Axicon Lens for Coherent Matter Waves

Raman Lab Research Projects

 
 

    Gaseous Bose-Einstein condensates (BECs) present unique possibilities as bright, coherent matter wave sources for applications to coherent atom optics, holography and interferometry.  There is much interest in creating novel atom optical elements for focusing and deposition, coupling of atoms with high efficiency into atom chip guides, collimation of atomic trajectories within an atomic clock to suppress systematic effects, and for the exploration of fundamental physics with matter waves.


    However, unlike photonic optics, propagation of matter waves is profoundly affected by the interactions between atoms.  For example, in a gaseous Bose-Einstein condensate, the “mean-field” driven expansion destroys the Heisenberg-limited momentum distribution possessed by a condensate while it is trapped, creating a matter wave with a broad spread of velocities that is undesirable for atom-optical applications.  Therefore, it is of great interest to discover methods of controlling and suppressing interaction effects during propagation of a matter wave field and within atom interferometers.

    We have realized a conical matter wave lens. The repulsive potential of a focused laser beam was used to launch a Bose-Einstein condensate into a radially expanding wavepacket whose perfect ring shape was ensured by energy conservation. In spite of significant interactions between atoms, the spatial and velocity widths of the ring along its radial dimension remained extremely narrow, as also confirmed by numerical simulations.  Our results open the possibility for cylindrical atom optics without the perturbing effect of mean-field interactions.

How We Make It

    Artistic rendition of the operation of the atomic axicon.  A condensate (wavefunction show in black and white) is initially localized near the origin.  The external potential is shown in false color.  (a) At time t = 0, the linear potential is turned off, and a blue-detuned optical plug is turned on.  (b) For times t > 0, the atoms rapidly “roll down” the potential hill, forming a ring-shaped density distribution that expands radially outwards in the x-y plane.

What one sees

Far field pattern of a conical atom beam.  On the left, a movie of the ring expansion.  On the right, a movie of ordinary BEC expansion.  The frame size is 2.6 mm x 2.6 mm

Side view of expanding ring shown at 10 ms (top: a,b) and 15 ms (below: c,d) for both ring shaped expansions (left: a,c) as well as ordinary BEC expansion (right: b,d).  Each image is 0.8 mm x 2.2 mm.