Difference between revisions of "Main Page/PHYS 4210/He-Ne Lasers"

From Physics Wiki
Jump to navigation Jump to search
 
(19 intermediate revisions by 3 users not shown)
Line 2: Line 2:
  
 
<p>In this experiment we first align an open-ended laser. Then we set up some transverse mode patterns, and perform further exercises and experiments to understand how a laser works.</p>
 
<p>In this experiment we first align an open-ended laser. Then we set up some transverse mode patterns, and perform further exercises and experiments to understand how a laser works.</p>
 +
 +
<h2> Key Concepts</h2>
 +
<table width=500>
 +
<td width=250><ul>
 +
<li>Stimulated Emission</li>
 +
<li>Spontaneous Emission</li>
 +
<li>Stimulated Emission</li>
 +
<li>Incoherent/Coherent Radiation</li>
 +
<li>Einstein Coefficients</li>
 +
<li>Population Inversion</li>
 +
<li>Forbidden Transitions</li>
 +
<li>Metastable States</li>
 +
<li>LS coupling</li>
 +
<li>Electric dipole selection rules</li>
 +
</ul>
 +
</td>
 +
<td width=250>
 +
<ul>
 +
<li>Axial Modes</li>
 +
<li>TEM modes</li>
 +
<li>Spectral Width</li>
 +
<li>Atomic Lineshape</li>
 +
<li>Loss/Gain Coefficient</li>
 +
<li>Index of Refraction</li>
 +
<li>Brewster’s Angle</li>
 +
<li>Malus’s Law</li>
 +
<li>Fresnel-Arago Law</li>
 +
<li>Q-Switch</li>
 +
</ul>
 +
</td>
 +
</table>
  
 
<h1>Reading and Exercises</h1>
 
<h1>Reading and Exercises</h1>
 
<ul>
 
<ul>
−
<li>Read pages 94 to 105 from Preston-Dietz. Carry out Exercise 1 (pg. 100), Exercise 2 (pg. 103) and Exercise 3 (pg. 104), but do not submit them as part of your report.</li>
+
<li>Read pages 94 to 105 and pages 100 to 112 from Preston-Dietz, [[Media:Lasers-AEP-1991.pdf|available here]]<ref>[https://www.library.yorku.ca/find/Record/1038893 The Art of Experimental Physics], John Wiley and Sons,1991.</ref>. </li>
−
<li>Continue with exercise 4 (pg. 104).</li>
+
<li>Carry out '''Exercise 1''' (pg. 100), '''Exercise 2''' (pg. 103), '''Exercise 3''' (pg. 104), and '''Exercise 4''' (pg. 104). </li>
−
<li>Read pages 100 to 112, on laser cavity modes.</li>
+
<li> Complete '''Exercise 1''' (pp 111-112). Do not forget to answer the last question of the exercise: Calculate the frequency difference between two adjacent axial modes TEM<sub>oom</sub> & TEM<sub>oo(m+1)</sub>.</li>
−
<li>Do exercise 1 (pp 111-112). Do not forget to answer the last question of the exercise: Calculate the frequency difference between two adjacent axial modes TEM<sub>oom</sub> & TEM<sub>oo(m+1)</sub>.</li>
+
<li> Submit all exercises as part of your report, either in the introduction or as an appendix as you deem appropriate. </li>
 
</ul>
 
</ul>
  
 
<h1>Experiments</h1>
 
<h1>Experiments</h1>
 
<h2>Aligning the laser</h2>
 
<h2>Aligning the laser</h2>
−
<p>Align the laser until it begins lasing using either, the instruction sheets "Aligning the Laser" by Preston or the Alternative method. Both methods are in a handbook (Red Binder) in the laboratory.</p>
+
<p>Align the laser until it begins lasing. The TA will discuss techniques to accomplish this.</p>
−
<p>When you are successful with the aligning process, and lasing is achieved, try varying the distances between the mirrors (using the adjusting screws on the laser mount) that still supports lasing. Record, in your lab book, the aligning process used, maximum, minimum and 'best' distances between the mirrors, radius of curvature of the mirrors etc. </p>
+
<p>When you are successful with the aligning process, and lasing is achieved, try varying the distances between the mirrors (using the adjusting screws on the laser mount) that still supports lasing. Record, in your lab book, the aligning process used, maximum, minimum and 'best' distances between the mirrors.</p>
−
<p>Use the polarizers to determine the polarization of the 'open' and 'aligning' lasers. Explain the difference(s), if any, between the two lasers.</p>
+
<p>What the radius of curvature of the mirrors which form the optical cavity? </p>
 +
<p>Use the polarizers to determine the polarization of laser.</p>
 
