TW202219134A - Radiation device, radiative cooling device, and method for manufacturing radiation device - Google Patents

Radiation device, radiative cooling device, and method for manufacturing radiation device Download PDF

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TW202219134A
TW202219134A TW110130841A TW110130841A TW202219134A TW 202219134 A TW202219134 A TW 202219134A TW 110130841 A TW110130841 A TW 110130841A TW 110130841 A TW110130841 A TW 110130841A TW 202219134 A TW202219134 A TW 202219134A
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conductor
flexible film
radiation device
mentioned
disks
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TW110130841A
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大塚節文
江畑惠司
井上武
髙原淳一
君野和也
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國立大學法人大阪大學
日商住友電氣工業股份有限公司
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    • BPERFORMING OPERATIONS; TRANSPORTING
    • B32LAYERED PRODUCTS
    • B32BLAYERED PRODUCTS, i.e. PRODUCTS BUILT-UP OF STRATA OF FLAT OR NON-FLAT, e.g. CELLULAR OR HONEYCOMB, FORM
    • B32B3/00Layered products comprising a layer with external or internal discontinuities or unevennesses, or a layer of non-planar shape; Layered products comprising a layer having particular features of form
    • B32B3/10Layered products comprising a layer with external or internal discontinuities or unevennesses, or a layer of non-planar shape; Layered products comprising a layer having particular features of form characterised by a discontinuous layer, i.e. formed of separate pieces of material
    • B32B3/14Layered products comprising a layer with external or internal discontinuities or unevennesses, or a layer of non-planar shape; Layered products comprising a layer having particular features of form characterised by a discontinuous layer, i.e. formed of separate pieces of material characterised by a face layer formed of separate pieces of material which are juxtaposed side-by-side
    • BPERFORMING OPERATIONS; TRANSPORTING
    • B32LAYERED PRODUCTS
    • B32BLAYERED PRODUCTS, i.e. PRODUCTS BUILT-UP OF STRATA OF FLAT OR NON-FLAT, e.g. CELLULAR OR HONEYCOMB, FORM
    • B32B7/00Layered products characterised by the relation between layers; Layered products characterised by the relative orientation of features between layers, or by the relative values of a measurable parameter between layers, i.e. products comprising layers having different physical, chemical or physicochemical properties; Layered products characterised by the interconnection of layers
    • B32B7/02Physical, chemical or physicochemical properties
    • B32B7/025Electric or magnetic properties
    • CCHEMISTRY; METALLURGY
    • C08ORGANIC MACROMOLECULAR COMPOUNDS; THEIR PREPARATION OR CHEMICAL WORKING-UP; COMPOSITIONS BASED THEREON
    • C08JWORKING-UP; GENERAL PROCESSES OF COMPOUNDING; AFTER-TREATMENT NOT COVERED BY SUBCLASSES C08B, C08C, C08F, C08G or C08H
    • C08J5/00Manufacture of articles or shaped materials containing macromolecular substances
    • C08J5/18Manufacture of films or sheets
    • FMECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
    • F25REFRIGERATION OR COOLING; COMBINED HEATING AND REFRIGERATION SYSTEMS; HEAT PUMP SYSTEMS; MANUFACTURE OR STORAGE OF ICE; LIQUEFACTION SOLIDIFICATION OF GASES
    • F25BREFRIGERATION MACHINES, PLANTS OR SYSTEMS; COMBINED HEATING AND REFRIGERATION SYSTEMS; HEAT PUMP SYSTEMS
    • F25B23/00Machines, plants or systems, with a single mode of operation not covered by groups F25B1/00 - F25B21/00, e.g. using selective radiation effect

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  • Polymers & Plastics (AREA)
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  • Structure Of Printed Boards (AREA)
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Abstract

This radiation device comprises a flexible film, an electroconductive layer provided on the flexible film, a semiconductor layer provided on the electroconductive layer, and a plurality of electroconductive discs that are provided on the semiconductor layer and that are positioned so as to be set apart from each other.

