TW201000822A - Optical adder - Google Patents

Optical adder Download PDF

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Publication number
TW201000822A
TW201000822A TW97132355A TW97132355A TW201000822A TW 201000822 A TW201000822 A TW 201000822A TW 97132355 A TW97132355 A TW 97132355A TW 97132355 A TW97132355 A TW 97132355A TW 201000822 A TW201000822 A TW 201000822A
Authority
TW
Taiwan
Prior art keywords
light
optical axis
light amount
amount region
source
Prior art date
Application number
TW97132355A
Other languages
Chinese (zh)
Other versions
TWI384178B (en
Inventor
Fumio Suzuki
Kazuhiro Noda
Hiroshi Morikawa
Original Assignee
Abel Systems Inc
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Publication date
Application filed by Abel Systems Inc filed Critical Abel Systems Inc
Publication of TW201000822A publication Critical patent/TW201000822A/en
Application granted granted Critical
Publication of TWI384178B publication Critical patent/TWI384178B/en

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Classifications

    • GPHYSICS
    • G02OPTICS
    • G02BOPTICAL ELEMENTS, SYSTEMS OR APPARATUS
    • G02B27/00Optical systems or apparatus not provided for by any of the groups G02B1/00 - G02B26/00, G02B30/00
    • G02B27/10Beam splitting or combining systems
    • G02B27/12Beam splitting or combining systems operating by refraction only
    • GPHYSICS
    • G02OPTICS
    • G02BOPTICAL ELEMENTS, SYSTEMS OR APPARATUS
    • G02B27/00Optical systems or apparatus not provided for by any of the groups G02B1/00 - G02B26/00, G02B30/00
    • G02B27/10Beam splitting or combining systems
    • G02B27/1006Beam splitting or combining systems for splitting or combining different wavelengths
    • GPHYSICS
    • G02OPTICS
    • G02BOPTICAL ELEMENTS, SYSTEMS OR APPARATUS
    • G02B27/00Optical systems or apparatus not provided for by any of the groups G02B1/00 - G02B26/00, G02B30/00
    • G02B27/10Beam splitting or combining systems
    • G02B27/108Beam splitting or combining systems for sampling a portion of a beam or combining a small beam in a larger one, e.g. wherein the area ratio or power ratio of the divided beams significantly differs from unity, without spectral selectivity
    • GPHYSICS
    • G02OPTICS
    • G02BOPTICAL ELEMENTS, SYSTEMS OR APPARATUS
    • G02B27/00Optical systems or apparatus not provided for by any of the groups G02B1/00 - G02B26/00, G02B30/00
    • G02B27/10Beam splitting or combining systems
    • G02B27/14Beam splitting or combining systems operating by reflection only
    • G02B27/143Beam splitting or combining systems operating by reflection only using macroscopically faceted or segmented reflective surfaces
    • GPHYSICS
    • G02OPTICS
    • G02BOPTICAL ELEMENTS, SYSTEMS OR APPARATUS
    • G02B27/00Optical systems or apparatus not provided for by any of the groups G02B1/00 - G02B26/00, G02B30/00
    • G02B27/10Beam splitting or combining systems
    • G02B27/14Beam splitting or combining systems operating by reflection only
    • G02B27/145Beam splitting or combining systems operating by reflection only having sequential partially reflecting surfaces

Abstract

To provide an optical adder capable of creating high-intensity light, which is compact in the radial direction with respect to the primary optical axis and has no restrictions in terms of the wavelengths of light which can be emitted from the light source, a construction is employed in which: a reflecting mirror M1 having a reflecting surface M12 formed on the surface thereof and a through hole M11 at the center of the reflecting surface M12 is disposed such that the central axis of the through hole M11 is aligned with the primary optical axis L, and the reflecting surface M12 is inclined relative to the primary optical axis L; a first light source 1 is provided which emits a first light, whose optical axis L1 coincides with the primary optical axis L, from the rear surface of the reflecting mirror M1 to the front surface; and a second light source that emits a second light with a low intensity region formed at the center and a high intensity region formed at the periphery is provided in a location deviated from the primary optical axis L, wherein the low intensity region and the high intensity region of the second light are irradiated onto the through hole M11 and the reflecting surface M12 respectively, and the optical axis L2 of the second light that is reflected from the reflecting surface M12 is aligned with the primary optical axis L so that the second light travels with the first light.

