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Conformal Geometric Algebra in Stochastic Optimization Problems ...

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2.2. BASIC CONCEPTS OF GA 49<br />

Def<strong>in</strong>ition 2.6 ( Null blades ):<br />

A blade A 〈k〉 is called a null blade if it squares to zero, or rather<br />

A 〈k〉 · A 〈k〉 = 0.<br />

Null blades can only occur <strong>in</strong> algebras of mixed signature. S<strong>in</strong>ce every blade has a<br />

representation <strong>in</strong> terms of mutually orthogonal vectors, at least one of these vectors<br />

must at the same time be a null vector <strong>in</strong> order to have a null blade.<br />

Example 2.6 ( Null blades ):<br />

Consider the mutually orthogonal vectors z1 = e1, z2 = e2 and z3 = e3 + e4 from<br />

� 3,1 . Their outer product is A 〈k〉 = e1e2e3 + e1e2e4. The square of A 〈k〉 is<br />

due to z2 3 = 0.<br />

A 2 〈k〉 = −(z1z2z3)(z3z2z1) = −z 2 1z 2 2z 2 3 = −(1)(1)(0) = 0<br />

Next to blades it exists another important class of multivectors <strong>in</strong> �p,q.<br />

Def<strong>in</strong>ition 2.7 ( Versor):<br />

A multivector is called a versor iff it can be expressed as the geometric product of<br />

(<strong>in</strong>vertible) non-null vectors.<br />

�<br />

Note that with this def<strong>in</strong>ition any non-null blade is a versor at the same time.<br />

Furthermore, bear <strong>in</strong> m<strong>in</strong>d that<br />

V ∈ �p,q versor �=⇒ V 2 ∈ �.<br />

Another neat application of proposition 2.6 effortlessly shows that<br />

A 〈k〉 bA 〈k〉 = z1z2 ...zk b z1z2 ...zk<br />

=<br />

k (k−1)<br />

(−1) 2 z1z2 ...zk b zkzk−1 ...z1<br />

=<br />

k (k−1)<br />

(−1) 2 z1(z2(...(zk−1(zk b zk)zk−1)...)z2)z1<br />

is (apart from a scalar factor s<strong>in</strong>ce z 2 i �= 1, i ∈ [1,k] � ) noth<strong>in</strong>g but a series of<br />

reflections of b <strong>in</strong> the vectors {z 1...k }. The result of A 〈k〉 bA 〈k〉 is therefore a vector<br />

as well, i.e.<br />

A 〈k〉 bA 〈k〉 ∈ � p,q . (2.40)<br />

It is known from l<strong>in</strong>ear algebra that a vector a can be decomposed with respect<br />

to its component a � <strong>in</strong>side and the component a⊥ outside a certa<strong>in</strong> subspace B 〈l〉<br />

, i.e. a = a � + a⊥. A decomposition with respect to a vector - a 1-blade - is<br />

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