Investigating fission-like fragments in 208Pb(12C,x)220Ra reaction at E⋆= 39.6 and 45.4 MeV Rupinderjeet Kaur, Amanjot, Priyanka, Malika Kaushik, Subham Kumar, Arshiya Sood, Yashraj Jangid, Rakesh Kumar, Manoj Kumar Sharma, Pushpendra P. Singh Results in Physics, 2025 The cross-sections of 25 fission-like fragments within the mass range 76 ≤ A ≤ 141, expected to be populated via fission of 220 Ra in 12 C+ 208 Pb system at E lab = 81.9 and 75.8 MeV, have been measured using offline activation analysis. The production yields of different fission-like fragments have been analyzed to generate isotopic and isobaric yield distributions. In the present work, the value of the mass dispersion parameter of fission-like fragments, σ A 2 , is found to be 2.93 and 2.65 for Antimony (Sb) at excitation energy E ⋆ = 45.4 and 39.6 MeV, and 1.24 for Indium (In) isotope at E ⋆ = 45.4 MeV. The charge dispersion parameter ( σ Z ) for Sb is estimated to be 0.769 and 0.714 at E ⋆ = 45.4 and 39.6 MeV, respectively. For In isotopes, the value of σ Z is found to be 0.430 at E ⋆ = 45.4 MeV. The values of mass and charge dispersion parameters for Sb and In isotopes show good agreement with those reported in the literature for similar systems. Further, the mass distribution of fission-like fragments is found to be fitted with a Gaussian function, except for a few fragments, indicating their production via compound nucleus fission. The mass variance ( σ M 2 ), obtained from the analysis of mass distributions, increases linearly with the compound nucleus excitation energy, indicating the fission-fragments mass spread with the excitation energy. • The cross-sections of 25 fission-like fragments within the mass range 76 ≤ A ≤ 141, expected to be populated via fission of 220Ra in the 12C+208Pb system at Elab = 81.9 and 75.8 MeV, have been measured using offline activation analysis. The production yields of different fission-like fragments have been analyzed to generate isotopic and isobaric yield distributions. • The values of mass and charge dispersion parameters for Sb and In isotopes display good agreement with the values reported in the literature for similar systems. • The mass distribution of fission-like fragments is found to be fitted with a Gaussian function, except for a few fragments, indicating their production via compound nucleus fission. The mass variance ( σ 2M ), obtained from the analysis of mass distributions, increases linearly with the compound nucleus excitation energy, indicating the fission-fragments mass spread with the excitation energy.
Approaching 100Sn: Structural evolution in 98,100Cd via lifetime measurements G. Zhang, M. Polettini, D. Mengoni, G. Benzoni, Z. Huang, M. Górska, A. Blazhev, L.M. Fraile, A. Gargano, G. De Gregorio, F. Nowacki, G. Aggez, U. Ahmed, O. Aktas, M. Al-Aqeel, B. Alayed, H.M. Albers, A. Algora, S. Alhomaidhi, F. Amjad, C. Appleton, T. Arıcı, M. Armstrong, B.Q. Arnés, A. Astier, M. Balogh, A. Banerjee, D. Bazzacco, J. Benito Garcìa, S. Bottoni, P. Boutachkov, A. Bracco, A. Bruce, D. Brugnara, C. Bruno, F. Camera, B. Cederwall, M. Cicerchia, M.M.R. Chishti, A. Corsi, M.L. Cortes, D. Cox, F.C.L. Crespi, B. Das, T. Davidson, G. de Angelis, T. Dickel, M. Doncel, A. Ertoprak, A. Esmaylzadeh, L. Gaffney, F. Galtarossa, E.R. Gamba, J. Garbe, D. Genna, J. Gerl, A. Goasduff, A. Gottardo, A. Gozzelino, T. Grahn, J. Ha, E. Haettner, O. Hall, L. Harkness-Brennan, H. Heggen, C. Hornung, Y. Hrabar, S.P. Hu, N. Hubbard, K.E. Ide, A. Illana, S. Jazrawi, P.R. John, J. Jolie, C. Jones, D. Joss, D. Judson, V. Karayonchev, E. Kazantseva, R. Kern, G.G. Kiss, L. Knafla, R. Knöbel, I. Kojouharov, A. Korgul, W. Korten, P. Koseoglou, D. Kostyleva, T. Kurtukian-Nieto, G. Kosir, N. Kurz, I. Kuti, M. Labiche, S.M. Lenzi, S. Leoni, G.