Abstract.We describe an algorithm for computing an inverse spherical harmonic transform suitable for graphic processing units (GPU). We use CUDA and base our implementation on a Fortran90 routine included in a publicly available parallel package, s 2 hat. We focus our attention on the two major sequential steps involved in the transforms computation, retaining the efficient parallel framework of the original code. We detail optimization techniques used to enhance the performance of the CUDA-based code and contrast them with those implemented in the Fortran90 version. We also present performance comparisons of a single CPU plus GPU unit with the s 2 hat code running on either a single or 4 processors. In particular we find that use of the latest generation of GPUs, such as NVIDIA GF100 (Fermi), can accelerate the spherical harmonic transforms by as much as 18 times with respect to s 2 hat executed on one core, and by as much as 5.5 with respect to s 2 hat on 4 cores, with the overall performance being limited by the Fast Fourier transforms.The work presented here has been performed in the context of the Cosmic Microwave Background simulations and analysis. However, we expect that the developed software will be of more general interest and applicability.1. Introduction. Spherical harmonic transforms are ubiquitous in diverse areas of science and practical applications, which need to deal with data distributed on a sphere. In particular, they are heavily used in various areas of cosmology, such as studies of the cosmic microwave background (CMB) radiation and its anisotropies, which have been our main motivations for this work. CMB is an electromagnetic radiation left over after the hot and very dense stage of early evolution of our Universe. The CMB measurements allow us to look back directly at the Universe when its age was only a small fraction (∼ 3%) of its current one (∼ 13Gyrs), and indirectly to learn about its status as far back as to ∼ 10 −35 sec after its nominal beginning (so called Big Bang). Not surprisingly, the CMB measurements play a vital role in the present-day cosmology and have been a driving force behind turning it into a high precision, data-driven science it is today.The CMB radiation is nearly isotropic but minute deviations, on order of 1 part in 10 5 , were first theoretically predicted and later detected. These so-called anisotropies encode the information about the Universe, its past and composition, and their detection and characterization has the major target of the CMB observations since the moment of its discovery in 1965. Over the time progressively more sophisticated and advanced observational apparata have been designed and deployed in search for their more subtle and taletelling characteristics. These include three major CMB satellites -American: Cosmic Microwave Background Explorer (COBE) [13], Wilkinson Microwave Anisotropy Probe (WMAP) [2], and European Planck 1 -and a few dozen of ground-based and balloon-borne projects. Some of these are operating at this time,
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