#include <kyosu/kyosu.hpp>
#include <eve/wide.hpp>
diff --git a/index.html b/index.html
index b24454db..399680c1 100644
--- a/index.html
+++ b/index.html
@@ -130,7 +130,7 @@
The Cayley-Dickson construction scheme defines a new algebra as a Cartesian product of an algebra with itself, with multiplication defined in a specific way (different from the componentwise multiplication) and an involution known as conjugation.
We currently only implement the Cayley-Dickson algebras based on the IEEE float and double representations of real numbers.
Kyosu proper usable objects are all in the namespace kyosu
.
-
+
Cayley-Dickson algebras
These are algebras over the real numbers with an involution named conjugation. The product of an element by its conjugate is 'real' and its positive square root is a norm on the vector space defined by the algebra.
Starting from the real numbers (supported by type T float or double) we define:
@@ -162,11 +162,11 @@
The functions commutator (resp. associator) can be used to see if two (resp. three) Cayley-Dickson value commute (resp. associate).
Greater dimensions are not even alternative but keep power-associativity which allows to define most elementary functions.
- Note
- Let us recall that alternative means that every subalgrebra generated by two elements is associative.
-
+
What does this implementation provide
All operators and functions implemented can receive a mix of scalar or simd of cayley-dickson and reals of various dimensionnality and are defined in the namespace kyosu.
Of course the algebra operation +, -, * and / are provided, but as \ is not an usable C++ character as an operator, the left division a \ b
is provided as the call ldiv(a,b).
-
+
Constructors
complex and quaternion can be constructed using callables facilities complex
and quaternion
.
complex can also be constructed from their polar representation
@@ -195,13 +195,13 @@
The third column references to the corresponding to_xxx version that gives back the chosen representation from a quaternion input.
TODO cayley_dickson<N> construction by a function.
-
+
Operators
Operators (as said before) +
, -
, *
and /
can be used in infix form and can mix cayley-dickson values of different dimensionalities. Of course the biggest dimensionlity is recovered in the output.
Prefix forms are also provided as add
, sub
, multiply
and div
. Also plus and minus for unary versions.
The left division sometimes necessary if the dimensionality is greater than 2 is given as ldiv
.
The left multiplication to the left by i or -i (i*i=-1) can be done calling respectively muli and mulmi
-
+
Functions
Most KYOSU callables are usable with all cayley_dickson types. The exceptions mainly being rotation related quaternion usage.
- Warning
- EVE callables that correspond to mathematical functions that are only defined on a proper part of the real axis as, for example,
acos
DOES NOT ever provide the same result if called in EVE or KYOSU context.
diff --git a/namespacekyosu.html b/namespacekyosu.html
index fbf9bf8e..fed4e8c6 100644
--- a/namespacekyosu.html
+++ b/namespacekyosu.html
@@ -276,6 +276,21 @@
constexpr auto | average = eve::functor<average_t> |
| Computes the average of the parameters.
|
|
+
constexpr auto | bessel_h = eve::functor<bessel_h_t> |
+
| Computes the spherical or cylindrical Hankel functions, extended to the complex plane and cayley_dickson algebras.
|
+
|
+
constexpr auto | bessel_i = eve::functor<bessel_i_t> |
+
| Computes the spherical or cylindrical modified Bessel functions of the second kind, extended to the complex plane and cayley_dickson algebras.
|
+
|
+
constexpr auto | bessel_j = eve::functor<bessel_j_t> |
+
| Computes the spherical or cylindrical Bessel functions of the first kind, extended to the complex plane and cayley_dickson algebras.
|
+
|
+
constexpr auto | bessel_k = eve::functor<bessel_k_t> |
+
| Computes the spherical or cylindrical modified Bessel functions of the second kind, extended to the complex plane and cayley_dickson algebras.
|
+
|
+
constexpr auto | bessel_y = eve::functor<bessel_y_t> |
+
| Computes the spherical or cylindrical Bessel functions of the second kind, extended to the complex plane and cayley_dickson algebras.
|
+
|
constexpr auto | beta = eve::functor<beta_t> |
| Computes the beta function: \(\displaystyle \mathbf{B}(x, y) = \frac{\Gamma(x)\Gamma(y)}{\Gamma(x+y)}\) for real or complex entries.
|
|
@@ -327,103 +342,6 @@
constexpr auto | cscpi = eve::functor<cscpi_t> |
| Computes the cosecant from the argument in \(\pi\) multiples.
|
|
-
constexpr auto | cyl_bessel_h1 = eve::functor<cyl_bessel_h1_t> |
-
| Computes the Bessel functions of the third kind (Hankel functions) \(H_{\nu}^{(1)}\).
