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+// Ceres Solver - A fast non-linear least squares minimizer
+// Copyright 2010, 2011, 2012 Google Inc. All rights reserved.
+// http://code.google.com/p/ceres-solver/
+//
+// Redistribution and use in source and binary forms, with or without
+// modification, are permitted provided that the following conditions are met:
+//
+// * Redistributions of source code must retain the above copyright notice,
+// this list of conditions and the following disclaimer.
+// * Redistributions in binary form must reproduce the above copyright notice,
+// this list of conditions and the following disclaimer in the documentation
+// and/or other materials provided with the distribution.
+// * Neither the name of Google Inc. nor the names of its contributors may be
+// used to endorse or promote products derived from this software without
+// specific prior written permission.
+//
+// THIS SOFTWARE IS PROVIDED BY THE COPYRIGHT HOLDERS AND CONTRIBUTORS "AS IS"
+// AND ANY EXPRESS OR IMPLIED WARRANTIES, INCLUDING, BUT NOT LIMITED TO, THE
+// IMPLIED WARRANTIES OF MERCHANTABILITY AND FITNESS FOR A PARTICULAR PURPOSE
+// ARE DISCLAIMED. IN NO EVENT SHALL THE COPYRIGHT OWNER OR CONTRIBUTORS BE
+// LIABLE FOR ANY DIRECT, INDIRECT, INCIDENTAL, SPECIAL, EXEMPLARY, OR
+// CONSEQUENTIAL DAMAGES (INCLUDING, BUT NOT LIMITED TO, PROCUREMENT OF
+// SUBSTITUTE GOODS OR SERVICES; LOSS OF USE, DATA, OR PROFITS; OR BUSINESS
+// INTERRUPTION) HOWEVER CAUSED AND ON ANY THEORY OF LIABILITY, WHETHER IN
+// CONTRACT, STRICT LIABILITY, OR TORT (INCLUDING NEGLIGENCE OR OTHERWISE)
+// ARISING IN ANY WAY OUT OF THE USE OF THIS SOFTWARE, EVEN IF ADVISED OF THE
+// POSSIBILITY OF SUCH DAMAGE.
+//
+// Author: keir@google.com (Keir Mierle)
+//
+// A simple implementation of N-dimensional dual numbers, for automatically
+// computing exact derivatives of functions.
+//
+// While a complete treatment of the mechanics of automatic differentation is
+// beyond the scope of this header (see
+// http://en.wikipedia.org/wiki/Automatic_differentiation for details), the
+// basic idea is to extend normal arithmetic with an extra element, "e," often
+// denoted with the greek symbol epsilon, such that e != 0 but e^2 = 0. Dual
+// numbers are extensions of the real numbers analogous to complex numbers:
+// whereas complex numbers augment the reals by introducing an imaginary unit i
+// such that i^2 = -1, dual numbers introduce an "infinitesimal" unit e such
+// that e^2 = 0. Dual numbers have two components: the "real" component and the
+// "infinitesimal" component, generally written as x + y*e. Surprisingly, this
+// leads to a convenient method for computing exact derivatives without needing
+// to manipulate complicated symbolic expressions.
+//
+// For example, consider the function
+//
+// f(x) = x^2 ,
+//
+// evaluated at 10. Using normal arithmetic, f(10) = 100, and df/dx(10) = 20.
+// Next, augument 10 with an infinitesimal to get:
+//
+// f(10 + e) = (10 + e)^2
+// = 100 + 2 * 10 * e + e^2
+// = 100 + 20 * e -+-
+// -- |
+// | +--- This is zero, since e^2 = 0
+// |
+// +----------------- This is df/dx!
+//
+// Note that the derivative of f with respect to x is simply the infinitesimal
+// component of the value of f(x + e). So, in order to take the derivative of
+// any function, it is only necessary to replace the numeric "object" used in
+// the function with one extended with infinitesimals. The class Jet, defined in
+// this header, is one such example of this, where substitution is done with
+// templates.
+//
+// To handle derivatives of functions taking multiple arguments, different
+// infinitesimals are used, one for each variable to take the derivative of. For
+// example, consider a scalar function of two scalar parameters x and y:
+//
+// f(x, y) = x^2 + x * y
+//
+// Following the technique above, to compute the derivatives df/dx and df/dy for
+// f(1, 3) involves doing two evaluations of f, the first time replacing x with
+// x + e, the second time replacing y with y + e.
