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Cell Imaging Using Picosecond Ultrasonics - Revision history
2024-03-29T07:47:10Z
Revision history for this page on the wiki
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Fernando Perez-Cota: /* Related Publications and Talks */
2018-07-18T11:02:09Z
<p><span dir="auto"><span class="autocomment">Related Publications and Talks</span></span></p>
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<td colspan='2' style="background-color: white; color:black; text-align: center;">← Older revision</td>
<td colspan='2' style="background-color: white; color:black; text-align: center;">Revision as of 11:02, 18 July 2018</td>
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<tr><td class='diff-marker'> </td><td style="background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;"><div>==Related Publications and Talks==</div></td><td class='diff-marker'> </td><td style="background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;"><div>==Related Publications and Talks==</div></td></tr>
<tr><td class='diff-marker'> </td><td style="background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;"></td><td class='diff-marker'> </td><td style="background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;"></td></tr>
<tr><td class='diff-marker'>−</td><td style="color:black; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #ffe49c; vertical-align: top; white-space: pre-wrap;"><div>Publications:</div></td><td class='diff-marker'>+</td><td style="color:black; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #a3d3ff; vertical-align: top; white-space: pre-wrap;"><div><ins class="diffchange diffchange-inline">===</ins>Publications:<ins class="diffchange diffchange-inline">===</ins></div></td></tr>
<tr><td class='diff-marker'> </td><td style="background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;"></td><td class='diff-marker'> </td><td style="background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;"></td></tr>
<tr><td class='diff-marker'>−</td><td style="color:black; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #ffe49c; vertical-align: top; white-space: pre-wrap;"><div>Cell imaging by phonon microscopy: sub-optical wavelength ultrasound for non-invasive imaging. Fernando Perez-Cota et al, Imaging & Microscopy 2017 (3).</div></td><td class='diff-marker'>+</td><td style="color:black; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #a3d3ff; vertical-align: top; white-space: pre-wrap;"><div><ins class="diffchange diffchange-inline">'''</ins>Cell imaging by phonon microscopy: sub-optical wavelength ultrasound for non-invasive imaging<ins class="diffchange diffchange-inline">'''</ins>. Fernando Perez-Cota et al, Imaging & Microscopy 2017 (3).</div></td></tr>
<tr><td class='diff-marker'> </td><td style="background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;"></td><td class='diff-marker'> </td><td style="background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;"></td></tr>
<tr><td class='diff-marker'>−</td><td style="color:black; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #ffe49c; vertical-align: top; white-space: pre-wrap;"><div>High resolution imaging of living cells with sub-optical wavelength phonons Perez-Cota F., Smith R. J. Moradi E., Marques L., Webb K, and Clark M. Scientific Reports.</div></td><td class='diff-marker'>+</td><td style="color:black; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #a3d3ff; vertical-align: top; white-space: pre-wrap;"><div><ins class="diffchange diffchange-inline">'''</ins>High resolution imaging of living cells with sub-optical wavelength phonons<ins class="diffchange diffchange-inline">''' </ins>Perez-Cota F., Smith R. J. Moradi E., Marques L., Webb K, and Clark M. Scientific Reports.</div></td></tr>
<tr><td class='diff-marker'> </td><td style="background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;"></td><td class='diff-marker'> </td><td style="background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;"></td></tr>
<tr><td class='diff-marker'>−</td><td style="color:black; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #ffe49c; vertical-align: top; white-space: pre-wrap;"><div>Thin film transdcuers for subcellular Brillouin oscillation imaging of individual biological cells, Perez-Cota F., Smith R. J. Moradi E., Marques L., Webb K, and Clark M.,Appl. Opts. 54 28 (2015)</div></td><td class='diff-marker'>+</td><td style="color:black; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #a3d3ff; vertical-align: top; white-space: pre-wrap;"><div><ins class="diffchange diffchange-inline">'''</ins>Thin film transdcuers for subcellular Brillouin oscillation imaging of individual biological cells<ins class="diffchange diffchange-inline">'''</ins>, Perez-Cota F., Smith R. J. Moradi E., Marques L., Webb K, and Clark M.,Appl. Opts. 54 28 (2015)</div></td></tr>
<tr><td class='diff-marker'> </td><td style="background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;"></td><td class='diff-marker'> </td><td style="background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;"></td></tr>
<tr><td class='diff-marker'>−</td><td style="color:black; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #ffe49c; vertical-align: top; white-space: pre-wrap;"><div>Optically excited nanoscaled ultrasonic transducers, Smith R. J. , Perez-Cota F., Marques L., Xuesheng C., Ahmet A., Webb K, Aylott J., Somekh M. G. and Clark M., JASA 137 1 (2015)</div></td><td class='diff-marker'>+</td><td style="color:black; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #a3d3ff; vertical-align: top; white-space: pre-wrap;"><div><ins class="diffchange diffchange-inline">'''</ins>Optically excited nanoscaled ultrasonic transducers<ins class="diffchange diffchange-inline">'''</ins>, Smith R. J. , Perez-Cota F., Marques L., Xuesheng C., Ahmet A., Webb K, Aylott J., Somekh M. G. and Clark M., JASA 137 1 (2015)</div></td></tr>
<tr><td class='diff-marker'> </td><td style="background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;"></td><td class='diff-marker'> </td><td style="background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;"></td></tr>
<tr><td class='diff-marker'> </td><td style="background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;"></td><td class='diff-marker'> </td><td style="background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;"></td></tr>
<tr><td class='diff-marker'>−</td><td style="color:black; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #ffe49c; vertical-align: top; white-space: pre-wrap;"><div>Proceedings:</div></td><td class='diff-marker'>+</td><td style="color:black; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #a3d3ff; vertical-align: top; white-space: pre-wrap;"><div><ins class="diffchange diffchange-inline">===</ins>Proceedings:<ins class="diffchange diffchange-inline">===</ins></div></td></tr>
<tr><td class='diff-marker'> </td><td style="background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;"></td><td class='diff-marker'> </td><td style="background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;"></td></tr>
<tr><td class='diff-marker'>−</td><td style="color:black; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #ffe49c; vertical-align: top; white-space: pre-wrap;"><div>Cell imaging with sub-optical wavelength ultrasound. Clark M., Marques L., Moradi E.,Perez-Cota F., Smith R. J., and Webb K. Asia Communications and Photonics Conference (2015).</div></td><td class='diff-marker'>+</td><td style="color:black; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #a3d3ff; vertical-align: top; white-space: pre-wrap;"><div><ins class="diffchange diffchange-inline">'''</ins>Cell imaging with sub-optical wavelength ultrasound<ins class="diffchange diffchange-inline">'''</ins>. Clark M., Marques L., Moradi E.,Perez-Cota F., Smith R. J., and Webb K. Asia Communications and Photonics Conference (2015).</div></td></tr>
<tr><td class='diff-marker'> </td><td style="background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;"></td><td class='diff-marker'> </td><td style="background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;"></td></tr>
<tr><td class='diff-marker'>−</td><td style="color:black; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #ffe49c; vertical-align: top; white-space: pre-wrap;"><div>Thin-film transducers for the detection and imaging of Brillouin oscillations in transmission on cultured cells. Perez-Cota F., Smith R. J. Moradi E., Webb K, and Clark M.,JPCS AFPAC (2015)</div></td><td class='diff-marker'>+</td><td style="color:black; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #a3d3ff; vertical-align: top; white-space: pre-wrap;"><div><ins class="diffchange diffchange-inline">'''</ins>Thin-film transducers for the detection and imaging of Brillouin oscillations in transmission on cultured cells<ins class="diffchange diffchange-inline">'''</ins>. Perez-Cota F., Smith R. J. Moradi E., Webb K, and Clark M.,JPCS AFPAC (2015)</div></td></tr>
<tr><td class='diff-marker'> </td><td style="background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;"></td><td class='diff-marker'> </td><td style="background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;"></td></tr>
<tr><td class='diff-marker'>−</td><td style="color:black; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #ffe49c; vertical-align: top; white-space: pre-wrap;"><div>Sound of nano J. Aylott, M. Clark, L. Marques, F. Perez-Cota, R.J. Smith and K. F. Webb. SPIE 8923, Micro/Nano Materials, Devices, and Systems Proceedings (2013).</div></td><td class='diff-marker'>+</td><td style="color:black; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #a3d3ff; vertical-align: top; white-space: pre-wrap;"><div><ins class="diffchange diffchange-inline">'''</ins>Sound of nano<ins class="diffchange diffchange-inline">''' </ins>J. Aylott, M. Clark, L. Marques, F. Perez-Cota, R.J. Smith and K. F. Webb. SPIE 8923, Micro/Nano Materials, Devices, and Systems Proceedings (2013).</div></td></tr>
