Growth and PhysioChemical Properties of Second-Order Nonlinear Optical L-Threonine Single Crystals

<table>Variation of <svg height="11.9625" id="M507" style="vertical-align:-3.3907pt" version="1.1" viewbox="0 0 19.35 11.9625" width="19.35" xmlns="http://www.w3.org/2000/svg" xmlns:xlink="http://www.w3.org/1999/xlink">
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q13 -21 0 -43z" id="x1D45F"></path></g>
<g transform="matrix(.012,-0,0,-.012,7.238,11.762)"><path d="M137 343l67 33q37 17 63 17q79 0 129.5 -53t50.5 -131q0 -92 -58 -156.5t-147 -64.5t-147 68t-58 182q0 63 17 119t43 95.5t61.5 72t69 52t67.5 31.5q62 22 128 33l6 -32q-56 -11 -108 -35q-149 -71 -184 -231zM227 337q-47 0 -95 -27q-6 -23 -6 -70q0 -93 36 -155.5
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q0 45 -26.5 69.5t-68.5 24.5q-67 0 -120 -79l-20 20l43 63q51 56 127 56h1q66 0 107 -37t41 -95q0 -42 -31 -71q-22 -23 -68 -54z" id="x33"></path></g>
</svg> and electro-optic susceptibility with wavelength.</table>

Advances in Materials Science and Engineering

fig37

Figure 37

Figure 37: Growth and PhysioChemical Properties of Second-Order Nonlinear Optical L-Threonine Single Crystals 