pinganaud, F.Plasil, M.L.Purschke, J.Rak, M.Rammler, R.Raniwala, S.Raniwala, N.K.Rao, F.Retier, K.Reygers, G.Roland, L.Rosselet, I.Roufanov, C.Roy, J.M.Rubio, S.S.Sambyal, R.Santo, S.Sato, H.Schlagheck, H.-R.Schmidt, Y.Schutz, G.Shabratova, T.H.Shah, I.Sibiriak, T.Siemiarczuk, D.Silvermyr, B.C.Sinha, N.Slavine, K.Soderstrom, G.Sood, S.P.Sorensen, P.Stankus, G.Stefanek, P.Steinberg, E.Stenlund, M.Sumbera, T.Svensson, A.Tsvetkov, L.Tykarski, E.C.v.d.Pijll, N.v.Eijndhoven, G.J.v.Nieuwenhuizen, A.Vinogradov, Y.P.Viyogi, A.Vodopianov, S.Voros, B.Wyslouch, G.R.Young Photon and η production in p + Pb and p + C collisions at √ sNN=17.4 GeV
doi: 10.1016/j.nuclphysa.2012.11.010
2011AG03 Phys.Rev. C 83, 024901 (2011), Erratum Phys.Rev. C 107, 049903 (2023) M.M.Aggarwal, for the STAR Collaboration Strange and multistrange particle production in Au+Au collisions at √ sNN = 62.4 GeV
doi: 10.1103/PhysRevC.83.024901
2011AG05 Phys.Rev. C 83, 034910 (2011) M.M.Aggarwal, for the STAR Collaboration Scaling properties at freeze-out in relativistic heavy-ion collisions
doi: 10.1103/PhysRevC.83.034910
2011AG13 Phys.Rev. C 83, 064905 (2011) M.M.Aggarwal, for the STAR Collaboration Pion femtoscopy in p + p collisions at √ s=200 GeV
doi: 10.1103/PhysRevC.83.064905
2011AG16 Phys.Rev. C 84, 034909 (2011) M.M.Aggarwal, for the STAR Collaboration K*0 production in Cu + Cu and Au + Au collisions at √ sNN=62.4 GeV and 200 GeV
doi: 10.1103/PhysRevC.84.034909
2011MA12 Acta Phys.Pol. B42, 643 (2011) I.Mazumdar, D.A.Gothe, G.Anil Kumar, M.Aggarwal Shape Transition and Isovector Giant Quadrupole Resonance Decay in Hot Rotating Nuclei NUCLEAR REACTIONS 180Hf(12C, X)192Pt/188Os, E=65 MeV; measured Eγ, Iγ; deduced deformed non-spherical shape, excess yield of high-energy γ-rays, possible first observation of the Isovector Giant Quadrupole Resonance (IVGQR) on excited state.
doi: 10.5506/APhysPolB.42.643
2010AG03 Phys.Rev. C 81, 047302 (2010) Angular momentum dependence of the nuclear level density parameter NUCLEAR STRUCTURE 108Cd, 109In, 112Sn, 113Sb, 122Te, 123I, 127Cs; calculated inverse level density parameter vs angular momentum, axial deformation parameter vs temperature. 109In; calculated excitation energies vs angular momentum. Calculations in the framework of statistical theory of a hot rotating nucleus. Comparison with experimental data.