<tr><td class='diff-marker'> </td><td style="background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;"></td><td class='diff-marker'> </td><td style="background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;"></td></tr>
<tr><td class='diff-marker'> </td><td style="background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;"></td><td class='diff-marker'> </td><td style="background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;"></td></tr>
<tr><td class='diff-marker'>−</td><td style="color:black; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #ffe49c; vertical-align: top; white-space: pre-wrap;"><div>Talks:</div></td><td class='diff-marker'>+</td><td style="color:black; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #a3d3ff; vertical-align: top; white-space: pre-wrap;"><div><ins class="diffchange diffchange-inline">===</ins>Talks:<ins class="diffchange diffchange-inline">===</ins></div></td></tr>
<tr><td class='diff-marker'> </td><td style="background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;"></td><td class='diff-marker'> </td><td style="background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;"></td></tr>
<tr><td class='diff-marker'>−</td><td style="color:black; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #ffe49c; vertical-align: top; white-space: pre-wrap;"><div>Cell investigations using picosecond laser ultrasound imaging Perez-Cota F., Smith R. J. Moradi E., Webb K, and Clark M. LU Linz Austria (2016) oral presentation.</div></td><td class='diff-marker'>+</td><td style="color:black; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #a3d3ff; vertical-align: top; white-space: pre-wrap;"><div>Cell investigations using picosecond laser ultrasound imaging Perez-Cota F., Smith R. J. Moradi E., Webb K, and Clark M. <ins class="diffchange diffchange-inline">'''</ins>LU Linz Austria (2016)<ins class="diffchange diffchange-inline">''' </ins>oral presentation.</div></td></tr>
<tr><td class='diff-marker'> </td><td style="background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;"></td><td class='diff-marker'> </td><td style="background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;"></td></tr>
<tr><td class='diff-marker'>−</td><td style="color:black; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #ffe49c; vertical-align: top; white-space: pre-wrap;"><div>Cell imaging based on Brillouin oscillations detection in transmission using thin-film transducers Perez-Cota F., Smith R. J. Moradi E., Webb K, and Clark M. LU Chicago IL (2015) oral presentation.</div></td><td class='diff-marker'>+</td><td style="color:black; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #a3d3ff; vertical-align: top; white-space: pre-wrap;"><div>Cell imaging based on Brillouin oscillations detection in transmission using thin-film transducers Perez-Cota F., Smith R. J. Moradi E., Webb K, and Clark M. <ins class="diffchange diffchange-inline">'''</ins>LU Chicago IL (2015)<ins class="diffchange diffchange-inline">''' </ins>oral presentation.</div></td></tr>
<tr><td class='diff-marker'> </td><td style="background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;"></td><td class='diff-marker'> </td><td style="background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;"></td></tr>
<tr><td class='diff-marker'>−</td><td style="color:black; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #ffe49c; vertical-align: top; white-space: pre-wrap;"><div>Design and application of nano-scaled ultrasonic transducers F. Perez Cota, R.J. Smith, L. Marques, K. F. Webb and M. Clark. RCNDE ERS Glasgow (2014), oral presentation.</div></td><td class='diff-marker'>+</td><td style="color:black; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #a3d3ff; vertical-align: top; white-space: pre-wrap;"><div>Design and application of nano-scaled ultrasonic transducers F. Perez Cota, R.J. Smith, L. Marques, K. F. Webb and M. Clark. <ins class="diffchange diffchange-inline">'''</ins>RCNDE ERS Glasgow (2014)<ins class="diffchange diffchange-inline">'''</ins>, oral presentation.</div></td></tr>
<tr><td class='diff-marker'> </td><td style="background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;"></td><td class='diff-marker'> </td><td style="background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;"></td></tr>
<tr><td class='diff-marker'>−</td><td style="color:black; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #ffe49c; vertical-align: top; white-space: pre-wrap;"><div>Nano-scale transducers for picosecond ultrasonics in living cells F Perez Cota, R. J.Smith, K. F. Webb and M. Clark. LU Yokohama Japan (2013) oral presentation.</div></td><td class='diff-marker'>+</td><td style="color:black; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #a3d3ff; vertical-align: top; white-space: pre-wrap;"><div>Nano-scale transducers for picosecond ultrasonics in living cells F Perez Cota, R. J.Smith, K. F. Webb and M. Clark. <ins class="diffchange diffchange-inline">'''</ins>LU Yokohama Japan (2013)<ins class="diffchange diffchange-inline">''' </ins>oral presentation.</div></td></tr>
<tr><td class='diff-marker'> </td><td style="background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;"></td><td class='diff-marker'> </td><td style="background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;"></td></tr>
<tr><td class='diff-marker'>−</td><td style="color:black; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #ffe49c; vertical-align: top; white-space: pre-wrap;"><div>Design and application of nano-scaled transducers R. J. Smith, F. Perez Cota, L. Marques, K. F. Webb and M. Clark. IOP Optics and Ultrasound day meeting at The University of Nottingham (2013), oral presentation.</div></td><td class='diff-marker'>+</td><td style="color:black; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #a3d3ff; vertical-align: top; white-space: pre-wrap;"><div>Design and application of nano-scaled transducers R. J. Smith, F. Perez Cota, L. Marques, K. F. Webb and M. Clark. <ins class="diffchange diffchange-inline">'''</ins>IOP Optics and Ultrasound day<ins class="diffchange diffchange-inline">''' </ins>meeting at The University of Nottingham (2013), oral presentation.</div></td></tr>
<tr><td class='diff-marker'> </td><td style="background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;"></td><td class='diff-marker'> </td><td style="background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;"></td></tr>
<tr><td class='diff-marker'>−</td><td style="color:black; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #ffe49c; vertical-align: top; white-space: pre-wrap;"><div>Nano-scale transducers for picosecond ultrasound in living cells F Perez Cota, R. J. Smith, K. F. Webb and M. Clark. AFPAC (2013) oral presentation.</div></td><td class='diff-marker'>+</td><td style="color:black; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #a3d3ff; vertical-align: top; white-space: pre-wrap;"><div>Nano-scale transducers for picosecond ultrasound in living cells F Perez Cota, R. J. Smith, K. F. Webb and M. Clark. <ins class="diffchange diffchange-inline">'''</ins>AFPAC (2013)<ins class="diffchange diffchange-inline">''' </ins>oral presentation.</div></td></tr>
</table>
Fernando Perez-Cota
https://optics.eee.nottingham.ac.uk/w/index.php?title=Cell_Imaging_Using_Picosecond_Ultrasonics&diff=3698&oldid=prev
Fernando Perez-Cota: /* Related Publications and Talks */
2018-07-18T10:56:24Z
<p><span dir="auto"><span class="autocomment">Related Publications and Talks</span></span></p>
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<td colspan='2' style="background-color: white; color:black; text-align: center;">← Older revision</td>
<td colspan='2' style="background-color: white; color:black; text-align: center;">Revision as of 10:56, 18 July 2018</td>
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<tr><td class='diff-marker'> </td><td style="background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;"></td><td class='diff-marker'> </td><td style="background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;"></td></tr>
<tr><td class='diff-marker'> </td><td style="background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;"><div>==Related Publications and Talks==</div></td><td class='diff-marker'> </td><td style="background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;"><div>==Related Publications and Talks==</div></td></tr>
<tr><td class='diff-marker'>−</td><td style="color:black; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #ffe49c; vertical-align: top; white-space: pre-wrap;"><div><del style="font-weight: bold; text-decoration: none;"><bibtex></del></div></td><td colspan="2"> </td></tr>
<tr><td class='diff-marker'>−</td><td style="color:black; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #ffe49c; vertical-align: top; white-space: pre-wrap;"><div><del style="font-weight: bold; text-decoration: none;">@article{perez-cota_thin-film_2015, title = {Thin-film optoacoustic transducers for subcellular Brillouin oscillation imaging of individual biological cells}, volume = {54}, issn = {0003-6935, 1539-4522}, url = {http://www.osapublishing.org/abstract.cfm?URI=ao-54-28-8388}, doi = {10.1364/AO.54.008388}, language = {en}, number = {28}, urldate = {2015-09-25}, journal = {Applied Optics}, author = {Pérez-Cota Fernando and Smith Richard J. and Moradi Emilia and Marques Leonel and Webb Kevin F. and Clark Matt}, month = {oct}, year = {2015}, pages = {8388}}</del></div></td><td colspan="2"> </td></tr>