Description

201000822 六、發明說明: 【發明所屬之技術領域】 【0001】 本發明係關於一種光累加裝置,其讓複數光源所射出之光線 以光軸重疊的方式一起前進。 【先前技術】 【0002】 專利文獻1揭示一種高光量光源裝置,其將複數LED密隼配 (^平面上,並將各LED所射出光線匯集朝同一方向前進。 ni'隹'密集配置’則LED所產生的熱能會降低發 【0004】 文獻2揭示一種光累加裝置,具備:第1咖,盆射 5 ίί /線;第2咖,其射出與該第1LE料同波長的 C,弟2先線,且其光軸與第1LED的光軸垂直;以及分1 f 置在該等光輛的交叉點t,日射」及刀7^鏡,其配 讓第斜。該裝置利用分光鏡 : 弟先線透射,並讓第2LED所射出的第2 【0005】 適當的Hi!用ίί鏡有效率地讓光線透射或反射,必須讓 複數種ΐί的LFn人》光鏡的透射面以及反射面’因此必須準備 【0006】 201000822 又,即使讓適當波長的光線射入分光鏡,射入透射面的光線 有相當的部分會被反射,而射入反射面的光線有相當的部分會透 射掉,故很難以高效率製作出高光量的光線。 專利文獻1 :曰本特開2005-108544號公報 專利文獻2 :日本特開2〇〇6_139〇44號公報 【發明内容】 [發明所欲解決的問題] 【0007】 有鑑於上述問題,本發明的目的在於提供一種光累加裝置, /、=適§地^發光源的熱量,使用光源所射出之光線的波長並無 ,疋,可精簡以主光軸為基準的徑向構造,進而製作出高光量的 光線。 [解決問題之技術手段] 【0008】 明之光累加裝置具備:反射鏡,其正面形成有反 诗、、δ又有貫通孔,該貫通孔的中心軸線與主光軸重疊,且 二主光軸傾斜;第1光源’其從該反射鏡的背面侧向 光軸與該主光軸重疊的第1光線;以及第2光源,其 ί智f轴的位置上,並射出中心部形成低光量區域且周 成區域的第2光線;該第2光線的低光量區域射入 區3到反射面上,使被反射面反射的第2光線 光軸豐的方式與第1光線—起前進。 射於裝置’光轴與該主光軸重疊的第1光線,會通過反 源二+二^通孔’從反射鏡的背面側前進到正面側,該第2光 光線,會被該反射面反射,而以光軸與主光軸i 前進’故能集中第1光線断線, [0010] 201000822 並 比較容峨。生的熱能 防止故障等問題發生。 生的"、、降低發光效率,201000822 VI. Description of the Invention: [Technical Field of the Invention] [0001] The present invention relates to a light accumulating device that advances light rays emitted from a plurality of light sources in such a manner that optical axes overlap. [Prior Art] [0002] Patent Document 1 discloses a high-light-quantity light source device in which a plurality of LEDs are closely arranged (on a plane, and light emitted from each LED is collected in the same direction. ni'隹' dense arrangement' The heat generated by the LED will be reduced. [0004] Document 2 discloses a light accumulating device having: a first coffee, a spray of 5 ίί / line; a second coffee, which emits the same wavelength as the first LE, C 2 The first line, and its optical axis is perpendicular to the optical axis of the first LED; and the division 1 f is placed at the intersection t of the light vehicles, the insolation and the knives, which are matched to the first oblique. The device uses a beam splitter: The first line is transmitted, and the second LED is emitted. [0005] Appropriate Hi! uses a ί mirror to efficiently transmit or reflect light. It is necessary to allow the transmission surface and reflection surface of a plurality of LFn lenses. 'Therefore, it must be prepared [0006] 201000822 Moreover, even if light of the appropriate wavelength is incident on the beam splitter, a considerable portion of the light incident on the transmission surface will be reflected, and a considerable portion of the light incident on the reflection surface will be transmitted. Therefore, it is difficult to produce high-intensity light with high efficiency. Patent Document 2: JP-A-2005-108544 (Patent Document 2) Japanese Laid-Open Patent Publication No. Hei No. Hei. No. Hei. No. Hei. No. Hei. The purpose is to provide a light accumulating device, /, = the heat of the light source, the wavelength of the light emitted by the light source is not used, and the radial structure based on the main optical axis can be simplified, and then High-light quantity of light [Technical means for solving the problem] [0008] The light accumulating device of the present invention includes: a mirror having a reverse poem formed on the front surface thereof, and a through hole having a central axis overlapping the main optical axis; And the two main optical axes are inclined; the first light source 'the first light beam from the back side of the mirror to the optical axis and the main optical axis; and the second light source at the position of the f-axis and the center of the emission a second light ray that forms a low light amount region and a circumferential region; the low light amount region of the second light ray enters the region 3 to the reflecting surface, and the second light ray reflected by the reflecting surface is abundance and the first light ray— Go forward. Shoot on the device 'optical axis and the The first light beam that overlaps the main optical axis advances from the back side of the mirror to the front side through the anti-source two + two through holes, and the second light ray is reflected by the reflecting surface, and the optical axis and the main The optical axis i advances, so it is possible to concentrate the first light break, [0010] 201000822 and compare the tolerance. The raw heat can prevent problems such as malfunctions. The raw ", reduce the luminous efficiency,

