IntroductionLiving/controlled free radical polymerization (LFRP) techniques such as nitroxide-mediated polymerization, atom transfer polymerization and reversible addition-fragmentation chain transfer (RAFT) polymerization gave rise to new designs and syntheses of well-defined materials with respect to size, shape, polydispersity and functionality. For example, macromolecular architectures such as stars, combs, block copolymers, core-shell nanoparticles and branched structures have become feasible [1][2][3][4][5][6][7][8][9][10][11][12][13][14][15], rendering these materials ideal for applications in biomaterials (e.g. drug delivery devices and diagnostic nanoparticles) and molecular electronics [1,8,[16][17][18][19].The reason why LFRPs give access to such a vast number of highly specific microstructure is that they yield materials with high-functionality and lowpolydispersity indices, PDI, as all radical chains nearly grow uniformly with increasing monomer consumption, i.e. polymerization time (see equation 4.1). Ideally, the chain length i depends solely on the fraction of monomer consumed, c 0 M X (where X denotes monomer conversion and c 0 M the initial monomer concentration) and c 0 LFRP , which is the concentration of the mediating agent before the reaction commenced, that is at t = 0 [1,[5][6][7][20][21][22][23][24].This feature is utilized in many ways for synthetic purposes because the chain length of the polymer product can be conveniently tuned -widely independent from the outer reaction conditions -simply by changing the monomer and mediating agent concentrations. Less realized is, however, that the correlation of equation 4.1 can also be a powerful tool in the hands of a physical chemist for the very same reason: it gives easy access to reactions and kinetic information of radicals with known, and moreover, adjustable size.