Description

輻射裝置、放射冷卻裝置及製造輻射裝置之方法Radiation device, radiation cooling device and method of making radiation device

本揭示係關於一種輻射裝置、放射冷卻裝置及製造輻射裝置之方法。本申請案基於2020年11月6日提出申請之日本專利申請案第2020-185732號而主張優先權,且援用上述日本專利申請案所記載之全部內容。The present disclosure relates to a radiation device, a radiation cooling device, and a method of manufacturing the radiation device. This application claims priority based on Japanese Patent Application No. 2020-185732 for which it applied on November 6, 2020, and uses all the contents described in the above Japanese Patent Application.

專利文獻1揭示一種選擇性放射冷卻構造體,該選擇性放射冷卻構造體具備:選擇性放出層,其包含聚合物、及分散於聚合物中之複數個介電質粒子。於製作微小球體分散之構造物之情形,有微小球體凝聚之情況。Patent Document 1 discloses a selective radiation cooling structure including a selective emission layer including a polymer and a plurality of dielectric particles dispersed in the polymer. In the case of making a structure in which the microspheres are dispersed, there are cases where the microspheres agglomerate.

專利文獻2揭示一種利用電漿子超穎材料之輻射裝置。因輻射裝置使用微影技術製作,故形成於具有平滑表面之矽基板上。 [先前技術文獻] [專利文獻] Patent Document 2 discloses a radiation device using a plasmonic metamaterial. Since the radiation device is fabricated using lithography, it is formed on a silicon substrate with a smooth surface. [Prior Art Literature] [Patent Literature]

專利文獻1:日本專利特表2019-515967號公報 專利文獻2:國際公開第2020/026345號 Patent Document 1: Japanese Patent Publication No. 2019-515967 Patent Document 2: International Publication No. 2020/026345

本揭示之一態樣之輻射裝置具備:可撓性膜;導電體層,其設置於上述可撓性膜上;半導體層,其設置於上述導電體層上;及複數個導電體碟,其等設置於上述半導體層上,且彼此隔開配置。A radiation device according to one aspect of the present disclosure includes: a flexible film; a conductor layer provided on the flexible film; a semiconductor layer provided on the conductor layer; and a plurality of conductive disks, etc. provided on the above-mentioned semiconductor layer, and are arranged apart from each other.

[本揭示所欲解決之問題] 國際公開第2020/026345號未揭示將輻射裝置搭載於具有彎曲表面之構件上之情況。 [Problems to be solved by this disclosure] International Publication No. 2020/026345 does not disclose that the radiation device is mounted on a member having a curved surface.

本揭示提供一種可彎曲之輻射裝置、放射冷卻裝置及製造輻射裝置之方法。The present disclosure provides a bendable radiation device, a radiation cooling device, and a method of manufacturing the radiation device.

[本揭示之效果] 根據本揭示,可提供一種可彎曲之輻射裝置、放射冷卻裝置及製造輻射裝置之方法。 [Effect of this disclosure] According to the present disclosure, a bendable radiation device, a radiation cooling device, and a method of manufacturing the radiation device can be provided.

[本揭示之實施形態之說明] 一實施形態之輻射裝置具備:可撓性膜;導電體層,其設置於上述可撓性膜上;半導體層,其設置於上述導電體層上;及複數個導電體碟,其等設置於上述半導體層上,且彼此隔開配置。 [Description of Embodiments of the Present Disclosure] A radiation device according to an embodiment includes: a flexible film; a conductor layer provided on the flexible film; a semiconductor layer provided on the conductor layer; and a plurality of conductor disks provided on the semiconductor layers, and are arranged spaced apart from each other.

根據上述輻射裝置,可藉由使可撓性膜彎曲,而使輻射裝置彎曲。According to the above radiation device, the radiation device can be bent by bending the flexible film.

亦可為,上述導電體層設置於上述可撓性膜之主面上,上述可撓性膜可以上述主面具有60 mm以下之曲率半徑之方式彎曲。於該情形時,可使輻射裝置較大彎曲。The conductor layer may be provided on the main surface of the flexible film, and the flexible film may be curved so that the main surface has a radius of curvature of 60 mm or less. In this case, the radiation device can be bent more.

