200829950 九、發明說明： 【發明所屬之技術領域】 本發明係與光學採集系統有關，特別係指一種太陽能 光學採集系統。 "b 5【先前技術】 按，時下能源緊缺已成為全球性問題，據專家估算， 以目前能源的使用需要，在地球上現有的能源如煤、天然 氣等僅夠50年左右的使用量，開發使用地球之外能源，如 將太陽能有效的利用轉化為可支配能源，是現在各行各業 10專家正在攻克的難題。 【發明内容】 本發明的目的在於提供一種利用光學系統對太陽能進 行採集的太陽能光學採集系統。 15 為實現上述目的，本發明的解決方案是：一種太陽能 光學採集系統，其是在光路中設有一球面反射鏡，球面反 射鏡上塗覆有反射膜；另在球面反射鏡的反射光路中設有 一光能收集器構成一光學系統。 在光學系統最前方進一步設有一非球面校正透鏡。 20 所述的非球面校正透鏡上塗覆有增透膜。 光能收集器是設在球面反射鏡的前方。 所述的球面反射鏡前方設有一與光轴呈45度放置的平 面反射板，位於此平面反射板的下方光路之外設有光能收 集器。 4 200829950 種太陽此光學採集系統，其是在光路中設有一非球 面反射鏡’非球面反射鏡上塗覆有反射膜；另在非球面反 射鏡的反射光路中設有一光能收集器構成一光學系統。 在光學系統最前方進一步設有一非球面校正透鏡。 5 所述的非球面校正透鏡上塗覆有增透膜。 光肖b收集裔是設在球面反射鏡的前方。 所述的非球面反射鏡前方設有一與光軸呈45度放置的 平面反射板，位於此平面反射板的下方光路之外設有光能 收集器。 10 種太〶能光學採集系統，其是在光路中設有兩反射 面相對的球面反射鏡，兩球面反射鏡上塗覆有反射膜；其 中小球面反射鏡位於球面反射鏡的前方，而在球面反射鏡 中心e又有供小球面反射鏡反射光線通過的通孔，在球面反 射鏡反射面的後方相對通孔的位置設有光能收集器以構成 15 一光學系統。 在光學系統最前方光路中設有一非球面校正透鏡。 所述非球面校正透鏡上塗覆有增透膜。 一種太陽能光學採集系統，其是在光路中設有兩反射 面相對的非球面反射鏡，兩非球面反射鏡上塗覆有反射 2〇 膜，其中小非球面反射鏡位於非球面反射鏡光路的前方， 而在非球面反射鏡中心設有供小非球面反射鏡反射光線通 過的通孔，在非球面反射鏡反射面的後方相對通孔的位置 設有光能收集器以構成一光學系統。 在光學系統最前方光路中設有一非球面校正透鏡。 5 200829950 所述非球面校正透鏡上塗覆有增透膜。200829950 IX. INSTRUCTIONS: TECHNICAL FIELD OF THE INVENTION The present invention relates to optical acquisition systems, and more particularly to a solar optical acquisition system. "b 5[Previous technology] According to the current energy shortage, it has become a global problem. According to experts' estimates, the current energy sources such as coal and natural gas on the earth are only about 50 years old. The development and use of energy outside the Earth, such as the efficient use of solar energy into disposable energy, is now a problem that 10 experts in all walks of life are conquering. SUMMARY OF THE INVENTION It is an object of the present invention to provide a solar optical acquisition system that utilizes an optical system for collecting solar energy. In order to achieve the above object, the solution of the present invention is: a solar optical acquisition system, which is provided with a spherical mirror in the optical path, the spherical mirror is coated with a reflective film; and another is provided in the reflected light path of the spherical mirror. The light energy collector constitutes an optical system. Further, an aspheric correction lens is provided at the forefront of the optical system. The aspheric correction lens of 20 is coated with an anti-reflection film. The light energy collector is placed in front of the spherical mirror. A spherical reflecting plate placed at an angle of 45 degrees with respect to the optical axis is disposed in front of the spherical mirror, and a light energy collector is disposed outside the optical path below the planar reflecting plate. 4 200829950 This kind of optical acquisition system is equipped with an aspherical mirror in the optical path. The aspherical mirror is coated with a reflective film. In addition, a light energy collector is arranged in the reflected light path of the aspherical mirror to form an optical system. Further, an aspheric correction lens is provided at the forefront of the optical system. 5 The aspheric correction lens is coated with an anti-reflection film. Light Xiao b collection is located in front of the spherical mirror. A plane reflector disposed at 45 degrees to the optical axis is disposed in front of the aspherical mirror, and a light energy collector is disposed outside the optical path below the planar reflector. 10 solar energy optical acquisition systems are provided with spherical mirrors opposite to each other in the optical path, and the two spherical mirrors are coated with a reflective film; wherein the spherical mirror is located in front of the spherical mirror and on the spherical surface The mirror center e has a through hole for the small spherical mirror to reflect the light, and a light energy collector is disposed at a position opposite to the through hole at the rear of the reflecting surface of the spherical mirror to constitute an optical system. An aspheric correction lens is provided in the optical path at the forefront of the optical system. The aspheric correction lens is coated with an anti-reflection film. A solar optical acquisition system is provided with an aspherical