Multidimensional RootFinding¶
This chapter describes functions for multidimensional rootfinding (solving nonlinear systems with equations in unknowns). The library provides low level components for a variety of iterative solvers and convergence tests. These can be combined by the user to achieve the desired solution, with full access to the intermediate steps of the iteration. Each class of methods uses the same framework, so that you can switch between solvers at runtime without needing to recompile your program. Each instance of a solver keeps track of its own state, allowing the solvers to be used in multithreaded programs. The solvers are based on the original Fortran library MINPACK.
The header file gsl_multiroots.h
contains prototypes for the
multidimensional root finding functions and related declarations.
Overview¶
The problem of multidimensional root finding requires the simultaneous solution of equations, , in variables, ,
In general there are no bracketing methods available for dimensional systems, and no way of knowing whether any solutions exist. All algorithms proceed from an initial guess using a variant of the Newton iteration,
where , are vector quantities and is the Jacobian matrix . Additional strategies can be used to enlarge the region of convergence. These include requiring a decrease in the norm on each step proposed by Newton’s method, or taking steepestdescent steps in the direction of the negative gradient of .
Several rootfinding algorithms are available within a single framework. The user provides a highlevel driver for the algorithms, and the library provides the individual functions necessary for each of the steps. There are three main phases of the iteration. The steps are,
initialize solver state,
s
, for algorithmT
update
s
using the iterationT
test
s
for convergence, and repeat iteration if necessary
The evaluation of the Jacobian matrix can be problematic, either because programming the derivatives is intractable or because computation of the terms of the matrix becomes too expensive. For these reasons the algorithms provided by the library are divided into two classes according to whether the derivatives are available or not.
The state for solvers with an analytic Jacobian matrix is held in a
gsl_multiroot_fdfsolver
struct. The updating procedure requires
both the function and its derivatives to be supplied by the user.
The state for solvers which do not use an analytic Jacobian matrix is
held in a gsl_multiroot_fsolver
struct. The updating procedure
uses only function evaluations (not derivatives). The algorithms
estimate the matrix or
by approximate methods.
Initializing the Solver¶
The following functions initialize a multidimensional solver, either with or without derivatives. The solver itself depends only on the dimension of the problem and the algorithm and can be reused for different problems.

type gsl_multiroot_fsolver¶
This is a workspace for multidimensional rootfinding without derivatives.

type gsl_multiroot_fdfsolver¶
This is a workspace for multidimensional rootfinding with derivatives.

gsl_multiroot_fsolver *gsl_multiroot_fsolver_alloc(const gsl_multiroot_fsolver_type *T, size_t n)¶
This function returns a pointer to a newly allocated instance of a solver of type
T
for a system ofn
dimensions. For example, the following code creates an instance of a hybrid solver, to solve a 3dimensional system of equations:const gsl_multiroot_fsolver_type * T = gsl_multiroot_fsolver_hybrid; gsl_multiroot_fsolver * s = gsl_multiroot_fsolver_alloc (T, 3);
If there is insufficient memory to create the solver then the function returns a null pointer and the error handler is invoked with an error code of
GSL_ENOMEM
.

gsl_multiroot_fdfsolver *gsl_multiroot_fdfsolver_alloc(const gsl_multiroot_fdfsolver_type *T, size_t n)¶
This function returns a pointer to a newly allocated instance of a derivative solver of type
T
for a system ofn
dimensions. For example, the following code creates an instance of a NewtonRaphson solver, for a 2dimensional system of equations:const gsl_multiroot_fdfsolver_type * T = gsl_multiroot_fdfsolver_newton; gsl_multiroot_fdfsolver * s = gsl_multiroot_fdfsolver_alloc (T, 2);
If there is insufficient memory to create the solver then the function returns a null pointer and the error handler is invoked with an error code of
GSL_ENOMEM
.

int gsl_multiroot_fsolver_set(gsl_multiroot_fsolver *s, gsl_multiroot_function *f, const gsl_vector *x)¶

int gsl_multiroot_fdfsolver_set(gsl_multiroot_fdfsolver *s, gsl_multiroot_function_fdf *fdf, const gsl_vector *x)¶
These functions set, or reset, an existing solver
s
to use the functionf
or function and derivativefdf
, and the initial guessx
. Note that the initial position is copied fromx
, this argument is not modified by subsequent iterations.

void gsl_multiroot_fsolver_free(gsl_multiroot_fsolver *s)¶

void gsl_multiroot_fdfsolver_free(gsl_multiroot_fdfsolver *s)¶
These functions free all the memory associated with the solver
s
.

