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== The derivative for quaternions ==
Since the time of Hamilton, it has been realized that requiring the independence of the [[derivative]] from the path that a differential follows toward zero is too restrictive: it excludes even <math>\ f(q) = q^2\ </math> from differentiation. Therefore, a direction-dependent derivative is necessary for functions of a quaternion variable.<ref>{{harvp|Hamilton|1866|loc=Chapter
Considering the increment of [[polynomial function]] of quaternionic argument shows that the increment is a linear map of increment of the argument.{{Dubious|date=March 2019}} From this, a definition can be made:
A continuous
<math>\ f: \mathbb H \rightarrow \mathbb H\ </math>
is called ''differentiable on the set'' <math>\ U \subset \mathbb H\ ,</math>
: <math> f(x+h) - f(x) = \frac{\operatorname d f(x)}{\operatorname d x} \circ h + o(h)</math>
where
: <math>\frac{\operatorname d f(x)}{\operatorname d x}:\mathbb H\rightarrow\mathbb H</math>
is [[linear map]] of quaternion algebra <math>\ \mathbb H\ ,</math> and
<math>\ o:\mathbb H\rightarrow \mathbb H\ </math>
: <math>\lim_{a \rightarrow 0} \frac{\ \left|\ o(a)\ \right|\ }{ \left|\ a\ \right| } = 0\ ,</math>
and the notation <math>\ \circ h\ </math> denotes
The linear map
<math>\frac{\operatorname d f(x)}{\operatorname d x}</math>
is called the derivative of the map <math>\ f ~.</math>
On the quaternions, the derivative may be expressed as
: <math>\frac{\operatorname d f(x)}{\operatorname d x} = \sum_s \frac{\operatorname{d}_{s0} f(x)}{\operatorname d x} \otimes \frac{\operatorname{d}_{s1} f(x)}{\operatorname d x} </math>
Therefore, the differential of the map <math>\ f\ </math> may be expressed as follows, with brackets on either side.
:<math>\frac{\operatorname d f(x)}{\operatorname d x}\circ \operatorname d x = \left(\sum_s \frac{\operatorname{d}_{s0} f(x)}{\operatorname d x} \otimes \frac{\operatorname{d}_{s1} f(x)}{\operatorname d x}\right)\circ \operatorname d x = \sum_s \frac{\operatorname{d}_{s0} f(x)}{\operatorname d x} \left( \operatorname d x \right) \frac{\operatorname{d}_{s1} f(x)}{\operatorname d x}</math>
The number of terms in the sum will depend on the function
<math>~~ \frac{\operatorname{d}_{sp}\operatorname d f(x)}{\operatorname d x} ~~ \mathsf{\ for\ } ~~ p = 0, 1 ~~</math> are called
components of derivative.
The derivative of a quaternionic function
: <math>\frac{\operatorname d f(x)}{\operatorname d x}\circ h = \lim_{t\to 0}\
The following equations then hold:
: <math>\frac{\operatorname d\left( f(x) + g(x) \right)}{\operatorname d x} = \frac{\operatorname d f(x)}{\operatorname d x} + \frac{\operatorname d g(x)}{\operatorname d x}</math>
: <math>\frac{\operatorname d\left( f(x)\ g(x)\right)}{\operatorname d x} = \frac{\operatorname d f(x) }{\operatorname d x}\ g(x) + f(x)\ \frac{\operatorname d g(x)}{\operatorname d x}</math>
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: <math>\frac{\operatorname d \left( a\ f(x)\ b\right)}{\operatorname d x}\circ h = a \left(\frac{\operatorname d f(x)}{\operatorname d x}\circ h\right) b</math>
For the function
{| class="wikitable"
|-
| <math> \frac{\operatorname d \left( a\ x\ b \right)}{\operatorname d x} = a \otimes b </math>
|style="background:white;"|  
| <math>
|}
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| <math> \frac{\operatorname{d}_{10} \left(a\ x\ b\right)}{\operatorname d x} = a </math>
|style="background:white;"|  
| <math> \frac{\operatorname{d}_{11} \left(a\ x\ b\right)}{\operatorname d x} = b </math>
|}
Similarly, for the function
{| class="wikitable"
|-
| <math>\frac{\operatorname d x^2}{\operatorname d x}=x \otimes 1 + 1 \otimes x</math>
|style="background:white;"|  
| <math>
|}
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|}
Finally, for the function
{| class="wikitable"
|-
| <math> \frac{\operatorname d x^{-1} }{\operatorname d x} = -x^{-1} \otimes x^{-1}</math>
|style="background:white;"|  
| <math>
|}
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| first = A.
| title = Quaternionic analysis
| journal = [[Mathematical Proceedings of the Cambridge Philosophical Society]]
| volume = 85
| issue = 2
|