亦可為,於以上述主面具有60 mm之曲率半徑之方式彎曲上述可撓性膜之情形,上述複數個導電體碟之各者之尺寸變化率之絕對值、與相鄰之上述複數個導電體碟間之間隔之尺寸變化率之絕對值在10%以下。於該情形時,即便使輻射裝置較大彎曲,亦可使各導電體碟及各間隔之尺寸變化率較小。藉此,可使尺寸變化引起之吸收波長之偏差之絕對值小至例如5 μm以下。In the case where the flexible film is bent so that the main surface has a radius of curvature of 60 mm, the absolute value of the dimensional change rate of each of the plurality of conductive discs and the adjacent plurality of The absolute value of the dimensional change rate of the spacing between the conductor discs is below 10%. In this case, even if the radiation device is made to bend more, the dimensional change rate of each conductor disk and each space can be made small. Thereby, the absolute value of the deviation of the absorption wavelength due to the dimensional change can be reduced to, for example, 5 μm or less.

上述可撓性膜亦可包含樹脂。上述可撓性膜亦可包含聚醯亞胺。The above-mentioned flexible film may contain resin. The above-mentioned flexible film may also contain polyimide.

亦可為,上述複數個導電體碟以於上述半導體層之主面中具有同一面積及同一形狀之複數個單位構成區域之各者具有相同配置圖案之方式配置,上述複數個單位構成區域之各者具有矩形形狀,該矩形形狀具有4.5 μm以上5.5 μm以下之長度之各邊,上述複數個單位構成區域以於沿上述主面彼此正交之2個方向之各者中相鄰之單位構成區域彼此具有共通之邊之方式陣列配置。於該情形時,輻射裝置可選擇性地放出與4.5 μm以上5.5 μm以下之波長域相當之「大氣窗口」之電磁波。The plurality of conductor disks may be arranged in such a manner that each of the plurality of unit constituent regions having the same area and the same shape has the same arrangement pattern on the principal surface of the above-mentioned semiconductor layer, and each of the plurality of unit constituent regions may be arranged in the same arrangement pattern. It has a rectangular shape with each side having a length of 4.5 μm or more and 5.5 μm or less, and the plurality of unit constituting regions are adjacent to each other in each of the two directions along the above-mentioned main surfaces that are orthogonal to each other. Arrays are arranged in such a way that they have a common edge with each other. In this case, the radiation device can selectively emit electromagnetic waves in the "atmospheric window" corresponding to the wavelength range of 4.5 μm to 5.5 μm.

亦可為,上述配置圖案藉由以與沿上述矩形形狀之第1邊排列3個導電體碟且沿與上述第1邊正交之第2邊排列3個導電體碟之3×3之矩陣對應之方式配置之9個導電體碟構成,上述9個導電體碟包含具有彼此不同之直徑之4種以上之導電體碟。於該情形時,可於具有4.5 μm以上5.5 μm以下之長度之各邊之矩形形狀內適當地配置9個導電體碟。The above-mentioned arrangement pattern may be formed by a 3×3 matrix in which three conductor disks are arranged along the first side of the rectangular shape and three conductor disks are arranged along the second side orthogonal to the first side. It is composed of 9 conductor disks arranged in a corresponding manner, and the 9 conductor disks include 4 or more types of conductor disks having mutually different diameters. In this case, nine conductor disks can be appropriately arranged in a rectangular shape having a length of 4.5 μm or more and 5.5 μm or less on each side.

一實施形態之放射冷卻裝置具備具有彎曲表面之構件、與上述輻射裝置,且上述輻射裝置以上述可撓性膜面向上述彎曲表面之方式設置於上述構件上。於該情形時,可以追隨彎曲表面之方式使可撓性膜彎曲。A radiation cooling device according to an embodiment includes a member having a curved surface, and the radiation device, and the radiation device is provided on the member so that the flexible film faces the curved surface. In this case, the flexible membrane can be bent in such a way as to follow the curved surface.

