Probing the critical behavior in the evolution of GDR width at very low temperatures in A∼100 mass region

[1]  D. Mondal,et al.  Giant dipole resonance width and the universality of a fluctuation model including critical temperature , 2013 .

[2]  I. Mukul,et al.  Effect of angular momentum on giant dipole resonance observables in the 28 Si+ 116 Cd reaction , 2013 .

[3]  D. Mondal,et al.  Giant dipole resonance width as a probe for nuclear deformation at finite excitation , 2013, 1305.3360.

[4]  H. Pai,et al.  Angular-momentum-gated light-particle evaporation spectra from 97 Tc * and 62 Zn * systems , 2012 .

[5]  N. D. Dang,et al.  Giant dipole resonance in 201 Tl at low temperature , 2012, 1210.5011.

[6]  N. D. Dang.  Damping of giant dipole resonances in hot rotating nuclei , 2012, 1206.3361.

[7]  S. Mukhopadhyay,et al.  Critical behavior in the variation of GDR width at low temperature , 2012, 1206.2719.

[8]  J. K. Meena,et al.  Measurement of giant dipole resonance width at low temperature: A new experimental perspective , 2011, 1112.0441.

[9]  S. Mukhopadhyay,et al.  A realistic technique for selection of angular momenta from hot nuclei: A case study with 4He + 115In → 119Sb* at ELab = 35 MeV , 2010, 1009.3344.

[10]  D. Gupta,et al.  Extreme nuclear shapes examined via giant dipole resonance lineshapes in hot light-mass systems , 2010, 1006.0557.

[11]  R. G. Pillay,et al.  Inhomogeneous and intrinsic damping of giant dipole resonance in hot rotating nuclei with A ~ 150 , 2010 .

[12]  S. Mukhopadhyay,et al.  Coherent bremsstrahlung and GDR width from 252Cf cold fission , 2009, 0912.4578.

[13]  J. K. Meena,et al.  Variation of neutron detection characteristics with dimension of BC501A neutron detector , 2009 .

[14]  E. Grosse,et al.  Photon data shed new light upon the GDR spreading width in heavy nuclei , 2008, 0810.2268.

[15]  S. Mukhopadhyay,et al.  Scaling of the giant dipole resonance widths in hot rotating nuclei from the ground state values , 2008, 0809.4161.

[16]  D. Gupta,et al.  Giant dipole resonance width in nuclei near Sn at low temperature and high angular momentum , 2008, 0801.3882.

[17]  A. Nannini,et al.  Giant dipole resonance in the hot and thermalized 132Ce nucleus: damping of collective modes at finite temperature. , 2006, Physical review letters.

[18]  D. Curien,et al.  Evidence for the Jacobi shape transition in hot 46Ti , 2004 .

[19]  B. Back,et al.  Radiative fusion from very symmetric reactions: the giant dipole resonance in the 179Au nucleus , 2003 .

[20]  T. Nakamura,et al.  Low-temperature measurement of the giant dipole resonance width , 2003 .

[21]  A. Woude,et al.  Giant Resonances: Fundamental High-Frequency Modes of Nuclear Excitation , 2001 .

[22]  J. Bearden,et al.  Probing the Shape of Hot 194Hg at High Spins With the Giant Dipole Resonance Decay in Selected Cascades , 1999 .

[23]  A. Arima,et al.  Temperature dependence of quantal and thermal dampings of the hot giant dipole resonance , 1998 .

[24]  Y. Alhassid,et al.  Scaling Properties of the Giant Dipole Resonance Width in Hot Rotating Nuclei , 1998, nucl-th/9807012.

[25]  A. Arima,et al.  QUANTAL AND THERMAL DAMPINGS OF GIANT DIPOLE RESONANCES IN 90ZR, 120SN, AND 208PB , 1998 .

[26]  Broglia,et al.  Temperature Dependence of the Width of the Giant Dipole Resonance in 120Sn and 208Pb. , 1996, Physical review letters.

[27]  T. Tveter,et al.  Thermal fluctuation and collisional damping effects in the GDR observables in hot rotating 176W nuclei , 1995 .

[28]  Kaplan,et al.  Spin-induced shape changes in light-medium mass compound nuclei. , 1995, Physical review. C, Nuclear physics.

[29]  Tveter,et al.  Increase in width of the giant dipole resonance in hot nuclei: Shape change or collisional damping? , 1995, Physical review letters.

[30]  W. Myers,et al.  Nuclear ground state masses and deformations , 1993, nucl-th/9308022.

[31]  J. Gaardhøje.  Nuclear Structure at High Excitation Energy Studied with Giant Resonances , 1992 .

[32]  A. Goodman.  Thermal shape fluctuations in hot rotating nuclei: Comparison of constant energy constraint and constant temperature constraint , 1991 .

[33]  H. Nifenecker,et al.  High Energy Photon Production in Nuclear Reactions , 1990 .

[34]  Levit,et al.  Thermal shape fluctuations, Landau theory, and giant dipole resonances in hot rotating nuclei. , 1988, Physical review letters.

[35]  Pacheco,et al.  Fluctuations in the shape transitions of hot nuclei. , 1988, Physical review letters.

[36]  R. Broglia,et al.  Role of thermal fluctuations in the damping of the giant dipole resonance of spherical and deformed nuclei: 90Zr and 164Er , 1987 .

[37]  M. Brack,et al.  The Strutinsky method and its foundation from the Hartree-Fock-Bogoliubov approximation at finite temperature , 1981 .

[38]  F. Pühlhofer.  On the interpretation of evaporation residue mass distributions in heavy-ion induced fusion reactions , 1977 .

[39]  H. Beil,et al.  A semi-phenomenological description of the giant dipole resonance width , 1974 .

[40]  V. Strutinsky,et al.  “Shells” in deformed nuclei , 1968 .

[41]  V. Strutinsky,et al.  Shell effects in nuclear masses and deformation energies , 1967 .