【0011】 X 的光線而將複數光源並排 故能精簡以主光軸為基準 另外,由於無須為了製作出高光量 配置在同-平面上以難光射出方向, 的4望向構造。 【0012】 背面側二S二光2反射鏡中央的貫11孔,並從反射鏡的 5 ί /ΐΐ __ ’第2光線則被反射鏡反射,故 ^ 2 光源靖㈣摘波長絲限定,第丨光源、 ^細—種類的光 【0013】 θ再者,由於第1光線通過反射鏡的貫通孔,第2光線的低光 置區域通過反射鏡的貫通孔,高光量區域則賴反射面上,故第i 光線以及第2光線的光量辭沒有損失,可以有效率的集中。 【0014】 ' 只要該第1光源具備第1發光元件以及使該第丨發光元件所 射出的該第1光線的光束收斂到該貫通孔大小的第丨光學元件, 该第1光源所射出的第1光線就不會被反射鏡遮住,而會從背面 側貫通到正面侧,讓光線更有效率的集中。 【0015】 、 只要該第2光源具備第2發光元件以及使該第2發光元件所 射出的該第2光線形成該低光量區域與該高光量區域的第2光學 元件,便可使該第2光線折射分開成低光量區域與高光量區域。 [0016] 該第2光學元件的具體實施態樣例如中央部有凹部的凸透 201000822 鏡。若依該等構件,射入凸透鏡中央部的光會被折射而偏到周[0011] The light of X is used to reduce the number of light sources in parallel with the main optical axis. In addition, since it is not necessary to produce a high light amount, it is arranged on the same plane to make it difficult to emit light in a direction of 4 directions. [0012] The back side of the two S 2 light 2 mirror in the center of the 11 holes, and the mirror from the 5 ί / ΐΐ __ 'the second light is reflected by the mirror, so ^ 2 source Jing (four) picking wavelength limit, the first丨Light source, ^fine-type light [0013] θ Further, since the first light passes through the through hole of the mirror, the low-light region of the second light passes through the through hole of the mirror, and the high-light amount region is on the reflective surface. Therefore, there is no loss in the amount of light of the i-th ray and the second ray, and the concentration can be efficiently. [0014] The first light source includes a first light-emitting element and a second optical element that converges the light flux of the first light emitted from the second light-emitting element to the through-hole, and the first light source emits 1 Light will not be covered by the mirror, but will pass from the back side to the front side, allowing the light to concentrate more efficiently. [0015] The second light source is provided with the second light emitting element, and the second light ray emitted from the second light emitting element forms the second optical element in the low light amount region and the high light amount region, so that the second light source can be made The light refraction is divided into a low light amount region and a high light amount region. [0016] A specific embodiment of the second optical element is, for example, a convex-transparent 201000822 mirror having a concave portion at the center portion. According to these components, light incident on the central portion of the convex lens is refracted and biased to the periphery.

部去,故可在中心部形成低光量區域,在周邊部形成高光 【0017】 A 只要該第2發光元件的定向特性為中心部低光量而周邊 1二1,/^可將該第2光線折射分開成低光量區域與高光量區域7 只要該第2光_全部光量都集巾龍高紐區域,就 儘可能不浪費第2光_光量的情況下,針第丨級 = 線。 、疋 f 【_】 射於若光量的光線,可沿著主光軸設_數個該反 並職各反雜設置難簡面㈣級的光源,該 祕I心Ξ械低光量區域’在周邊部形成高光量區域,低光量區 =^貝通孔,南光量區域射到反射面上,被反射面反射的光 /、光軸與該主光軸重疊而與該第丨光線一 、、、 【0020】 第! 該第2發光元件可以是例如LED,作為該 光源以及6亥第2光源的具體實施態樣。 【0021】 i 將光累加裝置當作丨個單元,在同 以構成照明裝置’則由於i個單元中 簡以主光轴為基準^向構造r “I的光線之外,更能精 【0022】 止發裝ΪΪ用於前燈’便能獲得高光量,並能防 為基;本發明之光累加裝置以主光轴 到限制的前燈。^間、用独絲為基準的彳!向空間受 [對照先前技術之功致] 【0023】 201000822 若依該J構造的光累加裝置,則由 光線以光傾疊的方式1前進,故能製作m射出之 高光量區域射到反射面上,=以域射人貫通孔, 隼中光線。再者,第i hi ^分规被反射’故能以高效率 先源與第2光源係分開配置,故能防Μ 的問題。另外,由於無須將複數光源以對齊光射出 ==式並排配置在同—平面上,故可精簡以主光軸 【實施方式】 【0026】 以下,參照圖面説明本發明—實施形態。 【0027】 〜 【οοίΓ_之光累加裝置_,可用來#作汽車前燈的光源。 •具體而言本實施形態之光累加裝置薦,如圖 ,呈 備丄第1反射鏡Μ卜其正面的反射面Μ12相對主光轴L呈^ 狀態,且設有中心軸線與主光軸L重疊的貫通孔Mh ; 、通 1 ’其從該第1反射鏡Ml的背面側朝正面側射出光軸u 車^重疊的第〗光線;以及第2光源2,其設置在偏離主光轴l 笛,可朝該反射鏡M1的反射面M12射出垂直主光軸[的 第2光線。絲’該反射面M12所反射的第2光線以 與該主光轴L·重疊的方式與第1光線—起前進。 ,、亢釉 【0029】 該反射鏡Ml為圓形薄板狀,其中心設有橢圓形 又,該反射鏡M1的該反射面Ml2與主光軸L的傾斜角度 為銳角45度。 【0030】 該第1光源1具備:第1LED11,其為第i發光元件;以 1光學元件12,其將該第1·Π所射出的第丄親的光束收敛 201000822 聚焦成該貫通孔Μη的大小。 【0031】 該第1光學元件12具備:第1LED透鏡121,其集中第1LED11 所射出的光線’以縮小光束的大小;以及第1平凸透鏡122,其設 置在離開该弟1LED透鏡121之光射出端若干距離的位置上,如 圖2所示的,讓第1LED透鏡121所集中的第1光線變成平行光 束貫通該貫通孔Mil。 【0032】 5亥第2光源2具備:第2LED21 ’其為第2發光元件;第2光 學兀件22,其在該第2LED21所射出的第2光線的中心部形成低 光量區域Lo,並在周邊部形成高光量區域ffl。