const char *gsl_multiroot_fsolver_name(const gsl_multiroot_fsolver *s)¶

const char *gsl_multiroot_fdfsolver_name(const gsl_multiroot_fdfsolver *s)¶
These functions return a pointer to the name of the solver. For example:
printf ("s is a '%s' solver\n", gsl_multiroot_fdfsolver_name (s));
would print something like
s is a 'newton' solver
.
Providing the function to solve¶
You must provide functions of variables for the root finders to operate on. In order to allow for general parameters the functions are defined by the following data types:

type gsl_multiroot_function¶
This data type defines a general system of functions with parameters.
int (* f) (const gsl_vector * x, void * params, gsl_vector * f)
this function should store the vector result in
f
for argumentx
and parametersparams
, returning an appropriate error code if the function cannot be computed.size_t n
the dimension of the system, i.e. the number of components of the vectors
x
andf
.void * params
a pointer to the parameters of the function.
Here is an example using Powell’s test function,
with . The following code defines a
gsl_multiroot_function
system F
which you could pass to a
solver:
struct powell_params { double A; };
int
powell (gsl_vector * x, void * p, gsl_vector * f) {
struct powell_params * params
= (struct powell_params *)p;
const double A = (params>A);
const double x0 = gsl_vector_get(x,0);
const double x1 = gsl_vector_get(x,1);
gsl_vector_set (f, 0, A * x0 * x1  1);
gsl_vector_set (f, 1, (exp(x0) + exp(x1)
 (1.0 + 1.0/A)));
return GSL_SUCCESS
}
gsl_multiroot_function F;
struct powell_params params = { 10000.0 };
F.f = &powell;
F.n = 2;
F.params = ¶ms;

type gsl_multiroot_function_fdf¶
This data type defines a general system of functions with parameters and the corresponding Jacobian matrix of derivatives,
int (* f) (const gsl_vector * x, void * params, gsl_vector * f)
this function should store the vector result in
f
for argumentx
and parametersparams
, returning an appropriate error code if the function cannot be computed.int (* df) (const gsl_vector * x, void * params, gsl_matrix * J)
this function should store the
n
byn
matrix resultin
J
for argumentx
and parametersparams
, returning an appropriate error code if the function cannot be computed.int (* fdf) (const gsl_vector * x, void * params, gsl_vector * f, gsl_matrix * J)
This function should set the values of the
f
andJ
as above, for argumentsx
and parametersparams
. This function provides an optimization of the separate functions for and —it is always faster to compute the function and its derivative at the same time.size_t n
the dimension of the system, i.e. the number of components of the vectors
x
andf
.void * params
a pointer to the parameters of the function.
The example of Powell’s test function defined above can be extended to include analytic derivatives using the following code:
int
powell_df (gsl_vector * x, void * p, gsl_matrix * J)
{
struct powell_params * params
= (struct powell_params *)p;
const double A = (params>A);
const double x0 = gsl_vector_get(x,0);
const double x1 = gsl_vector_get(x,1);
gsl_matrix_set (J, 0, 0, A * x1);
gsl_matrix_set (J, 0, 1, A * x0);
gsl_matrix_set (J, 1, 0, exp(x0));
gsl_matrix_set (J, 1, 1, exp(x1));
return GSL_SUCCESS
}
int
powell_fdf (gsl_vector * x, void * p,
gsl_matrix * f, gsl_matrix * J) {
struct powell_params * params
= (struct powell_params *)p;
const double A = (params>A);
const double x0 = gsl_vector_get(x,0);
const double x1 = gsl_vector_get(x,1);
const double u0 = exp(x0);
const double u1 = exp(x1);
gsl_vector_set (f, 0, A * x0 * x1  1);
gsl_vector_set (f, 1, u0 + u1  (1 + 1/A));
gsl_matrix_set (J, 0, 0, A * x1);
gsl_matrix_set (J, 0, 1, A * x0);
gsl_matrix_set (J, 1, 0, u0);
gsl_matrix_set (J, 1, 1, u1);
return GSL_SUCCESS
}
gsl_multiroot_function_fdf FDF;
FDF.f = &powell_f;
FDF.df = &powell_df;
FDF.fdf = &powell_fdf;
FDF.n = 2;
FDF.params = 0;
Note that the function powell_fdf
is able to reuse existing terms
from the function when calculating the Jacobian, thus saving time.
Iteration¶
The following functions drive the iteration of each algorithm. Each function performs one iteration to update the state of any solver of the corresponding type. The same functions work for all solvers so that different methods can be substituted at runtime without modifications to the code.