doi: 10.1103/PhysRevC.81.047302
2010AG05 Phys.Rev.Lett. 105, 022302 (2010) M.M.Aggarwal, for the STAR Collaboration Higher Moments of Net Proton Multiplicity Distributions at RHIC
doi: 10.1103/PhysRevLett.105.022302
2010AG08 Phys.Rev. C 82, 024905 (2010) M.M.Aggarwal, for the STAR Collaboration Balance functions from Au+Au, d+Au, and p+p collisions at √ sNN = 200 GeV
doi: 10.1103/PhysRevC.82.024905
2010AG09 Phys.Rev. C 82, 024912 (2010) M.M.Aggarwal, for the STAR Collaboration Azimuthal di-hadron correlations in d+ Au and Au + Au collisions at √ sNN = 200 GeV measured at the STAR detector
doi: 10.1103/PhysRevC.82.024912
2010AG10 Phys.Rev.Lett. 105, 202301 (2010) M.M.Aggarwal, for the STAR Collaboration Measurement of the Bottom Quark Contribution to Nonphotonic Electron Production in p+p Collisions at √ S=200 GeV
doi: 10.1103/PhysRevLett.105.202301
2009AG06 Phys.Rev. C 80, 024322 (2009) Deformation and shape transitions in hot rotating neutron deficient Te isotopes NUCLEAR STRUCTURE 103,104,105,106,107,108,109,110,111,112,113,114,115,116,117,118,119,120,121,122,123,124Te; calculated free energy, deformation and nuclear shapes under the influence of temperature (0-2 MeV) and rotation (up to spin 60) using macroscopic-microscopic calculations. Comparison with experimental data.
doi: 10.1103/PhysRevC.80.024322
2009MA24 Acta Phys.Pol. B40, 545 (2009) I.Mazumdar, D.A.Gothe, G.Anil kumar, M.Aggarwal, P.K.Joshi, R.Palit, H.C.Jain Search for Rare Shape Transition and GQR Decay in Hot Rotating 188Os Nucleus NUCLEAR REACTIONS 12C(180Hf, X), E=65 MeV; measured Eγ, Iγ;188Os, 192Pt; deduced giant dipole resonance strength distributions.
2008AG09 Int.J.Mod.Phys. E17, 1091 (2008) Neutron emission spectra and level density of hot rotating 132Sn NUCLEAR STRUCTURE 132Sn; calculated nuclear level density, neutron separation energy and neutron emission probability using statistical theory.
doi: 10.1142/S0218301308010295
2007MA43 Acta Phys.Pol. B38, 1463 (2007) I.Mazumdar, H.C.Jain, R.Palit, D.A.Gothe, P.K.Joshi, M.Aggarwal Search for Rare Shape Transition in Hot Rotating 188Os Nucleus NUCLEAR REACTIONS 176Yb(12C, F), E=65, 84 MeV; measured Eγ, Iγ, angular anisotropy from GDR decay. 188Os deduced shape parameters.
2006AG09 Phys.Lett. B 638, 39 (2006) M.M.Aggarwal, G.Sood, Y.P.Viyogi Event-by-event study of DCC-like fluctuation in ultra-relativistic nuclear collisions
doi: 10.1016/j.physletb.2006.05.013
2006AG13 Eur.Phys.J. C 48, 343 (2006) M.M.Aggarwal, and the WA98 Collaboration Pion freeze-out time in Pb+Pb collisions at 158 AGeV/c studied via π-/π+ and K-/K+ ratios NUCLEAR REACTIONS Pb(Pb, X), E at 158 GeV/c/nucleon; measured charged pion yield ratios vs transverse mass, centrality; deduced hyperon decay contribution, freeze-out time.
doi: 10.1140/epjc/s10052-006-0081-x
2006AG14 Phys.Scr. T125, 178 (2006) Two-proton radioactivity in proton-rich fp shell nuclei at high spin NUCLEAR STRUCTURE 45,46Fe, 48,49,50Ni, 54,55,56Zn; calculated one- and two-proton separation energies vs spin.
doi: 10.1088/0031-8949/2006/T125/039
2005AG06 Eur.Phys.J. C 41, 287 (2005) M.M.Aggarwal, and the WA98 Collaboration Azimuthal anisotropy of photon and charged particle emission in 208Pb + 208Pb collisions at 158A GeV/c NUCLEAR REACTIONS 208Pb(208Pb, X), E at 158 GeV/c/nucleon; measured photon and charged particles azimuthal distributions; deduced anisotropy coefficients.
