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    Stabilized HeNe Lasers - UNDER CONSTRUCTION

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    This chapter deals with the special case of HeNe lasers that have their frequency actively regulated either directly, or indirectly via control of intensity. Their output is generally either a single longitudinal mode (single optical frequency), a pair of adjacent longitudinal modes (two optical frequencies separated by 600 MHz to 1 GHz typical), or a pair of optical frequencies close together produced by Zeeman splitting of a single longitudinal mode (250 kHz to 8 Mhz typical) or an Acousto-Optic Modulator (AOM) generating a sideband of a single longitudinal mode (20 MHz typical).

    In almost all cases, these apply specifically to HeNe lasers operating on the so-called red transition around 633 nm (although when stabilized, there may be many many places to the right of the decimal point). HeNe lasers on other wavelengths can also be stabilized, though not all the same techniques can be used. This chapter deals almost exclusively with stabilized red HeNe lasers.

    General information on HeNe lasers as well as a brief introduction to stabilized HeNe lasers and typical locking schemes may be found in the chapter: Helium-Neon Lasers. Here, we delve into the topic in more detail.

    However, it is not intended to be an all encompassing treatise on stabilized laser with all the gory details including hairy math. :) For that, refer to the scientific literature, most from the 1960s or 1970s. Only a few references are included here, but Web searches will turn up numerous research papers, many of which are in the public domain. For those that are not, affiliation with a major university or other academic institution may be required to access them for free.

    Difference Between Stabilized and Unstabilized HeNe Lasers

    The popular conception of a laser is that it is a light source of a single specific color or wavelength. While such a description is good enough for most Mark I eyeballs (at least where the wavelength is in the visible spectrum), the output from real lasers is usually not so perfect.

    The behavior of any laser is determined by many factors but the most important two are:

    The useful output of most stabilized HeNe lasers is either a (ideally) single optical frequency, or a pair of optical frequencies separated by anywhere from a few 10s of kHz to hundreds of MHz. And in some applications, multiple frequencies (usaully 2 but it could be more) that are locked to a reference may be useful.

    Locking Techniques for Stabilized HeNe Lasers

    The purpose of locking in a stabilized HeNe laser is to assure that the desired output (single or two frequencies in most cases) has a controlled. optical frequency or frequencies. For use in metrology applications, this will mean that the single or dual lasing line is fixed at a known optical frequency (corresponding to a known wavelength related by c/f where c is the speed of light and f is the optical frequency). Therefore, the locking controller needs a reference, which can be intrinsic or extrinsic. An intrinsic reference uses the properties of the laser itself. An extrinsic reference requires some external device such as another laser (which itself has been locked to a known optical frequency), a gas cell having known spectral absorption with respect to optical frequency, or a physical device like a super high finesse Fabry-Perot etalon or interferometer. The chart below summaries the most popular locking techniques for red (~633 nm) HeNe lasers:

                                                Maximum     Optical       Optical
                                                Output     Frequency     Frequency
     Locking Type                                Power     Variation     Accuracy
     Unstabilized multiple transverse mode     >200 mW       ---            ---
     Unstabilized single transverse mode        >50 mW      1.5 GHz        3x10-6
     Thermal stabilization                        2 mW       75 MHz      1.5x10-7
     Single mode Intensity stabilization        1.5 mW       10 MHz        2x10-8
     Gain peak stabilization                    1.0 mW        5 Mhz+       1x10-8
     Lamb-Dip stabilization                     0.5 mW        5 Mhz+       1x10-8
     Dual mode polarization stabilization       2.0 mW        1 MHz        2x10-9
     Three mode stabilization                   3.5 mW        1 MHz*       2x10-9
     Secord order beat stabilization            3.5 mW      200 kHz*       4x10-10
     Transverse Zeeman beat stabilization       1.5 mW      100 kHz*       2x10-10
     External (Iodine Cell) stabilization       0.2 mW       <5 kHz+      <1x10-11
     External (Iodine Cell) offset locked       2.0 mW       <5 kHz       <1x10-11
     External reference stabilization           2.0 mW       <1 Hz        <2x10-15

    The useful output of these are NOT always absolutely pure single mode or single optical frequency limited by the laser dynamics:

    * denote techniques where the output has either a pair of modes of similar amplitude close together in optical frequency, or a small "ghost mode" next to the main mode.

    + denotes techniques based on Pound-Drever-Hall locking or a similar implementation that adds some dither to the optical frequency.

    The approaches listed in the first group are intrinsic and use the Neon Gain Curve (NGC) of the HeNe laser tube as the reference. The center of the NGC has an optical frequency which depends only on the neon isotope ratio, temperature, and pressure, all of which can be controlled fairly precisely. The gain bandwidth of the NGC is also relatively narrow (as these things go) at around 1.6 GHz which can both limit the number of longitudinal modes that are oscillating (more on this below) and make feedback using its profile be more precise. Thus the NGC can be used to accurately position the lasing line(s) at a known location. All but the most exotic (and expensive!) stabilized HeNe lasers use one of the intrinsic techniques based on the NGC listed above. The vast majority use single or two mode polarization stabilization.

    Relatively simple approaches using an external F-P resonator or other type of interferometer are possible. For example, using a low finesse Scanning Fabry-Perot Interferometer (SFPI) to monitor the longitudinal modes with a digital control loop maintaining them in a specific location on the NGC can be used with three mode polarization stabilization to obtain higher power with one mode centered. Single and dual mode polarization stabilization are limited to a maximum of around 2 mW; three mode stabilization is capable of up to around 3.5 mW or a bit more. But this is still an intrinsic technique. (This could also be used for single or dual mode stabilization but would probably not provide much, if any, benefit.)

    It should be noted that it is because the gain bandwidth of neon is relatively narrow at 1.6 GHz, that the NGC becomes so useful. Solid state (SS) lasers on the other hand have lasing medium gain bandwidths typically wider by a factor of 50 or more. While straightforward techniques can be used to force single mode in an SS laser, achieving precise control of optical frequency with such a wide gain bandwidth is more difficult. This is one of the primary reasons that SS lasers have for the most part as yet been unable to replace the lowly HeNe laser in applications requiring optical frequency accuracy and stability. Locking diode lasers at a specific optical frequency is even more complex.

    Of the extrinsic technigues, a stabilized HeNe laser making use of an iodine cell is probably the most precise optical frequency reference available commercially (with an equally high price to match). Its absolute optical frequency accuracy may be two orders of magnitude better than the technique of two-mode polarization stabilization, used in most commercial stabilized HeNe lasers now and in the past.

    Going beyond this level of precision to high finesse F-P resonators and such is generally the perview of advanced research. To get down to that <1 Hz requires massive isolation chambers and active damping to minimize vibration and other external influences. Such a system is not likely to be portable! ;-)

    The chart excludes any technques requiring use of intra-cavity devices like etalons to force single frequency operation. These are capable of both high power AND high stability but require special tubes and relatively complex control. Thus they are expensive and not at all common, though at least one company does claim to offer a 40 mW single frequency HeNe laser.