製造一實施形態之輻射裝置之方法包含以下步驟:於基板上設置可撓性膜;於上述可撓性膜上,依序形成導電體層、半導體層、彼此隔開配置之複數個導電體碟;及將上述可撓性膜自上述基板剝離。The method of manufacturing the radiation device of one embodiment includes the following steps: disposing a flexible film on a substrate; forming a conductor layer, a semiconductor layer, and a plurality of conductor disks spaced apart from each other in sequence on the flexible film; And peeling the said flexible film from the said board|substrate.

根據上述製造輻射裝置之方法,可獲得具備可撓性膜之輻射裝置。According to the above-described method of manufacturing a radiation device, a radiation device provided with a flexible film can be obtained.

設置上述可撓性膜之步驟亦可包含將上述可撓性膜藉由接著劑層接著於上述基板。於該情形時,可抑制可撓性膜相對於基板之位置偏移。The step of disposing the above-mentioned flexible film may also include bonding the above-mentioned flexible film to the above-mentioned substrate through an adhesive layer. In this case, positional displacement of the flexible film with respect to the substrate can be suppressed.

[本揭示之實施形態之細節] 以下,參照附加圖式且詳細說明本揭示之實施形態。於圖式之說明中,對同一或同等之要件使用同一符號,省略重複說明。於圖式中,根據需要,顯示彼此交叉之X軸方向、Y軸方向及Z軸方向。X軸方向、Y軸方向及Z軸方向例如彼此正交。 [Details of Embodiments of the Present Disclosure] Hereinafter, embodiments of the present disclosure will be described in detail with reference to the accompanying drawings. In the description of the drawings, the same symbols are used for the same or equivalent elements, and repeated descriptions are omitted. In the drawings, the X-axis direction, the Y-axis direction, and the Z-axis direction which intersect with each other are shown as needed. The X-axis direction, the Y-axis direction, and the Z-axis direction are, for example, orthogonal to each other.

圖1係模式性顯示一實施形態之輻射裝置之剖視圖。圖1所示之輻射裝置100具備:可撓性膜110;導電體層120,其設置於可撓性膜110上;半導體層130,其設置於導電體層120上;及複數個導電體碟150,其等設置於半導體層130上。FIG. 1 is a cross-sectional view schematically showing a radiation device according to an embodiment. The radiation device 100 shown in FIG. 1 includes: a flexible film 110; a conductor layer 120 disposed on the flexible film 110; a semiconductor layer 130 disposed on the conductor layer 120; and a plurality of conductor disks 150, They are disposed on the semiconductor layer 130 .

可撓性膜110具有於Z軸方向中彼此配置於相反側之下表面110a及上表面110b(主面)。Z軸方向相當於可撓性膜110之厚度方向。導電體層120設置於可撓性膜110之上表面110b上。導電體層120具有面向上表面110b之下表面120a、及與下表面120a為相反側之上表面120b。半導體層130設置於導電體層120之上表面120b上。半導體層130具有面向上表面120b之下表面130a、及與下表面130a為相反側之上表面130b(主面)。複數個導電體碟150設置於半導體層130之上表面120b上,且彼此隔開配置。各導電體碟150自Z軸方向觀察例如具有圓形。於半導體層130之上表面130b上,為保護複數個導電體碟150及防止光自外部入射等,亦可以覆蓋複數個導電體碟150之方式設置表面保護層140。表面保護層140亦可作為反射膜發揮功能。The flexible film 110 has a lower surface 110a and an upper surface 110b (main surface) which are arranged on the opposite sides to each other in the Z-axis direction. The Z-axis direction corresponds to the thickness direction of the flexible film 110 . The conductor layer 120 is disposed on the upper surface 110b of the flexible film 110 . The conductor layer 120 has a lower surface 120a facing the upper surface 110b, and an upper surface 120b opposite to the lower surface 120a. The semiconductor layer 130 is disposed on the upper surface 120b of the conductor layer 120 . The semiconductor layer 130 has a lower surface 130a facing the upper surface 120b, and an upper surface 130b (main surface) opposite to the lower surface 130a. A plurality of conductive disks 150 are disposed on the upper surface 120b of the semiconductor layer 130 and are spaced apart from each other. Each conductor disk 150 has, for example, a circular shape when viewed from the Z-axis direction. On the upper surface 130b of the semiconductor layer 130, a surface protection layer 140 can also be provided to cover the plurality of conductor disks 150 to protect the plurality of conductor disks 150 and prevent light from being incident from the outside. The surface protective layer 140 can also function as a reflective film.

