The non-perturbative nature of quantum chromodynamics (QCD) has historically left a gap in our understanding of the connection between the fundamental theory of the strong interactions and the rich structure of experimentally observed phenomena. For the simplest properties of stable hadrons, this is now circumvented by using lattice QCD. In this talk I discuss a path that will allow us to access a variety of previously unexplored sectors of QCD. As a proof of principle, I will focus my attention to the isoscalar mesonic sector of QCD. Carrying the quantum numbers of the vacuum, this is perhaps one the most interesting channels in hadronic physics. Beyond playing a crucial role in a range of phenomenologically important processes, it hosts some of the most intriguing states of QCD. For example, glueballs, which have long been upheld as a smoking gun of the low-energy validity of QCD, are expected to appear in this channel.

Faddeev equations in momentum space have a long tradition of utilizing separable interactions in order to arrive at sets of coupled integral equations in one variable. However, it needs to be demonstrated that their solution based on separable interactions agrees exactly with solutions based on non-separable forces. I will discuss calculations of the 6 Li ground state via momentum space Faddeev equations using the CD-Bonn neutron-proton force and a Woods- Saxon type neutron(proton)- 4 He force. For the latter the Pauli-forbidden s-wave bound state is projected out. Two methods for evaluating the 6 Li three-body ground state are considered. First, we solve the bound state Faddeev equations directly using the afore-mentioned two-body potentials. In the second approach, the interactions in the two-body subsystems are represented by separable interactions derived in the Ernst-Shakin-Thaler (EST) framework. We find that by utilizing the full parameter space of the EST separable expansion, one can attain a precision of upto four significant figures in three-body binding energy. It is also shown that the three-body binding energy computed in this manner agrees fully with the one obtained directly within the stated numerical precision. The momentum distributions computed in both approaches also fully agree with each other.

The Active Target and Time Projection Chamber (ACTAR TPC) is an ambitious European project whose goal is to design and construct a high-luminosity gas-filled detector to study reactions and decays of rare isotopes. The core detection system will consist of one (or possibly several) micro-pattern gaseous detectors (MPGDs) coupled to a highly pixelated pad plane with a pitch of only 2x2 mm2. Both the channel density (25 channels/cm2) and total number of electronics channels (16384) are the highest that have been achieved by any nuclear physics detector to date. In this presentation I will provide an overview of the project, discuss the principal challenges associated with constructing such a device and present the day one physics programs for ACTAR TPC when it goes online at the GANIL laboratory in France in 2018.

The era of FRIB will further clarify that one can never unambiguously extract structure information without a proper reaction description when strongly interacting probes are involved. An outline of an ambitious plan to tackle this issue in a consistent manner will be presented with emphasis on the dispersive optical model (DOM) that treats the structure and reaction domain simultaneously at least for single proton or neutron propagation. Apart from upgrading this framework to include nonlocality of the potentials and the treatment of pairing open-shell nuclei, attention will be given to an extension of this approach involving the deuteron in the initial or final state. A fresh analysis of the (e,e’p) reaction indicates that a consistent approach is indeed possible. Predictive features of the DOM include the neutron skin with results for 48Ca and (preliminary) 208Pb. The efficacy of this approach is further illustrated by considering the current state of the art of the (d,p) and (p,d) reaction. Additional insights into where binding is generated in the nucleus are discussed with future applications to asymmetric nuclei.

Heavy nuclei beyond the Fe-group are made primarily via r(apid)-process and s(low)-process n(eutron)-capture events. Although the s-process n-capture is fairly well understood, the r-process n-capture events remain poorly understood. The relative role of Core Collapse Supernova and n-star mergers will likely be understood in the next few decades. I will discuss recent studies of old Metal-Poor stars that are revealing some new details of nucleosynthesis. This progress is due to the availability of high resolution spectra from large ground based telescopes, access to the UV via the Hubble Space Telescope, and better laboratory data.

Strong coupling lattice QCD in the dual representation allows to study the full \\mu-T phase diagram, due to the mildness of the finite density sign problem. This has been done in the chiral limit, both at finite N_t and in the continuous time limit. We extend the phase diagram to finite quark masses and finite inverse gauge coupling. I present numerical results from direct Monte Carlo simulations via worm algorithm.

That would be a high-level view of the whole process of making nuclear data. It will explain how theories and experiments and models all get combined. Especially relevant if FRIB is to make nuclear data for new nuclides.

Rhenium-186 (186Re), arsenic-77 (77As), and rhodium-105 (105Rh) are radionuclides with nuclear properties suitable for “theranostics” in that they emit both beta particles for radiotherapy and gamma rays for imaging, with 90 h, 38.8 h and 35.4 h half-lives, respectively. Additionally, 72As is a positron emitter that is a true “matched pair” radioisotope for 77As. All of these radionuclides can be produced in high specific activity at either an accelerator or nuclear reactor. High specific activity 77As and 105Rh are produced by thermal neutron irradiation of 76Ge or 104Ru, followed by beta decay, with the 77As and 105Rh separated from the enriched targets. High specific activity 186Re can be produced by either proton or deuteron irradiation of enriched 186W or by proton irradiation of enriched Os targets, again followed by separation of the 186Re- from its target material. Sulfur-containing chelates (either thiols or thioethers) are used to form stable complexes with these radionuclides. The chemistry and radiochemistry from production through preliminary biological studies will be presented.

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