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A comprehensive guide for building an atom laser, including experiments on atom interferometry, precision measurements, and lithography. Detailed overview of experimental apparatus, Rydberg atom guiding, and design improvements for optimal results. Explore the world of atoms with this practical manual.
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Linear Atom guide: building an atom laser and other experiments Mallory Traxler April 2013
Motivation • Continuous atom laser • Continuous, coherent stream of atoms • Outcoupled from a BEC • Applications of atom lasers: • Atom interferometry • Electromagnetic fields • Gravitational fields • Precision measurement gyroscopes • Atom lithography
Overview • Guide α • Experimental apparatus • Experiments in guide α • Rydberg atom guiding • Design and manufacture of guide β • Improvements from guide α’s design • Outlook
Primary & secondaryMagneto-optical traps • Φpmot≈3x109 s-1 • <vz,pmot>≈22 m/s • 2D+ MOT • Φmmot≈4.8x108 s-1 • 2.2 m/s to 2.9 m/s
Optical detection • Detect atoms at the end • Uses pulsed probe (23) and probe repumper (12) • Optimize atoms in the guide
Ion Imaging • Three lasers for excitation • Repumper to get back to bright state • 5S1/25P3/2 • 480 nm to 59D • Ionize • Voltages on electrode, guard tube, MCP direct ions upward to MCP for detection
Introduction to Rydberg Atoms • High n-principal quantum number • Data here with n=59 • Physically large • r~n2 • Very susceptible to electric fields • α~n7 • Strong interactions • Other Rydberg atoms • Blackbody radiation
Experimentaltiming • Excitation to 59D • Variable delay time, td • MI or FI • Camera gated over ionization duration
Observed phenomena • Penning ionization • Remote field ionization • Initial • Delayed • Thermal ionization • (Radiative decay) • Microwave ionization • Field ionization
Observed phenomena • Penning ionization • Remote field ionization • Initial • Delayed • Thermal ionization • (Radiative decay) • Microwave ionization • Field ionization
Observed phenomena • Penning ionization • Remote field ionization • Initial • Delayed • Thermal ionization • (Radiative decay) • Microwave ionization • Field ionization
Observed phenomena • Penning ionization • Remote field ionization • Initial • Delayed • Thermal ionization • (Radiative decay) • Microwave ionization • Field ionization
Observed phenomena • Penning ionization • Remote field ionization • Initial • delayed • Thermal ionization • (Radiative decay) • Microwave ionization • Field ionization
Observed phenomena • Penning ionization • Remote field ionization • Initial • Delayed • Thermal ionization • (Radiative decay) • Microwave ionization • Field ionization
Observed phenomena • Penning ionization • Remote field ionization • Initial • Delayed • Thermal ionization • (Radiative decay) • Microwave ionization • Field ionization
Observed phenomena • Penning ionization • Remote field ionization • Initial • Delayed • Thermal ionization • (Radiative decay) • Microwave ionization • Field ionization
Rydberg guiding Data • Vary td from 5 μs to 5 ms • τMI=700 μs • τ59D5/2=150 μs
FI: internal state evolution • State-selective field ionization • Different electric field needed for different states • 59D peak broadens • State mixing
Rydberg guiding recap • Rydberg atoms excited from ground state atoms trapped in guide • Observe Rydberg guiding over several millisecondsusing microwave ionization and state selective field ionization • Numerous phenomena from Rydberg atoms within the guide
Guide β • Improvements over guide α • Zeeman slower • No launching • Magnetic injection • Mechanical shutter
1mot • Standard 6-beam MOT • Fed by Zeeman slower • Factor of 6.6 brighter • Expect closer to 10x
2MOT chamber • Most complicated part of the design • 4 racetrack 2MOT coils • 8 injection coils • Built-in water cooling • Magnetic compression • Mechanical shutter
2mot coils • 4 racetrack coils produce quadrupole magnetic field • Holes • Optical access • Venting of internal parts • Shutter • 2 locks for stationary shutter
Injection coil mount • 8 injection coils of varying diameters • Fits inside 2MOT coil package • Water cooling for all • Tapered inside and out
Steel piece, stationary shutter • Magnetic compression • Mount for waveplate-mirror • Stationary shutter
In-vacuum coils • Hand-turned on lathe • 2MOT coils on form • Injection coils directly on mount • Labeled with UHV compatible ceramic beads
Injection coils • High current power supply • Split off 2-3 A for each coil • Adiabatically inject atoms into the guide
Surface adsorption evaporative cooling • 21 equally spaced silicon surfaces • Bring guided atomic flow closer to these surfaces • Atoms not adsorbed onto surface rethermalize at lower temperature
Guide recap β • Fully constructed • Preliminary tests well on the way • Good transfer of atoms into the 2MOT • Need Zeeman slower and 2MOT working simultaneously to optimize
Short term outlook:Transverse cooling • Increase capture volume of Zeeman slower • Reduce transverse velocity by factor of x, increase density by factor of x2 • Most optics already in place
Longer term outlook:Potential Barrier • Potential barrier at the end of the guide • Form BEC upstream • Use coil to create potential • Study BEC loading dynamics, number fluctuations • Later use light shield barrier • Tunnel atoms through to make first continuous atom laser
Raithel Group • PI • Prof. Georg Raithel • Former Post Docs • Erik Power • Rachel Sapiro • Former Grad Students (on this project) • Spencer Olson • RahulMhaskar • Cornelius Hempel • Recent Ph.D. • Eric Paradis • Graduate Students • Andrew Cadotte • Andrew Schwarzkopf • David Anderson • Kaitlin Moore • NithiwadeeThaicharoen • Sarah Anderson • Stephanie Miller • Yun-Jhih Chen • Current Undergraduate • Matt Boguslawski • Former Undergrads • VarunVaidya • Steven Moses • Karl Lundquist