Files in ginettelafit/PowerLAPIM
Power Analysis Longitudinal APIM with Quadratic Effects

DESCRIPTION
NAMESPACE
R/Performance.Dyad.Model.1.R R/Performance.Dyad.Model.1.lag.R R/Performance.Dyad.Model.10.R R/Performance.Dyad.Model.10.lag.R R/Performance.Dyad.Model.11.R R/Performance.Dyad.Model.11.lag.R R/Performance.Dyad.Model.12.R R/Performance.Dyad.Model.12.lag.R R/Performance.Dyad.Model.13.R R/Performance.Dyad.Model.13.lag.R R/Performance.Dyad.Model.14.R R/Performance.Dyad.Model.14.lag.R R/Performance.Dyad.Model.15.R R/Performance.Dyad.Model.15.lag.R R/Performance.Dyad.Model.16.R R/Performance.Dyad.Model.16.lag.R R/Performance.Dyad.Model.2.R R/Performance.Dyad.Model.2.lag.R R/Performance.Dyad.Model.3.R R/Performance.Dyad.Model.3.lag.R R/Performance.Dyad.Model.4.R R/Performance.Dyad.Model.4.lag.R R/Performance.Dyad.Model.5.R R/Performance.Dyad.Model.5.lag.R R/Performance.Dyad.Model.6.R R/Performance.Dyad.Model.6.lag.R R/Performance.Dyad.Model.7.R R/Performance.Dyad.Model.7.lag.R R/Performance.Dyad.Model.8.R R/Performance.Dyad.Model.8.lag.R R/Performance.Dyad.Model.9.R R/Performance.Dyad.Model.9.lag.R R/Performance.Dyad.Model.lag.R R/Sim.Dyad.Data.IL.R R/Sim.Dyad.Model.1.R R/Sim.Dyad.Model.1.lag.R R/Sim.Dyad.Model.10.R R/Sim.Dyad.Model.10.lag.R R/Sim.Dyad.Model.11.R R/Sim.Dyad.Model.11.lag.R R/Sim.Dyad.Model.12.R R/Sim.Dyad.Model.12.lag.R R/Sim.Dyad.Model.13.R R/Sim.Dyad.Model.13.lag.R R/Sim.Dyad.Model.14.R R/Sim.Dyad.Model.14.lag.R R/Sim.Dyad.Model.15.R R/Sim.Dyad.Model.15.lag.R R/Sim.Dyad.Model.16.R R/Sim.Dyad.Model.16.lag.R R/Sim.Dyad.Model.2.R R/Sim.Dyad.Model.2.lag.R R/Sim.Dyad.Model.3.R R/Sim.Dyad.Model.3.lag.R R/Sim.Dyad.Model.4.R R/Sim.Dyad.Model.4.lag.R R/Sim.Dyad.Model.5.R R/Sim.Dyad.Model.5.lag.R R/Sim.Dyad.Model.6.R R/Sim.Dyad.Model.6.lag.R R/Sim.Dyad.Model.7.R R/Sim.Dyad.Model.7.lag.R R/Sim.Dyad.Model.8.R R/Sim.Dyad.Model.8.lag.R R/Sim.Dyad.Model.9.R R/Sim.Dyad.Model.9.lag.R R/Sim.Dyad.Model.lag.R R/Sim.model.Dyad.IL.R R/Summary.model.Dyad.IL.R README.md
ginettelafit/PowerLAPIM documentation built on Jan. 21, 2022, 5:38 a.m.