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SHORT VERSION: Does the Meyers-Serrin theorem hold on complete, non-compact Riemannian manifolds, i.e. $W^{k,p}(M) = H^{k,p}(M)$? My guess is that this holds for the special case $k=1$ (and all $p\geq 1$), and can fail to hold in general, but I didn't find any explicit reference in the literature.

LONG VERSION: As it is well known (?), many facts about Sobolev spaces that are well known on $\mathbb{R}^n$ are no longer true when the base space is a complete, non-compact Riemannian manifold (e.g. $C^\infty_c(M)$ is not necessarily dense in $H^{k}(M)$, for $k \geq 2$). This is mostly a reference request about the very definition of Sobolev spaces on manifolds.

On $\mathbb{R}^n$, Sobolev spaces are usually defined in two ways. I'm mainly interested in the case $p=2$ and $k=1$, so I will stick to this case.

The first definition is as follows:

$$W^{1,2}(\mathbb{R}^n):=\{u \in L^2(\mathbb{R}^n) \mid D_i u \in L^2(\mathbb{R}^n),\; \forall i =1,\ldots,n\},$$

where $D_i u$ is a partial derivative in the sense of distributions. $W^{1,2}(\mathbb{R}^n)$ is equipped with the norm

$$\|u\|_{W^{1,2}(\mathbb{R}^n)}^2 = \|u\|^2_{L^2(\mathbb{R}^n)} + \sum_{i=1}^n \| D_i u \|^2_{L^2(\mathbb{R}^n)}.$$

The second definition is as the completion

$$ H^{1,2}(\mathbb{R}^n):=\overline{C^\infty(\mathbb{R}^n) \cap W^{1,2}(\mathbb{R}^n)},$$

with the norm defined above.

It is a textbook result (Meyers-Serrin theorem) that $W^{1,2}(\mathbb{R}^n) = H^{1,2}(\mathbb{R}^n)$, i.e. the two definitions are equivalent. Actually $W^{k,p}(\mathbb{R}^n) = H^{k,p}(\mathbb{R}^n)$ for all $k \in \mathbb{N},p \geq 1$.

What happens on manifolds? Let $M$ be a Riemannian manifold (not compact, in general, but always without boundary and complete). Hebey, in his book (Chapter 3), defines Sobolev space $H^{1,2}(M)$, in the non-compact case, as the closure of the space $C^\infty(M)$ of smooth functions with the norm

$$\| u\|_{W^{1,2}(M)}^2:= \|u\|^2_{L^2(M)} + \int_M g(\nabla u,\nabla u) d\mu.$$

The fact that he does not present a definition similar to $W^{1,2}(\mathbb{R}^n)$ for manifolds made me wonder. For a Riemannian manifold $M$ and an $L^2_{\mathrm{loc}}(M)$ function, the weak gradient $\nabla u$ is the following linear functional on smooth, compactly supported sections:

$$ \nabla u[ X] := (u, \nabla^* X)_{L^2(M)}, \qquad \forall X \in \Gamma_c^{\infty}(TM), $$

where $\nabla^* X = - \mathrm{div}(X)$ is the formal adjoint. If there exists an $L^2$ section $V$ of $TM$ such that

$$ (u,\nabla^* X) = \int_M g(V,X) d\omega, $$

then we say that $V = \nabla u \in L^2(TM)$. Then, we can define

$$ W^{1,2}(M) := \{ u \in L^2(M) \mid \nabla u \in L^2(TM) \}$$,

equipped with the norm

$$ \| u\|^2_{W^{1,2}(M)} : = \|u\|^2_{L^2(M)} + \int_M g(\nabla u,\nabla u)d\omega. $$

Does this definition make sense? Why did Hebey not mention it in his book (while he mentions both the possible definitions and their equivalence in the case of $M=\mathbb{R}^n$)? Are the two definitions equivalent? Is there a standard reference where the definition of $W^{1,2}(M)$ as above is presented ?

