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

uLtqLxp=(u(t,)Lxpqdt)1/q,1p,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 pqp\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 aqbp\|a\|_q\|b\|_p. In particular, LtLx2L^\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.