mirror opposite to two reflecting surfaces in the optical path, and the two aspherical mirrors are coated with a reflective 2〇 film, wherein the small aspherical mirror is located in front of the aspherical mirror optical path A through hole for reflecting light passing through the small aspherical mirror is disposed at the center of the aspherical mirror, and a light energy collector is disposed at a position opposite to the through hole at the rear of the reflecting surface of the aspherical mirror to constitute an optical system. An aspheric correction lens is provided in the optical path at the forefront of the optical system. 5 200829950 The aspheric correction lens is coated with an anti-reflection coating.
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一種太陽能光學採集系統，其是在光路中設有兩反身士 面相對的球面和非球面反射鏡，兩球面和非球面反射於上 塗覆有反射膜；其中小球面或小非球面反射鏡位於非球面 或球面反射鏡光路的前方，而在非球面或球面反射鏡中心 設有供小球面或小非球面反射鏡反射光線通過的通孔，在 非球面或球面反射鏡反射面的後方相對通孔的位置設有光 能收集器以構成一光學系統。 在光學系統最前方光路中設有一非球面校正透鏡。 所述非球面校正透鏡上塗覆有增透膜。 採用上述方案後，由於本發明在太陽光的光路中設有 由球面或非球面反射鏡配合光能收集器組合而成的光學採 集系統，則太陽光光能可以通過球面或非球面反射鏡將光 點有效的集中在光能收集器上實現光能收集的功能，同時 在球面或非球面反射鏡上塗鍍有反射膜，該鍍膜可以將太 陽光中有用的部份反射至光能收集器，而無用有害的部分 (如紫外線波長400納米以下）全部吸收掉，進而將其轉 化為可利用能源。 20【實施方式】 為能更詳細說明本發明之特徵，茲舉本發明較佳之實 施例並配合圖式說明如下；其中： 在陳述具體實施例之前，需要說明光學設計中的幾個 參數概念： 6 200829950 像差.指在光學系統中由透鏡材料的特性或折射（或 反射）表面的幾何形狀引起實際像與理想像的偏差。理想 像是由理想光學系統所成的像。實際的光學系統，須有一 定大小的成像空間和光束孔徑，同時還由於成像光束多是 5由不同波長的光組成的，闾一介質的折射率隨波長而異。 因此η際光學系統的成像具有一系列的缺陷，這就是像 差。像差的大小反映了光學系統品質的優劣。 球差：由軸上點發出的同心光束，經光學系統各個折 射面折射後，不同孔徑角的光線交光軸於不同點上，相對 10於理想象點的位置有不同的偏離，這就是球面像差，簡稱 球差。其值由軸上點發出的不同孔徑角的光線經系統後的 象方截距和其近軸光像方截距之差表示。球差越小，能量 的均勻度越好，在一個晶片上，光點均勻地分佈其上，有 利於能量的收集。 15 色差·光學系統大多是白光成像。白光是各種不同波 長（顏色）的早色光組成的。光學材料對不同波長的色光 折射率不同，白光比光學系統第一表面折射後，各種色光 被分開，在光學系統内以各自的光路傳播，造成各色光之 間成像位置和大小的差異，在像面上形成彩色的彌散圓。 2〇複色光成像時，由不同色光而引起的像差稱為色差。色差 越小’能量收集越佳。 點列圖：光學設計必須校正光學系統的像差，但既不 可能無必要把像差校正到完全理想的程度，因此需要選擇 像差的最佳校正方案，也需要確定校正到怎樣的程度才能 7 200829950 滿足使用要求，即確定像差容限。 由一點發出的許多光線經光學系統後，因像差使其與 ，面的交點不再集中於同一點，而形成了一個散佈在二/定 範圍的彌散圖形，稱為點列圖。用點列圖中點的密集程度 5可以衡量系統成像品質的優劣。點的集中性高、密度高時， 聚能效果更好。 τ 實施例一： 如第一圖至第三圖所示，本發明的太陽能光學採集結 構，其主要包括球面反射鏡1 (或非球面反射鏡丨，）及光 10能收集器3，在球面反射鏡1 (或非球面反射鏡丨，）上汾 鍍有反射膜，該膜可以將太陽光中有用的部份反射至光^ 收集器3，而無用有害的部分（如紫外線波長4〇〇納米以 全部吸收掉。球面反射鏡1(或非球面反射鏡〗，）是置於 太陽光光路中，而光能收集器3是置於球面反射鏡丨（或非 I1 2 3 4球面反射鏡1 )的前方的光軸上以構成一光學系統。 如此結構的光學系統，其形成的色差為0,而最大球差 為2·46，見第二圖所示為色差與球差形成的曲線圖；如第 三圖所示為此光學系統形成的點列圖。 8 1 〇 實施例二： 2 如第四圖至第六圖所示，太陽能光學採集結構，其主 3 要包括球面反射鏡1、光能收集器3及非球面校正透鏡4， 4 在球面反射鏡1上塗鍍有反射膜，球面反射鏡i是置於太 陽光光路中，而光能收集器3是置於球面反射鏡丨的前方 200829950 的光轴上崎成—光學祕，在光學系統最前方再加設有 非球面权正透鏡4’非球面校正透鏡4上塗覆有增透膜。 如此結構的光學系統，其形成的色差為⑽3，而最大 求差為_ A第五圖所示為色差與球差形成的曲線圖； 六圖所示為此光學系統形成的點列圖。 實施例三： 如第七圖至第九圖所示，太陽能光學採集結構，其主 要包括非球面反射鏡Γ 、光能收集器3及非球面校正透鏡 1〇 1，在非球面反賊Γ i塗鑛有反射膜，非球面反射鏡广 是置於太，光光路中，而光能收集器3是置於非球面反射 鏡1的别方的光軸上以構成一光學系統，在光學系統最前 方再加設有非球面校正透鏡4,非球面校正透鏡4上塗覆有 增透膜。 15 如此結構的光學系統，其形成的色差為-0.048，而最大 球差為0.026,見第八圖所示為色差與球差形成的曲線圖；. 如第九圖所示為此光學系統形成的點列圖。 實施例四： 2〇 如第十圖至第十一圖所示，本發明的太陽能光學採集 2構，其主要包括球面反射鏡i、平面反光板5及光能收集 器3，在球面反射鏡1及平面反光板5上塗鍍有反射膜，該 反射膜可以將太陽光中有用的部份反射至光能收集器3,而 無用有害的部分（如紫外線波長4〇0納米以下）全部吸收 9 200829950 掉。球面反射鏡1是置於太陽光光路中，平面反光板5與 光軸呈45度放置於球面反射鏡1的前方的光轴上，而光能 收集器3是置於平面反光板5下方的光路之外。 如此結構的光學系統，其形成的色差為〇,而最大球差 為-1.98，見第十一圖所示為色差與球差形成的曲線圖；如 第十二圖所示為此光學系統形成的點列圖。 實施例五： 如第十三圖至第十五圖所示，本發明的太陽能光學採 1〇集結構’其主要包括非球面反射鏡Γ 、平面反光板5及光 月匕收集裔3，在非球面反射鏡1’及平面反光板5上塗鍵 有反射膜，該反射膜可以將太陽光中有用的部份反射至光 月匕收集裔3 ’而無用有害的部分（如紫外線波長4〇〇納米以 1下）全部吸收掉。非球面反射鏡1，是置於太陽光光路中， 15平面反光板5與光軸呈45度放置於非球面反射鏡丨，的前 方的光軸上，而光能收集器3是置於平面反光板5下方的 光路之外。 、如此結構的光學系統，其形成的色差為〇,而最大球差 2，〇·567 ’見第十四圖所示為色差與球差形成的曲線圖；如 第十五圖所不為此光學系統形成的點列圖。 貫施例六： 如第十六圖至第十八圖所示，太陽能光學採集結構， 其主要包括非球面反射鏡1，、平面反光板5、光能收集器 200829950 3及非球面校正錢4，在_岐㈣1，及平面反光板 5上塗錄有反⑽，㈣面反概丨，是置於太陽光光路 中二平面反光板5與光軸呈45度放置於非球面反射鏡Γ 的刚方的光幸由上，而光能收集器3是置於平面反光板5下 5方的光路之外，另平面反光板5的反光面後方的光路中設 有一非球面校正透鏡4，非球面校正透鏡4上塗覆有增透 膜。 如此結構的光學系統，其形成的色差為 0.03，而最大 球爰為=·07，見第十七圖所示為色差與球差形成的曲線 ίο圖，如第十八圖所示為此光學系統形成的點列圖。 實施例七： 如第十九圖至第二十一圖所示，太陽能光學採集結 構，其主要包括球面反射鏡丨、平面反光板5、光能收集器 I5 3及非球面校正透鏡4，在球面反射鏡及平面反光板5上塗 鑛有反射膜’球面反射鏡是置於太陽光光路中，平面反光 板5與光軸呈45度放置於球面反射鏡1的前方的光軸上， 而光能收集器3是置於平面反光板5下方的光路之外，另 平面反光板5的反光面後方的光路中設有一非球面校正透 2〇鏡4，非球面校正透鏡4上塗覆有增透膜。 如此結構的光學系統，其形成的色差為0.03，而最大 球差為-0.11 ’見第二十圖所示為色差與球差形成的曲線 圖；如第二十一圖所示為此光學系統形成的點列圖。 11 200829950 實施例八： >如第一十一圖至第二十四圖所示，本發明太陽能光學 採集裝置’其主要包括球面反射鏡i、小球面反射鏡2及光 忐收集益3’在球面反射鏡1及小球面反射鏡2上均塗鍍有 5反射膜，該反射膜可以將太陽光中有用的部份反射至光能 收集裔3’而無用有害的部分（如紫外線波長4〇〇納米以下） 全部吸收掉。