    Having said all that, it's remarkably simple - almost trivial - to control the behavior of a common HeNe laser tube similar to those that used to be found in grocery store barcode scanners to provide a single frequency output with a stability of better than 1 part in 10,000,000. In fact, it can be done with a total of 4 parts costing only a couple dollars (besides the laser tube and power supplies). Nearly every possible technique imaginable has been explored at some time in the past. It's quite possible that trained pigeons have even been pressed into service for this purpose, and there's probably a patent on it. ;-) What are described here are only the most common (electronic) approaches.

    But before any of these can be described in more detail, a primer or laser modes is required.

    Longitudinal Modes and Their Significance for Stabilized HeNe Lasers

    We assume familiarity with general laser mode principles. For an introduction to HeHe lasers and longitudinal modes, see Theory of Operation, Modes, Coherence Length, On-Line Course.

    For everything that follows, it is assumed that the spatial mode structure of the HeNe laser is near pure TEM00 resulting in close to a Gaussian beam profile. We are not aware of any stabilized HeNes using multi-spatial mode tubes.

    Lasing is determined by the round trip gain at the laser's optical frequency or wavelength, and resonance wihin the laser cavity. For everything in this chapter, we assume a linear "Fabry-Perot" cavity - the classic "gain medium between mirrors" laser - and the one used in virtually all HeNe lasers and even close to all stabilized HeNe lasers. But ring and other geometries would have similar constraints.

    As with any resonant structure, there will be a fundamental frequency at which it can respond (n=1), as well as an inifinite range of harmonics (n=2,3,4.....infinity). For an organ pipe or violin string resosnance is at its fundamental and several harmonics. However, due to the short wavelength of light and relatively large resonant cavity length, for a HeNe laser, there is no fundamental and the harmonics have values of n in the hundreds of thousands or more.

    In order to sustain laser oscillation, the round trip gain must exceed losses for photon at an optical frequency that is close to a cavity resonance as defined by n*c/2L. L is the distance between the mirrors, c is the speed of light, and n is an integer that results in the equation being equal to an optical frequency with a net gain greater than one for the lasing medium gain and cavity geometry.

    For a red (633 nm) HeNe laser, the Neon Gain Curve (NGC) has a width of 1.5 to 1.6 GHz FWHM and is centered at around 474 THz. (We will have much more precise values later.) As an example, for a cavity length of 200 mm, c/2L is around 725 MHz. Thus, 1 to 3 modes may oscillate at the same time depending on their precise position within the NGC, but never more than that. Typical values for n in this case would be successive integers near 987,500. (There are other more subtle effects such as mode pulling and mode pushing that offset the actual optical frquencies by a small amount, but for now, the exact cavity resonances are sufficiently accurate.)

    Higher power longer tubes will support more than 3 modes. And due to the shape of the NGC, the power in the strongest mode increases sub-linearly with tube length. So even if it could be isolated for a single frequency laser (which beyond 3 is not really practical), its power would not be that high, perhaps 6 mW for a tube outputting 35 mW . Further, due to mode competition, the power in each mode in longer tubes tends to fluctuate at random among them and stabilization doesn't help. This can be an issue even with the tube used in three mode stabilization.

    When a HeNe laser is powered, whichever cavity resonances - also called "cavity modes" are within the NGC and have sufficient round trip gain will lase. These are the longitudunal or axial modes of the laser. Each of these "lasing lines" is a very nearly pure optical frequency in a HeNe laser, with a bandwidth of under 1 kHz and possibly as low as a few Hz or less. Thus, the term "single frequency" is appropriate (except for the most die-hard purists) where one of these modes is the output of a stabilized laser.

    If the distance between the mirrors changes, the position of the modes will drift through the NGC. For large frame laboratory HeNe lasers, the resonator structure is designed to have a very low coefficient of thermal expansion. However, for common HeNe laser tubes of the type used in most stabilized HeNe lasers, the heating effects of the plasma discharge will cause the distance between the mirrors the change. As this occurs, the longitudinal modes will drift through the NGC. A mode at the high frequency-end will eventually disappear and be replaced by a new one appearing at the low-frequency-end. This is "mode sweep". An animation of the mode behavior of a tube similar to those used in many stabilized HeNes can be found at HeNe Laser Mode Sweep: 200 mm (~8 inch) Cavity Length. Of course, the movement is continuous but it's tiring to create an infinite number of slides. ;-)

    To stabilize such a tube, the cavity length needs to be controlled in a feedback loop. A variety of means can be used to affect cavity length. A heater wrapped around the tube is most common, but others include an internal heater wrapped around the bore, an induction heater on one of the mirror mount stems, or the use of a PeiZo Transducer (PZT) behind one of mirror. It's even possible to use a magnetic actuator to press on one of the mirror mounts. With stabilization, the longitudinal modes can be precisely "parked" on the NGC. It's possible to do this in the animation by careful use of the left and right arrow keys to keep one mode centered. Fortunately, analog or digital electronics is much more effective and doesn't get tired as easily. ;-)

    Characteristics of the Neon Gain Curve

    All intrinsic HeNe stabilization techniques are based on controlling the mode position using the NGC itself as the optical frequency reference. Thus, depending on what precision is required, its absolute optical frequency, width, and profile must be known. These are affected primarily by the temperature, pressure, and He:Ne isotope ratio in the tube. However, due to mode competition, the length of the tube may have a significant effect on the shape of the NGC, especially for the shorter tubes of interest here.

    Note that while the NGC is discussed, it is actually the "Laser Output Power Curve" or LOPC that provides the input variables for most of these techniques. However, we may use the two interchangeably in discussions, even though purists will probably object. :)

    Methods of Controlling Cavity Length

    All stablization schemes are based on the precise control of the HeNe laser's cavity length, either directly or indirectly:

    Implementation Issues Common to all Locking Techniques

    In actually designing a practical stabilized HeNe, there are several functions that need to be performed regardless of how it is actually locked:

    1. Turn on the laser tube and detect that it lights with adequate power.
    2. For thermally controlled lasers, warm up the tube to the desired operating point.
    3. Lock the laser to the reference (intrinsic or estrinsic).
    4. Detect loss of lock or inability to lock, loss of beam, etc.

    For a very basic implementation, (1), (2), and (4) can be done manually, though most systems use either a temperature sensor some type of timing of mode sweep or simply a fixed delay to determine when the laser is ready. Actual locking (3) may use a variety of electronic from simple to complex, a microprocessor, or a combination of the two.

    Before the availability of inexpensive microprocessors in the early 1980s or thereabouts, controller implementation consisted of TTL or CMOS ICs for logic and timing along with op-amps for the actual feedback loop. (Or discrete transistors or vacuum tubes before that!) These were effective, inexpensive, and easy to repair should the need arise. But as time went on, the parts that were used have become harder to find. At least one company, Agilent, came up with an intermediate solution using a Field Programmable Gate Array (FPGA) that essentialy replicated the a large portion of the discrete logic in a single chip. And engineers just can't resist redesigning perfectly satisfactory systems. ;-) Nowadays, a dirt-cheap single chip microprocessor or microcontroller (same thing) is the solution of choice.

