Least squares method is usually mentioned in two contexts. First, its application is widely known in regression analysis. It is used to construct models on the basis of noisy experimental data. At that, besides constructing a model, it usually performed an estimate of the error with which parameters were calculated. Some other problems could be solved as well. Secondly, the least-squares method is often applied as an fitting method without any connection to statistics.
Most fitting algorithms implemented in ALGLIB are build on top of the linear least squares solver:
First three methods are important special cases of the 1-dimensional curve fitting. Last method can be used for 1-dimensional or multidimensional fitting.
ALGLIB package supports nonlinear fitting by user-defined functions using Levenberg-Marquardt optimizer. Interface described below is just a convenience wrapper around underlying optimizer.
If you don't know what method to choose or just want to explore all features of the ALGLIB package, you can use our Guide to Fitting Algorithms. If you want:
You can make polynomial fit with polynomialfit (unconstrained unweighted fitting) and polynomialfitwc (constrained weighted fitting) functions. Second function supports arbitrary number of constrains on function value - f(xc)=yc - or its derivative - df(xc)/dx=yc. Time needed to solve problem is O(N·M^{ 2}) (where N is the number of points, M is the basis size).
Note #1
Excessive constraints can be inconsistent, especially when you fit data by low degree polynomial.
Read comments on polynomialfitwc for more information on this subject.
Both functions use Chebyshev basis with automatic scaling/translation internally, which allows to reduce condition number. However, they return fitting result in the barycentric form, which is used by ALGLIB to store polynomial and rational functions.
ALGLIB package uses barycentric representation for polynomial operations because it is more stable than the power basis representation. Coefficients of barycentric model are stored in the barycentricinterpolant object. There are two subpackages - polint and ratint - which provide functions for operations with this object (evaluation, differentiation, etc.). More information on this subject can be obtained in the User Guide on polynomial interpolation.
However, sometimes users need polynomial coefficients, not some black box which can be used to evaluate polynomial at any point. You can use two functions to do so:
Examples below describe polynomial fitting. If you want to know about polynomial interpolation in the ALGLIB, we can recommend you to read polint subpackage description from ALGLIB Reference Manual or to read ALGLIB User Guide on polynomial interpolation.
ALGLIB package includes two functions for rational curve fitting using Floater-Hormann basis: barycentricfitfloaterhormann, which solves unconstrained unweighted problems, and barycentricfitfloaterhormannwc, which solves problem with individual weighs and constraints. Latter one supports arbitrary number of constraints on function value or first derivative: f(xc)=yc or df(xc)/dx=yc. As result, barycentricinterpolant object is returned. You can use functions provided by ratint subpackage to work with barycentric interpolant (evaluate, differentiate, etc.). More information on this subject can be obtained in the User Guide on rational interpolation.
Note #2
Excessive constraints can be inconsistent.
Read comments on barycentricfitfloaterhormannwc for more information on this subject.
Both functions use Floater-Hormann basis built on equidistant grid with M nodes. They search for optimal D in [0,9] ("optimal" means "least weighted RMS error"). Because such fitting task is linear, linear solver with O(N·M^{ 2}) complexity is used (here N is a number of points, M is a basis size).
It is important to note that reduced set of rational functions is used for fitting - set of Floater-Hormann rational functions, which have no poles on the real axis. From the one side, Floater-Hormann fitting is more stable than fitting by arbitrary rational functions. From the other side, Floater-Hormann functions have less degrees of freedom than general rational function. You may achieve error as small as 10^{ -3}...10^{ -5} using only moderate number of points. But interpolation/fitting error have geometric, not exponential convergence, thus Floater-Hormann function are not well suited for tasks where extra high precision with limited number of points is needed.
ALGLIB package supports three types of spline fits:
Last two algorithms are inferior to the first one and are not described here. They are still supported by ALGLIB, but because of backward compatibility only.
Penalized regression spline is a 1-dimensional curve fitting algorithm which is suited for noisy fitting problems, underdetermined problems, and problems which need adaptive control over smoothing. It is cubic spline with continuous second derivative, with M uniformly distributed nodes, whose coefficients are obtained as minimizer of sum of LS (approximation error) and P (penalty function which suppresses nonlinearity):
You can built penalized regression spline with two functions:
Both functions reduce minimization of LS+P to the linear least squares problem with O(N·M^{ 2}+M^{ 3}) time complexity. As result, they return spline1dinterpolant object which contains cubic spline. ALGLIB package offers a lot of functions which operate with this object. They are described in documentation on spline1d subpackage. Some additional information can be found in the User Guide on cubic splines.