SHORT VERSION: Does the Meyers-Serrin theorem hold on complete, non-compact Riemannian manifolds, i.e. $W^{k,p}(M) = H^{k,p}(M)$? My guess is that this holds for the special case $k=1$ (and all $p\geq 1$), and can fail to hold in general, but I didn't find any explicit reference in the literature.

LONG VERSION: As it is well known (?), many facts about Sobolev spaces that are well known on $\mathbb{R}^n$ are no longer true when the base space is a complete, non-compact Riemannian manifold (e.g. $C^\infty_c(M)$ is not necessarily dense in $H^{k}(M)$, for $k \geq 2$).

On $\mathbb{R}^n$, Sobolev spaces are usually defined in two ways. I'm mainly interested in the case $p=2$ and $k=1$, so I will stick to this case.

The first definition is as follows:

$$W^{1,2}(\mathbb{R}^n):=\{u \in L^2(\mathbb{R}^n) \mid D_i u \in L^2(\mathbb{R}^n),\; \forall i =1,\ldots,n\},$$

where $D_i u$ is a derivative in the sense of distributions. $W^{1,2}(\mathbb{R}^n)$ is equipped with the norm

$$\|u\|_{W^{1,2}(\mathbb{R}^n)}^2 = \|u\|^2_{L^2(\mathbb{R}^n)} + \sum_{i=1}^n \| D_i u \|^2_{L^2(\mathbb{R}^n)}.$$

The second definition is as the completion

$$ H^{1,2}(\mathbb{R}^n):=\overline{C^\infty(\mathbb{R}^n) \cap W^{1,2}(\mathbb{R}^n)},$$

with the norm defined above.

It is a textbook result (Meyers-Serrin theorem) that $W^{1,2}(\mathbb{R}^n) = H^{1,2}(\mathbb{R}^n)$, i.e. the two definitions are equivalent. Actually $W^{k,p}(\mathbb{R}^n) = H^{k,p}(\mathbb{R}^n)$ for all $k \in \mathbb{N},p \geq 1$.

What happens on manifolds? Let $M$ be a Riemannian manifold (not compact, in general, but always without boundary and complete). Hebey, in his book (Chapter 3), defines Sobolev space $H^{1,2}(M)$, in the non-compact case, as the closure of the space $C^\infty(M)$ of smooth functions with the norm

$$\| u\|_{W^{1,2}(M)}^2:= \|u\|^2_{L^2(M)} + \int_M g(\nabla u,\nabla u) d\mu.$$

The fact that he does not present a definition similar to $W^{1,2}(\mathbb{R}^n)$ for manifolds made me wonder. For a Riemannian manifold $M$ and an $L^2_{\mathrm{loc}}(M)$ function, the weak gradient $\nabla u$ is the following linear functional on smooth, compactly supported sections:

$$ \nabla u[ X] := (u, \nabla^* X)_{L^2(M)}, \qquad \forall X \in \Gamma_c^{\infty}(TM), $$

where $\nabla^* X = - \mathrm{div}(X)$ is the formal adjoint. If there exists an $L^2$ section $V$ of $TM$ such that

$$ (u,\nabla^* X) = \int_M g(V,X) d\omega, $$

then we say that $V = \nabla u \in L^2(TM)$. Then, we can define

$$ W^{1,2}(M) := \{ u \in L^2(M) \mid \nabla u \in L^2(TM) \}$$,

equipped with the norm

$$ \| u\|^2_{W^{1,2}(M)} : = \|u\|^2_{L^2(M)} + \int_M g(\nabla u,\nabla u)d\omega. $$

Does this definition make sense? Why did Hebey not mention it in his book (while he mentions both the possible definitions and their equivalence in the case of $M=\mathbb{R}^n$)? Are the two definitions equivalent? Is there a standard reference where the definition of $W^{1,2}(M)$ as above is presented ?