int gsl_multiroot_fsolver_iterate(gsl_multiroot_fsolver *s)¶

int gsl_multiroot_fdfsolver_iterate(gsl_multiroot_fdfsolver *s)¶
These functions perform a single iteration of the solver
s
. If the iteration encounters an unexpected problem then an error code will be returned,GSL_EBADFUNC
the iteration encountered a singular point where the function or its derivative evaluated to
Inf
orNaN
.GSL_ENOPROG
the iteration is not making any progress, preventing the algorithm from continuing.
The solver maintains a current best estimate of the root s>x
and its function value s>f
at all times. This information can
be accessed with the following auxiliary functions,

gsl_vector *gsl_multiroot_fsolver_root(const gsl_multiroot_fsolver *s)¶

gsl_vector *gsl_multiroot_fdfsolver_root(const gsl_multiroot_fdfsolver *s)¶
These functions return the current estimate of the root for the solver
s
, given bys>x
.

gsl_vector *gsl_multiroot_fsolver_f(const gsl_multiroot_fsolver *s)¶

gsl_vector *gsl_multiroot_fdfsolver_f(const gsl_multiroot_fdfsolver *s)¶
These functions return the function value at the current estimate of the root for the solver
s
, given bys>f
.

gsl_vector *gsl_multiroot_fsolver_dx(const gsl_multiroot_fsolver *s)¶

gsl_vector *gsl_multiroot_fdfsolver_dx(const gsl_multiroot_fdfsolver *s)¶
These functions return the last step taken by the solver
s
, given bys>dx
.
Search Stopping Parameters¶
A root finding procedure should stop when one of the following conditions is true:
A multidimensional root has been found to within the userspecified precision.
A userspecified maximum number of iterations has been reached.
An error has occurred.
The handling of these conditions is under user control. The functions below allow the user to test the precision of the current result in several standard ways.

int gsl_multiroot_test_delta(const gsl_vector *dx, const gsl_vector *x, double epsabs, double epsrel)¶
This function tests for the convergence of the sequence by comparing the last step
dx
with the absolute errorepsabs
and relative errorepsrel
to the current positionx
. The test returnsGSL_SUCCESS
if the following condition is achieved,for each component of
x
and returnsGSL_CONTINUE
otherwise.

int gsl_multiroot_test_residual(const gsl_vector *f, double epsabs)¶
This function tests the residual value
f
against the absolute error boundepsabs
. The test returnsGSL_SUCCESS
if the following condition is achieved,and returns
GSL_CONTINUE
otherwise. This criterion is suitable for situations where the precise location of the root, , is unimportant provided a value can be found where the residual is small enough.
Algorithms using Derivatives¶
The root finding algorithms described in this section make use of both the function and its derivative. They require an initial guess for the location of the root, but there is no absolute guarantee of convergence—the function must be suitable for this technique and the initial guess must be sufficiently close to the root for it to work. When the conditions are satisfied then convergence is quadratic.

type gsl_multiroot_fdfsolver_type¶
The following are available algorithms for minimizing functions using derivatives.

gsl_multiroot_fdfsolver_type *gsl_multiroot_fdfsolver_hybridsj¶
This is a modified version of Powell’s Hybrid method as implemented in the HYBRJ algorithm in MINPACK. Minpack was written by Jorge J. Moré, Burton S. Garbow and Kenneth E. Hillstrom. The Hybrid algorithm retains the fast convergence of Newton’s method but will also reduce the residual when Newton’s method is unreliable.
The algorithm uses a generalized trust region to keep each step under control. In order to be accepted a proposed new position must satisfy the condition , where is a diagonal scaling matrix and is the size of the trust region. The components of are computed internally, using the column norms of the Jacobian to estimate the sensitivity of the residual to each component of . This improves the behavior of the algorithm for badly scaled functions.
On each iteration the algorithm first determines the standard Newton step by solving the system . If this step falls inside the trust region it is used as a trial step in the next stage. If not, the algorithm uses the linear combination of the Newton and gradient directions which is predicted to minimize the norm of the function while staying inside the trust region,
This combination of Newton and gradient directions is referred to as a dogleg step.
The proposed step is now tested by evaluating the function at the resulting point, . If the step reduces the norm of the function sufficiently then it is accepted and size of the trust region is increased. If the proposed step fails to improve the solution then the size of the trust region is decreased and another trial step is computed.
The speed of the algorithm is increased by computing the changes to the Jacobian approximately, using a rank1 update. If two successive attempts fail to reduce the residual then the full Jacobian is recomputed. The algorithm also monitors the progress of the solution and returns an error if several steps fail to make any improvement,
GSL_ENOPROG
the iteration is not making any progress, preventing the algorithm from continuing.
GSL_ENOPROGJ
reevaluations of the Jacobian indicate that the iteration is not making any progress, preventing the algorithm from continuing.

