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PROCEEDINGS OF SPIE

SPIEDigitalLibrary.org/conference-proceedings-of-spie

Multimodal tissue perfusion imaging

using multi-spectral and

thermographic imaging systems

applied on clinical data

John H. G. M. Klaessens, Martin Nelisse, Rudolf M.

Verdaasdonk, Herke Jan Noordmans

John H. G. M. Klaessens, Martin Nelisse, Rudolf M. Verdaasdonk, Herke Jan

Noordmans, "Multimodal tissue perfusion imaging using multi-spectral and

thermographic imaging systems applied on clinical data," Proc. SPIE 8574,

Multimodal Biomedical Imaging VIII, 85740F (13 March 2013); doi:

10.1117/12.2003823

Event: SPIE BiOS, 2013, San Francisco, California, United States

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Multimodal tissue perfusion imaging using multi-spectral and

thermographic imaging systems, applied on clinical data

John H.G.M. Klaessens

*

, Martin Nelisse

*

, Rudolf M. Verdaasdonk

+

, Herke Jan Noordmans

* *

Department of Medical Technology & Clinical Physics, University Medical Center Utrecht, Utrecht,

The Netherlands.

+

Department Physics and Medical Technology, Free University Medical Center, Amsterdam, The

Netherlands

ABSTRACT

Clinical interventions can cause changes in tissue perfusion, oxygenation or temperature. Real-time imaging of these phenomena could be useful for surgical strategy or understanding of physiological regulation mechanisms. Two non-contact imaging techniques were applied for imaging of large tissue areas: LED based multispectral imaging (MSI, 17 different wavelengths 370 nm-880 nm) and thermal imaging (7.5 to 13.5 μm). Oxygenation concentration changes were calculated using different analyzing methods. The advantages of these methods are presented for stationary and dynamic applications. Concentration calculations of chromophores in tissue require right choices of wavelengths The effects of different wavelength choices for hemoglobin concentration calculations were studied in laboratory conditions and consequently applied in clinical studies. Corrections for interferences during the clinical registrations (ambient light fluctuations, tissue movements) were performed. The wavelength dependency of the algorithms were studied and wavelength sets with the best results will be presented. The multispectral and thermal imaging systems were applied during clinical intervention studies: reperfusion of tissue flap transplantation (ENT), effectiveness of local anesthetic block and during open brain surgery in patients with epileptic seizures. The LED multispectral imaging system successfully imaged the perfusion and oxygenation changes during clinical interventions. The thermal images show local heat distributions over tissue areas as a result of changes in tissue perfusion. Multispectral imaging and thermal imaging provide complementary information and are promising techniques for real-time diagnostics of physiological processes in medicine.

Keywords: Multi-spectral, Near Infrared, Hemoglobin, Oxygen, Thermography Algorithms.

1. INTRODUCTION

For many clinical applications wide field functional information from the tissue would give the surgeon direct feedback of the tissue response to the intervention. Reflectance multi-spectral imaging is a non-invasive method for tissue imaging, which can provide functional information over a wide field of view and, when using near infrared light, can penetrate millimeters deep into the tissue. Near infrared (NIR) light has already been used for over 3 decades to study regional blood and tissue oxygenation changes in animal studies, clinical intervention studies for oxygen supply and consumption in the brain and muscles 1-5. In these studies, point measurements were performed using fiber systems, they acquired regional tissue information from deeper tissue layer. In this paper functional imaging of large surface areas will be described.. The theory to calculate tissue oxygenation changes is adapted from these applications. Diffuse optical reflectance imaging using a CMOS camera is an attractive method for monitoring hemodynamic and metabolic changes in superficial tissue layers like skin, muscle or brain (open skull) over a larger area6. An IR thermal camera is used for

measuring absolute surface temperatures. Both these techniques can be used to study localized differences in tissue characteristics and dynamic changes in the tissue (e.g. perfusion, oxygenation and temperature changes).