+//
+// For df/dx:
+//
+// f(1 + e, y) = (1 + e)^2 + (1 + e) * 3
+// = 1 + 2 * e + 3 + 3 * e
+// = 4 + 5 * e
+//
+// --> df/dx = 5
+//
+// For df/dy:
+//
+// f(1, 3 + e) = 1^2 + 1 * (3 + e)
+// = 1 + 3 + e
+// = 4 + e
+//
+// --> df/dy = 1
+//
+// To take the gradient of f with the implementation of dual numbers ("jets") in
+// this file, it is necessary to create a single jet type which has components
+// for the derivative in x and y, and passing them to a templated version of f:
+//
+// template<typename T>
+// T f(const T &x, const T &y) {
+// return x * x + x * y;
+// }
+//
+// // The "2" means there should be 2 dual number components.
+// Jet<double, 2> x(0); // Pick the 0th dual number for x.
+// Jet<double, 2> y(1); // Pick the 1st dual number for y.
+// Jet<double, 2> z = f(x, y);
+//
+// LG << "df/dx = " << z.a[0]
+// << "df/dy = " << z.a[1];
+//
+// Most users should not use Jet objects directly; a wrapper around Jet objects,
+// which makes computing the derivative, gradient, or jacobian of templated
+// functors simple, is in autodiff.h. Even autodiff.h should not be used
+// directly; instead autodiff_cost_function.h is typically the file of interest.
+//
+// For the more mathematically inclined, this file implements first-order
+// "jets". A 1st order jet is an element of the ring
+//
+// T[N] = T[t_1, ..., t_N] / (t_1, ..., t_N)^2
+//
+// which essentially means that each jet consists of a "scalar" value 'a' from T
+// and a 1st order perturbation vector 'v' of length N:
+//
+// x = a + \sum_i v[i] t_i
+//
+// A shorthand is to write an element as x = a + u, where u is the pertubation.
+// Then, the main point about the arithmetic of jets is that the product of
+// perturbations is zero:
+//
+// (a + u) * (b + v) = ab + av + bu + uv
+// = ab + (av + bu) + 0
+//
+// which is what operator* implements below. Addition is simpler:
+//
+// (a + u) + (b + v) = (a + b) + (u + v).
+//
+// The only remaining question is how to evaluate the function of a jet, for
+// which we use the chain rule:
+//
+// f(a + u) = f(a) + f'(a) u
+//
+// where f'(a) is the (scalar) derivative of f at a.
+//
+// By pushing these things through sufficiently and suitably templated
+// functions, we can do automatic differentiation. Just be sure to turn on
+// function inlining and common-subexpression elimination, or it will be very
+// slow!
+//
+// WARNING: Most Ceres users should not directly include this file or know the
+// details of how jets work. Instead the suggested method for automatic
+// derivatives is to use autodiff_cost_function.h, which is a wrapper around
+// both jets.h and autodiff.h to make taking derivatives of cost functions for
+// use in Ceres easier.
+
+#ifndef CERES_PUBLIC_JET_H_
+#define CERES_PUBLIC_JET_H_
+
+#include <cmath>
+#include <iosfwd>
+#include <iostream> // NOLINT
+#include <string>
+
+#include "Eigen/Core"
+#include "ceres/fpclassify.h"
+
+namespace ceres {
+
+template <typename T, int N>
+struct Jet {
+ enum { DIMENSION = N };
+
+ // Default-construct "a" because otherwise this can lead to false errors about
+ // uninitialized uses when other classes relying on default constructed T
+ // (where T is a Jet<T, N>). This usually only happens in opt mode. Note that
+ // the C++ standard mandates that e.g. default constructed doubles are
+ // initialized to 0.0; see sections 8.5 of the C++03 standard.
+ Jet() : a() {
+ v.setZero();
+ }
+
+ // Constructor from scalar: a + 0.
+ explicit Jet(const T& value) {
+ a = value;
+ v.setZero();
+ }
+
+ // Constructor from scalar plus variable: a + t_i.
+ Jet(const T& value, int k) {
+ a = value;
+ v.setZero();
+ v[k] = T(1.0);
+ }
+
+ // Compound operators
+ Jet<T, N>& operator+=(const Jet<T, N> &y) {
+ *this = *this + y;
+ return *this;
+ }
+
+ Jet<T, N>& operator-=(const Jet<T, N> &y) {
+ *this = *this - y;
+ return *this;
+ }
+
+ Jet<T, N>& operator*=(const Jet<T, N> &y) {
+ *this = *this * y;
+ return *this;
+ }
+
+ Jet<T, N>& operator/=(const Jet<T, N> &y) {
+ *this = *this / y;
+ return *this;
+ }
+
+ // The scalar part.