可撓性膜110亦可包含樹脂。樹脂之例包含聚醯亞胺。可撓性膜110亦可包含例如具有0.5 GPa以上100 GPa以下之楊氏模量之材料。可撓性膜110之厚度為例如1 μm以上300 μm以下。可撓性膜110亦可包含無機材料。可撓性膜110亦可為例如具有20 μm以上500 μm以下之厚度之薄玻璃板(例如日本電玻璃公司製之G-Leaf(註冊商標)等)。可撓性膜110可具有對有機溶劑及強酸較高之耐性。可撓性膜110之上表面130b之50 μm左右之區域(基準長度)之平均表面粗度Ra(算數平均粗度)亦可為5 nm以下。於可撓性膜110之上表面130b設置有高度100 nm左右之針狀突起之情形時,針狀突起可藉由氧電漿處理(灰化)等去除。此外,可撓性膜110之上表面130b之全面積(遍及全體之基準長度)之平均表面粗度Ra亦可為500 nm以下。The flexible film 110 may also contain resin. Examples of resins include polyimides. The flexible film 110 may also include, for example, a material having a Young's modulus of 0.5 GPa or more and 100 GPa or less. The thickness of the flexible film 110 is, for example, 1 μm or more and 300 μm or less. The flexible film 110 may also include inorganic materials. The flexible film 110 may be, for example, a thin glass plate having a thickness of not less than 20 μm and not more than 500 μm (eg, G-Leaf (registered trademark) manufactured by Nippon Denki Glass Co., Ltd.). The flexible film 110 may have higher resistance to organic solvents and strong acids. The average surface roughness Ra (arithmetic average roughness) of the region (reference length) of the upper surface 130b of the flexible film 110 about 50 μm may be 5 nm or less. When the upper surface 130b of the flexible film 110 is provided with needle-like protrusions with a height of about 100 nm, the needle-like protrusions can be removed by oxygen plasma treatment (ashing). In addition, the average surface roughness Ra of the entire area of the upper surface 130b of the flexible film 110 (the reference length over the entirety) may be 500 nm or less.

導電體層120亦可包含金屬。金屬之例包含鋁(Al)、金(Au)、銀(Ag)及銅(Cu)。導電體層120之厚度亦可大於導電體碟150之厚度。導電體層120之厚度亦可為100 nm以上200 nm以下。若增大導電體層120之厚度,則可抑制電磁波之透過。The conductor layer 120 may also include metal. Examples of metals include aluminum (Al), gold (Au), silver (Ag), and copper (Cu). The thickness of the conductor layer 120 may also be greater than the thickness of the conductor disk 150 . The thickness of the conductor layer 120 may be not less than 100 nm and not more than 200 nm. If the thickness of the conductor layer 120 is increased, the transmission of electromagnetic waves can be suppressed.

半導體層130亦可包含矽(Si)及鍺(Ge)之至少1者。於該情形時,於中紅外波長域即短於8 μm之波長域中,半導體層130之吸收率變小。半導體層130之厚度亦可為100 nm以上1000 nm以下。The semiconductor layer 130 may also include at least one of silicon (Si) and germanium (Ge). In this case, in the mid-infrared wavelength region, that is, in the wavelength region shorter than 8 μm, the absorptivity of the semiconductor layer 130 becomes small. The thickness of the semiconductor layer 130 may also be 100 nm or more and 1000 nm or less.