-S. Li, Z. Liu, M. Llanos Expósito, R. Lozeva, J.B. Lu, M. Luoma, G. Mantovani, T. Marchi, M. Mazzocco, R. Menegazzo, T.J. Mertzimekis, M. Mikolajczuk, B. Million, A.K. Mistry, I. Mukha, E. Nacher, D.R. Napoli, B.S. Nara Singh, S.E.A. Orrigo, R.D. Page, P. Papadakis, G. Pasqualato, J. Pellumaj, S. Pelonis, R.M. Peréz Vidal, C.M. Petrache, J. Petrovic, N. Pietralla, S. Pietri, S. Pigliapoco, Zs. Podolyák, C. Porzio, A. Raggio, F. Recchia, P.H. Regan, J.M. Régis, P. Reiter, K. Rezynkina, E. Rocco, J. Rodriguez Murias, H. Rösch, P. Roy, B. Rubio, M. Rudigier, P. Ruotsalainen, E. Sahin, L.G. Sarmiento, M.-M. Satrazani, H. Schaffner, Ch. Scheidenberger, L. Sexton, A. Sharma, M. Siciliano, J. Simpson, J. Smallcombe, P. Söderström, D. Sohler, A. Sood, F. Soramel, B.-H. Sun, H.B. Sun, A. Sveiczer, N. Szegedi, Y.K. Tanaka, J.J. Valiente-Dobón, P. Vasileiou, J. Vesic, M. von Tresckow, L. Waring, H. Watanabe, H. Weick, V. Werner, J. Wiederhold, O. Wieland, K. Wimmer, H.-J. Wollersheim, P. Woods, J. Wu, A. Yaneva, I. Zanon, J. Zhao, H.Q. Zhang, G.L. Zhang, K.K. Zheng, L.H. Zhu, R. Zidarova, S. Ziliani, A. Zyriliou Physics Letters Section B Nuclear Elementary Particle and High Energy Physics, 2025 The lifetimes of low-lying excited states below the 8 + seniority isomer were directly measured using fast timing detectors in the neutron-deficient isotopes 98,100 Cd. This experiment was conducted with the DEcay SPECtroscopy (DESPEC) setup at GSI, where the ions of interest were produced via a fragmentation reaction and identified using the FRagment Separator (FRS) before being implanted in the AIDA active stopper system, and the γ rays emitted during the de-excitation of isomeric states were detected by the LaBr 3 FATIMA Array. The newly deduced values for the reduced transition probabilities were compared with shell-model calculations using different interactions and effective charges. The results indicate that, while 98 Cd aligns well with a seniority scheme description, in 100 Cd the transition strengths among low-lying states are not fully reproduced, and the nature of these states remains an open problem within the present theoretical description. Ultimately, a key element in the description of this region, crucial for nuclear physics and astrophysics, appears to be the proton-neutron term of the nuclear effective interaction.
First Identification of Excited States in Zr 78 and Implications for Isospin Nonconserving Forces in Nuclei G. L. Zimba, P. Ruotsalainen, D. G. Jenkins, W. Satuła, J. Uusitalo, R. Wadsworth, X. Pereira Lopez, K. Auranen, A. D. Briscoe, B. Cederwall, S. Chen, G. de Angelis, M. Doncel, A. Ertoprak, T. Grahn, P. T. Greenlees, A. Illana, H. Joukainen, R. Julin, H. Jutila, J. Keatings, J. Louko, M. Luoma, A. M. Plaza, J. Sarén, B. S. Nara Singh, J. Ojala, J. Pakarinen, P. Rahkila, J. Romero, A. Sood, A. Stott, C. Sullivan, H. Tann, A. Tolosa Delgado Physical Review Letters, 2025 At a fundamental level, the interactions between protons and protons, protons and neutrons, and neutrons and neutrons are not identical. Such isospin nonconserving interactions emerge when comparing the excitation energy of analog states in T=1 triplet nuclei. Here, we extend such an analysis to the A=78, T=1 triplet system-the heaviest system for which such complete data exists-and find strong disagreement with contemporary theory. This was achieved by pioneering the technique of recoil-β-β tagging to identify excited states in ^{78}Zr. We also established a ^{78}Zr half-life of 25_{-8}^{+17} ms and extended the T=1 band in ^{78}Y to J^{π}=(10^{+}).