|
-
|
-
constexpr auto | cyl_bessel_h12 = eve::functor<cyl_bessel_h12_t> |
-
| Computes the Hankel functions of the first and second kind,.
|
-
|
-
constexpr auto | cyl_bessel_h12n = eve::functor<cyl_bessel_h12n_t> |
-
| Computes the Hankel functions of the first and second kind,.
|
-
|
-
constexpr auto | cyl_bessel_h12r = eve::functor<cyl_bessel_h12r_t> |
-
| Computes the Hankel functions of the first and second kind,.
|
-
|
-
constexpr auto | cyl_bessel_h1_0 = eve::functor<cyl_bessel_h1_0_t> |
-
| Computes the Bessel function of the third kind, \( H^{(1)}_0(x)\),.
|
-
|
-
constexpr auto | cyl_bessel_h1_1 = eve::functor<cyl_bessel_h1_1_t> |
-
| Computes the Bessel function of the third kind, \( H^{(1)}_1(x)\),.
|
-
|
-
constexpr auto | cyl_bessel_h1n = eve::functor<cyl_bessel_h1n_t> |
-
| Computes the Bessel/Hankel functions of the third kind, \( H_n^{(1)}(z) = J_n(z)+iY_n(z)\).
|
-
|
-
constexpr auto | cyl_bessel_h2 = eve::functor<cyl_bessel_h2_t> |
-
| Computes the Bessel functions of the third kind (Hankel functions) \(H_{\nu}^{(2)}\).
|
-
|
-
constexpr auto | cyl_bessel_h2_0 = eve::functor<cyl_bessel_h2_0_t> |
-
| Computes the Bessel function of the third kind, \( H^{(2)}_0(x)\).
|
-
|
-
constexpr auto | cyl_bessel_h2_1 = eve::functor<cyl_bessel_h2_1_t> |
-
| Computes the Bessel function of the third kind, \( H^{(2)}_1(x)\),.
|
-
|
-
constexpr auto | cyl_bessel_h2n = eve::functor<cyl_bessel_h2n_t> |
-
| Computes the Bessel/Hankel functions of the third kind , \( H_n^{(2)} = J_n(z)-iY_n(z)\).
|
-
|
-
constexpr auto | cyl_bessel_i = eve::functor<cyl_bessel_i_t> |
-
| Computes the modified Bessel functions of the first kind,.
|
-
|
-
constexpr auto | cyl_bessel_i0 = eve::functor<cyl_bessel_i0_t> |
-
| Computes the modified Bessel function of the first kind \(I_{0}(x)=J_{0}(ix)\) extended to the complex plane and cayley_dickson algebras.
|
-
|
-
constexpr auto | cyl_bessel_i1 = eve::functor<cyl_bessel_i1_t> |
-
| Computes the modified Bessel function of the first kind, \( I_1(x)= iJ_1(ix) \) extended to the complex plane and cayley_dickson algebras.
|
-
|
-
constexpr auto | cyl_bessel_ik = eve::functor<cyl_bessel_ik_t> |
-
| Computes the simultaneous Bessel functions of the first and second kind,.
|
-
|
-
constexpr auto | cyl_bessel_ikn = eve::functor<cyl_bessel_ikn_t> |
-
| Computes simultaneously the modified Bessel functions of the first and second kind of integer orders,.
|
-
|
-
constexpr auto | cyl_bessel_in = eve::functor<cyl_bessel_in_t> |
-
| Computes the modified Bessel functions of the first kind \(I_{n}(x)=i^{-n}J_{n }(ix)\), extended to the complex plane and cayley_dickson algebras.
|
-
|
-
constexpr auto | cyl_bessel_j = eve::functor<cyl_bessel_j_t> |
-
| Computes the Bessel functions of the first kind, \( J_{\nu}(x)=\sum_{p=0}^{\infty}{\frac{(-1)^p}{p!\,\Gamma (p+\nu +1)}}
- {\left({x \over 2}\right)}^{2p+\nu }\) extended to the complex plane and cayley_dickson values.
|
-
|
-
constexpr auto | cyl_bessel_j0 = eve::functor<cyl_bessel_j0_t> |
-
| Computes the Bessel function of the first kind, \( J_0(x)=\frac1{\pi }\int _{0}^{\pi}\cos(x\sin \tau)
- \,\mathrm {d} \tau \) extended to the complex plane and cayley_dickson algebras.
|
-
|
-
constexpr auto | cyl_bessel_j1 = eve::functor<cyl_bessel_j1_t> |
-
| Computes the Bessel function of the first kind, \( J_1\).
