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TWI864286B - Laser light source depolarizer and projection device having the same - Google Patents

Laser light source depolarizer and projection device having the same Download PDF

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TWI864286B
TWI864286B TW110118818A TW110118818A TWI864286B TW I864286 B TWI864286 B TW I864286B TW 110118818 A TW110118818 A TW 110118818A TW 110118818 A TW110118818 A TW 110118818A TW I864286 B TWI864286 B TW I864286B
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laser light
light source
depolarizer
birefringent crystal
adjustment element
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TW110118818A
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TW202246852A (en
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呂俊賢
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台達電子工業股份有限公司
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Abstract

A laser light source depolarizer includes a laser light source, a light angle adjusting element, a birefringent crystal, and an integration rod. The laser light source is configured to emit a laser light. The light angle adjusting element is configured to change the diffusion angle of the laser light. The light angle adjusting element is disposed between the laser light source and the birefringent crystal. The birefringent crystal is disposed between the light angle adjusting element and the integration rod, and the birefringent crystal is configured to break the polarity of the laser light.

Description

雷射光源解偏器及具有雷射光源解偏器的投影機設備Laser light source depolarizer and projector device having the same

本揭露是有關於一種雷射光源解偏器以及具有雷射光源解偏器的投影機設備。The present disclosure relates to a laser light source depolarizer and a projector device having the laser light source depolarizer.

現行的雷射光源投影機大多採用獨立的光學系統進行光耦合,將不同顏色的雷射光源合併成單一光軸。Most current laser light source projectors use independent optical systems for optical coupling, combining laser light sources of different colors into a single optical axis.

由於雷射光為偏振光,若應用於背投影架構,則容易因為背投影架構的屏幕本身的內應力造成雷射光通過時產生色塊的現象。若將雷射光源應用於偏振式3D眼鏡,則容易使觀看者察覺不均勻的光極化性,使得視覺上產生色塊。Since laser light is polarized light, if it is used in a rear projection structure, it is easy for the internal stress of the screen of the rear projection structure to cause color blocks when the laser light passes through. If the laser light source is used in polarized 3D glasses, it is easy for the viewer to perceive the uneven polarization of the light, resulting in color blocks in vision.

有鑑於此,如何提供一種可解決上述問題的投影機系統雷射光源,仍是目前業界亟需研究的目標之一。In view of this, how to provide a laser light source for a projector system that can solve the above problems is still one of the goals that the industry urgently needs to study.

本揭露之一技術態樣為一種雷射光源解偏器。One technical aspect of the present disclosure is a laser light source depolarizer.

在本揭露一實施例中,雷射光源解偏器包含雷射光源、光束角度調整元件、雙折射晶體以及積分器。雷射光源配置以發出雷射光。光束角度調整元件配置以改變雷射光的擴散角度。光束角度調整元件位在雷射光源與雙折射晶體之間。雙折射晶體位在光束角度調整元件與積分器之間,雙折射晶體配置以破壞該雷射光的極性。In one embodiment of the present disclosure, a laser light source depolarizer includes a laser light source, a beam angle adjustment element, a birefringent crystal, and an integrator. The laser light source is configured to emit laser light. The beam angle adjustment element is configured to change the divergence angle of the laser light. The beam angle adjustment element is located between the laser light source and the birefringent crystal. The birefringent crystal is located between the beam angle adjustment element and the integrator, and the birefringent crystal is configured to destroy the polarity of the laser light.

在本揭露一實施例中,雙折射晶體面對光束角度調整元件的表面與雙折射晶體面對積分器的表面互相平行。In an embodiment of the present disclosure, a surface of the birefringent crystal facing the beam angle adjustment element and a surface of the birefringent crystal facing the integrator are parallel to each other.

在本揭露一實施例中,雙折射晶體為一體成形。In one embodiment of the present disclosure, the birefringent crystal is formed in one piece.

在本揭露一實施例中,光束角度調整元件為擴散片或透鏡。In an embodiment of the present disclosure, the beam angle adjustment element is a diffuser or a lens.

在本揭露一實施例中,雷射光源解偏器還包含光學膠層,位在光束角度調整元件與雙折射晶體之間。In one embodiment of the present disclosure, the laser light source depolarizer further includes an optical glue layer located between the beam angle adjustment element and the birefringent crystal.

