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Scientific Proof of the Flying Spaghetti Monster!

Indeed His Great and Tasty Noodliness exists, and our lab was blessed with His appearance during a bake-out of the vacuum chambers.  We have yet to encounter Real Pirates, but assume that our lab’s collective adherence to the observance and recognition of International Talk Like A Pirate Day has not gone without notice by His Tomato-Sauciness. 

FSM sighting!

Indeed in these rare photographs one can see clearly His Noodly Appendages reaching out from under the foil wrapping as if to touch fellow Pastafarians with His Slimy Tomato Sauce. 

Another view of the FSM

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Homebuilt laser!

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Of all the cool projects I’ve been involved in during my school career through my Physics career, I’ve got to say that getting to build a custom laser is the one I’m going to have the most fun talking about.  Not that it is the most interesting project ever…but come on, a home-built laser!  It should be a requirement for getting a Physics degree.

The laser light itself is supplied by a laser diode, this one is actually a commercial one used in DVD reader/recorder units.  The experiment requires the use of light locked to a 671nm wavelength, but this is not in the range of commonly available commercial lasers.  Laser diodes actually emit a range of frequencies around a central frequency, which can be shifted by heat and also stimulation of a particular frequency.  In fact by shining light at precisely the desired wavelength of light back onto the diode, this increases the diode’s emission at that one frequency, and can narrow the amount of light emitted at other frequencies.

The trick we will use in achieving a 671nm wavelength is to use a Littrow-mount feedback system.  Light from the laser is shined onto a diffraction grating, which reflects most of the light.  A small amount of light is reflected at precise angles based on its wavelength, (as is expected from the physics of diffraction gratings), and the grating’s first-order reflection is made to reflect back onto the laser diode.  By changing the orientation of the grating, a particular wavelength can be made to shine back onto the diode (again, this is explained by the basic science of diffraction gratings – like a shiny CD, wavelengths hitting a grating are reflected at angles proportional to their wavelength), and so select the desired wavelength to stimulate in the diode.

The zeroth-order reflection (essentially the mirror reflection off of the grating) is reflected from a mirror, then out parallel to the original beam path.  The grating and mirror are mounted as a unit on a swing-arm in front of the diode laser, so that rotation of the mirror/grating unit can be achieved by a piezo-electric unit.  This allows the first-order reflection to be locked onto the laser, while not (largely) affecting the attitude of the outgoing beam.

The parts I have made were all from plans which the professor in charge of the Ultracold Atoms Experiment obtained through a group he had worked with at Berkeley.  So producing the whole system was quite straight-forward and took about a week of actual work in total, once all the parts were together.

Bare laser mount

In the picture above, the diode mount is a modified lens mount with aluminum blocks attached to the front end (the laser emits to the left of the photo).  The aluminum block with an angled cut and Allen screws on top will hold the diffraction grating, and the aluminum bar it sits on holds the mirror, as seen below:

Laser, Grating, and Mirror

The laser diode itself is behind the bluish collimating lens, which can be adjusted by turning the threaded steel ring around it.  The black cylinder around this is a commercial diode mount, with a layer of "thermal goop" between it and a modified mounting unit, with more goop between it and the modified lens mount.  The thermal paste helps heat get to the laser diode efficiently.

Down the front of the laser

Laser and Base

The unit as seen above sandwiches a thermoelectric cooler (TEC, also known as a Peltier device), which acts as a "heat pump" when current is applied to it, by moving heat from one side of its body to the other (the red and black wires attach to it).  This is all attached to a massive (about 7-8 lbs.) brass block, and its mass and a rubber sheet below it help to dampen vibrations which might make their way through the optics table.  Everything sits inside a housing box, which is lined with Acoustiblock material to keep out sound vibrations traveling over the table.


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Posted in Experiment, Physics, Projects, Work.

Ultracold Atomic Experiments

I have been working for some time with an Ultracold Atomic Experiment group at the University of Washington.  This has been one of my more enjoyable jobs, and has kept me busy machining parts, soldering together circuits, building lasers, taking pictures, and all sorts of other fun things.  The entire series of chambers is pulled to a very pristine vacuum – around 1E-10 torr or better.   Achieving such a good vacuum is a very involved and interesting process.  One of the steps is to heat the chamber walls to release embedded atoms so they can be pumped out; Below is a picture of the chamber wrapped in band heaters and other heating elements, which are each supplied power by one of the many variacs seen floating around the chamber.

Variacs!

