TW578022B - Collecting and condensing apparatus, system for collecting and condensing electromagnetic radiation, and optical device and method for folding electromagnetic radiation - Google Patents
Collecting and condensing apparatus, system for collecting and condensing electromagnetic radiation, and optical device and method for folding electromagnetic radiation Download PDFInfo
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578022 A7 ____B7 五、發明説明(1 ) liLt 景 相關申請齎照: 本申請專利範圍係優先於2000年1〇月26日建檔之臨時申 請專利編號60/243,280,該臨時申請專利係納於本發明以供 參考。 發明範圍: 本發明係關於藉反折一弧光於其本身以增加一弧光燈之 亮度。 相關技藝說明: 納於本發明以參考之美國專利編號09/604,921係披露一雙 拋物面反光器系統,該系統係可用於耦合一弧光燈之光於 一目標中,如一單一光纖或光纖束之標準波導管,或輸出 電磁輻射至一投影機之均化器。如圖1所示之該光學集合與 聚光系統係使用二大致對稱配置之拋物面反光器1 〇,1 1, 這樣,自該第一反光器1 〇反射之光係接收於該第二反光器 11之一對應段中。自一光源12,如一弧光燈,發射之光特 別係藉該第一拋物面反光器10集合及沿該光軸向該第二反 光器11準直。該第二反光器11係接收該準直光束及使光聚 焦於位在該聚焦點之目標13。 圖1所示之該光學系統係可以一向後反光器14與該第一拋 物面反光器10—同使用,以捕捉該光源12在該第一拋物面 反光器10之外一方向發射的輻射及向回反射該捕捉之輻射 使之通過該光源12。該向後反光器14特別係具有一大致呈 球形之形狀並具有一大致接近於該光源12 (即該第一拋物面 -4- 本紙張尺度適用中國國家標準(CNS) A4規格(210 X 297公釐) " ' -----578022 A7 ____B7 V. Description of the invention (1) liLt Scenery related application photos: The patent scope of this application is prior to the provisional application patent number 60 / 243,280 filed on October 26, 2000. This provisional application patent is incorporated in this Invented for reference. Scope of the invention: The present invention relates to increasing the brightness of an arc lamp by refracting an arc light on itself. Relevant technical description: US Patent No. 09 / 604,921, which is incorporated herein by reference, discloses a double parabolic reflector system that can be used to couple the light of an arc lamp to a target, such as a single optical fiber or a standard of optical fiber bundles A waveguide, or a homogenizer that outputs electromagnetic radiation to a projector. The optical collection and condensing system shown in FIG. 1 uses two parabolic reflectors 10, 11 which are arranged approximately symmetrically. In this way, the light reflected from the first reflector 10 is received by the second reflector. One of 11 corresponds to the segment. The light emitted from a light source 12, such as an arc lamp, is especially collected by the first parabolic reflector 10 and collimated along the optical axis of the second reflector 11. The second reflector 11 receives the collimated light beam and focuses the light on a target 13 located at the focal point. The optical system shown in FIG. 1 can be used with both the retro-reflector 14 and the first parabolic reflector 10 to capture the radiation emitted by the light source 12 in a direction outside the first parabolic reflector 10 and back. The captured radiation is reflected and passed through the light source 12. The backward reflector 14 has a substantially spherical shape and has a shape substantially close to the light source 12 (i.e., the first parabolic surface -4- This paper size applies to the Chinese National Standard (CNS) A4 specification (210 X 297 mm) ) " '-----