Key benefits of penalized regression spline are:
Penalized regression spline is quite different from other fitting algorithms. It is one of the best one dimensional fitting algorithms. If you need stable and easy to tune fitting algo, we recommend you to choose penalized splines.
As many other algorithms, penalized spline needs some simple tuning:
Thus, algorithm tuning includes two independent stages. Parameters are tuned separately, and you can set M in the "set and forget" fashion, concentrating on tuning of the ρ parameter.
Consider application of penalized regression spline to the smoothing of noisy data. We will try to fit f, given by its values on N equidistant nodes, by spline with M degrees of freedom and different values of penalty coefficient ρ.
f is composed from three terms: the first one is low-frequency part, the second one is medium-frequency noise, and the third one is high frequency noise. On the first of two charts below you can see low-frequency part (blue curve) and noisy function we pass to the smoother (red curve). Two harmonics are clearly seen in the noise - one with frequency equal to 10, and another with frequency equal to 100.
Second chart shows us three splines corresponding to different values of ρ. Blue curve was generated using very low value of ρ (although it is not the lowest value possible - ρ can be negative). Dark red line was generated with moderate amount of smoothing, which damped high frequency components, but left medium frequency components almost unchanged. And finally, green curve was generated with high amount of smoothing, which fully suppressed noise in the data.
Note #3
Take into the account that number of degrees of freedom M was significantly larger than number of points N, but we see no signs of overfitting.
We do not provide source code for example above because it does not fit into our automated multilingual example generation framework. However, ALGLIB reference manual includes other spline-related examples with source code:
ALGLIB package contains two functions for solution of the unconstrained linear least squares problems:
Linear least squares fitting can be used if function being fitted is represented as linear combination of basis functions. Basis functions themselves can be nonlinear with respect to x.
For example, f_{POL } (see below), demonstrates that polynomial is actually linear function with respect to its coefficients c. Another function, f_{SIN }, demonstrates usage of sines as basis functions .
The solution of the least squares problem is c - vector of coefficients which minimizes fitting error E(x). Below you can find two formulae for E(x) - one for weighted problem, another for unweighted one:
Note #4
Note that weights, if there are any, are squared.
Minimizer of such function can be found by solution of linear system, which allows us to use linear solver which has fixed O(N·M^{ 2}) time complexity. We use direct solver, so you don't have to wait some unknown amount of time for convergence of iterative algorithm. Another benefit, arising from problem linearity, is that you don't have to repeatedly calculate values of basis functions. Just calculate them once in all sample points and pass matrix of values to the algorithm.
Note #5
We use SVD-based solver, which allows us to solve even degenerate problems with linearly dependent systems of basis functions.
Note #6
Most fitting algorithm described on this page are actually wrappers around linear solver described here.
If you have LLS problem with linear equality constraints on coefficient vector c
you can use:
As in unconstrained case, problem reduces to the solution of the linear system.
Note #7
Constraints can be inconsistent, i.e. there may not exists such c which satisfies all of them simultaneously.
In this case, corresponding error code will be returned.
This section contains links to examples of linear least squares fitting:
RBF models allow to approximate scalar or vector functions in 2D or 3D space. This method has no limitations on location of points, which can be sampled irregularly or even be non-distinct. It makes RBF models interesting alternative to another algorithms, like 2D/3D approximating splines. ALGLIB package implements efficient RBF fitting algorithm with O(N·logN) working time (rbf unit). This algorithm is studied in more details in the article on ALGLIB implementation of RBFs, which we recommend to anyone who have to solve fitting problems in 2D/3D.
ALGLIB package supports nonlinear curve fitting using Levenberg-Marquardt method. Nonlinear fitting is supported by lsfit subpackage which provides several important features:
Nonlinear fitting is quite different from linear one: 1) linear problems have fixed time complexity, whereas solution of nonlinear problem is an iterative process, whose convergence speed is problem-dependent, and 2) nonlinear methods generally have more tunable parameters than linear ones. Linear problems are solved in one step - we pass data to the solver and get our result. Nonlinear fitting includes several steps:
ALGLIB users can choose between three operating modes of nonlinear solver which differ in what information about function being fitted they need:
Any of the modes mentioned above can be used to solve unweighted or weighted problems. Letters in the mode name are appended to the constructor function name; if you use weighted version, W is appended too. So we have 6 versions of constructor functions:
What operating mode to choose? For a quick start we recommend to choose F-mode, because it is the simplest of all nonlinear fitting modes provided by ALGLIB. You just calculate function value at given point x with respect to the vector of tunable parameters c, and ALGLIB package solves all numerical differentiation issues. However, as we told above, gradient-free nonlinear fitting is easy to use, but is not efficient. Furthermore, numerical differentiation doesn't allow us to find solution with accuracy significantly higher than numerical differentiation step. Thus if you need high performance or high accuracy, you should implement calculation of analytic gradient and switch to FG-mode.
