tm:yag laser
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2021 ◽  
pp. 103942
Author(s):  
Linjun Li ◽  
Tianqi Qi ◽  
Wenqiang Xie ◽  
Xining Yang ◽  
Long Zhou ◽  
...  

Author(s):  
Simon Hein ◽  
Ralf Petzold ◽  
Rodrigo Suarez-Ibarrola ◽  
Martin Schoenthaler ◽  
Christian Gratzke ◽  
...  

Abstract Purpose To objectively determine whether there is potential thermal tissue damage during Tm:YAG laser-based LUTS treatment. Methods Our experimental model was comprised of a prostatic resection trainer placed in a 37 °C water bath. In a hollowed-out central area simulating the urethral lumen, we placed a RigiFib 800 fibre, irrigation inflow regulated with a digital pump, and a type K thermocouple. A second thermocouple was inserted 0.5/1 cm adjacently and protected with an aluminum barrier to prevent it from urethral fluid. We investigated continuous and intermittent 120 W and 80 W laser application with various irrigation rates in eight measurement sessions lasting up to 14 min. Thermal measurements were recorded continuously and in real-time using MatLab. All experiments were repeated five times to balance out variations. Results Continuous laser application at 120 W and 125 ml/min caused a urethral ∆T of ~ 15 K and a parenchymal temperature increase of up to 7 K. With 50 ml/min irrigation, a urethral and parenchymal ∆T of 30 K and 15 K were reached, respectively. Subsequently and in absence of laser application, prostatic parenchyma needed over 16 min to reach baseline body temperature. At 80 W lower temperature increases were reached compared to similar irrigation but higher power. Conclusions We showed that potentially harming temperatures can be reached, especially during high laser power and low irrigation. The heat generation can also be conveyed to the prostate parenchyma and deeper structures, potentially affecting the neurovascular bundles. Further clinical studies with intracorporal temperature measurement are necessary to further investigate this potentially harming surgical adverse effect.


2021 ◽  
pp. 103849
Author(s):  
Wensheng Zhang ◽  
Linjun Li ◽  
Qiong Gao ◽  
Sheng Zhou
Keyword(s):  

Author(s):  
Stephan Huusmann ◽  
Marcel Lafos ◽  
Ingo Meyenburg ◽  
Rolf Muschter ◽  
Heinrich-Otto Teichmann ◽  
...  

Abstract Purpose The objective of this study is to evaluate the laser-tissue effects of laser radiation emitted by a newly developed high frequency pulsed Tm:YAG laser in comparison to the continuous wave Tm:YAG laser and the pulsed Ho:YAG laser. Methods Ex-vivo experiments were performed on freshly slaughtered porcine kidneys in a physiological saline solution. Experiments were performed using two different laser devices in different settings: A Tm:YAG laser was operated in a pulsed mode up to 300 Hz and in a continuous wave (CW) mode. Results were compared with a 100 W standard pulsed Ho:YAG laser system. Comparative tissue experiments were performed at 5 W, 40 W and 80 W. The incision depth and the laser damage zone were measured under a microscope using a calibrated ocular scale. Results Increased laser power resulted in increased incision depth and increased laser damage zone for all investigated lasers in this set-up. The Ho:YAG created the largest combined tissue effect at the 5 W power setting and seems to be the least controllable laser at low power for soft tissue incisions. The CW Tm:YAG did not incise at all at 5 W, but created the largest laser damage zone. For the new pulsed Tm:YAG laser the tissue effect grew evenly with increasing power. Conclusion Among the investigated laser systems in this setting the pulsed Tm:YAG laser shows the most controllable behavior, insofar as both the incision depth and the laser damage zone increase evenly with increasing laser power.


Author(s):  
Yusuke Okabayashi ◽  
Yasuhiro Tomihari ◽  
Shinichi Imai ◽  
Masaki Yumoto ◽  
Satoshi Wada ◽  
...  
Keyword(s):  

2021 ◽  
Vol 9 ◽  
Author(s):  
Jörg Körner ◽  
Venkatesan Jambunathan ◽  
Fangxin Yue ◽  
Jürgen Reiter ◽  
Ondřej Slezák ◽  
...  

Abstract We present a diode-pumped, electro-optically Q-switched Tm:YAG laser with a cryogenically cooled laser crystal at 120 K. Output pulses of up to 2.55 mJ and 650 ns duration were demonstrated in an actively Q-switched configuration with a repetition rate of 1 Hz. By using cavity dumping the pulse duration was shortened to 18 ns with only a slightly lower output energy of 2.22 mJ. Furthermore, using a simplified rate equation model, we discuss design constraints on the pump fluence in a pulse pump approach for Tm:YAG to maximize the energy storage capability at a given pump power.


2020 ◽  
Vol 111 ◽  
pp. 103539
Author(s):  
Yingjie Shen ◽  
Xiaohu Han ◽  
Linjun Li ◽  
Xiaoming Duan ◽  
Long Zhou ◽  
...  

2020 ◽  
Vol 124 ◽  
pp. 105986 ◽  
Author(s):  
Linjun Li ◽  
Long Zhou ◽  
Tianxin Li ◽  
Xining Yang ◽  
Wenqiang Xie ◽  
...  

2020 ◽  
Vol 101 ◽  
pp. 109745 ◽  
Author(s):  
Lauren Guillemot ◽  
Pavel Loiko ◽  
Esrom Kifle ◽  
Jean-Louis Doualan ◽  
Alain Braud ◽  
...  

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