在本揭露一實施例中,光學膠層接觸雙折射晶體。In one embodiment of the present disclosure, an optical adhesive layer contacts a birefringent crystal.

在本揭露一實施例中,雷射光源解偏器還包含光學膠層,位在雙折射晶體與積分器之間。In one embodiment of the present disclosure, the laser light source depolarizer further includes an optical glue layer located between the birefringent crystal and the integrator.

在本揭露一實施例中,雙折射晶體具有抗反射膜。In one embodiment of the present disclosure, the birefringent crystal has an anti-reflection film.

在本揭露一實施例中,雙折射晶體面對光束角度調整元件的表面與雙折射晶體面對積分器的表面具有夾角。In an embodiment of the present disclosure, a surface of the birefringent crystal facing the beam angle adjustment element and a surface of the birefringent crystal facing the integrator have an angle.

本揭露之另一技術態樣為一種投影機設備。Another technical aspect of the present disclosure is a projector device.

在本揭露一實施例中,投影機設備包含雷射解偏器、屏幕以及投影模組。屏幕具有位在相反兩側的投影面及觀看面。投影模組接收從積分器出來的光線,並將光線轉化為畫面投射至屏幕。投影模組位在屏幕的投影面。In an embodiment of the present disclosure, a projector device includes a laser depolarizer, a screen, and a projection module. The screen has a projection surface and a viewing surface located on opposite sides. The projection module receives light from the integrator and converts the light into an image and projects it onto the screen. The projection module is located on the projection surface of the screen.

在上述實施例中,雷射光源解偏器透過光束角度調整元件降低雷射光的光準直性以增加雷射光的擴散角度,並透過雙折射晶體破壞雷射光的光極化性。接著,透過積分器均勻化雷射光。如此一來,可使得通過積分器後的雷射光適合應用於投影機設備中,例如背投影架構或偏振式的3D眼鏡。因藉由雷射光源解偏器破壞雷射光的光準直性以及光極化性,可提升顯示畫面的均勻度、減少色塊並提高投影畫面的品質。In the above embodiment, the laser light source depolarizer reduces the light collimation of the laser light through the beam angle adjustment element to increase the diffusion angle of the laser light, and destroys the light polarization of the laser light through the birefringent crystal. Then, the laser light is uniformed through the integrator. In this way, the laser light after passing through the integrator can be suitable for application in projector equipment, such as rear projection architecture or polarized 3D glasses. Because the laser light source depolarizer destroys the light collimation and light polarization of the laser light, the uniformity of the display image can be improved, color blocks can be reduced, and the quality of the projected image can be improved.

以下將以圖式揭露本發明之複數個實施方式,為明確說明起見,許多實務上的細節將在以下敘述中一併說明。然而,應瞭解到,這些實務上的細節不應用以限制本發明。也就是說,在本發明部分實施方式中,這些實務上的細節是非必要的。此外,為簡化圖式起見,一些習知慣用的結構與元件在圖式中將以簡單示意的方式繪示之。且為了清楚起見,圖式中之層和區域的厚度可能被誇大,並且在圖式的描述中相同的元件符號表示相同的元件。The following will disclose multiple embodiments of the present invention with drawings. For the purpose of clarity, many practical details will be described together in the following description. However, it should be understood that these practical details should not be used to limit the present invention. That is to say, in some embodiments of the present invention, these practical details are not necessary. In addition, in order to simplify the drawings, some commonly used structures and components will be depicted in the drawings in a simple schematic manner. And for the sake of clarity, the thickness of the layers and regions in the drawings may be exaggerated, and the same element symbols represent the same elements in the description of the drawings.

第1圖為根據本揭露一實施例之雷射光源解偏器100的示意圖。雷射光源解偏器100包含雷射光源110、光束角度調整元件120、雙折射晶體130以及積分器140。雷射光源110配置以發出雷射光L1。光束角度調整元件120配置以改變雷射光L1的擴散角度θ。光束角度調整元件120位在雷射光源110與雙折射晶體130之間。雙折射晶體130位在光束角度調整元件120與積分器140之間。FIG. 1 is a schematic diagram of a laser light source depolarizer 100 according to an embodiment of the present disclosure. The laser light source depolarizer 100 includes a laser light source 110, a beam angle adjustment element 120, a birefringent crystal 130, and an integrator 140. The laser light source 110 is configured to emit laser light L1. The beam angle adjustment element 120 is configured to change the divergence angle θ of the laser light L1. The beam angle adjustment element 120 is located between the laser light source 110 and the birefringent crystal 130. The birefringent crystal 130 is located between the beam angle adjustment element 120 and the integrator 140.