<p>Assume that the He-Ne produces 3 mW of laser output power and that the electrical data given applies to your gas discharge tube. Compute the efficiency, in percent, for converting electrical energy to red laser light energy with this He-Ne laser. Discuss your results.</p>
 
<p>Assume that the He-Ne produces 3 mW of laser output power and that the electrical data given applies to your gas discharge tube. Compute the efficiency, in percent, for converting electrical energy to red laser light energy with this He-Ne laser. Discuss your results.</p>
  
 
<h2>Brewster's Angle</h2>
 
<h2>Brewster's Angle</h2>
−
<p>Using the etalon, find an approximate value for the Brewster's angle. You can determine this by rotating the etalon until lasing stops. Only at the Brewster's angle does lasing resume.</p>
+
<p>Using the glass plate provided, find an approximate value for the Brewster's angle. You can determine this by rotating the glass plate until lasing stops. Only at the Brewster's angle does lasing resume.</p>
 
<p>Knowing that the tangent of the Brewster's angle is the ratio of the refractive indices of the lasing medium to air, determine the refractive index of the glass medium.</p>
 
<p>Knowing that the tangent of the Brewster's angle is the ratio of the refractive indices of the lasing medium to air, determine the refractive index of the glass medium.</p>
 
<p>Every resonant laser cavity has a characteristic quality factor or Q that measures the internal losses. The higher the Q, the lower the losses.</p>
 
<p>Every resonant laser cavity has a characteristic quality factor or Q that measures the internal losses. The higher the Q, the lower the losses.</p>
Line 26: Line 58:
 
<table width=200 align=center>
 
<table width=200 align=center>
 
<td>
 
<td>
−
<p align=justify>[[File:HeNe-eqn1.png|180px|center]]
+
<p align=justify>[[File:HeNe-eqn1a.png|180px|center]]
 
</p>
 
</p>
 
</td></table>
 
</td></table>
Line 49: Line 81:
 
<h2>Beam Profile of the TEM<sub>oom</sub> and the TEM<sub>10m</sub> modes</h2>
 
<h2>Beam Profile of the TEM<sub>oom</sub> and the TEM<sub>10m</sub> modes</h2>
 
<p>Realign the beam to produce the TEM<sub>oom</sub> mode.</p>
 
<p>Realign the beam to produce the TEM<sub>oom</sub> mode.</p>
−
<p>Set up the travelling microscope with the photo-detector at approximately 3 to 4 meters from the output coupler. Connect the detector to either a voltmeter or storage scope. Scan the beam to obtain the beam profile, i.e., transverse distance (x) versus intensity. Record the distance from the output coupler.</p>
+
<p>You will use a rotating mirror and a photodiode monitored on an oscilloscope to observe the profile of the laser beam.</p>
−
<p><b>Note:</b>If the storage scope is used to measure the intensity, you may have to use a cardboard to modulate (chop) the beam. Depending on the distance from the output coupler, you may want to use a NEUTRAL density (Wratten ND) filter to reduce to beam intensity.</p>
+
<p>Be sure to ensure the photodiode is not saturating when the laser is aligned onto it. If it is, switch the scale of the photodiode amplifier to a lower gain setting.</p>
 
<p>Repeat your observations for the TEM<sub>o1m</sub> mode. Remember that photodetectors are square-law detectors, i.e., the current density J is proportional to the square of the electric field. (See Preston for details). Sketch the beam profiles for both modes.</p>
 
