We report on the first realization of a microwave trap for neutral ato
ms, as proposed originally for use with spin-polarized hydrogen [1]. T
his trap is advantageous for attaining Bose condensation because it ca
n contain strong or weak field seekers, while static magnetic traps co
ntain only the less-stable weak-field seeking states. In this experime
nt, Cs atoms were confined in the microwave field of a room-temperatur
e spherical resonator (Q almost-equal-to 5500) whose TE 110 mode is tu
ned to the blue of the ground state hyperfine splitting (9.2 GHz). Usi
ng up to 83 W of microwave power, the trap is shallow (less-than-or-eq
ual-to 100 muK), large (almost-equal-to 1 cm) and cannot, by itself, h
old Cs atoms up against gravity. We levitate atoms in the trapping sta
te (F = 4, m(F) = 4 ground state) with a static magnetic field gradien
t. The trap is loaded with atoms cooled to 5 muK in optical molasses.
To detect the atoms, we either release them from the trap and detect t
heir fluorescence as they fall through a probe laser beam, or we obser
ve them with a ccd camera as we illuminate them with laser pulses. Pla
ns for applying this technique to spin-polarized hydrogen will be disc
ussed in a separate presentation [2].