光束角度調整元件120配置以改變雷射光L1的行進方向。換句話說,光束角度調整元件120可增加雷射光L1的擴散角度θ,以破壞雷射光L1的準直性。光束角度調整元件120、雙折射晶體130以及積分器140排列於雷射光L1的行進方向,即圖中的第一方向D1上。雙折射晶體130配置以破壞通過光束角度調整元件120後的雷射光L2的極性。積分器140配置以均勻化通過雙折射晶體130後的雷射光L3以傳輸至投影機設備的投影模組中。The beam angle adjustment element 120 is configured to change the traveling direction of the laser light L1. In other words, the beam angle adjustment element 120 can increase the diffusion angle θ of the laser light L1 to destroy the collimation of the laser light L1. The beam angle adjustment element 120, the birefringent crystal 130 and the integrator 140 are arranged in the traveling direction of the laser light L1, that is, the first direction D1 in the figure. The birefringent crystal 130 is configured to destroy the polarity of the laser light L2 after passing through the beam angle adjustment element 120. The integrator 140 is configured to uniformly transmit the laser light L3 after passing through the birefringent crystal 130 to the projection module of the projector device.

在一實施例中,光束角度調整元件120可以是擴散片。在其他實施例中,光束角度調整元件120可以是透鏡。舉例來說,光束角度調整元件120可為菲涅耳透鏡(Fresnel Lens)或者具有不同屈光度的透鏡,只要是可以增加雷射光L1的擴散角度θ以破壞雷射光L1的準直性之光學元件即可。In one embodiment, the beam angle adjustment element 120 may be a diffuser. In other embodiments, the beam angle adjustment element 120 may be a lens. For example, the beam angle adjustment element 120 may be a Fresnel lens or lenses with different refractive powers, as long as it is an optical element that can increase the diffusion angle θ of the laser light L1 to destroy the collimation of the laser light L1.

在本實施例中,通過光束角度調整元件120後的雷射光L2具有不同行進方向,使得雷射光L2進入雙折射晶體130時已具有不同的光程差。因此,在本實施例中,雙折射晶體130面對光束角度調整元件120的表面132與雙折射晶體130面對積分器140的表面134可為互相平行的。換句話說,本實施例中的雙折射晶體130可不必具有斜角。此外,本實施例中的雙折射晶體130為一體成形。在一些實施例中,雙折射晶體130面對光束角度調整元件120的表面132可具有鍍膜,例如抗反射膜(AR coating),以降低雷射光L2被反射的機率,提升雷射光L2的穿透率。在一些實施例中,雷射光源解偏器100還具有匯聚光線的透鏡(圖未示),設置在雙折射晶體130與積分器140之間,但本揭露並不以此為限。In the present embodiment, the laser light L2 after passing through the beam angle adjustment element 120 has different traveling directions, so that the laser light L2 has different optical path differences when entering the birefringent crystal 130. Therefore, in the present embodiment, the surface 132 of the birefringent crystal 130 facing the beam angle adjustment element 120 and the surface 134 of the birefringent crystal 130 facing the integrator 140 may be parallel to each other. In other words, the birefringent crystal 130 in the present embodiment does not need to have an oblique angle. In addition, the birefringent crystal 130 in the present embodiment is formed in one piece. In some embodiments, the surface 132 of the birefringent crystal 130 facing the beam angle adjustment element 120 may have a coating, such as an anti-reflection coating (AR coating), to reduce the probability of the laser light L2 being reflected and improve the transmittance of the laser light L2. In some embodiments, the laser light source depolarizer 100 further includes a lens (not shown) for converging light, which is disposed between the birefringent crystal 130 and the integrator 140, but the present disclosure is not limited thereto.

根據上述可知,本揭露的雷射光源解偏器100透過光束角度調整元件120降低雷射光L1的光準直性以增加雷射光L1的擴散角度θ,並透過雙折射晶體130破壞雷射光L2的光極化性。接著,透過積分器140均勻化雷射光L3。如此一來,可使得通過積分器140後的雷射光L4適合應用於投影機設備中。具體來說,採用多色雷射光的投影機設備,可先使各色雷射光源透過雷射光源解偏器100後再進行光耦合之操作。According to the above, the laser light source depolarizer 100 disclosed in the present invention reduces the light collimation of the laser light L1 through the beam angle adjustment element 120 to increase the diffusion angle θ of the laser light L1, and destroys the light polarization of the laser light L2 through the birefringent crystal 130. Then, the laser light L3 is uniformed through the integrator 140. In this way, the laser light L4 after passing through the integrator 140 can be suitable for application in the projector device. Specifically, the projector device using multi-color laser light can first allow each color laser light source to pass through the laser light source depolarizer 100 before performing the optical coupling operation.

第2圖為第1圖之雷射光源解偏器100應用於投影機設備10中的示意圖。投影機設備10包含雷射光源解偏器100以及投影系統200。如第1圖中所述,依序經過光束角度調整元件120、雙折射晶體130以及積分器140後的雷射光L4行進至投影系統200。在本實施例中,投影機設備10是應用在背投影架構中。投影系統200接收從積分器140出來的雷射光L4,並將雷射光L4轉化為投影畫面投射至薄型屏幕300上,且觀看者400與投影機設備10位在薄型屏幕300的相反兩側,例如投影面304與觀看面302。FIG. 2 is a schematic diagram of the laser light source depolarizer 100 of FIG. 1 being applied to the projector device 10. The projector device 10 includes the laser light source depolarizer 100 and the projection system 200. As described in FIG. 1, the laser light L4 passes through the beam angle adjustment element 120, the birefringent crystal 130 and the integrator 140 in sequence and travels to the projection system 200. In this embodiment, the projector device 10 is applied in a rear projection architecture. The projection system 200 receives the laser light L4 from the integrator 140, and converts the laser light L4 into a projection image and projects it onto the thin screen 300, and the viewer 400 and the projector device 10 are located on opposite sides of the thin screen 300, such as the projection surface 304 and the viewing surface 302.

薄型屏幕300在製造過程中,可能因加熱等製程產生內應力。當具有高準直性及單極化性的雷射光通過時,會產生不均勻的吸收效果而導致顯示畫面上出現色塊。因此,藉由雷射光源解偏器100破壞雷射光的光準直性以及光極化性,可提升顯示畫面的均勻度、減少色塊並提高投影畫面的品質。During the manufacturing process of the thin screen 300, internal stress may be generated due to heating and other processes. When the laser light with high collimation and single polarization passes through, it will produce uneven absorption effect and cause color blocks to appear on the display screen. Therefore, by destroying the light collimation and polarization of the laser light by the laser light source depolarizer 100, the uniformity of the display screen can be improved, the color blocks can be reduced, and the quality of the projected screen can be improved.

在一些其他實施例中,雷射光源解偏器100也可應用於搭配偏振式的3D眼鏡的投影設備。由於雷射光具有高極化性的,觀看者透過偏振式的3D眼鏡容易察覺不均勻的光極化性。因此,藉由雷射光源解偏器100破壞雷射光的光準直性以及光極化性,可提升顯示畫面的均勻度、減少色塊並提高投影畫面的品質。In some other embodiments, the laser light source depolarizer 100 can also be applied to a projection device that is used with polarized 3D glasses. Since laser light has high polarization, viewers can easily perceive uneven light polarization through polarized 3D glasses. Therefore, by destroying the light collimation and light polarization of the laser light through the laser light source depolarizer 100, the uniformity of the displayed image can be improved, color blocks can be reduced, and the quality of the projected image can be improved.