STRUCTURE OF LOW-SPIN STATES IN45Sc STUDIED VIA COULOMB EXCITATION M. Matejska-Minda, P.J. Napiorkowski, K. Sieja, P. Bednarczyk, T. Abraham, A. Agarwal, I. Ahmed, S. Bhattacharya, R.K. Bhowmik, D.T. Doherty, S. Dutt, K. Hadyńska-Klęk, J. Iwanicki, A. Jhingan, J. Kaur, M. Kicińska-Habior, M. Kisieliński, M. Komorowska, M. Kowalczyk, M. Kumar, R. Kumar, S. Kumar, D. Kumar, A. Maj, T. Marchlewski, P. Matuszczak, V. Nanal, A. Nannini, M. Palacz, R. Palit, L. Próchniak, N.K. Rai, M. Rocchini, M. Saxena, W. Satuła, M. Shuaib, M. Siciliano, A. Sood, J. Srebrny, A. Stolarz, J. Styczeń, T. Trivedi, A.K. Tyagi, B. Wasilewska, H.J. Wollersheim, K. Wrzosek-Lipska, M. Zielińska Acta Physica Polonica B Proceedings Supplement, 2024 The electromagnetic structure of <sup>45</sup>Sc at low excitation energy was investigated via low-energy Coulomb excitation at the Heavy Ion Laboratory (HIL) of the University of Warsaw and at the Inter-University Accelerator Centre (IUAC) in New Delhi. A set of reduced E2, E3, and M1 matrix elements was extracted from the collected data using the GOSIA code. The reduced transition probability B(E2; 11/2<sup>–</sup> → 7/2<sup>–</sup>) has been determined, allowing us to deduce the lifetime of the 11/2<sup>–</sup> state at 1237 keV. In addition, the upper limit on the reduced transition probability B(E3; 7/2<sup>–</sup> → 5/2<sup>+</sup>) has been determined for the first time. Finally, new large-scale shellmodel and beyond-mean-field calculations were performed to interpret the structure of this nucleus.
Decay studies in the A ∼ 225 Po-Fr region from the DESPEC campaign at GSI in 2021 M. Polettini, J. Pellumaj, G. Benzoni, J.J. Valiente-Dobón, G. Zhang, et al. Nuovo Cimento Della Societa Italiana Di Fisica C, 2022 The HISPEC-DESPEC collaboration aims at investigating the structure of exotic nuclei formed in fragmentation reactions with decay spectroscopymeasurements, as part of the FAIR Phase-0 campaign at GSI. This paper reportson first results of an experiment performed in spring 2021, with a focus on β-decaystudies in the Po-Fr nuclei in the 220 <A< 230 island of octupole deformationexploiting the DESPEC setup. Ion-beta correlations and fast-timing techniques arebeing employed, giving an insight into this difficult-to-reach region.
The DESPEC setup for GSI and FAIR A.K. Mistry, H.M. Albers, T. Arıcı, A. Banerjee, G. Benzoni, B. Cederwall, J. Gerl, M. Górska, O. Hall, N. Hubbard, I. Kojouharov, J. Jolie, T. Martinez, Zs. Podolyák, P.H. Regan, J.L. Tain, A. Tarifeno-Saldivia, H. Schaffner, V. Werner, G. Ağgez, J. Agramunt, U. Ahmed, O. Aktas, V. Alcayne, A. Algora, S. Alhomaidhi, F. Amjad, C. Appleton, M. Armstrong, M. Balogh, K. Banerjee, P. Bednarczyk, J. Benito, C. Bhattacharya, P. Black, A. Blazhev, S. Bottoni, P. Boutachkov, A. Bracco, A.M. Bruce, M. Brunet, C.G. Bruno, I. Burrows, F. Calvino, R.L. Canavan, D. Cano-Ott, M.M.R. Chishti, P. Coleman-Smith, M.L. Cortés, G. Cortes, F. Crespi, B. Das, T. Davinson, A. De