gsl_multiroot_fdfsolver_type *gsl_multiroot_fdfsolver_hybridj¶
This algorithm is an unscaled version of HYBRIDSJ. The steps are controlled by a spherical trust region , instead of a generalized region. This can be useful if the generalized region estimated by HYBRIDSJ is inappropriate.

gsl_multiroot_fdfsolver_type *gsl_multiroot_fdfsolver_newton¶
Newton’s Method is the standard rootpolishing algorithm. The algorithm begins with an initial guess for the location of the solution. On each iteration a linear approximation to the function is used to estimate the step which will zero all the components of the residual. The iteration is defined by the following sequence,
where the Jacobian matrix is computed from the derivative functions provided by
f
. The step is obtained by solving the linear system,using LU decomposition. If the Jacobian matrix is singular, an error code of
GSL_EDOM
is returned.

gsl_multiroot_fdfsolver_type *gsl_multiroot_fdfsolver_gnewton¶
This is a modified version of Newton’s method which attempts to improve global convergence by requiring every step to reduce the Euclidean norm of the residual, . If the Newton step leads to an increase in the norm then a reduced step of relative size,
is proposed, with being the ratio of norms . This procedure is repeated until a suitable step size is found.

gsl_multiroot_fdfsolver_type *gsl_multiroot_fdfsolver_hybridsj¶
Algorithms without Derivatives¶
The algorithms described in this section do not require any derivative information to be supplied by the user. Any derivatives needed are approximated by finite differences. Note that if the finitedifferencing step size chosen by these routines is inappropriate, an explicit usersupplied numerical derivative can always be used with the algorithms described in the previous section.

type gsl_multiroot_fsolver_type¶
The following are available algorithms for minimizing functions without derivatives.

gsl_multiroot_fsolver_type *gsl_multiroot_fsolver_hybrids¶
This is a version of the Hybrid algorithm which replaces calls to the Jacobian function by its finite difference approximation. The finite difference approximation is computed using
gsl_multiroots_fdjac()
with a relative step size ofGSL_SQRT_DBL_EPSILON
. Note that this step size will not be suitable for all problems.

gsl_multiroot_fsolver_type *gsl_multiroot_fsolver_hybrid¶
This is a finite difference version of the Hybrid algorithm without internal scaling.

gsl_multiroot_fsolver_type *gsl_multiroot_fsolver_dnewton¶
The discrete Newton algorithm is the simplest method of solving a multidimensional system. It uses the Newton iteration
where the Jacobian matrix is approximated by taking finite differences of the function
f
. The approximation scheme used by this implementation is,where is a step of size with being the machine precision (). The order of convergence of Newton’s algorithm is quadratic, but the finite differences require function evaluations on each iteration. The algorithm may become unstable if the finite differences are not a good approximation to the true derivatives.

gsl_multiroot_fsolver_type *gsl_multiroot_fsolver_broyden¶
The Broyden algorithm is a version of the discrete Newton algorithm which attempts to avoids the expensive update of the Jacobian matrix on each iteration. The changes to the Jacobian are also approximated, using a rank1 update,
where the vectors and are the changes in and . On the first iteration the inverse Jacobian is estimated using finite differences, as in the discrete Newton algorithm.
This approximation gives a fast update but is unreliable if the changes are not small, and the estimate of the inverse Jacobian becomes worse as time passes. The algorithm has a tendency to become unstable unless it starts close to the root. The Jacobian is refreshed if this instability is detected (consult the source for details).
This algorithm is included only for demonstration purposes, and is not recommended for serious use.