又,第2LED21與 第1LED11為同種類的LED,可射出相同波長的 【0033】 ' 該第2光學元件22具備:第2LED透鏡221,其將該第2LED21 所射出^第2光線變成平行光;以及第2雙凸透鏡222弟其設置在 離開该第2LED透鏡221之光射出端若干距離的位置上。如圖2 藉由偏移調整該第2雙凸透鏡222的焦點,而在該第2 ϋΐίί部形成低光量區域L。,在周邊部形成高光量區域Hi, Lo射入貫通孔MU,高光量區域則射到反射面 被及㈣^2紐大部分光量的高光量區域迅的光線, 進㈣讀,以妹U魅妹L重疊的方式與第 【0034】 光線二之主本先實 Μ1的U先軸L重1的方式射出,並通過第1反射鏡 L2 t二Π衫2光線蚊射面Μ12反射之後,其光軸 盘第2 3上重並曰與第1光線-起前進,故能集中第1光線 弟2九線而形成高光量的光線。 【0035】 再者,由於利用第i光學元件12將第(光線的光束大小縮小 201000822 到貫通孔Mjl大小而使其能通過貫通孔Mn,故約略全部的光線 都可通過。第2甘光線由於高光量區域ffi的光被反射面购反射, 故僅喪失低^量H域Lo所含極小部分的光而已,而與第丨光線一 起珂進。因此’可將第1LED11以及第2LEm 乎全部集巾’以高效挪絲光量的光。 木〕尤成 【0036】 再者’由於只有第1光線通過貫通孔Mil,而第2光線被反 射面M12反射’故第〗級與第2光線所制驗錢無限定。 因此,可以使用相同種類的光源,以降低成本。 【0037】 又 而第2 ί^源W其光軸齡絲L重疊的方式配置, 方戈配詈"m 光軸L並對主光軸L垂直射出第2光線的 iiHi =與第2led21以互相_的方式配置, 7發散的熱而導致發級率降低或發生故 ^。 - 光泝了製造高枝的光而將第1光源1以及第2 ί:9Γ 小以光軸為基準的徑向空間。 其次就本發明其他實施形態説、 實施形態的構件會賦刊目同符號/之在以下㈣中對應上达 【0040】 光源置㈣彡㈣光1加裝置當作1個 且中央部上設有貫=M2f 傾斜設置’ 第2光線,使其貫通該貫通孔第1光線2 偏離主光軸L的位置上,· 3 及4 3光源3,其設置於 讓弟3九線射到該第2反射鏡M2的反 10 201000822 射面M22上。 【0041】 第2反射鏡M2,其形成圓形薄板狀,且反射面M22傾斜設 置,而與主光軸L夾鋭角45度,中央部的貫通孔M21的中心軸 線與主光軸L重疊。第2反射鏡M2與第1反射鏡mi相比,其 直徑比較大。 a 【0042】 該集光it件c ’係由2辦凸透鏡α、C2所構成,讓集中過 =第1光線以及第2光線變成平行光,使其光束大小集中而與該 第2反射鏡M2的貫通孔M21的大小相同。因此,可讓第i光線 與第2光線全部的光通過第2反射鏡m2的貫通孔m2 1。 【0043】 、 一該第3光源3以射出時第3光線的光軸L 3垂直主光轴L的方 式巧置:該第3光源3具備··第3LED31 ;以及第3光學元件32, 其讓該第3LED31所射出的第3光線在中心部形成低光量區域 Lo ’並在周邊部形成高光量區域。 【0044】 第3光學元件32具備:第3LED透鏡321,其讓該第3LED31 戶5射出的第3光線變成平行光;第3雙凸透鏡322,其設置在與該 (第3LED透鏡321的光射出端間隔若干距離的位置上;以及 鏡323,其設置在第3雙凸透鏡322與第2反射鏡M2之間。 該第3雙凸透鏡322與凹透鏡323的焦點,以調整出在第3 的:央部形成低光量區域L〇,在周邊部形成高光量區域扭,讓低 光量區域L〇射入貫通孔M21,並讓高光量區域Hi照射到反射面 M22上的狀態。 沿认射面 【0045】 、若依該等裝置,則由於在光軸L1、L2與主光軸L重疊一起前Since the portion is formed, a low light amount region can be formed in the center portion, and a highlight can be formed in the peripheral portion. [0017] A The second light ray can be used as long as the directional characteristic of the second light emitting element is the low light amount at the center portion. The refraction is divided into a low light amount region and a high light amount region 7 as long as the second light_total light amount is in the area of the towel, and the second light_light amount is not wasted as much as possible.疋f [_] The light that strikes the amount of light can be set along the main optical axis. _ Several of these anti-combination counters are used to set the light source of the difficult (4) level. a high-light-amount region is formed in the peripheral portion, and a low-light-quantity region=^bepass-through hole is formed, and the south-light-amount region is incident on the reflective surface, and the light/optical axis reflected by the reflective surface overlaps with the main optical axis to be adjacent to the second light. , [0020] No.! The second light-emitting element may be, for example, an LED, as a specific embodiment of the light source and the second light source. [0021] i The light accumulating device is regarded as a unit, and in the same way, the lighting device is configured to be more precise than the light of the structure r "I" based on the main optical axis of the i cells. 】 The hair extension device can be used for the headlights to obtain high light amount and can be prevented from being used as the base; the light accumulating device of the present invention uses the main optical axis to the limited headlights. Space is subject to [compared with the prior art] [0023] 201000822 According to the light accumulating device of the J structure, the light is advanced by the way of light tilting, so that the high-light-amount region emitted by m can be made to be incident on the reflecting surface. , = shoots the through hole in the field, and illuminates the light in the middle. Furthermore, the i hi ^ rule is reflected. Therefore, it can be separated from the second light source by the high efficiency source, so it can prevent the problem. In addition, since it is not necessary The plurality of light sources are arranged side by side in the same plane as the alignment light emission ==, so that the main optical axis can be simplified. [Embodiment] Hereinafter, the present invention will be described with reference to the drawings. [0027] ~ [οοίΓ _ light accumulation device _, can be used as # light source for car