PHTN1300: Lasers and Light Sources
Lab #3A Helium-Neon Lasers (2017F)
Students will study the electrical and optical characteristics of a commercial helium-neon gas laser tube. Specific topics that will be investigated in the course of the lab are the characteristics of gas discharges (e.g. negative resistance and the need for ballast resistance), determination of the optical elements of a typical gas laser (e.g. cavity mirror reflectivities), and computation of threshold gain for a given optical configuration.
This is one of the two most important labs in this course (They might be called "Über labs"!)
Here, a HeNe tube mounted in two three-point mounts is seen lasing. The power supply is the small block behind the unit on the breadboard - the thick red wire is the high-voltage output and connects to the anode of the tube via a series ballast resistance. It runs from a 12 volt lab-bench power supply. Note that there is output from both ends of the laser - this will be used to determine the reflectivity of each optic.
The purpose of this lab is to expose students to techniques involved in using gas laser tubes and their related power supplies. Be aware that these lasers operate at 1500 VOLTS and the starting pulse for such a tube can reach 10,000 VOLTS. With currents limited to under 5mA, death is unlikely (possible, but unlikely) but PAIN IS LIKELY, so be careful when performing this lab experiment and AVOID touching the metal ends of the tube. Use the high-voltage shields provided to cover live anode terminals to prevent accidental exposure. Also, short-out the high voltage terminal to ground before touching the wiring since capacitors in the supply can store energy even after it is turned off (do this by attaching a jumper to the grounded cathode first then touching the other end of the jumper to the anode terminal briefly). Failure to short-out the HV terminal will result in the student learning what CAPACITANCE is the hard way (i.e. through a nasty jolt!)
|WARNING: Arrival to the lab without your parts kit will result in being marked ABSENT with the accompanying penalty (including a deduction in marks and being placed on course condition) - you will NOT be permitted time to "run home" to obtain your kit.
- Read chapter 9 from Fundamentals by Csele on the helium-neon laser which provides a basic outline of the laser used in this lab and the next.
- Read HeNe Laser Notes (Many answers to the lab questions can be found here - it is required reading)
- Read section 2.2 (pp. 32) of Laser Modeling by Csele on tube structure (gain and absorption lengths) as you will need to measure these in the lab
- Bring jumper leads (from your parts kit) to the lab to connect the supply and discharge it before touching
- The following prelab assignment (worth 10% of the total lab mark), is due at the beginning of the first lab period. Late marks are not assigned if the prelab is not received at the beginning of the lab: you lose 10% of the total lab marks immediately with no recourse if it is not received upon entering the lab (extensions will NOT be given to "print it out" in the lab ... be prepared with the hardcopy already printed).
HeNe Gain Threshold Calculations
Using the basic gain threshold equation from the text (equation 4.9.2 in Fundamentals of Light Sources and Lasers or 2.5 in Laser Modeling in which the gain and attenuation lengths are considered to be the same - a misconception that will be corrected later in this lab), and knowing the small-signal gain (g0) of the HeNe laser medium (found in table 8.1 on page 222 of Laser Modeling), compute (in the same manner as the end-of-chapter question 4.9 in FLL) the minimum reflectivity of the OC for both the longest and the shortest HeNe tubes which Melles-Griot manufactures (which range from 0.4mW to 35mW in output power). Attenuation can be found on pg 222 of the Laser Modeling text.
You will need to look at this Listing of Melles-Griot Red HeNe Tubes at SAM's laser FAQ for physical tube parameters.
As usual, show all work for both sets of calculations for marks (answers without calculations shown will receive a mark of zero).
Start the small HeNe laser at the bench (the commercial, packaged one, not the bare tubes used for the rest of this procedure) and allow it to stabilize during the first part of the experiment (below). You may close the shutter on the front of the laser for safety but leave the laser energized the entire time (read chapter 9 of FLL by Csele to see why this happens). This laser will be needed LATER in the experiment to measure the reflectivity of laser optics.
Install an unmounted Siemens LGR7641 HeNe laser tube in two three-point mounts on a breadboard as shown in the photo at the top of this page. Face the output end (with the warning label "Laserstrahl") of the tube towards a Gentec UNO power meter also on the breadboard. Turn on the meter and set for a wavelength of 633nm.
Now wire the laser power supply as follows:
- Turn ON the variable power supply, set the output voltage for 12 volts, and turn it OFF.