doi: 10.1140/epjc/s2005-02249-2
2005AG14 Nucl.Phys. A762, 129 (2005) M.M.Aggarwal, and the WA98 Collaboration Centrality and transverse momentum dependence of collective flow in 158 A GeV Pb + Pb collisions measured via inclusive photons NUCLEAR REACTIONS 208Pb(208Pb, X), E=158 GeV/nucleon; measured inclusive photons direct and elliptic flow vs centrality, rapidity, and transverse momentum; deduced neutral pion flow features.
doi: 10.1016/j.nuclphysa.2005.08.004
2004AG02 Phys.Rev. C 69, 034602 (2004) Hot rotating fp shell nuclei near proton drip NUCLEAR STRUCTURE 44,45,46,47,48,49,50,51,52,53,54,55,56,57,58,59,60Fe; calculated proton separation energies, level density and deformation parameters vs temperature. 46,50,54,58Fe; calculated rotational bands energy vs spin, related features. Determination of particle stability discussed.
doi: 10.1103/PhysRevC.69.034602
2004AG03 Phys.Rev.Lett. 93, 022301 (2004) M.M.Aggarwal, and the WA98 Collaboration Interferometry of Direct Photons in Central 208Pb + 208Pb Collisions at 158A GeV NUCLEAR REACTIONS 208Pb(208Pb, X), E=158 GeV/nucleon; measured two-photon correlations; deduced source radii, direct photon yields.
doi: 10.1103/PhysRevLett.93.022301
2004AG08 Int.J.Mod.Phys. E13, 1239 (2004) Neutron emission spectra of excited 126-140Sn nuclei NUCLEAR STRUCTURE 126,128,130,132,134,136,138,140Sn; calculated one- and two-neutron emission probability, neutron spectra vs excitation energy.
doi: 10.1142/S0218301304002697
2003AG01 Phys.Rev. C 67, 014906 (2003) M.M.Aggarwal, and the WA98 Collaboration One-, two-, and three-particle distributions from 158A GeV/c central Pb+Pb collisions NUCLEAR REACTIONS Pb(Pb, X), E at 158 GeV/c/nucleon; measured negative pion and kaon transverse mass spectra, two- and three-pion correlations; deduced source features. Hydrodynamical model analysis.
doi: 10.1103/PhysRevC.67.014906
2003AG06 Phys.Rev. C 67, 044901 (2003) M.M.Aggarwal, and the WA98 Collaboration Centrality dependence of charged-neutral particle fluctuations in 158A GeV 208Pb+208Pb collisions NUCLEAR REACTIONS 208Pb(208Pb, X), E at 158 GeV/c/nucleon; measured charged particle and photon multiplicity, fluctuations vs centrality; deduced nonstatistical fluctuations, upper limit on disoriented chiral condensate formation.
doi: 10.1103/PhysRevC.67.044901
2003AG09 Pramana 60, 987 (2003) M.M.Aggarwal, and the WA98 Collaboration Event-by-event search for charged-neutral fluctuations in Pb-Pb collisions at 158 A GeV NUCLEAR REACTIONS Pb(Pb, X), E=158 GeV/nucleon; analyzed data; deduced event-by-event fluctuations, azimuthal distributions.
doi: 10.1007/BF02707017
2002AG05 Eur.Phys.J. C 23, 225 (2002) M.M.Aggarwal, and the WA98 Collaboration Transverse Mass Distributions of Neutral Pions from 208Pb-Induced Reactions at 158.A GeV NUCLEAR REACTIONS Nb, Pb(208Pb, X), E=158 GeV/nucleon; measured neutral pion transverse mass and multiplicity distributions. Comparisons with model predictions.
