A Twonky Stabilized HeNe Laser Head

The Mostly True Saga of a Misbehaving Orphaned Laser

Introduction:

This partial laser head was found on the side of the road with no markings and no return address! :) (Don't I wish one could find lasers on the curb. Regrettably, all one finds around here are very dead lawn mowers. But I can't reveal the actual source, so some trivial details of this story have been modified in a way that has no effect on its technical accuracy.)

The reason I deduced it must be for a stabilized HeNe laser was the pair of extra wires sticking out of the front of the head with a low resistance between them - the heater. (I knew it wasn't a bomb because it didn't explode when the resistance was checked.) And the rear end-cap has the usual Alden cable as well as another one, exact purpose unknown. It's only a partial head because the front section which presumably would have the beam sampler and possibly other optical or electronic components was missing, apparently removed against the head's wishes with a pipe cutter. :( :)

From the appearance of the front of the laser tube inside the head cylinder, the visible part of a metal tube cylinder, it is clearly from PMS or REO. Being fairly new, that leaves REO. At this point I assumed it would be a bog-standard 2 to 3 mW random polarized laser tube, which isn't all that exciting other than its use in a stabilized application.

What ultimately attracted my interest to this laser head (no pun intended) aside from its existence was that a battery literally decided to roll toward the cylinder and then stuck to it. Huh? A magnet inside a cylindrical laser head? Now that's weird. I had never ever seen a cylindrical laser head - stabilized or not - with an internal magnet. Magnets may be present in Zeeman-split two-frequency HeNe metrology lasers or larger (and mostly older) HeNes with exposed bores, but never in modern cylindrical heads.

Basic lasing test:

The head ran fine on a HeNe laser power supply intended for 2 to 3 mW lasers, a Melles Griot 05-LPL-379 with an optimal current for maximum power of around 5 mA. The beam is boring red (633 nm), clean, and well collimated. The output power is around 3 mW and peaks after warmup, which is excellent for a head of this size. The mirror alignment is near optimal as determined by pressing on the exposed OC mirror mount. Based on these factors, easy start and run, and low dropout current, it's probably new or near new.

Lasing modes:

This is where its lasing behavior begins to become unusual. On the Scanning Fabry-Perot Interferometer (SFPI), it's clear that something strange is going on. Using my dual-polarization detector, the display is shown in Dual Polarization SPFI Display of HeNe Laser with Higher Order Spatial Modes. As shown, in addition to the normal expected orthogonally polarized modes (the mostly tall peaks), there are a pair of "rogue" modes at locations that are not a multiple of the longitudinal mode spacing. These are almost certainly higher order spatial modes meaning that the beam is not pure TEM00. However, since the amplitude of the rogue modes is relatively small, any deviation from pure TEM00 is not visible by eye and might not even show up using a fancy beam profiler. No wonder this was abandoned on the side of the road! A stabilized HeNe laser must be pure TEM00 to produce the desired single frequency when one polarized mode is selected at the output.

Removing the tube:

Well no sense is postponing the inevitable: Time to remove the tube from the cylinder. As soon as the rear end-cap was pulled off, it became clear that the tube would be even more interesting and there was no turning back. The actual removal process turned out to not be as terrible as I had feared. Although anchored using RTV Silicone (which doesn't yield to any solvents in finite time that don't also liquify human internal organs), it was soft enough, in small enough beads, and relatively near each end of the cylinder, that a thin steel strip could be used to cut through it all around. And in under 15 minutes, the tube was free and removing the unsightly RTV residue was straightforward. But what a strange tube this is....

See REO Tube from Stabilized HeNe Laser Head.

As expected, glued to the metal tube was a Kapton thin-film heater with what must be a temperature sensor - a 3 pin TO92 package glued near the center, unused with its legs clipped. The magnet is now clearly visible - a ferrite ring pressed onto the tube next to the where the metal part begins towards HR-end of the tube. But rather than the usual HR mirror, this tube has a funny dual HR configuration - one mirror at 45 degrees with another at 90 degrees to the tube axis. What???? Why???? Closeups of all of these "features" are shown in REO Stabilized HeNe Laser Tube Dual HR, Magnet, and Temperature Sensor.

At this point there are at least 3 mysteries:

  1. What's up with the higher order spatial modes? The usual cause in a tube intended to be TEM00 is that the bore is too wide for the mirror geometry. The HRs here are almost certainly planar, so this would mean the Radius of Curvature (RoC) of the OC is too small or the bore is too wide.

  2. What is the purpose of the dual HR? This configuration has sometimes been seen in low gain green REO tubes to introduce a polarization asymmetry in place of a Brewster plate. (The benefit is the potentially reduced losses compared to a Brewster plate that may be imperfectly cleaned and aligned, and have scatter from its surfaces.) That polarization preference is much less than the 7 percent or so introduced by a Brewster plate but adequate to completely linearly polarize a low gain laser. A quick test revealed that the waste beam exiting the 45 degree mirror is purely linearly polarized while the waste beam exiting the 90 degree mirror contains both polarizations. The pure linear polarization might be useful for sensing of one of the polarized modes but that's like turning a tree trunk on a lathe to manufacture a single toothpick. :) There are much cheaper ways of accomplishing the same thing.

  3. Why is there a magnet stuck to the tube and why doesn't it turn this thing into a Zeeman-split two-frequency laser (which would definitely NOT be desirable in a stabilized HeNe)?

Mode sweep:

The next step was to document the mode sweep of the orthogonal polarized modes (assuming that's what they were) from a cold start with and without the magnet in place. See Behavior of Tube Used in REO Stabilized HeNe Laser. Red is the horizontal mode and blue is the vertical mode with the 90 degree HR mirror pointing up. The time scale on all four plots is 1.0 second per box (30 boxes total in each plot).