+ T a;
+
+ // The infinitesimal part.
+ //
+ // Note the Eigen::DontAlign bit is needed here because this object
+ // gets allocated on the stack and as part of other arrays and
+ // structs. Forcing the right alignment there is the source of much
+ // pain and suffering. Even if that works, passing Jets around to
+ // functions by value has problems because the C++ ABI does not
+ // guarantee alignment for function arguments.
+ //
+ // Setting the DontAlign bit prevents Eigen from using SSE for the
+ // various operations on Jets. This is a small performance penalty
+ // since the AutoDiff code will still expose much of the code as
+ // statically sized loops to the compiler. But given the subtle
+ // issues that arise due to alignment, especially when dealing with
+ // multiple platforms, it seems to be a trade off worth making.
+ Eigen::Matrix<T, N, 1, Eigen::DontAlign> v;
+};
+
+// Unary +
+template<typename T, int N> inline
+Jet<T, N> const& operator+(const Jet<T, N>& f) {
+ return f;
+}
+
+// TODO(keir): Try adding __attribute__((always_inline)) to these functions to
+// see if it causes a performance increase.
+
+// Unary -
+template<typename T, int N> inline
+Jet<T, N> operator-(const Jet<T, N>&f) {
+ Jet<T, N> g;
+ g.a = -f.a;
+ g.v = -f.v;
+ return g;
+}
+
+// Binary +
+template<typename T, int N> inline
+Jet<T, N> operator+(const Jet<T, N>& f,
+ const Jet<T, N>& g) {
+ Jet<T, N> h;
+ h.a = f.a + g.a;
+ h.v = f.v + g.v;
+ return h;
+}
+
+// Binary + with a scalar: x + s
+template<typename T, int N> inline
+Jet<T, N> operator+(const Jet<T, N>& f, T s) {
+ Jet<T, N> h;
+ h.a = f.a + s;
+ h.v = f.v;
+ return h;
+}
+
+// Binary + with a scalar: s + x
+template<typename T, int N> inline
+Jet<T, N> operator+(T s, const Jet<T, N>& f) {
+ Jet<T, N> h;
+ h.a = f.a + s;
+ h.v = f.v;
+ return h;
+}
+
+// Binary -
+template<typename T, int N> inline
+Jet<T, N> operator-(const Jet<T, N>& f,
+ const Jet<T, N>& g) {
+ Jet<T, N> h;
+ h.a = f.a - g.a;
+ h.v = f.v - g.v;
+ return h;
+}
+
+// Binary - with a scalar: x - s
+template<typename T, int N> inline
+Jet<T, N> operator-(const Jet<T, N>& f, T s) {
+ Jet<T, N> h;
+ h.a = f.a - s;
+ h.v = f.v;
+ return h;
+}
+
+// Binary - with a scalar: s - x
+template<typename T, int N> inline
+Jet<T, N> operator-(T s, const Jet<T, N>& f) {
+ Jet<T, N> h;
+ h.a = s - f.a;
+ h.v = -f.v;
+ return h;
+}
+
+// Binary *
+template<typename T, int N> inline
+Jet<T, N> operator*(const Jet<T, N>& f,
+ const Jet<T, N>& g) {
+ Jet<T, N> h;
+ h.a = f.a * g.a;
+ h.v = f.a * g.v + f.v * g.a;
+ return h;
+}
+
+// Binary * with a scalar: x * s
+template<typename T, int N> inline
+Jet<T, N> operator*(const Jet<T, N>& f, T s) {
+ Jet<T, N> h;
+ h.a = f.a * s;
+ h.v = f.v * s;
+ return h;
+}
+
+// Binary * with a scalar: s * x
+template<typename T, int N> inline
+Jet<T, N> operator*(T s, const Jet<T, N>& f) {
+ Jet<T, N> h;
+ h.a = f.a * s;
+ h.v = f.v * s;
+ return h;
+}
+
+// Binary /
+template<typename T, int N> inline
+Jet<T, N> operator/(const Jet<T, N>& f,
+ const Jet<T, N>& g) {
+ Jet<T, N> h;
+ // This uses:
+ //
+ // a + u (a + u)(b - v) (a + u)(b - v)
+ // ----- = -------------- = --------------
+ // b + v (b + v)(b - v) b^2
+ //
+ // which holds because v*v = 0.