大、小球面反射鏡卜2是置於太陽光光路中， 小球面反射鏡2是置於球面反射鏡丨的前方，而在球面反 射鏡1中心设有供小球面反射鏡2反射光線通過的通孔 1〇 11，在球面反射鏡1反射面的後方相對通孔的位置設有光 能收集器3以構成一光學系統。 如此結構的光學系統，其形成的色差為-〇,而最大球差 為-1〇·83，見第二十三圖所示為色差與球差形成的曲線圖； 如第二十四圖所示為此光學系統形成的點列圖。 15 實施例九： 如第二十五圖至第二十七圖所示，本發明的太陽能光 學採集裝置’其主要包括非球面反射鏡丨，、小球面反射鏡 2及光能收集器3 ’在非球面反射鏡〗，及小球面反射鏡2 2〇上均塗鍍有反射膜，該反射膜可以將太陽光中有用的部份 反射至光能收集器3，而無用有害的部分（如紫外線波長 400納米以下）全部吸收掉。非球面反射鏡丨，、小球面反 射鏡2疋置於太光光路中，小球面反射鏡2是置於非球 面反射鏡Γ前方，而在非球面反射鏡1，中心設有供小球 12 200829950 面反射鏡2反射光線通過的通孔ii，，在非球面反射鏡^ 反射面的後方相對通孔11，的位置設有光能收集器3以構 成一光學系統。 如此結構的光學系統，其形成的色差為-〇,而最大球差 5為-3·ι〇，見苐一十六圖所示為色差與球差形成的曲線圖； • 如第二十七圖所示為此光學系統形成的點列圖。 _ 實施例十·· 如第二十八圖至第三十圖所示，本發明的太陽能光學 10採集裝置，其主要包括球面反射鏡i、小球面反射鏡2、光 能收集器3及非球面校正透鏡4,在球面反射鏡i及小球面 反射鏡2上均塗鍍有反射膜，該反射膜可以將太陽光中有 用的部份反射至光能收集器3。大小球面反射鏡1、2是置 於太陽光光路中，小球面反射鏡2是置於球面反射鏡i前 15方，而在球面反射鏡1中心設有供小球面反射鏡2反射光 ❿ 線通過的通孔11，在球面反射鏡1反射面的後方相對通孔 • ，位置設有光能收集器3以構成一光學系統。在光學系統 最前方光路中設有一非球面校正透鏡4，非球面校正透鏡4 上塗覆有增透膜。 20 ,如此結構的光學系統，其形成的色差為-0.18，而最大 球差為-0·52，見第二十九圖所示為色差與球差形成的曲線 圖，如第二十圖所示為此光學系統形成的點列圖。 實施例十一： 13 200829950 如第三十-圖至第三十三圖所示，本發明的太陽能光 學採集裝置，其主要包括_面反射鏡2，、小球面反射鏡 2、光忐收集器3及非球面校正透鏡4,在非球面反射鏡γ 及小球面反射鏡2上均塗鍍有反射膜。非球面反射鏡丨，及 5小球面反射鏡2是置於太陽光光路中，小球面反射鏡2是 置於非球面反射鏡1，前方，而在非球面反射鏡1，中心設 有供小球面反射鏡2反射光線通過的通孔n，，在非球面 反^鏡1，反射面的後方相對通孔U，的位置設有光能收 集器3以構成一光學系統。在光學系統最前方光路中設有 1〇 一非球面校正透鏡4，非球面校正透鏡4上塗覆有增透膜。 ,如此結構的光學系統，其形成的色差為_〇·22而最大 球差為^.038’ I第二十二圖所示為色差與球差形成的曲線 圖，如第二十三圖所示為此光學系統形成的點列圖。 15 實施例十二： ^如第二十四圖至第三十六圖所示，本發明的太陽能光 學採集裝置’其主要包括非球面反射鏡丨，、小非球面反射 鏡f 、光能收集器3及非球面校正透鏡4,在非球面反射 鏡1’及小非球面反射鏡2，上均塗鍍有反射膜。大小非球 2〇面反射鏡Γ、2,是置於太陽光光路中，小非球面反射鏡 2’是置於非球面反射鏡〗，前方，而在非球面反射鏡工， 中心設有供小非球面反射鏡2，反射光線通過的通孔 11’ ，在非球面反射鏡1，反射面的後方相對通孔η，的 位置設有光能收集器3以構成一光學系統。另在光學系統 14 200829950 最前方光路中設有一非球面校正透鏡4，非球面校正透鏡4 上塗覆有增透膜。 如此結構的光學系統，其形成的色差為-0.12，而最大 球差為-0.029,見第三十五圖所示為色差與球差形成的曲線 5圖；如第三十六圖所示為此光學系統形成的點列圖。 15 200829950 【圖式簡單說明】 第一圖是本發明實施例一的結構示意圖（光路圖）； 第二圖是本發明實施例一的色差與球差曲線圖； 第三圖是本發明實施例一的點列圖； 5 第四圖是本發明實施例一的結構示意圖（光路圖）； 第五圖是本發明實施例二的色差與球差曲線圖； 第六圖是本發明實施例二的點列圖； 第七圖是本發明實施例三的結構示意圖（光路圖）； 第八圖是本發明實施例三的色差與球差曲線圖； 10 第九圖是本發明實施例三的點列圖。 第十圖是本發明實施例四的結構示意圖（光路圖）; 第十一圖是本發明實施例四的色差與球差曲線圖； 第十二圖是本發明實施例四的點列圖； 第十三圖是本發明實施例五的結構示意圖（光路圖）； 15 第十四圖是本發明實施例五的色差與球差曲線圖； 第十五圖是本發明實施例五的點列圖； 第十六圖是本發明實施例六的結構示意圖（光路圖）； 第十七圖是本發明實施例六的色差與球差曲線圖； 第十八圖是本發明實施例六的點列圖； 20 第十九圖是本發明實施例七的的結構示意圖（光路 圖）； 第二十圖是本發明實施例七的色差與球差曲線圖； 第二十一圖是本發明實施例七的點列圖。 第二十二圖是本發明實施例八的結構示意圖（光路 16 200829950 圖）， 第二十三圖是本發明實施例八的色差與球差曲線圖； 第二十四圖是本發明實施例八的點列圖； 第二十五圖是本發明實施例九的結構示意圖（光路 5圖）， 第二十六圖是本發明實施例九的色差與球差曲線圖； 第二十七圖是本發明實施例九的點列圖； 第二十八圖是本發明實施例十的結構示意圖（光路 圖）， 10 第二十九圖是本發明實施例十的色差與球差曲線圖； .第三十圖是本發明實施例十的點列圖； 第三十一圖是本發明實施例十一的的結構示意圖（光 路圖）； 第三十二圖是本發明實施例十一的色差與球差曲線 15 圖； 第三十三圖是本發明實施例十一的點列圖； 第三十四圖是本發明實施例十二的的結構示意圖（光 路圖）； 第三十五圖是本發明實施例十二的色差與球差曲線 20 圖； 第三十六圖是本發明實施例十二的點列圖。 17 200829950 【主要元件符號說明】 球面反射鏡1 非球面反射鏡r 光能收集器3 非球面校正透鏡4 平面反光板5 小球面反射鏡2 5 小非球面反射鏡2’ 通孔11 通孔11’A solar optical acquisition system is provided with two spherical and aspheric mirrors opposite to each other in the optical path, and the two spherical surfaces and the aspherical surface are coated with a reflective film; wherein the spherical surface or the small aspherical mirror is located at a non-spherical surface The front of the spherical or spherical mirror light path, and the center of the aspherical or spherical mirror is provided with a through hole for the small spherical surface or the small aspherical mirror to reflect the light, and the opposite side of the aspherical or spherical mirror reflecting surface The position is provided with a light energy collector to constitute an optical system. An aspheric correction lens is provided in the optical path at the forefront of the optical system. The aspheric correction lens is coated with an anti-reflection film. After adopting the above scheme, since the present invention is provided with an optical collecting system composed of a spherical or aspherical mirror combined with a light energy collector in the optical path of the sunlight, the solar light energy can be passed through a spherical or aspherical mirror. The light spot effectively concentrates on the light energy collector to realize the function of light energy collection, and the spherical or aspherical mirror is coated with a reflective film, which can reflect the useful part of the sunlight to the light energy collector. The useless and harmful parts (such as ultraviolet wavelengths below 400 nm) are