twinstimtwinstim model as described in Meyer et al. (2012) requires
  the specification of the spatial and temporal interaction functions
  ($f$ and $g$, respectively), 
  i.e. how infectivity decays with increasing spatial and temporal
  distance from the source of infection.
  It is of course possible to define own functions (see
  siaf and tiaf, respectively), but the
  package already predefines some useful dispersal kernels returned by
  the constructor functions documented here.
  See Meyer and Held (2014) for various spatial interaction functions,
  and Meyer et al. (2016, Section 3) for an illustration of
  the implementation.# predefined spatial interaction functions
siaf.constant()
siaf.step(knots, maxRange = Inf, nTypes = 1, validpars = NULL)
siaf.gaussian(nTypes = 1, logsd = TRUE, density = FALSE,
              F.adaptive = TRUE, effRangeMult = 6, validpars = NULL)
siaf.powerlaw(nTypes = 1, validpars = NULL)
siaf.powerlawL(nTypes = 1, validpars = NULL)
siaf.student(nTypes = 1, validpars = NULL)# predefined temporal interaction functions
tiaf.constant()
tiaf.step(knots, maxRange = Inf, nTypes = 1, validpars = NULL)
tiaf.exponential(nTypes = 1, validpars = NULL)
knots.
    Per default (maxRange=Inf), the step function
    never drops to 0 but keeps the last height for any distance larger
    than the last knot. However, this might not work in some cases,
    wnTypes=1. Otherwise nTypesdensity=TRUE, siaf.gaussian uses the density of the
    bivariate, isotropic normal distribution as the spatial interaction
    function. Otherwise (defaF.adaptive = TRUE, then an adaptive bandwidth of
    adapt*sd will be used in the midpoint-cubature
    (polyCub.midpoint in package effRangeMult=6
    the $6 \sigma$ region around the event is considered as
    the relsiaf).
    If logsd=FALSE and one prefers not to use
    method="L-BFGS-B" for fitting the twinstim's likelihood involves cubature of the
  spatial interaction function over polygonal domains. Various
  approaches have been compared by Meyer (2010, Section 3.2) and a new
  efficient method, which takes advantage of the assumed isotropy, has
  been proposed by Meyer and Held (2014, Supplement B, Section 2) for
  evaluation of the power-law kernels.
  These cubature methods are available in the dedicated Rpackage
    Meyer, S., Elias, J. and H
  Meyer, S. and Held, L. (2014):
  Power-law models for infectious disease spread.
  The Annals of Applied Statistics, 8 (3), 1612-1639.
DOI-Link: 
  Meyer, S., Held, L. and H
twinstim, siaf, tiaf,
  and package # constant temporal dispersal
tiaf.constant()
# step function kernel
tiaf.step(c(3,7), maxRange=14, nTypes=2)
# exponential decay specification
tiaf.exponential()
# Type-dependent Gaussian spatial interaction function using an adaptive
# two-dimensional midpoint-rule to integrate it over polygonal domains
siaf.gaussian(2, F.adaptive=TRUE)
# Type-independent power-law kernel
siaf.powerlaw()
# "lagged" power-law
siaf.powerlawL()
# (reparametrized) t-kernel
siaf.student()
# step function kernel
siaf.step(c(10,20,50), maxRange=100)Run the code above in your browser using DataLab