|
-
|
-
constexpr auto | cyl_bessel_jn = eve::functor<cyl_bessel_jn_t> |
-
| Computes the Bessel functions of the first kind, \( J_{n}(x)=\sum_{p=0}^{\infty}{\frac{(-1)^p}{p!\,\Gamma (p+n +1)}}
- {\left({x \over 2}\right)}^{2p+n }\) extended to the complex plane and cayley_dickson algebras.
|
-
|
-
constexpr auto | cyl_bessel_jy = eve::functor<cyl_bessel_jy_t> |
-
| Computes the simultaneous Bessel functions of the first and second kind,.
|
-
|
-
constexpr auto | cyl_bessel_jyn = eve::functor<cyl_bessel_jyn_t> |
-
| Computes the simultaneous Bessel functions of the first and second kind,.
|
-
|
-
constexpr auto | cyl_bessel_k = eve::functor<cyl_bessel_k_t> |
-
| Computes the Modified Bessel functions of the second kind.
|
-
|
-
constexpr auto | cyl_bessel_k0 = eve::functor<cyl_bessel_k0_t> |
-
| Computes the modified Bessel function of the second kind, \( K_0(x)=\lim_{\alpha\to 0}{\frac {\pi }{2}}{\frac {I_{-\alpha }(x)-I_{\alpha }(x)}{\sin \alpha \pi }}\). extended to the complex plane and cayley_dickson values.
|
-
|
-
constexpr auto | cyl_bessel_k1 = eve::functor<cyl_bessel_k1_t> |
-
| Computes the Bessel function of the second kind, \( K_1(x)\lim_{\alpha\to 1}{\frac {\pi }{2}}{\frac {I_{-\alpha }(x)-I_{\alpha }(x)}{\sin \alpha \pi }}\) extended to the complex plane and cayley_dickson values.
|
-
|
-
constexpr auto | cyl_bessel_kn = eve::functor<cyl_bessel_kn_t> |
-
| Computes the modified Bessel functions of the second kind, \( Y_n(x)=\lim_{\alpha\to n}{{\frac {J_{\alpha }(x)\cos(\alpha\pi)-J_{-\alpha }(x)}{\sin(\alpha\pi)}}}\), extended to the complex plane and cayley_dickson algebras.
|
-
|
-
constexpr auto | cyl_bessel_y = eve::functor<cyl_bessel_y_t> |
-
| Computes the Bessel functions of the first kind, \( J_{\nu}(x)=\sum_{p=0}^{\infty}{\frac{(-1)^p}{p!\,\Gamma (p+\nu +1)}}
- {\left({x \over 2}\right)}^{2p+\nu }\) extended to the complex plane and cayley_dickson values.
|
-
|
-
constexpr auto | cyl_bessel_y0 = eve::functor<cyl_bessel_y0_t> |
-
| Computes the Bessel function of the second kind, \( Y_0(x)=\lim_{\alpha\to 0}{{\frac {J_{\alpha }(x)\cos(\alpha\pi)-J_{-\alpha }(x)}{\sin(\alpha\pi)}}}\), extended to the complex plane and cayley_dickson algebras.
|
-
|
-
constexpr auto | cyl_bessel_y1 = eve::functor<cyl_bessel_y1_t> |
-
| Computes the Bessel function of the second kind, \( Y_1(x)=\lim_{\alpha\to 1}{{\frac {J_{\alpha }(x)\cos(\alpha\pi)-J_{-\alpha }(x)}{\sin(\alpha\pi)}}}\), extended to the complex plane and cayley_dickson algebras.
|
-
|
-
constexpr auto | cyl_bessel_yn = eve::functor<cyl_bessel_yn_t> |
-
| Computes the modified Bessel functions of the second kind, \( Y_n(x)=\lim_{\alpha\to n}{{\frac {J_{\alpha }(x)\cos(\alpha\pi)-J_{-\alpha }(x)}{\sin(\alpha\pi)}}}\), extended to the complex plane and cayley_dickson algebras.
|
-
|
constexpr auto | dec = eve::functor<dec_t> |
| decrements the argument by 1.
|
|
@@ -803,69 +721,6 @@
constexpr auto | slerp = eve::functor<slerp_t> |
| Computes the spherical interpolation between unitary quaternions.
|
|
-
constexpr auto | sph_bessel_h1_0 = eve::functor<sph_bessel_h1_0_t> |
-
| Computes the spherical Bessel/hankel functions of the third kind, \( h_0^{(1)}(z) = j_1(z)+iy_1(z)\).