    So, most stabilized HeNe lasers that are not legacy products from the 1980s or before use a microprocessor to perform most logic, timing, testing, and control functions, though some may use a purely analog implementation for actual locking feedback loop to reduce noise in the control signals that could end up modulating the optical frequency. For most users, this is not a problem. But as an example, the Melles Griot 05-STP-901 and functionally identical Spectra-Physics 117A which date from the early 1980s or before used Pulse Width Modulation - PWM - to drive the heater wrapped around the tube. (Many modern microprocessor-based implementations including µSLC1 use PWM as well.) Very finicky users have detected the residual ~5 kHz PWM in the laser's optical frequency and complained. This would probably only show up if the output of a laser like this were beat - combined so that a difference frequency could be detected - with the output of another laser and the result displayed on an RF spectrum analyzer or similar instrument. A trivial change to the electronics can convert the PWM to a purely linear control loop. With a microprocessor, switching to a Digital to Analog (D/A) output instead of PWM would also greatly reduce digital noise in the feedback loop.

    The benefits to the user of a microprocessor-based controller are in flexibility, reliability, and cost. The benefits for the manufacturer also include the system now being proprietary - user repair, among other things, is virtually impossible because the smarts are in the software/firmware, which is generally not made available to anyone outside the company or their authorized service organization. If a TL084 op-amp went belly-up in an SP-117A, basic troubleshooting techniques could be used to repair it. Or if the laser tube required replacing, there were three trim-pots to perform all adjustments. With a similar modern laser, repair of all but the most obvious problems like a bad DC power supply or blown fuse is virtually impossible. In some cases, replacing the tube requires access to firmware parameters to set various constants. Even identical model HeNe laser tubes (assuming one is avilable) may differ in the output power of the waste beam from the back of the tube - which is often used for the feedback. There may be workarounds by adding a PCB with adjustable op-amp circuits to fake the signals derived from the tube to match what the firmware expects, but these are not ideal solutions. There is a silver lining for the user though - it's impossible to break anything by opening the case and twiddling adjustments because there are none. (Although that's not always strictly the case, as with µSLC1 where the coarse mode gain adjustments are trim-pots!)

    Having said all that, any new stabilized HeNe IS going to use a microprocessor for the bulk of the controller, with perhaps an analog section for the actual feedback loop. Being able to tune the control loop by changing parameters rather than soldering components or even adjusting trim-pots is just far superior for development and maintenance. However, there will then generally be No User Serviceable Parts inside. ;-)

    Effects of Temperature, Pressure, and Gas-Fill

    Aside from the effects on the physical dimensions of the tube, the center of the NGC depends on the gas temperature and pressure, and ambient/tube temperature affects the internal pressure directly as well as from changes to the tube structure.

          Cause             Sensitivity       Comments    
      Helium Pressure      +22 MHz/Torr       Pressure of He decreases with use
      Neon Pressure        -25 MHz/Torr       Pressure of Ne decreases with use
      Neon Isotopic Ratio  +10 MHz/% of 22Ne   Ratio of 22Ne:20Ne Decreases with use
      Temperature          +280 kHz/°C        Affected by specific lock point

    Under normal conditions, the changes in internal pressure are likely to be much less than 1 Torr and temperature itself has only a small affect on the gain center. The major one is gas fill ratio of 22Ne:20Ne. This is of course determined at the time of manufacture (and may not be that accurate), but will also decline slightly with use as 22Ne will be trapped at a slightly a higher rate than 20Ne.

    One way to assure that the tube itself runs at a relatively fixed known temperature is to warm it up to a set-point temperature rather than using an indirect method like the rate of mode sweep to determine when to lock. And then to fine tune that after awhile to give everything time to reach thermal equilibrium. Once locked in this manner, the temperature of the tube will remain relatively constant. The improve it even further, at least two companies (Lab for Science and MicroG) put the tube (with its heater wrap) in a temperature-controlled housing. Most do not.

    More on this may be found in the chapter: Commercial Stabilized HeNe Lasers.

    Testing of Stabilized HeNe Lasers

  • Back to Stabilized HeNe Lasers Sub-Table of Contents.

    Intrinsic Stabilization Techniques

    Tube Requirements for Non-Zeeman Stabilized HeNe Lasers

    While the laser tubes used in many very expensive stabilized HeNe lasers may be virtually identical to those that used to be found in grocery store barcode scanners, one cannot take any old tube found on the street and expect it to be usable in a stabilized laser. Most of these requirements are common to all of the intrinsic stabilization techniques. Any specific ones will be noted.

    Where multiple modes are present when the laser is locked, all of them may be used as output. Specifically where 2 modes are present, the laser may be set up to produce a beam with two optical frequencies separated by approximately the longitudinal mode spacing of the laser tube. Since the locking techniques do not change for these, they are not coveered separately.

    Unstabilized HeNe Lasers

    In the grand scheme of things, common mass produced internal mirror HeNe laser tubes are darn good without requiring any fancy stabilization. They have a typical coherence length of a few inches and an absolute optical frequency accuracy of around 2 to 3 ppm. For many applications, even high precision ones including interferometry where the path length difference is small or holography of small objects, these are more than good enough. And we have the NGC to thank for it all. ;-) Thus, before committing to a much more expensive stabilized HeNe laser, a determination needs to be made of the actual requirements. And generally, unstabilized HeNes are capable of much higher power.

    In the chart above, there is an entry for multiple transverse mode (non-TEM00) lasers. While technically, the lasing modes are all within the NGC and thus limited to a gain bandwidth of 1.5 or 1.6 GHz and thus around 3 ppm, as a practical matter, their relative optical frequencies is for all intents and purposes, unpreidctable. So, using such a laser as a reference for anything could be....interesting. Thus, there are no values given for the optical frequency variation or accuracy.

    For the unstabilized single transverse mode laser - which describes most red HeNe lasers that aren't stabilized - there will be multiple longitudinal modes but they will be separated by approximately the cavity FSR or c/2L. Coherence length (or period) is thus predictable, if short compared to single longitudinal mode stabilized lasers. However, as the length of the tube and output power increases, the modes become much less well behaved due to mode competition. The relative amplitudes of the modes tends to change at random with only loose regard for the profile of the NGC.

    Stabilization without Active Feedback

    It is possible to stabilize a HeNe laser by simply controlling its environment, mainly temperature. Of course, that will generally require some feedback of its own, but not of the laser tube specifically. One of the earliest stabilized HeNe lasers - the Spectra-Physics 119 - was available both with and without the "Servo Option". Without it, stabilization was strictly based on setting the temperaturee of the tube enclosure. With a sufficiently long warmup of a few hours (!!) this was effective reducing the uncertainly in optical frequency from the width of the NGC (1.5 to 1.6 GHz) to around 75 MHz - a reduction by a factor of 20 or more to below 0.15 parts per million (ppm). But with the Servo Option, which provided Lamp Dip stabilization (see the section below) uncertainty dropped to 5 MHz or 10 parts per billion (ppb).

    While there is no active feedback based on the NGC, a human must set the mode position based on the NGC, so it is still intrinsic. ;-)

    Any HeNe laser tube suitable for a stabilized HeNe laser can be controlled in this manner. Depending on tube size, a 1 °C change in tube temperature will change the mode position by few hundred MHz or more, so temperature control is required to a small fraction of a degree is required. But this is not difficult even with the electronics that was available in the 1960s.

    However, to truly reduce the uncertainly, some form of optical feedback is needed.

    Stabilization using a Single Mode

    This means that the feedback variable is derived from only a single lasing mode.

