Let μ be a Borel measure on the Euclidean plane R². Given three (distinct) points x, y and z in R², let R(x, y, z) be the radius of the Euclidean circle that joins all three of them, or +∞ if they are collinear. The Menger curvature c(x, y, z) is defined to be

${\displaystyle c(x,y,z)={\frac {1}{R(x,y,z)}},}$ 

with the natural convention that c(x, y, z) = 0 if x, y and z are collinear. It is also conventional to extend this definition by setting c(x, y, z) = 0 if any of the points x, y and z coincide. The Menger-Melnikov curvature c²(μ) of μ is defined to be

${\displaystyle c^{2}(\mu )=\iiint _{\mathbb {R} ^{2}}c(x,y,z)^{2}\,\mathrm {d} \mu (x)\mathrm {d} \mu (y)\mathrm {d} \mu (z).}$ 

More generally, for α ≥ 0, define c^2α(μ) by

${\displaystyle c^{2\alpha }(\mu )=\iiint _{\mathbb {R} ^{2}}c(x,y,z)^{2\alpha }\,\mathrm {d} \mu (x)\mathrm {d} \mu (y)\mathrm {d} \mu (z).}$ 

One may also refer to the curvature of μ at a given point x:

${\displaystyle c^{2}(\mu ;x)=\iint _{\mathbb {R} ^{2}}c(x,y,z)^{2}\,\mathrm {d} \mu (y)\mathrm {d} \mu (z),}$ 

in which case

${\displaystyle c^{2}(\mu )=\int _{\mathbb {R} ^{2}}c^{2}(\mu ;x)\,\mathrm {d} \mu (x).}$ 

• The trivial measure has zero curvature.
• A Dirac measure δ_a supported at any point a has zero curvature.
• If μ is any measure whose support is contained within a Euclidean line L, then μ has zero curvature. For example, one-dimensional Lebesgue measure on any line (or line segment) has zero curvature.
• The Lebesgue measure defined on all of R² has infinite curvature.
• If μ is the uniform one-dimensional Hausdorff measure on a circle C_r or radius r, then μ has curvature 1/r.

In this section, R² is thought of as the complex plane C. Melnikov and Verdera (1995) showed the precise relation of the boundedness of the Cauchy kernel to the curvature of measures. They proved that if there is some constant C₀ such that

${\displaystyle \mu (B_{r}(x))\leq C_{0}r}$ 

for all x in C and all r > 0, then there is another constant C, depending only on C₀, such that

${\displaystyle \left|6\int _{\mathbb {C} }|{\mathcal {C}}_{\varepsilon }(\mu )(z)|^{2}\,\mathrm {d} \mu (z)-c_{\varepsilon }^{2}(\mu )\right|\leq C\|\mu \|}$ 

for all ε > 0. Here c_ε denotes a truncated version of the Menger-Melnikov curvature in which the integral is taken only over those points x, y and z such that

${\displaystyle |x-y|>\varepsilon ;}$ 

${\displaystyle |y-z|>\varepsilon ;}$ 

${\displaystyle |z-x|>\varepsilon .}$ 

Similarly, ${\displaystyle {\mathcal {C}}_{\varepsilon }}$  denotes a truncated Cauchy integral operator: for a measure μ on C and a point z in C, define

${\displaystyle {\mathcal {C}}_{\varepsilon }(\mu )(z)=\int {\frac {1}{\xi -z}}\,\mathrm {d} \mu (\xi ),}$ 

where the integral is taken over those points ξ in C with

${\displaystyle |\xi -z|>\varepsilon .}$ 

• Mel'nikov, Mark S. (1995). "Analytic capacity: a discrete approach and the curvature of measure". Matematicheskii Sbornik. 186 (6): 57–76. ISSN 0368-8666.
• Melnikov, Mark S.; Verdera, Joan (1995). "A geometric proof of the L² boundedness of the Cauchy integral on Lipschitz graphs". International Mathematics Research Notices. 1995 (7): 325–331. doi:10.1155/S1073792895000249.
• Tolsa, Xavier (2000). "Principal values for the Cauchy integral and rectifiability". Proceedings of the American Mathematical Society. 128 (7): 2111–2119. doi:10.1090/S0002-9939-00-05264-3.