- Connect GROUND on the laser supply (the black wire of the twisted pair of wires coming from the epoxy block with a spade terminal on it) to the Negative terminal on the variable power supply
- Connect POWER on the laser supply (the red wire with the spade terminal) to the Positive terminal on the variable power supply. If you forgot to turn OFF the supply you should get a nasty shock right now - pay attention :)
- Connect GROUND on the laser supply to the cathode of the laser tube. The cathode is the large cylinder. Snap the clip firmly onto the tube cathode.
- Connect the high voltage output from the power supply (with a 91K resistor already in series) to the positive terminal of the tube, again using the clip attached.
- Install a plastic shield over the anode to help prevent accidental contact with the live anode (and hence a shock).
- Turn the power ON and ensure you get laser output.
- Move the photodetector as far away from the tube as possible to prevent stray light from the tube from being measured. Intercept the beam near the tube with a small blockage and zero the meter, then allow the beam to strike the detector and measure the output power from the tube.
- Move the detector to the rear of the tube (the HR end) and carefully measure the power output from the tube. This power will be quite small so be careful to zero the meter and block stray light.
- Turn the power OFF
- After discharging the power supply (short the anode to ground with a jumper), measure the length (between the mirrors, the length over which attenuation occurs) of the tube and VERY specifically, the length of the gain medium (the small capillary inside the tube where gain actually occurs, not simply the distance between the optics - see page 32 of of Laser Modeling by Csele for a cutaway of a tube). You will hence have two length measurements for each tube.
Turn off the tube and repeat power measurements for the other two tubes - a Uniphase 098-1 and a Melles-Griot 05-LHR-097. The power supply we use (a 'block' type supply) is current regulated and so the current through each of the three tubes will be the same allowing a reasonable comparison of output powers. When turning the tube off, briefly short the tube with a piece of wire to discharge any capacitance in the supply.
Now, measure the reflectivity of the OC optic provided (extracted from a Melles-Griot 05-LHR-097 tube above) as follows:
- Mount the OC optic (already mounted in a stainless-steel tube as shown to the right) in a three-point mount on the breadboard.
- Mount the cylindrical lab bench laser (now preheated and stabilized - it was turned on at the beginning of the lab) in a laser mount and align the beam so that it passes directly through the optic at perpendicular angles. The beam must enter the optic from the "cavity" side (i.e. passing through the stainless-steel mount first) and exiting on the "glass" side.
- Carefully measure (i) the power into the optic and (ii) power passing through the optic. Be careful to zero the meter carefully and compensate for stray light and select the lowest range possible for maximum measurement precision.
- Calculate the transmission, then calculate the reflection, of the optic. Expect an answer of approximately 1% T.
The setup for measuring OC transmission. Note that the power meter must be over 30cm from the front of the preheated bench laser to avoid measuring spontaneous emission from the front of the laser (the "blue glow").
You will measure the optical parameters for only the Melles-Griot 05-LHR-097 tube (and will base gain calculations on that specific tube only)
Analysis (for the MG LHR Tube Only)
Now, for the 05-LHR-097 tube only
, for which you were provided with separate optics, calculate the following parameters of the tube (in order):
- Compute the transmission of the OC (measured), and then the reflectivity (R = 1.0 - T) of the OC. Use the measurements taken on the separate optic to do this.
- Knowing the OC transmission and the output power of the laser (measured on that same type of tube in the first part), compute the intra-cavity power (Poutput=Pintra-cavity * T).
- Knowing the output power from the HR of the laser (the very weak emission from the laser, also measured in the first part), compute the transmission, then the reflectivity of the HR
For that one tube, then, you should now have values for %ROC, %RHR, and length of the gain medium (OC = Approx 99%, HR > 99.9%, but you will compute both as part of this lab using the procedure outlined above).
For the 05-LHR-097 tube only, compute the threshold gain of the laser (gth) in the same manner as example 2.1 in Laser Modeling by Csele. Gamma (γ) is attenuation of the medium and can found on page 222, R1 and R2 are the reflectivities of the OC and HR which you have computed/measured as part of this lab (and are dimensionless so that "1.00" represents 100% reflection), and xg is the length of the actual gain medium in m - you must measure this in the lab - it is the length of the inner glass tube (approx 1mm diameter bore) through which the discharge is confined and actual laser gain occurs (where the discharge is not confined, such as the space between this inner glass tube and the rear optic, no laser gain occurs).
The FIRST PAGE must be a title page containing nothing more than the title of the lab, the course, the student's name and ID number, and the names of your lab partner(s).
