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class="newsContent-in"> <h1 class="rich_media_title " id="activity-name"><span style="font-size: 13px;font-family: 宋體;visibility: visible">超輻射發(fā)光二極管（<span style="visibility: visible">Superluminescent Diode</span>，<span style="visibility: visible">SLD</span>）</span><span style="font-size: 13px;font-family: 宋體;visibility: visible">主要基于半導體的受激發(fā)射和自發(fā)發(fā)射機制，</span><span style="font-size: 13px;font-family: 宋體;visibility: visible">是一種性能介于激光二極管（<span style="visibility: visible">LD</span>）與發(fā)光二極管（<span style="visibility: visible">LED</span>）之間的半導體光電器件。<span style="visibility: visible">SLD</span>通過(guò)放大自發(fā)輻射產(chǎn)生光，其光學(xué)性質(zhì)介于<span style="visibility: visible">LD</span>和<span style="visibility: visible">LED</span>之間，具有比<span style="visibility: visible">LD</span>更寬的發(fā)光光譜和更短的相干長(cháng)度，比<span style="visibility: visible">LED</span>有更高的輸出功率和更高的調制帶寬。</span></h1><p style="visibility: visible"><span style="font-family: 宋體;visibility: visible">一<span style="visibility: visible">. </span>自發(fā)輻射與受激發(fā)射</span></p><p style="visibility: visible"><span style="font-family: 宋體;visibility: visible">1</span><span style="font-family: 宋體;visibility: visible">、自發(fā)輻射：在<span style="visibility: visible">SLD</span>中，電子和空穴在活性區復合時(shí)，會(huì )自發(fā)地躍遷到低能態(tài)并發(fā)射光子。這些光子的能量、方向、位相和偏振等均不相同，是一種非相干光。</span></p><p style="visibility: visible"><span style="font-family: 宋體;visibility: visible">2</span><span style="font-family: 宋體;visibility: visible">、受激發(fā)射：當注入電流較高時(shí)，增益介質(zhì)中的激發(fā)密度很高，自發(fā)輻射的光子進(jìn)一步激發(fā)載流子復合產(chǎn)生相同的光子。這些受激發(fā)射的光子在增益介質(zhì)內傳播過(guò)程中不斷產(chǎn)生更多的受激輻射光子，從而使光子數量呈指數型增加。</span></p><p style="visibility: visible"><span style="font-family: 宋體;visibility: visible">二、無(wú)諧振腔設計</span></p><p style="visibility: visible"><span style="font-family: 宋體;visibility: visible">1</span><span style="font-family: 宋體;visibility: visible">、無(wú)諧振腔：與激光二極管（<span style="visibility: visible">LD</span>）不同，<span style="visibility: visible">SLD</span>沒(méi)有諧振腔結構。在<span style="visibility: visible">LD</span>中，腔體兩端面的反射作用會(huì )形成法布里－珀羅諧振，當注入電流高于閾值電流時(shí)，端面輸出增大，形成激光。而在<span style="visibility: visible">SLD</span>中，器件后端面處的反射強度不足以形成光的反饋諧振，因此<span style="visibility: visible">SLD</span>輸出的是非相干光。</span></p><p style="visibility: visible"><span style="font-family: 宋體;visibility: visible">2</span><span style="font-family: 宋體;visibility: visible">、單程放大：<span style="visibility: visible">SLD</span>中的光子只經(jīng)歷了單程的放大過(guò)程，而不是多次反射放大。因此，要達到與激光等光強，<span style="visibility: visible">SLD</span>必須工作在更高的電流密度下。</span></p><p style="visibility: visible"><span style="font-family: 宋體;visibility: visible">三<span style="visibility: visible">. </span>寬帶光譜特性</span></p><p style="visibility: visible"><span style="font-family: 宋體;visibility: visible">1</span><span style="font-family: 宋體;visibility: visible">、光譜變窄：雖然<span style="visibility: visible">SLD</span>最初的自發(fā)發(fā)射譜與<span style="visibility: visible">LED</span>相同，但在增益過(guò)程中，靠近中心增益波長(cháng)的光子得到更大的放大，遠離中心增益波長(cháng)的光子得到的較小的放大，從而使光譜變窄。