+ h.a = f.a / g.a;
+ h.v = (f.v - f.a / g.a * g.v) / g.a;
+ return h;
+}
+
+// Binary / with a scalar: s / x
+template<typename T, int N> inline
+Jet<T, N> operator/(T s, const Jet<T, N>& g) {
+ Jet<T, N> h;
+ h.a = s / g.a;
+ h.v = - s * g.v / (g.a * g.a);
+ return h;
+}
+
+// Binary / with a scalar: x / s
+template<typename T, int N> inline
+Jet<T, N> operator/(const Jet<T, N>& f, T s) {
+ Jet<T, N> h;
+ h.a = f.a / s;
+ h.v = f.v / s;
+ return h;
+}
+
+// Binary comparison operators for both scalars and jets.
+#define CERES_DEFINE_JET_COMPARISON_OPERATOR(op) \
+template<typename T, int N> inline \
+bool operator op(const Jet<T, N>& f, const Jet<T, N>& g) { \
+ return f.a op g.a; \
+} \
+template<typename T, int N> inline \
+bool operator op(const T& s, const Jet<T, N>& g) { \
+ return s op g.a; \
+} \
+template<typename T, int N> inline \
+bool operator op(const Jet<T, N>& f, const T& s) { \
+ return f.a op s; \
+}
+CERES_DEFINE_JET_COMPARISON_OPERATOR( < ) // NOLINT
+CERES_DEFINE_JET_COMPARISON_OPERATOR( <= ) // NOLINT
+CERES_DEFINE_JET_COMPARISON_OPERATOR( > ) // NOLINT
+CERES_DEFINE_JET_COMPARISON_OPERATOR( >= ) // NOLINT
+CERES_DEFINE_JET_COMPARISON_OPERATOR( == ) // NOLINT
+CERES_DEFINE_JET_COMPARISON_OPERATOR( != ) // NOLINT
+#undef CERES_DEFINE_JET_COMPARISON_OPERATOR
+
+// Pull some functions from namespace std.
+//
+// This is necessary because we want to use the same name (e.g. 'sqrt') for
+// double-valued and Jet-valued functions, but we are not allowed to put
+// Jet-valued functions inside namespace std.
+//
+// Missing: cosh, sinh, tanh, tan
+// TODO(keir): Switch to "using".
+inline double abs (double x) { return std::abs(x); }
+inline double log (double x) { return std::log(x); }
+inline double exp (double x) { return std::exp(x); }
+inline double sqrt (double x) { return std::sqrt(x); }
+inline double cos (double x) { return std::cos(x); }
+inline double acos (double x) { return std::acos(x); }
+inline double sin (double x) { return std::sin(x); }
+inline double asin (double x) { return std::asin(x); }
+inline double pow (double x, double y) { return std::pow(x, y); }
+inline double atan2(double y, double x) { return std::atan2(y, x); }
+
+// In general, f(a + h) ~= f(a) + f'(a) h, via the chain rule.
+
+// abs(x + h) ~= x + h or -(x + h)
+template <typename T, int N> inline
+Jet<T, N> abs(const Jet<T, N>& f) {
+ return f.a < T(0.0) ? -f : f;
+}
+
+// log(a + h) ~= log(a) + h / a
+template <typename T, int N> inline
+Jet<T, N> log(const Jet<T, N>& f) {
+ Jet<T, N> g;
+ g.a = log(f.a);
+ g.v = f.v / f.a;
+ return g;
+}
+
+// exp(a + h) ~= exp(a) + exp(a) h
+template <typename T, int N> inline
+Jet<T, N> exp(const Jet<T, N>& f) {
+ Jet<T, N> g;
+ g.a = exp(f.a);
+ g.v = g.a * f.v;
+ return g;
+}
+
+// sqrt(a + h) ~= sqrt(a) + h / (2 sqrt(a))
+template <typename T, int N> inline
+Jet<T, N> sqrt(const Jet<T, N>& f) {
+ Jet<T, N> g;
+ g.a = sqrt(f.a);
+ g.v = f.v / (T(2.0) * g.a);
+ return g;
+}
+
+// cos(a + h) ~= cos(a) - sin(a) h
+template <typename T, int N> inline
+Jet<T, N> cos(const Jet<T, N>& f) {
+ Jet<T, N> g;
+ g.a = cos(f.a);
+ T sin_a = sin(f.a);
+ g.v = - sin_a * f.v;
+ return g;
+}
+
+// acos(a + h) ~= acos(a) - 1 / sqrt(1 - a^2) h
+template <typename T, int N> inline
