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Making cold molecules from cold atoms
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Photoassociation (AB)* Ground state A + B
Photoassociation is resonant in the photon energy Usually achieved by adding an extra laser to a MOT – the PA laser Very little heating involved – the molecules are ultracold Molecules will be in low-lying rotational states Produces molecules in highly excited vibrational states
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Photoassociation – decay channels
Decay to free atoms Decay to bound state Ground state A + B (AB)*
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Photoassociation properties
Most efficient for high-lying vibrational states – tend to form “long-range molecules” Extremely inefficient for tightly bound states Decay to a deeply bound state of the molecular ground state is unlikely Decay to two free atoms is accompanied by a large release of energy – trap loss Li2, Na2, K2, Rb2, Cs2, Sr2 , Ca2 , LiCs, KRb, RbCs….
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Detection methods PRL 85, 2292 (2000) Trap loss spectroscopy – the number of atoms in a MOT decreases when the molecules are formed. Example below: Ca2 Rev. Mod. Phys. 78, 483 (2006) Ion detection. Ionize the molecules and count the ions produced.
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Example: production of ultracold LiCs in the ground state
v=4 Photoassociation into v=4 (500mW, 946nm) Spontaneous decay into ground state Two-photon resonant ionization PRL 101, (2008) 5000 ground state molecules per second
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Photoassociation - advantages and limitations
Molecules are formed at ultracold temperatures Possible to reach the ground state (though difficult) Limited to constituents that can be laser-cooled Production rate is usually very slow resulting in low phase-space densities
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Magnetoassociation through a Feshbach resonance
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Reminder about s-wave scattering
At ultracold temperatures, scattering is described by the s-wave scattering length, a All other partial waves are suppressed by the angular momentum barrier Toy example: V=∞ V=V0 V=0 Zero-energy scattering state Uppermost bound state u(R) exp(-R/a) u(R) (R – a)
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Feshbach resonance
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Reminder about level crossings
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Atoms into molecules via a Feshbach resonance
B / B0 Bound molecules Free atoms
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