A superconducting-phase quantum bit (qubit) involves three or more Josephso
n junctions combined into a superconducting loop and defines one of the pro
mising solid-state device implementations for quantum computing. Recently,
so called pi junctions, Josephson junctions with a ground state characteriz
ed by a pi -phase shift across, have attracted much attention. We show how
to make use of such pi junctions in the construction of superconducting pha
se qubits and discuss the advantage over conventional designs based on magn
etically frustrated loops. Starting from a basic five-junction loop with on
e pi junction, we show how to construct effective junctions with degenerate
minima characterized by phase shifts 0 and pi and superconducting-phase sw
itches. These elements are then combined into a superconducting-phase qubit
which operates exclusively with switches, thus avoiding permanent contact
with the environment through external biasing. The resulting superconductin
g-phase qubits can be understood as the macroscopic analog of the ''quiet''
s-wave-d-waves-wave Josephson-junction qubits introduced by Ioffe et al. [
Nature (London) 398, 679 (1999)].