Traditional SQUID magnetometers offer an ultimate sensitivity of about
5x10(-8) emu and, depending on the system, tile differential sensitiv
ity call be as good as 1x10(-8) emu. When magnetometers employ superco
nducting solenoids as source of magnetic field, those sensitivities ca
n be reduced to values as low as 1x10(-6) emu at fields of 7 Tesla due
to magnet ''noise''. Magnet noise is especially a problem under condi
tions of continuously ramping applied field, even below 1 Tesla. We ha
v deployed a new sample transport mechanism for the Quantum Design SQU
ID magnetometer (MPMS), capable of oscillating the sample at frequenci
es up to 4 Hz. Using this new technique on measurements of small sampl
es, we have demonstrated that differential sensitivities of 3x10(-9) e
mu can be achieved. In addition, the new reciprocating sample motion s
ignificantly attenuates the magnet noise during measurements.