    Intensity Stabilizion

    Basic intensity stabilization uses the amplitude of the output of a single polarized mode for locking as shown in Single-Mode Single-Frequency Stabilized HeNe Laser. The diagram shows a purely analog electronic implementation of the controller, but modern systems would likely use a microcontroller to implement the locking algorithm. An example is shown in Single or Dual Mode Polarization Stabilized HeNe Laser using µSLC1 Controller.

    A random polarized tube is generally used since over a large portion of mode sweep, even a relatively short tube will actually produce 2 modes. For use with random polarized tubes, a polarizing beam splitter blocks the unwanted mode and a non-polarizing beam sampler diverts a small portion of the output beam to a photodiode to be used for locking feedback. Or if both modes are desired in the output, the mode used for feedback can be diverted using a beam sampler, or taken from the waste beam at the back of the laser.

    To provide the ability to move the lock point over a large portion of the LOPC with no possibility of a third mode popping up, the tube must have a cavity length of less than about 200 mm.

    Short polarized tubes could also be intensity-locked, though it's not clear why this would be desirable: There is no advantage to using a polarized tube in a single frequency laser with a serious limitation in output power since the tube has to be short enough so that only a single mode is lasing when locked as the unwanted mode cannot be removed with a polarizer.

    The only purely single mode stabilized HeNes I am aware of are the Aerotech S100 which morphed into the Melles Griot 05-STP-91x series. These are NOT microprocessor controlled. ;-) Although newer versions of this laser actually have hooks in place to support conversion to a dual mode stabilized laser by adding a photodiode and changing a jumper, this is not publicized. :) The 05-STP-91x lasers lock on the side of the LOPC using a novel induction heating approach originally developed by Aerotech. This is compact and allows for fast time-to-lock, but the more conventional heater wrap can also be used. More info on these lasers may be found in the section: Aerotech Stabilized HeNe Lasers.

    Most dual mode stabilized HeNe lasers have a user selectable option (switch, jumper, or logic input) to lock to a single mode. These are described below.

    Gain Peak Stabilizion

    Lamb Dip Stabilizion

    Stabilization using Two Modes

    Dual Mode Polarization Stabilization

    Dual mode polarization stabilization uses the relative amplitudes of the two polarizations from the laser tube for locking. See Dual-Mode Single-Frequency Stabilized HeNe Laser. For frequency stabilization, they are generally forced to be equal and thus parked equidistant on either side of the LOPC. However, their relative position can be changed (slowly) over a modest range if desired. This is usually done by a knob, an external modulation signal, or a software command. A polarizer can block the unwanted mode because they are orthogonally polarized. Or, the laser may be used with both modes thus outputting two frequencies separated by the tube's longitudinal mode spacing. The diagram shows a purely analog electronic implementation of the controller, but most modern systems use a microcontroller to implement the locking algorithm. An example is shown in Single or Dual Mode Polarization Stabilized HeNe Laser using uSLC1d1.gif Controller.

    Dual mode polarization is by far the most popular technique used in commercial stabilized HeNe lasers at the present time. It is also the only common approach offering the highest power in a pure single longitudinal mode (single optical frequency). With a lively tube, this can be 2 mW or more in a single mode when the modes are balanced. For greater power, they can be offset somewhat with either frequency or intensity stabilization providing up to 2.25 mW or even more in a pure single mode. (However, 1.5 mW and 1.75 mW, respectively, are more typical in stock tubes unless specifically selected for high power.) The limiting factor is either where a third mode appears, or where the output mode approaches the center of the NGC. To get higher power without fancy and expensive additional complexity like an intra-cavity tuned etalon requires going to three mode stabilization. But then the output mode is never quite pure regardless of locking technique. For many applications a few percent of unwanted amplitude or frequency modulation may be acceptable.

    Laboratory lasers using dual mode polarization stabilization often also have optional intensity stabilization selected by a switch, logic level, jumper, or software, where one of the modes is locked to a reference level rather than the two modes being compared. A means of changing the reference level may also be provided. There will still be only a single mode present (when the other one is blocked) over a fairly wide range of optical frequencies on either side of the point where the two modes are equal so that the output intensity can be adjusted up or down. Specifically, with intensity stabilization, it may be set up to output somewhat higher power.

    The tradeoff is that the optical frequency accuracy and stability is better when both modes are used, but at the expense of intensity stability. But the intensity stability is better using the single mode.

    Stabilization using Three Modes

    Three mode stabilization can provide just about the highest power possible in a stabilized HeNe laser using an off-the-shelf internal mirror laser tube. This can be double or more compared to the typical 1.5 mW of commercial dual polarization stabilized lasers.

    However, it is not without drawbacks. These are related to mode purity and long term absolute frequency drift. When three modes are lasing in a HeNe tube, there will also be three relatively weak "ghost" modes very close to the lasing modes. There are caused by third order non-linear dynamics. The difference in optical frequency between the ghost modes and lasing modes of a up to a few hundred kHz is exploited by second order beat stabilization for locking (but not for the other techniques). There is no practical way to remove the ghost mode associated with the centered (main) mode from the output. So, strictly speaking, the output of these lasers is not truly pure single mode. In addition, to maximize output power, it's possible that some tubes may have small 4th and 5th normal lasing modes present 400 to 500 MHz from the closest desired lasing modes. Both of these are typically under 5 percent of the amplitude of the output, which could be acceptable for many applications. Two mode stabilization does not suffer from either of these issues except during warmup when three modes may be present during part of mode sweep. This is generally of no consequence to the ultimate application unless the laser is used during this period. So these two potential issues should be kept in mind in determining if the increased output power provided by the three mode techniques outweighs the presence of extra low level modes.

    A well behaved random polarized single transverse mode (TEMOO) HeNe laser tube 13 to 14 inches in length can provide 3 to 4 mW in a nearly pure single mode if it is centered on the LOPC. (As above, "well behaved" means that adjacent modes are orthogonally polarized and it is a non-flipper.) Two modes of the opposite polarization will straddle it and can be blocked in the output beam with a polarizer. Ideally, there will not be any other modes present. The next two ones would be just beyond the tails of the NGC. However, if the tube is very lively or a bit too long, they may poke their heads up and result in weak rogue modes that cannot be eliminated because they will have the same polarization as the desired centered mode. If the tube is shorter, those weak modes can be guaranteed to disappear entirely, but with a sacrifice in output power. So, it's a tradeoff of output in the dominant mode versus the rogue weak ones. For many applications, a few percent in modes almost 1 GHz or more away from the dominant made is acceptable. However, for some stabilization techniques, the additional modes, even though weak, may introduce noise in the locking signal. The ramafication so of this are left as an exercise for the student.

    Suitable tubes for three Mode stabilized laser should include the Melles Griot 05-LHR-150, Siemens/LASOS LGR-7627, and JDSU 1125 as long as they are confirmed to have well behaved modes - they are not bouncing around due to mode competition and are not-flipping polarization. Nearly all red (633 nm) HeNes satisfy the requirement for adjacent modes to be orthogonally polarized. All three types should be available new or surplus. The older Aerotech OEM5R may also be suitable. These are all rated 5 mW but new samples may have much more power output up to 8 mW or more.

    Three approches to three mode stabilization are discussed below. The simplest one overall is probably second order beat stabilization and has the potential to provide the best optical frequency stability.

