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<title>Diffusing-wave spectroscopy</title>
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<span id="openzim-page-title" class="mw-page-title-main"><span class="mw-page-title-main">Diffusing-wave spectroscopy</span></span>
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<div id="mw-content-text" class="mw-body-content mw-content-ltr" lang="en" dir="ltr"><div class="mw-content-ltr mw-parser-output" lang="en" dir="ltr"><p><b>Diffusing-wave spectroscopy</b> (<b>DWS</b>) is an optical technique derived from <a href="Dynamic_light_scattering" title="Dynamic light scattering">dynamic light scattering</a> (DLS) that studies the dynamics of scattered light in the limit of strong multiple scattering.<sup id="cite_ref-1" class="reference"><a href="#cite_note-1"><span class="cite-bracket">[</span>1<span class="cite-bracket">]</span></a></sup><sup id="cite_ref-2" class="reference"><a href="#cite_note-2"><span class="cite-bracket">[</span>2<span class="cite-bracket">]</span></a></sup> It has been widely used in the past to study colloidal <a href="Suspension_(chemistry)" title="Suspension (chemistry)">suspensions</a>, <a href="Emulsions" class="mw-redirect" title="Emulsions">emulsions</a>, <a href="Foams" class="mw-redirect" title="Foams">foams</a>, gels, biological media and other forms of <a href="Soft_matter" title="Soft matter">soft matter</a>. If carefully calibrated, DWS allows the quantitative measurement of microscopic motion in a soft material, from which the <a href="Rheological" class="mw-redirect" title="Rheological">rheological</a> properties of the complex medium can be extracted via the <a href="Microrheology" title="Microrheology">microrheology</a> approach.
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<div class="mw-heading mw-heading2"><h2 id="One-speckle_diffusing-wave_spectroscopy">One-speckle diffusing-wave spectroscopy</h2></div>
<p>Laser light is sent to the sample and the outcoming transmitted or backscattered light is detected by an optoelectric sensor. The light intensity detected is the result of the interference of all the optical waves coming from the different light paths.
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<div class="gallerytext">Typical setup of diffusing-wave spectroscopy</div>
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<p>The signal is analysed by calculating the intensity <a href="Autocorrelation" title="Autocorrelation">autocorrelation</a> function called g<sub>2</sub>.
<span class="mwe-math-element mwe-math-element-inline"><span class="mwe-math-mathml-inline mwe-math-mathml-a11y" style="display: none;"><math xmlns="http://www.w3.org/1998/Math/MathML" alttext="{\displaystyle g_{2}(\tau )={\frac {\langle I(t)I(t+\tau )\rangle _{t}}{\langle I(t)\rangle _{t}^{2}}}}">
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<annotation encoding="application/x-tex">{\displaystyle g_{2}(\tau )={\frac {\langle I(t)I(t+\tau )\rangle _{t}}{\langle I(t)\rangle _{t}^{2}}}}</annotation>
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</math></span><img src="./f88dd241b57c7b9e37809386665ff5e1a1bec39f.svg" class="mwe-math-fallback-image-inline mw-invert skin-invert" aria-hidden="true" style="vertical-align: -2.838ex; width:23.428ex; height:6.676ex;" alt="{\displaystyle g_{2}(\tau )={\frac {\langle I(t)I(t+\tau )\rangle _{t}}{\langle I(t)\rangle _{t}^{2}}}}" loading="lazy"></span>
</p><p>For the case of non-interacting particles suspended in a (complex) fluid a direct relation between g<sub>2</sub>-1 and the <a href="Mean_squared_displacement" title="Mean squared displacement">mean squared displacement</a> of the particles &lt;Δr<sup>2</sup>&gt; can be established. Let us note P(s) the probability density function (PDF) of the photon path length s. The relation can be written as follows:<sup id="cite_ref-3" class="reference"><a href="#cite_note-3"><span class="cite-bracket">[</span>3<span class="cite-bracket">]</span></a></sup>