Blas, T. Dickel, M. Doncel, A. Ertoprak, A. Esmaylzadeh, B. Fornal, L.M. Fraile, F. Galtarossa, A. Gottardo, V. Guadilla, J. Ha, E. Haettner, G. Häfner, H. Heggen, P. Herrmann, C. Hornung, S. Jazrawi, P.R. John, A. Jokinen, C.E. Jones, D. Kahl, V. Karayonchev, E. Kazantseva, R. Kern, L. Knafla, R. Knöbel, P. Koseoglou, G. Kosir, D. Kostyleva, N. Kurz, N. Kuzminchuk, M. Labiche, J. Lawson, I. Lazarus, S.M. Lenzi, S. Leoni, M. Llanos-Expósito, R. Lozeva, A. Maj, J.K. Meena, E. Mendoza, R. Menegazzo, D. Mengoni, T.J. Mertzimekis, M. Mikolajczuk, B. Million, N. Mont-Geli, A.I. Morales, P. Morral, I. Mukha, J.R. Murias, E. Nacher, P. Napiralla, D.R. Napoli, B.S. Nara-Singh, D. O’Donnell, S.E.A. Orrigo, R.D. Page, R. Palit, M. Pallas, J. Pellumaj, S. Pelonis, H. Pentilla, A. Pérez de Rada, R.M. Pérez-Vidal, C.M. Petrache, N. Pietralla, S. Pietri, S. Pigliapoco, J. Plaza, M. Polettini, C. Porzio, V.F.E. Pucknell, F. Recchia, P. Reiter, K. Rezynkina, S. Rinta-Antila, E. Rocco, H.A. Rösch, P. Roy, B. Rubio, M. Rudigier, P. Ruotsalainen, S. Saha, E. Şahin, Ch. Scheidenberger, D.A. Seddon, L. Sexton, A. Sharma, M. Si, J. Simpson, A. Smith, R. Smith, P.A. Söderström, A. Sood, A. Soylu, Y.K. Tanaka, J.J. Valiente-Dobón, P. Vasileiou, J. Vasiljevic, J. Vesic, D. Villamarin, H. Weick, M. Wiebusch, J. Wiederhold, O. Wieland, H.J. Wollersheim, P.J. Woods, A. Yaneva, I. Zanon, G. Zhang, J. Zhao, R. Zidarova, G. Zimba, A. Zyriliou Nuclear Instruments and Methods in Physics Research Section A Accelerators Spectrometers Detectors and Associated Equipment, 2022
Role of precursor nuclei in heavy-ion induced reactions at low energies Ishfaq Majeed Bhat, Mohd. Shuaib, M. Shariq Asnain, Manoj Kumar Sharma, Abhishek Yadav, Vijay R. Sharma, Pushpendra P. Singh, Devendra P. Singh, Sunita Gupta, Unnati Gupta, Rudra N. Sahoo, Arshiya Sood, Malika Kaushik, Sushil Kumar, R. Kumar, B. P. Singh, R. Prasad Physical Review C, 2022 In heavy-ion induced reactions, generally, a large number of residues are populated through different reaction channels. In some cases the same residue is populated via two different modes viz., (i) directly from a given reaction and (ii) via $\ensuremath{\beta}$ and/or electron capture decay of a nuclide (precursor). Separation of the two is required for a better understanding of reaction dynamics. The procedure existing in the literature for extracting the independent production cross section from the cumulative cross section employs the assumptions of half-life of the daughter being much larger in comparison to the half-life of the precursor $({t}_{1/2}^{p}\ensuremath{\ll}{t}_{1/2}^{d})$ and require the counting to be performed after large cooling times $({t}_{l}\ensuremath{\rightarrow}\ensuremath{\infty})$. A general and more exact expression is obtained in the present work surpassing the assumptions as well as difficulties reported earlier. Analysis of the experimental reaction data sets covering a broader range of possibilities $({t}_{1/2}^{p}>{t}_{1/2}^{d}$; ${t}_{1/2}^{p}\ensuremath{\approx}{t}_{1/2}^{d};$ ${t}_{1/2}^{p}<{t}_{1/2}^{d})$ presented shows the importance of the current formulations. The advantage of the generalized expression even when the assumptions hold true is also discussed. A comparison of results obtained from the traditional method in the context of its assumptions instead of the calculations from the exact expression has been made. The results obtained with the presently derived formulations are found to give justified values of cross sections for all the cases in contrast to the traditional formulation.