|
-
|
-
constexpr auto | sph_bessel_h1_1 = eve::functor<sph_bessel_h1_1_t> |
-
| Computes the spherical Bessel/hankel functions of the third kind, \( h_1^{(1)}(z) = j_1(z)+iy_1(z)\).
|
-
|
-
constexpr auto | sph_bessel_h1n = eve::functor<sph_bessel_h1n_t> |
-
| Computes the spherical Bessel/hankel functions of the third kind, \( h_n^{(1)}(z) = j_n(z)+iy_n(z)\).
|
-
|
-
constexpr auto | sph_bessel_h2_0 = eve::functor<sph_bessel_h2_0_t> |
-
| Computes the spherical Bessel/hankel functions of the third kind, \( h_0^{(2)}(z) = j_0(z)-iy_0(z)\).
|
-
|
-
constexpr auto | sph_bessel_h2_1 = eve::functor<sph_bessel_h2_1_t> |
-
| Computes the spherical Bessel/hankel functions of the third kind, \( h_1^{(2)}(z) = j_1(z)-iy_1(z)\).
|
-
|
-
constexpr auto | sph_bessel_h2n = eve::functor<sph_bessel_h2n_t> |
-
| Computes the spherical Bessel/hankel functions of the third kind, \( h_n^{(2)}(z) = j_n(z)-iy_n(z)\).
|
-
|
-
constexpr auto | sph_bessel_i1_0 = eve::functor<sph_bessel_i1_0_t> |
-
| Computes the Bessel function, \( i_0^{(1)}(z) = j_0(iz)\) extended to the complex plane and cayley_dickson algebras.
|
-
|
-
constexpr auto | sph_bessel_i1_1 = eve::functor<sph_bessel_i1_1_t> |
-
| Computes the Bessel function, \( i_1^{(1)}(z) = -i j_1(iz)\) extended to the complex plane and cayley_dickson algebras.
|
-
|
-
constexpr auto | sph_bessel_i1n = eve::functor<sph_bessel_i1n_t> |
-
| Computes the spherical Bessel functions of the first kind, extended to the complex plane and cayley_dickson algebras.
|
-
|
-
constexpr auto | sph_bessel_i2_0 = eve::functor<sph_bessel_i2_0_t> |
-
| Computes the Bessel function, \( i_0^{(2)}(z) = -i y_0(iz)\) extended to the complex plane and cayley_dickson algebras.
|
-
|
-
constexpr auto | sph_bessel_i2_1 = eve::functor<sph_bessel_i2_1_t> |
-
| Computes the Bessel function, \( i_1^{(2)}(z) = -y_1(iz)\) extended to the complex plane and cayley_dickson algebras.
|
-
|
-
constexpr auto | sph_bessel_i2n = eve::functor<sph_bessel_i2n_t> |
-
| Computes the spherical Bessel functions of the first kind, extended to the complex plane and cayley_dickson algebras.
|
-
|
-
constexpr auto | sph_bessel_j0 = eve::functor<sph_bessel_j0_t> |
-
| Computes the Bessel function of the first kind, \( j_0(z)=\sin z/z \) extended to the complex plane and cayley_dickson algebras.
|
-
|
-
constexpr auto | sph_bessel_j1 = eve::functor<sph_bessel_j1_t> |
-
| Computes the Spherical Bessel function of the first kind, \( j_1(z)= \sin z/z^2 -\cos z/z\) extended to the complex plane and cayley_dickson values.
|
-
|
-
constexpr auto | sph_bessel_jn = eve::functor<sph_bessel_jn_t> |
-
| Computes the spherical Bessel functions of the first kind, extended to the complex plane and cayley_dickson algebras.
|
-
|
-
constexpr auto | sph_bessel_k0 = eve::functor<sph_bessel_k0_t> |
-
| Computes the spherical Bessel function of the first kind, \( k_0(z)= \pi e^{-z}/(2z) \) extended to the complex plane and cayley_dickson algebras.
|
-
|
-
constexpr auto | sph_bessel_k1 = eve::functor<sph_bessel_k1_t> |
-
| Computes the spherical Bessel function of the first kind, \( k_1(z)= (\pi/2) e^{-z}(1/z+1/z^2)\) extended to the complex plane and cayley_dickson algebras.
|
-
|
-
constexpr auto | sph_bessel_kn = eve::functor<sph_bessel_kn_t> |
-
| Computes the spherical Bessel functions of the first kind, extended to the complex plane and cayley_dickson algebras.
