Using Digital Micromirror Devices for focusing light through
turbid media
Sri Nivas Chandrasekaran, Hans Ligtenberg, Wiendelt Steenbergen, Ivo M. Vellekoop
Biomedical Photonic Imaging Group, MIRA Institute for Biomedical Technology and Technical
Medicine, University of Twente, P.O. Box 217, 7500 AE Enschede, Netherlands
ABSTRACT
The holy grail of biomedical optical imaging is to perform microscopy deep inside living tissue. Unfortunately,
biological tissue scatters light, which prevents the formation of a sharp focus. However, recently it was shown that
wavefront shaping can be used to focus light through and inside turbid materials. So far, most experiments used
liquid crystal devices, which are too slow to match the dynamics of perfused tissue. Since DMD technology is
approximately 1000 times faster, it may bring wavefront shaping to in-vivo applications. We will compare
analytically the performance of different methods for focusing light through scattering media with an intensity-only
light modulator.
Keywords: Keywords: DLP, DMD, Wavefront Shaping, Turbidity Suppression
1. INTRODUCTION
Optical methods for biomedical imaging can roughly be divided into two categories. Methods in the first category use
ballistic (‘unscattered’) light for imaging and/or manipulation. This category includes, a. o., conventional microscopy,
fluorescence microscopy, two photon microscopy, and optical coherence tomography. Although these methods have a
very high resolution (<ͳ ߤ), the penetration depth in biological tissue is generally limited to about one millimeter
because the ballistic component of the incident light decreases exponentially with depth. The second category is that of
methods using diffuse light, such as diffuse optical tomography. These methods generally penetrate up to ten centimeters
in tissue, at the expense of a severely compromised resolution: typically the resolution is about 1/3 of the penetration
depth
1
.
A third category of methods is currently under rapid development. These methods shape the wavefront of the incident
beam to control the propagation of light inside scattering materials
2
. Light was focused through
3
and inside
4
scattering
materials and subsequently used for high-resolution imaging
5-8
and manipulation
9
. The focus is a result of multi-path
interference of scattered waves, and it can be as sharp as the Rayleigh diffraction limit, regardless of how many times the
light was scattered
10
. The biomedical potential for wavefront shaping is enormous as it combines microscopic resolution
with macroscopic imaging depths
11, 12
.
Digital wavefront-shaping makes use of a spatial light modulator to shape the incident wave and use iterative algorithms
or phase conjugation to construct the optimal wave for focusing at a desired target. Although several analog wavefront
shaping techniques exist
13-15
, digital wavefront shaping has several advantages over conventional methods, such as the
ability to have an arbitrarily high gain in phase conjugation experiments, and the ability to freely freeze and modify the
generated wavefront, for instance to raster scan the generated focus.
The main drawback of digital methods is their relative lack of speed. The wavefront shaping system needs to be fast
enough to construct a wavefront before Brownian motion or other movement decorrelates the sample. Typically, for
perfused tissue the typical time scale is around 1 ms or less. At the moment of writing, commercially available digital
micromirror device (DMD) intensity-only light modulators achieve frame rates as high as 32kfps
16
. For iterative
wavefront shaping methods
5, 17, 18
, tens to hundreds of measurements are needed to find the optimal wavefront, so it is
important to use these measurements as efficiently as possible. Also, for digital optical phase conjugation the question
Emerging Digital Micromirror Device Based Systems and Applications VI, edited by Michael R. Douglass,
Philip S. King, Benjamin L. Lee, Proc. of SPIE Vol. 8979, 897905 · © 2014 SPIE
CCC code: 0277-786X/14/$18 · doi: 10.1117/12.2038893
Proc. of SPIE Vol. 8979 897905-1
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