A LED multi-spectral imaging system has been developed and has been validated under laboratory conditions imaging the skin during arm clamping. The results from this validation study will be described in this proceeding. Algorithms are

Multimodal Biomedical Imaging VIII, edited by Fred S. Azar, Xavier Intes, Proc. of SPIE Vol. 8574, 85740F · © 2013 SPIE · CCC code: 1605-7422/13/$18 · doi: 10.1117/12.2003823

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LED on Illlllllllllllllllllllllllllllllllllllllla\\\\\\\\\\\\\ Camaaoutpot Imageaquisitiw Softwmerull 1000µs ntegeotiontime 1000µs Integration time

being developed7 to calculate oxygenation changes in the superficial skin or tissue layer (~1 mm depth). The influence of

the wavelength choices are studied and will be discussed. With the results from laboratory experiments, the imaging methods were applied in clinical studies, and the first results will be presented.

2. MATERIAL AND METHODS

The LED multispectral imaging system was developed and tested during laboratory experiments to validate the correct functioning of the total system. To explore the effects of different wavelengths on the oxygenation calculations a number of sequences of wavelengths were applied during a standardized arm clamping experiment. The effect of the arm clamping on oxygenation changes are well known: during clamping the oxy hemoglobin will decrease and the deoxyhemoglobin will increase, after opening of the clamp the oxy- and deoxy-hemoglobin will return to the starting levels (sometimes first with a small overshoot). The results form the oxy and deoxy calculations have to agree with this.

2.1 Imaging systems

A tunable VIS-NIR LED light source (370nm – 880 nm) has been developed consisting of a 2-D flat panel with a total of 600 LEDs, consisting of 17 different wavelengths, a CMOS camera is mounted in the middle of the panel (figure 1)8.

Figure 1. The tunable LED light source for the multi-spectral imaging system. On the right the scheme of controlling the

switching of the LEDs and the integration time of the camera.

The LED controllers are tuned that all the wavelengths give the same intensity and the LEDs are arranged over the panel to achieve a homogeneous light distribution over the object. The camera is synchronized with the flashing sequence of the LEDs. The software controls which LEDs will be turned on and for how long. Because the camera triggers the LED controller, a software call from the main application will give an output trigger for the camera that will turn on the specified LEDs; a second software from the main application call will start the integration of the camera for a specified time. This guaranties that the collected light is always in the stable period of the LEDs and that only the intended LED light is collected (no overlap with other wavelengths).

Simultaneously with the multispectral imaging the thermal camera is used. Thermography was performed with a calibrated IR thermal camera (FLIR ThermoCam SC640, Seattle, USA), uncooled micro-bolometer with a 640x480 pixel array.

2.2 Arm clamp experiment

The measuring systems and analyzing methods were tested under ideal conditions, dark environment and no movements. The temperature and oxygenation changes were induced during arm clamping experiments on volunteers (Figure 2). The arm is clamped using a blood pressure cuff attached to the upper arm. A pressure of 240 mmHg was applied for 5 minutes to block all the blood flow to the arm. Images at the normoxic, hypoxic and reperfusion stage with the two systems are collected and analyzed.

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8 Bit

CMOS camera LED Light panel

Diffusor

Iirl1111

11111111

LED controller

Cuff

=

t= 0 t= 2 t= 7

Time schedule of arm clamp experiment

t= 12 minutes

Figure 2. The experimental setup of the arm clamp measurement: the LED illumination around the CMOS camera and the thermal camera next to it. Below the time scheme of the clamp experiment is shown.

A selected set of LEDs flash sequentially, the light is diffused homogeneously over the object (hand) and the backscattered light from the tissue is received by the CMOS camera. The time schedule of the clamping is 2 minutes normoxic skin, 5 minutes clamping with total occlusion, and 5 minutes registration after reperfusion. The thermal data were collected with a temperature resolution of 0.1 degree Kelvin acquired at a 1 second interval.

Physiological response to arterial and venous occlusion is: The blood flow stops and total hemoglobin (tHb) will remain constant, deoxygenated hemoglobin (HHb) will increase and oxygenated hemoglobin (O2Hb) will decrease, the

temperature of the hand will decrease. The reperfusion will do the opposite: increase in O2Hb and decrease of HHb and

because of hyper-perfusion increase in tHb, and the temperature will increase.