</p><p><span class="mwe-math-element mwe-math-element-inline"><span class="mwe-math-mathml-inline mwe-math-mathml-a11y" style="display: none;"><math xmlns="http://www.w3.org/1998/Math/MathML" alttext="{\displaystyle g_{2}(\tau )-1=[\int {dsP(s)\exp(-(s/l*)k_{0}^{2}\langle \Delta r^{2}(\tau )\rangle )}]^{2}}">
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<annotation encoding="application/x-tex">{\displaystyle g_{2}(\tau )-1=[\int {dsP(s)\exp(-(s/l*)k_{0}^{2}\langle \Delta r^{2}(\tau )\rangle )}]^{2}}</annotation>
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</math></span><img src="./b4749882fffb6d3e6d9dd48ad98b43e707862788.svg" class="mwe-math-fallback-image-inline mw-invert skin-invert" aria-hidden="true" style="vertical-align: -2.338ex; width:48.756ex; height:5.676ex;" alt="{\displaystyle g_{2}(\tau )-1=[\int {dsP(s)\exp(-(s/l*)k_{0}^{2}\langle \Delta r^{2}(\tau )\rangle )}]^{2}}" loading="lazy"></span>
</p><p>with <span class="mwe-math-element mwe-math-element-inline"><span class="mwe-math-mathml-inline mwe-math-mathml-a11y" style="display: none;"><math xmlns="http://www.w3.org/1998/Math/MathML" alttext="{\displaystyle k_{0}={\frac {2\pi n}{\lambda }}}">
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<annotation encoding="application/x-tex">{\displaystyle k_{0}={\frac {2\pi n}{\lambda }}}</annotation>
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</math></span><img src="./f44a6bb33ac755ce4492814a771348e214efb519.svg" class="mwe-math-fallback-image-inline mw-invert skin-invert" aria-hidden="true" style="vertical-align: -2.005ex; width:10.089ex; height:5.343ex;" alt="{\displaystyle k_{0}={\frac {2\pi n}{\lambda }}}" loading="lazy"></span> and <span class="mwe-math-element mwe-math-element-inline"><span class="mwe-math-mathml-inline mwe-math-mathml-a11y" style="display: none;"><math xmlns="http://www.w3.org/1998/Math/MathML" alttext="{\displaystyle l*}">
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</math></span><img src="./a366d1873178559c309cca2bf468fd073fb8f9a2.svg" class="mwe-math-fallback-image-inline mw-invert skin-invert" aria-hidden="true" style="vertical-align: -0.338ex; width:1.856ex; height:2.176ex;" alt="{\displaystyle l*}" loading="lazy"></span> is the transport mean free path of scattered light.
</p><p>For simple cell geometries, it is thus possible to calculate the mean squared displacement of the particles &lt;Δr<sup>2</sup>&gt; from the measured g<sub>2</sub>-1 values analytically. For example, for the backscattering geometry, an infinitely thick cell, large laser spot illumination and detection of photons coming from the center of the spot, the relationship between g<sub>2</sub>-1 and &lt;Δr<sup>2</sup>&gt; is:
</p><p><span class="mwe-math-element mwe-math-element-inline"><span class="mwe-math-mathml-inline mwe-math-mathml-a11y" style="display: none;"><math xmlns="http://www.w3.org/1998/Math/MathML" alttext="{\displaystyle g_{2}(\tau )-1=\exp \left(-2\gamma {\sqrt {\langle \Delta r^{2}(\tau )\rangle k_{0}^{2}}}\right)}">
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<annotation encoding="application/x-tex">{\displaystyle g_{2}(\tau )-1=\exp \left(-2\gamma {\sqrt {\langle \Delta r^{2}(\tau )\rangle k_{0}^{2}}}\right)}</annotation>
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</math></span><img src="./e027ebac7d3fe22206166399e8590eaaba0d8b95.svg" class="mwe-math-fallback-image-inline mw-invert skin-invert" aria-hidden="true" style="vertical-align: -1.838ex; width:36.285ex; height:4.843ex;" alt="{\displaystyle g_{2}(\tau )-1=\exp \left(-2\gamma {\sqrt {\langle \Delta r^{2}(\tau )\rangle k_{0}^{2}}}\right)}" loading="lazy"></span>, γ value is around 2.
