# Overview¶

FINUFFT is a multi-threaded library to compute efficiently the three most common types of nonuniform fast Fourier transform (NUFFT) to a specified precision, in one, two, or three dimensions, on a multi-core shared-memory machine. It is extremely fast (typically achieving \(10^6\) to \(10^8\) points per second), has very simple interfaces to most major numerical languages (C/C++, Fortran, MATLAB, octave, python, and julia), but also has more advanced (vectorized and “guru”) interfaces that allow multiple strength vectors and the reuse of FFT plans. It is written in C++ (with limited use of ++ features), OpenMP, and uses FFTW. It has been developed at the Center for Computational Mathematics at the Flatiron Institute, by Alex Barnett and others, and is released under an Apache v2 license.

## What does FINUFFT do?¶

As an example, given \(M\) real numbers \(x_j \in [0,2\pi)\), and complex numbers \(c_j\), with \(j=1,\dots,M\), and a requested integer number of modes \(N\), FINUFFT can efficiently compute the 1D “type 1” transform, which means to evaluate the \(N\) complex outputs

As with other “fast” algorithms, FINUFFT does not evaluate this sum directly—which would take \(O(NM)\) effort—but rather uses a sequence of steps (in this case, optimally chosen spreading, FFT, and deconvolution) to approximate the vector of answers (1) to within the user’s desired relative tolerance, with only \(O(N \log N +M)\) effort, ie, in almost linear time. Thus the speed-up is similar to that of the FFT. You may now want to jump to quickstart, or see the definitions of the other transforms in general dimension.

One interpretation of (1) is: the returned values \(f_k\) are the
*Fourier series coefficients* of the \(2\pi\)-periodic
distribution \(f(x) := \sum_{j=1}^M c_j \delta(x-x_j)\),
a sum of point-masses with arbitrary locations \(x_j\) and strengths \(c_j\).
Such exponential sums are needed in many applications in science and engineering, including signal processing (scattered data interpolation, applying convolutional transforms, fast summation), imaging (cryo-EM, CT, MRI gridding, coherent diffraction, Fresnel aperture modeling, VLBI astronomy),
numerical analysis
(computing Fourier *transforms* of functions,
moving between non-conforming quadrature grids,
solving partial differential equations, Ewald methods), and finance (correlation estimators).
See our tutorials and demos pages
and the related works
for examples of how to use the NUFFT in applications.
In fact, there are several application areas where it has been overlooked
that the needed computation is simply a NUFFT
(eg, particle-mesh Ewald in molecular dynamics).

## Why FINUFFT? Features and comparison against other NUFFT libraries¶

The basic scheme used by FINUFFT is not new, but there are many mathematical and software engineering improvements over other libraries. As is common in NUFFT algorithms, under the hood is an FFT on a regular “fine” (upsampled) grid—the user has no need to access this directly. Nonuniform points are either spread to, or interpolated from, this fine grid, using a specially designed kernel (see right figure above). Our main features are:

**High speed**. For instance, at similar accuracy, FINUFFT is up to 10x faster than the multi-threaded Chemnitz NFFT3 library, and (in single-thread mode) up to 50x faster than the CMCL NUFFT library. This is achieved via:a simple new “exponential of semicircle” kernel that is provably close to optimal

quadrature approximation for this kernel’s Fourier transform

load-balanced multithreaded spreading/interpolation

bin-sorting of points to improve cache reuse

a low upsampling option for smaller FFTs, especially in type 3 transforms

piecewise polynomial kernel evaluation (additions and multiplications only) that SIMD-vectorizes reliably on open-source compilers

**Less RAM**. Our kernel is so fast that there is no point in precomputation; it is always evaluated on the fly. Thus our memory footprint is often an order of magnitude less than the fastest (precomputed) modes of competitors such as NFFT3 and MIRT, especially at high accuracy.**Automated kernel parameters**. Unlike many competitors, we do not force the user to worry about kernel choice or parameters. The user simply requests a desired relative accuracy, then FINUFFT chooses parameters to target this accuracy as fast as possible.**Simplicity**. We provide interfaces that perform a NUFFT with a single command—just like an FFT—from seven common languages/environments. For advanced users we also have “many vector” interfaces that can be much faster than repeated calls to the simple interface with the same points. Finally (like NFFT3) we have a “guru” interface for maximum flexibility, in all of these languages.

For technical details on much of the above see our papers. Note that there are other tasks (eg, transforms on spheres, inverse NUFFTs) provided by other libraries, such as NFFT3, that FINUFFT does not provide.

## Do I even need a NUFFT?¶

A user’s need for a nonuniform fast Fourier transform is often obscured by the lack of mathematical description in science application areas. Therefore, read our tutorials and demos to try and match to your task. Write the task in terms of one of the three transform types. If both \(M\) and \(N\) are larger than of order \(10^2\), FINUFFT should be the ticket. However, if \(M\) and/or \(N\) is small (of order \(10\) or less), there is no need for a “fast” algorithm: simply evaluate the sums directly.

If you need to fit off-grid data to a Fourier representation
(eg, if you have off-grid \(\mathbf{k}\)-space samples of an unknown image)
but you
do not have *quadrature weights* for the off-grid points, you may
need to *invert* the NUFFT, which actually means solving a large linear system;
see references [GLI] [KKP], and, soon, our tutorials and demos.
Poor coverage by the nonuniform point set will cause ill-conditioning and
a heavy reliance on regularization.

Another scenario is that you wish to evaluate a forward transform such as
(1) repeatedly with
the same set of nonuniform points \(x_j\), but *fresh* strength vectors
\(\{c_j\}_{j=1}^M\), as in the “many vectors” interface mentioned above.
For small such problems it may be even faster to fill an
\(N\)-by-\(M\) matrix \(A\) with entries
\(a_{kj} = e^{ik x_j}\), then use BLAS3 (eg `ZGEMM`

) to compute \(F = AC\),
where each column of \(F\) and \(C\) is a new instance of (1).
If you have very many columns this can be competitive with a NUFFT
even for \(M\) and \(N\) up to \(10^4\), because BLAS3 is so fast.