|
-
|
-
constexpr auto | sph_bessel_y0 = eve::functor<sph_bessel_y0_t> |
-
| Computes the spherical Bessel function of the first kind, \( y_0(x)=\cos z/z \) extended to the complex plane and cayley_dickson algebras.
|
-
|
-
constexpr auto | sph_bessel_y1 = eve::functor<sph_bessel_y1_t> |
-
| Computes the spherical Bessel function of the first kind, \( y_1(x)= -\coz z/z^2 -\sin z/z\) extended to the complex plane and cayley_dickson values.
|
-
|
-
constexpr auto | sph_bessel_yn = eve::functor<sph_bessel_yn_t> |
-
| Computes the spherical Bessel functions of the second kind, extended to the complex plane and cayley_dickson algebras.
|
-
|
constexpr auto | sqr = eve::functor<sqr_t> |
| Computes the square value.
|
|
diff --git a/navtreedata.js b/navtreedata.js
index 0c498387..3baa13bd 100644
--- a/navtreedata.js
+++ b/navtreedata.js
@@ -25,11 +25,11 @@
var NAVTREE =
[
[ "kyosu", "index.html", [
- [ "Cayley-Dickson algebras", "index.html#autotoc_md22", null ],
- [ "What does this implementation provide", "index.html#autotoc_md23", [
- [ "Constructors", "index.html#autotoc_md24", null ],
- [ "Operators", "index.html#autotoc_md25", null ],
- [ "Functions", "index.html#autotoc_md26", null ]
+ [ "Cayley-Dickson algebras", "index.html#autotoc_md23", null ],
+ [ "What does this implementation provide", "index.html#autotoc_md24", [
+ [ "Constructors", "index.html#autotoc_md25", null ],
+ [ "Operators", "index.html#autotoc_md26", null ],
+ [ "Functions", "index.html#autotoc_md27", null ]
] ],
[ "How-Tos", "usergroup0.html", null ],
[ "Reference Documentation", "usergroup1.html", [
diff --git a/navtreeindex0.js b/navtreeindex0.js
index a6d6f578..cd83bd5e 100644
--- a/navtreeindex0.js
+++ b/navtreeindex0.js
@@ -11,11 +11,11 @@ var NAVTREEINDEX0 =
"group__traits.html":[3,3],
"group__types.html":[3,0],
"index.html":[],
-"index.html#autotoc_md22":[0],
-"index.html#autotoc_md23":[1],
-"index.html#autotoc_md24":[1,0],
-"index.html#autotoc_md25":[1,1],
-"index.html#autotoc_md26":[1,2],
+"index.html#autotoc_md23":[0],
+"index.html#autotoc_md24":[1],
+"index.html#autotoc_md25":[1,0],
+"index.html#autotoc_md26":[1,1],
+"index.html#autotoc_md27":[1,2],
"licence.html":[4,0],
"pages.html":[],
"usergroup0.html":[2],
diff --git a/search/all_1.js b/search/all_1.js
index 27838379..ec2a2c73 100644
--- a/search/all_1.js
+++ b/search/all_1.js
@@ -1,4 +1,9 @@
var searchData=
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+ ['bessel_5fh_0',['bessel_h',['../group__functions_ga1d55a602f923650e17ff59f3ce1327f2.html#ga1d55a602f923650e17ff59f3ce1327f2',1,'kyosu']]],
+ ['bessel_5fi_1',['bessel_i',['../group__functions_ga4deb7ab94ca8f87eae86f51e66324d58.html#ga4deb7ab94ca8f87eae86f51e66324d58',1,'kyosu']]],
+ ['bessel_5fj_2',['bessel_j',['../group__functions_ga483502b0a398f721aee5b7095e25e016.html#ga483502b0a398f721aee5b7095e25e016',1,'kyosu']]],
+ ['bessel_5fk_3',['bessel_k',['../group__functions_ga0153dc797fee1fd05255e729f21ce789.html#ga0153dc797fee1fd05255e729f21ce789',1,'kyosu']]],
+ ['bessel_5fy_4',['bessel_y',['../group__functions_ga4e656e84fd3efa77c0c763238c471e24.html#ga4e656e84fd3efa77c0c763238c471e24',1,'kyosu']]],
+ ['beta_5',['beta',['../group__functions_ga64a0550a46270d01b31593e38a364f72.html#ga64a0550a46270d01b31593e38a364f72',1,'kyosu']]]
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diff --git a/search/all_12.js b/search/all_12.js
index f74f6624..4699cf3b 100644
--- a/search/all_12.js
+++ b/search/all_12.js
@@ -14,28 +14,7 @@ var searchData=
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index f334a5cc..62e84e50 100644
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