第3圖為根據本揭露另一實施例之雷射光源解偏器100a的示意圖。雷射光源解偏器100a與第1圖所示的雷射光源解偏器100大致相同,其差異在於雷射光源解偏器100a還包含位在光束角度調整元件120與雙折射晶體130之間的光學膠層150。在此實施例中,光學膠層150黏合光束角度調整元件120與雙折射晶體130。換句話說,光學膠層150接觸雙折射晶體130的表面132a。光學膠層150可減少雷射光L2的界面反射,因此雙折射晶體130a的表面132a可不必具有前述的抗反射膜。此外,由於光學膠層150可具有較薄的厚度,因此可避免產生光減損的影響。FIG. 3 is a schematic diagram of a laser light source depolarizer 100a according to another embodiment of the present disclosure. The laser light source depolarizer 100a is substantially the same as the laser light source depolarizer 100 shown in FIG. 1, except that the laser light source depolarizer 100a further includes an optical adhesive layer 150 located between the beam angle adjustment element 120 and the birefringent crystal 130. In this embodiment, the optical adhesive layer 150 bonds the beam angle adjustment element 120 and the birefringent crystal 130. In other words, the optical adhesive layer 150 contacts the surface 132a of the birefringent crystal 130. The optical adhesive layer 150 can reduce the interface reflection of the laser light L2, so the surface 132a of the birefringent crystal 130a does not need to have the aforementioned anti-reflection film. In addition, since the optical adhesive layer 150 can have a thinner thickness, the effect of light loss can be avoided.

在本實施例中,雷射光源解偏器100a還包含位在雙折射晶體130與積分器140之間的光學膠層160。光學膠層160黏合雙折射晶體130與積分器140。在一些實施例中,雷射光源解偏器100a也可以只具有光學膠層160,而不具有光學膠層150。雷射光源解偏器100a與第1圖所示的雷射光源解偏器100具有相同的技術功效,於此不再贅述。In this embodiment, the laser light source depolarizer 100a further includes an optical adhesive layer 160 between the birefringent crystal 130 and the integrator 140. The optical adhesive layer 160 bonds the birefringent crystal 130 and the integrator 140. In some embodiments, the laser light source depolarizer 100a may also only have the optical adhesive layer 160 without the optical adhesive layer 150. The laser light source depolarizer 100a has the same technical effects as the laser light source depolarizer 100 shown in FIG. 1, and will not be described in detail here.

第4圖為根據本揭露另一實施例之雷射光源解偏器100b的示意圖。雷射光源解偏器100b與第1圖所示的雷射光源解偏器100大致相同,其差異在於雷射光源解偏器100b的雙折射晶體130b為楔形。雙折射晶體130b的表面132a與表面134a具有夾角。換句話說,雙折射晶體130b可使雷射光L2進一步形成光程差,以破壞雷射光L2的光極化性。雷射光源解偏器100b也可具有匯聚光線的透鏡(圖未示),設置在雙折射晶體130b與積分器140之間,但本揭露並不以此為限。FIG. 4 is a schematic diagram of a laser light source depolarizer 100b according to another embodiment of the present disclosure. The laser light source depolarizer 100b is substantially the same as the laser light source depolarizer 100 shown in FIG. 1, except that the birefringent crystal 130b of the laser light source depolarizer 100b is wedge-shaped. The surface 132a and the surface 134a of the birefringent crystal 130b have an angle. In other words, the birefringent crystal 130b can cause the laser light L2 to further form an optical path difference to destroy the optical polarization of the laser light L2. The laser light source depolarizer 100b may also have a lens (not shown) for converging light, which is disposed between the birefringent crystal 130b and the integrator 140, but the present disclosure is not limited thereto.

第5圖為根據本揭露另一實施例之雷射光源解偏器100c的示意圖。雷射光源解偏器100c與第4圖所示的雷射光源解偏器100b大致相同,其差異在於雷射光源解偏器100c的雙折射晶體130c由兩個楔形的雙折射材料136、138構成。雙折射材料136、138互相配合,使雷射光L2進一步形成光程差,並且使雷射光L2在穿透過雙折射晶體130c後的擴散角度θ不變,以破壞雷射光L2的光極化性。雷射光源解偏器100c也可具有匯聚光線的透鏡(圖未示),設置在雙折射晶體130c與積分器140之間,但本揭露並不以此為限。FIG. 5 is a schematic diagram of a laser light source depolarizer 100c according to another embodiment of the present disclosure. The laser light source depolarizer 100c is substantially the same as the laser light source depolarizer 100b shown in FIG. 4, except that the birefringent crystal 130c of the laser light source depolarizer 100c is composed of two wedge-shaped birefringent materials 136 and 138. The birefringent materials 136 and 138 cooperate with each other to further form an optical path difference for the laser light L2, and to keep the diffusion angle θ of the laser light L2 unchanged after passing through the birefringent crystal 130c, so as to destroy the optical polarization of the laser light L2. The laser light source depolarizer 100c may also have a lens (not shown) for converging light, which is disposed between the birefringent crystal 130c and the integrator 140, but the present disclosure is not limited thereto.