    But whether it is worth going to any of these more complex, more expensive, and physically larger schemes for a benefit of few tenths of a mW will depend on the application. As a practical matter, to guarantee that the rogue mode amplitude will be minimal, at most 3.5 mW will be available in a single (mostly) pure mode. And to accomodate variations in tube performances, it may be closer to 3.0 mW. Consider that the slightly shorter tubes for dual mode polarization stabilization can be spec'd to 4 mW or more. I've measured output power from tubes that were not brand new as high as 4.5 mW. But even at 4.0 mW, the balanced lock point would be 2.0 mW. And by offsetting the lock point slightly, 2.25 mW or even slightly greater power may be available in a single pure mode with a simpler more conventional system.

    In addition, when designed for maximum power, there will be little to no tunability of optical frequency - the output mode MUST be centered on the NGC. Where tunability is a requirement, three mode stabilization can still be used, but maximum output power will be somewhat lower, and will vary with the lock point. However, it will then provide higher power from a tube otherwise suitable for dual mode stabilization since the region at the peak of the NGC will be usable.

    Three Mode Stabilization using Second Order Beat

    This is a relatively simple implementation as shown in HeNe Laser Using Second Order Beat Frequency Stabilization. It may also be capable of the highest stability of any of the intrinsic techniques, at least short term, though this is not really known. But the same considerations with respect to additional complexity, size, and cost discussed above will apply.

    The HeNe laser tube requirements are basically as discussed above, where (ideally) at most 3 modes can oscillate when one of them is centered on the NGC. In the diagram, the tube length is such that this requirement is met. If one is willing to accept a small amount of output on the two additional modes that would be present with a slightly longer tube, or one that is livelier, then a bit more power in the centered mode may be possible. However, the rogue modes will result in additional low level beat signals which may result in locking problems. Thus, assuring the tube is pure 3 modes is desirable, at least until the basic design has been tested. This can be often be accomplished on a lively or slighty too long tube with little loss of power by carefully slightly misaligning the OC mirror.

    When a HeNe laser is oscillating with three longitudinal modes, there will be primary difference frequencies corresponding to the distances between the lasing modes, and secondary difference frequencies between pairs of primaries. While the primary difference frequencies differ by approximately the longitudinal mode spacing of 400 to 500 MHz for this length tube, the secondary difference frequencies are in the hundreds of kHz range and easily detected and used as the locking variable. Note that if there are rogue 4th and 5th modes oscillating, there may be other primary, secondary, and tertiary difference frequencies to contend with.

    A paper describing the use of the second order beat for stabilizing a HeNe laser is: "Frequency stabilized HeNe gas laser with 3.5 mW from a single mode", Jonathan D. Ellis, Dirk Voigt, Jo W. Spronck, Ad L. Verlaan, Robert H. Munnig Schmidt, Elservier, Precision Engineering, 36(2012), pp. 203-209.

    From the paper:

    "When nearly symmetric in the HeNe gain profile, the three mode laser contains three additional low power modes. The three additional smaller modes arise from third-order non-linear harmonics and their exact frequency difference with respect to their nearest adjacent mode depends on cavity tuning and the excitation state of the active medium. In this work, the frequency difference between a smaller mode and its main mode, vb, ranged between 200 kHz and 550 kHz. The three main modes from lowest frequency to highest are v1, v2, and v3 and the three smaller mode frequencies are (2v2-v3), (v1+v2-v3), and (2v2-v1). Alternative expressions for the three smaller modes are (v1+vb), (v2-vb), and (v3+vb), respectively."

    Since the frequency of (v2-vb) will be in the range of hundreds of kHz and a strong function of center mode position on the NGC, it can be used for locking.

    The only known commercial stabilized HeNe laser that is known to have employed the Second Order Beat (SOB) locking technique was the Laboratory for Science 260. Only about 10 of these were ever manufactured and can you believe it, I have not seen a single sample. :( :) The LFS-260 dates from the late 1980s or early 1990s and used a Phase Locked Loop (PLL) IC to lock the beat to a crystal controlled frequency synthesizer. This still may be the approach with the best precision and stability, but nowadays a microprocessor can do almost as good a job with much more flexibility. I suppose LFS didn't publish to (1) keep the technology proprietary and (2) so others wouldn't think they were nutcases. :)

    Here is the theory of operation from the LFS-260 brochure:

    "In a laser with three TEM00 modes, there will be two primary beat frequencies corresponding to the difference frequencies between the central mode and each of the modes on either side of center. These two beat frequencies, typically in the range of 400 to 500 MHz, will in general not be exactly the same because the frequency pulling effects on each mode will vary with the differing slopes at the respective operating points on the Doppler gain curve. The difference between these two beat frequencies will yield a third or intercombinational beat frequency typically in the range of 100 kHz. In an integral end mirror tube, where the alternate modes are orthogonally polarized, the intercombinational beat frequency will not be zero even when the central mode is at line center because of the birefringence of the mirrors. In the Model 260, the laser tube is preselected not only for power but also for an appropriate range in the intercombinational beat frequency. The median frequency is then tightly phase locked to the frequency of a crystal controlled frequency synthesizer. "

    In HeNe Laser Using Second Order Beat Frequency Stabilization, the tube length is such that only three modes can oscillate when one of them is centered on the NGC. If one is willing to accept a small amount of output on the two additional modes that would be present with a slightly longer tube, or one that is livelier, then a bit more power in the centered mode would be possible.

    The Black Hole is supposed to capture every last photon of the undesired modes. (LFS called their version a "black etalon", but I think black hole better captures the spirit of its function.) However, something more easily obtained will suffice, just as long as it doesn't reflect back into the laser. ;-)

    The above paper uses a photodetector sampling the output polarization to obtain the beat signal for use in locking. In my initial tests using a Melles Griot 05-LHR-150 tube, there was a strong beat present at the lock point when taken from both the output polarization (centered mode) and blocked polarization (outer modes). So it may also be possible to use the blocked polarization since it contains the outer modes. In that case, the Black Hole would need to be moved to after the beam sampler. I hope it doesn't weigh too much. :) However, the paper suggests that this may have more non-linearities in the locking signal. There's a lot going on here, some of which may not be intuitively obvious.

    The exact beat frequency where the lasing mode is centered is not the same for each tube sample due to differences in parameters like mirror birefringence and orientation, this would need to be tested and entered as a constant into the firmware or PLL synthesizer. The correspondance of lock frequency to aboluste optical frequency depends on many factors. While LFS claims locking parameters in the model 260 don't change much. this may not be entirely true. For example, the lock point for the same absolute optical frequency is a strong function of tube (gas) temperature and pressure. So the exact lock temperature and tube aging will affect them. And maintaining the same optical frequency may impact the output power if it moves off from center on the NGC.

    The locking variable is the second order beat frequency. This typically a few hundred kHz in amplitude modulation depth of between 0.5 and 5 percent of the power in the centered mode. Extracting it and converting to a TTL signal is not entirely trivial, expecially where it is desired to minimize reduction in the usable output power. Ideally, it should be taken from the waste beam which has a typical single mode power of only around 25 µW, resulting in a DC photodiode current of around 10 µA and an AC signal of under 1 nA. The detector circuit would require careful analog design using low noise construction techniques. For my prototype, I am sampling the output beam with a glass plate and using an HP/Agilent 10780A, which has barely enough sesitivity even with the 300 µW available there. It would not work at all using the waste beam. (The 10780 has no problem with under 10 µW when used in its normal application with HP/Agilent two frequency HeNe lasers, but then the useful signal is 25 to 50 percent of the total power, not under 5 percent or less.)

