Detecting Leaks from Carbon Sequestration Using LIBS and Raman Spectroscopy
Dustin McIntyre, of the National Energy Technology Laboratory, US Department of Energy in Morgantown, West Virginia, has been
exploring the use of laser-induced breakdown spectroscopy (LIBS) to measure subsurface gases, liquids, and solids at subsurface
conditions. He recently shared with Spectroscopy a look at some of the work he's been doing and his thoughts on ways in which his technique can be used.
What sparked your idea for an improved LIBS elemental composition detection system?
In my graduate work, I focused on using a miniaturized diode pumped solid-state passively Q-switched laser as an engine ignition
system. While discussing laser spark plug technology with a colleague, we realized that we could use a similar concept to
place a miniaturized laser below ground to produce a LIBS spark for atomic chemical analysis. We also realized that we could
easily adapt the laser for Raman analysis to run molecular chemical analysis as well. My current area of research is carbon
capture, utilization, and storage (CCUS), in which CO2 is captured from an electric power plant, compressed, and subsequently injected underground for permanent storage. The questions
we are investigating are related to storage permanence and how to ensure that, once injected, CO2 will remain in its intended location underground. This new LIBS system will enable monitoring of downhole fluids to detect
any chemistry changes that would be characteristic of undesirable CO2 migration.
What is innovative about your approach and how does it differ from currently used methods? What are its advantages?
Our system uses a remotely diode pumped solid state passively Q-switched laser to produce output for Raman and LIBS analysis.
Other systems designed to provide these types of measurements rely on an above-ground, laboratory-scale laser to deliver either
Raman excitation energy or the high peak energy LIBS pulse through optical fibers to the subsurface. Delivering the LIBS high
peak energy can easily destroy the fiber and complicate refocusing of the laser beam. Using Raman in a long optical fiber
can significantly interfere with the stimulated response primarily due to the Raman response of the optical fiber material
itself. Our system uses a remotely positioned laser diode that is coupled to an optical fiber where the peak power is only
a few hundred watts instead of megawatts. The light from the diode travels through the optical fiber where it is then focused
into a monolithic laser gain medium to form an end-pumped laser system. The passively Q-switched laser, once properly excited
by the fiber-delivered light, produces a high peak power pulse that is directed and focused at the location of interest. The
light from the spark is then collected and either transferred back up the fiber for analysis by a laboratory-scale spectrometer
or simply directed into a miniaturized narrow-band gated spectrometer that is situated alongside the solid-state laser.
For the full interview, go to: