3 <meta http-equiv="Content-Type" content="text/html; charset=US-ASCII">
5 <link rel="stylesheet" href="../../math.css" type="text/css">
6 <meta name="generator" content="DocBook XSL Stylesheets V1.79.1">
7 <link rel="home" href="../../index.html" title="Math Toolkit 2.11.0">
8 <link rel="up" href="../double_exponential.html" title="Double-exponential quadrature">
9 <link rel="prev" href="de_thread.html" title="Thread Safety">
10 <link rel="next" href="de_refes.html" title="References">
12 <body bgcolor="white" text="black" link="#0000FF" vlink="#840084" alink="#0000FF">
13 <table cellpadding="2" width="100%"><tr>
14 <td valign="top"><img alt="Boost C++ Libraries" width="277" height="86" src="../../../../../../boost.png"></td>
15 <td align="center"><a href="../../../../../../index.html">Home</a></td>
16 <td align="center"><a href="../../../../../../libs/libraries.htm">Libraries</a></td>
17 <td align="center"><a href="http://www.boost.org/users/people.html">People</a></td>
18 <td align="center"><a href="http://www.boost.org/users/faq.html">FAQ</a></td>
19 <td align="center"><a href="../../../../../../more/index.htm">More</a></td>
22 <div class="spirit-nav">
23 <a accesskey="p" href="de_thread.html"><img src="../../../../../../doc/src/images/prev.png" alt="Prev"></a><a accesskey="u" href="../double_exponential.html"><img src="../../../../../../doc/src/images/up.png" alt="Up"></a><a accesskey="h" href="../../index.html"><img src="../../../../../../doc/src/images/home.png" alt="Home"></a><a accesskey="n" href="de_refes.html"><img src="../../../../../../doc/src/images/next.png" alt="Next"></a>
26 <div class="titlepage"><div><div><h3 class="title">
27 <a name="math_toolkit.double_exponential.de_caveats"></a><a class="link" href="de_caveats.html" title="Caveats">Caveats</a>
28 </h3></div></div></div>
30 A few things to keep in mind while using the tanh-sinh, exp-sinh, and sinh-sinh
34 These routines are <span class="bold"><strong>very</strong></span> aggressive about
35 approaching the endpoint singularities. This allows lots of significant digits
36 to be extracted, but also has another problem: Roundoff error can cause the
37 function to be evaluated at the endpoints. A few ways to avoid this: Narrow
38 up the bounds of integration to say, [a + ε, b - ε], make sure (a+b)/2 and
39 (b-a)/2 are representable, and finally, if you think the compromise between
40 accuracy an usability has gone too far in the direction of accuracy, file
44 Both exp-sinh and sinh-sinh quadratures evaluate the functions they are passed
45 at <span class="bold"><strong>very</strong></span> large argument. You might understand
46 that x<sup>12</sup>exp(-x) is should be zero when x<sup>12</sup> overflows, but IEEE floating point
47 arithmetic does not. Hence <code class="computeroutput"><span class="identifier">std</span><span class="special">::</span><span class="identifier">pow</span><span class="special">(</span><span class="identifier">x</span><span class="special">,</span> <span class="number">12</span><span class="special">)*</span><span class="identifier">std</span><span class="special">::</span><span class="identifier">exp</span><span class="special">(-</span><span class="identifier">x</span><span class="special">)</span></code> is an indeterminate form whenever <code class="computeroutput"><span class="identifier">std</span><span class="special">::</span><span class="identifier">pow</span><span class="special">(</span><span class="identifier">x</span><span class="special">,</span>
48 <span class="number">12</span><span class="special">)</span></code>
49 overflows. So make sure your functions have the correct limiting behavior;
52 <pre class="programlisting"><span class="keyword">auto</span> <span class="identifier">f</span> <span class="special">=</span> <span class="special">[](</span><span class="keyword">double</span> <span class="identifier">x</span><span class="special">)</span> <span class="special">{</span>
53 <span class="keyword">double</span> <span class="identifier">t</span> <span class="special">=</span> <span class="identifier">exp</span><span class="special">(-</span><span class="identifier">x</span><span class="special">);</span>
54 <span class="keyword">if</span><span class="special">(</span><span class="identifier">t</span> <span class="special">==</span> <span class="number">0</span><span class="special">)</span>
55 <span class="special">{</span>
56 <span class="keyword">return</span> <span class="number">0</span><span class="special">;</span>
57 <span class="special">}</span>
58 <span class="keyword">return</span> <span class="identifier">t</span><span class="special">*</span><span class="identifier">pow</span><span class="special">(</span><span class="identifier">x</span><span class="special">,</span> <span class="number">12</span><span class="special">);</span>
59 <span class="special">};</span>
62 has the correct behavior for large <span class="emphasis"><em>x</em></span>, but <code class="computeroutput"><span class="keyword">auto</span> <span class="identifier">f</span> <span class="special">=</span> <span class="special">[](</span><span class="keyword">double</span>
63 <span class="identifier">x</span><span class="special">)</span> <span class="special">{</span> <span class="keyword">return</span> <span class="identifier">exp</span><span class="special">(-</span><span class="identifier">x</span><span class="special">)*</span><span class="identifier">pow</span><span class="special">(</span><span class="identifier">x</span><span class="special">,</span> <span class="number">12</span><span class="special">);</span> <span class="special">};</span></code> does
67 Oscillatory integrals, such as the sinc integral, are poorly approximated
68 by double-exponential quadrature. Fortunately the error estimates and L1
69 norm are massive for these integrals, but nonetheless, oscillatory integrals
70 require different techniques.