</span></p><p><span style="font-family:宋體">2</span><span style="font-family:宋體">、寬帶輸出：SLD的設計目標是產(chǎn)生寬帶光譜，通常通過(guò)優(yōu)化器件結構和材料來(lái)實(shí)現。例如，通過(guò)調整活性區的材料和結構，可以控制光子的發(fā)射和放大過(guò)程，從而獲得較寬的光譜。</span></p><p><span style="font-family:宋體">四. 低相干性</span></p><p><span style="font-family:宋體">SLD</span><span style="font-family:宋體">的光譜寬度較寬，相干長(cháng)度較短。這意味著(zhù)在相干長(cháng)度內，隨著(zhù)參考光與信號光光程差的變化，系統得到的干涉條紋的對比度會(huì )產(chǎn)生較大的變化，而在相干長(cháng)度之外時(shí)，不會(huì )發(fā)生干涉。這一特性使得SLD在光纖陀螺儀（FOG）、光學(xué)相干層析術(shù)（OCT）等應用中具有優(yōu)勢。</span></p><p><span style="font-family:宋體">五. 高輸出功率</span></p><p><span style="font-family:宋體">1</span><span style="font-family:宋體">、高功率輸出：SLD通過(guò)高電流密度注入，使得增益介質(zhì)中的激發(fā)密度很高，從而實(shí)現較高的輸出功率。SLD的輸出功率通常比LED高，但比LD低。</span></p><p><span style="font-family:宋體">2</span><span style="font-family:宋體">、光纖耦合效率：SLD的光纖耦合效率比LED高，這使得SLD在光纖傳感器和光纖通信等應用中具有更好的性能。</span></p><p><span style="font-family:宋體">六. 結構設計</span></p><p><span style="font-family:宋體">1</span><span style="font-family:宋體">、抗反射膜：為了減少腔面反射，SLD的腔面通常鍍有抗反射膜，以抑制法布里－珀羅模式下的振蕩，從而獲得更平滑的光譜。</span></p><p><span style="font-family:宋體">2</span><span style="font-family:宋體">、非泵浦吸收區：在一些設計中，SLD腔面后面引入非泵浦吸收區，以進(jìn)一步減少反射，提高光譜的平滑度。</span></p><p><span style="font-family:宋體">七. 驅動(dòng)電路設計</span></p><p><span style="font-family:宋體">1</span><span style="font-family:宋體">、恒流驅動(dòng)：SLD的驅動(dòng)電路通常采用恒流驅動(dòng)，以確保穩定的電流注入，從而保證穩定的光輸出。</span></p><p><span style="font-family:宋體">2</span><span style="font-family:宋體">、溫度控制：SLD的性能會(huì )受到溫度的影響，因此通常配備有溫度控制電路，如半導體制冷器（TEC），以保持器件在穩定的溫度下工作。</span></p><p><span style="font-family:宋體">八. 應用領(lǐng)域</span></p><p><span style="font-family:宋體">1</span><span style="font-family:宋體">、光纖陀螺儀（FOG）：SLD的寬光譜和低相干性使其成為光纖陀螺儀的理想光源，能夠有效減少瑞利散射噪聲，提高測量精度。</span></p><p><span style="font-family:宋體">2</span><span style="font-family:宋體">、光學(xué)相干層析術(shù)（OCT）：SLD的寬帶光譜和短相干長(cháng)度使其在OCT系統中具有高定位精度，能夠靈敏地檢測光程差的變化。</span></p><p><span style="font-family:宋體">3</span><span style="font-family:宋體">、波分復用（WDM）：SLD的高輸出功率和寬光譜特性使其能夠用于波分復用技術(shù)，實(shí)現單一光源的多波長(cháng)輸出。<br/></span></p><p style="margin-bottom: 0px">廈門(mén)亨光芯睿的SLD超輻射光源產(chǎn)品，是國內較早實(shí)現完全自主可控的SLD產(chǎn)品，具有設計結構精巧、性能優(yōu)越、長(cháng)期穩定性好的特征，支持了國家重大項目的建設和發(fā)展。近年進(jìn)入民用市場(chǎng)，是國產(chǎn)替代的最佳選擇之一！</p><p><br/></p> </div> </div> <div id="6eqb8tr3fa" class="news-others"> <div id="6eqb8tr3fa" class="pre-next"> <div id="6eqb8tr3fa" class="news-prev"> prev： <a href="http://www.jiawuxl.com/news/item/43957.html" title="光芯所至，睿見(jiàn)未來(lái)！——亨光芯睿首秀深圳CIOE2025，邀您共鑒自主光子芯片硬實(shí)力">光芯所至，睿見(jiàn)未來(lái)！——亨光芯睿首秀深圳CIOE2025，邀您共鑒自主光子芯片硬實(shí)力</a> </div> <div id="6eqb8tr3fa" class="news-next"> next： <a href="http://www.jiawuxl.com/new.html" title="窄譜超輻射SLD系列半導體光源的優(yōu)勢和應用領(lǐng)域">窄譜超輻射SLD系列半導體光源的優(yōu)勢和應用領(lǐng)域</a> </div> </div> <div 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