gsl_multiroot_fsolver_type *gsl_multiroot_fsolver_hybrids¶
Examples¶
The multidimensional solvers are used in a similar way to the onedimensional root finding algorithms. This first example demonstrates the HYBRIDS scaledhybrid algorithm, which does not require derivatives. The program solves the Rosenbrock system of equations,
with . The solution of this system lies at in a narrow valley.
The first stage of the program is to define the system of equations:
#include <stdlib.h>
#include <stdio.h>
#include <gsl/gsl_vector.h>
#include <gsl/gsl_multiroots.h>
struct rparams
{
double a;
double b;
};
int
rosenbrock_f (const gsl_vector * x, void *params,
gsl_vector * f)
{
double a = ((struct rparams *) params)>a;
double b = ((struct rparams *) params)>b;
const double x0 = gsl_vector_get (x, 0);
const double x1 = gsl_vector_get (x, 1);
const double y0 = a * (1  x0);
const double y1 = b * (x1  x0 * x0);
gsl_vector_set (f, 0, y0);
gsl_vector_set (f, 1, y1);
return GSL_SUCCESS;
}
The main program begins by creating the function object f
, with
the arguments (x,y)
and parameters (a,b)
. The solver
s
is initialized to use this function, with the gsl_multiroot_fsolver_hybrids
method:
int
main (void)
{
const gsl_multiroot_fsolver_type *T;
gsl_multiroot_fsolver *s;
int status;
size_t i, iter = 0;
const size_t n = 2;
struct rparams p = {1.0, 10.0};
gsl_multiroot_function f = {&rosenbrock_f, n, &p};
double x_init[2] = {10.0, 5.0};
gsl_vector *x = gsl_vector_alloc (n);
gsl_vector_set (x, 0, x_init[0]);
gsl_vector_set (x, 1, x_init[1]);
T = gsl_multiroot_fsolver_hybrids;
s = gsl_multiroot_fsolver_alloc (T, 2);
gsl_multiroot_fsolver_set (s, &f, x);
print_state (iter, s);
do
{
iter++;
status = gsl_multiroot_fsolver_iterate (s);
print_state (iter, s);
if (status) /* check if solver is stuck */
break;
status =
gsl_multiroot_test_residual (s>f, 1e7);
}
while (status == GSL_CONTINUE && iter < 1000);
printf ("status = %s\n", gsl_strerror (status));
gsl_multiroot_fsolver_free (s);
gsl_vector_free (x);
return 0;
}
Note that it is important to check the return status of each solver step, in case the algorithm becomes stuck. If an error condition is detected, indicating that the algorithm cannot proceed, then the error can be reported to the user, a new starting point chosen or a different algorithm used.
The intermediate state of the solution is displayed by the following
function. The solver state contains the vector s>x
which is the
current position, and the vector s>f
with corresponding function
values:
int
print_state (size_t iter, gsl_multiroot_fsolver * s)
{
printf ("iter = %3u x = % .3f % .3f "
"f(x) = % .3e % .3e\n",
iter,
gsl_vector_get (s>x, 0),
gsl_vector_get (s>x, 1),
gsl_vector_get (s>f, 0),
gsl_vector_get (s>f, 1));
}
Here are the results of running the program. The algorithm is started at far from the solution. Since the solution is hidden in a narrow valley the earliest steps follow the gradient of the function downhill, in an attempt to reduce the large value of the residual. Once the root has been approximately located, on iteration 8, the Newton behavior takes over and convergence is very rapid:
iter = 0 x = 10.000 5.000 f(x) = 1.100e+01 1.050e+03
iter = 1 x = 10.000 5.000 f(x) = 1.100e+01 1.050e+03
iter = 2 x = 3.976 24.827 f(x) = 4.976e+00 9.020e+01
iter = 3 x = 3.976 24.827 f(x) = 4.976e+00 9.020e+01
iter = 4 x = 3.976 24.827 f(x) = 4.976e+00 9.020e+01
iter = 5 x = 1.274 5.680 f(x) = 2.274e+00 7.302e+01
iter = 6 x = 1.274 5.680 f(x) = 2.274e+00 7.302e+01
iter = 7 x = 0.249 0.298 f(x) = 7.511e01 2.359e+00
iter = 8 x = 0.249 0.298 f(x) = 7.511e01 2.359e+00
iter = 9 x = 1.000 0.878 f(x) = 1.268e10 1.218e+00
iter = 10 x = 1.000 0.989 f(x) = 1.124e11 1.080e01
iter = 11 x = 1.000 1.000 f(x) = 0.000e+00 0.000e+00
status = success
Note that the algorithm does not update the location on every iteration. Some iterations are used to adjust the trustregion parameter, after trying a step which was found to be divergent, or to recompute the Jacobian, when poor convergence behavior is detected.