SHORT VERSION: Does the Meyers-Serrin theorem hold on complete, non-compact Riemannian manifolds, i.e. $W^{k,p}(M) = H^{k,p}(M)$? My guess is that this holds for $k=1$ (and all $p\geq 1$), and can fail to hold in general, but I didn't find any explicit reference in the literature.

LONG VERSION: As it is well known (?), many facts about Sobolev spaces that are well known on $\mathbb{R}^n$ are no longer true when the base space is a complete, non-compact Riemannian manifold (e.g. $C^\infty_c(M)$ is not necessarily dense in $H^{k}(M)$, for $k \geq 2$). This is mostly a reference request about the very definition of Sobolev spaces on manifolds.

On $\mathbb{R}^n$, Sobolev spaces are usually defined in two ways. I'm mainly interested in the case $p=2$ and $k=1$, so I will stick to this case.

The first definition is as follows:

$$W^{1,2}(\mathbb{R}^n):=\{u \in L^2(\mathbb{R}^n) \mid D_i u \in L^2(\mathbb{R}^n),\; \forall i =1,\ldots,n\},$$

where $D_i u$ is a partial derivative in the sense of distributions. $W^{1,2}(\mathbb{R}^n)$ is equipped with the norm

$$\|u\|_{W^{1,2}(\mathbb{R}^n)}^2 = \|u\|^2_{L^2(\mathbb{R}^n)} + \sum_{i=1}^n \| D_i u \|^2_{L^2(\mathbb{R}^n)}.$$

The second definition is as the completion

$$ H^{1,2}(\mathbb{R}^n):=\overline{C^\infty(\mathbb{R}^n) \cap W^{1,2}(\mathbb{R}^n)},$$

with the norm defined above.

It is a textbook result (Meyers-Serrin theorem) that $W^{1,2}(\mathbb{R}^n) = H^{1,2}(\mathbb{R}^n)$, i.e. the two definitions are equivalent. Actually $W^{k,p}(\mathbb{R}^n) = H^{k,p}(\mathbb{R}^n)$ for all $k \in \mathbb{N},p \geq 1$.

What happens on manifolds? Let $M$ be a Riemannian manifold (not compact, in general, but always without boundary and complete). Hebey, in his book (Chapter 3), defines Sobolev space $H^{1,2}(M)$, in the non-compact case, as the closure of the space $C^\infty(M)$ of smooth functions with the norm

$$\| u\|_{W^{1,2}(M)}^2:= \|u\|^2_{L^2(M)} + \int_M g(\nabla u,\nabla u) d\mu.$$

The fact that he does not present a definition similar to $W^{1,2}(\mathbb{R}^n)$ for manifolds made me wonder. For a Riemannian manifold $M$ and an $L^2_{\mathrm{loc}}(M)$ function, the weak gradient $\nabla u$ is the following linear functional on smooth, compactly supported sections:

$$ \nabla u[ X] := (u, \nabla^* X)_{L^2(M)}, \qquad \forall X \in \Gamma_c^{\infty}(TM), $$

where $\nabla^* X = - \mathrm{div}(X)$ is the formal adjoint. If there exists an $L^2$ section $V$ of $TM$ such that

$$ (u,\nabla^* X) = \int_M g(V,X) d\omega, $$

then we say that $V = \nabla u \in L^2(TM)$. Then, we can define

$$ W^{1,2}(M) := \{ u \in L^2(M) \mid \nabla u \in L^2(TM) \}$$,

equipped with the norm

$$ \| u\|^2_{W^{1,2}(M)} : = \|u\|^2_{L^2(M)} + \int_M g(\nabla u,\nabla u)d\omega. $$

Does this definition make sense? Why did Hebey not mention it in his book (while he mentions both the possible definitions and their equivalence in the case of $M=\mathbb{R}^n$)? Are the two definitions equivalent? Is there a standard reference where the definition of $W^{1,2}(M)$ as above is presented ?