<p>Repeat your observations for the TEM<sub>o1m</sub> mode. Remember that photodetectors are square-law detectors, i.e., the current density J is proportional to the square of the electric field. (See Preston for details). Sketch the beam profiles for both modes.</p>
 +
 +
<h2>Beam Profile or Shape</h2>
 +
<p>A laser beam has a certain profile with most energy concentrated at the center. The beam has the following form</p>
 +
 +
<table width=400 align=center><td>
 +
<p align=justify>[[File:HeNe-fig1v2.jpg|400px|border|center]]
 +
<b>Figure 1 -</b> Amplitude distribution across laser beam oscillating in the TEM<sub>oo</sub> mode.
 +
<br clear=right>
 +
</p>
 +
</td></table>
 +
<table width=200 align=center>
 +
<td>
 +
<p align=justify>[[File:HeNe-eqn4.png|120px|center]]
 +
</p>
 +
</td></table>
 +
 +
<p>where ''w'' is the radius of the beam. The Gaussian function, exp [- (''r''/''w'')<sup>2</sup> ] falls to 1/e, when ''r'' = ''w'', i.e.,</p>
 +
<table width=200 align=center>
 +
<td>
 +
<p align=justify>[[File:HeNe-eqn5.png|90px|center]]
 +
</p>
 +
</td></table>
 +
<p>Since the energy is proportional to the square of the amplitude, the beam radius, or SPOT SIZE, ''w'', is defined as that distance from the axis where the power has dropped to 1/e<sup>2</sup> of its value at the center. Twice that distance, 2''w'', is the beam diameter.</p>
 +
<p>The beam radius, ''w'', is the function of distance along the axis. If we call ''x'' the axial distance measured from the midpoint between the two (concave) mirrors, then the parameter ''w'' is given by</p>
 +
<table width=200 align=center>
 +
<td>
 +
<p align=justify>[[File:HeNe-eqn6.png|160px|center]]
 +
</p>
 +
</td></table>
 +
<p>where λ is the wavelength and ''w<sub>0</sub>'' is the minimum beam radius between mirrors.</p>
 +
<table width=400 align=center><td>
 +
<p align=justify>[[File:HeNe-fig2v2.jpg|400px|border|center]]
 +
<br clear=right>
 +
</p>
 +
</td></table>
 +
 +
<p>Note that from ''w<sub>x</sub>'' above; at ''x'' = 0, ''w<sub>x</sub>'' = ''w<sub>o</sub>''.</p>
 +
<p>From Preston (equation 21, p. 102),</p>
 +
<table width=200 align=center>
 +
<td>
 +
<p align=justify>[[File:HeNe-eqn7.png|160px|center]]
 +
</p>
 +
</td></table>
 +
<p>Calculate ''w<sub>o</sub>'' and ''w<sub>x</sub>''.</p>
 +
<p>From your observations of the beam profile for the TEM<sub>oom</sub>, determine ''w<sub>x</sub>'', the beam radius. How does your calculated value compare with the experimental value?  Explain any differences.</p>
 +
 +
<h2>Malus's Law</h2>
 +
<p>Malus’ law states that when a linearly polarized light beam of intensity ''I<sub>0</sub>'' passes through a linear polarizer with its axis rotated by angle ''A'' from the light beam polarization, the emergent intensity ''I'' is given by</p>
 +
<table width=200 align=center>
 +
<td>
 +
<p align=justify>[[File:HeNe-eqn8.png|90px|center]]
 +
</p>
 +
</td></table>
 +
<p>Use the rotatable polarizer and photodiode detector to verify this law quantitatively. Make detector readings at several values of angle ''A'' and record them in a neat table in your notebook. Graph your data to demonstrate the expected cos<sup>2</sup>''A''dependence.</p>
 +
 +
<h2>Verification of the Fresnel-Arago Law</h2>
 +
<p>Fresnel-Arago law state that two coherent light rays which are polarized right angles to each other will not mutually interfere. </p>
 +
<p>Use the laser to set up the Michelson interferometer as shown below to form an interference pattern. </p>
 +
<p>Insert polarizers P<sub>1</sub> and P<sub>2</sub> such that their axes of polarization is in the same direction. You may have to make slight adjustments to retain the interference pattern. Now, rotate ONE of the polarizers through 90º. Verify that the law is true. Try to take pictures of the resulting effect and include them with your report.</p>
 +
 +
<h1>References</h1>
 +
<references/>

Latest revision as of 11:40, 15 January 2021

He-Ne Lasers

In this experiment we first align an open-ended laser. Then we set up some transverse mode patterns, and perform further exercises and experiments to understand how a laser works.

Key Concepts

  • Stimulated Emission
  • Spontaneous Emission
  • Stimulated Emission
  • Incoherent/Coherent Radiation
  • Einstein Coefficients
  • Population Inversion
  • Forbidden Transitions
  • Metastable States
  • LS coupling
  • Electric dipole selection rules
  • Axial Modes
  • TEM modes
  • Spectral Width
  • Atomic Lineshape
  • Loss/Gain Coefficient
  • Index of Refraction
  • Brewster’s Angle
  • Malus’s Law
  • Fresnel-Arago Law
  • Q-Switch

Reading and Exercises

  • Read pages 94 to 105 and pages 100 to 112 from Preston-Dietz, available here[1].
  • Carry out Exercise 1 (pg. 100), Exercise 2 (pg. 103), Exercise 3 (pg. 104), and Exercise 4 (pg. 104).
  • Complete Exercise 1 (pp 111-112). Do not forget to answer the last question of the exercise: Calculate the frequency difference between two adjacent axial modes TEMoom & TEMoo(m+1).
  • Submit all exercises as part of your report, either in the introduction or as an appendix as you deem appropriate.

Experiments

Aligning the laser

Align the laser until it begins lasing. The TA will discuss techniques to accomplish this.

When you are successful with the aligning process, and lasing is achieved, try varying the distances between the mirrors (using the adjusting screws on the laser mount) that still supports lasing. Record, in your lab book, the aligning process used, maximum, minimum and 'best' distances between the mirrors.