<tr><td class='diff-marker'>−</td><td style="color:black; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #ffe49c; vertical-align: top; white-space: pre-wrap;"><div><del style="font-weight: bold; text-decoration: none;"></bibtex></del></div></td><td colspan="2"> </td></tr>
<tr><td class='diff-marker'> </td><td style="background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;"></td><td class='diff-marker'> </td><td style="background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;"></td></tr>
<tr><td class='diff-marker'>−</td><td style="color:black; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #ffe49c; vertical-align: top; white-space: pre-wrap;"><div><del class="diffchange diffchange-inline"><bibtex>@article{smith_optically_2015, title = {Optically excited nanoscale ultrasonic transducers}, volume = {137}, issn = {0001-4966}, url = {http</del>:<del class="diffchange diffchange-inline">//scitation.aip.org/content/asa/journal/jasa/137/1/10.1121/1.4904487}, doi = {10.1121/1.4904487},}, number = {1}, urldate = {2015-02-09}, journal = {The Journal of the Acoustical Society of America}, author = {Smith Richard J. and Cota Fernando Perez and Marques Leonel and Chen Xuesheng and Arca Ahmet and Webb Kevin and Aylott Jonathon and Somekh Micheal G. and Clark Matt}, month = {jan}, year = {2015}, keywords = {Acoustic sensing, Optical resonators, Proteins, Ultrasonic transducers, Ultrasonography}, pages = {219--227},</del></div></td><td class='diff-marker'>+</td><td style="color:black; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #a3d3ff; vertical-align: top; white-space: pre-wrap;"><div><ins class="diffchange diffchange-inline">Publications</ins>:</div></td></tr>
<tr><td class='diff-marker'>−</td><td style="color:black; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #ffe49c; vertical-align: top; white-space: pre-wrap;"><div><del class="diffchange diffchange-inline"></bibtex></del></div></td><td colspan="2"> </td></tr>
<tr><td class='diff-marker'> </td><td style="background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;"></td><td class='diff-marker'> </td><td style="background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;"></td></tr>
<tr><td class='diff-marker'>−</td><td style="color:black; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #ffe49c; vertical-align: top; white-space: pre-wrap;"><div><del class="diffchange diffchange-inline">Richard Smith, </del>Fernando Perez<del class="diffchange diffchange-inline">, LeonelMarques, Matt Clark,Design and application of nano</del>-<del class="diffchange diffchange-inline">scaled transducers,Institute of Physics Optics + Ultrasound One Day Meeting, May 2013, Nottingham</del>, <del class="diffchange diffchange-inline">UK</del></div></td><td class='diff-marker'>+</td><td style="color:black; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #a3d3ff; vertical-align: top; white-space: pre-wrap;"><div><ins class="diffchange diffchange-inline">Cell imaging by phonon microscopy: sub-optical wavelength ultrasound for non-invasive imaging. </ins>Fernando Perez-<ins class="diffchange diffchange-inline">Cota et al</ins>, <ins class="diffchange diffchange-inline">Imaging & Microscopy 2017 (3).</ins></div></td></tr>
<tr><td class='diff-marker'> </td><td style="background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;"></td><td class='diff-marker'> </td><td style="background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;"></td></tr>
<tr><td class='diff-marker'>−</td><td style="color:black; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #ffe49c; vertical-align: top; white-space: pre-wrap;"><div><del class="diffchange diffchange-inline">Fernando </del>Perez Cota, M. Clark, K. F. Webb, and R.J. Smith, <del class="diffchange diffchange-inline">Nanoscale </del>transducers for picosecond <del class="diffchange diffchange-inline">laser </del>ultrasonics in cells,<del class="diffchange diffchange-inline">3rd symposium </del>of <del class="diffchange diffchange-inline">laser ultrasonics</del>, <del class="diffchange diffchange-inline">June </del>2013, <del class="diffchange diffchange-inline">Yokohamma</del>, <del class="diffchange diffchange-inline">Japan</del>,</div></td><td class='diff-marker'>+</td><td style="color:black; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #a3d3ff; vertical-align: top; white-space: pre-wrap;"><div><ins class="diffchange diffchange-inline">High resolution imaging of living cells with sub-optical wavelength phonons </ins>Perez<ins class="diffchange diffchange-inline">-</ins>Cota <ins class="diffchange diffchange-inline">F.</ins>, <ins class="diffchange diffchange-inline">Smith R. J. Moradi E., Marques L., Webb K, and Clark </ins>M. <ins class="diffchange diffchange-inline">Scientific Reports.</ins></div></td></tr>
<tr><td colspan="2"> </td><td class='diff-marker'>+</td><td style="color:black; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #a3d3ff; vertical-align: top; white-space: pre-wrap;"><div> </div></td></tr>
<tr><td colspan="2"> </td><td class='diff-marker'>+</td><td style="color:black; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #a3d3ff; vertical-align: top; white-space: pre-wrap;"><div><ins class="diffchange diffchange-inline">Thin film transdcuers for subcellular Brillouin oscillation imaging of individual biological cells, Perez-Cota F., Smith R. J. Moradi E., Marques L., Webb K, and </ins>Clark <ins class="diffchange diffchange-inline">M.,Appl. Opts. 54 28 (2015)</ins></div></td></tr>
<tr><td colspan="2"> </td><td class='diff-marker'>+</td><td style="color:black; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #a3d3ff; vertical-align: top; white-space: pre-wrap;"><div> </div></td></tr>
<tr><td colspan="2"> </td><td class='diff-marker'>+</td><td style="color:black; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #a3d3ff; vertical-align: top; white-space: pre-wrap;"><div><ins class="diffchange diffchange-inline">Optically excited nanoscaled ultrasonic transducers, Smith R. J. , Perez-Cota F., Marques L., Xuesheng C., Ahmet A.</ins>, <ins class="diffchange diffchange-inline">Webb </ins>K<ins class="diffchange diffchange-inline">, Aylott J</ins>.<ins class="diffchange diffchange-inline">, Somekh M. G. and Clark M., JASA 137 1 (2015)</ins></div></td></tr>
<tr><td colspan="2"> </td><td class='diff-marker'>+</td><td style="color:black; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #a3d3ff; vertical-align: top; white-space: pre-wrap;"><div> </div></td></tr>
<tr><td colspan="2"> </td><td class='diff-marker'>+</td><td style="color:black; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #a3d3ff; vertical-align: top; white-space: pre-wrap;"><div> </div></td></tr>
<tr><td colspan="2"> </td><td class='diff-marker'>+</td><td style="color:black; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #a3d3ff; vertical-align: top; white-space: pre-wrap;"><div><ins class="diffchange diffchange-inline">Proceedings:</ins></div></td></tr>
<tr><td colspan="2"> </td><td class='diff-marker'>+</td><td style="color:black; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #a3d3ff; vertical-align: top; white-space: pre-wrap;"><div> </div></td></tr>
<tr><td colspan="2"> </td><td class='diff-marker'>+</td><td style="color:black; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #a3d3ff; vertical-align: top; white-space: pre-wrap;"><div><ins class="diffchange diffchange-inline">Cell imaging with sub-optical wavelength ultrasound. Clark M., Marques L., Moradi E.,Perez-Cota </ins>F.<ins class="diffchange diffchange-inline">, Smith R. J., and </ins>Webb <ins class="diffchange diffchange-inline">K. Asia Communications and Photonics Conference (2015).</ins></div></td></tr>
<tr><td colspan="2"> </td><td class='diff-marker'>+</td><td style="color:black; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #a3d3ff; vertical-align: top; white-space: pre-wrap;"><div> </div></td></tr>
<tr><td colspan="2"> </td><td class='diff-marker'>+</td><td style="color:black; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #a3d3ff; vertical-align: top; white-space: pre-wrap;"><div><ins class="diffchange diffchange-inline">Thin-film transducers for the detection and imaging of Brillouin oscillations in transmission on cultured cells. Perez-Cota F., Smith R. J. Moradi E., Webb K</ins>, and <ins class="diffchange diffchange-inline">Clark M.,JPCS AFPAC (2015)</ins></div></td></tr>
<tr><td colspan="2"> </td><td class='diff-marker'>+</td><td style="color:black; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #a3d3ff; vertical-align: top; white-space: pre-wrap;"><div> </div></td></tr>
<tr><td colspan="2"> </td><td class='diff-marker'>+</td><td style="color:black; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #a3d3ff; vertical-align: top; white-space: pre-wrap;"><div><ins class="diffchange diffchange-inline">Sound of nano J. Aylott, M. Clark, L. Marques, F. Perez-Cota, </ins>R.J. Smith <ins class="diffchange diffchange-inline">and K. F. Webb. SPIE 8923</ins>, <ins class="diffchange diffchange-inline">Micro/Nano Materials, Devices, and Systems Proceedings (2013).</ins></div></td></tr>
<tr><td colspan="2"> </td><td class='diff-marker'>+</td><td style="color:black; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #a3d3ff; vertical-align: top; white-space: pre-wrap;"><div> </div></td></tr>
<tr><td colspan="2"> </td><td class='diff-marker'>+</td><td style="color:black; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #a3d3ff; vertical-align: top; white-space: pre-wrap;"><div> </div></td></tr>