複數個導電體碟150之各者亦可包含金屬。金屬之例包含與導電體層120之材料之例相同之材料。為提高形狀之控制性及抑制製造成本,各導電體碟150之厚度亦可為30 nm以上100 nm以下。於該情形時,即使輻射特性因導電體碟150厚度之變化而變化,亦可於波長8 μm以上13 μm以下之波長域中獲得足夠之輻射率。各導電體碟150之尺寸(直徑)可以於0.8 μm以上1.5 μm以下之範圍內重複FDTD法(Finite-difference time-domain:有限差分時域法)之解析,於8 μm以上13 μm以下之波長域中獲得高輻射率之方式選擇。Each of the plurality of conductor disks 150 may also include metal. The example of the metal includes the same material as the example of the material of the conductor layer 120 . In order to improve the controllability of the shape and reduce the manufacturing cost, the thickness of each conductor disk 150 may be not less than 30 nm and not more than 100 nm. In this case, even if the radiation characteristics vary due to the thickness of the conductor disk 150, a sufficient emissivity can be obtained in the wavelength region of 8 μm to 13 μm. The size (diameter) of each conductor disk 150 can repeat the analysis of the FDTD method (Finite-difference time-domain: finite difference time domain method) in the range of 0.8 μm to 1.5 μm, and the wavelength of 8 μm to 13 μm. The choice of way to obtain high emissivity in the domain.

圖2係顯示陣列配置之複數個單位構成區域之俯視圖。圖3係顯示各單位構成區域之導電體碟之配置圖案之俯視圖。以下,對圖2及圖3之例進行說明。導電體碟之配置圖案未限定於本例。FIG. 2 is a top view showing a plurality of unit constituent regions of an array configuration. FIG. 3 is a plan view showing the arrangement pattern of the conductor disks in each unit constituting region. Hereinafter, the example of FIG. 2 and FIG. 3 is demonstrated. The arrangement pattern of the conductor disks is not limited to this example.

複數個導電體碟150可以於半導體層130之上表面130b中具有同一面積及同一形狀之複數個單位構成區域R之各者具有相同配置圖案之方式配置。複數個單位構成R之各者亦可具有矩形形狀,該矩形形狀具有4.5 μm以上5.5 μm以下之長度之各邊。夾著1個內角而相鄰之2邊之長度亦可彼此不同,又可彼此相等。於本例中,複數個單位構成區域R之各者具有正方形狀,該正方形狀具有4.5 μm以上5.5 μm以下之長度之各邊。複數個單位構成區域R可以於沿上表面130b之彼此正交之X軸方向及Y軸方向之各者中相鄰之單位構成區域R彼此具有共通之邊之方式陣列配置。複數個單位構成區域R無間隙配置。藉此,於上表面130b中,構成複數個導電體碟150之配置圖案之二維週期構造。二維週期構造係產生中紅外波長域之電磁波之紅外電漿子週期構造。單位構成區域R之一邊之長度相當於二維週期構造之週期間距P。於本例中,各單位構成區域R之配置圖案藉由以對應3×3之矩陣之方式配置之9個導電體碟150而構成。於3×3之矩陣中,沿矩形形狀之第1邊排列3個導電體碟150且沿與第1邊正交之第2邊排列3個導電體碟150。於線a1、a2及a3、與線b1、b2及b3之9個交點(格柵點)C之各者,配置對應之導電體碟150。各導電體碟150之中心與各交點C一致。線a1、a2及a3平行於X軸方向延伸,於Y軸方向等間隔設定。線b1、b2及b3平行於Y軸方向延伸,於X軸方向等間隔設定。線a1、a2及a3於Y軸方向依序配置。線b1、b2及b3於X軸方向依序配置。The plurality of conductor disks 150 may be arranged in such a manner that each of the plurality of unit constituent regions R having the same area and the same shape has the same arrangement pattern on the upper surface 130b of the semiconductor layer 130 . Each of a plurality of units constituting R may also have a rectangular shape having each side with a length of 4.5 μm or more and 5.5 μm or less. The lengths of the two adjacent sides sandwiching an interior angle can be different from each other, and can also be equal to each other. In this example, each of the plurality of unit constituting regions R has a square shape, and each side of the square shape has a length of 4.5 μm or more and 5.5 μm or less. The plurality of unit constituent regions R may be arranged in an array such that adjacent unit constituent regions R in each of the X-axis direction and the Y-axis direction orthogonal to each other along the upper surface 130b have a common side. A plurality of units constituting the region R are arranged without gaps. Thereby, a two-dimensional periodic structure of the arrangement pattern of the plurality of conductor disks 150 is formed on the upper surface 130b. The two-dimensional periodic structure is an infrared plasmon sub-periodic structure that generates electromagnetic waves in the mid-infrared wavelength domain. The length of one side of the unit constituent region R corresponds to the periodic pitch P of the two-dimensional periodic structure. In this example, the arrangement pattern of each unit constituting region R is constituted by nine conductor disks 150 arranged in a matrix corresponding to 3×3. In a 3×3 matrix, three conductor disks 150 are arranged along a first side of the rectangular shape and three conductor disks 150 are arranged along a second side orthogonal to the first side. Corresponding conductor disks 150 are arranged on each of the lines a1 , a2 and a3 and the nine intersection points (grid points) C of the lines b1 , b2 and b3 . The center of each conductor disk 150 coincides with each intersection point C. Lines a1, a2, and a3 extend parallel to the X-axis direction, and are set at equal intervals in the Y-axis direction. The lines b1, b2, and b3 extend parallel to the Y-axis direction, and are set at equal intervals in the X-axis direction. Lines a1, a2, and a3 are sequentially arranged in the Y-axis direction. The lines b1, b2, and b3 are arranged in order in the X-axis direction.