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線 578022 A7 B7 五、發明説明(2 反光器之聚焦點處)之焦點朝向該第一拋物面反光器,因而 增加自該處反射之準直輻射線的強度。 納於本發明以參考之美國專利編號〇9/669,841,係披露一 雙抱物面反光器系統,該系統係可用於耦合一弧光燈之光 於一目標中。如圖2所示之該光學集合與聚光系統係使用二 大致對稱配置之橢面反光器2〇,21,這樣,自該第一反光 器20反射之光係接收於該第二反光器21之一對應段中。自 该光源22發射之光特別係藉該第一橢面反光器2〇集合及使 之沿该光軸25向該第二反光器21準直。該第二反光器2!係 接收该準直光束及使該光聚焦於該位在聚焦點之目標23。 岫述系統之集合,聚光,及耦合電磁輻射於一目標中係 可在該目標之該電磁輻射強度最大化。該等系統係有效及 具有相當長之使用壽命。 弧光燈,如金屬卣素燈,氣氣燈,或高壓水銀燈,通常 係在前述系統中作光源之用。一獲得高亮度之方法係藉使 该燈之弧隙縮小而得,這樣,所有光線係自一小點發出。 一理想光源係點光源,即可不考慮電極間距離之光源。縮 減電極間距離至-定值以下係具有實作之限制。在伴隨二 較短弧之限制係發射效率之損失及縮短電極之壽命。,而 極之使用壽命即隨之縮短。 P 以包 因弧光燈之間隙係不可無限縮小,故 双而要增加弧光燈以 較大間隙發射之該電磁輻射的亮度,以供耦合至一 ®才浪中0 發明概诚 黾磁無射於一光 一光學裝置係藉耥合一折回目的本身之 本紙張尺度適用中國國家標準(CNS) Α4ίϊ格(210X297公|)一 -5- 578022 A7 B7 五、發明説明(3 ) 源發射之電磁輻射而增加該電磁輻射的亮度。該光學裝置 係包括電磁輻射源,該電磁輻射源負有一第一寬度;一具 有第一輸入端與一反光端之第一光導管’該第一輸入端係 具有一第二寬度;一第二光導管係以平行該第一光導管方 式配置,該第二光導管係更進一步具有一與該第一光導管 之第一輸入端併列的第二輸入端,該第二輸入端係具有一 第三寬度;一第一反光器係具有一第一光軸及一第一聚焦 點在該第一光軸上;及一第二反光器,該反光器係具有一 第二光軸及一第二聚焦點在該第二光軸上,該第二反光器 係以大致對稱於該第一反光器方式配置,這樣,該第一光 軸係大致與該第二光軸共線。該源係位於大致鄰近該第一 反光器之第一聚焦點處,所產生之幅照光線係自該第一反 光器反射至該第二反光器及大致會合該第二聚焦點;該第 一及第二光導管之輸入端係鄰近於該第二反光器之第二聚 焦點,以收集該電磁輻射。該第一寬度係大致等於或小於 該第二與第三寬度之和。 本發明之前述與其他特點與優點係會由下述參照隨附圖 式之實例詳細說明更暸解。 圖式簡單說明 圖1係用於本發明一實例之使用拋物面反光器集合及聚光 的裝置不意圖, 圖2用於本發明一實例之使用橢面反光器集合及聚光的裝 置意圖, 圖3係根據本發明第一實例之用以反折一光源發射之電磁 -6 - 本紙張尺度適用中國國家標準(CNS) A4規格(210 X 297公釐)Line 578022 A7 B7 V. Description of the invention (at the focal point of the reflector) The focus of the reflector is toward the first parabolic reflector, thereby increasing the intensity of the collimated radiation reflected from there. U.S. Patent No. 09 / 669,841, which is incorporated herein by reference, discloses a double clasp reflector system that can be used to couple the light of an arc lamp to a target. The optical collection and condensing system shown in FIG. 2 uses two ellipsoidal reflectors 20, 21, which are arranged approximately symmetrically. In this way, the light reflected from the first reflector 20 is received by the second reflector 21 One corresponds to the segment. The light emitted from the light source 22 is particularly collected by the first ellipsoidal reflector 20 and collimated along the optical axis 25 toward the second reflector 21. The second reflector 2! Receives the collimated light beam and focuses the light on the target 23 located at the focus point. The collection, description, and coupling of electromagnetic radiation to a target can maximize the intensity of the target's electromagnetic radiation. These systems are effective and have a long service life. Arc lamps, such as metal halogen lamps, gas lamps, or high-pressure mercury lamps, are usually used as light sources in the aforementioned systems. One way to achieve high brightness is by reducing the arc gap of the lamp so that all light is emitted from a small spot. An ideal light source is a point light source, that is, a light source that does not consider the distance between electrodes. Reducing the electrode-to-electrode distance to a value below-has a practical limitation. The limitation associated with the two shorter arcs is the loss of emission efficiency and shortened electrode life. , And the extremely long service life will be shortened accordingly. P Because the gap of the arc lamp cannot be infinitely reduced, so the brightness of the electromagnetic radiation emitted by the arc lamp with a large gap must be increased for coupling to a 才 only. One light and one optical device is the original paper size that is folded back by the combination of one and the other. The Chinese paper standard (CNS) Α4ίϊ 格 (210X297 公 |) -5- 578022 A7 B7 V. Description of the invention (3) Electromagnetic radiation