headlights. Specifically, in the light accumulating device of the present embodiment, as shown in the figure, the reflecting surface Μ12 of the first reflecting mirror is disposed in a state relative to the main optical axis L, and is provided with a central axis and a main optical axis L. The overlapping through holes Mh; and the passage 1' emit a first light that overlaps the optical axis u from the back side of the first mirror M1 toward the front side; and the second light source 2 is disposed offset from the main optical axis The flute can emit a second ray of the vertical main optical axis toward the reflecting surface M12 of the mirror M1. The second ray reflected by the reflecting surface M12 of the wire is overlapped with the main optical axis L· and the first ray亢 前进 。 , , 该 该 该 该 该 该 该 该 该 该 该 该 该 该 该 该 该 该 该 该 该 该 该 该 该 该 该 该 该 该 该 该 该 该 该 该 该 该 该 该 该 该 该 该 该 该 该 该 该 该[0030] The first light source 1 includes a first LED 11 that is an ith illuminating element, and an optical element 12 that focuses the beam of the first 射 that is emitted by the first Π 20 201000822 into the through hole Μ [0031] The first optical element 12 includes a first LED lens 121 that concentrates the first LED 11 and emits a line 'to reduce the size of the beam; and a first plano-convex lens 122 disposed at a distance from the light exit end of the LED 1 lens 121, as shown in FIG. 2, the first LED lens 121 is concentrated (1) The second light source 2 includes a second LED 21' as a second light-emitting element, and a second optical element 22, the second light emitted from the second LED 21 The center portion is formed with the low light amount region Lo, and the high light amount region ff1 is formed in the peripheral portion. Further, the second LED 21 and the first LED 11 are the same type of LED, and the same wavelength can be emitted. [0033] The second optical element 22 includes: The 2LED lens 221 converts the second light emitted by the second LED 21 into parallel light, and the second lenticular lens 222 is disposed at a position spaced apart from the light emitting end of the second LED lens 221. As shown in FIG. 2, the focus of the second lenticular lens 222 is adjusted by offset, and the low light amount region L is formed in the second ϋΐ ί. In the peripheral portion, a high-light-amount region Hi, Lo is incident on the through-hole MU, and a high-light-amount region is incident on the reflecting surface and the light of the high-light-quantity region of most of the light amount of the (4)^2 New Zealand is entered into the (four) reading. The way in which the sister L overlaps is emitted in the manner that the U-axis L of the first light ray 1 of the first light ray 1 is 1 and is reflected by the first mirror L2 t 2 Π 2 光线 蚊 光线 光线 , , The optical axis disc 2 is heavy and the first light is moved forward, so that the first light ray 2 and the nine lines can be concentrated to form a high light amount of light. Further, since the first optical element 12 reduces the beam size of the light beam by 201000822 to the size of the through hole Mj1 so as to pass through the through hole Mn, approximately all of the light can pass. The light of the high-light-quantity area ffi is reflected by the reflection surface, so that only a very small portion of the light contained in the low-range H-domain Lo is lost, and it is merged with the second-order light. Therefore, the first LED 11 and the second LEm can be collectively set. The towel's light with high efficiency. Wood] Youcheng [0036] Furthermore, since only the first light passes through the through hole Mil, and the second light is reflected by the reflecting surface M12, the second light is made by the second light. There is no limit to the money inspection. Therefore, the same kind of light source can be used to reduce the cost. [0037] The second ί^ source W is arranged in such a way that the optical axis L is overlapped, and the square optical 詈"m optical axis L The iiHi= and the second led 21 that emit the second light beam perpendicularly to the main optical axis L are disposed so as to be mutually _, and the heat which is dissipated by 7 causes the emission rate to decrease or occurs. - The light traces the light of the high branch. 