<tr><td colspan="2"> </td><td class='diff-marker'>+</td><td style="color:black; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #a3d3ff; vertical-align: top; white-space: pre-wrap;"><div><ins class="diffchange diffchange-inline">Talks:</ins></div></td></tr>
<tr><td colspan="2"> </td><td class='diff-marker'>+</td><td style="color:black; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #a3d3ff; vertical-align: top; white-space: pre-wrap;"><div> </div></td></tr>
<tr><td colspan="2"> </td><td class='diff-marker'>+</td><td style="color:black; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #a3d3ff; vertical-align: top; white-space: pre-wrap;"><div><ins class="diffchange diffchange-inline">Cell investigations using picosecond laser ultrasound imaging Perez-Cota F., Smith R. J. Moradi E., Webb K, and Clark M. LU Linz Austria (2016) oral presentation.</ins></div></td></tr>
<tr><td colspan="2"> </td><td class='diff-marker'>+</td><td style="color:black; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #a3d3ff; vertical-align: top; white-space: pre-wrap;"><div> </div></td></tr>
<tr><td colspan="2"> </td><td class='diff-marker'>+</td><td style="color:black; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #a3d3ff; vertical-align: top; white-space: pre-wrap;"><div><ins class="diffchange diffchange-inline">Cell imaging based on Brillouin oscillations detection in transmission using thin-film transducers Perez-Cota F., Smith R. J. Moradi E., Webb K, and Clark M. LU Chicago IL (2015) oral presentation.</ins></div></td></tr>
<tr><td colspan="2"> </td><td class='diff-marker'>+</td><td style="color:black; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #a3d3ff; vertical-align: top; white-space: pre-wrap;"><div> </div></td></tr>
<tr><td colspan="2"> </td><td class='diff-marker'>+</td><td style="color:black; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #a3d3ff; vertical-align: top; white-space: pre-wrap;"><div><ins class="diffchange diffchange-inline">Design and application of nano-scaled ultrasonic transducers F. Perez Cota, R.J. Smith, L. Marques, K. F. Webb and M. Clark. RCNDE ERS Glasgow (2014), oral presentation.</ins></div></td></tr>
<tr><td colspan="2"> </td><td class='diff-marker'>+</td><td style="color:black; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #a3d3ff; vertical-align: top; white-space: pre-wrap;"><div> </div></td></tr>
<tr><td colspan="2"> </td><td class='diff-marker'>+</td><td style="color:black; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #a3d3ff; vertical-align: top; white-space: pre-wrap;"><div><ins class="diffchange diffchange-inline">Nano-scale </ins>transducers for picosecond ultrasonics in <ins class="diffchange diffchange-inline">living </ins>cells <ins class="diffchange diffchange-inline">F Perez Cota, R. J.Smith</ins>, <ins class="diffchange diffchange-inline">K. F. Webb and M. Clark. LU Yokohama Japan (2013) oral presentation.</ins></div></td></tr>
<tr><td colspan="2"> </td><td class='diff-marker'>+</td><td style="color:black; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #a3d3ff; vertical-align: top; white-space: pre-wrap;"><div> </div></td></tr>
<tr><td colspan="2"> </td><td class='diff-marker'>+</td><td style="color:black; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #a3d3ff; vertical-align: top; white-space: pre-wrap;"><div><ins class="diffchange diffchange-inline">Design and application </ins>of <ins class="diffchange diffchange-inline">nano-scaled transducers R. J. Smith, F. Perez Cota, L. Marques</ins>, <ins class="diffchange diffchange-inline">K. F. Webb and M. Clark. IOP Optics and Ultrasound day meeting at The University of Nottingham (</ins>2013<ins class="diffchange diffchange-inline">)</ins>, <ins class="diffchange diffchange-inline">oral presentation.</ins></div></td></tr>
<tr><td colspan="2"> </td><td class='diff-marker'>+</td><td style="color:black; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #a3d3ff; vertical-align: top; white-space: pre-wrap;"><div> </div></td></tr>
<tr><td colspan="2"> </td><td class='diff-marker'>+</td><td style="color:black; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #a3d3ff; vertical-align: top; white-space: pre-wrap;"><div><ins class="diffchange diffchange-inline">Nano-scale transducers for picosecond ultrasound in living cells F Perez Cota</ins>, <ins class="diffchange diffchange-inline">R. J. Smith</ins>, <ins class="diffchange diffchange-inline">K. F. Webb and M. Clark. AFPAC (2013) oral presentation.</ins></div></td></tr>
</table>
Fernando Perez-Cota
https://optics.eee.nottingham.ac.uk/w/index.php?title=Cell_Imaging_Using_Picosecond_Ultrasonics&diff=3697&oldid=prev
Fernando Perez-Cota: /* Ultrasonic imaging of cells */
2018-07-18T10:42:49Z
<p><span dir="auto"><span class="autocomment">Ultrasonic imaging of cells</span></span></p>
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<td colspan='2' style="background-color: white; color:black; text-align: center;">← Older revision</td>
<td colspan='2' style="background-color: white; color:black; text-align: center;">Revision as of 10:42, 18 July 2018</td>
</tr><tr><td colspan="2" class="diff-lineno" id="mw-diff-left-l43" >Line 43:</td>
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<tr><td class='diff-marker'> </td><td style="background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;"></td><td class='diff-marker'> </td><td style="background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;"></td></tr>
<tr><td class='diff-marker'> </td><td style="background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;"><div>==Ultrasonic imaging of cells==</div></td><td class='diff-marker'> </td><td style="background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;"><div>==Ultrasonic imaging of cells==</div></td></tr>
<tr><td class='diff-marker'>−</td><td style="color:black; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #ffe49c; vertical-align: top; white-space: pre-wrap;"><div>An example trace is shown below, there are three main components present in the signal<del class="diffchange diffchange-inline">. </del></div></td><td class='diff-marker'>+</td><td style="color:black; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #a3d3ff; vertical-align: top; white-space: pre-wrap;"><div>An example <ins class="diffchange diffchange-inline">of an experimental </ins>trace <ins class="diffchange diffchange-inline">obtained using a glass substrate </ins>is shown below, there are three main components present in the signal<ins class="diffchange diffchange-inline">: </ins>A signal from the transducer <ins class="diffchange diffchange-inline">resonance</ins>, one from Brillouin oscillations in the glass, and one from the cell or media. These signals are all clearly separated in the the frequency domain as shown by the FFT.</div></td></tr>
<tr><td class='diff-marker'>−</td><td style="color:black; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #ffe49c; vertical-align: top; white-space: pre-wrap;"><div>A signal from the transducer <del class="diffchange diffchange-inline">substrate</del>, one from Brillouin oscillations in the glass, and one from the cell or media. These signals are all clearly separated in the the frequency domain as shown by the FFT.</div></td><td colspan="2"> </td></tr>
<tr><td class='diff-marker'> </td><td style="background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;"><div>{|class="wikitable" align=""</div></td><td class='diff-marker'> </td><td style="background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;"><div>{|class="wikitable" align=""</div></td></tr>
<tr><td class='diff-marker'> </td><td style="background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;"><div>|-</div></td><td class='diff-marker'> </td><td style="background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;"><div>|-</div></td></tr>
</table>
Fernando Perez-Cota
https://optics.eee.nottingham.ac.uk/w/index.php?title=Cell_Imaging_Using_Picosecond_Ultrasonics&diff=3696&oldid=prev
Fernando Perez-Cota: /* Substrate Design */
2018-07-18T10:41:00Z
<p><span dir="auto"><span class="autocomment">Substrate Design</span></span></p>
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<td colspan='2' style="background-color: white; color:black; text-align: center;">← Older revision</td>
<td colspan='2' style="background-color: white; color:black; text-align: center;">Revision as of 10:41, 18 July 2018</td>
</tr><tr><td colspan="2" class="diff-lineno" id="mw-diff-left-l25" >Line 25:</td>
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<tr><td class='diff-marker'> </td><td style="background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;"><div>|}</div></td><td class='diff-marker'> </td><td style="background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;"><div>|}</div></td></tr>
<tr><td class='diff-marker'> </td><td style="background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;"></td><td class='diff-marker'> </td><td style="background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;"></td></tr>