all absorbed and converted into usable energy. [Embodiment] In order to explain the features of the present invention in more detail, the preferred embodiments of the present invention are described below with reference to the accompanying drawings; wherein: Before describing a specific embodiment, several parameter concepts in optical design need to be explained: 6 200829950 Aberration. Refers to the deviation of the actual image from the ideal image caused by the characteristic of the lens material or the geometry of the refractive (or reflective) surface in the optical system. The ideal is like an image made of an ideal optical system. The actual optical system must have a certain size of imaging space and beam aperture, and also because the imaging beam is mostly composed of different wavelengths of light, and the refractive index of the medium varies with wavelength. Therefore, the imaging of the η optical system has a series of defects, which is the aberration. The size of the aberration reflects the quality of the optical system. Spherical aberration: Concentric beam emitted by the point on the axis, after being refracted by the respective refractive surfaces of the optical system, the ray of different aperture angles is at different points, and the position of 10 is different from the position of the ideal image point. This is the spherical surface. Aberration, referred to as spherical aberration. The value of the light at different aperture angles from the point on the axis is represented by the difference between the image's image intercept and its paraxial image intercept. The smaller the spherical aberration, the better the uniformity of energy. On a wafer, the spot is evenly distributed, which is beneficial to the collection of energy. 15 Chromatic aberration · Optical systems are mostly white light imaging. White light is composed of early colors of various wavelengths (colors). The optical material has different refractive indices for different wavelengths of light, and after the white light is refracted than the first surface of the optical system, the various colored lights are separated and propagated in respective optical paths in the optical system, resulting in a difference in imaging position and size between the respective colored lights. A colored circle of circles is formed on the surface. In the case of 2 〇 complex light imaging, aberrations caused by different color lights are called chromatic aberrations. The smaller the color difference, the better the energy collection. Point map: The optical design must correct the aberration of the optical system, but it is impossible to correct the aberration to a completely ideal degree. Therefore, it is necessary to select the optimal correction scheme for the aberration, and also to determine the degree of correction. 7 200829950 Meet the usage requirements, that is, determine the aberration tolerance. After a large amount of light emitted from one point passes through the optical system, the intersection of the faces and the faces are no longer concentrated at the same point due to the aberrations, and a diffused pattern scattered in the second/fixed range is formed, which is called a dot-column map. Use the intensity of the points in the dot plot to measure the quality of the system's imaging quality. When the concentration of the dots is high and the density is high, the energy gathering effect is better. τ Embodiment 1: As shown in the first to third figures, the solar optical acquisition structure of the present invention mainly comprises a spherical mirror 1 (or an aspheric mirror 丨,) and a light 10 energy collector 3, on a spherical surface. The mirror 1 (or aspherical mirror 丨,) is coated with a reflective film that reflects the useful part of the sunlight to the light collector 3, with no harmful parts (such as UV wavelength 4〇〇). The nanometer is completely absorbed. The spherical mirror 1 (or aspheric mirror) is placed in the solar light path, and the light energy collector 3 is placed in the spherical mirror 丨 (or non-I1 2 3 4 spherical mirror) 1) on the optical axis in front to form an optical system. The optical system thus constructed has a chromatic aberration of 0 and a maximum spherical aberration of 2.46, as shown in the second figure, which is a curve formed by chromatic aberration and spherical aberration. Figure; a dot plot formed for this optical system as shown in Figure 3. 