For a jointly measurable u(t,x)u(t,x) on a product of sigma-finite measure spaces, the mixed Lebesgue norm LtqLxpL^q_tL^p_x is

∥u∥LtqLxp=(∫∥u(t,⋅)∥Lxpq dt)1/q,1≤p,q<∞.\|u\|_{L^q_tL^p_x} =\left(\int \|u(t,\cdot)\|_{L^p_x}^{q}\,dt\right)^{1/q}, \qquad 1\le p,q<\infty.

Replace an integral norm by the corresponding when its exponent is infinite. For vector fields use the Euclidean magnitude inside the spatial norm.

Order and examples

The order matters when p≠qp\ne q. If p=q<∞p=q<\infty, Tonelli's theorem identifies the mixed norm with the product-space LpL^p norm. For a separated function u(t,x)=a(t)b(x)u(t,x)=a(t)b(x), it equals ∥a∥q∥b∥p\|a\|_q\|b\|_p. In particular, Lt∞Lx2L^\infty_tL^2_x gives a bound on spatial energy for almost every time, not automatically a chosen representative at every time.

Banach-valued notation

The notation Lq(I;Lp(X))L^q(I;L^p(X)) also commonly denotes a Bochner space. For p=∞p=\infty, strong measurability of the map into L∞(X)L^\infty(X) is an additional issue; joint scalar measurability alone does not always give that property.