Singular General Relativity - Theory.nipne.ro
Singular General Relativity - Theory.nipne.ro
Singular General Relativity - Theory.nipne.ro
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The mathematics of singularities<br />
Degenerate inner p<strong>ro</strong>duct<br />
Degenerate inner p<strong>ro</strong>duct - algebraic p<strong>ro</strong>perties<br />
Definition<br />
An inner p<strong>ro</strong>duct on a vector space V is a symmetric bilinear form<br />
g ∈ V ∗ ⊗ V ∗ . The pair (V , g) is named inner p<strong>ro</strong>duct space. We use<br />
alternatively the notation 〈u, v〉 := g(u, v), for u, v ∈ V . The inner<br />
p<strong>ro</strong>duct g is degenerate if there is a vector v ∈ V , v ≠ 0, so that<br />
〈u, v〉 = 0 for all u ∈ V , otherwise g is non-degenerate. There is always a<br />
basis, named orthonormal basis, in which g takes a diagonal form:<br />
⎛<br />
⎞<br />
O r<br />
g = ⎝ −I s<br />
⎠ . (5)<br />
+I t<br />
where O r is the ze<strong>ro</strong> operator on R r , and I q , q ∈ {s, t} is the identity<br />
operator in R q . The signature of g is defined as the triple (r, s, t).<br />
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