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Thesis (pdf) - Swinburne University of Technology

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several million up to several hundred million atoms at these very low tem-<br />

peratures. These break-throughs were rewarded with the award <strong>of</strong> the Nobel<br />

prize for physics to Steven Chu, William Phillips and Claude Cohen-Tannoudji<br />

in 1997. Having such cold atoms in such numbers allowed the creation <strong>of</strong><br />

several types <strong>of</strong> atom interferometers, which the field <strong>of</strong> metrology has bene-<br />

fited from. These interferometers ranged from devices to measure the Earth’s<br />

gravity [Pet99] and rotation [Gus97] to atomic clocks, which in principle are<br />

interferometers only in the time domain [Rus98, Wil02], and to interferome-<br />

ters that were used to measure atomic properties [Eks95] or natural constants<br />

[Gup02]. All <strong>of</strong> these interferometers work with free atoms, either falling or<br />

accelerated from the trap in which they were cooled, and the beamsplitters<br />

needed for interferometry are created by light pulses and the change <strong>of</strong> the<br />

atomic momentum on absorption <strong>of</strong> a photon [Kas91]. With the thermal mo-<br />

tion and kinetic energy being greatly reduced, it became possible to trap and<br />

confine large numbers <strong>of</strong> atoms with rather weak forces, stemming for example<br />

from the interaction between a magnetic field and the magnetic moment <strong>of</strong><br />

an atom or from the interaction <strong>of</strong> the induced atomic electric dipole-moment<br />

with an electro-magnetic field. With these magnetic and optical traps even<br />

more versatile atom interferometer set-ups are possible.<br />

Two main implementations <strong>of</strong> atom interferometers have been proposed: in<br />

the first example, an otherwise stationary trap is split into two, held there and<br />

recombined [Hin01]. The second example works with confined atoms that pass<br />

through wave guides and beam splitters. Only recently it has become possible<br />

to create these time dependent (in the first case) or spatially dependent (in the<br />

second case) potentials. Here either micron-sized optics and lenses are used to<br />

create optical traps which can be split and recombined [Dum02b] or waveguides<br />

are constructed [Dum02a]. For magnetic traps, the proposal [Wei95, Thy99]<br />

and realisation [Rei99, Ott01] <strong>of</strong> the so-called “atom chip” made the tailoring<br />

4

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