配置於1個單位構成區域R內之9個導電體碟150包含具有彼此不同之直徑之4種以上之導電體碟150。於本例中,於單位構成區域R內,9個導電體碟150a至150i以於線a1至a3與線b1至b3之交點C上彼此隔開之狀態配置。第1導電體碟150a配置於線a3與線b1之交點C。第2導電體碟150b配置於線a3與線b2之交點C。第3導電體碟150c配置於線a3與線b3之交點C。第4導電體碟150d配置於線a2與線b1之交點C。第5導電體碟150e配置於線a2與線b2之交點C。第6導電體碟150f配置於線a2與線b3之交點C。第7導電體碟150g配置於線a1與線b1之交點C。第8導電體碟150h配置於線a1與線b2之交點C。第9導電體碟150i配置於線a1與線b3之交點C。第1導電體碟150a之直徑為0.9 μm。第2導電體碟150b之直徑為1.1 μm。第3導電體碟150c之直徑為0.9 μm。第4導電體碟150d之直徑為1.4 μm。第5導電體碟150e之直徑為1.5 μm。第6導電體碟150f之直徑為1.2 μm。第7導電體碟150g之直徑為0.9 μm。第8導電體碟150h之直徑為1.3 μm。第9導電體碟150i之直徑為1.0 μm。因此,於本例中,配置於1個單位構成區域R內之9個導電體碟150包含具有最小直徑(0.9 μm)之3個導電體碟150a、150c、150g。9個導電體碟150包含具有彼此不同之直徑之7種(0.9 μm、1.0 μm、1.1 μm、1.2 μm、1.3 μm、1.4 μm、1.5 μm)之導電體碟150a、150b、150d、150e、150f、150h、150i。於本例中,彼此相鄰之導電體碟150之中心間隔(即,交點C間之間隔)為1.7 μm。於本例中,相當於週期間距P之單位構成區域R之一邊之長度為5.1 μm。The nine conductor disks 150 arranged in one unit configuration region R include four or more types of conductor disks 150 having mutually different diameters. In this example, in the unit configuration region R, the nine conductor disks 150a to 150i are arranged in a state of being spaced apart from each other at the intersection C of the lines a1 to a3 and the lines b1 to b3. The first conductor disk 150a is arranged at the intersection C of the line a3 and the line b1. The second conductor disk 150b is arranged at the intersection C of the line a3 and the line b2. The third conductor disk 150c is arranged at the intersection point C of the line a3 and the line b3. The fourth conductor disk 150d is arranged at the intersection point C of the line a2 and the line b1. The fifth conductor disk 150e is arranged at the intersection point C of the line a2 and the line b2. The sixth conductor disk 150f is arranged at the intersection point C of the line a2 and the line b3. The seventh conductor disk 150g is arranged at the intersection point C of the line a1 and the line b1. The eighth conductor disk 150h is disposed at the intersection point C of the line a1 and the line b2. The ninth conductor disk 150i is arranged at the intersection point C of the line a1 and the line b3. The diameter of the first conductor disk 150a is 0.9 μm. The diameter of the second conductor disk 150b is 1.1 μm. The diameter of the third conductor disk 150c is 0.9 μm. The diameter of the fourth conductor disk 150d is 1.4 μm. The diameter of the fifth conductor disk 150e is 1.5 μm. The diameter of the sixth conductor disk 150f is 1.2 μm. The diameter of the seventh conductor disk 150g is 0.9 μm. The diameter of the eighth conductor disk 150h is 1.3 μm. The diameter of the ninth conductor disk 150i is 1.0 μm. Therefore, in this example, the nine conductor disks 150 arranged in one unit configuration region R include three conductor disks 150a, 150c, and 150g having the smallest diameter (0.9 μm). The 9 conductor disks 150 include 7 kinds (0.9 μm, 1.0 μm, 1.1 μm, 1.2 μm, 1.3 μm, 1.4 μm, 1.5 μm) of conductor disks 150a, 150b, 150d, 150e, 150f having different diameters from each other , 150h, 150i. In this example, the center-to-center interval (ie, the interval between the intersections C) of the conductive disks 150 adjacent to each other is 1.7 μm. In this example, the length of one side of the unit constituting region R corresponding to the period pitch P is 5.1 μm.