<tr><td class='diff-marker'>−</td><td style="color:black; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #ffe49c; vertical-align: top; white-space: pre-wrap;"><div>The cells are grown on a transducer substrate similar to those described  [[Nanoscale_Ultrasonic_Transducers|here]]. The optimization of the  transducer layer <del class="diffchange diffchange-inline">is different </del>in this case<del class="diffchange diffchange-inline">. Here we are much more concerned with optimizing the optical properties of </del>the <del class="diffchange diffchange-inline">transducers. The  goal is </del>to <del class="diffchange diffchange-inline">reduce the amount </del>of <del class="diffchange diffchange-inline">blue light reaching the cell </del>and <del class="diffchange diffchange-inline">either  maximize </del>the <del class="diffchange diffchange-inline">reflected or transmitted </del>light <del class="diffchange diffchange-inline">for the probe beam</del>. <del class="diffchange diffchange-inline">We still have to ensure that the </del>acoustic <del class="diffchange diffchange-inline"> performance of the </del>transducer is <del class="diffchange diffchange-inline">ok and that </del>the <del class="diffchange diffchange-inline">acoustic bandwidth </del>is <del class="diffchange diffchange-inline"> sufficient </del>to <del class="diffchange diffchange-inline">generate waves in </del>the <del class="diffchange diffchange-inline">Brillouin </del>frequency <del class="diffchange diffchange-inline">range </del>of <del class="diffchange diffchange-inline">the sample</del>.</div></td><td class='diff-marker'>+</td><td style="color:black; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #a3d3ff; vertical-align: top; white-space: pre-wrap;"><div>The cells are grown on a transducer substrate similar to those described  [[Nanoscale_Ultrasonic_Transducers|here]]. The optimization of the  transducer layer in this case <ins class="diffchange diffchange-inline">has </ins>the <ins class="diffchange diffchange-inline">purpose </ins>to <ins class="diffchange diffchange-inline">facilitate detection </ins>of <ins class="diffchange diffchange-inline">Brillouin scattering in transmission </ins>and <ins class="diffchange diffchange-inline">protecting </ins>the <ins class="diffchange diffchange-inline">cells against pump </ins>light <ins class="diffchange diffchange-inline">and heat</ins>. <ins class="diffchange diffchange-inline">This is achieved by using an optical cavity/mechanical cavity as an opto-</ins>acoustic transducer<ins class="diffchange diffchange-inline">. The cavity </ins>is <ins class="diffchange diffchange-inline">designed to have maximum transmission at the probe wavelength while minimum at </ins>the <ins class="diffchange diffchange-inline">pump wavelength. The cavity also </ins>is <ins class="diffchange diffchange-inline">designed </ins>to <ins class="diffchange diffchange-inline">resonate at </ins>the <ins class="diffchange diffchange-inline">desired </ins>frequency <ins class="diffchange diffchange-inline">for optimized SNR. Finally heat is managed through the use </ins>of <ins class="diffchange diffchange-inline">a high thermal-conductivity substrate</ins>.</div></td></tr>
<tr><td class='diff-marker'> </td><td style="background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;"></td><td class='diff-marker'> </td><td style="background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;"></td></tr>
<tr><td class='diff-marker'> </td><td style="background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;"><div><br style="clear:both" /></div></td><td class='diff-marker'> </td><td style="background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;"><div><br style="clear:both" /></div></td></tr>
</table>
Fernando Perez-Cota
https://optics.eee.nottingham.ac.uk/w/index.php?title=Cell_Imaging_Using_Picosecond_Ultrasonics&diff=3695&oldid=prev
Fernando Perez-Cota: /* Detection mechanism - Brillouin scattering in transmission */
2018-07-18T10:34:14Z
<p><span dir="auto"><span class="autocomment">Detection mechanism - Brillouin scattering in transmission</span></span></p>
<table class="diff diff-contentalign-left" data-mw="interface">
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<col class='diff-content' />
<tr style='vertical-align: top;' lang='en'>
<td colspan='2' style="background-color: white; color:black; text-align: center;">← Older revision</td>
<td colspan='2' style="background-color: white; color:black; text-align: center;">Revision as of 10:34, 18 July 2018</td>
</tr><tr><td colspan="2" class="diff-lineno" id="mw-diff-left-l12" >Line 12:</td>
<td colspan="2" class="diff-lineno">Line 12:</td></tr>
<tr><td class='diff-marker'> </td><td style="background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;"><div>To solve some of the challenges of phonon imaging on cells, a novel detection configuration is being developed. In this configuration, an inverted microscope is used to deliver the pump and probe laser beams through the substrate where an opto-acoustic transducer converts pump light into a coherent phonon field while protecting the cells against unnecessary exposure to pump-light(UVA) and heat. The transmitted probe light (NIR) interacts with the generated phonon-field via Brillouin scattering which is collected and detected for imaging. Since the phonon field is propagating through the sample, its velocity and amplitude is related to the sample's elasticity.   </div></td><td class='diff-marker'> </td><td style="background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;"><div>To solve some of the challenges of phonon imaging on cells, a novel detection configuration is being developed. In this configuration, an inverted microscope is used to deliver the pump and probe laser beams through the substrate where an opto-acoustic transducer converts pump light into a coherent phonon field while protecting the cells against unnecessary exposure to pump-light(UVA) and heat. The transmitted probe light (NIR) interacts with the generated phonon-field via Brillouin scattering which is collected and detected for imaging. Since the phonon field is propagating through the sample, its velocity and amplitude is related to the sample's elasticity.   </div></td></tr>
<tr><td class='diff-marker'> </td><td style="background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;"></td><td class='diff-marker'> </td><td style="background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;"></td></tr>
<tr><td class='diff-marker'>−</td><td style="color:black; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #ffe49c; vertical-align: top; white-space: pre-wrap;"><div>To detect the phonon field the scattered light interferes with the directly propagating light at the detector leading to an oscillating  signal. These oscillations are termed Brillouin Oscillations and the Brillouin frequency ''f_B'' of the oscillation is given by the simple equation:</div></td><td class='diff-marker'>+</td><td style="color:black; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #a3d3ff; vertical-align: top; white-space: pre-wrap;"><div>To detect the phonon field the scattered light interferes with the directly propagating light at the detector leading to an oscillating  signal. These oscillations are termed Brillouin Oscillations and the Brillouin frequency ''f_B'' of the oscillation is given by the simple equation: ''f_B = 2*Va*n/λ'' <ins class="diffchange diffchange-inline">which relates </ins>the acoustic velocity ''Va'' with the probe wavelength ''λ'' and the refractive index ''n''.</div></td></tr>
<tr><td class='diff-marker'>−</td><td style="color:black; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #ffe49c; vertical-align: top; white-space: pre-wrap;"><div>''f_B = 2*Va*n/λ''</div></td><td colspan="2"> </td></tr>
<tr><td class='diff-marker'>−</td><td style="color:black; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #ffe49c; vertical-align: top; white-space: pre-wrap;"><div> </div></td><td colspan="2"> </td></tr>
<tr><td class='diff-marker'>−</td><td style="color:black; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #ffe49c; vertical-align: top; white-space: pre-wrap;"><div><del class="diffchange diffchange-inline">Which related </del>the acoustic velocity ''Va'' with the probe wavelength ''λ'' and the refractive index ''n''.</div></td><td colspan="2"> </td></tr>
<tr><td class='diff-marker'> </td><td style="background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;"></td><td class='diff-marker'> </td><td style="background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;"></td></tr>
<tr><td class='diff-marker'> </td><td style="background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;"><div><br style="clear:both" /></div></td><td class='diff-marker'> </td><td style="background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;"><div><br style="clear:both" /></div></td></tr>
</table>
Fernando Perez-Cota
https://optics.eee.nottingham.ac.uk/w/index.php?title=Cell_Imaging_Using_Picosecond_Ultrasonics&diff=3693&oldid=prev
Fernando Perez-Cota: /* Motivation */
2018-07-17T15:32:18Z
<p><span dir="auto"><span class="autocomment">Motivation</span></span></p>
<table class="diff diff-contentalign-left" data-mw="interface">
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<col class='diff-marker' />
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<td colspan='2' style="background-color: white; color:black; text-align: center;">← Older revision</td>
<td colspan='2' style="background-color: white; color:black; text-align: center;">Revision as of 15:32, 17 July 2018</td>
</tr><tr><td colspan="2" class="diff-lineno" id="mw-diff-left-l2" >Line 2:</td>
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<tr><td class='diff-marker'> </td><td style="background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;"><div>This project aims to develop an instrument for imaging cells using their mechanical properties as a contrast mechanism and with high resolution. The goal is to design and build a microscopy system that can be used as a general microscopy tool for cell biologists.</div></td><td class='diff-marker'> </td><td style="background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;"><div>This project aims to develop an instrument for imaging cells using their mechanical properties as a contrast mechanism and with high resolution. The goal is to design and build a microscopy system that can be used as a general microscopy tool for cell biologists.</div></td></tr>