doi: 10.1088/0143-0807/23/2/316
2002AG08 Phys.Rev. C65, 054912 (2002) M.M.Aggarwal, and the WA98 Collaboration Event-by-Event Fluctuations in Particle Multiplicities and Transverse Energy Produced in 158A GeV Pb + Pb Collisions NUCLEAR REACTIONS Pb(Pb, X), E=158 GeV/nucleon; measured particle multiplicities, total transverse energy, event-by-event fluctuations, centrality dependence. Comparison with participant model results.
doi: 10.1103/PhysRevC.65.054912
2001AG04 Eur.Phys.J. C 18, 651 (2001) M.M.Aggarwal, and the WA98 Collaboration Scaling of Particle and Transverse Energy Production in 208Pb + 208Pb Collisions at 158.A GeV NUCLEAR REACTIONS 208Pb(208Pb, X), E=158 GeV/nucleon; measured fragments transverse energy, pseudorapidity vs centrality; deduced scaling features.
2001AG07 Phys.Rev. C64, 011901 (2001) M.M.Aggarwal, and the WA98 Collaboration Localized Charged-Neutral Fluctuations in 158A GeV Pb + Pb Collisions NUCLEAR REACTIONS Pb(Pb, X), E=158 GeV/nucleon; analyzed particle multiplicities, azimuthal distributions, event-by-event fluctuations.
doi: 10.1103/PhysRevC.64.011901
2000AG02 Phys.Lett. 477B, 37 (2000) M.M.Aggarwal, and the WA98 Collaboration Δ++ Production in 158 A GeV 208Pb + 208Pb Interactions at the CERN SPS NUCLEAR REACTIONS 208Pb(208Pb, X), E=158 GeV/nucleon; measured Δ++ resonance yields.
doi: 10.1016/S0370-2693(00)00224-0
2000AG05 Eur.Phys.J. C 16, 445 (2000) M.M.Aggarwal, and the WA98 Collaboration Central Pb + Pb Collisions at 158 A GeV/c Studied by π-π- Interferometry NUCLEAR REACTIONS Pb(Pb, X), E=158 GeV/nucleon; measured two-pion correlations; deduced emission source size, expansion characteristics. Interferometry analysis.
2000AG06 Phys.Rev.Lett. 85, 2895 (2000) M.M.Aggarwal, and the WA98 Collaboration Three-Pion Interferometry Results from Central Pb + Pb Collisions at 158A GeV/c NUCLEAR REACTIONS 208Pb(208Pb, X), E at 158 GeV/c/nucleon; analyzed two-, three-pion correlations; deduced source features.
doi: 10.1103/PhysRevLett.85.2895
2000AG08 Phys.Rev.Lett. 85, 3595 (2000) M.M.Aggarwal, and the WA98 Collaboration Observation of Direct Photons in Central 158A GeV 208Pb + 208Pb Collisions NUCLEAR REACTIONS 208Pb(208Pb, X), E=158 GeV/nucleon; measured direct Eγ, Iγ, transverse momentum spectra vs centrality. Comparison with proton-induced reactions.
doi: 10.1103/PhysRevLett.85.3595
1999AG04 Phys.Lett. 458B, 422 (1999) M.M.Aggarwal, and the WA98 Collaboration Systematics of Inclusive Photon Production in 158.A GeV Pb Induced Reactions on Ni, Nb, and Pb Targets NUCLEAR REACTIONS Ni, Nb, Pb(Pb, X), E=158 GeV/nucleon; measured photon multiplicity, pseudorapidity distributions, mean transverse momentum. Comparison with model predictions.
doi: 10.1016/S0370-2693(99)00560-2
1999AG05 Phys.Rev.Lett. 83, 926 (1999) M.M.Aggarwal, and the WA98 Collaboration Freeze-Out Parameters in Central 158A GeV 208Pb + Pb Collisions NUCLEAR REACTIONS 208Pb(208Pb, X), E=158 GeV/nucleon; measured neutral pion transverse mass spectra; deduced freeze-out parameters. Hydrodynamical model.