Effect of non- α -cluster projectile on incomplete-fusion dynamics: Experimental study of the N 14 + Ta 181 system M. Shariq Asnain, Mohd. Shuaib, Ishfaq Majeed, Manoj Kumar Sharma, Vijay R. Sharma, Abhishek Yadav, Devendra P. Singh, Pushpendra P. Singh, Unnati Gupta, Rudra N. Sahoo, Arshiya Sood, Malika Kaushik, Sushil Kumar, R. Kumar, B. P. Singh, R. Prasad Physical Review C, 2021 In order to study incomplete fusion (ICF) reaction dynamics, the present work manifests the role of a non-$\ensuremath{\alpha}$-cluster $^{14}\mathrm{N}$ projectile on $^{181}\mathrm{Ta}$ target at energies $\ensuremath{\approx}4--7$ MeV/nucleon using the offline $\ensuremath{\gamma}$-ray spectroscopy. The excitation functions for 15 reaction residues populated in $^{14}\mathrm{N}+^{181}\mathrm{Ta}$ system have been measured and analyzed within the framework of statistical model code PACE4. The experimentally measured excitation functions of evaporation residues populated via xn/pxn channels are found to be well reproduced by the predictions of code PACE4, which confirms their production solely via complete fusion process. However, an enhancement in the measured excitation function as compared to PACE4 calculations, particularly in tail portion of $^{192}\mathrm{Hg}$ residue ($3n$ channel) has been observed indicating the presence of precompound emission. A significant contribution from precursor decay in pxn channels has also been observed. An enhancement in the measured excitation functions for $\ensuremath{\alpha}$-emitting channels as compared to the PACE4 predictions has been observed and attributed to the incomplete fusion process. Further, the contribution from incomplete fusion process in the $^{14}\mathrm{N}+^{181}\mathrm{Ta}$ system has also been deduced in terms of strength function (${F}_{\mathrm{ICF}}$). The results have been discussed in terms of the parameters which influence the dynamics of ICF process. The ${F}_{\mathrm{ICF}}$ is found to depend strongly on projectile energies, the product of projectile and target charges, and $\ensuremath{\alpha}\ensuremath{-}Q$ value of the projectile.
Disentangling complete and incomplete fusion events in 12C + 169Tm reaction by spin-distribution measurements Arshiya Sood, Swati Thakur, Arzoo Sharma, Vijay R Sharma, Abhishek Yadav, Manoj K Sharma, B P Singh, R Kumar, R K Bhowmik, Pushpendra P Singh Journal of Physics G Nuclear and Particle Physics, 2021 The spin-distributions of different reaction products populated via x n and α/2αx n channels in C 12 + Tm 169 system have been measured at E lab ≈ 6, 7 and 7.5 MeV A−1 to disentangle complete and incomplete fusion events. Particle (p, α)-γ-coincidences were recorded to identify evaporation residues channel-by-channel. The spin-distributions of fusion evaporation and direct-α-emitting channels are found to be distinct corroborating the involvement of entirely different reaction dynamics in their production, respectively termed as complete (CF) and incomplete fusion (ICF). The values of mean input angular momenta, obtained from the analysis of the spin-distributions, involved in ICF-α/2α xn channels are estimated to be larger than that observed in CF-xn/α xn channels. For ICF-α/2αxn channels, the multiplicity of fast-α particle emission increases with the magnitude of input angular momentum imparted into the system. The CF residues display a population of broad spin range while the ICF residues are confined to a narrow spin range generally localized in the higher spin states. Findings of the present work conclusively demonstrate the possibility to populate high spin states in final reaction products using ICF, which are otherwise not accessible. Further, an attempt has been made to study the variation of input angular momentum with the choice of different entrance-channel parameters. It has been observed that the value of input angular momentum involved in ICF-α/2α xn channels increases with the deformation and entrance-channel mass-asymmetry parameter, indicating strong entrance-channel dependence of ICF dynamics.