3. THEORY

3.1 Algorithm for tissue oxygenation calculation

The theory has been described before9 and is based on the modified Lambert-Beer law. The backscattered light was

analyzed by calculating the O2Hb and HHb concentration changes. Three different algorithms were applied: delta time

method (dt or Δt), the delta wavelength method (dl or Δλ) and the Fit method (FIT). In short these methods are described. The attenuation of light in tissue can be comprised in the modified Lambert-Beer law10 (MLBL):

( ) ( ) ( ) ( ) ( ) ( )

Aλ ε λ= c t DPF λ d G+ λ +H t (3-1) With A( )λ the measured absorbance [-], ε λ( )the molar extinction coefficients [mM-1cm-1], c(t) the concentration of

molecules [mM], G( )λ the oxygen independent and wavelength dependent losses [-], H t( )are the oxygen independent and time dependent losses [-], d is the source detector distance [cm], DPF( )λ is the differential path length factor [-]. DPF(λ) is the differential path-length factor, which corrects the geometrical source-detector distance to the mean optical path in the tissue. G(λ) and H(t) are the oxygen independent loss caused by scattering, absorption, geometry and other boundary losses1,11.

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Equation 3-1 can be written out for multiple wavelengths to calculate the concentration of chromophores in the skin (example with 3 wavelengths):

( )

2 2 2 2 1 1 1 1 1 1 2 2 2 2 2 2 3 3 3 3 3 3 ( ) ( ) ( ) ( ) ( , ) ( ) ( ) ( ) ( ) ( ) ( ) ( , ) ( ) ( ) ( ) ( ) ( ) ( ) ( ) ( ) ( , ) ( ) O Hb HHb O Hb O Hb HHb HHb O Hb HHb DPF DPF G A t H t c t DPF DPF A t d G H t c t H t DPF DPF A t G ε λ λ ε λ λ λ λ ε λ λ ε λ λ λ λ ε λ λ ε λ λ λ λ ⎡ ⎤ ⎡ ⎤ ⎡ ⎤ ⎢ ⎥ ⎢ ⎥ ⎢ ⎥ ⎡ ⎤ = + ⎢ ⎥ + ⎢ ⎥ ⎢ ⎥ ⎢ ⎥ ⎢ ⎥ ⎣ ⎦ ⎢ ⎥ ⎢ ⎥ ⎢ ⎥ ⎣ ⎦ ⎣ ⎦ ⎣ ⎦ ⎤ ⎥ ⎥ ⎢ ⎥⎦ (3.2)

Two different methods can be applied to calculate the concentration changes; the classical Δt-method and the Δλ-method7.

Delta time method (∆t) solves the Lambert Beer equation by taking differences in time relative to a steady base level to remove the unknown constant in the equation. Delta wavelength method (∆λ) uses differences between the wavelengths to remove the unknown constant in the Lambert Beer equation, this is done instantaneously. The delta FIT method uses the pseudo inverse method Moore-Penrose to match the found spectra with the literature reflection spectra and is a generalization of the delta wavelength method. This method can be used with more than three wavelength.

The collected multi spectral images of the skin surface can be converted to the reflectance spectrum by correcting them for spatially non uniform light distribution and the camera dark current:

Ref ( , ) ( ) ( , ) ( , ) ( ) S t D R t W t D λ λ λ λ λ − = − (3-3)

With S(λ) the measured light CCD camera, D(λ) the dark current signal and Wref(λ) the reference of 100% reflectance of

a white standard.

4. LIGHT SEQUENCE AND AMBIENT LIGHT CORRECTION

In the (pre-) operation room the ambient light is not constant in intensity (movement of surgeons, head lightening, changing in room lightning), it is not always possible to dim the light in the room. These fluctuations in ambient light will be superimposed on each of the collected wavelength images of the multispectral imaging data cube. To calculate the oxygenation changes in tissue the tunable LED light source will flash sequentially 3 or more wavelengths. In the validation experiments 7 wavelengths were selected in the visible and near infrared region, based on the absorption spectra of oxy and deoxy-hemoglobin. We selected the sequence: 470, 525, 625, 690. 750, 810 and 850nm. These wavelengths were repeatedly flashed during the period of the experiment (12 minutes). The time between the wavelengths was 10 milliseconds and the time between the sequences was set to 800ms this resulted in one sequence of images per second. To correct for the fluctuations in the ambient light an extra image was acquired during each sequence with the LED lights turned off. This acquired image was real-time subtracted from the other wavelength images in that sequence. The intensity of the LED’s were optimized such that the 8-bit CMOS sensor did not saturate.