1 light source 1 and 2nd ί:9Γ small diameter based on the optical axis Next, in the other embodiments of the present invention, the components of the embodiment will be assigned the same symbol/in the following (4) corresponding to the [0040] light source (four) 彡 (four) light 1 plus device as one and the central portion The second light is disposed at a position where the first light ray 2 is inclined away from the main optical axis L, and the light source 3 is disposed at the position of the third brother and the third light. The second mirror M2 is inverted 10 201000822 on the surface M22. [0041] The second mirror M2 is formed in a circular thin plate shape, and the reflecting surface M22 is inclined, and is at an angle of 45 degrees to the main optical axis L, and the central portion The central axis of the through hole M21 overlaps with the main optical axis L. The second mirror M2 has a larger diameter than the first mirror mi. a [0042] The light collecting member c' is composed of 2 convex lenses α In the case of C2, the concentrated first light and the second light are converted into parallel light, and the beam size is concentrated to be the same as the size of the through hole M21 of the second mirror M2. Therefore, the ith light and the first light can be made. All of the light of the second light passes through the through hole m2 1 of the second mirror m2. [0043] One of the third light sources 3 is emitted. The optical axis L 3 of the third light ray is perpendicular to the main optical axis L. The third light source 3 includes a third LED 31 and a third optical element 32 that allows the third light emitted by the third LED 31 to be The central portion forms a low light amount region Lo' and forms a high light amount region in the peripheral portion. [0044] The third optical element 32 includes a third LED lens 321 that causes the third light emitted from the third LED 31 to be parallel light; The lenticular lens 322 is provided at a position spaced apart from the light emitting end of the third LED lens 321 by a distance; and a mirror 323 is provided between the third lenticular lens 322 and the second mirror M2. The third lenticular lens 322 and the focal point of the concave lens 323 are adjusted to form a low light amount region L〇 in the third central portion, and a high light amount region twist is formed in the peripheral portion, and the low light amount region L〇 is incident on the through hole M21. And the state in which the high light amount region Hi is irradiated onto the reflection surface M22. Along the incident surface [0045], according to these devices, before the optical axes L1, L2 overlap with the main optical axis L

進白^第1光線與第2光線上,再讓第3光線以光軸L3與^光軸L 重疊的方式一起前進’故能製作出更高光量的光線。 【0046】 11 201000822 再者,由於係沿著主光軸L追加光源,故可在以主光軸l為 基準的徑向構造維持精簡的情況下,製作出更高光量的光。 【0047】 此外,本發明並非僅限於上述實施態樣而已。 【0048】 、例如,可以把光累加裝置當作一個單元,然後在同一平面上 並^複數個單元,作出可射出高光量光線的巨大光源。由於每j 個單兀中j主光轴L為基準的徑向構造很精簡,故即使像這樣並 排製作出高光量的紐,也能夠精簡以大統s駐[為基 準的徑向構造。 【0049】 w又,如圖4所示的,在第2光學元件22中,亦可使用中央部 ϋ ΓΓ 2221的雙凸透鏡222。利用此等構件,入射到雙凸透鏡 2中央,的光會向,部折射,如是便能在中央部形成低光量區 以曰^上周邊部形成面光量區域Hi。另夕卜射出光線的LED可 以疋面光源,也可以是點光源。 【0050】 量區成低光量11域’在周邊部形成高光 量,二==Ξί^:ΕΜ1的配光特性而在中央部形成低光 【0051】 ^集中第1光線與第2光線形成高光量一 設置;出=量1用跟第3光源同樣的方式進一步 主光轴重疊的方式-起前^ 所射出之光線 第2光源或第3光源亦可用在光射㈣光財响對主光轴 12 201000822 ^傾斜的方式設置。這樣的話’便能在以主光軸為基準的半徑方 向上更進一步精簡光累加裝置的構造。 【0054】 反射鏡並^限於圓織錄而已,卩、要具備反射面與貫通孔 ^可^了。例如,反射鏡亦可形成從斜向切斷關侧面的形狀, =斷面具有反射面,並具有從底面巾央部向蝴面巾央貫通的 貝通孔。 ^ ’反射鏡的貫通孔的形狀並非僅限 以疋長方形等的各種形狀。 也J rnn<d 【0055】 例如,亦可使用繞射光柵,將第1 並且把第2光線折射成低光量區域 、 光學元件並不限於透鏡 光線的光束形成貫通孔大小 以及高光量區域。 【0056】 陰極件並不限於LED,也可以是有機EL、氤燈、氪燈、冷 【0057】 【〇〇51】累加裝置除了用於前燈以外,亦可用作投影機等的光源。 電磁ί等t朗料’觸紐包対歧、紅外線、紫外線、 【0059】 的範圍内可以有各已,在未超出發明精神 【產業利用性】 【_】 並可 13 201000822 【圖式簡單說明】 圖1係本實施形態之光累加裝置的示意圖。 圖2係示意圖,表示在相同實施形態中從各光源射出之光線 的光束。 圖3係另一實施形態之光累加裝置的示意圖。 圖4係再另一實施形態之第2光源的示意圖。 