| Day | Time | Title | Speaker |
| Monday | 9 to 9:30 | Welcome | Paris and deBoer |
| 9:30 to 10:30 | Reflections on the History of R-Matrix Theory and its Application to Light Nuclear Reactions | Hale | |
| 10:30 to 11 | Break | ||
| 11 to 12 | Introduction to R-matrix Theory | Thompson | |
| 12:30 to 2 | Lunch | ||
| 2 to 3 | Introduction to R-matrix Theory (cont.) | Thompson | |
| 3 to 3:30 | Break | ||
| 3:30 to 4 | SAMMY: An R-matrix Bayesian Nuclear Data Evaluation Code | Arbanas | |
| 4:00 to 4:30 | R-matrix Methods & Applications with EDA | Paris | |
| 4:30 to 6 | AZURE2: Tutorial | deBoer | |
| Tuesday | 9 to 9:30 | Study of states in 38Ca that are important for the 34Ar(a,p)37K reaction rate through 37K+p elastic scattering | Lauer |
| 9:30 to 10 | Analysis of 13C excited states above the a-threshold by R-matrix analysis of alpha+9Be elastic and inelastic scattering data | Dell'Aquila | |
| 10 to 10:45 | Discussion/break: Analysis of scattering reactions in R-matrix | ||
| 10:45 to 11:15 | Commissioning the SONIK (Scattering of Nuclei in Inverse Kinematics) scattering chamber | Connolly | |
| 11:15 to 11:45 | Study of O-14 through resonant alpha scattering | Ahn | |
| 11:45 to 12:30 | Discussion: Analysis of scattering reactions in R-matrix (cont.) | ||
| 12:30 to 2 | Lunch | ||
| 2 to 2:30 | R-matrix theory in the analysis of fission cross-sections | Lynn | |
| 2:30 to 3 | Analysis of experimental data and uncertainty evaluation | Kopecky | |
| 3 to 3:30 | Break | ||
| 3:30 to 4:15 | Discussion/break: neutron induced fission on heavy nuclei | ||
| 4:15 to 4:45 | Underground Nuclear Astrophysics | Strieder | |
| 4:45 to 5:15 | R-matrix analysis and indirect measurement of 19Ne states relevant to novae explosions | Riley | |
| 5:15 to 5:45 | New data on 14N(p,gamma)15O at 0.4 - 1.4 MeV for improved R-Matrix fits | Wagner | |
| 5:45 to 6:30 | Disscussion: R-matrix in Nuclear Astrophysics | ||
| Wednesday | 8:30 to 9 | R-matrix for beta-decay and three-body decays | Fynbo |
| 9 to 9:30 | R-matrix analysis of the 3H(t,2n) neutron spectrum produced by inertial confinement fusion experiments | Sayre | |
| 9:30 to 10 | Neutron-Induced Breakup Reactions Using 100-ps Pulses from Direct-Drive D-T Implosions on OMEGA | Forrest | |
| 10 to 10:45 | Disscussion/break: Three body break up in light systems | ||
| 10:45 to 11:15 | Estimating experimental covariances... and the uncertainties within | Neudecker | |
| 11:15 to 11:45 | Consideration of model defects associated with R-matrix based evaluations | Leeb | |
| 11:45 to 12:30 | Discussion: Covariances in R-matrix | ||
| 12:30 to 2 | Lunch | ||
| 2 to 2:30 | Reich-Moore R-matrix parameters for n+16O (*) | Pigni | |
| 2:30 to 3 | Overview of 12C(alpha,gamma)16O | Brune | |
| 3 to 3:30 | Can R-Matrix Results be More Accurate Than the Data Itself?; The case of 12C(a,g) | Gai | |
| 3:30 to 4 | Error analysis in extrapolations | Gialenella | |
| 4 to 4:45 | Discussion: 12C(a,g) | ||
| Thursday | 8:30 to 9 | R-matrix approach based on hybrid representation | Srdinko |
| 9 to 9:30 | R matrix for Trojan Horse method as indirect technique in nuclear astrophysics. | Mukhamedzhanov | |
| 9:30 to 10 | Resonance and virtual states from a calculable R-matrix approach | Dohet-Eraly | |
| 10 to 10:45 | Discussion/break: Theory advances in R-matrix | ||
| 10:45 to 11:15 | Linking ab initio models, phenomenology, and data | Nollett | |
| 11:15 to 11:45 | R-matrix theory and ab initio calculations of light-nucleus reactions | Quaglioni | |
| 11:45 to 12:30 | Discussion: Ab Initio and phenomenology | ||
| 12:30 to 2 | Lunch | ||
| 2 to 2:30 | Experimental application of the generalized R-matrix approach (19F(p,a) and 13C(a,n)) | LaCognata | |
| 2:30 to 3 | Systematic R-matrix analysis of 13C(a,n)16O Reaction And 13C(a,a ) Scattering At Astrophysical Energies | Chakraborty | |
| 3 to 3:30 | Determining the 16O(n,a) reaction cross section via a forward-propagating analysis | Lee | |
| 3:30 to 4:15 | Discussion/break: 13C(a,n) | ||
| 4:15 to 4:45 | |||
| 4:45 to 5:15 | Spin parity determination of unbound states in 26Mg from neutron spectroscopy | Massimi | |
| 5:15 to 5:45 | Calculated Resonance Properties from the New Resolved Resonance Region Evaluations of Copper | Sobes | |
| 5:45 to 6:30 | Discussion: neutron induced reactions | ||
| Friday | 8:30 to 9 | Cluster structures and what we can learn from resonant scattering | Freer |
| 9 to 9:30 | Constraining R-Matrix Fits with the Shell Model | Massey | |
| 9:30 to 10 | Evaluation of the differential cross-sections for Ion Beam Analysis | Gurbich | |
| 10 to 10:45 | Discussion/break: potential models and R-matrix | ||
| 10:45 to 11:15 | An R-matrix code AMUR for the cross-section evaluation and preliminary approaches to open issues in the analysis | Kunieda | |
| 11:15 to 12:00 | Discussion: R-matrix codes | ||