8 1 〇 Example 2: 2 As shown in Figures 4 through 6, the solar optical acquisition structure, the main 3 of which includes a spherical mirror 1. The light energy collector 3 and the aspheric correction lens 4, 4 are inversely spherical. The mirror 1 is coated with a reflective film, the spherical mirror i is placed in the solar light path, and the light energy collector 3 is placed on the optical axis of the front of the spherical mirror 2008 200829950 - optical secret, the most optical system An aspherical positive lens is attached to the front. The 4' aspherical correction lens 4 is coated with an antireflection film. The optical system thus constructed has a chromatic aberration of (10)3 and a maximum difference of _A. A graph of chromatic aberration and spherical aberration; Figure 6 shows a dot plot formed for this optical system. Embodiment 3: As shown in the seventh to ninth, solar optical acquisition structure, which mainly includes an aspheric mirror Γ, the light energy collector 3 and the aspherical correction lens 1〇1, the aspherical anti-thief Γ i coated with a reflective film, the aspherical mirror is widely placed in the light path, and the light energy collector 3 is The optical axis of the other side of the aspherical mirror 1 is placed to form an optical system, and an aspherical correction lens 4 is further disposed at the forefront of the optical system, and the aspherical correction lens 4 is coated with an anti-reflection film. Optical system, which produces a color difference of -0.048 The maximum spherical aberration is 0.026, as shown in the eighth figure, which is a graph of chromatic aberration and spherical aberration; a dot plot formed for this optical system as shown in Fig. 9. Embodiment 4: 2〇 As shown in FIG. 11 , the solar optical acquisition structure of the present invention mainly comprises a spherical mirror i, a planar reflector 5 and a light energy collector 3, and the spherical mirror 1 and the planar reflector 5 are coated with a reflection. a film that reflects a useful portion of the sunlight to the light energy collector 3, and the useless harmful portions (such as ultraviolet wavelengths below 4 〇 0 nm) are all absorbed 9 200829950. The spherical mirror 1 is placed In the solar light path, the plane reflecting plate 5 is placed at an angle of 45 degrees with respect to the optical axis on the optical axis in front of the spherical mirror 1, and the light energy collector 3 is disposed outside the optical path below the planar reflecting plate 5. The optical system thus constructed has a chromatic aberration of 〇 and a maximum spherical aberration of -1.98, as shown in Fig. 11 is a graph of chromatic aberration and spherical aberration; as shown in Fig. 12, the optical system is formed. Point map. Embodiment 5: As shown in the thirteenth to fifteenth drawings, the solar optical collection structure of the present invention mainly includes an aspherical mirror Γ, a planar reflector 5, and an optical moon collection 3, The aspherical mirror 1' and the planar reflector 5 are coated with a reflective film, which can reflect a useful part of the sunlight to the part of the light moon collecting 3' and useless (such as ultraviolet wavelength 4〇〇). Nano is absorbed by 1). The aspherical mirror 1 is placed in the solar light path, and the 15 plane reflector 5 is placed at 45 degrees with the optical axis on the optical axis in front of the aspherical mirror ,, and the light energy collector 3 is placed on the plane. Outside the light path below the reflector 5. The optical system thus structured has a chromatic aberration of 〇 and a maximum spherical aberration of 2, 〇·567 'see the graph of chromatic aberration and spherical aberration as shown in the fourteenth figure; A dot plot formed by the optical system. Example 6: As shown in Figures 16 to 18, the solar optical acquisition structure mainly includes an