doi: 10.1103/PhysRevLett.83.926
1999AG07 Phys.Lett. 469B, 30 (1999) M.M.Aggarwal, and the WA98 Collaboration Elliptic Emission of K+ and π+ in 158 A.GeV Pb + Pb Collisions NUCLEAR REACTIONS Pb(Pb, X), E=158 GeV/nucleon; measured kaon, pion azimuthal distributions; deduced possible in-medium potential effects. Relativistic quantum molecular dynamics calculations.
doi: 10.1016/S0370-2693(99)01289-7
1998AG02 Phys.Lett. 420B, 169 (1998) M.M.Aggarwal, and the WA98 Collaboration Search for Disoriented Chiral Condensates in 158 AGeV Pb + Pb Collisions NUCLEAR REACTIONS Pb(Pb, X), E=158 GeV/nucleon; measured charged, neutral multplicity distributions; deduced upper limit for production of disoriented chiral condensates.
doi: 10.1016/S0370-2693(97)01528-1
1998AG07 Phys.Rev. C58, 1146 (1998) M.M.Aggarwal, and the WA93 Collaboration Multiplicity and Pseudorapidity Distribution of Photons in the S + Au Reaction at 200A GeV NUCLEAR REACTIONS 197Au(S, X), E=200 GeV/nucleon; measured photons multiplicity, pseudorapidity distributions.
doi: 10.1103/PhysRevC.58.1146
1998AG11 Phys.Lett. 438B, 357 (1998) M.M.Aggarwal, V.S.Bhatia, A.C.Das, Y.P.Viyogi Event-by-Event Fluctuation of Rapidity Distributions in Heavy-Ion Collisions NUCLEAR REACTIONS Pb(Pb, X), E=high; analyzed photon rapidity distribution; deduced power spectrum quark-gluon plasma detection method.
doi: 10.1016/S0370-2693(98)01130-7
1998AG12 Phys.Rev.Lett. 81, 4087 (1998); Erratum Phys.Rev.Lett. 84, 578 (2000) M.M.Aggarwal, and the WA98 Collaboration Centrality Dependence of Neutral Pion Production in 158A GeV 208Pb + 208Pb Collisions NUCLEAR REACTIONS 208Pb(208Pb, X), E=158 GeV/nucleon; measured neutral pions transverse mass, transverse momentum spectra; deduced centrality dependence, possible thermal emission process.
doi: 10.1103/PhysRevLett.81.4087
1998RA13 Int.J.Mod.Phys. E7, 389 (1998) Neutron Separation Energies of Extremely Neutron Rich Excited Nuclei from Z = 30 to 70 NUCLEAR STRUCTURE Z=30-70; calculated one-neutron separation energy for neutron-rich even-even nuclei; deduced rotation, thermal excitation effects. Microscopic-macroscopic approach.
doi: 10.1142/S021830139800018X
1998RA28 Phys.Rev. C58, 2743 (1998) Proton Drip Line Nuclei Around Z = 30 to 40 NUCLEAR STRUCTURE 54,56,58,60Zn, 58,60,62,64Ge, 70,72,74,76Sr, 67,69,71Br, 63,65,67As; calculated proton separation energy vs angular momentum, temperature; deduced alteration of proton drip line. Macroscopic-microscopic model.
doi: 10.1103/PhysRevC.58.2743
1997AG07 Phys.Rev. C56, 1160 (1997) M.M.Aggarwal, and the WA93 Collaboration Soft Photon Production in Central 200 GeV/nucleon 32S + Au Collisions NUCLEAR REACTIONS 197Au(32S, X), E=200 GeV/nucleon; measured photon inclusive σ; deduced soft photon excess over expectation from neutral meson decay. Small acceptance BGO detector.
doi: 10.1103/PhysRevC.56.1160
1997AG09 Phys.Lett. 403B, 390 (1997) M.M.Aggarwal, and the WA93 Collaboration Azimuthal Anisotropy in S + Au Reactions at 200 A GeV NUCLEAR REACTIONS 197Au(S, X), E=200 GeV/nucleon; measured mid-rapidity produced photons azimuthal correlations; deduced anisotropy related features.