The next example program adds derivative information, in order to
accelerate the solution. There are two derivative functions
rosenbrock_df
and rosenbrock_fdf
. The latter computes both
the function and its derivative simultaneously. This allows the
optimization of any common terms. For simplicity we substitute calls to
the separate f
and df
functions at this point in the code
below:
int
rosenbrock_df (const gsl_vector * x, void *params,
gsl_matrix * J)
{
const double a = ((struct rparams *) params)>a;
const double b = ((struct rparams *) params)>b;
const double x0 = gsl_vector_get (x, 0);
const double df00 = a;
const double df01 = 0;
const double df10 = 2 * b * x0;
const double df11 = b;
gsl_matrix_set (J, 0, 0, df00);
gsl_matrix_set (J, 0, 1, df01);
gsl_matrix_set (J, 1, 0, df10);
gsl_matrix_set (J, 1, 1, df11);
return GSL_SUCCESS;
}
int
rosenbrock_fdf (const gsl_vector * x, void *params,
gsl_vector * f, gsl_matrix * J)
{
rosenbrock_f (x, params, f);
rosenbrock_df (x, params, J);
return GSL_SUCCESS;
}
The main program now makes calls to the corresponding fdfsolver
versions of the functions:
int
main (void)
{
const gsl_multiroot_fdfsolver_type *T;
gsl_multiroot_fdfsolver *s;
int status;
size_t i, iter = 0;
const size_t n = 2;
struct rparams p = {1.0, 10.0};
gsl_multiroot_function_fdf f = {&rosenbrock_f,
&rosenbrock_df,
&rosenbrock_fdf,
n, &p};
double x_init[2] = {10.0, 5.0};
gsl_vector *x = gsl_vector_alloc (n);
gsl_vector_set (x, 0, x_init[0]);
gsl_vector_set (x, 1, x_init[1]);
T = gsl_multiroot_fdfsolver_gnewton;
s = gsl_multiroot_fdfsolver_alloc (T, n);
gsl_multiroot_fdfsolver_set (s, &f, x);
print_state (iter, s);
do
{
iter++;
status = gsl_multiroot_fdfsolver_iterate (s);
print_state (iter, s);
if (status)
break;
status = gsl_multiroot_test_residual (s>f, 1e7);
}
while (status == GSL_CONTINUE && iter < 1000);
printf ("status = %s\n", gsl_strerror (status));
gsl_multiroot_fdfsolver_free (s);
gsl_vector_free (x);
return 0;
}
The addition of derivative information to the gsl_multiroot_fsolver_hybrids
solver does
not make any significant difference to its behavior, since it able to
approximate the Jacobian numerically with sufficient accuracy. To
illustrate the behavior of a different derivative solver we switch to
gsl_multiroot_fdfsolver_gnewton
. This is a traditional Newton solver with the constraint
that it scales back its step if the full step would lead “uphill”. Here
is the output for the gsl_multiroot_fdfsolver_gnewton
algorithm:
iter = 0 x = 10.000 5.000 f(x) = 1.100e+01 1.050e+03
iter = 1 x = 4.231 65.317 f(x) = 5.231e+00 8.321e+02
iter = 2 x = 1.000 26.358 f(x) = 8.882e16 2.736e+02
iter = 3 x = 1.000 1.000 f(x) = 2.220e16 4.441e15
status = success
The convergence is much more rapid, but takes a wide excursion out to the point . This could cause the algorithm to go astray in a realistic application. The hybrid algorithm follows the downhill path to the solution more reliably.
References and Further Reading¶
The original version of the Hybrid method is described in the following articles by Powell,
M.J.D. Powell, “A Hybrid Method for Nonlinear Equations” (Chap 6, p 87–114) and “A Fortran Subroutine for Solving systems of Nonlinear Algebraic Equations” (Chap 7, p 115–161), in Numerical Methods for Nonlinear Algebraic Equations, P. Rabinowitz, editor. Gordon and Breach, 1970.
The following papers are also relevant to the algorithms described in this section,
J.J. Moré, M.Y. Cosnard, “Numerical Solution of Nonlinear Equations”, ACM Transactions on Mathematical Software, Vol 5, No 1, (1979), p 64–85
C.G. Broyden, “A Class of Methods for Solving Nonlinear Simultaneous Equations”, Mathematics of Computation, Vol 19 (1965), p 577–593
J.J. Moré, B.S. Garbow, K.E. Hillstrom, “Testing Unconstrained Optimization Software”, ACM Transactions on Mathematical Software, Vol 7, No 1 (1981), p 17–41