+Jet<T, N> acos(const Jet<T, N>& f) {
+ Jet<T, N> g;
+ g.a = acos(f.a);
+ g.v = - T(1.0) / sqrt(T(1.0) - f.a * f.a) * f.v;
+ return g;
+}
+
+// sin(a + h) ~= sin(a) + cos(a) h
+template <typename T, int N> inline
+Jet<T, N> sin(const Jet<T, N>& f) {
+ Jet<T, N> g;
+ g.a = sin(f.a);
+ T cos_a = cos(f.a);
+ g.v = cos_a * f.v;
+ return g;
+}
+
+// asin(a + h) ~= asin(a) + 1 / sqrt(1 - a^2) h
+template <typename T, int N> inline
+Jet<T, N> asin(const Jet<T, N>& f) {
+ Jet<T, N> g;
+ g.a = asin(f.a);
+ g.v = T(1.0) / sqrt(T(1.0) - f.a * f.a) * f.v;
+ return g;
+}
+
+// Jet Classification. It is not clear what the appropriate semantics are for
+// these classifications. This picks that IsFinite and isnormal are "all"
+// operations, i.e. all elements of the jet must be finite for the jet itself
+// to be finite (or normal). For IsNaN and IsInfinite, the answer is less
+// clear. This takes a "any" approach for IsNaN and IsInfinite such that if any
+// part of a jet is nan or inf, then the entire jet is nan or inf. This leads
+// to strange situations like a jet can be both IsInfinite and IsNaN, but in
+// practice the "any" semantics are the most useful for e.g. checking that
+// derivatives are sane.
+
+// The jet is finite if all parts of the jet are finite.
+template <typename T, int N> inline
+bool IsFinite(const Jet<T, N>& f) {
+ if (!IsFinite(f.a)) {
+ return false;
+ }
+ for (int i = 0; i < N; ++i) {
+ if (!IsFinite(f.v[i])) {
+ return false;
+ }
+ }
+ return true;
+}
+
+// The jet is infinite if any part of the jet is infinite.
+template <typename T, int N> inline
+bool IsInfinite(const Jet<T, N>& f) {
+ if (IsInfinite(f.a)) {
+ return true;
+ }
+ for (int i = 0; i < N; i++) {
+ if (IsInfinite(f.v[i])) {
+ return true;
+ }
+ }
+ return false;
+}
+
+// The jet is NaN if any part of the jet is NaN.
+template <typename T, int N> inline
+bool IsNaN(const Jet<T, N>& f) {
+ if (IsNaN(f.a)) {
+ return true;
+ }
+ for (int i = 0; i < N; ++i) {
+ if (IsNaN(f.v[i])) {
+ return true;
+ }
+ }
+ return false;
+}
+
+// The jet is normal if all parts of the jet are normal.
+template <typename T, int N> inline
+bool IsNormal(const Jet<T, N>& f) {
+ if (!IsNormal(f.a)) {
+ return false;
+ }
+ for (int i = 0; i < N; ++i) {
+ if (!IsNormal(f.v[i])) {
+ return false;
+ }
+ }
+ return true;
+}
+
+// atan2(b + db, a + da) ~= atan2(b, a) + (- b da + a db) / (a^2 + b^2)
+//
+// In words: the rate of change of theta is 1/r times the rate of
+// change of (x, y) in the positive angular direction.
+template <typename T, int N> inline
+Jet<T, N> atan2(const Jet<T, N>& g, const Jet<T, N>& f) {
+ // Note order of arguments:
+ //
+ // f = a + da
+ // g = b + db
+
+ Jet<T, N> out;
+
+ out.a = atan2(g.a, f.a);
+
+ T const temp = T(1.0) / (f.a * f.a + g.a * g.a);
+ out.v = temp * (- g.a * f.v + f.a * g.v);
+ return out;
+}
+
+
+// pow -- base is a differentiatble function, exponent is a constant.
+// (a+da)^p ~= a^p + p*a^(p-1) da
+template <typename T, int N> inline
+Jet<T, N> pow(const Jet<T, N>& f, double g) {
+ Jet<T, N> out;
+ out.a = pow(f.a, g);
+ T const temp = g * pow(f.a, g - T(1.0));
+ out.v = temp * f.v;
+ return out;
+}
+
+// pow -- base is a constant, exponent is a differentiable function.
