The celebrated Smith–Minkowski–Siegel mass formula expresses the mass of a quadratic lattice  $(L,Q)$ as a product of local factors, called the local densities of
$(L,Q)$ as a product of local factors, called the local densities of  $(L,Q)$. This mass formula is an essential tool for the classification of integral quadratic lattices. In this paper, we will describe the local density formula explicitly by observing the existence of a smooth affine group scheme
$(L,Q)$. This mass formula is an essential tool for the classification of integral quadratic lattices. In this paper, we will describe the local density formula explicitly by observing the existence of a smooth affine group scheme  $\underline{G}$ over
$\underline{G}$ over  $\mathbb{Z}_{2}$ with generic fiber
$\mathbb{Z}_{2}$ with generic fiber  $\text{Aut}_{\mathbb{Q}_{2}}(L,Q)$, which satisfies
$\text{Aut}_{\mathbb{Q}_{2}}(L,Q)$, which satisfies  $\underline{G}(\mathbb{Z}_{2})=\text{Aut}_{\mathbb{Z}_{2}}(L,Q)$. Our method works for any unramified finite extension of
$\underline{G}(\mathbb{Z}_{2})=\text{Aut}_{\mathbb{Z}_{2}}(L,Q)$. Our method works for any unramified finite extension of  $\mathbb{Q}_{2}$. Therefore, we give a long awaited proof for the local density formula of Conway and Sloane and discover its generalization to unramified finite extensions of
$\mathbb{Q}_{2}$. Therefore, we give a long awaited proof for the local density formula of Conway and Sloane and discover its generalization to unramified finite extensions of  $\mathbb{Q}_{2}$. As an example, we give the mass formula for the integral quadratic form
$\mathbb{Q}_{2}$. As an example, we give the mass formula for the integral quadratic form  $Q_{n}(x_{1},\dots ,x_{n})=x_{1}^{2}+\cdots +x_{n}^{2}$ associated to a number field
$Q_{n}(x_{1},\dots ,x_{n})=x_{1}^{2}+\cdots +x_{n}^{2}$ associated to a number field  $k$ which is totally real and such that the ideal
$k$ which is totally real and such that the ideal  $(2)$ is unramified over
$(2)$ is unramified over  $k$.
$k$.