5. RESULTS

5.1 Laboratory arm clamp experiment

The results of one example of the arm clamp experiment are shown in figure 3. A clear response in temperature is seen in the thermal images and in the oxygenation images, in the ROI the temperature and oxygenation changes clearly describe the response of the clamping experiment.

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1K lhexmogsaphy images Skin hemoglobin

38 C concentration changes in both hands

1125

I7

411IIb AO2Hb x 26 C

-

Ring finger (L) Little finger (L) - Ring finger (R) - Little finger (R) Ring finger (R) AO2Hb 0 1 2 3

4 5

6 7 8 9 10 11 Time [minute] dA 1 2 3 4 5 6 7 470 525 X X X 625 690 X X X X X 750 X X X X X 810 X X X 850 X X X X X

PRIa©ae©saa

470 690 750 810 850 X X X X X X X X X X X x x x x x x x x X X - - X X X -X X X X X X X X

Figure 3, a total occlusion is performed on the right arm, on the left the thermal images, in the middle the oxygenation

(O2Hb and HHb) changes and on the right the graphs of the temperature changes and the oxygenation changes, in a

region of interest (finger tip right hand) are presented.

5.2 Effects of wavelength choices on the oxygenation algorithms

The concentration algorithms (∆t, ∆λ and FIT method) were tested for 7 or 8 different wavelength combinations (table 1). For all the arm clamping registrations by volunteers the concentration changes were calculated.

Table 1. The wavelengths selection for the three different concentration algorithms.

To qualify which wavelengths are most optimal for performing oxygenation experiments all the calculated concentration changes (for all volunteers, for all methods and for all wavelengths sets) were scored (2 correct, 1 partially correct and 0 wrong). This was also done for the signal to noise level ratios (2 low noise levels, 1 some noise and 0 large noise levels). The results are presented in table 2.

The concentration algorithms give for all three methods good results when using the following wavelengths: ∆t method

with 525nm, 625nm, 750nm and 850nm, or 525nm, 690nm, 750nm 810nm and 850nm ,∆λ method with 525nm, 690nm and 750nm or 525nm, 690nm and 850nm, FIT method 525nm, 750nm and 850nm. These result are applied

in clinical trials and the first results are presented.

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e ' Method

∆t

FIT

∆λ

Wavelength set Si gn al Noise Sign al Noise Sign al Noise

1

6

1

3

0

3

0

2

2

6

3

0

0

0

3

6

6

6

0

3

0

4

6

5

6

6

2

0

5

6

3

6

0

6

5

6

6

6

6

1

6

6

7

3

5

0

0

6

6

8

4

3

1

0

Table 2. The quality of the methods using different wavelength sets. The higher the value the better the correctness of

the signal and the signal to noise ratios are. The green combinations give good results.

5.3 ENT radial lower arm flap transplantation

Harvesting and the reperfusion of a skin graft are the critical moments during transplantation surgery. Multi-spectral imaging was used during surgery to confirm the full reperfusion of the donor and graft area before and after transplantation. This to have an early warning of ischemic areas in the flap.

Figure 4, Oxygenation of the harvested flap. Blue represent low and red high oxy-hemoglobin concentration. The top

line shows the ∆t and the 2e line shows the ∆λ method.

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29.5 F 27.5 25.5 1 2 3 Time [minutes]

t=Ommutes t=2.5 minutes r 4 minutes

32 c 28 c 26c 6 A02 HB

-

DEQB

Figure 5, Thermal images of the flap during reperfusion after harvesting on the arm. Note that the flap is clearly cooler (blue in circle).

5.4 Local anesthetic block of arm

To perform local surgery on the extremities, a nerve block may be used to anesthetize the limbs. A nerve block functions by anesthetizing the sensory and motor nerve of the extremity. A block will give vasodilatation of the blood vessels resulting in temperature rise and increase of blood content in the hand.

Figure 6, thermal images of the hand in at the start of the block and at 6 and 12 minutes after the start. In the bottom

row, the oxygenation and temperature changes are given in regions of interest on the hand.