<tr><td class='diff-marker'> </td><td style="background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;"></td><td class='diff-marker'> </td><td style="background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;"></td></tr>
<tr><td class='diff-marker'>−</td><td style="color:black; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #ffe49c; vertical-align: top; white-space: pre-wrap;"><div>To map the elasticity of cells with optical or higher resolution is very challenging. Ultrasound is a way to image with contrast derived from elasticity however, to obtain high resolution imaging this way necessitates phonons (GHz frequency ultrasound <del class="diffchange diffchange-inline">[link to Bordeaux]</del>). To work at this regime poses many challenges: phonon generation requires laser light and heat which can damage cells,  at GHz frequencies the phonons do not travel very far and the pump-probe detection method is typically low in signal-to-noise ratio and slow in acquisition speed.  </div></td><td class='diff-marker'>+</td><td style="color:black; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #a3d3ff; vertical-align: top; white-space: pre-wrap;"><div>To map the elasticity of cells with optical or higher resolution is very challenging. Ultrasound is a way to image with contrast derived from elasticity however, to obtain high resolution imaging this way necessitates phonons (GHz frequency ultrasound). To work at this regime poses many challenges: phonon generation requires laser light and heat which can damage cells,  at GHz frequencies the phonons do not travel very far and the pump-probe detection method is typically low in signal-to-noise ratio and slow in acquisition speed.  </div></td></tr>
<tr><td class='diff-marker'> </td><td style="background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;"></td><td class='diff-marker'> </td><td style="background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;"></td></tr>
<tr><td class='diff-marker'>−</td><td style="color:black; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #ffe49c; vertical-align: top; white-space: pre-wrap;"><div>If all those challenges are solved, then there can be potentially greater benefits: the energy carried by phonons is orders of magnitude lower than that of light, which is suitable for live-cell imaging and allows to use arbitrarily small wavelengths for imaging leading to super-resolution. The contrast mechanism does not require the use of dyes so its label-free and of course it will provide means to image cells based on elasticity at a resolution never achieved before. <del class="diffchange diffchange-inline"> </del></div></td><td class='diff-marker'>+</td><td style="color:black; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #a3d3ff; vertical-align: top; white-space: pre-wrap;"><div>If all those challenges are solved, then there can be potentially greater benefits: the energy carried by phonons is orders of magnitude lower than that of light, which is suitable for live-cell imaging and allows to use arbitrarily small wavelengths for imaging leading to super-resolution. The contrast mechanism does not require the use of dyes so its label-free and of course it will provide means to image cells based on elasticity at a resolution never achieved before.</div></td></tr>
<tr><td class='diff-marker'> </td><td style="background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;"></td><td class='diff-marker'> </td><td style="background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;"></td></tr>
<tr><td class='diff-marker'> </td><td style="background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;"><div>==Detection mechanism - Brillouin scattering in transmission==</div></td><td class='diff-marker'> </td><td style="background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;"><div>==Detection mechanism - Brillouin scattering in transmission==</div></td></tr>
</table>
Fernando Perez-Cota
https://optics.eee.nottingham.ac.uk/w/index.php?title=Cell_Imaging_Using_Picosecond_Ultrasonics&diff=3692&oldid=prev
Fernando Perez-Cota: /* Detection mechanism - Brillouin scattering in transmission */
2018-07-17T15:18:12Z
<p><span dir="auto"><span class="autocomment">Detection mechanism - Brillouin scattering in transmission</span></span></p>
<table class="diff diff-contentalign-left" data-mw="interface">
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<col class='diff-marker' />
<col class='diff-content' />
<tr style='vertical-align: top;' lang='en'>
<td colspan='2' style="background-color: white; color:black; text-align: center;">← Older revision</td>
<td colspan='2' style="background-color: white; color:black; text-align: center;">Revision as of 15:18, 17 July 2018</td>
</tr><tr><td colspan="2" class="diff-lineno" id="mw-diff-left-l8" >Line 8:</td>
<td colspan="2" class="diff-lineno">Line 8:</td></tr>
<tr><td class='diff-marker'> </td><td style="background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;"><div>==Detection mechanism - Brillouin scattering in transmission==</div></td><td class='diff-marker'> </td><td style="background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;"><div>==Detection mechanism - Brillouin scattering in transmission==</div></td></tr>
<tr><td class='diff-marker'> </td><td style="background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;"></td><td class='diff-marker'> </td><td style="background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;"></td></tr>
<tr><td class='diff-marker'>−</td><td style="color:black; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #ffe49c; vertical-align: top; white-space: pre-wrap;"><div>[[Image:Brillouin simple.png|<del class="diffchange diffchange-inline">150px</del>|right]]</div></td><td class='diff-marker'>+</td><td style="color:black; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #a3d3ff; vertical-align: top; white-space: pre-wrap;"><div>[[Image:Brillouin simple.png|<ins class="diffchange diffchange-inline">250px</ins>|right]]</div></td></tr>
<tr><td class='diff-marker'> </td><td style="background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;"></td><td class='diff-marker'> </td><td style="background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;"></td></tr>
<tr><td class='diff-marker'> </td><td style="background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;"><div>To solve some of the challenges of phonon imaging on cells, a novel detection configuration is being developed. In this configuration, an inverted microscope is used to deliver the pump and probe laser beams through the substrate where an opto-acoustic transducer converts pump light into a coherent phonon field while protecting the cells against unnecessary exposure to pump-light(UVA) and heat. The transmitted probe light (NIR) interacts with the generated phonon-field via Brillouin scattering which is collected and detected for imaging. Since the phonon field is propagating through the sample, its velocity and amplitude is related to the sample's elasticity.   </div></td><td class='diff-marker'> </td><td style="background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;"><div>To solve some of the challenges of phonon imaging on cells, a novel detection configuration is being developed. In this configuration, an inverted microscope is used to deliver the pump and probe laser beams through the substrate where an opto-acoustic transducer converts pump light into a coherent phonon field while protecting the cells against unnecessary exposure to pump-light(UVA) and heat. The transmitted probe light (NIR) interacts with the generated phonon-field via Brillouin scattering which is collected and detected for imaging. Since the phonon field is propagating through the sample, its velocity and amplitude is related to the sample's elasticity.   </div></td></tr>
</table>
Fernando Perez-Cota
https://optics.eee.nottingham.ac.uk/w/index.php?title=Cell_Imaging_Using_Picosecond_Ultrasonics&diff=3690&oldid=prev
Fernando Perez-Cota at 15:07, 17 July 2018
2018-07-17T15:07:45Z
<p></p>
<table class="diff diff-contentalign-left" data-mw="interface">
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<td colspan='2' style="background-color: white; color:black; text-align: center;">← Older revision</td>
<td colspan='2' style="background-color: white; color:black; text-align: center;">Revision as of 15:07, 17 July 2018</td>
</tr><tr><td colspan="2" class="diff-lineno" id="mw-diff-left-l1" >Line 1:</td>
<td colspan="2" class="diff-lineno">Line 1:</td></tr>
<tr><td class='diff-marker'> </td><td style="background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;"><div>==Motivation==</div></td><td class='diff-marker'> </td><td style="background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;"><div>==Motivation==</div></td></tr>
<tr><td class='diff-marker'>−</td><td style="color:black; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #ffe49c; vertical-align: top; white-space: pre-wrap;"><div>This project <del class="diffchange diffchange-inline">is </del>to develop an instrument for imaging cells using their mechanical properties as a contrast mechanism. The goal is to <del class="diffchange diffchange-inline">produce </del>a system that can be used as a general microscopy tool for cell biologists.</div></td><td class='diff-marker'>+</td><td style="color:black; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #a3d3ff; vertical-align: top; white-space: pre-wrap;"><div>This project <ins class="diffchange diffchange-inline">aims </ins>to develop an instrument for imaging cells using their mechanical properties as a contrast mechanism <ins class="diffchange diffchange-inline">and with high resolution</ins>. The goal is to <ins class="diffchange diffchange-inline">design and build </ins>a <ins class="diffchange diffchange-inline">microscopy </ins>system that can be used as a general microscopy tool for cell biologists.</div></td></tr>
