Quaternion: Difference between revisions

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Quaternions are a number system which can be used to represent [[rotations]] in 3D space.

~~An extension called~~ [[Dual quaternion]]~~, involving quaternions of dual numbers or two quaternions of real numbers, are able to~~ represent both rotations and translations in 3D space.

Double quaternion allows representing 4D rotations using two quaternions.

[[Dual quaternion]] allows represent both rotations and translations in 3D space.

The algebra of quaternions, double quaternions, and dual quaternions is called Clifford algebras.

==Background==

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The conjugate is <math>\bar{q} = (q_0, -\mathbf{q})</math>.

===Multiplication===

Multiplication is <math>~~\mathbf{~~q} * ~~\mathbf{~~p} = (q_0 p_0 - \mathbf{q} \cdot \mathbf{p}, q_0 \mathbf{p} + p_0 \mathbf{q} + \mathbf{q} \times \mathbf{p})</math>.

Multiplication is <math>q*p = (q_0 p_0 - \mathbf{q} \cdot \mathbf{p}, q_0 \mathbf{p} + p_0 \mathbf{q} + \mathbf{q} \times \mathbf{p})</math>.

Similar to imaginary numbers, <math>\mathbf{i}^2=\mathbf{j}^2=\mathbf{k}^2=\mathbf{i}\mathbf{j}\mathbf{k}=-1</math>.

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The quaternion <math>q=(\cos(\theta/2), \hat{n}_1 \sin(\theta/2), \hat{n}_2 \sin(\theta/2), \hat{n}_3 \sin(\theta/2))</math> is equivalent to the rotation around axis <math>\hat{n}</math> by angle <math>\theta</math>.

The quaternion <math>q=(\cos(\frac{\theta}{2}), \hat{n}_1 \sin(\frac{\theta}{2}), \hat{n}_2 \sin(\frac{\theta}{2}), \hat{n}_3 \sin(\frac{\theta}{2}))=\cos(\frac{\theta}{2}) + \sin(\frac{\theta}{2}) \mathbf{\hat{n}}</math> is equivalent to the rotation around axis <math>\hat{n}</math> by angle <math>\theta</math>.

===Slurp===

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\mathbf{S}_{\text{chord}} = \sum_{k=1}^{N}\left( \min( \Vert (q*p_k) - r_k \Vert, \Vert (q*p_k)+r_k \Vert ) \right)^2

</math>

==Double Quaternions==

Note that double quaternions are different from dual quaternions.

Double quaternions are written as <math>q_1 + \epsilon q_2</math> with <math>\epsilon^2 = 1</math> and applied to a quaternion <math>p</math> representing a point as <math>q_1 p \bar{q}_2</math>.

Dual quaternions are written as <math>q_1 + \varepsilon q_2</math> with <math>\varepsilon^2 = 0</math> and applied to a dual quaternion <math>p</math> representing a point as <math>(q_1 + \varepsilon q_2) p (\bar{q}_1 + \varepsilon \bar{q}_2)</math>

===Cayley Factorization===

See [Federico Thomas].

Any 4D rotation matrix can be decomposed into a right and a left isoclinic rotation matrix:

<math>R^R</math> and <math>R^L</math> can be viewed as a matrix representation of single double quaternion <math>(q_1, q_2)</math>.

For a double quaternion, the 4D rotation written is <math>x' = q_1 x q_2</math>.

The product of left and right isoclinic rotation matrices commute.

Furthermore, the product of two left isoclinic rotation matrices is a left isoclinic rotation matrix. Same with right.

Thus, <math>R_1 R_2 = (R_1^L R_1^R) (R_2^L R_2^R) = (R_1^L R_2^L) (R_1^R R_2^R) = R</math>.

This shows that the composition of two double quaternions will be a double quaternion.

===Approximating 3D Translations using Double quaternions===

See Ge ''et. al.''<ref name="ge1998double"></ref>

<!-- {{hidden | Algebraic Verification |

Suppose our point is <math>\mathbf{x} \in \mathbb{R}^3</math> and our translation has direction <math>\mathbf{d} \in \mathbb{R}^3</math> with distance <math>d</math>.

