However the total number of spins must be small as the τ0 obtained from the dynamical scaling is atomic-like (∼ 10−13 s).
The nanoscale phase separation in hole-doped manganites
The RD of each of the fully relaxed structures was obtained by counting the number of atoms within bins of 10−3˚A, up to the ﬁfth coordination shell.
Thermodynamic properties of binary HCP solution phases from special quasirandom structures
Equation (10) predicts that α 6= 0 due to contributions from the Coulomb and surface terms, whose relevance increases as the differences between the mass and/or the atomic numbers of the sources become larger.
Temperature effects in the nuclear isoscaling
AM U is the atomic mass number of the species from which we measure the observed line width ∆V , and ∆Vth is the expected thermal line width for that species, assuming a temperature of 10 K.
Spitzer and HHT observations of starless cores: masses and environments
Here, the same ion is used for all data points. (The micromotion of the ion was compensated to about 10 mK for these measurements.) The atom number reaches a minimum when the dipole trap is centered onto the ion.
An apparatus for immersing trapped ions into an ultracold gas of neutral atoms