aspheric mirror 1, a plane reflector 5, a light energy collector 200829950 3, and an aspheric correction money 4 On the _岐(4)1, and the plane reflector 5, there is an anti-(10), (four) plane inverse 丨, which is placed in the solar light path, the two-plane reflector 5 and the optical axis are placed at 45 degrees on the aspheric mirror Γ The light is collected by the light, and the light energy collector 3 is disposed outside the optical path of the lower side of the plane reflector 5, and an aspheric correction lens 4 is disposed in the optical path behind the reflective surface of the planar reflector 5, and the aspheric correction is performed. The lens 4 is coated with an antireflection film. The optical system thus constructed has a chromatic aberration of 0.03 and a maximum spherical = of =·07, as shown in Fig. 17 is a curve formed by chromatic aberration and spherical aberration, as shown in Fig. 18 for this optical A point map formed by the system. Embodiment 7: As shown in the nineteenth to twenty-first embodiments, the solar optical collection structure mainly includes a spherical mirror 丨, a planar reflector 5, a light energy collector I53, and an aspheric correction lens 4, The spherical mirror and the planar reflector 5 are coated with a reflective film. The spherical mirror is placed in the solar light path, and the planar reflector 5 is placed at an angle of 45 degrees with respect to the optical axis in front of the spherical mirror 1, and the light is The energy collector 3 is disposed outside the optical path below the planar reflector 5, and an aspherical correction lens 2 is disposed in the optical path behind the reflective surface of the planar reflector 5, and the aspheric correction lens 4 is coated with an antireflection lens. membrane. The optical system thus structured has a chromatic aberration of 0.03 and a maximum spherical aberration of -0.11'. See the twentieth diagram for a graph of chromatic aberration and spherical aberration; as shown in Fig. 21, the optical system is shown. A dot map formed. 11 200829950 Embodiment 8: > As shown in the first to fourth figures, the solar optical collecting device of the present invention mainly includes a spherical mirror i, a spherical mirror 2, and a light collecting and collecting 3' The spherical mirror 1 and the spherical mirror 2 are coated with a five-reflection film, which can reflect a useful part of the sunlight to the light-collecting part of the light-collecting 3' (such as ultraviolet wavelength 4) 〇〇Nano below) All absorbed. The large and small spherical mirrors 2 are placed in the solar light path, the spherical mirror 2 is placed in front of the spherical mirror 丨, and the center of the spherical mirror 1 is provided for the small spherical mirror 2 to reflect the light. The through hole 1〇11 is provided with a light energy collector 3 at a position opposite to the through hole at the rear of the reflecting surface of the spherical mirror 1 to constitute an optical system. The optical system thus constructed has a chromatic aberration of -〇 and a maximum spherical aberration of -1 〇 83, as shown in the twenty-third figure, which is a graph of chromatic aberration and spherical aberration; A dot plot formed for this optical system is shown. 15 Embodiment 9: As shown in the twenty-fifth to twenty-seventh drawings, the solar optical collecting device of the present invention mainly includes an aspherical mirror 丨, a spherical spherical mirror 2, and a light energy collector 3' The aspherical mirror and the spherical mirror 2 2 are coated with a reflective film, which can reflect a useful part of the sunlight to the light energy collector 3, and use no harmful parts (such as All of the ultraviolet wavelengths below 400 nm are absorbed. The aspherical mirror 丨, the small spherical mirror 2 疋 is placed in the solar light path, the small spherical mirror 2 is placed in front of the aspherical mirror ,, and in the aspherical mirror 1 , the center is provided with the small ball 12 200829950 The face mirror 2 reflects the through hole ii through which the light passes, and the light energy collector 3 is disposed at a position