Let \(\psi\in L^ 2(\mathbb{R}^ d)\) be an admissible wavelet, \(\psi_ \xi(x)= t^{-d/2} \psi\Bigl({x-v\over t}\Bigr)\), \(\xi= (v,t)\), \(G\) the ``\(ax+ b\)''-group, i.e. \(G=\{\xi= (v,t): v\in \mathbb{R}^ d, t>0\}\), \(d\xi= t^{d-1}dv dt\) the left invariant measure on \(G\). For a Borel measure \(\mu\) on \(G\), for which \[ {\mathcal D}(T_ \mu)= \left\{f\in L_ 2(\mathbb{R}^ d): \int_ G |\langle f,\psi_ \xi\rangle|^ 2 d|\mu|<\infty\right\} \] is dense in \(L^ 2(\mathbb{R}^ d)\), a Calderón-Toeplitz operator is defined by the formula \[ \langle T_ \mu f,g\rangle= \int_ G \langle f,\psi_ \xi\rangle\langle\psi_ \xi,g\rangle d\mu, \] where \(f,g\in {\mathcal D}(T_ \mu)\). Calderón-Toeplitz operators are connected with Calderón-Zygmund operators. On the other hand these operators generalize Toeplitz operators defined on weight Bergman spaces on the upper half plane. The author discusses boundness and Schatten ideal criteria for a class Calderón-Toeplitz operators.