emitted by the source The brightness of the electromagnetic radiation is increased. The optical device includes a source of electromagnetic radiation, the source of electromagnetic radiation bears a first width; a first light pipe having a first input end and a reflective end; the first input end has a second width; a second The light pipe is arranged in parallel with the first light pipe, and the second light pipe further has a second input end parallel to the first input end of the first light pipe, and the second input end has a first Three widths; a first reflector having a first optical axis and a first focus point on the first optical axis; and a second reflector having a second optical axis and a second The focus point is on the second optical axis, and the second reflector is arranged approximately symmetrically to the first reflector, so that the first optical axis is substantially collinear with the second optical axis. The source is located at a first focusing point substantially adjacent to the first reflector, and the irradiated light rays are reflected from the first reflector to the second reflector and approximately meet the second focusing point; the first And the input end of the second light pipe is adjacent to the second focusing point of the second reflector to collect the electromagnetic radiation. The first width is substantially equal to or less than the sum of the second and third widths. The foregoing and other features and advantages of the present invention will be better understood from the following detailed description with reference to the accompanying drawings. Brief description of the drawings: Figure 1 is a schematic diagram of a device using a parabolic reflector assembly and focusing system according to an example of the present invention, and Figure 2 is a schematic view of an apparatus using an ellipsoidal reflector assembly and focusing system according to an example of the present invention. 3 is the electromagnetic radiation used to reverse the light emitted by a light source according to the first example of the present invention-6-This paper size is applicable to China National Standard (CNS) A4 (210 X 297 mm)
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五、發明説明(4 ) 輻射於其本身的一光學裝置示意圖; 圖4(a)係圖3所示實例中該光導管之詳圖 圖4(b)圖4(a)所示不同長度之光導管實例 圖5係圖3所示實例之至一波導管的輸出;及 圖6係圖3所示實例之至一投影系統之輸出,·及 圖7根據本發明第二實例之用以 $ n ^± 、 及折一先源發射之電磁輻 射於其本身的一光學裝置示意圖。 恶佳實性 圖3所示係一集合與聚光裝置3〇〇之第一實例。該裝置係 包括-電磁n射3G2之源3G1,該電仙射具有第—寬度3〇3 。在-最佳實例中,該源301係—發光之孤光燈。源3〇1係 可為-氤氣燈,-金屬_素燈’ _Hm燈,或—水銀燈。源 301係更換為白熾燈。 如源301為一弧光燈,對一交流燈而言,寬度3〇3係應為 其電極間之直線距離,對一直流燈而言,寬度3〇3係應為其 陽極與陰極間之直線距離。源3〇1為一白熾燈,第一寬度 303係應為該燈絲之熱長度,即該引線間之長度。 一具有一第一輸入端305及一反光端3〇6之第一光導管3〇4 係以平行於一第二光導管307方式配置,該第二光導管係具 有一第二輸入端308及一輸出端3〇9。該第一輸入端3〇5及該 第二輸入端308係併列。反光端3〇6及輸出端3〇9係也可併列 ,如第一光導管304及第二光導管3〇7長度相似時,如圖4(勾 所示,即無嚴格之需要。光導管3〇7係可如圖4(b)所示長於 光導管304。該第一輸入端305係具有一第二寬度3 1〇,而該 -7- I紙張尺度適用中國國家標準(CNS) A4規格(210X^^------ 578022 A7V. Description of the invention (4) A schematic diagram of an optical device radiating to itself; Figure 4 (a) is a detailed view of the light pipe in the example shown in Figure 3; Figure 4 (b) and Figure 4 (a) Light Pipe Example FIG. 5 is the output from a waveguide to the example shown in FIG. 3; and FIG. 6 is the output from a projection system to the example shown in FIG. 3; and FIG. n ^ ±, and a schematic diagram of an