opposite to the through hole 11 at the rear of the aspherical mirror surface to constitute an optical system. The optical system thus constructed has a chromatic aberration of -〇 and a maximum spherical aberration of 5 -3·ι〇, as shown in the figure of 苐16, which is a graph of chromatic aberration and spherical aberration; The figure shows a dot plot formed for this optical system. _ Embodiment 10· As shown in the twenty-eighth to thirtieth drawings, the solar optical 10 collecting device of the present invention mainly comprises a spherical mirror i, a spherical mirror 2, a light energy collector 3 and a non- The spherical correcting lens 4 is coated with a reflecting film on the spherical mirror i and the spherical mirror 2, and the reflecting film can reflect a useful portion of the sunlight to the light energy collector 3. The spherical mirrors 1 and 2 are placed in the solar light path, the spherical mirror 2 is placed in front of the spherical mirror i, and the center of the spherical mirror 1 is provided with a spherical mirror 2 for reflecting the light. The through hole 11 passing through is opposite to the through hole at the rear of the reflecting surface of the spherical mirror 1, and the light energy collector 3 is disposed at a position to constitute an optical system. An aspherical correction lens 4 is disposed in the forefront optical path of the optical system, and the aspherical correction lens 4 is coated with an anti-reflection film. 20 , the optical system of such a structure, the color difference formed is -0.18, and the maximum spherical aberration is -0.52, as shown in the twenty-ninth figure is a graph formed by the color difference and the spherical aberration, as shown in the twentieth figure. A dot plot formed for this optical system is shown. Embodiment 11: 13 200829950 As shown in the thirtieth to thirteenth thirteenth, the solar optical collecting device of the present invention mainly comprises a mirror Mirror 2, a spherical mirror 2, and a pupil collector. 3 and the aspheric correction lens 4 are coated with a reflection film on both the aspherical mirror γ and the spherical mirror 2 . The aspherical mirror 丨, and the 5 small spherical mirror 2 are placed in the solar light path, the small spherical mirror 2 is placed in front of the aspherical mirror 1, and the aspherical mirror 1 is provided at the center for small The spherical mirror 2 reflects the through hole n through which the light passes, and the optical energy collector 3 is disposed at a position opposite to the through hole U at the rear of the aspherical mirror 1 to constitute an optical system. An aspherical correction lens 4 is disposed in the optical path of the forefront of the optical system, and an aspherical correction lens 4 is coated with an anti-reflection film. The optical system thus structured has a chromatic aberration of _〇·22 and a maximum spherical aberration of ^.038'. The twenty-second graph shows a graph of chromatic aberration and spherical aberration, as shown in the twenty-third diagram. A dot plot formed for this optical system is shown. 15 Embodiment 12: ^ As shown in the twenty-fourth to thirty-sixth drawings, the solar optical collecting device of the present invention mainly includes an aspherical mirror 丨, a small aspherical mirror f, and light energy collection. The aspherical mirror 3 and the aspherical correction lens 4 are coated with a reflective film on both the aspherical mirror 1' and the small aspherical mirror 2. The size of the aspherical 2 〇 mirror Γ, 2, is placed in the solar light path, the small aspherical mirror 2' is placed in the aspherical mirror, in front, and in the aspheric mirror, the center is provided The small aspherical mirror 2, the through hole 11' through which the reflected light passes, is provided with a light energy collector 3 at a position opposite to the through hole η at the rear of the aspherical mirror 1 and the reflecting surface to constitute an optical system. In addition, an aspherical correction lens 4 is disposed in the forefront optical path of the optical system 14 200829950, and the aspheric correction lens 4 is coated with an anti-reflection film. The optical system thus structured has a chromatic aberration of -0.12 and a maximum spherical aberration of -0.029. See the graph of the chromatic aberration and the spherical aberration shown in the thirty-fifth figure; as shown in the thirty-sixth figure, A dot plot formed by this optical system. 