Let <math>q=1+\frac{d}{2}\mathbf{n}</math> and <math>q^* = 1-\frac{d}{2}\mathbf{n}</math>.

<math>

\begin{aligned}

q(1+\mathbf{x})(q^*)^* &= (1+\frac{d}{2}\mathbf{n})(1+\mathbf{x})(1+\frac{d}{2}\mathbf{n})\\

&= [(1 - \frac{d}{2} \mathbf{n} \cdot \mathbf{x}) + (\frac{d}{2}\mathbf{n} + \mathbf{x} + \frac{d}{2}\mathbf{n} \times \mathbf{x})](1+\frac{d}{2}\mathbf{n})\\

&= \left(1 - \frac{d}{2} \mathbf{n} \cdot \mathbf{x} - ((\frac{d}{2}\mathbf{n} + \mathbf{x} + \frac{d}{2}\mathbf{n} \times \mathbf{x})) \cdot \frac{d}{2} \mathbf{n}\right) + \left(\frac{d}{2}\mathbf{n} + \mathbf{x} + \frac{d}{2}\mathbf{n} \times \mathbf{x} +\frac{d}{2}\mathbf{n} + (\frac{d}{2}\mathbf{n} + \mathbf{x} + \frac{d}{2}\mathbf{n} \times \mathbf{x})\times(\frac{d}{2}\mathbf{n})\right)\\

&= c + \left(d\mathbf{n} + \mathbf{x} + \frac{d}{2}\mathbf{n} \times \mathbf{x} + (\frac{d}{2}\mathbf{n}\times(\frac{d}{2}\mathbf{n}) + \mathbf{x}\times(\frac{d}{2}\mathbf{n}) + (\frac{d}{2}\mathbf{n} \times \mathbf{x})\times(\frac{d}{2}\mathbf{n}))\right)\\

&= c + \left(d\mathbf{n} + \mathbf{x} + \frac{d}{2}\mathbf{n} \times \mathbf{x} + (0 + \mathbf{x}\times(\frac{d}{2}\mathbf{n}) + 0)\right)\\

&= c + \left(d\mathbf{n} + \mathbf{x} + \frac{d}{2}\mathbf{n} \times \mathbf{x} - \frac{d}{2}\mathbf{n}\times \mathbf{x}\right)\\

&= c + \left(\mathbf{x} + d\mathbf{n}\right)\\

\end{aligned}

</math>

}} -->

==Dual Quaternions==

Dual quaternions are used to represent 3D rotations and translations together.

==Combined Point + Frame Alignment Problem==

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==Resources==

* [https://arxiv.org/pdf/1804.03528.pdf The Quaternion-Based Spatial Coordinate and Orientation Frame Alignment Problems by Andrew Hanson] [https://journals.iucr.org/a/issues/2020/04/00/ib5072/ib5072.pdf Edited Paper]

* [https://www.researchgate.net/publication/265550132_Approaching_Dual_Quaternions_From_Matrix_Algebra Approaching Dual Quaternions From Matrix Algebra by Federico Thomas]

* Double Quaternions for Motion Interpolation by Q.J. Ge, Amitabh Varshney, Jai P. Menon, Chu-Fei Chang

* [https://probablydance.com/2017/08/05/intuitive-quaternions/ Less Weird Quaternions by Malte Skarupke]

** Derives rotations as a sequence of reflection and quaternion algebra from wedge products.

** Presents quaternions as a sequence of (90 deg rotation + scaling) operations in 3D space.

==References==

{{reflist|refs=

<ref name="ge1998double">Q.J. Ge, Amitabh Varshney, Jai P. Menon, Chu-Fei Chang (1998) Double Quaternions for Motion Interpolation</ref>