optical device that emits electromagnetic radiation emitted by a source. Fig. 3 shows a first example of a collection and focusing device 300. The device comprises a source 3G1 of electromagnetic n-radiation 3G2, which has a first width of 303. In the -best example, the source 301 is a light-emitting solitary lamp. The source 301 series may be-a tritium gas lamp, a -metal_prime lamp'_Hm lamp, or a mercury lamp. Source 301 was replaced with an incandescent lamp. If the source 301 is an arc lamp, for an AC lamp, the width of 303 should be the straight distance between the electrodes, and for the DC lamp, the width of 303 should be the straight between the anode and the cathode. distance. The source 301 is an incandescent lamp, and the first width 303 should be the thermal length of the filament, that is, the length between the leads. A first light pipe 304 having a first input end 305 and a light reflecting end 306 is arranged parallel to a second light pipe 307. The second light pipe has a second input end 308 and An output terminal 309. The first input terminal 305 and the second input terminal 308 are juxtaposed. The reflective end 3006 and the output end 3009 can also be juxtaposed. For example, when the first light pipe 304 and the second light pipe 3007 are similar in length, as shown in Figure 4 (marked, there is no strict need. Light pipe The 307 series can be longer than the light pipe 304 as shown in Fig. 4 (b). The first input end 305 has a second width of 3 10, and the 7-1 paper size applies the Chinese National Standard (CNS) A4 Specifications (210X ^^ ------ 578022 A7
第二輸入端308則具有一第三寬度311。 如第一光導管304及第二光導管307具有大致呈長方形截 面時,孩第二寬度31〇及第三寬度311,於特別方向測量, 係分別與第一輸入端305及第二輸入端3〇8等寬。在一最佳 實例中,第一光導管304及第二光導管3〇7同係大致呈錐形 之光導管。第一光導管304及第二光導管3〇7係可用石英, 玻璃塑膠或丙婦製造。 一具有一第一光軸313及一第一聚焦點314在第一光軸313 上之第一反光器3 12的配置係大致對稱於一具有一第二光轴 316及一第二聚焦點317之第二反光器315。第一光軸313係 大致與第二光軸3 16共線。一平面係分別對稱於第一及第二 反光器312及315且正交於該光軸313及316。因此,第二反 光器315係藉反映第一反光器312通過對稱平面而形成。 在一實例中,第一及第二反光器312及315係具有一塗層 ’該塗層係僅反射電磁輻射光譜之一預定部份。在一最佳 實例中,該塗層係僅反射可見光輻射,韓射之一預定光帶 ’或輻射之一特定顏色。 在一最佳實例,第一及第二反光器312及3 15係各具有至 少一部份之旋轉拋物表面。在另一不重要之實例中,第一 及第二反光器312及315係各具至少一邵份之旋轉環形,球 體形,雙曲面,或橢球面。 光源301係配置在大致鄰近第一反光器3 12之第一聚焦點 314處,以產生輻射線302,該輻射線係自第一反光器312反 射至第二反光器315及大致在第二聚焦點316會合。第一及 -8 - 本紙張尺度適用中國國家標準(CNS) A4規格(210 X 297公釐) 578022 A7 B7 五、發明説明(6 第一輸入端305及308係位於大致鄰近第二反光器315之第二 聚焦點3 17處,以集合電磁輻射3〇2。因第一輸入端3〇5及第 二輸入端308係併列,故第二寬度310及第三寬度311係可端 對端而成一直線。沿第二寬度3 1 〇及第三寬度3丨丨定向之線 係大致平行於第一寬度303,即自源301之一電極至另一電 極之方向。 在一最佳實例中,第一寬度303係大致等於第二寬度31〇 及第三寬度3 11之和。縱使減低效率,但第一寬度3〇3係可 小於或大於第二寬度310及第三寬度311之和。如圖4所示, 第二寬度310及第三寬度311係可成任何比例,只要二者之 和等於大致第一寬度303即可。第二寬度31〇係可大致等於 第三寬度311,或第二寬度310係大致為第三寬度311之二 倍。 源301發射之電磁輻射302的一部份係直接撞擊第一反光 器3 12及電磁輪射3 02的一部份係不直接撞擊第一反光器3 12 。為集合不直接撞擊第一反光器312之電磁輻射302,系統 300係包括一輔助反光器321,以反射至少一部份不直接撞 •^弟反光^§*312之電磁輪射302經第一反光器312的第一聚 焦點314至第一反光器312,以增加聚合光線之流量強度。 在一最佳實例中,輔助反光器321係一球形向後反射之反 光器,該反光器係以相對第一反光器312方式配置在源3〇1 之一側,以通過第一反光器312第一聚焦點314自遠離第一 反光器312之方向反射電磁輻射3〇2至第一反光器。 