15 200829950 [Simplified description of the drawings] The first figure is a schematic structural view (optical path diagram) of the first embodiment of the present invention; the second figure is a chromatic aberration and spherical aberration diagram of the first embodiment of the present invention; 5 is a schematic diagram of the structure of the first embodiment of the present invention (optical path diagram); the fifth diagram is a diagram of the chromatic aberration and spherical aberration of the second embodiment of the present invention; 7 is a schematic structural view (optical path diagram) of the third embodiment of the present invention; eighth is a chromatic aberration and spherical aberration diagram of the third embodiment of the present invention; 10 ninth is a third embodiment of the present invention Click on the map. 11 is a schematic structural view (optical path diagram) of Embodiment 4 of the present invention; FIG. 11 is a chromatic aberration and spherical aberration diagram of Embodiment 4 of the present invention; and FIG. 12 is a dot-column diagram of Embodiment 4 of the present invention; Figure 13 is a schematic structural view (optical path diagram) of the fifth embodiment of the present invention; 15th is a graph of chromatic aberration and spherical aberration according to the fifth embodiment of the present invention; and fifteenth diagram is a list of points according to the fifth embodiment of the present invention Figure 16 is a schematic structural view (optical path diagram) of the sixth embodiment of the present invention; the seventeenth embodiment is a chromatic aberration and spherical aberration diagram of the sixth embodiment of the present invention; and the eighteenth embodiment is the point of the sixth embodiment of the present invention. FIG. 19 is a schematic structural view (optical path diagram) of Embodiment 7 of the present invention; FIG. 20 is a chromatic aberration and spherical aberration diagram of Embodiment 7 of the present invention; The point chart of Example 7. Figure 22 is a schematic structural view of the eighth embodiment of the present invention (light path 16 200829950), and the twenty-third figure is a color difference and spherical aberration chart of the eighth embodiment of the present invention; Figure 28 is a schematic diagram of the structure of the ninth embodiment of the present invention (the optical path 5 is shown), and the twenty-sixth is a chromatic aberration and spherical aberration of the ninth embodiment of the present invention; It is a dot-column diagram of the ninth embodiment of the present invention; the twenty-eighthth embodiment is a schematic structural diagram (optical path diagram) of the tenth embodiment of the present invention, and the twenty-ninth aspect is a graph of chromatic aberration and spherical aberration of the tenth embodiment of the present invention; Figure 30 is a dot-column diagram of the tenth embodiment of the present invention; Figure 31 is a schematic structural view (optical road diagram) of the eleventh embodiment of the present invention; Chromatic aberration and spherical aberration curve 15; Figure 33 is a dot-column diagram of the eleventh embodiment of the present invention; and thirty-fourth is a schematic structural view (optical road diagram) of the twelfth embodiment of the present invention; Figure is a chromatic aberration and spherical aberration curve 20 of the twelfth embodiment of the present invention; FIG thirty-six embodiment of the present invention is a spot diagram twelve. 17 200829950 [Description of main components] Spherical mirror 1 Aspherical mirror r Light energy collector 3 Aspheric correction lens 4 Planar reflector 5 Spherical mirror 2 5 Small aspheric mirror 2' Through hole 11 Through hole 11 '
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