<tr><td class='diff-marker'> </td><td style="background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;"></td><td class='diff-marker'> </td><td style="background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;"></td></tr>
<tr><td class='diff-marker'>−</td><td style="color:black; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #ffe49c; vertical-align: top; white-space: pre-wrap;"><div><del class="diffchange diffchange-inline">This </del>is very challenging <del class="diffchange diffchange-inline">as </del>to obtain high resolution imaging necessitates <del class="diffchange diffchange-inline">using high </del>frequency ultrasound and at <del class="diffchange diffchange-inline">high </del>frequencies the <del class="diffchange diffchange-inline">waves </del>do not travel very far. <del class="diffchange diffchange-inline"> Picosecond laser ultrasound has been shown (link </del>to <del class="diffchange diffchange-inline">bordeaux) </del>to <del class="diffchange diffchange-inline">be </del>a <del class="diffchange diffchange-inline">promising candidate</del>.</div></td><td class='diff-marker'>+</td><td style="color:black; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #a3d3ff; vertical-align: top; white-space: pre-wrap;"><div><ins class="diffchange diffchange-inline">To map the elasticity of cells with optical or higher resolution </ins>is very challenging<ins class="diffchange diffchange-inline">. Ultrasound is a way to image with contrast derived from elasticity however, </ins>to obtain high resolution imaging <ins class="diffchange diffchange-inline">this way </ins>necessitates <ins class="diffchange diffchange-inline">phonons (GHz </ins>frequency ultrasound <ins class="diffchange diffchange-inline">[link to Bordeaux]). To work at this regime poses many challenges: phonon generation requires laser light </ins>and <ins class="diffchange diffchange-inline">heat which can damage cells,  </ins>at <ins class="diffchange diffchange-inline">GHz </ins>frequencies the <ins class="diffchange diffchange-inline">phonons </ins>do not travel very far <ins class="diffchange diffchange-inline">and the pump-probe detection method is typically low in signal-to-noise ratio and slow in acquisition speed</ins>.  </div></td></tr>
<tr><td colspan="2"> </td><td class='diff-marker'>+</td><td style="color:black; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #a3d3ff; vertical-align: top; white-space: pre-wrap;"><div> </div></td></tr>
<tr><td colspan="2"> </td><td class='diff-marker'>+</td><td style="color:black; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #a3d3ff; vertical-align: top; white-space: pre-wrap;"><div><ins class="diffchange diffchange-inline">If all those challenges are solved, then there can be potentially greater benefits: the energy carried by phonons is orders of magnitude lower than that of light, which is suitable for live-cell imaging and allows to use arbitrarily small wavelengths for imaging leading </ins>to <ins class="diffchange diffchange-inline">super-resolution. The contrast mechanism does not require the use of dyes so its label-free and of course it will provide means </ins>to <ins class="diffchange diffchange-inline">image cells based on elasticity at </ins>a <ins class="diffchange diffchange-inline">resolution never achieved before</ins>. <ins class="diffchange diffchange-inline"> </ins></div></td></tr>
<tr><td colspan="2"> </td><td class='diff-marker'>+</td><td style="color:black; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #a3d3ff; vertical-align: top; white-space: pre-wrap;"><div> </div></td></tr>
<tr><td colspan="2"> </td><td class='diff-marker'>+</td><td style="color:black; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #a3d3ff; vertical-align: top; white-space: pre-wrap;"><div><ins class="diffchange diffchange-inline">==Detection mechanism - Brillouin scattering in transmission==</ins></div></td></tr>
<tr><td class='diff-marker'> </td><td style="background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;"></td><td class='diff-marker'> </td><td style="background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;"></td></tr>
<tr><td class='diff-marker'>−</td><td style="color:black; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #ffe49c; vertical-align: top; white-space: pre-wrap;"><div><del style="font-weight: bold; text-decoration: none;">==Detection mechanism - Brillouin Oscillations==</del></div></td><td colspan="2"> </td></tr>
<tr><td class='diff-marker'> </td><td style="background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;"><div>[[Image:Brillouin simple.png|150px|right]]</div></td><td class='diff-marker'> </td><td style="background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;"><div>[[Image:Brillouin simple.png|150px|right]]</div></td></tr>
<tr><td class='diff-marker'>−</td><td style="color:black; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #ffe49c; vertical-align: top; white-space: pre-wrap;"><div><del style="font-weight: bold; text-decoration: none;">The  probe light is reflected from the sample surface to the detector, and if the sample is transparent there is also a reflection from the acoustic wave packet traveling in  the sample. This happens because the acoustic wave causes a change in  the local refractive index and so acts as a weak mirror.  These reflections interfere at the detector and as the phase of the  reflection from the acoustic wave is changing with time it leads to an oscillating  signal. These oscillations are termed Brillouin Oscillations.</del></div></td><td colspan="2"> </td></tr>
<tr><td class='diff-marker'> </td><td style="background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;"></td><td class='diff-marker'> </td><td style="background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;"></td></tr>
<tr><td class='diff-marker'>−</td><td style="color:black; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #ffe49c; vertical-align: top; white-space: pre-wrap;"><div>The frequency ''<del class="diffchange diffchange-inline">F</del>'' of the oscillation is given by the simple equation:</div></td><td class='diff-marker'>+</td><td style="color:black; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #a3d3ff; vertical-align: top; white-space: pre-wrap;"><div><ins class="diffchange diffchange-inline">To solve some of the challenges of phonon imaging on cells, a novel detection configuration is being developed. In this configuration, an inverted microscope is used to deliver the pump and probe laser beams through the substrate where an opto-acoustic transducer converts pump light into a coherent phonon field while protecting the cells against unnecessary exposure to pump-light(UVA) and heat. </ins>The <ins class="diffchange diffchange-inline">transmitted probe light (NIR) interacts with the generated phonon-field via Brillouin scattering which is collected and detected for imaging. Since the phonon field is propagating through the sample, its velocity and amplitude is related to the sample's elasticity.  </ins></div></td></tr>
<tr><td class='diff-marker'>−</td><td style="color:black; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #ffe49c; vertical-align: top; white-space: pre-wrap;"><div>''<del class="diffchange diffchange-inline">F </del>= 2*Va*n/λ''</div></td><td class='diff-marker'>+</td><td style="color:black; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #a3d3ff; vertical-align: top; white-space: pre-wrap;"><div> </div></td></tr>
<tr><td colspan="2"> </td><td class='diff-marker'>+</td><td style="color:black; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #a3d3ff; vertical-align: top; white-space: pre-wrap;"><div><ins class="diffchange diffchange-inline">To detect the phonon field the scattered light interferes with the directly propagating light at the detector leading to an oscillating  signal. These oscillations are termed Brillouin Oscillations and the Brillouin </ins>frequency ''<ins class="diffchange diffchange-inline">f_B</ins>'' of the oscillation is given by the simple equation:</div></td></tr>
<tr><td colspan="2"> </td><td class='diff-marker'>+</td><td style="color:black; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #a3d3ff; vertical-align: top; white-space: pre-wrap;"><div>''<ins class="diffchange diffchange-inline">f_B </ins>= 2*Va*n/λ''</div></td></tr>
<tr><td class='diff-marker'> </td><td style="background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;"></td><td class='diff-marker'> </td><td style="background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;"></td></tr>
<tr><td class='diff-marker'>−</td><td style="color:black; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #ffe49c; vertical-align: top; white-space: pre-wrap;"><div><del class="diffchange diffchange-inline">So  if we can measure this signal we can measure </del>the acoustic velocity ''Va''<del class="diffchange diffchange-inline">, as  long as we know </del>the <del class="diffchange diffchange-inline">laser </del>wavelength ''λ'' and the refractive index ''n''.</div></td><td class='diff-marker'>+</td><td style="color:black; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #a3d3ff; vertical-align: top; white-space: pre-wrap;"><div><ins class="diffchange diffchange-inline">Which related </ins>the acoustic velocity ''Va'' <ins class="diffchange diffchange-inline">with </ins>the <ins class="diffchange diffchange-inline">probe </ins>wavelength ''λ'' and the refractive index ''n''.</div></td></tr>