SHORT VERSION: Does the Meyers-Serrin theorem hold on complete, non-compact Riemannian manifolds, i.e. $W^{k,p}(M) = H^{k,p}(M)$? My guess is that this holds for the special case $k=1$ (and all $p\geq 1$), and can fail to hold in general, but I didn't find any explicit reference in the literature.

LONG VERSION: As it is well known (?), many facts about Sobolev spaces that are well known on $\mathbb{R}^n$ are no longer true when the base space is a complete, non-compact Riemannian manifold (e.g. $C^\infty_c(M)$ is not necessarily dense in $H^{k}(M)$, for $k \geq 2$). This is mostly a reference request about the very definition of Sobolev spaces on manifolds.

On $\mathbb{R}^n$, Sobolev spaces are usually defined in two ways. I'm mainly interested in the case $p=2$ and $k=1$, so I will stick to this case.

The first definition is as follows:

$$W^{1,2}(\mathbb{R}^n):=\{u \in L^2(\mathbb{R}^n) \mid D_i u \in L^2(\mathbb{R}^n),\; \forall i =1,\ldots,n\},$$

where $D_i u$ is a partial derivative in the sense of distributions. $W^{1,2}(\mathbb{R}^n)$ is equipped with the norm

$$\|u\|_{W^{1,2}(\mathbb{R}^n)}^2 = \|u\|^2_{L^2(\mathbb{R}^n)} + \sum_{i=1}^n \| D_i u \|^2_{L^2(\mathbb{R}^n)}.$$

The second definition is as the completion

$$ H^{1,2}(\mathbb{R}^n):=\overline{C^\infty(\mathbb{R}^n) \cap W^{1,2}(\mathbb{R}^n)},$$

with the norm defined above.

It is a textbook result (Meyers-Serrin theorem) that $W^{1,2}(\mathbb{R}^n) = H^{1,2}(\mathbb{R}^n)$, i.e. the two definitions are equivalent. Actually $W^{k,p}(\mathbb{R}^n) = H^{k,p}(\mathbb{R}^n)$ for all $k \in \mathbb{N},p \geq 1$.

What happens on manifolds? Let $M$ be a Riemannian manifold (not compact, in general, but always without boundary and complete). Hebey, in his book (Chapter 3), defines Sobolev space $H^{1,2}(M)$, in the non-compact case, as the closure of the space $C^\infty(M)$ of smooth functions with the norm

$$\| u\|_{W^{1,2}(M)}^2:= \|u\|^2_{L^2(M)} + \int_M g(\nabla u,\nabla u) d\mu.$$

The fact that he does not present a definition similar to $W^{1,2}(\mathbb{R}^n)$ for manifolds made me wonder. For a Riemannian manifold $M$ and an $L^2_{\mathrm{loc}}(M)$ function, the weak gradient $\nabla u$ is the following linear functional on smooth, compactly supported sections:

$$ \nabla u[ X] := (u, \nabla^* X)_{L^2(M)}, \qquad \forall X \in \Gamma_c^{\infty}(TM), $$

where $\nabla^* X = - \mathrm{div}(X)$ is the formal adjoint. If there exists an $L^2$ section $V$ of $TM$ such that

$$ (u,\nabla^* X) = \int_M g(V,X) d\omega, $$

then we say that $V = \nabla u \in L^2(TM)$. Then, we can define

$$ W^{1,2}(M) := \{ u \in L^2(M) \mid \nabla u \in L^2(TM) \}$$,

equipped with the norm

$$ \| u\|^2_{W^{1,2}(M)} : = \|u\|^2_{L^2(M)} + \int_M g(\nabla u,\nabla u)d\omega. $$

Does this definition make sense? Why did Hebey not mention it in his book (while he mentions both the possible definitions and their equivalence in the case of $M=\mathbb{R}^n$)? Are the two definitions equivalent? Is there a standard reference where the definition of $W^{1,2}(M)$ as above is presented ?