73 A special mention should be made about integrating through zero: while our
74 range adaptors preserve precision when one endpoint is zero, things get harder
75 when the origin is neither in the center of the range, nor at an endpoint.
78 <div class="blockquote"><blockquote class="blockquote"><p>
79 <span class="serif_italic">1 / (1 +x^2)</span>
80 </p></blockquote></div>
82 Over (a, ∞). As long as <code class="computeroutput"><span class="identifier">a</span> <span class="special">>=</span> <span class="number">0</span></code> both
83 the tanh_sinh and the exp_sinh integrators will handle this just fine: in
84 fact they provide a rather efficient method for this kind of integral. However,
85 if we have <code class="computeroutput"><span class="identifier">a</span> <span class="special"><</span>
86 <span class="number">0</span></code> then we are forced to adapt the range
87 in a way that produces abscissa values near zero that have an absolute error
88 of ε, and since all of the area of the integral is near zero both integrators
89 thrash around trying to reach the target accuracy, but never actually get
90 there for <code class="computeroutput"><span class="identifier">a</span> <span class="special"><<</span>
91 <span class="number">0</span></code>. On the other hand, the simple expedient
92 of breaking the integral into two domains: (a, 0) and (0, b) and integrating
93 each seperately using the tanh-sinh integrator, works just fine.
96 Finally, some endpoint singularities are too strong to be handled by <code class="computeroutput"><span class="identifier">tanh_sinh</span></code> or equivalent methods, for example
97 consider integrating the function:
99 <pre class="programlisting"><span class="keyword">double</span> <span class="identifier">p</span> <span class="special">=</span> <span class="identifier">some_value</span><span class="special">;</span>
100 <span class="identifier">tanh_sinh</span><span class="special"><</span><span class="keyword">double</span><span class="special">></span> <span class="identifier">integrator</span><span class="special">;</span>
101 <span class="keyword">auto</span> <span class="identifier">f</span> <span class="special">=</span> <span class="special">[&](</span><span class="keyword">double</span> <span class="identifier">x</span><span class="special">){</span> <span class="keyword">return</span> <span class="identifier">pow</span><span class="special">(</span><span class="identifier">tan</span><span class="special">(</span><span class="identifier">x</span><span class="special">),</span> <span class="identifier">p</span><span class="special">);</span> <span class="special">};</span>
102 <span class="keyword">auto</span> <span class="identifier">Q</span> <span class="special">=</span> <span class="identifier">integrator</span><span class="special">.</span><span class="identifier">integrate</span><span class="special">(</span><span class="identifier">f</span><span class="special">,</span> <span class="number">0</span><span class="special">,</span> <span class="identifier">constants</span><span class="special">::</span><span class="identifier">half_pi</span><span class="special"><</span><span class="keyword">double</span><span class="special">>());</span>
105 The first problem with this function, is that the singularity is at π/2, so
106 if we're integrating over (0, π/2) then we can never approach closer to the
107 singularity than ε, and for p less than but close to 1, we need to get <span class="emphasis"><em>very</em></span>
108 close to the singularity to find all the area under the function. If we recall
109 the identity <code class="literal">tan(π/2 - x) == 1/tan(x)</code> then we can rewrite
110 the function like this:
112 <pre class="programlisting"><span class="keyword">auto</span> <span class="identifier">f</span> <span class="special">=</span> <span class="special">[&](</span><span class="keyword">double</span> <span class="identifier">x</span><span class="special">){</span> <span class="keyword">return</span> <span class="identifier">pow</span><span class="special">(</span><span class="identifier">tan</span><span class="special">(</span><span class="identifier">x</span><span class="special">),</span> <span class="special">-</span><span class="identifier">p</span><span class="special">);</span> <span class="special">};</span>
115 And now the singularity is at the origin and we can get much closer to it
116 when evaluating the integral: all we have done is swap the integral endpoints
120 This actually works just fine for p < 0.95, but after that the <code class="computeroutput"><span class="identifier">tanh_sinh</span></code> integrator starts thrashing around
121 and is unable to converge on the integral. The problem is actually a lack
122 of exponent range: if we simply swap type double for something with a greater
123 exponent range (an 80-bit long double or a quad precision type), then we
124 can get to at least p = 0.99. If we want to go beyond that, or stick with
125 type double, then we have to get smart.