}}

@@ Line 1: / Line 1: @@
 Quaternions are a number system which can be used to represent [[rotations]] in 3D space.
-An extension called [[Dual quaternion]], involving quaternions of dual numbers or two quaternions of real numbers, are able to represent both rotations and translations in 3D space.
+Double quaternion allows representing 4D rotations using two quaternions.
+[[Dual quaternion]] allows represent both rotations and translations in 3D space.
+The algebra of quaternions, double quaternions, and dual quaternions is called Clifford algebras.
 ==Background==
@@ Line 8: / Line 11: @@
 The conjugate is <math>\bar{q} = (q_0, -\mathbf{q})</math>.
 ===Multiplication===
-Multiplication is <math>\mathbf{q} * \mathbf{p} = (q_0 p_0 - \mathbf{q} \cdot \mathbf{p}, q_0 \mathbf{p} + p_0 \mathbf{q} + \mathbf{q} \times \mathbf{p})</math>.
+Multiplication is <math>q*p = (q_0 p_0 - \mathbf{q} \cdot \mathbf{p}, q_0 \mathbf{p} + p_0 \mathbf{q} + \mathbf{q} \times \mathbf{p})</math>.
 Similar to imaginary numbers, <math>\mathbf{i}^2=\mathbf{j}^2=\mathbf{k}^2=\mathbf{i}\mathbf{j}\mathbf{k}=-1</math>.
@@ Line 25: / Line 28: @@
 <math>R(q*p) = R(q) \cdot R(p)</math>
-The quaternion <math>q=(\cos(\theta/2), \hat{n}_1 \sin(\theta/2), \hat{n}_2 \sin(\theta/2), \hat{n}_3 \sin(\theta/2))</math> is equivalent to the rotation around axis <math>\hat{n}</math> by angle <math>\theta</math>.
+The quaternion <math>q=(\cos(\frac{\theta}{2}), \hat{n}_1 \sin(\frac{\theta}{2}), \hat{n}_2 \sin(\frac{\theta}{2}), \hat{n}_3 \sin(\frac{\theta}{2}))=\cos(\frac{\theta}{2}) + \sin(\frac{\theta}{2}) \mathbf{\hat{n}}</math> is equivalent to the rotation around axis <math>\hat{n}</math> by angle <math>\theta</math>.
 ===Slurp===
@@ Line 107: / Line 110: @@
 \mathbf{S}_{\text{chord}} = \sum_{k=1}^{N}\left( \min( \Vert (q*p_k) - r_k \Vert, \Vert (q*p_k)+r_k \Vert ) \right)^2
 </math>
+==Double Quaternions==
+Note that double quaternions are different from dual quaternions.
+Double quaternions are written as <math>q_1 + \epsilon q_2</math> with <math>\epsilon^2 = 1</math> and applied to a quaternion <math>p</math> representing a point as <math>q_1 p \bar{q}_2</math>.
+Dual quaternions are written as <math>q_1 + \varepsilon q_2</math> with <math>\varepsilon^2 = 0</math> and applied to a dual quaternion <math>p</math> representing a point as <math>(q_1 + \varepsilon q_2) p (\bar{q}_1 + \varepsilon \bar{q}_2)</math>
+===Cayley Factorization===
+See [Federico Thomas].
+Any 4D rotation matrix can be decomposed into a right and a left isoclinic rotation matrix:
+<math>R = R^L R^R = R^R R^L</math>
+<math>R^R</math> and <math>R^L</math> can be viewed as a matrix representation of single double quaternion <math>(q_1, q_2)</math>.
+For a double quaternion, the 4D rotation written is <math>x' = q_1 x q_2</math>.
+The product of left and right isoclinic rotation matrices commute.
+Furthermore, the product of two left isoclinic rotation matrices is a left isoclinic rotation matrix. Same with right.