【主要元件符號說明】 100光累加裝置 C 1第1光源 2第2光源 3第3光源 Ml第1反射鏡 M2 第2反射鏡 Mil 貫通孔 M12 反射面 M21 貫通孔 M22 反射面 I ' LI、L2、L3 光車由 L主光車由 11第1發光元件(第1LED) 12第1光學元件 121 第1LED透鏡 122第1平凸透鏡 21第2發光元件(第2LED) 22第2光學元件 221 第2LED透鏡 222 第2雙凸透鏡 2221 凹部 14 201000822 31 第 3LED 32第3光學元件 321 第3LED透鏡 322 第3雙凸透鏡 323 凹透鏡 C集光元件In the white light, the first light and the second light, and the third light is advanced together with the optical axis L3 and the optical axis L, it is possible to produce a light of a higher light amount. Further, since the light source is added along the main optical axis L, it is possible to produce light of a higher amount of light when the radial structure based on the main optical axis 1 is kept compact. Further, the present invention is not limited to the above embodiment. [0048] For example, the light accumulating device can be regarded as a unit, and then a plurality of cells are combined on the same plane to make a huge light source that can emit high-intensity light. Since the radial structure with reference to the main optical axis L of j in every j single 很 is very compact, even if a high-light ray is produced side by side in this way, it is possible to streamline the radial structure based on the squad. Further, as shown in FIG. 4, in the second optical element 22, a lenticular lens 222 of the center portion 221 2221 may be used. With these members, the light incident on the center of the lenticular lens 2 is refracted toward the portion, and a low light amount region can be formed at the center portion to form the surface light amount region Hi on the peripheral portion. In addition, the LED that emits light can be a surface light source or a point light source. [0050] The measurement area is in the low light amount 11 field 'high light amount is formed in the peripheral portion, and the light distribution characteristic of =1 is low light is formed in the central portion. [0051] ^The first light and the second light are concentrated. The light quantity is set; the output quantity 1 is further superimposed on the main optical axis in the same manner as the third light source - the light emitted from the front ^ is the second light source or the third light source can also be used in the light (four) light energy to the main light Axis 12 201000822 ^ Tilt mode setting. In this case, the configuration of the optical accumulating device can be further simplified in the radial direction based on the main optical axis. [0054] The mirror is limited to circular weaving, and it is necessary to have a reflecting surface and a through hole. For example, the mirror may have a shape in which the side surface is cut obliquely, and the cross section has a reflecting surface, and has a beacon hole penetrating from the center of the bottom surface toward the center of the butterfly. ^ The shape of the through hole of the mirror is not limited to various shapes such as a rectangular shape. Also, J rnn <d [0055] For example, a diffraction grating may be used to refract the first light and refract the second light into a low light amount region, and the optical element is not limited to the lens light beam to form the through hole size and the high light amount region. [0056] The cathode member is not limited to the LED, and may be an organic EL, a xenon lamp, a xenon lamp, or a cold. [0057] The accumulating device may be used as a light source for a projector or the like in addition to the headlight. Electromagnetic ί, etc. can be found in the range of 'touching the package, infrared, ultraviolet, and [0059], without exceeding the spirit of the invention [industrial use] [_] and 13 201000822 Fig. 1 is a schematic view of a light accumulating device of the embodiment. Fig. 2 is a schematic view showing a light beam of light emitted from each light source in the same embodiment. Figure 3 is a schematic illustration of a light accumulating device of another embodiment. Fig. 4 is a schematic view showing a second light source according to still another embodiment. [Description of main component symbols] 100 optical accumulation device C 1 first light source 2 second light source 3 third light source M1 first mirror M2 second mirror Mil through hole M12 reflection surface M21 through hole M22 reflection surface I ' LI, L2 L3 light vehicle is composed of L main light vehicle 11 first light-emitting element (first LED) 12 first optical element 121 first LED lens 122 first plano-convex lens 21 second light-emitting element (second LED) 22 second optical element 221 second LED Lens 222 second lenticular lens 2221 concave portion 14 201000822 31 third LED 32 third optical element 321 third LED lens 322 third lenticular lens 323 concave lens C light collecting element