綜上所述,本揭露的雷射光源解偏器透過光束角度調整元件降低雷射光的光準直性以增加雷射光的擴散角度,並透過雙折射晶體破壞雷射光的光極化性。接著,透過積分器均勻化雷射光。如此一來,可使得通過積分器後的雷射光適合應用於投影機設備中,例如背投影架構或偏振式的3D眼鏡。因藉由雷射光源解偏器破壞雷射光的光準直性以及光極化性,可提升顯示畫面的均勻度、減少色塊並提高投影畫面的品質。In summary, the laser light source depolarizer disclosed in the present invention reduces the light collimation of the laser light through the beam angle adjustment element to increase the diffusion angle of the laser light, and destroys the light polarization of the laser light through the birefringent crystal. Then, the laser light is uniformed through the integrator. In this way, the laser light after passing through the integrator can be suitable for application in projector equipment, such as rear projection structure or polarized 3D glasses. Because the laser light source depolarizer destroys the light collimation and light polarization of the laser light, the uniformity of the display image can be improved, color blocks can be reduced, and the quality of the projected image can be improved.

雖然本發明已以實施方式揭露如上,然其並非用以限定本發明,任何熟習此技藝者,在不脫離本發明之精神和範圍內,當可作各種之更動與潤飾,因此本發明之保護範圍當視後附之申請專利範圍所界定者為準。Although the present invention has been disclosed in the above embodiments, it is not intended to limit the present invention. Anyone skilled in the art can make various changes and modifications without departing from the spirit and scope of the present invention. Therefore, the protection scope of the present invention shall be subject to the scope defined in the attached patent application.

100,100a,100b,100c:雷射光源解偏器 110:雷射光源 120:光束角度調整元件 130:雙折射晶體 140:積分器 150,160:光學膠層 132,134,132a,134a,132b,134b:表面 136,138:雙折射材料 200:投影系統 300:薄型屏幕 302:觀看面 304:投影面 400:觀看者 L1,L2,L3,L4:雷射光 D1:第一方向 θ:擴散角度 100,100a,100b,100c: laser light source depolarizer 110: laser light source 120: beam angle adjustment element 130: birefringent crystal 140: integrator 150,160: optical glue layer 132,134,132a,134a,132b,134b: surface 136,138: birefringent material 200: projection system 300: thin screen 302: viewing surface 304: projection surface 400: viewer L1,L2,L3,L4: laser light D1: first direction θ: diffusion angle

第1圖為根據本揭露一實施例之雷射光源解偏器的示意圖。 第2圖為第1圖之雷射光源解偏器應用於投影機設備中的示意圖。 第3圖為根據本揭露另一實施例之雷射光源解偏器的示意圖。 第4圖為根據本揭露另一實施例之雷射光源解偏器的示意圖。 第5圖為根據本揭露另一實施例之雷射光源共軸設備的示意圖。 FIG. 1 is a schematic diagram of a laser light source depolarizer according to an embodiment of the present disclosure. FIG. 2 is a schematic diagram of the laser light source depolarizer of FIG. 1 applied to a projector device. FIG. 3 is a schematic diagram of a laser light source depolarizer according to another embodiment of the present disclosure. FIG. 4 is a schematic diagram of a laser light source depolarizer according to another embodiment of the present disclosure. FIG. 5 is a schematic diagram of a laser light source coaxial device according to another embodiment of the present disclosure.

100:雷射光源解偏器 100: Laser light source depolarizer

110:雷射光源 110:Laser light source

120:光束角度調整元件 120: Beam angle adjustment element

130:雙折射晶體 130: Birefringent crystal

140:積分器 140: Integrator

132,134:表面 132,134:Surface

L1,L2,L3,L4:雷射光 L1, L2, L3, L4: Laser light

D1:第一方向 D1: First direction

θ:擴散角度 θ: Diffusion angle

Claims (10)

