The only
moving part in a modern laser shutter is a low-mass, flexible, ferromagnetic
cantilever membrane that is moved in and out of the beam by an electromagnet.
DAVID C. WOODRUFF
High-irradiance
lasers can be found in a vast range of applications from semiconductor
fabrication to the laser-guide-star adaptive-optics system at the Keck
Observatory (Mauna Kea, HI). These lasers are extremely versatile tools, but
they are potentially dangerous. In all cases a highly reliable means of beam
termination must be available. In the case of semiconductor fabrication, the
beam must be shut down immediately if there is a safety breach of the system.
In the case of the observatory, the beam must be shut down, for instance, if an
aircraft approaches. The shutdown function is generally performed using a laser
shutter.
When the
shutter is open, the beam travels through undisturbed. Closure completely
blocks the beam (see Fig. 1). During closure, the energy of the beam is
diverted into an integral light-absorbing baffle that can, in some units,
heat-sink beams in laser safety shutter the kilowatt range
indefinitely. There is thus no need to power down the laser. The beam is
modified only during the switching transitions that typically last hundreds of
microseconds.
Laser-shutter
applications are not limited to switching high-irradiance laser beams, they are
also used to pass low-level light and even to block flying debris. For example,
in lidar systems, shutters are used to block the receivers to protect
photosensors from being overdriven by the initial backscatter of the outgoing
laser pulse. After the initial pulse, the shutter quickly opens to catch the
low-level returning light. Such shutters are used when researching x-ray
spectra from pulsed laser targets. The shutter closes fast enough to prevent
debris from the exploding target from reaching the x-ray spectrometer. Modern
shutter technology can deliver bursts of laser energy at rates as fast as 500
Hz, with periods as short as a millisecond. The duration of such bursts is also
highly reproducible. laser beam shutter
Beyond solenoids
Early laser
shutters used solenoids. Typically, a rotary solenoid and spring were provided
to rotate an aperture in a metal plate through the laser beam. Lubricated
bearings were provided to keep the friction low. To minimize vibration and the
size of the solenoid, the inertia had to be kept low. This meant that the metal
plate had to be thin, which lessened the plate's ability to sink heat. Heat was
thus conducted to the bearings and increased the outgassing of wet lubricants,
which became gummed with foreign particles. Dry lubricants could not be used
because they contributed to particle debris. Even with low-inertia systems,
vibration introduced by the acceleration and deceleration of the solenoid at
the end of its stroke was considerable. At best, such shutters had life spans
on the order of 100,000 to a million cycles.
Modern laser
shutters have no bearings and require no lubricant. The only moving part is a
low-mass, flexure mirror assembly consisting of a flexible, ferromagnetic
cantilever membrane that is moved in and out of the beam by an electromagnet.
When this assembly is in the laser-beam path, a mirror in the flexure diverts
almost all of the laser energy into an integral light-baffle heat sink
Geometry,
surface morphology, and the atomic material of the light baffle guarantees that
most of the radiant energy is absorbed and passed to the heat sink. Conduction
cooling is achieved through mechanical mounting to a large mass. Some
high-energy lasers require a water-cooled heat sink, such as a
water-circulating "chiller plate" that can easily be attached to the
heat-sink mass.
To make the
shutter fail-safe (shut down when power fails) the highly reliable
cantilever-flexure closes when power is removed from the electromagnet. In some
units, switching is accomplished in less than 200 µs and any bounce of the
flexure is designed well out of the beam area, ensuring complete on-and-off
operation. The fail-safe flexure mechanism can be interlocked with the rest of
the system, such that any faulty device creates an open loop, ultimately
dropping the voltage to the controller input. optical beam shutter
Modern
shutter designs are also scalable. Shutters with larger apertures have longer
switching periods, which vary with mass. Attachment of dielectric optics can
increase the power handling but slow the acceleration. Typically, the flexure
passes through the beam at about 2 mm/millisecond, but it can reach speeds of 6
mm/ms (6 m/s).
An
aluminum-coated mirror on the flexure surface is often sufficient to divert the
energy of a wide range of laser beams with various wavelengths. Gold mirrors
are an option for infrared beams. Dielectric mirrors on attached glass
substrates are provided for high-energy lasers at specific wavelengths. The
mirrors are designed to maximize reflectivity when the flexure is closed,
providing a high damage threshold. For metal mirrors, an arrow marked on the
shutter's input aperture indicates the direction of the beam's electric vector,
facilitating proper alignment with the laser. The flexures are designed to move
rapidly in response to the switching force of the magnetic field, to conform in
shape and provide an intimate fit with the surfaces of the electromagnet poles
at the beam exit, and to be rigid enough to present an essentially flat surface
to the beam.
Electromagnets
are wet-wound in epoxy resins that ensure outgassing levels low enough to
surpass NASA outgassing standards. Gapped toroidal shapes and closed-path
couplings minimize flux leakage. A thin sheet of steel is usually more than
adequate to isolate even the most magnetically sensitive devices such as
faraday rotators.
The catenary
shape of the electromagnetic poles assures equal force on the flexure mirror
assembly when accelerating. Since forces are distributed equally across the
flexure, contact with the pole is nearly simultaneous everywhere, with minimum
pressure points. Equal distribution of the force also ensures intimate contact
of the flexure with a pole at the end of travel. laser safety interlock
Heat
management of the magnet is accomplished by using thermal-conducting epoxy and
a metal path to the base plate of the shutter (see Fig. 3). After the flexure
reaches the pole, the controller delivers only a small holding current. Keeping
the magnet cool ensures that the resistance of the coil doesn't change,
enabling the current and switching times to remain constant. Heat management of
the magnet also greatly reduces thermal air gradients introduced into the
beam's path.
Controllers
drive the magnet. A simple capacitor discharge controller is adequate for
simple shutters, and offers advantages as a result of having few parts,
including low cost, high reliability, and a very long mean time between
failures. The capacitor discharge controller can easily be constructed by the
OEM as an integral part of the product.
More-sophisticated
controllers deliver a sculptured, voltage-regulated waveform to drive faster
shutters. This waveform is designed to rapidly accelerate the flexure and bring
it to rest with sufficient holding current. Slight overdamping of such systems
eliminates ring and reduces bounce for high-speed closure. Close proximity to
critical damping also minimizes energy transferred to the magnet, further
enhances heat management, and greatly reduces mechanical shock and vibration.
Visit www.nmlaser.com to find more about us.
What is the
future of electromechanical laser shutters? As lasers get bigger and better
they can only place greater demand on shutters. Engineers at nmLaser are
developing a shutter with a noncontact flexure designed to close at a position
slightly away from the pole, essentially floating in air to eliminate any
potential vibration or bounce caused by rapid deceleration of even the low-mass
flexure. Slightly overdamped controllers will eliminate system ring, ensuring
efficient energy transfer to the magnet. Such flexures will be unaffected by
foreign particles clinging to the magnetic pole. They will also be suitable for
use in clean rooms and offer much longer lifetimes than is currently available.
DAVID C.
WOODRUFF is the president of nmLaser Products, 337 Piercy Road, San Jose, CA
95138;
e-mail: dave@nmlaser.com ; www.nmlaser.com.
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