因第一輸入端305及第二輸入端308併列於第二聚焦點316 本紙張尺度適用中國國家標準(CNS) A4規格(210X 297公釐)The second input terminal 308 has a third width 311. For example, when the first light pipe 304 and the second light pipe 307 have a substantially rectangular cross section, the second width 31 ° and the third width 311 are measured in a particular direction, and are respectively connected to the first input terminal 305 and the second input terminal 3 〇8 equal width. In a preferred embodiment, the first light pipe 304 and the second light pipe 307 are of the same tapered light pipe. The first light pipe 304 and the second light pipe 307 can be made of quartz, glass plastic, or acrylic. The arrangement of a first reflector 3 12 having a first optical axis 313 and a first focusing point 314 on the first optical axis 313 is substantially symmetrical to a second optical axis 316 and a second focusing point 317. Of the second reflector 315. The first optical axis 313 is substantially collinear with the second optical axis 3 16. A plane is symmetrical to the first and second reflectors 312 and 315 and orthogonal to the optical axes 313 and 316, respectively. Therefore, the second reflector 315 is formed by reflecting the first reflector 312 through the plane of symmetry. In one example, the first and second reflectors 312 and 315 are provided with a coating layer 'which reflects only a predetermined portion of the electromagnetic radiation spectrum. In a preferred embodiment, the coating reflects only visible light radiation, one of the predetermined light bands, or a specific color of the radiation. In a preferred embodiment, the first and second reflectors 312 and 315 each have at least a portion of a rotating parabolic surface. In another unimportant example, the first and second reflectors 312 and 315 each have a rotating ring, a sphere, a hyperboloid, or an ellipsoidal surface each having at least one component. The light source 301 is disposed at a first focusing point 314 substantially adjacent to the first reflector 312 to generate a radiation 302, which is reflected from the first reflector 312 to the second reflector 315 and is approximately focused at the second Point 316 meets. No. 1 and -8-This paper size applies Chinese National Standard (CNS) A4 (210 X 297 mm) 578022 A7 B7 V. Description of the invention (6 The first input terminals 305 and 308 are located near the second reflector 315 The second focus point 3 is 17 to collect electromagnetic radiation 30.2. Because the first input terminal 3505 and the second input terminal 308 are side by side, the second width 310 and the third width 311 can be end-to-end. A straight line. The lines oriented along the second width 3 10 and the third width 3 丨 丨 are substantially parallel to the first width 303, that is, the direction from one electrode of the source 301 to the other electrode. In a best example, The first width 303 is approximately equal to the sum of the second width 31 ° and the third width 31. Although the efficiency is reduced, the first width 303 may be smaller or larger than the sum of the second width 310 and the third width 311. As shown in FIG. 4, the second width 310 and the third width 311 may be in any ratio, as long as the sum of the two is equal to the first width 303. The second width 31 ° may be approximately equal to the third width 311, or The second width 310 is approximately twice the third width 311. One of the electromagnetic radiation 302 emitted by the source 301 The part directly impacts the first reflector 3 12 and the part of the electromagnetic wheel 3 02 does not directly impact the first reflector 3 12. In order to collect the electromagnetic radiation 302 that does not directly impact the first reflector 312, the system 300 