Cl、C2平凸透鏡 Hi高光量區域 Lo低光量區域Cl, C2 plano-convex lens Hi high light area Lo low light area

Claims (1)

201000822 七、申請專利範圍: 卜一種光累加裝置,其特徵為包含:反射鏡,正面形成有反射面, 反f面的中央設有貫通孔,以該貫通孔的中心轴線與主光軸重疊 且S亥反射面對主光軸傾斜的方式配置; 第1光源,從該反射鏡的背面側向正面側射出光轴與該主光 1光線;以及第2光源,設置在偏離主光軸的位置上, f射,”部形成低光量區域且周邊部形成高光量區域的第2光 二2光線中,低光量區域的光線射人該貫通孔,高光量 二盘到該反射面上’被該反射面所反射的第2光線以 先軸。該主光軸重疊的方式隨同第}光線一起前進。 2第ΐΐΐ專ΐ範圍第1項之光累加裝置,其中,該第1 *源包含: 之該第1光線的光束收斂到該貫通牛孔的 1=弟1U讀所射出 如申味專利範圍弟1項之光累力裝 第2發光元件.以月签9古風一加衣置其中、亥弟2先源包含: 之9 ,及第2先予兀件,其讓該第2發光元件所射屮 之邊弟2光線形成該低光量區域以及該高光量區域。午斤射出 為中央部設有m卩的凸透鏡 裝置,其中,_ 2光學元件 5、如申請專利範圍第3項之光累加裝置, 光特性為在中心部形成低光量,在周邊部形成高光量^件 加裝置,其中,該第2光線全部 置複^個ΐΓίί置,其中,沿著該主光輛設 應於各反射鏡設置對其反射面射出光線 16 201000822 =源;該光線在中心部形成低光量區域,在周邊部形成高光量 低光量區域的絲射人貫通孔,高光量區域的光線照射到 隨同該第1 射的丄光=:=== 其中,該第1發光元件 8、如申請專利範圍第2項之光累加裝置, 為 LED。 9、 為=請專利範圍第3項之光累加襄置,其中,該第2發光元件 $署=照明裝置,其特徵為: 裝置當作1個單元,該照明I置月寻,圍弟1項之先累加 所構成。 糸在同一平面上並排複數個單元 項之光累加 =置:_燈’其特徵為:使用了中請專利範圍第】201000822 VII. Patent application scope: A light accumulating device, comprising: a mirror having a reflecting surface formed on the front surface, and a through hole at the center of the reverse f surface, wherein the central axis of the through hole overlaps with the main optical axis And the S-ray reflection is disposed so as to be inclined with respect to the main optical axis; the first light source emits the optical axis and the main light 1 from the back side of the mirror toward the front side; and the second light source is disposed offset from the main optical axis In the position, the second light beam is formed in the low light amount region and the high light amount region is formed in the peripheral portion, and the light in the low light amount region is incident on the through hole, and the high light amount is transmitted to the reflective surface. The second light reflected by the reflecting surface is a first axis. The manner in which the main optical axis overlaps advances along with the first light. 2 The light accumulating device of the first item, wherein the first * source comprises: The light beam of the first light converges to the 1=Dang 1U reading of the penetrating horn, and the second illuminating element of the light-filled device, such as the patent of the patent scope, is added to the second light-emitting device. Brother 2 source includes: 9th, and 2nd first The light source 2 is formed by the second light-emitting element to form the low light amount region and the high light amount region. The punch is emitted as a convex lens device having a center portion, wherein the optical element 5 is The optical accumulating device of claim 3, wherein the optical characteristic is that a low light amount is formed at the center portion, and a high light amount adding device is formed at the peripheral portion, wherein the second light is all set to be ΐΓίί, wherein The main light device is disposed on each of the mirrors to emit light to the reflecting surface thereof. 1600800822=Source; the light forms a low light amount region in the center portion, and forms a high-light amount and a low light amount region in the peripheral portion. The light of the area is irradiated with the light of the first shot ===== wherein the first light-emitting element 8 is a light accumulating device of the second item of the patent application, and is an LED. The light accumulating device of the three items, wherein the second illuminating device is a illuminating device, and the illuminating device is characterized in that: the device is regarded as one unit, and the illumination is set by the moon, and the first item of the sibling is accumulated first. Side by side on the same plane The light accumulation of a plurality of unit items = set: _ light' is characterized by the use of the patent scope
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