What the radius of curvature of the mirrors which form the optical cavity?

Use the polarizers to determine the polarization of laser.

Assume that the He-Ne produces 3 mW of laser output power and that the electrical data given applies to your gas discharge tube. Compute the efficiency, in percent, for converting electrical energy to red laser light energy with this He-Ne laser. Discuss your results.

Brewster's Angle

Using the glass plate provided, find an approximate value for the Brewster's angle. You can determine this by rotating the glass plate until lasing stops. Only at the Brewster's angle does lasing resume.

Knowing that the tangent of the Brewster's angle is the ratio of the refractive indices of the lasing medium to air, determine the refractive index of the glass medium.

Every resonant laser cavity has a characteristic quality factor or Q that measures the internal losses. The higher the Q, the lower the losses.

A Q-switch pulse can be made by blocking one end of the mirror, then exciting the medium and then quickly unblocking the mirror. Stimulated emission will quickly drain the stored laser energy from the cavity in a short pulse with peak power much higher than the laser can produce. One can think of a Q-switch as a device that quickly switches from absorbing to transmitting, suddenly reducing cavity losses.

The Q-switch pulse length is given by

HeNe-eqn1a.png

where t is the round trip time (back and forth in the cavity), and R is the output mirror reflectivity ( >98% ).

Therefore

HeNe-eqn2.png

where L is the distance between the mirrors, n1 is the refractive index of the medium, and c is the speed of light. Pulse length can then be written as

HeNe-eqn3.png

Using the data from your laser, what is the theoretical value for the pulse length?

TEM Modes

Set up a camera with the screen at about 1 to 2 meters from the output mirror. Adjust the output coupler screws (or any other adjustments) to produce the TEM00m, TEM10m, TEM01m, .... modes. Photograph or sketch a few of them.

Beam Profile of the TEMoom and the TEM10m modes

Realign the beam to produce the TEMoom mode.

You will use a rotating mirror and a photodiode monitored on an oscilloscope to observe the profile of the laser beam.

Be sure to ensure the photodiode is not saturating when the laser is aligned onto it. If it is, switch the scale of the photodiode amplifier to a lower gain setting.

Repeat your observations for the TEMo1m mode. Remember that photodetectors are square-law detectors, i.e., the current density J is proportional to the square of the electric field. (See Preston for details). Sketch the beam profiles for both modes.

Beam Profile or Shape

A laser beam has a certain profile with most energy concentrated at the center. The beam has the following form

HeNe-fig1v2.jpg

Figure 1 - Amplitude distribution across laser beam oscillating in the TEMoo mode.

HeNe-eqn4.png

where w is the radius of the beam. The Gaussian function, exp [- (r/w)2 ] falls to 1/e, when r = w, i.e.,

HeNe-eqn5.png

Since the energy is proportional to the square of the amplitude, the beam radius, or SPOT SIZE, w, is defined as that distance from the axis where the power has dropped to 1/e2 of its value at the center. Twice that distance, 2w, is the beam diameter.

The beam radius, w, is the function of distance along the axis. If we call x the axial distance measured from the midpoint between the two (concave) mirrors, then the parameter w is given by

HeNe-eqn6.png

where λ is the wavelength and w0 is the minimum beam radius between mirrors.

HeNe-fig2v2.jpg


Note that from wx above; at x = 0, wx = wo.

From Preston (equation 21, p. 102),

HeNe-eqn7.png

Calculate wo and wx.

From your observations of the beam profile for the TEMoom, determine wx, the beam radius. How does your calculated value compare with the experimental value? Explain any differences.

Malus's Law

Malus’ law states that when a linearly polarized light beam of intensity I0 passes through a linear polarizer with its axis rotated by angle A from the light beam polarization, the emergent intensity I is given by

HeNe-eqn8.png

Use the rotatable polarizer and photodiode detector to verify this law quantitatively. Make detector readings at several values of angle A and record them in a neat table in your notebook. Graph your data to demonstrate the expected cos2Adependence.

Verification of the Fresnel-Arago Law

Fresnel-Arago law state that two coherent light rays which are polarized right angles to each other will not mutually interfere.

Use the laser to set up the Michelson interferometer as shown below to form an interference pattern.

Insert polarizers P1 and P2 such that their axes of polarization is in the same direction. You may have to make slight adjustments to retain the interference pattern. Now, rotate ONE of the polarizers through 90º. Verify that the law is true. Try to take pictures of the resulting effect and include them with your report.

References

  1. ↑ The Art of Experimental Physics, John Wiley and Sons,1991.
Retrieved from "https://physwiki.apps01.yorku.ca//index.php?title=Main_Page/PHYS_4210/He-Ne_Lasers&oldid=62476"