128 The easiest method is to notice that for small x, then <code class="literal">tan(x) ≅ x</code>,
129 and so we are simply integrating x<sup>-p</sup>. Therefore we can use this approximation
130 over (0, small), and integrate numerically from (small, π/2), using ε as a suitable
131 crossover point seems sensible:
133 <pre class="programlisting"><span class="keyword">double</span> <span class="identifier">p</span> <span class="special">=</span> <span class="identifier">some_value</span><span class="special">;</span>
134 <span class="keyword">double</span> <span class="identifier">crossover</span> <span class="special">=</span> <span class="identifier">std</span><span class="special">::</span><span class="identifier">numeric_limits</span><span class="special"><</span><span class="keyword">double</span><span class="special">>::</span><span class="identifier">epsilon</span><span class="special">();</span>
135 <span class="identifier">tanh_sinh</span><span class="special"><</span><span class="keyword">double</span><span class="special">></span> <span class="identifier">integrator</span><span class="special">;</span>
136 <span class="keyword">auto</span> <span class="identifier">f</span> <span class="special">=</span> <span class="special">[&](</span><span class="keyword">double</span> <span class="identifier">x</span><span class="special">){</span> <span class="keyword">return</span> <span class="identifier">pow</span><span class="special">(</span><span class="identifier">tan</span><span class="special">(</span><span class="identifier">x</span><span class="special">),</span> <span class="identifier">p</span><span class="special">);</span> <span class="special">};</span>
137 <span class="keyword">auto</span> <span class="identifier">Q</span> <span class="special">=</span> <span class="identifier">integrator</span><span class="special">.</span><span class="identifier">integrate</span><span class="special">(</span><span class="identifier">f</span><span class="special">,</span> <span class="identifier">crossover</span><span class="special">,</span> <span class="identifier">constants</span><span class="special">::</span><span class="identifier">half_pi</span><span class="special"><</span><span class="keyword">double</span><span class="special">>())</span> <span class="special">+</span> <span class="identifier">pow</span><span class="special">(</span><span class="identifier">crossover</span><span class="special">,</span> <span class="number">1</span> <span class="special">-</span> <span class="identifier">p</span><span class="special">)</span> <span class="special">/</span> <span class="special">(</span><span class="number">1</span> <span class="special">-</span> <span class="identifier">p</span><span class="special">);</span>
140 There is an alternative, more complex method, which is applicable when we
141 are dealing with expressions which can be simplified by evaluating by logs.
142 Let's suppose that as in this case, all the area under the graph is infinitely
143 close to zero, now inagine that we could expand that region out over a much
144 larger range of abscissa values: that's exactly what happens if we perform
145 argument substitution, replacing <code class="computeroutput"><span class="identifier">x</span></code>
146 by <code class="computeroutput"><span class="identifier">exp</span><span class="special">(-</span><span class="identifier">x</span><span class="special">)</span></code> (note
147 that we must also multiply by the derivative of <code class="computeroutput"><span class="identifier">exp</span><span class="special">(-</span><span class="identifier">x</span><span class="special">)</span></code>).