    In addition, any ripple in the HeNe laser power supply also modulates the amplitude of the laser's output, and it may have similar or greater AC amplitude as the second order beat. If the DC current is set optimally, the dominant contribution of the ripple frequency will be at twice the power supply switching frequency. In tests, it was necessary to add an external ripple reducer to the standard Melles Griot 05-LPL-902 power supply for the 05-LHR-150 laser tube and another stage might be desirable. While the typical switching frequency is below the expected beat frequency and the optical receiver can filter this to some extent, strong harmonics will still be present, especially that second harmonic. A fully analog supply would be suprior with additional filtering of both the DC rail (to eliminate ripple at the AC line frequency and its harmonics) and ripple reduction in the output (to suppress zener noise/plasma oscillation ripple).

    The controller would need to warmup the tube as with other more mundane locking techniques, and then use the a value derived from the difference between the reference value and actual second order beat to drive the heater. Since the relation of beat frequency to mode position and absolute optical frequency is a strong function of tube conditiona (internal temperature and pressure), it may be best to use tube temperature to determine when to turn on locking, rather than some measure of mode sweep rate or count.

    I am in the process of building a system of this type using a variation on the µSLC1 controller, µSLC2. A diagram is shown in in Three Mode HeNe Laser Using Second Order Beat Stabilization and a photo in Prototype Three Mode Stabilized HeNe Hardware with µSLC2. This provides both the P and S mode signals from the back of the tube and the beat signal using a modified HP 10780A optical receiver sampling the output beam. Using the output beam was done out of convenience since even sampling only 10 percent of it has much higher power than the waste beam and even then, the 10780A is barely sensitive enough.

    Stay tuned.

    To summarize some of the major issues:

    1. While the beat in the few hundred kHz range is used for locking, it will also be present in the output of the laser as a low level amplitude modulation or ripple, which cannot be removed. So strictly speaking, this type of stabilized HeNe laser is NOT pure single longitudinal mode or single frequency even without any rogue 4th and 5th modes present. The impurity is probably between 0.5 and 5 percent of the total power. The same would be true of ANY HeNe with 3 or more longitudinal modes present from the tube, not only those using second order beat stabilization.

    2. Since the beam detector looks at amplitude modulation of the output, the HeNe laser power supply will need to be a very low noise unit. Preferably this would be fully linear, but that would probably mean a custom design as virtually all modern HeNe laser power supplies are switchmode. These operate in the 20-100 kHz range with harmonics similar to the relevant frequencies for the beat signal. More than one stage of ripple reduction on the output may be required.

    3. According to the paper, it appears as though the operating temperature critically affects the beat-versus-optical frequency/location on the neon gain curve. Therefore, it may be necessary to add a temperature sensor to the tube and warmup to a specific temperature rather than going by mode sweep cycle time to determine when to lock.

    4. It's not clear how tube use/aging will affect behavior since this also results in changes to the gas pressure/temperature of the tube. So it is not known if these can be a "set and forget" type system or whether they would require periodic tuning and/or whether this can be automatically performed by the controller firmware.

      Each system will need to be set up and tuned for the specific tube used. It's not known if all samples of tubes of the same model will even be satisfactory in terms of beat range and behavior since the manufacturer is not going to test the relevant parameters and is usually optimizing for total power.

    5. Although the paper claims 3.5 mW, it is not known whether this is realistic in a production system. Hopefully the manufacturer will be able to tweak the design for maximum power in the main mode but at low volume, this may not be realistic.

    So there's a lot going on here compared to the traditional dual mode laser. (Much of this applies to any three mode laser, not only one using second order beat stabilization.)

    Three Mode Stabilization using PDH Locking

    > It may also be possible to use the amplitudes of the polarized modes to lock.

    However, (1) the modes do not change in amplitude by very much - perhaps 5 to 10 percent of the total power and (2) the lock point will NOT be where their amplitudes cross as with the dual mode stabilization, but rather where one is maximum and the other is minimum, and they are nearly constant in these locations. Therefore, a simple comparator cannot be used. Rather a technique that locks to the peak or valley of a function of the mode signals is required. One is called Pound-Drever-Hall locking. Essentially, the cavity length is periodically dithered by a small amount and the laser is locked to a zero crossing of the 2nd harmonic of the mode signal. This sounds hairier than it is. A microprocessor can do it in real-time and electronic systems and even ICs exist for various applications. They are called "lock-in amplifiers", "synchronous demodulators", or "phase sensitive detectors.

    As noted, a microprocessor can also implement PDH locking. For something inexpensive like the Atmega Nano 3.0 used in µSLC1, the dither frequency would need to be limited to a few hundred Hz. Although dither frequencies of a few kHz have typically been used, this should be adequate.

    Hardware is similar to that of seond order locking, but with no need for the beat detector. A photodiode is needed to monitor one of the polarized mode amplitudes to be used as the PDH variable, but monitoring both will provide double the signal-noise-ratio. There would also need to be some means of dithering the cavity. A suitably designed heater may have enough bandwidth if driven with a high level AC signal on top of the one for maintaining cavity length, but if not, then an electromagnetic (voice coil or solenoid) could be attached to act on one of the mirror mount stems. This dither will show up in the output as modulation of the optical frequency (along with the second order beat signal).

    It's not likely that PDH locking would provide any real advantage compared to either of the other approaches and using the second order beat is probably simpler.

    Stabilization of Axial Zeeman HeNe Lasers

    Tube Requirements for Axial Zeeman Two Frequency Stabilized HeNe Lasers

    The tube requirements for two-frequency axial Zeeman lasers are very similar to those for non-Zeeman stabilized HeNe lasers but not identical:

    Two Frequency Axial Zeeman Stabilization

    Nearly all the two-frequency HeNe lasers used to position wafers in multi-multi-million dollar semiconductor Fabs and other super high precision metrology applications use dual mode polarization stabilization. See Dual-Mode Stabilized Axial Zeeman-Split Dual-Frequency HeNe Laser, which can also, of course use microprocessor as in µSLC1. The shape of the NGC/LOPC differs due to mode competition of the short tube in its axial Zeeman magnetic field, but locking is similar. And non-Zeeman two-frequency lasers such as those from Zygo also use dual mode polarization stabilization.

    There are a few variations. Most HP/Agilent/Keysight lasers use a clever implementation with a single photodiode behind an LCD polarization rotator and polarizing filter that alternately samples the H and V polarized modes. Sample-and-hold circuits capture the values and these are what are used to control the feedback loop. This approach is largely immune to drift in the electronics over the life of the laser tube. The Spindler and Hoywer ZL-150 is the only known axial Zeeman laser that does not use dual mode polarization stabilization, but rather mechanically dithers the laser tube cavity length and locks to the point where the split frequency is a maximum.