Role of neutron transfer in sub-barrier fusion Rudra N. Sahoo, Malika Kaushik, Arshiya Sood, Arzoo Sharma, Swati Thakur, Pawan Kumar, Md. Moin Shaikh, Rohan Biswas, Abhishek Yadav, Manoj K. Sharma, J. Gehlot, S. Nath, N. Madhavan, R. G. Pillay, E. M. Kozulin, G. N. Knyazheva, K. V. Novikov, Pushpendra P. Singh Physical Review C, 2020
Evidence of narrow range high spin population in incomplete fusion Arshiya Sood, Pawan Kumar, R.N. Sahoo, Pushpendra P. Singh, Abhishek Yadav, Vijay R. Sharma, Manoj K. Sharma, R. Kumar, R.P. Singh, S. Muralithar, B.P. Singh, R.K. Bhowmik Acta Physica Polonica B, 2020
Revised lifetime of the 11/2- state in 45Sc via coulomb excitation M. Matejska-Minda, P.J. Napiorkowski, R. Kumar, M. Saxena, S. Dutt, A. Agarwal, I. Ahmed, S. Bhattacharya, A. Jhingan, J. Kaur, M. Kicińska-Habior, M. Kumar, S. Kumar, D. Kumar, V. Nanal, R. Palit, N.K. Rai, M. Shuaib, A. Sood, A. Stolarz, T. Trivedi, A.K. Tyagi, R.K. Bhowmik, H.J. Wollersheim Acta Physica Polonica B, 2020
Fabrication of thin 130Te target foils for sub-barrier fusion studies Rudra N. Sahoo, G. Naga Jyothi, Arshiya Sood, S.R. Abhilash, G.R. Umapathy, D. Kabiraj, Sunil Ojha, P.V. Madhusudhan Rao, Pushpendra P. Singh Nuclear Instruments and Methods in Physics Research Section A Accelerators Spectrometers Detectors and Associated Equipment, 2019
Insights into the low energy incomplete fusion Rudra N. Sahoo, Malika Kaushik, Arshiya Sood, Pawan Kumar, Vijay R. Sharma, Abhishek Yadav, Pushpendra P. Singh, Manoj K. Sharma, R. Kumar, B. P. Singh, S. Aydin, R. Prasad Nuclear Physics A, 2019
Investigation of an intruder band in 45 Sc via coulomb excitation ∗ M. Matejska-Minda, R. Kumar, P.J. Napiorkowski, M. Saxena, S. Dutt, A. Agarwal, I. Ahmed, S. Bhattacharya, A. Jhingan, J. Kaur, M. Kicińska-Habior, M. Kumar, S. Kumar, D. Kumar, V. Nanal, R. Palit, N.K. Rai, M. Shuaib, A. Sood, A. Stolarz, T. Trivedi, A.K. Tyagi, R.K. Bhowmik, H.J. Wollersheim Acta Physica Polonica B, 2019
Sub-barrier fusion in the Cl 37 + Te 130 system Rudra N. Sahoo, Malika Kaushik, Arshiya Sood, Pawan Kumar, Arzoo Sharma, Swati Thakur, Pushpendra P. Singh, P. K. Raina, Md. Moin Shaikh, Rohan Biswas, Abhishek Yadav, J. Gehlot, S. Nath, N. Madhavan, V. Srivastava, Manoj K. Sharma, B. P. Singh, R. Prasad, Anjali Rani, A. Banerjee, Unnati Gupta, Nabendu K. Deb, B. J. Roy Physical Review C, 2019
Entrance channel effect on incomplete fusion R.N. Sahoo, M. Kaushik, A. Sood, P. Kumar, V.R. Sharma, A. Yadav, M. Shuaib, D.P. Singh, P.P. Singh, U. Gupta, M.K. Sharma, R. Kumar, B.P. Singh, S. Aydin, H.J. Wollersheim, R. Prasad Acta Physica Polonica B, 2018
Fission-like events in the C 12 + Tm 169 system at low excitation energies Arshiya Sood, Pushpendra P. Singh, Rudra N. Sahoo, Pawan Kumar, Abhishek Yadav, Vijay R. Sharma, Mohd. Shuaib, Manoj K. Sharma, Devendra P. Singh, Unnati Gupta, R. Kumar, S. Aydin, B. P. Singh, H. J. Wollersheim, R. Prasad Physical Review C, 2017
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Sub-barrier fusion in the system RN Sahoo, M Kaushik, A Sood, P Kumar, A Sharma, S Thakur, PP Singh, ... Physical Review C 99 (2), 024607 , 2019 2019 Citations: 35
Role of neutron transfer in sub-barrier fusion RN Sahoo, M Kaushik, A Sood, A Sharma, S Thakur, P Kumar, ... Physical Review C 102 (2), 024615 , 2020 2020 Citations: 32
Fission-like events in the system at low excitation energies A Sood, PP Singh, RN Sahoo, P Kumar, A Yadav, VR Sharma, M Shuaib, ... Physical Review C 96 (1), 014620 , 2017 2017 Citations: 28
