E. Duco Jansen, Martin Frenz, Kamuran A Kadipasaoglu, T

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Laser–Tissue Interaction During Transmyocardial Laser Revascularization  E.Duco Jansen, Martin Frenz, Kamuran A Kadipasaoglu, T.Joshua Pfefer, Hans J Altermatt, Massoud Motamedi, Ashley J Welch  The Annals of Thoracic Surgery  Volume 63, Issue 3, Pages 640-647 (March 1997) DOI: 10.1016/S0003-4975(96)01143-5 Copyright © 1997 The Society of Thoracic Surgeons Terms and Conditions

Fig. 1 Chronology of the events associated with continuous-wave laser ablation of soft tissue. The Annals of Thoracic Surgery 1997 63, 640-647DOI: (10.1016/S0003-4975(96)01143-5) Copyright © 1997 The Society of Thoracic Surgeons Terms and Conditions

Fig. 2 The experimental setup used to take the time-resolved, fast flash images of the ablation-associated events in a transparent medium (water or tissue phantom gels). For tissue burn-through studies, the helium-neon (HeNe) aiming beam, which is coaligned with the CO2 beam, is detected by a photodetector (PD) underneath the water bath. As the channel is formed, the remaining thickness of the tissue decreases and thus the transmitted He-Ne signal increases. (BS = beam splitter; CCD = charge-coupled device [video camera]; ECG = electrocardiographic; VCR = video cassette recorder.) The Annals of Thoracic Surgery 1997 63, 640-647DOI: (10.1016/S0003-4975(96)01143-5) Copyright © 1997 The Society of Thoracic Surgeons Terms and Conditions

Fig. 3 Sequence of images taken during the irradiation of water with the 800-W CO2 laser. Pulse duration was 10 ms (8 J), and the spot size at the surface was 1 mm in diameter. The delay times with respect to the start of the laser pulse are shown in the lower righthand corner. The scale in the images is a millimeter scale. The Annals of Thoracic Surgery 1997 63, 640-647DOI: (10.1016/S0003-4975(96)01143-5) Copyright © 1997 The Society of Thoracic Surgeons Terms and Conditions

Fig. 4 Length of the vapor channel in water as a function of time. The measurements were taken from images like those in Fig. 3. Pulse durations were 10, 30, 50, and 70 ms, but no differences in channel length at any time were seen for the different pulse durations. Shown are the average channel length and standard deviation (n = 20). The line represents a logarithmic fit to the data (r = 0.98). The Annals of Thoracic Surgery 1997 63, 640-647DOI: (10.1016/S0003-4975(96)01143-5) Copyright © 1997 The Society of Thoracic Surgeons Terms and Conditions

Fig. 5 Hydrophone trace measured during a 40-ms CO2 laser pulse in water. The CO2 laser pulse is indicated by the horizontal line. The hydrophone was positioned with the tip 12 mm in the water and 3 mm away from the center of the laser beam. The signal was amplified 200 times, causing it to be quite noisy. However, it can be seen that pressure transients occurred during the laser pulse. The maximum absolute pressure at the sensor corresponded to 0.12 bar. (AU = arbitrary units.) The Annals of Thoracic Surgery 1997 63, 640-647DOI: (10.1016/S0003-4975(96)01143-5) Copyright © 1997 The Society of Thoracic Surgeons Terms and Conditions

Fig. 6 The trace of the photodiode-collecting helium-neon laser light at the bottom of a tissue slab (porcine myocardium) with a thickness of 20.5 mm (A). Also shown is the trace from the 40-ms CO2 laser pulse (B). The CO2 laser was coaligned with the helium-neon laser (aiming beam) and ablated the tissue, causing an increase in helium-neon light transmission. The time to penetration was 17.5 ms. (AU = arbitrary units.) The Annals of Thoracic Surgery 1997 63, 640-647DOI: (10.1016/S0003-4975(96)01143-5) Copyright © 1997 The Society of Thoracic Surgeons Terms and Conditions

Fig. 7 Tissue thickness (porcine myocardium) as a function of the time needed to ablate a channel all the way through the tissue. The burn-through time was determined from the helium-neon traces shown in Fig. 6. Also shown is the fitted curve of the channel depth versus time in water from Fig. 4. The Annals of Thoracic Surgery 1997 63, 640-647DOI: (10.1016/S0003-4975(96)01143-5) Copyright © 1997 The Society of Thoracic Surgeons Terms and Conditions

Fig. 8 Time-resolved photographs of the bottom of a 10-mm-thick slab of porcine myocardium in water. The dark areas on the top are the bottom of the tissue (silhouette). The images on the left are control pictures taken before the laser pulse. The images on the right were obtained just after total tissue penetration was achieved at 7 ms after the start of the 40-ms laser pulse (top) and 20 ms after total tissue penetration (ie, 27 ms after the start of the 40-ms laser pulse) (bottom). The scale represents a millimeter scale. The Annals of Thoracic Surgery 1997 63, 640-647DOI: (10.1016/S0003-4975(96)01143-5) Copyright © 1997 The Society of Thoracic Surgeons Terms and Conditions

Fig. 9 Histologic cross-sections of porcine myocardium irradiated in vitro with an 800-W CO2 laser. The tissue was irradiated from the epicardial side, and the sections were taken close to the surface. (a, b) Pulse duration of 50 ms (40 J). (c, d) pulse duration of 10 ms (8 J). a and c are the standard light microscopic images and b and d are the birefringence images. The Annals of Thoracic Surgery 1997 63, 640-647DOI: (10.1016/S0003-4975(96)01143-5) Copyright © 1997 The Society of Thoracic Surgeons Terms and Conditions