Nuclear Mass Segment

Experimental mass excesses

Experimental mass excesses evaluated by Audi and Wapstra [1] are included along with the FRDM and HFB results below.

References
[1] G. Audi and A. H. Wapstra (1995) Nucl. Phys. A595, 409.

FRDM

Ground state properties calculated within the Finite Range Droplet Model (FRDM) [1].

References
[1] P. Moller, J. R. Nix, W. D. Myers, W. J. Swiatecki (1995) At. Data and Nucl. Data Tables 59, 185.

Data File (689kB)
README File (3.3kB)

HFB

Ground state properties calculated within the Hartree-Fock-Bogolubov (HFB) method [1-3].

References
[1] M. Samyn, S. Goriely, J. M. Pearson, (2002) Phys. Rev. C submitted
[2] M. Samyn, S. Goriely, P. -H. Heenen, J. M. Pearson and F. Tondeur (2002) Nucl. Phys. A, in press.
[3] E. Nadjakov, K. Marinova and Y. Gangrsky (1994) Atomic Data and Nucl. Data Tables 56, 134.

Data File (966kB)
README File (4.4kB)

Duflo-Zuker96

FORTRAN code for estimating nuclear masses with the 10 parameter formula of J. Duflo and A.P. Zuker [1,2].

References
[1] J. Duflo and A. P. Zuker (1995) Phys. Rev. C52, 23.
[2] J. Duflo and A. P. Zuker (1996) at http://csn-srv3.in2p3.fr/AMDC/theory/du_zu_10.feb96fort

Code (12kB)
README File (1.6kB)

Natural Abundances

Reformatted data from the Nuclear Wallet cards, as retrieved from Brookhaven National Laboratory.

Data File (9.5kB)
README File (0.9kB)

Retrieval of Mass Excesses and Natural Abundances

Atomic number (Z) Mass number (A) (blank for all)

Ground-state Deformations

328 experimental deformation parameters beta2 derived from the model-independent experimental values of the reduced electric quadrupole transition probability B(E2) [1,2].

References
[1] S. Raman, C.H. Malarkey, W.T. Milner, C.W. Nestor, J.R. and P.H. Stelson (1987), At. Data Nucl. Data Tables 36, 1.
[2] S. Raman, C.W. Nestor, JR. and P. Tikkanen (2001), At. Data Nucl. Data Tables 78, 1.

Data File (9.6kB)
README File (1.6kB)

Retrieval of Ground-state Deformations

Atomic number (Z) Mass number (A) (blank for all)

Nuclear Matter Densities

Neutron and proton distributions predicted within the Hartree-Fock-Bogolubov (HFB) method based on the BSk2 Skyrme force [1-4].

References
[1] M. Samyn, S. Goriely, J. M. Pearson, (2002) Phys. Rev. C submitted.
[2] M. Samyn, S. Goriely, P. -H. Heenen, J. M. Pearson and F. Tondeur (2002) Nucl. Phys. A, in press.
[3] G. Audi and A. H. Wapstra (1995) Nucl. Phys. A595, 409.
[4] E. Nadjakov, K. Marinova and Y. Gangrsky (1994) Atomic Data and Nucl. Data Tables 56, 134.

README File (2.8kB)

Retrieval of Nuclear Matter Densities

Atomic number (Z) Mass number (A)

Q-value calculation

Set atomic (Z) and mass (A) numbers for target and projectile and specify number of emitted particles

ZA
Target Nuclide
Projectile
Emitted Particles number of particles
neutrons
protons
deuterons
tritons
He-3
alphas