includes An auxiliary reflector 321 to reflect at least a part of it that does not directly collide. ^ Brother reflector ^ § * 312 of the electromagnetic wheel 302 passes the first focus point 314 of the first reflector 312 to the first reflector 312 to increase the aggregation The flow intensity of light. In a preferred example, the auxiliary reflector 321 is a spherical retro-reflective reflector, and the reflector is arranged on one side of the source 301 relative to the first reflector 312 to pass through the first reflector 321. The first focus point 314 of the reflector 312 reflects electromagnetic radiation 302 from the direction far from the first reflector 312 to the first reflector. Because the first input terminal 305 and the second input terminal 308 are juxtaposed at the second focus point 316 Paper size applies to China National Standard (CNS) A4 (210X 297 mm)
578022 A7578022 A7
裝Hold
訂Order
578022 A7 ______Β7 五、發明説明(8 ) 在如圖6所示之另一實例中,一聚光透鏡319係可配置於 大致鄰近第二光導管307之輸出端3〇9處。一影像投影系統 320係可配置於大致鄰近於聚光透鏡319之一輸出端處,以 藉釋放集合與聚光之輻射照明一影像而顯示該影像。 圖7係說明集合與聚光裝置6〇〇之第二實例。除反光器之 定向及基曲線外,集合與聚光裝置6〇〇係小於集合與聚光裝 置 300。 一具有一第一光軸613及一第一聚焦點614在第一光軸613 上之弟' 反光為612係以大致對稱於>^^具有一第二光轴616 及一第二聚焦點617之第二反光器615方式配置。第一光軸 613係大致與第二光軸616同線。其中具有二對稱平面,一 對稱平面係正交於光軸613及61 6,而另一對稱平面係正交 於弟一對稱平面及包括光轴613及616。因此,第一反光器 612係大致對稱於第二反光器615,其中該第一反光器612係 通過該二對稱平面反射該第二反光器615,反之亦然。 在一最佳實例中,第一及第二反光器612及615係各自具 有至少一部份之大致旋轉橢球形表面。在其他實例中,第 一及第二反光器612及615係各自具有至少一部份之大致旋 轉環形面,球體形面,雙曲面,或橢球面。 因弟一輸入端6 0 5及第二輸入端6 0 8併列於第二聚焦點616 ’故聚光於第一輸入端605及第二輸入端608之輻射線602係 具有與自源601發射之輕射線602相同大小。因第一寬度603 大致等於第二寬度610及第三寬度611之和,故輻射線602係 以第二寬度610與第三寬度611之比分配於第一輸入端6〇 5及 -11 - 本紙張尺度適用中Η國家標準(CNS) A4規格(21〇Χ297公f) ' 578022 A7 B7 五、發明説明(9 ) 第二輸入端608。因此,一部份之輻射線602係會耦合至第 一光導管604中,而剩餘之輻射線602係會耦合至第二光導 管607中。 耦合至第二光導管607之一部份的輻射線602係通過第二 光導管607及自輸出端609出現。同時,耦合至第一光導管 604之一部份的輻射線602係在反射端606反射及經第一光導 管604再發射而出現於第一輸入端605。自第一輸入端605出 現之射線係第二反光器615向第一反光器612反射,而聚光 於第一聚焦點614。而後,聚光之射線係通過該弧隙,藉輔 助反光器61-9再反射至第一反光器612,進而與應耦合至該 目標之其他射線結合。部份之輻射係會耦合於第二光導管 607之中及自輸出端609出現。因此,具有第一寬度603之弧 隙的自源601發射之電磁輻射602係會聚焦於小於第一寬度 603之點。 一反折藉一源發射之電磁輻射至其本身,以增加該源之 亮度的方法係如下述。一電磁輻射源係配置在一第一反光 器之一聚焦點處,該源係具有第一寬度。輻射線係藉由該 源產生。該輻射線係藉該第一反光器反射至一第二反光器 。該輻射線係會合該第二反光器之一聚焦點處。一第一光 導管係具有一第一輸入端及一反射端,該第一輸入端係更 進一步具有一第二寬度,及一第二光導管係具有一第二輸 入端及一逾出端,該第二輸入端係更進一步具有一第三寬 度,其配置係該第一及第二輸入端大致鄰近於該第二反光 器之聚焦點,及其中該第一寬度係等於該第二及第三寬度 -12- 本紙張尺度適用中國國家標準(CNS) A4規格(210 X 297公釐) 578022 A7578022 A7 ______B7 V. Description of the Invention (8) In another example shown in FIG. 6, a condenser lens 319 may be disposed approximately 309 near the output end of the second light pipe 307. An image projection system 320 may be disposed at an output end substantially adjacent to the condenser lens 319 to display an image by illuminating an image with a set of collected and focused radiation. FIG. 7 illustrates a second example of the focusing and focusing device 600. Except for the orientation and base curve of the reflector, the collection and collection device 600 is smaller than the collection and collection device 300. A younger having a first optical axis 613 and a first focusing point 614 on the first optical axis 613 'has a reflection of 612 and is approximately symmetrical to > ^^ has a second optical axis 616 and a second focusing point The second reflector 617 is configured in 615 way. The first optical axis 613 is substantially on the same line as the second