Difference between revisions of "Interferometers"

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The mach-zehnder interferometer setup is shown in Figure 4.
 
The mach-zehnder interferometer setup is shown in Figure 4.
[[File:mach.jpg|400px|right|thumb|Figure 2: Mach-Zehnder interferometer setup]]
+
[[File:mach.jpg|400px|right|thumb|Figure 2: Setup of the Mach-Zehnder interferometer]]
  
 
As with the Michelson interferometer, an optial iris was employed to minimize outside noise.  However, the optical isolator proved unnecessary with the Mach-Zehnder interferometer as no fringe drift was observed.
 
As with the Michelson interferometer, an optial iris was employed to minimize outside noise.  However, the optical isolator proved unnecessary with the Mach-Zehnder interferometer as no fringe drift was observed.
  
 
The Setup of the Sagnac interferometer is shown below.
 
The Setup of the Sagnac interferometer is shown below.

Revision as of 15:08, 21 March 2014

The goal of the spectroscopy project was to create a michelson, mach-zehnder and sagnac Interferometer. Each setup utilized a 632.8nm Helium-Neon laser.

In order to reduce fringe-drift, the michelson interferometer employed both an optical iris and an optical isolator. The setup of the michelson interferometer is shown in Figure 1.

Figure 1: Setup of the Michelson Interferometer


The Michelson interferometer was used to measure both the "voltage-to-expansion" ratio of a PZT and the coherence length of the He-Ne laser.

To measure the "voltage-to-expansion" ratio, the PZT was wedged in the track of he adjustable mirror. By increasing the voltage across the PZT and simultaneously counting the number of fringes that passed an arbitrary point on the projection screen, it was possible to measure the expansion distance of the PZT using the relation d=m*lambda/2. Multiple measurements were recorded and plotted in Figure 2.

Figure 2: Voltage per meter measurements of PZT

The slope of the graph indicates the PZT expands at a rate 100nm/Volt.

To measure the coherence length of the He-Ne laser, mirror 1 was gradually moved backwards until the interference pattern was no longer visible. The coherence length <l>, is given by the relation <l>=2*d, where d is the difference in length between the arms of the interferometer (Figure 3). The coherence length was determined to be 78cm.

Figure 3: Arm lengths are given by d1 and d2. Mirror 1 moved backwards until interference pattern no longer visible. Coherence length given by <l>=2(d1-d2).

The mach-zehnder interferometer setup is shown in Figure 4.

Figure 2: Setup of the Mach-Zehnder interferometer

As with the Michelson interferometer, an optial iris was employed to minimize outside noise. However, the optical isolator proved unnecessary with the Mach-Zehnder interferometer as no fringe drift was observed.

The Setup of the Sagnac interferometer is shown below.