Understanding the coupling mechanism between SQUID (superconducting qu
antum interference device) loop and resonator in high-frequency SQUIDs
is essential for the application of these devices in sensitive magnet
ometers or controllable microwave devices. We have investigated, there
fore, two kinds of planar microstrip tank circuit resonators: (1) S-sh
aped lambda/2-resonators with direct or indirect coupling to the SQUID
loop with optional flux-focussing pads and (2) conventional rf-washer
-SQUID structures for which we have found resonant modes of the washer
providing a coupling to the SQUID loop. A lumped element representati
on of SQUID loop and resonator is presented in order to describe the e
ffective SQUID-resonator coupling in case of direct or indirect coupli
ng. According to this approach, the square of-the effective coupling c
onstant k in both cases is equal to the ratio of the magnetic energy s
tored in the SQUID loop to that stored in the resonator. For the indir
ect coupled S-shaped lambda/2-resonators, k can be described in terms
of a geometry-defined mutual inductance. The predictions of the lumped
element description are compared with simulations using a standard fu
ll-wave analysis computer program in order to quantify the effect of t
he different layouts on microwave current distribution and on k. A met
hod for the determination of k by simulation is described, leading to
useful design rules for the optimization of high-frequency SQUIDs. The
simulation results will also be compared with experimental data. (C)
1995 American Institute of Physics.