<tr><td class='diff-marker'> </td><td style="background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;"></td><td class='diff-marker'> </td><td style="background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;"></td></tr>
<tr><td class='diff-marker'> </td><td style="background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;"><div><br style="clear:both" /></div></td><td class='diff-marker'> </td><td style="background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;"><div><br style="clear:both" /></div></td></tr>
</table>
Fernando Perez-Cota
https://optics.eee.nottingham.ac.uk/w/index.php?title=Cell_Imaging_Using_Picosecond_Ultrasonics&diff=2479&oldid=prev
Richard Smith: /* Related Publications and Talks */
2016-01-21T10:54:19Z
<p><span dir="auto"><span class="autocomment">Related Publications and Talks</span></span></p>
<table class="diff diff-contentalign-left" data-mw="interface">
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<td colspan='2' style="background-color: white; color:black; text-align: center;">← Older revision</td>
<td colspan='2' style="background-color: white; color:black; text-align: center;">Revision as of 10:54, 21 January 2016</td>
</tr><tr><td colspan="2" class="diff-lineno" id="mw-diff-left-l114" >Line 114:</td>
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<tr><td class='diff-marker'> </td><td style="background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;"></td><td class='diff-marker'> </td><td style="background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;"></td></tr>
<tr><td class='diff-marker'> </td><td style="background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;"><div>==Related Publications and Talks==</div></td><td class='diff-marker'> </td><td style="background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;"><div>==Related Publications and Talks==</div></td></tr>
<tr><td colspan="2"> </td><td class='diff-marker'>+</td><td style="color:black; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #a3d3ff; vertical-align: top; white-space: pre-wrap;"><div><ins style="font-weight: bold; text-decoration: none;"><bibtex></ins></div></td></tr>
<tr><td colspan="2"> </td><td class='diff-marker'>+</td><td style="color:black; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #a3d3ff; vertical-align: top; white-space: pre-wrap;"><div><ins style="font-weight: bold; text-decoration: none;">@article{perez-cota_thin-film_2015, title = {Thin-film optoacoustic transducers for subcellular Brillouin oscillation imaging of individual biological cells}, volume = {54}, issn = {0003-6935, 1539-4522}, url = {http://www.osapublishing.org/abstract.cfm?URI=ao-54-28-8388}, doi = {10.1364/AO.54.008388}, language = {en}, number = {28}, urldate = {2015-09-25}, journal = {Applied Optics}, author = {Pérez-Cota Fernando and Smith Richard J. and Moradi Emilia and Marques Leonel and Webb Kevin F. and Clark Matt}, month = {oct}, year = {2015}, pages = {8388}}</ins></div></td></tr>
<tr><td colspan="2"> </td><td class='diff-marker'>+</td><td style="color:black; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #a3d3ff; vertical-align: top; white-space: pre-wrap;"><div><ins style="font-weight: bold; text-decoration: none;"></bibtex></ins></div></td></tr>
<tr><td colspan="2"> </td><td class='diff-marker'>+</td><td style="color:black; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #a3d3ff; vertical-align: top; white-space: pre-wrap;"><div><ins style="font-weight: bold; text-decoration: none;"></ins></div></td></tr>
<tr><td class='diff-marker'> </td><td style="background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;"><div><bibtex>@article{smith_optically_2015, title = {Optically excited nanoscale ultrasonic transducers}, volume = {137}, issn = {0001-4966}, url = {http://scitation.aip.org/content/asa/journal/jasa/137/1/10.1121/1.4904487}, doi = {10.1121/1.4904487},}, number = {1}, urldate = {2015-02-09}, journal = {The Journal of the Acoustical Society of America}, author = {Smith Richard J. and Cota Fernando Perez and Marques Leonel and Chen Xuesheng and Arca Ahmet and Webb Kevin and Aylott Jonathon and Somekh Micheal G. and Clark Matt}, month = {jan}, year = {2015}, keywords = {Acoustic sensing, Optical resonators, Proteins, Ultrasonic transducers, Ultrasonography}, pages = {219--227},</div></td><td class='diff-marker'> </td><td style="background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;"><div><bibtex>@article{smith_optically_2015, title = {Optically excited nanoscale ultrasonic transducers}, volume = {137}, issn = {0001-4966}, url = {http://scitation.aip.org/content/asa/journal/jasa/137/1/10.1121/1.4904487}, doi = {10.1121/1.4904487},}, number = {1}, urldate = {2015-02-09}, journal = {The Journal of the Acoustical Society of America}, author = {Smith Richard J. and Cota Fernando Perez and Marques Leonel and Chen Xuesheng and Arca Ahmet and Webb Kevin and Aylott Jonathon and Somekh Micheal G. and Clark Matt}, month = {jan}, year = {2015}, keywords = {Acoustic sensing, Optical resonators, Proteins, Ultrasonic transducers, Ultrasonography}, pages = {219--227},</div></td></tr>
<tr><td class='diff-marker'> </td><td style="background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;"><div></bibtex></div></td><td class='diff-marker'> </td><td style="background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;"><div></bibtex></div></td></tr>
</table>
Richard Smith
https://optics.eee.nottingham.ac.uk/w/index.php?title=Cell_Imaging_Using_Picosecond_Ultrasonics&diff=2351&oldid=prev
Richard Smith: /* Ultrasonic imaging of cells */
2015-06-08T06:41:31Z
<p><span dir="auto"><span class="autocomment">Ultrasonic imaging of cells</span></span></p>
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<td colspan='2' style="background-color: white; color:black; text-align: center;">← Older revision</td>
<td colspan='2' style="background-color: white; color:black; text-align: center;">Revision as of 06:41, 8 June 2015</td>
</tr><tr><td colspan="2" class="diff-lineno" id="mw-diff-left-l43" >Line 43:</td>
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<tr><td class='diff-marker'> </td><td style="background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;"><div>==Ultrasonic imaging of cells==</div></td><td class='diff-marker'> </td><td style="background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;"><div>==Ultrasonic imaging of cells==</div></td></tr>
<tr><td class='diff-marker'> </td><td style="background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;"><div>An example trace is shown below, there are three main components present in the signal.  </div></td><td class='diff-marker'> </td><td style="background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;"><div>An example trace is shown below, there are three main components present in the signal.  </div></td></tr>
<tr><td class='diff-marker'>−</td><td style="color:black; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #ffe49c; vertical-align: top; white-space: pre-wrap;"><div>A signal from the transducer substrate, <del class="diffchange diffchange-inline">once </del>from Brillouin <del class="diffchange diffchange-inline">oscialltions </del>in the glass, and one from the cell or media. These signals are all clearly separated in the the frequency domain as shown by the FFT.</div></td><td class='diff-marker'>+</td><td style="color:black; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #a3d3ff; vertical-align: top; white-space: pre-wrap;"><div>A signal from the transducer substrate, <ins class="diffchange diffchange-inline">one </ins>from Brillouin <ins class="diffchange diffchange-inline">oscillations </ins>in the glass, and one from the cell or media. These signals are all clearly separated in the the frequency domain as shown by the FFT.</div></td></tr>
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<tr><td class='diff-marker'> </td><td style="background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;"></td><td class='diff-marker'> </td><td style="background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;"></td></tr>
<tr><td class='diff-marker'> </td><td style="background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;"><div>===Live Cells===</div></td><td class='diff-marker'> </td><td style="background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;"><div>===Live Cells===</div></td></tr>
<tr><td class='diff-marker'>−</td><td style="color:black; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #ffe49c; vertical-align: top; white-space: pre-wrap;"><div>Measuring live cells is much more challenging, this is because the amount of light they can tolerate without being <del class="diffchange diffchange-inline">effected </del>is much lower than the amount that would damage fixed cells. Secondly the cells can move around and so the scans need to be taken as quickly as possible.  </div></td><td class='diff-marker'>+</td><td style="color:black; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #a3d3ff; vertical-align: top; white-space: pre-wrap;"><div>Measuring live cells is much more challenging, this is because the amount of light they can tolerate without being <ins class="diffchange diffchange-inline">affected </ins>is much lower than the amount that would damage fixed cells. Secondly the cells can move around and so the scans need to be taken as quickly as possible.  </div></td></tr>
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Richard Smith