optical axis 616. There are two planes of symmetry, one plane of symmetry is orthogonal to the optical axes 613 and 616, and the other plane of symmetry is orthogonal to the plane of symmetry and includes the optical axes 613 and 616. Therefore, the first reflector 612 is substantially symmetrical to the second reflector 615, wherein the first reflector 612 reflects the second reflector 615 through the two symmetrical planes, and vice versa. In a preferred embodiment, the first and second reflectors 612 and 615 each have at least a portion of a generally spheroidal surface. In other examples, the first and second reflectors 612 and 615 each have at least a portion of a generally rotating annular surface, a spherical surface, a hyperboloid surface, or an ellipsoidal surface. Since the first input terminal 6 0 5 and the second input terminal 6 0 8 are juxtaposed at the second focus point 616 ′, the radiation line 602 focused on the first input terminal 605 and the second input terminal 608 has the same emission as the source 601. The light rays 602 are the same size. Since the first width 603 is approximately equal to the sum of the second width 610 and the third width 611, the radiation line 602 is distributed to the first input terminals 605 and -11 at a ratio of the second width 610 to the third width 611. The paper size applies the China National Standard (CNS) A4 specification (21〇297297 f) '578022 A7 B7 V. Description of the invention (9) The second input terminal 608. Therefore, a portion of the radiation 602 is coupled into the first light pipe 604, and the remaining radiation 602 is coupled into the second light pipe 607. The radiation 602 coupled to a part of the second light pipe 607 appears through the second light pipe 607 and the self-output terminal 609. At the same time, the radiation line 602 coupled to a part of the first light pipe 604 is reflected at the reflection terminal 606 and re-emitted through the first light pipe 604 and appears at the first input terminal 605. The rays emerging from the first input terminal 605 are reflected by the second reflector 615 toward the first reflector 612, and are collected at the first focus point 614. Then, the focused rays pass through the arc gap, and are reflected by the auxiliary reflector 61-9 to the first reflector 612, and then combined with other rays that should be coupled to the target. Part of the radiation is coupled into the second light pipe 607 and emerges from the output terminal 609. Therefore, the electromagnetic radiation 602 emitted from the source 601 with an arc gap of the first width 603 is focused at a point smaller than the first width 603. The method of reversing the electromagnetic radiation emitted by a source to itself to increase the brightness of the source is as follows. An electromagnetic radiation source is disposed at a focal point of a first reflector, and the source has a first width. Radiation is generated by this source. The radiation is reflected to a second reflector by the first reflector. The radiation line meets a focal point of one of the second reflectors. A first light pipe system has a first input end and a reflective end, the first input end system further has a second width, and a second light pipe system has a second input end and an exit end. The second input terminal further has a third width, and the configuration is that the first and second input terminals are approximately adjacent to the focal point of the second reflector, and wherein the first width is equal to the second and first Three widths -12- This paper size applies to China National Standard (CNS) A4 (210 X 297 mm) 578022 A7
