Graduate Difference Between Outer and Tensor

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The discussion clarifies the distinction between the tensor product and the outer product in the context of Hilbert spaces. The tensor product, denoted as u⊗v, combines elements from two spaces U and V, while the outer product, represented as |u><v|, acts as a linear functional. It is suggested that the outer product can be expressed as u⊗_Ov = u⊗v*, indicating a relationship between the two operations. Additionally, the tensor product is identified as a type (2,0) tensor, whereas the outer product is classified as a type (1,1) tensor. The term "outer product" is context-sensitive, with various interpretations in different mathematical frameworks.
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Say, we have two Hilbert spaces ##U## and ##V## and their duals ##U^*, V^*##.
Then, we say, ##u\otimes v~ \epsilon~ U\otimes V##, where ##'\otimes'## is defined as the tensor product of the two spaces, ##U\times V \rightarrow U\otimes V##.

In Dirac's Bra-Ket notation, this is written as, ##u\otimes v:=\left|u\right>\otimes \left| v\right>:=\left|u\right>\left| v\right>##What is the outer product, then?

In Dirac notation, it is written as ##\left|u\right> \left< v\right|##. Which makes it clear that the outer product is a linear functional acting on some ##v'\epsilon ~V## and giving some ##u'\epsilon~ U##, such that ##\left| u'\right>=\left<v|v'\right>\left|v\right>##.
So, would it be correct to say that (##\otimes_O## is the outer product)
$$u\otimes _Ov:=u\otimes v^* $$
for, ##u,~ v,~v^*~\epsilon ~U, V, V^*##, respectively?

Also, would it be correct to say that ##u\otimes v## is a type ##(2,0)## tensor while, ##u\otimes _O v## is a type ##(1,1)## tensor?
 
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The term "outer product" is context sensitive. There are three multiplications which are occasionally called outer:
  1. Graßmann algebra: https://en.wikipedia.org/wiki/Exterior_algebra
  2. Tensor product: https://en.wikipedia.org/wiki/Outer_product
  3. Cross product: https://en.wikipedia.org/wiki/Cross_product
Personally I think that only the first one deserves this attribute, which makes it a tensor product with the additional requirement that ##u \wedge u = 0##. The usage you spoke about looks like you refer to the second one.
 
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