148 Now the singularity at zero is moved to +∞, and the π/2 bound to -log(π/2).
149 Initially our argument substituted function looks like:
151 <pre class="programlisting"><span class="keyword">auto</span> <span class="identifier">f</span> <span class="special">=</span> <span class="special">[&](</span><span class="keyword">double</span> <span class="identifier">x</span><span class="special">){</span> <span class="keyword">return</span> <span class="identifier">exp</span><span class="special">(-</span><span class="identifier">x</span><span class="special">)</span> <span class="special">*</span> <span class="identifier">pow</span><span class="special">(</span><span class="identifier">tan</span><span class="special">(</span><span class="identifier">exp</span><span class="special">(-</span><span class="identifier">x</span><span class="special">)),</span> <span class="special">-</span><span class="identifier">p</span><span class="special">);</span> <span class="special">};</span>
154 Which is hardly any better, as we still run out of exponent range just as
155 before. However, if we replace <code class="computeroutput"><span class="identifier">tan</span><span class="special">(</span><span class="identifier">exp</span><span class="special">(-</span><span class="identifier">x</span><span class="special">))</span></code> by
156 <code class="computeroutput"><span class="identifier">exp</span><span class="special">(-</span><span class="identifier">x</span><span class="special">)</span></code> for
157 suitably small <code class="computeroutput"><span class="identifier">exp</span><span class="special">(-</span><span class="identifier">x</span><span class="special">)</span></code>, and
158 therefore <code class="literal">x > -log(ε)</code>, we can greatly simplify the expression
159 and evaluate by logs:
161 <pre class="programlisting"><span class="keyword">auto</span> <span class="identifier">f</span> <span class="special">=</span> <span class="special">[&](</span><span class="keyword">double</span> <span class="identifier">x</span><span class="special">)</span>
162 <span class="special">{</span>
163 <span class="keyword">static</span> <span class="keyword">const</span> <span class="keyword">double</span> <span class="identifier">crossover</span> <span class="special">=</span> <span class="special">-</span><span class="identifier">log</span><span class="special">(</span><span class="identifier">std</span><span class="special">::</span><span class="identifier">numeric_limits</span><span class="special"><</span><span class="keyword">double</span><span class="special">>::</span><span class="identifier">epsilon</span><span class="special">());</span>
164 <span class="keyword">return</span> <span class="identifier">x</span> <span class="special">></span> <span class="identifier">crossover</span> <span class="special">?</span> <span class="identifier">exp</span><span class="special">((</span><span class="identifier">p</span> <span class="special">-</span> <span class="number">1</span><span class="special">)</span> <span class="special">*</span> <span class="identifier">x</span><span class="special">)</span> <span class="special">:</span> <span class="identifier">exp</span><span class="special">(-</span><span class="identifier">x</span><span class="special">)</span> <span class="special">*</span> <span class="identifier">pow</span><span class="special">(</span><span class="identifier">tan</span><span class="special">(</span><span class="identifier">exp</span><span class="special">(-</span><span class="identifier">x</span><span class="special">)),</span> <span class="special">-</span><span class="identifier">p</span><span class="special">);</span>
165 <span class="special">};</span>
168 This form integrates just fine over (-log(π/2), +∞) using either the <code class="computeroutput"><span class="identifier">tanh_sinh</span></code> or <code class="computeroutput"><span class="identifier">exp_sinh</span></code>
172 <table xmlns:rev="http://www.cs.rpi.edu/~gregod/boost/tools/doc/revision" width="100%"><tr>
173 <td align="left"></td>
174 <td align="right"><div class="copyright-footer">Copyright © 2006-2019 Nikhar
175 Agrawal, Anton Bikineev, Paul A. Bristow, Marco Guazzone, Christopher Kormanyos,
176 Hubert Holin, Bruno Lalande, John Maddock, Jeremy Murphy, Matthew Pulver, Johan
177 Råde, Gautam Sewani, Benjamin Sobotta, Nicholas Thompson, Thijs van den Berg,
178 Daryle Walker and Xiaogang Zhang<p>
179 Distributed under the Boost Software License, Version 1.0. (See accompanying
180 file LICENSE_1_0.txt or copy at <a href="http://www.boost.org/LICENSE_1_0.txt" target="_top">http://www.boost.org/LICENSE_1_0.txt</a>)
185 <div class="spirit-nav">
186 <a accesskey="p" href="de_thread.html"><img src="../../../../../../doc/src/images/prev.png" alt="Prev"></a><a accesskey="u" href="../double_exponential.html"><img src="../../../../../../doc/src/images/up.png" alt="Up"></a><a accesskey="h" href="../../index.html"><img src="../../../../../../doc/src/images/home.png" alt="Home"></a><a accesskey="n" href="de_refes.html"><img src="../../../../../../doc/src/images/next.png" alt="Next"></a>