We consider the existence of normalized ground states to the following Sobolev critical Schrodinger systems with linear and nonlinear couplings. { -triangle v(1) + mu (1)v(1) - kappa v(2 )= |v(1)|(2 & lowast;-2)v(1) +xi alpha|v(1)|(alpha-2)|v(2)|beta(v1), in R-N, -triangle v(2) + mu 2v(2) - kappa v(1) = |v(2)|(2 & lowast;-2)v(2) +xi beta|v(1)|alpha|v(2)|beta-2(v2), in R-N, integral(RN) v(1)(2)dx= a(2)(1),integral(RN) v(2)(2)dx = a(2)(2), where N = 3 or 4, a1, a2 > 0, kappa is an element of R, xi>0, alpha>1, beta>1, alpha+beta is an element of (2, 2 & lowast;]\{2+ 4/N } and 2 & lowast; = 2N /N-2. Firstly, in the case alpha+ beta<2 + 4/N, by Ekeland's variational principle, we prove for any xi > 0, kappa > 0, the system admits a radially symmetric normalized solution provided a1, a2 are small; secondly, when 2 + 4N <alpha+ beta < 2 & lowast;, we also employ Ekeland's variational principle to prove that for any a1, a2 > 0, there are two positive constants xi(& lowast;& lowast;) and xi(& lowast;) with xi(& lowast;& lowast; )> xi(& lowast;) > 0 such that for any xi is an element of (xi(& lowast;), xi(& lowast;& lowast;)), the system possesses a radially symmetric normalized ground state solution whenever kappa is an element of (0, kappa<overline>) for some kappa<overline> > 0. In both cases above, we overcome the lack of compactness of the L2-norm by virtue of some delicate energy estimates. Finally, when alpha + beta = 2(& lowast;), we prove that the system does not have any nontrivial nonnegative solutions.