+// (a)^(p+dp) ~= a^p + a^p log(a) dp
+template <typename T, int N> inline
+Jet<T, N> pow(double f, const Jet<T, N>& g) {
+ Jet<T, N> out;
+ out.a = pow(f, g.a);
+ T const temp = log(f) * out.a;
+ out.v = temp * g.v;
+ return out;
+}
+
+
+// pow -- both base and exponent are differentiable functions.
+// (a+da)^(b+db) ~= a^b + b * a^(b-1) da + a^b log(a) * db
+template <typename T, int N> inline
+Jet<T, N> pow(const Jet<T, N>& f, const Jet<T, N>& g) {
+ Jet<T, N> out;
+
+ T const temp1 = pow(f.a, g.a);
+ T const temp2 = g.a * pow(f.a, g.a - T(1.0));
+ T const temp3 = temp1 * log(f.a);
+
+ out.a = temp1;
+ out.v = temp2 * f.v + temp3 * g.v;
+ return out;
+}
+
+// Define the helper functions Eigen needs to embed Jet types.
+//
+// NOTE(keir): machine_epsilon() and precision() are missing, because they don't
+// work with nested template types (e.g. where the scalar is itself templated).
+// Among other things, this means that decompositions of Jet's does not work,
+// for example
+//
+// Matrix<Jet<T, N> ... > A, x, b;
+// ...
+// A.solve(b, &x)
+//
+// does not work and will fail with a strange compiler error.
+//
+// TODO(keir): This is an Eigen 2.0 limitation that is lifted in 3.0. When we
+// switch to 3.0, also add the rest of the specialization functionality.
+template<typename T, int N> inline const Jet<T, N>& ei_conj(const Jet<T, N>& x) { return x; } // NOLINT
+template<typename T, int N> inline const Jet<T, N>& ei_real(const Jet<T, N>& x) { return x; } // NOLINT
+template<typename T, int N> inline Jet<T, N> ei_imag(const Jet<T, N>& ) { return Jet<T, N>(0.0); } // NOLINT
+template<typename T, int N> inline Jet<T, N> ei_abs (const Jet<T, N>& x) { return fabs(x); } // NOLINT
+template<typename T, int N> inline Jet<T, N> ei_abs2(const Jet<T, N>& x) { return x * x; } // NOLINT
+template<typename T, int N> inline Jet<T, N> ei_sqrt(const Jet<T, N>& x) { return sqrt(x); } // NOLINT
+template<typename T, int N> inline Jet<T, N> ei_exp (const Jet<T, N>& x) { return exp(x); } // NOLINT
+template<typename T, int N> inline Jet<T, N> ei_log (const Jet<T, N>& x) { return log(x); } // NOLINT
+template<typename T, int N> inline Jet<T, N> ei_sin (const Jet<T, N>& x) { return sin(x); } // NOLINT
+template<typename T, int N> inline Jet<T, N> ei_cos (const Jet<T, N>& x) { return cos(x); } // NOLINT
+template<typename T, int N> inline Jet<T, N> ei_pow (const Jet<T, N>& x, Jet<T, N> y) { return pow(x, y); } // NOLINT
+
+// Note: This has to be in the ceres namespace for argument dependent lookup to
+// function correctly. Otherwise statements like CHECK_LE(x, 2.0) fail with
+// strange compile errors.
+template <typename T, int N>
+inline std::ostream &operator<<(std::ostream &s, const Jet<T, N>& z) {
+ return s << "[" << z.a << " ; " << z.v.transpose() << "]";
+}
+
+} // namespace ceres
+
+namespace Eigen {
+
+// Creating a specialization of NumTraits enables placing Jet objects inside
+// Eigen arrays, getting all the goodness of Eigen combined with autodiff.
+template<typename T, int N>
+struct NumTraits<ceres::Jet<T, N> > {
+ typedef ceres::Jet<T, N> Real;
+ typedef ceres::Jet<T, N> NonInteger;
+ typedef ceres::Jet<T, N> Nested;
+
+ static typename ceres::Jet<T, N> dummy_precision() {
+ return ceres::Jet<T, N>(1e-12);
+ }
+
+ enum {
+ IsComplex = 0,
+ IsInteger = 0,
+ IsSigned,
+ ReadCost = 1,
+ AddCost = 1,
+ // For Jet types, multiplication is more expensive than addition.
+ MulCost = 3,
+ HasFloatingPoint = 1
+ };
+};
+
+} // namespace Eigen
+
+#endif // CERES_PUBLIC_JET_H_