doi: 10.1016/S0370-2693(97)00566-2
1997AG10 Phys.Lett. 404B, 207 (1997) M.M.Aggarwal, and the WA93 Collaboration Event by Event Measurement of <p(T)> of Photons in S + Au Collisions at 200 A.GeV NUCLEAR REACTIONS 197Au(S, X), E at 200 GeV/nucleon; measured electromagnetic transverse energy, photon multiplicity ratio; deduced photons mean transverse momentum, centrality dependence.
doi: 10.1016/S0370-2693(97)00567-4
1995AG05 Int.J.Mod.Phys. E4, 477 (1995) Review of Rapidity Density Distributions in Heavy-Ion Induced Interactions at Relativistic Energies NUCLEAR REACTIONS 27Al, W, Ag, Br(16O, X), S, Ag, 27Al, 197Au(32S, X), E=200 GeV/nucleon; compiled, reviewed pseudorapidity distributions, data, analyses, relativistic collisions. Other reactions, aspects studied.
doi: 10.1142/S0218301395000183
1989AD13 Phys.Rev.Lett. 63, 2349 (1989) M.Aderholz, M.M.Aggarwal, H.Akbari, P.P.Allport, P.V.K.S.Baba, S.K.Badyal, M.Barth, J.P.Baton, H.H.Bingham, E.B.Brucker, R.A.Burnstein, R.C.Campbell, R.Cence, T.K.Chatterjee, E.F.Clayton, G.Corrigan, C.Coutures, D.Deprospo, Devanand, E.De Wolf, P.J.W.Faulkner, W.B.Fretter, V.K.Gupta, J.Guy, J.Hanlon, G.Harigel, F.Harris, M.A.Jabiol, P.Jacques, V.Jain, G.T.Jones, M.D.Jones, R.W.L.Jones, T.Kafka, M.Kalelkar, P.Kasper, P.Kasper, G.L.Kaul, M.Kaur, J.M.Kohli, E.L.Koller, R.J.Krawiec, M.Lauko, J.Lys, W.A.Mann, P.Marage, R.H.Milburn, D.B.Miller, I.S.Mittra, M.M.Mobayyen, J.Moreels, D.R.O.Morrison, G.Myatt, P.Nailor, R.Naon, A.Napier, M.Neveu, D.Passmore, M.W.Peters, V.Z.Peterson, R.Plano, N.K.Rao, H.A.Rubin, J.Sacton, B.Saitta, P.Schmid, N.Schmitz, J.Schneps, R.Sekulin, S.Sewell, J.B.Singh, P.M.Sood, W.Smart, P.Stamer, K.E.Varvell, W.Venus, L.Verluyten, L.Voyvodic, H.Wachsmuth, S.Wainstein, S.Willocq, W.Wittek, G.P.Yost Coherent Production of π+ and π- Mesons by Charged-Current Interactions of Neutrinos and Antineutrinos on Neon Nuclei at the Fermilab Tevatron NUCLEAR REACTIONS 1H, Ne(ν, X), (ν-bar, X), E=40-300 GeV; measured coherent single π+, π- production σ, kinematic distributions. Meson dominance, partial axial-vector current conservation model.
doi: 10.1103/PhysRevLett.63.2349
1984IS02 Phys.Rev.Lett. 52, 1280 (1984) A.Z.M.Ismail, M.S.El-Nagdy, K.L.Gomber, M.M.Aggarwal, P.L.Jain Mean Free Paths of He, Li, and Be Produced in Heavy-Ion Collisions at 2 GeV/u NUCLEAR REACTIONS 56Fe(40Ar, He), (40Ar, Li), (40Ar, Be), E=2 GeV/nucleon; measured fragment mean free paths; deduced no anomalous effects.
doi: 10.1103/PhysRevLett.52.1280
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