SHORT VERSION: Does the Meyers-Serrin theorem hold on complete, non-compact Riemannian manifolds ?

LONG VERSION: As it is well known, many facts about Sobolev spaces that are well known on $\mathbb{R}^n$ are no longer true when the base space is a complete, non-compact Riemannian manifold (e.g. $C^\infty_c(M)$ is not necessarily dense in $H^{k}(M)$, for $k \geq 2$). This is mostly a reference request about the very definition of Sobolev spaces on manifolds.

On $\mathbb{R}^n$, Sobolev spaces are usually defined in two ways. I'm mainly interested in the case $p=2$ and $k=1$, so I will stick to this case.

The first definition is as follows:

$$W^{1,2}(\mathbb{R}^n):=\{u \in L^2(\mathbb{R}^n) \mid D_i u \in L^2(\mathbb{R}^n),\; \forall i =1,\ldots,n\},$$

where $D_i u$ is a partial derivative in the sense of distributions. $W^{1,2}(\mathbb{R}^n)$ is equipped with the norm

$$\|u\|_{W^{1,2}(\mathbb{R}^n)}^2 = \|u\|^2_{L^2(\mathbb{R}^n)} + \sum_{i=1}^n \| D_i u \|^2_{L^2(\mathbb{R}^n)}.$$

The second definition is as the completion

$$ H^{1,2}(\mathbb{R}^n):=\overline{C^\infty(\mathbb{R}^n) \cap W^{1,2}(\mathbb{R}^n)},$$

with the norm defined above.

It is a textbook result (Meyers-Serrin theorem) that $W^{1,2}(\mathbb{R}^n) = H^{1,2}(\mathbb{R}^n)$, i.e. the two definitions are equivalent. Actually $W^{k,p}(\mathbb{R}^n) = H^{k,p}(\mathbb{R}^n)$ for all $k \in \mathbb{N},p \geq 1$.

What happens on manifolds? Let $M$ be a Riemannian manifold (not compact, in general, but always without boundary and complete). Hebey, in his book (Chapter 3), defines Sobolev space $H^{1,2}(M)$, in the non-compact case, as the closure of the space $C^\infty(M)$ of smooth functions with the norm

$$\| u\|_{W^{1,2}(M)}^2:= \|u\|^2_{L^2(M)} + \int_M g(\nabla u,\nabla u) d\mu.$$

The fact that he does not present a definition similar to $W^{1,2}(\mathbb{R}^n)$ for manifolds made me wonder. For a Riemannian manifold $M$ and an $L^2_{\mathrm{loc}}(M)$ function, the weak gradient $\nabla u$ is the following linear functional on smooth, compactly supported sections:

$$ \nabla u[ X] := (u, \nabla^* X)_{L^2(M)}, \qquad \forall X \in \Gamma_c^{\infty}(TM), $$

where $\nabla^* X = - \mathrm{div}(X)$ is the formal adjoint. If there exists an $L^2$ section $V$ of $TM$ such that

$$ (u,\nabla^* X) = \int_M g(V,X) d\omega, $$

then we say that $V = \nabla u \in L^2(TM)$. Then, we can define

$$ W^{1,2}(M) := \{ u \in L^2(M) \mid \nabla u \in L^2(TM) \}$$,

equipped with the norm

$$ \| u\|^2_{W^{1,2}(M)} : = \|u\|^2_{L^2(M)} + \int_M g(\nabla u,\nabla u)d\omega. $$

Does this definition make sense? Why did Hebey not mention it in his book (while he mentions both the possible definitions and their equivalence in the case of $M=\mathbb{R}^n$)? Are the two definitions equivalent? Is there a standard reference where the definition of $W^{1,2}(M)$ as above is presented ?

