117 results on '"Shirikova, N. Yu."'
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2. Prediction of the excitation energies of the 2$^+_1$ states for superheavy nuclei based on the microscopically derived Grodzins relation
3. Fine Structure of the Isovector Giant Dipole Resonance in $^{142-150}$Nd and $^{152}$Sm
4. Microscopically Derived Grodzins Relation and Prediction of the Excitation Energies of the \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$2_{1}^{ + }$$\end{document} States for Some Superheavy Nuclei
5. Triplet structure of nuclear scissors mode
6. Spectroscopy of 230Th in the (p,t) reaction
7. On neutron number dependence of B(E1;0+ --> 1-) reduced transition probability
8. Q-phonon description of low lying 1^- two-phonon states in spherical nuclei
9. Microscopically Derived Grodzins Relation and Prediction of the Excitation Energies of the $$2_{1}^{ + }$$ States for Some Superheavy Nuclei
10. Coriolis mixing of the K = 1 and K = 0 mixed symmetry states in the well deformed even–even nuclei
11. Spin-isospin structure of the nuclear scissors mode
12. Structure of the low-lying states of the odd-neutron nuclei with Z ≈ 100
13. Prediction of the excitation energies of the 21+ states for superheavy nuclei based on the microscopically derived Grodzins relation
14. Low-Lying Vibrational States in Deformed Nuclei
15. Relation between the mass coefficients for rotational and γ-vibrational modes in well-deformed nuclei
16. Fine structure of the isovector giant dipole resonance in Nd142-150 and Sm-152
17. E0 transitional density for nuclei between spherical and deformed shapes
18. High-resolution study of 0+ and 2+ excitations in 168Er with the (p, t) reaction
19. Fine structure of the isovector giant dipole resonance in Nd142–150 and Sm152
20. Gamma deexcitation of the 180m Ta isomer
21. Structure of Superheavy Nuclei
22. Dipole γ-ray transition rates in 238U
23. Excitation energy dependence of the moments of inertia of well deformed nuclei
24. Low-Lying Vibrational States in Deformed Nuclei
25. SOME RESULTS ON THE STRUCTURE OF SUPERHEAVY NUCLEI
26. Quasiparticle structure of superheavy nuclei in α -decay chains of 285 Fl and 291,293 Lv
27. Description of low-lying vibrationalK π≠0+ states of deformed nuclei in the quasiparticle-phonon nuclear model
28. On collective two-phonon states in deformed nuclei
29. Description of charge-exchange resonances in deformed nuclei
30. Application of Sturm-Liouville functions to the solution of the Schrödinger equation with an anisotropic saxon-woods potential
31. Relation between the mass coefficients for rotational and γ-vibrational motion in axially symmetric deformed nuclei
32. Low-lying excited states of the odd-proton nuclei withZ≈100
33. ISOMERIC STATES AND COLLECTIVE EXCITATIONS OF HEAVIEST NUCLEI
34. Relation Between the Mass Coefficients for Rotational and γ-Vibrational Modes in Well-Deformed Nuclei
35. Structure of some low lying two-quasiparticle and collective states in nuclei withZ∼ 100 considered in the quasiparticle phonon model
36. Schematic microscopic approach to the description ofM1transitions between mixed-symmetry and fully symmetric collective states inγ-soft nuclei based on RPA-IBM boson mapping
37. Spectroscopy ofTh230in the(p,t)reaction
38. LOW-LYING 0+ STATES IN DEFORMED NUCLEI
39. Q-PHONON APPROACH FOR LOW-LYING 1− TWO-PHONON STATES IN SPHERICAL NUCLEI
40. On neutron number dependence of B(E1;0+ 1 → 1- 1) reduced transition probability
41. High-resolution study of 0+and 2+excitations inEr168with the (p,t) reaction
42. Microscopic structure of low-lying0+states in deformed nuclei
43. GAMMA TRANSITIONS BETWEEN CONFIGURATIONS “QUASIPARTICLE ⊗ PHONON”
44. MICROSCOPIC STUDY OF LOW-LYING 0+ STATES IN DEFORMED NUCLEI
45. LOW-LYING 0+ STATES IN DEFORMED NUCLEI.
46. Q-PHONON APPROACH FOR LOW-LYING 1- TWO-PHONON STATES IN SPHERICAL NUCLEI.
47. MICROSCOPIC STUDY OF LOW-LYING 0+ STATES IN DEFORMED NUCLEI.
48. 76-Osmium.
49. 75-Rhenium.
50. 74-Tungsten.
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