</p><p>For less thick cells and in transmission, the relationship depends also on l* (the transport length).<sup id="cite_ref-4" class="reference"><a href="#cite_note-4"><span class="cite-bracket">[</span>4<span class="cite-bracket">]</span></a></sup>
</p><p>For quasi-transparent cells, an angle-independent variant method called cavity amplified scattering spectroscopy<sup id="cite_ref-5" class="reference"><a href="#cite_note-5"><span class="cite-bracket">[</span>5<span class="cite-bracket">]</span></a></sup> makes use of an <a href="Integrating_sphere" title="Integrating sphere">integrating sphere</a> to isotropically probe samples from all directions, elongating photon paths through the sample in the process, allowing for the study of low turbidity samples under the DWS formalism.
</p>
<div class="mw-heading mw-heading2"><h2 id="Multispeckle_diffusing-wave_spectroscopy_(MSDWS)">Multispeckle diffusing-wave spectroscopy (MSDWS)</h2></div>
<p>This technique either uses a camera to detect many speckle grains (see <a href="Speckle_pattern" class="mw-redirect" title="Speckle pattern">speckle pattern</a>) or a ground glass to create a large number of speckle realizations (Echo-DWS<sup id="cite_ref-6" class="reference"><a href="#cite_note-6"><span class="cite-bracket">[</span>6<span class="cite-bracket">]</span></a></sup>). In both cases an average over a large number of statistically independent intensity values is obtained, allowing a much faster data acquisition time.
</p>
<ul class="gallery mw-gallery-traditional">
<li class="gallerybox" style="width: 155px">
<div class="thumb" style="width: 150px; height: 150px;"><span typeof="mw:File"></span></div>
<div class="gallerytext">Typical setup of Multispeckle Diffusing-wave spectroscopy</div>
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<p><span class="mwe-math-element mwe-math-element-inline"><span class="mwe-math-mathml-inline mwe-math-mathml-a11y" style="display: none;"><math xmlns="http://www.w3.org/1998/Math/MathML" alttext="{\displaystyle g_{2}(\tau )={\frac {\langle I(t)I(t+\tau )\rangle _{p}}{\langle I(t)\rangle _{p}^{2}}}}">
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<annotation encoding="application/x-tex">{\displaystyle g_{2}(\tau )={\frac {\langle I(t)I(t+\tau )\rangle _{p}}{\langle I(t)\rangle _{p}^{2}}}}</annotation>
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</p><p>MSDWS is particularly adapted for the study of slow dynamics and non ergodic media. Echo-DWS allows seamless integration of MSDWS in a traditional DWS-scheme with superior <a href="Temporal_resolution" title="Temporal resolution">temporal resolution</a> down to 12&nbsp;ns.<sup id="cite_ref-7" class="reference"><a href="#cite_note-7"><span class="cite-bracket">[</span>7<span class="cite-bracket">]</span></a></sup> Camera based adaptive image processing allows online measurement of particle dynamics for example during drying.<sup id="cite_ref-8" class="reference"><a href="#cite_note-8"><span class="cite-bracket">[</span>8<span class="cite-bracket">]</span></a></sup>
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<div class="mw-heading mw-heading2"><h2 id="References">References</h2></div>
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<div class="mw-heading mw-heading2"><h2 id="External_links">External links</h2></div>
<ul><li><a rel="nofollow" class="external text" href="https://web.archive.org/web/20110930154856/http://www.formulaction.com/technology_dws.html">Diffusing Wave Spectroscopy Overview with video</a></li>
<li><a rel="nofollow" class="external text" href="http://www.lsinstruments.ch/technology/diffusing_wave_spectroscopy_dws/">Diffusing Wave Spectroscopy Overview with Animations</a> <a rel="nofollow" class="external text" href="https://web.archive.org/web/20140520215951/http://www.lsinstruments.ch/technology/diffusing_wave_spectroscopy_dws">Archived</a> 2014-05-20 at the <a href="Wayback_Machine" title="Wayback Machine">Wayback Machine</a></li>
<li><a rel="nofollow" class="external text" href="http://www.lsinstruments.ch/technology/diffusing_wave_spectroscopy_dws/dws_particle_sizing/">Particle Sizing using Diffusing Wave Spectroscopy</a> <a rel="nofollow" class="external text" href="https://web.archive.org/web/20140520220247/http://www.lsinstruments.ch/technology/diffusing_wave_spectroscopy_dws/dws_particle_sizing/">Archived</a> 2014-05-20 at the <a href="Wayback_Machine" title="Wayback Machine">Wayback Machine</a></li></ul></div><!--htdig_noindex--><div><div class="zim-footer">
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