SHORT VERSION: Does the Meyers-Serrin theorem hold on complete, non-compact Riemannian manifolds, i.e. $W^{k,p}(M) = H^{k,p}(M)$? My guess is that this holds for $k=1$ (and all $p\geq 1$), and can fail to hold in general, but I didn't find any explicit reference in the literature.

LONG VERSION: As it is well known (?), many facts about Sobolev spaces that are well known on $\mathbb{R}^n$ are no longer true when the base space is a complete, non-compact Riemannian manifold (e.g. $C^\infty_c(M)$ is not necessarily dense in $H^{k}(M)$, for $k \geq 2$). This is mostly a reference request about the very definition of Sobolev spaces on manifolds.

On $\mathbb{R}^n$, Sobolev spaces are usually defined in two ways. I'm mainly interested in the case $p=2$ and $k=1$, so I will stick to this case.

The first definition is as follows:

$$W^{1,2}(\mathbb{R}^n):=\{u \in L^2(\mathbb{R}^n) \mid D_i u \in L^2(\mathbb{R}^n),\; \forall i =1,\ldots,n\},$$

where $D_i u$ is a partial derivative in the sense of distributions. $W^{1,2}(\mathbb{R}^n)$ is equipped with the norm

$$\|u\|_{W^{1,2}(\mathbb{R}^n)}^2 = \|u\|^2_{L^2(\mathbb{R}^n)} + \sum_{i=1}^n \| D_i u \|^2_{L^2(\mathbb{R}^n)}.$$

The second definition is as the completion

$$ H^{1,2}(\mathbb{R}^n):=\overline{C^\infty(\mathbb{R}^n) \cap W^{1,2}(\mathbb{R}^n)},$$

with the norm defined above.

It is a textbook result (Meyers-Serrin theorem) that $W^{1,2}(\mathbb{R}^n) = H^{1,2}(\mathbb{R}^n)$, i.e. the two definitions are equivalent. Actually $W^{k,p}(\mathbb{R}^n) = H^{k,p}(\mathbb{R}^n)$ for all $k \in \mathbb{N},p \geq 1$.

What happens on manifolds? Let $M$ be a Riemannian manifold (not compact, in general, but always without boundary and complete). Hebey, in his book (Chapter 3), defines Sobolev space $H^{1,2}(M)$, in the non-compact case, as the closure of the space $C^\infty(M)$ of smooth functions with the norm

$$\| u\|_{W^{1,2}(M)}^2:= \|u\|^2_{L^2(M)} + \int_M g(\nabla u,\nabla u) d\mu.$$

The fact that he does not present a definition similar to $W^{1,2}(\mathbb{R}^n)$ for manifolds made me wonder. For a Riemannian manifold $M$ and an $L^2_{\mathrm{loc}}(M)$ function, the weak gradient $\nabla u$ is the following linear functional on smooth, compactly supported sections:

$$ \nabla u[ X] := (u, \nabla^* X)_{L^2(M)}, \qquad \forall X \in \Gamma_c^{\infty}(TM), $$

where $\nabla^* X = - \mathrm{div}(X)$ is the formal adjoint. If there exists an $L^2$ section $V$ of $TM$ such that

$$ (u,\nabla^* X) = \int_M g(V,X) d\omega, $$

then we say that $V = \nabla u \in L^2(TM)$. Then, we can define

$$ W^{1,2}(M) := \{ u \in L^2(M) \mid \nabla u \in L^2(TM) \}$$,

equipped with the norm

$$ \| u\|^2_{W^{1,2}(M)} : = \|u\|^2_{L^2(M)} + \int_M g(\nabla u,\nabla u)d\omega. $$

Does this definition make sense? Why did Hebey not mention it in his book (while he mentions both the possible definitions and their equivalence in the case of $M=\mathbb{R}^n$)? Are the two definitions equivalent? Is there a standard reference where the definition of $W^{1,2}(M)$ as above is presented ?