Effect of non- -cluster projectile on incomplete-fusion dynamics: Experimental study of the system MS Asnain, M Shuaib, I Majeed, MK Sharma, VR Sharma, A Yadav, ... Physical Review C 104 (3), 034616 , 2021 2021 Citations: 25
Fabrication of thin 130Te target foils for sub-barrier fusion studies RN Sahoo, GN Jyothi, A Sood, SR Abhilash, GR Umapathy, D Kabiraj, ... Nuclear Instruments and Methods in Physics Research Section A: Accelerators … , 2019 2019 Citations: 19
Effect of projectile structure on break-up fusion for 14N+ 175Lu system at intermediate energies IM Bhat, M Shuaib, MS Asnain, VR Sharma, A Yadav, MK Sharma, ... Nuclear Physics A 1021, 122421 , 2022 2022 Citations: 14
Self-supporting thin Tin targets fabricated by ultra-high vacuum evaporation for heavy-ion induced reactions PP Arshiya Sood, G. R. Umapathy, Arzoo Sharma, Abhilash S.R., S. Ojha, D ... Vacuum , 2019 2019 Citations: 13
Insights into the low energy incomplete fusion RN Sahoo, M Kaushik, A Sood, P Kumar, VR Sharma, A Yadav, PP Singh, ... Nuclear Physics A 983, 145-165 , 2019 2019 Citations: 11
Role of precursor nuclei in heavy-ion induced reactions at low energies IM Bhat, M Shuaib, MS Asnain, MK Sharma, A Yadav, VR Sharma, ... Physical Review C 105 (5), 054607 , 2022 2022 Citations: 10
First Identification of Excited States in and Implications for Isospin Nonconserving Forces in Nuclei GL Zimba, P Ruotsalainen, DG Jenkins, W Satuła, J Uusitalo, ... Physical Review Letters 134 (2), 022502 , 2025 2025 Citations: 5
Isomeric Lifetime Measurement in the Neutron-rich 189 Ta S Alhomaidhi, E Sahin, V Werner, J Jolie, P Regan, N Pietralla, J Gerl, ... EPJ Web of Conferences 290, 02007 , 2023 2023 Citations: 3
Disentangling complete and incomplete fusion events in 12 C + 169 Tm reaction by spin-distribution measurements A Sood, S Thakur, A Sharma, VR Sharma, A Yadav, MK Sharma, ... Journal of Physics G: Nuclear and Particle Physics 48 (2), 025105 , 2021 2021 Citations: 3
REVISED LIFETIME OF THE 11/2 - STATE IN 45 Sc VIA COULOMB EXCITATION. M Matejska-Minda, PJ Napiorkowski, R Kumar, M Saxena, S Dutt, ... Acta Physica Polonica B 51 (3) , 2020 2020 Citations: 3
Decay studies in the A∼ 225 Po-Fr region from the DESPEC campaign at GSI in 2021 M Polettini, J Pellumaj, G Benzoni, G Zhang, D Mengoni, RMP Vidal, ... Il Nuovo Cimento C , 2022 2022 Citations: 2
ENTRANCE CHANNEL EFFECTS ON FISSION FRAGMENT MASS DISTRIBUTION IN 12 C+ 169 Tm SYSTEM. A Sood, P Kumar, RN Sahoo, PP Singh, A Yadav, VR Sharma, ... Acta Physica Polonica B 50 (3) , 2019 2019 Citations: 1
Effect of target neutron skin thickness on incomplete fusion probability RN Sahoo, M Kaushik, A Sood, P Kumar, M Shuaib, VR Sharma, A Yadav, ... Proceedings of the DAE Symp. on Nucl. Phys 62, 586 , 2017 2017 Citations: 1
Entrance Channel Effect on Incomplete Fusion RN Sahoo, M Kaushik, A Sood, P Kumar, VR Sharma, A Yadav, M Shuaib, ... 2017 Citations: 1
Understanding the reaction dynamics of 16O+165Ho interactions using the quasi-elastic barrier distribution G Ram, A Yadav, MM Shaikh, A Jhingan, M Kumar, N Saneesh, I Bala, ... Proceedings of the DAE Symp. on Nucl. Phys 66, 557 , 2022 2022
Effect of the target structure on the quasi-elastic barrier distribution A Yadav, G Ram, MM Shaikh, A Jhingan, M Kumar, N Saneesh, I Bala, ... Proceedings of the DAE Symp. on Nucl. Phys 66, 555 , 2022 2022