之和 寬度之比通過輻射線係以該第二寬度與該第三 W弟一及弟二光導箐裳_ 通過該第二光導管 · —及弟二輸入細。 , <輻射線係輸出之輻射線。通過該第一 光導官之輻射線係向 該源。 W-及昂-反光器’而至 雖本發明係於前述詳細說明 明之實例。精此技藝者係 述實例的使用與修改。 主要元件符號說明 10 第一反光器 11 第一反光器 12 光源 13 目標 14 向後反光器 20 第一反光器 21 弟二反光器 22 光源 23 目標 24 向後反光器 25 光幸由 300 集合及聚光裝置 301 源 302 電磁輻射 303 第一寬度 304 第一光導管 可作 ,但本發明係不限於前述說 不脫離本發明概念之不同前 -13- 本紙張尺度適用中國國家標準(CNS) Α4規格(210 X 297公釐) 578022 A7 B7 五、發明説明(11 ) 305 第一輸入端 306 反光端 307 第二光導管 308 第二輸入端 309 輸出端 310 第二寬度 3 11 第三寬度 3 12 第一反光器 313 第一光轴 3 14 第一聚焦點 315 第二反光器 3 16 第二光軸 3 17 第二聚焦點 3 18 波導管 3 19 聚光透鏡 320 影像投影系統 321 輔助反光器 600 集合及聚光裝置 601 源 602 輻射線 603 第一寬度 604 第一光導管 605 第一輸入端 606 反射端 607 第二光導管 -14- 訂 本紙張尺度適用中國國家標準(CNS) A4規格(210x 297公釐)The ratio of the sum of the width and the width of the third width through the radiation line to the third W1 and W2 light guides _ through the second light pipe-and the W2 input is thin. , < Radiation line is the radiation output. The radiation passing through the first light guide is directed to the source. W- and Angstrom-reflectors', although the present invention is based on the examples described in the foregoing detailed description. The use and modification of the examples described by this artist. Description of main component symbols 10 First reflector 11 First reflector 12 Light source 13 Target 14 Backward reflector 20 First reflector 21 Second reflector 22 Light source 23 Target 24 Backward reflector 25 Light collection by 300 and focusing device 301 Source 302 Electromagnetic radiation 303 First width 304 First light pipe can be used, but the present invention is not limited to the aforementioned differences without departing from the concept of the present invention -13- This paper size applies to China National Standard (CNS) Α4 specifications (210 X 297 mm) 578022 A7 B7 V. Description of the invention (11) 305 First input end 306 Reflective end 307 Second light pipe 308 Second input end 309 Output end 310 Second width 3 11 Third width 3 12 First reflector 313 First optical axis 3 14 First focus point 315 Second reflector 3 16 Second optical axis 3 17 Second focus point 3 18 Waveguide 3 19 Condensing lens 320 Image projection system 321 Auxiliary reflector 600 Assembly and focusing Device 601 source 602 radiation 603 first width 604 first light pipe 605 first input end 606 reflection end 607 second light pipe -14- The size of the paper is applicable to China National Standard (CNS) A4 (210x 297 mm)
578022 A7 B7 五 、發明説明 ( 12 ) 608 第 一 _ 輸 入 端 609 輸 出 端 610 第 二 寬 度 61 1 第 三 寬 度 612 第 一 反 光 器 613 第 -' 光 轴 614 第 一 聚 焦 點 615 第 二 反 光 器 616 第 二 光 軸 617 第 二 聚 焦 點 619 輔 助 反 光 器 -15-本紙張尺度適用中國國家標準(CNS) A4規格(210 X 297公釐)578022 A7 B7 V. Description of the invention (12) 608 First _ input end 609 output end 610 second width 61 1 third width 612 first reflector 613th-'optical axis 614 first focus point 615 second reflector 616 Second optical axis 617 Second focus point 619 Auxiliary reflector -15- This paper size applies to China National Standard (CNS) A4 (210 X 297 mm)
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