The tensor product of a Hilbert space with a finite dimensional vector space and the adjoint operator on that space

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I am really trying hard to understand how to view the tensor product of a Hilbert space with an $n$-dimensional vector space as being isomorphic to an $n$-dimensional Hibert space. The specific statements are in the following. (This is from the book titled "Hypocoercivity" written by Cedric Villani, one of the Fields medalists.)

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(1) Could you help me understand how to view $\mathcal{H} \otimes \mathcal{V}$ as isomorphic to $\mathcal{H}^n$?

(2) Also, here it says the adjoint operator $A^*$. Is it defined from the Hilbert space $\mathcal{H} \otimes \mathcal{V} \to \mathcal{H}$ and $\langle Ah_1, h_2 \rangle_{\mathcal{H} \otimes \mathcal{V}} = \langle h_1, A^{*}h_2 \rangle_{\mathcal{H}} $?

I'd really appreciate it if you'd help me. Thank you.

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Well, there is an isomorphism

$H\otimes_{\Bbb R}{\Bbb R}^m \simeq (H\otimes_{\Bbb R}{\Bbb R})\oplus \ldots \oplus (H\otimes_{\Bbb R}{\Bbb R})$ ($m$-times)

of $\Bbb R$-vector spaces with $H\otimes_{\Bbb R}{\Bbb R}\simeq H$.