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Pulsing 1550 nm Lasers for Lidar

Pulsing 1550 nm Lasers for Lidar

四月 20, 2021

Pulsed lidar systems typically use either 905 nm or 1550 nm lasers for optical emission.  Above 1400 nm, various elements of the eye absorb the light, impeding it from reaching and damaging the retina.  As laser power is increased, not all of it is absorbed, and at some point, retinal damage may occur.  Since 905 nm light does not get absorbed, it does reach the retina, so care must be used to limit the energy density to prevent damage.

If the decision is to use 1550 nm light, efficiency differences in the semiconductor laser make it necessary to use higher current for the same optical power emitted compared with 905 nm light.  Additionally, the same characteristics that allow the light to be absorbed by the eye before getting to the retina cause it to be absorbed by the atmosphere.  This phenomenon is amplified as humidity increases to fog, rain, or snow.  The drive power required for a 1550 nm laser may be up to 10 times higher than for a 905 nm laser based system.  Fortunately, there is a solution to deliver the power necessary to drive 1550 nm lasers while maintaining the edge speed and pulse required for high resolution in pulsed lidar applications.

EPC’s eGaN® FET technology has the ability to drive a wide range of pulse currents in very short times using small, inexpensive circuitry.  The range of technology is from amps to hundreds of amps, all capable of pulse widths from 1 ns to 5 ns using power devices rated from 15 V to 200 V.

Resonant discharge is typical for high power direct time of flight (DToF) where a capacitor is charged, and then the laser driver discharges it into the laser.  The resonant frequency is derived primarily from the power storage capacitance and the stray inductance as 1/(2π√LC). With CStore and LStray fixed, peak power is a function of capacitor voltage.  The image below shows the basic circuit and the basic waveforms.

DToF Basic Circuit and the Basic Waveforms

For high power while maintaining a narrow pulse width, a 160 V source can be used.  EPC2034C is a 200 V device that is capable of a peak current of over 213 A.  eGaN technology has ultra-low capacitance, and its wafer level packaging making it ideal for high speed pulsed lidar systems.  Waveforms for the EPC2034C show a peak current of 221 A with a full width at half maximum (FWHM) time of 2.9 ns.

EPC2034C Waveforms

Upcoming work expects to show a pulse of > 300 A with a FWHM of < 5 ns.  This work will use the 100 V EPC2032 off an 80 V bus.

In addition to discrete eGaN FETs being driven by silicon integrated circuit gate drivers, EPC has introduced eToF™ laser driver ICs. The first products have 40 V, 10 A capability, and are monolithically integrated using EPC’s standard eGaN process.  EPC21601 uses 3.3 V input logic, while the EPC21603 uses an LVDS receiver.  Both require a 5 V logic supply.  These laser drivers are fast, small, and cost- effective solutions to both direct time-of-flight (DToF) and indirect time-of-flight (IToF) 3D cameras.  A block diagram and an image of the bump side of the EPC21601 are shown below.  These integrated laser drivers have the power capability to bring 1550 nm lasers to IToF for short range applications.

eToF Laser Driver ICs

Results for the EPC21601 at 20 V, 10 A, using a resistive load, give a very impressive 410 ps drain fall time at turn on and 320 ps drain rise time at turn off.  Waveforms are shown below.

EPC21601 at 20 V, 10 A, Using a Resistive Load

While 1550 nm systems greatly improve eye safety, they have the fundamental challenge of requiring much more power than 905 nm systems. eGaN FETs and eToF laser drivers solve the problem of powering them.  Look for EPC’s expansion of its eTOF product line, and for special applications, ask us about a customized solution.