    Note that locking to a specific split frequency using a PLL or similar technique is generally NOT recommended as its exact value depends on many factors including the power output of the tube and local magnetic fields. As the tube ages with use, power output generally declines and the splite frequency increases. Any external magnetic fields - even the magnetized base of an optics mount or another similar Zeeman laser - will change the split frequency. So, the laser may not remain at the center of the split gain curves as desired.

    Stabilization of Transverse Zeeman HeNe Lasers

    Tube Requirements for Transverse Zeeman Two Frequency Stabilized HeNe Lasers

    Two Frequency Transverse Zeeman Stabilization

    The transverse Zeeman HeNe has to potential to produce truly high power (at least for this sort of laser), in a split single mode than any of the others discussed so far. When a transverse magnetic field is applied to a random polarized HeNe operating with 3 modes with one centered (as in the three mode lasers described above), if the field strength is such that the Zeeman shift is the same as the cavity mode spacing, it is possible for the modes on the sides to be suppressed with all the power collapsing into the main center cavity mode. Up to 5 mW or more may be possible with this scheme. The required field strength should be on the order of c/2L/2.8 G, or around 150 G for a typical 5 mW tube with a cavity length of 350 cm.

    However, there is, as always, a catch. ;-) Although the papers talk about a single mode, it's actually a pair of closely-spaced H and V compoennts using the same cavity mode, similar to the axial Zeeman laser but generally with a much smaller frequency difference in the 10s to 100s of kHz range. For many applications, a coherence length of a mile is still adequate. :) Of course either of the H and V components can be separated out with a polarizer, but then the power is cut in half.

    When I found the first reference, I thought it really meant pure single mode greater than 5 mW. Nope, must read the fine print. :( :)

    Reference: Robert J. Knollenberg, "Prospects for the Helium-Neon Laser Through the End of the Century", SPIE Vol. 741, Design of Optical Systems Incorporating Low Power Lasers (1987). The paper mentions it briefly, but has two other references, 17 and 18 which should be more detailed. (This paper also describes the original HP axial Zeeman laser and doesn't get it quite right, unless it's a prototype that documented anywhere.)

    There were at least two commercial transverse Zeeman stabilized HeNe laser. The most well known (to me at least) is the Laboratory for Science 220. And, yes, I have two working samples of this laser. ;-) The only one I know of (at least in a product blurb) is the NEOARK NEO-262.

    Scanning Fabry-Perot Interferometer Stabilization

    This is a very straightforward (if challenging) implementation in which a microcontroller essentially replaces the human observer looking at a Scanning Fabry-Perot Interferometer (SFPI) display of the lasing modes in real-time. See HeNe Laser Using Scanning Fabry-Perot Interferometer for Stabilization. This is shown for a three mode stabilized HeNe laser implementation, but the same technique can be used with single or dual mode stabilization, though it's not clear what, if any benefits it may provide where the simpler alternatives described above exist. In the diagram, the tube length is such that only three modes can oscillate when one of them is centered on the NGC. If one is willing to accept a small amount of output on the two additional modes that would be present with a slightly longer tube, or one that is livelier, then a bit more power in the centered mode would be possible. For single or dual mode polarization stabilization, the tube would be limited to a length of around 250 mm so that two orthogonally polarized modes would straddle the gain curve with no additional modes present of the same polarization as the one selected for the output.

    The feedback is implemented with a low finesse SFPI using the waste beam behind the HR mirror. The low finesse results in spread out peaks, but these are better to analyze because they can be averaged and are then less sensitive to the exact position of the digital samples. As a result, to reduce the space requirements for the SFPI using available mirrors, a sub-confocal spherical or hemispherical SFPI cavity can be used with an FSR larger than the neon gain bandwidth and a mirror spacing of under 1 cm.

    To simplify computing requirements, a dual polarization SFPI detector can be employed. Then the orthogonally polarized modes will be separated resulting in unambiguous determination of the polarization of the modes of orthogoanl polarization orientation. However, for a dual polarization detector to be effective, the SFPI mirrors must either have zero birefringence, or their birefringent axes must be aligned with the tube's polarization axes. Otherwise, the mirror birefringence will overwhelm the polarization of the modes.

    As with any HeNe laser, back-reflections must be minimized to the maximum extent possible by orienting the optics such that direct reflections back into the tube are prevented. Thus the PBS should be at a slight angle and the SFPI should be offset and have an aperture as shown in the diagram so that the internal reflected beams do not re-enter the laser.

    A polarizing beam-splitter at the front of the laser both selects the desired polarized mode for output and provides feedback to monitor laser power since doing that through the SFPI may not be consistent. Although the sampled power is of the blocked mode(s), not the output mode, the output power can be inferred since their relative amplitudes can be determined by the firmware. If preferred, a non-polarizing beam sampler could be added to obtain the amplitudes of both polarized modes. But that would reduce output power slightly.

    The locking algorithm would have the same general state structure as for the single and dual polarized mode locked except that the error terms will be determined by analyzing SFPI data in real time to center a mode of the desired polarization. Thus a microprocessor with higher performance including a higher A/D sampling rate may be desirable.

    Note that this is NOT quite the same as using an external reference for locking. (More on that below.) It's still an intrinsic method using the NGC as the reference. Thus, while drift in the SFPI due to temperature changes or whatever is still a consideration and will impact the locking algorithm, it will not affect he ultimate performance in terms of absolute optical frequency accuracy or stability.

    General Purpose Intrinsic Stabilized HeNe Laser Testbed

    This platform would permit any of the common techniques to be implemented including hardware, firmware, and GUI. With its build-in SFPI, it would also provide mode monitoring even if not used for stabilization.

  • Back to Stabilized HeNe Lasers Sub-Table of Contents.

    Extrinsic Stabilization Techniques

    Iodine (or Other Gas) Cell Stabilization

    These use the absorption spectrum or emission spectrum of a material - usually a gas - as the reference. For the HeNe laser, iodine vapor has been the preferred substance. Iodine at a controlled temperature and pressure has numerous absorption lines in its spectrum at precisely known locations in terms of optical frequency or wavelength. There are about a dozen within the NGC which can act as markers for stabilization. The most accurate commercial HeNe optical frequency reference lasers use iodine stabilization.

    NIST/Frazier Intra-Cavity Implementations

    The Iodine Stabilized HeNe Laser (ISHL) provides the most precise absolute optical frequency reference in any commercial system. It is based on the fact that iodine (or more accurately, I2 vapor) under a range of temperature and pressure has numerous spectral absorption lines whose absolute optical frequency is essentially fixed and known for each one. To make use of this, the ISHL essentially locks to one of these absorption lines using an "iodine cell" - a sealed temperature-controlled glass tube with Brewster window termination to minimize losses and a speck of solid iodine inside that maintains a constant pressure of I2 vapor.