5.5 Open brain surgery in patients with epileptic seizures

During brain surgery the cortex of an epilepsy patient with recurring seizures was imaged with the multi -spectral camera. Intracranial EEG examination located the epileptic center in the sensory cortex. During seizures an increase in oxygenated and total blood volume in the same area of the sensory cortex could be observed in the calculated hemoglobin images. Multispectral oxygenation imaging opens prospects of intra operative function localization.

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6. CONCLUSIONS

The results of the validation study of the LED based multi-spectral imaging system prove that this system can measure the perfusion and oxygenation changes caused by physiological changes in the tissue during arm clamping and the thermal camera can measure the absolute temperature changes of the skin. Both measurements have a good correlation with each other and can be used as complementairy information in clinical situations. The concentration algorithms give for all three methods good results, the methods are wavelength sensitive, for each method sets of wavelengths are selected which give correct results with a good signal to noise ratio. During clinical studies precautions have to be taken to avoid disturbances by movement of the patient and ambient light fluctuations in the operation room. Our laboratory and the first clinical studies show that thermography and multi-spectral imaging prove to be promising techniques for real-time diagnostics of dynamic physiological processes in medicine.

REFERENCES

[1] Delpy, D. T. and Cope, M., "Quantification in tissue near-infrared spectroscopy",

Philosophical Transactions of the Royal Society B-Biological Sciences352, 649-659 (1997).

[2] Ferrari, M., Mottola, L., and Quaresima, V., "Principles, techniques, and limitations of near

infrared spectroscopy", Can.J.Appl.Physiol29, 463-487 (2004).

[3] Jobsis, F. F., "Noninvasive, infrared monitoring of cerebral and myocardial oxygen

sufficiency and circulatory parameters", Science198, 1264-1267 (1977).

[4] Klaessens, J. H., Hopman, J. C., Liem, K. D., van Os, S. H., and Thijssen, J. M., "Effects of

skin on bias and reproducibility of near-infrared spectroscopy measurement of cerebral

oxygenation changes in porcine brain", J.Biomed.Opt.10, 44003 (2005).

[5] Madsen, P. L. and Secher, N. H., "Near-infrared oximetry of the brain", Prog.Neurobiol.58,

541-560 (1999).

[6] Kawauchi, S., Nishidate, I., Uozumi, Y., Nawashiro, H., Ashida, H., and Sato, S., "Diffuse

light reflectance signals as potential indicators of loss of viability in brain tissue due to

hypoxia: charge-coupled-device-based imaging and fiber-based measurement",

J.Biomed.Opt.18, 15003 (2013).

[7] Klaessens, J. H. G. M., Noordmans, H. J., de Roode, R., and Verdaasdonk, R. M.,

"Non-invasive skin oxygenation imaging using a multi-spectral camera system: effectiveness of

various concentration algorithms applied on human skin", SPIE Vol: 7174 (2009).

[8] Klaessens, J. H. G. M., de Roode, R., Verdaasdonk, R. M., and Noordmans, H. J.,

"Hyperspectral imaging system for imaging O

2

Hb and HHb concentration changes in tissue

for various clinical applications ", Advanced Biomedical and Clinical Diagnostic Systems

IX,SPIE Proceedings Vol. 7890 (2011).

[9] Klaessens, J. H. G. M., Landman, M., de Roode, R., Noordmans, H. J., and Verdaasdonk, R.

M., "Thermographic and oxygenation imaging system for non-contact skin measurements to

determine the effects of regional block anesthesia", SPIE7548G-157, Session 3 (2010).

[10] Delpy, D. T., Cope, M., van der Zee, P., Arridge, S., Wray, S., and Wyatt, J., "Estimation of

optical pathlength through tissue from direct time of flight measurement",

.Phys.Med.Biol.33, 1433-1442 (1988).

[11] Edwards, A. D., Richardson, C., van der, Z. P., Elwell, C., Wyatt, J. S., Cope, M., Delpy, D.

T., and Reynolds, E. O., "Measurement of hemoglobin flow and blood flow by near-infrared

spectroscopy", J.Appl.Physiol75, 1884-1889 (1993).

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