The experiment will be trapping Lithium (Li) and Ytterbium (Yb) atoms, which get boiled off from separate ovens, slowed through Zeeman slowers, and combined into the central Magneto-Optical Trap, where they are further cooled by evaporative cooling until finally cold enough to settle into the lowest energy quantum state as a Bose-Einstein Condensate (BEC).  The projects I am or have been involved with include:

  • Create or Update Documentation for most projects
  • Data Acquisition Software and Hardware
    • Working with National Instruments Hardware and Software (interfaces with break-out boxes listed below)
    • Interfacing with Atticus/Cicero control software developed by a group at MIT
    • Digital Camera
      • Research and set-up of camera
      • Programming of User Interface
  • Construction of Electronics and Other Hardware
    • Diode Laser Lock Boxes
    • Lithium and Ytterbium Oven Control Units (Torture Units Li and Yb…)
    • 12 and 40 amp MOSFET switch boxes (BFW Housing Boxes)
    • Analog and Digital Isolation Break-Out Boxes
    • Enhancement Cavity Mode Lock Box
    • RF Driver boxes
    • 671nm Littrow-configuration laser
  • Create website for group
  • Take Photographs of experiment and lab
  • General Tasks
    • Troubleshoot/testing of various lab hardware and circuits
    • Organizing and maintaining electronics and other areas of lab (Research and purchase electronics parts)
    • Creating and now maintaining shared computer file system, software, and datasheets
  • Unicycle to Electronics Shop and back

Posted in Experiment, Physics, Projects, Work.

Michelson Interferometer – Part 2

This is the portion of my physics group project report that I wrote.

Interferometer Page 1


Measuring Static Frictional Forces using Interferometry

Interferometer Setup
Fig. 1:  Interferometer Setup and Labels
Fringes from Michelson Interferometer
Fig. 2:  Interferometer Fringes

Introduction

It is often not understood that even when dealing with static friction, application of less-than-critical sheering forces (that is, forces which do not cause breaking of static friction) creates an actual displacement between an object and the surface it rests on. The amount of movement is typically very small and barely if at all visible (displacement can be large enough to be seen when, for example, the surface is a rubber mat). When the sheering force is let off, static friction becomes a restoring force, returning the objects to its original position respective to the surface. This restoring force can be thought of as spring tension, and in this thinking ought to be proportional to object displacement.

This experiment sought to verify the linear F = k x relationship of static frictional forces between various materials at less-than-critical sheering forces. Very precise measurements of displacement were measured using a Michelson-type interferometer. The results showed a definite linear relationship between applied force and displacement of the test object for Styrofoam and particleboard surfaces.

Procedure

The first goal achieved was forming the ‘fringing’ patterns with the interferometer. The basic setup follows the Michelson interferometer design.

As shown in Fig. 1 , the beam emitted by the Laser (while a laser pointer is shown, a HeNe laser was used for actual collection of data) passed through one or two Lenses . The Lenses simply made the laser beam diverge and created a larger beam for viewing. The beam then hit the Beam Splitter , separating into two partial beams. Each partial beam bounced from a mirror back onto the beam splitter so that they overlapped and projected as a spot of light on a viewing surface (in the direction of the sheet of paper in Fig. 1). The Reference Mirror held a fixed position and created a reference beam. The Test Mirror was attached to a movable Test Block , and the surface under the block could be changed.

More difficult was developing the apparatus to precisely add and measure sheer force to the Test Mirror. The resulting design is shown in Fig. 3 (NOTE–Figure 3 isn’t here yet). The end of a Fishing Line was attached to a hook on back of the Test Block . The Line passed through the two Static Pulleys and terminated at the Force Probe . The Moveable Pulley could then be pushed into the Fishing Line, causing a Tension felt equally by both the Force Probe and Test Block. It should be noted that the Test Block and Force Probe were adjusted carefully so that they were directly aligned with the Fishing Line. In this way, the Pulley system ensured that only the desired vector component of force was applied to the Probe and Block.  When everything was secured properly, this system worked remarkably well and tension could be applied and held fairly precisely by hand.

A computer captured data directly from the calibrated Force Probe. To take a data run, the apparatus was first adjusted so little or no force acted on the Test Mirror and Force Probe. The state (bright or dark) of the central dot (see Fig. 2) was noted, the force was captured and 0 was entered as the fringe number. The Moveable Pulley was then pushed into the Fishing Line until the central dot grew into a ring with its alternate state in the center. The force was again captured and entered as fringe # 1. For example, in Figure 2, the initial central dot is red. If tension were applied to the Test Block, it would grow into a ring with a dark spot in its center. The dark spot becomes the new central dot, and was counted as one fringe when it became the same size as the original bright spot.

This process was repeated for multiple surfaces, and for most runs it was verified that as tension was let off the same number of fringes disappeared as had previously appeared. For the final run of a surface, the attempt was made to capture data until holding the Moveable Pulley became too difficult or the static friction bonds were broken and the Test Mirror slid out of position.

Interferometer Page 1


 

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