Optical Probe Thermometry Using Optically Trapped Erbium Oxide Nanoparticles

2015 ◽  
Vol 1779 ◽  
pp. 59-67
Author(s):  
Samuel C. Johnson ◽  
Susil Baral ◽  
Arwa A. Alaulamie ◽  
Hugh H. Richardson

ABSTRACTA new thermal imaging technique is characterized that uses an optically trapped erbium oxide nanoparticle cluster of approximately 150 nm. This technique can measure absolute temperature and has an imaging spatial resolution of the trapped particle. Scanning optical probe thermometry has been used to thermally image a cluster of gold nanowires that were excited with the trapping laser. Following a deconvolution of the measured thermal profile, a point spread function of the imaging technique has been determined to be a Gaussian with a FWHM of 165 nm. This width is a function of the clustering of Er2O3 nanoparticles used to image the nanowire. Optical probe thermometry has further been used to measure the temperature of nucleation events where a dichotomy of temperature for nucleated water occurs from degassed water and native water. Degassed water has been measured to nucleate at 555K confirming water adjacent to the gold nanoparticle superheats to the spinodal decomposition temperature before nucleating into a water vapor bubble. Following this event, the temperature inside the vapor bubble rises to the melting point of the gold nanoparticle, 1300 K which is followed by temperature stabilization. The rapid and significant temperature increase is attributed to the loss of a thermal dissipation pathway, to the surrounding water, previously available to the gold nanoparticle due to the insulator nature of the growing vapor envelope around the gold nanoparticle.

1991 ◽  
Vol 236 ◽  
Author(s):  
Adrian D. Zweig ◽  
T.F. Deutsch

AbstractWe study acoustic effects associated with the ablation of polyimide under water confinement. Ablation launches a shock in the target. After the shock propagates into the surrounding water we measure its velocity with an optical probe system. In the water the shocks decay after propagating a few hundred microns. The peak shock pressure scales with the square root of the laser fluence. Our observations can be explained by a simple model that interprets the generated pressures as being due to the heating of a confined ideal gas.


2012 ◽  
Vol 108 (1) ◽  
Author(s):  
Alexander Ohlinger ◽  
Andras Deak ◽  
Andrey A. Lutich ◽  
Jochen Feldmann

2016 ◽  
Vol 122 (4) ◽  
Author(s):  
Susil Baral ◽  
Samuel C. Johnson ◽  
Arwa A. Alaulamie ◽  
Hugh H. Richardson

2010 ◽  
Vol 57 (5A) ◽  
pp. 972-975 ◽  
Author(s):  
Yu-Ping Zhang ◽  
Jun Chen ◽  
Lian-Yang Bai ◽  
Xiao-Mao Zhou ◽  
Li-Ming Wang

2018 ◽  
Vol 1 (1) ◽  
pp. 32-38 ◽  
Author(s):  
Masaki Michihata ◽  
Jonggang Kim ◽  
Satoru Takahashi ◽  
Kiyoshi Takamasu ◽  
Yasuhiro Mizutani ◽  
...  

2014 ◽  
Author(s):  
Yoshihiko Arita ◽  
Martin Ploschner ◽  
Maciej Antkowiak ◽  
Frank Gunn-Moore ◽  
Kishan Dholakia

2018 ◽  
Vol 115 (30) ◽  
pp. 7676-7681 ◽  
Author(s):  
Yuliang Wang ◽  
Mikhail E. Zaytsev ◽  
Guillaume Lajoinie ◽  
Hai Le The ◽  
Jan C. T. Eijkel ◽  
...  

When illuminated by a laser, plasmonic nanoparticles immersed in water can very quickly and strongly heat up, leading to the nucleation of so-called plasmonic vapor bubbles. While the long-time behavior of such bubbles has been well-studied, here, using ultrahigh-speed imaging, we reveal the nucleation and early life phase of these bubbles. After some delay time from the beginning of the illumination, a giant bubble explosively grows, and collapses again within 200 μs (bubble life phase 1). The maximal bubble volume Vmax remarkably increases with decreasing laser power, leading to less total dumped energy E. This dumped energy shows a universal linear scaling relation with Vmax, irrespective of the gas concentration of the surrounding water. This finding supports that the initial giant bubble is a pure vapor bubble. In contrast, the delay time does depend on the gas concentration of the water, as gas pockets in the water facilitate an earlier vapor bubble nucleation, which leads to smaller delay times and lower bubble nucleation temperatures. After the collapse of the initial giant bubbles, first, much smaller oscillating bubbles form out of the remaining gas nuclei (bubble life phase 2). Subsequently, the known vaporization dominated growth phase takes over, and the bubble stabilizes (life phase 3). In the final life phase 4, the bubble slowly grows by gas expelling due to heating of the surrounding. Our findings on the explosive growth and collapse during the early life phase of a plasmonic vapor bubble have strong bearings on possible applications of such bubbles.


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