+Thus, <math>R_1 R_2 = (R_1^L R_1^R) (R_2^L R_2^R) = (R_1^L R_2^L) (R_1^R R_2^R) = R</math>.
+This shows that the composition of two double quaternions will be a double quaternion.
+===Approximating 3D Translations using Double quaternions===
+See Ge ''et. al.''<ref name="ge1998double"></ref>
+<!-- {{hidden | Algebraic Verification |
+Suppose our point is <math>\mathbf{x} \in \mathbb{R}^3</math> and our translation has direction <math>\mathbf{d} \in \mathbb{R}^3</math> with distance <math>d</math>.
+Let <math>q=1+\frac{d}{2}\mathbf{n}</math> and <math>q^* = 1-\frac{d}{2}\mathbf{n}</math>.
+<math>
+\begin{aligned}
+q(1+\mathbf{x})(q^*)^* &= (1+\frac{d}{2}\mathbf{n})(1+\mathbf{x})(1+\frac{d}{2}\mathbf{n})\\
+&= [(1 - \frac{d}{2} \mathbf{n} \cdot \mathbf{x}) + (\frac{d}{2}\mathbf{n} + \mathbf{x} + \frac{d}{2}\mathbf{n} \times \mathbf{x})](1+\frac{d}{2}\mathbf{n})\\
+&= \left(1 - \frac{d}{2} \mathbf{n} \cdot \mathbf{x} - ((\frac{d}{2}\mathbf{n} + \mathbf{x} + \frac{d}{2}\mathbf{n} \times \mathbf{x})) \cdot \frac{d}{2} \mathbf{n}\right) + \left(\frac{d}{2}\mathbf{n} + \mathbf{x} + \frac{d}{2}\mathbf{n} \times \mathbf{x} +\frac{d}{2}\mathbf{n} + (\frac{d}{2}\mathbf{n} + \mathbf{x} + \frac{d}{2}\mathbf{n} \times \mathbf{x})\times(\frac{d}{2}\mathbf{n})\right)\\
+&= c + \left(d\mathbf{n} + \mathbf{x} + \frac{d}{2}\mathbf{n} \times \mathbf{x} + (\frac{d}{2}\mathbf{n}\times(\frac{d}{2}\mathbf{n}) + \mathbf{x}\times(\frac{d}{2}\mathbf{n}) + (\frac{d}{2}\mathbf{n} \times \mathbf{x})\times(\frac{d}{2}\mathbf{n}))\right)\\
+&= c + \left(d\mathbf{n} + \mathbf{x} + \frac{d}{2}\mathbf{n} \times \mathbf{x} + (0 + \mathbf{x}\times(\frac{d}{2}\mathbf{n}) + 0)\right)\\
+&= c + \left(d\mathbf{n} + \mathbf{x} + \frac{d}{2}\mathbf{n} \times \mathbf{x} - \frac{d}{2}\mathbf{n}\times \mathbf{x}\right)\\
+&= c + \left(\mathbf{x} + d\mathbf{n}\right)\\
+\end{aligned}
+</math>
+}} -->
+==Dual Quaternions==
+{{main | Dual quaternion}}
+Dual quaternions are used to represent 3D rotations and translations together.
 ==Combined Point + Frame Alignment Problem==
@@ Line 121: / Line 168: @@
 ==Resources==
 * [https://arxiv.org/pdf/1804.03528.pdf The Quaternion-Based Spatial Coordinate and Orientation Frame Alignment Problems by Andrew Hanson] [https://journals.iucr.org/a/issues/2020/04/00/ib5072/ib5072.pdf Edited Paper]
+* [https://www.researchgate.net/publication/265550132_Approaching_Dual_Quaternions_From_Matrix_Algebra Approaching Dual Quaternions From Matrix Algebra by Federico Thomas]
+* Double Quaternions for Motion Interpolation by Q.J. Ge, Amitabh Varshney, Jai P. Menon, Chu-Fei Chang
+* [https://probablydance.com/2017/08/05/intuitive-quaternions/ Less Weird Quaternions by Malte Skarupke]
+** Derives rotations as a sequence of reflection and quaternion algebra from wedge products.
+** Presents quaternions as a sequence of (90 deg rotation + scaling) operations in 3D space.
+==References==
+{{reflist|refs=
+<ref name="ge1998double">Q.J. Ge, Amitabh Varshney, Jai P. Menon, Chu-Fei Chang (1998) Double Quaternions for Motion Interpolation</ref>
+}}