Answer each question as "1", "2", etc with each new question starting on a NEW PAGE so that question 2 starts on the top of a new page (with the title "Question 2") and question 3 starts at the top of a different page (with the title "Question 3"), etc. You'll have, therefore, at _least_ fourteen pages in this report.
The lab must be submitted in a report cover (either a three-hole punched cover or one with a clamp on the left side, not a binder), and NEVER as a stapled mass of loose papers
Failure to follow this simple outline, used for all condensed labs in this course, will result in deduction of marks
To be done individually ...
Electrical Characteristics (primarily from the prelab reading)
- What is the purpose of the ballast resistance in a HeNe supply? Make specific reference to the electrical characteristics of a gas discharge as compared to an "ohmic" resistance. What might happen to a power supply if the ballast resistor was omitted?
- Why is a high voltage (> 5kV) start pulse required (i.e. describe what happens in the plasma tube)? Describe another CW gas laser which has "start pulse" generator (an actual physical circuit designed exclusively to produce a start pulse) and a 'run' voltage much lower voltage than the start pulse (cite the source where you found this).
- Describe all optical elements in a typical HeNe laser tube using a diagram. Give specific information on typical parameters for the optical elements (such as %T, %R, Radius of curvature).
- Describe the electrical elements of the tube (the anode and cathode) and describe why they are constructed as they are (i.e. the size, material, and structure of these elements). Specifically, answer why one element is much larger than the other and why one is made of a specific type of metal.
- Why does the output power of a HeNe laser DECREASE, eventually reaching zero, as current through the plasma tube is increased? Be very specific and make reference to the quantum excitation and de-excitation mechanisms (and specific atomic neon energy levels affected) in the laser to explain this. You will need to explain populations of excited atoms at both the LLL and ULL and how these change as current is increased.
Optical Characteristics (primarily from the lab)
For all numerical solutions, use the accepted parameters (e.g. attenuation) for the HeNe laser from chapter 8 of Laser Modeling which lists parameters for all common lasers
- Show observations (with an explanation of how you accomplished this) of the forward vs. reverse output beam power for all three types of tubes examined. Include measurements of attenuation and gain lengths as observed in the lab.
- For the one tube with separate optics provided (for which you measured the reflectivity of the OC), calculate the intra-cavity power and then the reflectivity of the HR. Be sure to show calculations. Using these values, compute the threshold gain of the tube (this is the minimum gain the medium must supply to allow the tube to oscillate). Use xa and xg parameters as done in the lectures.
- How do mirrors for most lasers achieve high (>95%) reflectivity not possible with simple metal coatings alone? Describe the structure of these mirrors (include a diagram showing the "stack" of multiple layers used) and describe, in a paragraph, how dielectric mirrors (also called "dichroic" mirrors) work. Be sure to detail the principles of operation, the thickness of the layers, and why that thickness is a critical parameter.
- Using an estimate for the small-signal gain (g0) of the HeNe laser of 0.15m-1 (and attenuation as per Laser Modeling), knowing the length of the gain medium of each tube (as measured in the lab), and assuming an HR of 100%R, calculate the minimum required reflectivity of the OC for each tube to allow it to oscillate. To do this, set gth equal to 0.15m-1 and solve for the reflectivity of the OC (usually R1 in the gain equation). Report all three figures and show all work (again, use xa and xg parameters in the same method as outlined in lectures).
- Assuming the green (543.5nm) HeNe laser transition has a small-signal gain (g0) of only 0.06 times that of a red HeNe laser (see chapter 9 of Fundamentals by Csele, which was a required prelab reading), calculate the minimum reflectivity of the OC for a "GreeNe" assuming the same parameters (including HR reflectivity) as question 7 which pertains to the stronger red transition. (Expect a reflectivity much higher than required for the red transition but it must obviously be less than 100% - if it is not, you have a calculation error). Do this calculation only for the one tube for which separate optics were provided (M-G 097 tube).
- Regardless of the output line selected (632.8nm or 543.5nm), the infrared line at 3.39μm has a much higher gain (see Laser Modeling of Csele section 2.6). Since this infrared line shares an upper lasing level with all visible transitions, this infrared line must be INHIBITED from lasing by selecting optics with a reflectivity below that required for lasing threshold of that line. Calculate the maximum reflectivity of the OC for the tube above (assuming the HR is broadband and has almost perfect reflectivity at 3.39μm) in order to inhibit this line and hence allow visible transitions to oscillate.