It is well known that Levenberg-Marquardt method converges quadratically when all points are close to the best-fit curve ("good fit"). However, on a "bad fit" problems convergence becomes linear. If you (a) need very good performance on a "bad fit" problems and (b) have cheap Hessian, you can try using FGH-mode. It requires less iterations, but iteration cost is somewhat higher, so it is hard to tell whether it will be beneficial or not. However, in some situations it is worth a try.
ALGLIB package offers three types of stopping criteria:
You may set one or several criteria by calling lsfitsetcond function. After algorithm is done, you can analyze completion code and determine why it stopped.
We recommend you to use first criterion (sufficiently small step). Step size is problem dependent, but we recommend to use some small value, significantly smaller than desired accuracy. Sometimes, in the hard places, algorithm can make very small step. And if length of last step was 0.001, it does not mean that distance to the solution has same magnitude. For example, it can mean that our quadratic model is too old and needs recalculation. Or that we move through valley with hard turns.
Note #8
Additionally you may limit number of algorithm iterations - if you want to guarantee that algorithm won't work for too long.
For example, such criterion is useful in some embedded/real-time applications where you need something right now - or nothing at all.
Note #9
"sufficiently small gradient" criterion is inaccessible to user because it is hard to tell what value of
"gradient of weighted sum of squared residuals" is sufficiently small.
Stepsize or function change criteria are more intuitive.
Before you start to use optimizer, we recommend you to set scale of the variables with lsfitsetscale function. Scaling is essential for correct work of the stopping criteria (and sometimes for convergence of optimizer). You can do without scaling if your problem is well scaled. However, if some variables are up to 100 times different in magnitude, we recommend you to tell solver about their scale. And we strongly recommend to set scaling in case of larger difference in magnitudes.
We recommend you to read separate article on variable scaling, which is worth reading unless you solve some simple toy problem.
ALGLIB package supports fitting with boundary constraints, i.e. constraints of the form l_{i }≤c_{i }≤u_{i }. Boundary constraints can be set with lsfitsetbc function. These constraints are handled very efficiently - computational overhead for having N constraints is just O(N) additional operations per function evaluation. Finally, these constraints are always exactly satisfied. We won't calculate function at points outside of the interval given by [l_{i },u_{i }]. Optimization result will be inside [l_{i },u_{i }] or exactly at its boundary.
Additionally, ALGLIB users can:
Nonlinear least squares solver described here is actually a convenience wrapper around Levenberg-Marquardt optimizer. Working with specialized interface is more convenient that using underlying optimization algorithm directly. From the other side, convenience interface is somewhat slower than original algorithm because of additional level of abstraction it provides. When Levenberg-Marquardt algorithm makes one call of user-defined function, convenience wrapper makes N calls (N is a number of points), each of them being accompanied with complex movement of data between internal structures. It is especially important for small-scale problems (1-3 parameters to fit) with very cheap functions/gradients - in such cases performance may be up to several times lower.
What to choose - performance or convenience? If you are new to ALGLIB and want to quickly get some code which works, we recommend you to use nonlinear least squares solver described here. You will save some development time and you will be able to qiuckly build working prototype.
However, if you need high performance, we recommend you to work directly with underlying optimizer. Or alternatively you can start from lsfit subpackage (specialized interface) and, after getting familiar with ALGLIB, switch to minlm subpackage (underlying optimizer).
This section contains links to examples of nonlinear least squares fitting:
This article is intended for personal use only.
C# source.
C++ source.
C++ source. MPFR/GMP is used.
GMP source is available from gmplib.org. MPFR source is available from www.mpfr.org.
FreePascal version.
Delphi version.
VB.NET version.
VBA version.
Python version (CPython and IronPython are supported).
ALGLIB® - numerical analysis library, 1999-2015. |