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Applications of Long-Wavelength Sources and
Detectors for Medical Monitoring
Jonathon T. Olesberg
Optical Science and Technology Center
and the Department of Chemistry
University of Iowa, Iowa City, IA
There are several exciting possible applications
of optical sensing for medical monitoring. Optical
monitoring of body chemistry offers several advantages
over conventional chemical techniques. Long-wavelength
semiconductor source and detector technology will likely
play a key role in making these applications possible and
practical.
There are several biochemicals for which
medical monitoring would be useful, including urea,
lactate, cholesterol, and creatinine. The best-knownpotential application of non-invasive optical monitoring,
however, is the measurement of blood glucose for
individuals with diabetes. Although the importance of
frequent blood glucose monitoring is clear, and standard
reagent-based technology for measuring blood glucose is
well developed, most individuals with diabetes do not
monitor their blood glucose values nearly as often as they
should. The primary reasons given for inadequate testing
are the pain of drawing a sample of blood and the cost of
the reagent-carrying test strip. Optical measurements can
do away with both of these factors, allowing the
measurement to be performed non-invasively and
reagentlessly.
Although development of optical blood glucose
sensors has been pursued aggressively for several years,
there are still no commercially available instruments. This
is due to a combination of factors, including an extremely
high signal-to-noise requirement and the difficulty of
properly interpreting spectral absorption information. The
factors required for successful noninvasive biochemical
monitoring, especially as they relate to the potential
impact of the development of semiconductor source and
detector technology in the 2.0-10 m wavelength range,
will be discussed.
Biomolecule absorption in the infrared is due to
interaction of the optical field with vibrational modes of
the molecule. In this regard, infrared optical sensing is
much more difficult than the measurement of hemoglobin
oxygenation in pulse oxymetry, which utilizes electronic
transitions in the hemoglobin molecule. The most intense
vibrational interactions are due to bonds involving
hydrogen atoms, such as, O-H, C-H, and N-H bonds.
Fundamental vibrational modes exist in the 4-10 m
wavelength range. Weaker nonlinear combinations of
fundamental modes exist in the 2.0-2.5 m wavelength
range, and yet weaker overtones exist in the 1.5-1.8 m
and 0.8-1.2 m ranges.
Any measurement in a biological material must
deal with the presence of water. Water has significant
absorption throughout the long-wavelength infrared,
requiring the selection of wavelength bands lying in water
absorption windows. The dominant water transmission
windows in the long-wavelength infrared occur between
2.0-2.5 m, 3.3-5.9 m, and 6.2-11 m.
Much of the work in noninvasive sensing has
utilized the shorter wavelength regions (0.8-1.8 m
wavelength) because of the greater penetration depth of
water and the abundance of well-developed source and
detector technology. However, the optical interaction
strength with glucose is very weak in these ranges. Thefield of biochemical sensing will be greatly aided by
advances in device technology in the 2.0-2.5 m and
3-10 m wavelength ranges.
The requirements for biomolecule sensing in
aqueous environments are very different from gas
sensing, where absorption lines are narrow. In an aqueous
environment, absorption features are broad and highly
overlapped. Fortunately, though, the exact structure of the
absorption bands depends on the chemical environment
surrounding the active bonds. Because of this, the
absorption spectrum of each chemical species is unique.
But absorption measurements must be made at several
wavelengths in order to provide enough degrees of
freedom to identify glucose in the presence of other
interfering compounds.
Much of the present non-invasive chemical
sensing research is performed using broad-band optical
sources (e.g., tungsten lamps or glow-bars) and FTIR
spectrometers. Spectral quality is typically limited by
detector noise due to the small optical powers provided by
broad-band sources. In addition, tissue throughput is
small due to water absorption and tissue scattering: peak
transmission in the 2.0-2.5 m wavelength range is
significantly less than 1% per millimeter of tissue.
Tunable laser sources or arrays of laser diodes caneliminate the low signal limitation, even with modest
powers (e.g., 10 mW). Unlike gas sensing applications,
narrow linewidth is not important, but wavelength
stability (for lasers in an array) or wavelength
reproducibility (for a tunable system) is critical.
Successful noninvasive measurements will likely require
very large (>105) signal-to-noise-ratios, so wavelength
deviations must be very small.
Abs. 283, 205th Meeting, 2004 The Electrochemical Society, Inc.