一種雷射光源解偏器,包含:一雷射光源,配置以發出一第一雷射光;一光束角度調整元件,配置以改變該第一雷射光的一擴散角度以產生一第二雷射光;一雙折射晶體,其中該光束角度調整元件位在該雷射光源與該雙折射晶體之間,其中具有不同行進方向的該第二雷射光通過該雙折射晶體,且該雙折射晶體配置以破壞該第二雷射光的極性;以及一積分器,其中該雙折射晶體位在該光束角度調整元件與該積分器之間。 A laser light source depolarizer comprises: a laser light source configured to emit a first laser light; a beam angle adjustment element configured to change a diffusion angle of the first laser light to generate a second laser light; a birefringent crystal, wherein the beam angle adjustment element is located between the laser light source and the birefringent crystal, wherein the second laser light with different traveling directions passes through the birefringent crystal, and the birefringent crystal is configured to destroy the polarity of the second laser light; and an integrator, wherein the birefringent crystal is located between the beam angle adjustment element and the integrator. 如請求項1所述之雷射光源解偏器,其中該雙折射晶體面對該光束角度調整元件的表面與該雙折射晶體面對該積分器的表面互相平行。 The laser light source depolarizer as described in claim 1, wherein the surface of the birefringent crystal facing the beam angle adjustment element and the surface of the birefringent crystal facing the integrator are parallel to each other. 如請求項1所述之雷射光源解偏器,其中該雙折射晶體為一體成形。 A laser light source depolarizer as described in claim 1, wherein the birefringent crystal is formed in one piece. 如請求項1所述之雷射光源解偏器,其中該光束角度調整元件為擴散片或透鏡。 A laser light source depolarizer as described in claim 1, wherein the beam angle adjustment element is a diffuser or a lens. 如請求項1所述之雷射光源解偏器,還包含一光學膠層,位在該光束角度調整元件與該雙折射晶體之 間。 The laser light source depolarizer as described in claim 1 further comprises an optical glue layer located between the beam angle adjustment element and the birefringent crystal. 如請求項5所述之雷射光源解偏器,其中該光學膠層接觸該雙折射晶體。 A laser light source depolarizer as described in claim 5, wherein the optical glue layer contacts the birefringent crystal. 如請求項1所述之雷射光源解偏器,還包含一光學膠層,位在該雙折射晶體與該積分器之間。 The laser light source depolarizer as described in claim 1 further comprises an optical glue layer located between the birefringent crystal and the integrator. 如請求項1所述之雷射光源解偏器,其中該雙折射晶體具有一抗反射膜。 A laser light source depolarizer as described in claim 1, wherein the birefringent crystal has an anti-reflection film. 如請求項1所述之雷射光源解偏器,其中該雙折射晶體面對該光束角度調整元件的表面與該雙折射晶體面對該積分器的表面具有一夾角。 The laser light source depolarizer as described in claim 1, wherein the surface of the birefringent crystal facing the beam angle adjustment element and the surface of the birefringent crystal facing the integrator have an angle. 一種投影機設備,包含:如請求項1所述的雷射光源解偏器;一屏幕,具有位在相反兩側的一投影面及一觀看面;以及一投影模組,接收從該積分器出來的光線,並將該光線轉化為畫面投射至該屏幕;其中,該投影模組位在該屏幕的投影面。 A projector device, comprising: a laser light source depolarizer as described in claim 1; a screen having a projection surface and a viewing surface located on opposite sides; and a projection module, receiving light from the integrator and converting the light into an image to be projected onto the screen; wherein the projection module is located on the projection surface of the screen.
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Citations (4)

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Publication number Priority date Publication date Assignee Title
TW200613926A (en) * 2004-06-21 2006-05-01 Canon Kk Illumination optical system, exposure apparatus, and device manufacturing method
US20100202725A1 (en) * 2007-07-26 2010-08-12 Sbg Labs Inc. Laser illumination device
TW201248297A (en) * 2011-03-28 2012-12-01 Casio Computer Co Ltd Projecting device, projecting method and recording media
TWI444748B (en) * 2008-05-15 2014-07-11 Eastman Kodak Co Laser projection using spatial and temporal mixing

Patent Citations (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
TW200613926A (en) * 2004-06-21 2006-05-01 Canon Kk Illumination optical system, exposure apparatus, and device manufacturing method
US20100202725A1 (en) * 2007-07-26 2010-08-12 Sbg Labs Inc. Laser illumination device
TWI444748B (en) * 2008-05-15 2014-07-11 Eastman Kodak Co Laser projection using spatial and temporal mixing
TW201248297A (en) * 2011-03-28 2012-12-01 Casio Computer Co Ltd Projecting device, projecting method and recording media

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