    However a normal internal mirror HeNe laser tube cannot be used since (1) locking requires the use of the PDH technique involving dithering the cavity length and (2) the dip in power due to these lines is only about 0.15 percent. At least that was the thinking of the designers of these lasers in the 1980s. Dithering is possible. In fact, as noted, it may occur inadvertently due to the heater characteristics. And a special heater could be designed that maximizes rather than minimizes this vibration. Dither could also be introduced by a mechanical means such as a voice coil positioner attached to one end of the tube. This was in fact done for an axial Zeeman laser, the Spindler and Hoyer ZL-150. so a higher power than can be provided by a single freqeuncy HeNe laser is required. Getting enough power is perhaps more of an issue. The solution generally used was to place the iodine cell inside the laser cavity where a HeNe laser tube with two Brewster windows was used as the gain medium. Putting the iodine cell inside the cavity can take advantage of the higher circulating power there AND there would be an amplification effect on small changes in absorption not present if simply put in a beam with a single pass. And PZTs on one or both mirrors would then be able to easily dither the cavity length for the PDH locking, as well as changing it by a larger amount to select the lock point. But going intra-cavity creates problems of its own. Specifically that to accomodate the length of a two-Brewster tube with enough power to be useful AND the iodine cell, the total cavity length needs to be more than 300 mm. It is actually around 350 mm for the Frazier version. And as we know from previous discussions, such a long laser will NEVER be single frequency (one mode oscillating, required for the ISHL) unless special means are taken to force it to be so. One method that has been used in these lasers is to introduce sufficient losses that only a single mode has enough gain to lase. This cam be accomplished by using a very low reflectivity output mirror - only 93% reflectance in the original NIST paper. However, deliberate misalignment of the Brewster orientation of the laser tube and I2 cell would work just as well and provide a means of increasing power as the tube ages. And tests of a ISHL resonator similar to the one used by Frazier confirms an OC reflectivity of between 0.99 and 0.994 percent. Its Radius of Curvature (RoC) is around 60 cm which is long enough to have no impact on longitudinal mode selection with the planar HR. The downside of any approach using such a long cavity is than when designed or adjusted so only a single longitudinal mode can oscillate, the available output power from the laser is order of only 100 µW! Anything higher and there will be another mode present which cannot be removed inside the cavity. To obtain higher power, one technique is to "offset lock" a conventional stabilized HeNe laser to the ISHL. While strightforward, this does of course add complexity and cost.

    Some straightforward modifications would enable the cavity to be somewhat shorter as well as simplifying maintenance. Substituting a one-Brewster 05-LHB-270 for the 05-LHB-290 would eliminate one Brewster window and the external HR mirror, both of which can collect dust and other contamination, as well as the additional losses from the inner surface of the 2-B tube's second window. These tubes are otherwise identical in size and bore diameter. However, the internal HR mirror is not planar but probably has an RoC of 60 cm. Apparently, putting the I2 cell close to the planar mirror is preferred anyhow due to desire for planar wavefronts in there. Using the 1-B tube would not permit a PZT behind the HR, so a single PZT for the OC would be driven with the dither and line selection PZT drive signals combined electronically. If it is necessary to maintain the same cavity geometry, a planar mirror could be used for the external OC.

    ISHL Using Internal Mirror HeNe Laser Tube 1

    As noted above, the use of the intra-cavity two-Brewster HeNe laser (gain) tube and 2-B iodine cell is an established technique that works but requires a special and expensive HeNe laser tube, requires meticulous cleanliness of 6 optical surfaces, critical alignment, and suffers from low power. And the low power is an inherent result of special means being required to force single longitudinal mode operation in the necessarily long cavity. Of course, one can't get around the need for an iodine cell, which is in itself expensive, but perhaps there are ways to get around the other deficiencies.

    Three things must be provided for an ISHL:

    1. Optical frequency tuning for line selection (slow and large).
    2. Optical frequency dither for the PDH locking (fast and small).
    3. Detection of the iodine line location.

    It should be possible to implement (1) and (2) using an off-the-shelf random polarized internal mirror HeNe laser tube suitable for a dual mode polarization stabilizeed HeNe laser, capable of up to 2 mW or perhaps even a bit more in a single longitudinal mode. Although a tube suitable for three mode stabilized laser can have over 3 mW in a single mode, that is only true when a mode is close to the center of the NGC. Go off to one side or the other, and another mode of the same polarization will appear, which cannot be eliminated by a polarizer or other (simple) means. But getting around 2 mW is 20 times better than the 100 µW of the intra-cavity ISHL.

    1. When run at a temperature slightly above typical for lasers using a heater surrounding the tube AND with adequate reserve power to the heater should be able to provide an optical frequency scan rate of one mode sweep cycle per second or better.

    2. For dither, there are a couple of options. It may be possible using a custom heater with the wires or conductors oriented mostly in the longitudinal direction - parallel to the tube axis. Then, applying an AC signal (on top of the cavity tuning signal) to the heater will result in a fairly fast response. Since this only needs to scan order of 1/1,000th of a full mode sweep cycle or less, it may be enough if the heater is in intimite contact/glued to the tube.

      Another possibility is to use a solenoid or voice coil positioner to push on one of the end-caps. Any parts with magnetization must be located away from the tube, but a small selenoid of the type used to xmove a shutter or actuate a lock can be attached via a plastic rod to one of the mirror mount stems and driven with an AC signal.

    Getting enough sensitivity from the iodine cell may be more of a challenge. The raw variation in absorption for the length iodine cell used in the NIST/Frazier ISHLs is around 0.15%. With the intra-cavity implementation, that is multiplied by circulating power of around 10 mW (100 µW output with a 99%R OC mirror). It is also increased by being relative to the lasing threshold by perhaps another factor of 2 or 3. So, even with a 2 mW beam, that's still a factor of 10 to 15 greater. One way to boost the sensitivity with an external iodine cell would be to force the beam to traverse it multiple times. With a cell of sufficient width, a pair of planar HR mirrors could be positioned such that the beam made multiple passes through the iodine cell. Better yet would be a custom cell that had the mirrors inside, thus eliminating most of the losses from the Brewster windows. Five round trips should not be difficult but more might be possible with careful alignment. Adjacent beam should not overlap to avoid etalon effects. Of course, such a custom iodine cell won't be inexpensive - assuming one can find a company willing to build such a thing. So, it may come down to constructing one at home. More on this below. :)

    ISHL Using Internal Mirror HeNe Laser Tube 2

    Rather than requiring a possibly custom multi-pass iodine cell, a normal one could be put inside the cavity of a high finesse SFPI. Then as the HeNe laser tube is tuned across the NGC, the SFPI would be set up to track it while the cavity length of the internal mirror HeNe laser tube is dithered. At an iodine absorption line, the finesse would drop significantly due to the additional 0.15% loss on each pass (equivalent to each mirror have a 0.15% reduction in reflectivity). The result would a dip that could blocked using a PDH technique. Depending on the desired tuning, range, the useful output power could be 2 to 3 mW. Dither Line select External sensitivity multiplier Multipass hall of mirrors SFPI Fluorescence instead of absorption detection

    External Reference Stabilization

    Offset Laser Stabilization

    Where higher power or a tunable output is desired from a reference like an iodine stabilized HeNe laser, the technique of choice is usually "offset locking". For example, a conventional dual mode stabilized HeNe laser can be offset locked to the ISHL by heterodying (beating) the two lasers together and using a Phase Locked Loop (PLL) to control the higher power laser's optical frequency. The offset can be adjusted using a the PLL configured as a frequency synthesizer. The offset can also be 0 Hz. In fact, this can be done with $10 in Radio Shack parts (at least when Radio Shack used to sell parts).

    Even higher power is possible using a temperature-controlled intra-cavity etalon to force single frequency in a large-frame HeNe laser, but this is beyond what we want to deal with here. ;-)

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