WHAT IS NEW IN ATOMIC MASS DETERMINATIONS? Aaldert H. Wapstra and Georges Audi Atomic mass determinations with Penning traps have considerably improved the precision in our knowledge of the masses of fundamentally important atoms like the three lightest hydrogens and the two lightest heliums. A new determination of the capture gamma ray leading to deuterium then also leads to an improved mass value for the neutron. And the recent evaluation of natural constants now allows to express the corresponding mass excess values, both in mass units and in electronvolts, essentially without loss of precision. This is even true for some heavier nuclides (e. g. 23Na, 86Rb??, 133Cs) for which Penning trap measurements also have yielded very precise mass values. Unfortunately, though, measurements intended to solve the 20 years old 20 keV uncertainty (compared to a suggested precision of less than 2 keV) in the masses of the mercury isotopes did not yet yield a convincing answer. Using the new data, we checked and, where necessary, improved all reported reaction energies for (n,gamma), (p,gamma) and (p,n) reactions. In some cases, this lead to removal of earlier discrepancies - but also new ones appeared, requiring further study. Continuation of the Mainz Penning trap work yielded about 10 keV precise mass values for many proton-rich nuclides of Xe isotopes and ones around 146Gd. In addition, Darmstadt measurements of frequency spectra in the big storage ring have yielded many, partly only slightly less precise values for proton-rich nuclides in the region A=100-200. Combination with measurements of decay energies in (series of successive) alpha decays (several made in Jyvaskula), this led to many more mass values. Thus, interesting information has been obtained on the course of the poton separation energies around and just above the proton drip line. Even more information on that subject arose from the continued measurements of nuclides decaying both by proton and alpha particle emission. Such measurements also yielded much information on the occurenece of isomers. We also looked at the resulting new information on the neutron pairing energies in proton-rich Hg and Pb nuclei. The Jensen-Hansen-Jonson estimate is decidedly better than the earlier formula (12 MeV)/$A sup half$. Several Mainz and Darmstadt measurements only yielded an average value for the mass of isomeric pairs, or even triplets, with half-lives comparable with the measuring times, nowadays one or a few seconds but may be less in the future. For this reason, among others, we partook in constructing a file NUBASE with data on isomers with a half-life above one milliescond. We consider to keep it yup to date, to lower the limit to 100 ns, and to keep it available om internet. Extremely interesting are the newly reported results on very heavy nuclides, up to Z=118. Though there are doubts about the validity of some of those reports, we intend to accept them provisionally for our atomic mass calculations as long as not proven wrong. We continue our habit to estimate mass values for nuclides for which no sufficient data are avauilable. For proton-rich nuclides in the region A<100, we make use of estimates from the isobaric multuiplet mass eqaution when possible; for A>230 systematics of relative energies of Nilsson levels.