圖4係模式性顯示彎曲之圖1之輻射裝置之剖視圖。如圖4所示,可撓性膜110亦可以可撓性膜110之上表面110b具有60 mm以下之曲率半徑CR之方式彎曲。於圖4中,可撓性膜110可以上表面110b凸出之方式彎曲。可撓性膜110亦可以上表面110b凹窪之方式彎曲,上表面110b亦可以包含凸區域與凹區域之兩者之方式彎曲。可撓性膜110可以包圍沿上表面110b之中心軸CN之方式彎曲。於以包圍沿Y軸方向之中心軸CN之方式使可撓性膜110彎曲之情形時,曲率半徑CR相當於中心軸CN至上表面110b之距離。於以上表面110b具有60 mm之曲率半徑CR之方式彎曲可撓性膜110之情形時,複數個導電體碟150之各者之尺寸變化率之絕對值、與相鄰之複數個導電體碟150間之間隔之尺寸變化率之絕對值亦可為10%以下。各導電體碟150之尺寸及各間隔之變化亦可為不可逆。FIG. 4 is a cross-sectional view of the radiation device of FIG. 1 schematically showing bending. As shown in FIG. 4 , the flexible film 110 may also be bent such that the upper surface 110 b of the flexible film 110 has a curvature radius CR of 60 mm or less. In FIG. 4, the flexible film 110 may be bent in such a manner that the upper surface 110b is convex. The flexible film 110 can also be curved in a way that the upper surface 110b is concave, and the upper surface 110b can also be curved in a way of including both a convex area and a concave area. The flexible film 110 can be bent so as to surround the central axis CN along the upper surface 110b. When the flexible film 110 is bent so as to surround the central axis CN along the Y-axis direction, the curvature radius CR corresponds to the distance from the central axis CN to the upper surface 110b. When the flexible film 110 is bent in such a way that the upper surface 110b has a radius of curvature CR of 60 mm, the absolute value of the dimensional change rate of each of the plurality of conductor disks 150 and the adjacent plurality of conductor disks 150 The absolute value of the dimensional change rate of the interval may be 10% or less. The size of each conductor disk 150 and the change of each interval can also be irreversible.

複數個導電體碟150之各者之尺寸變化率RT1(%)可藉由以下計算式算出。

Figure 02_image001
Dn1表示於單位構成區域R內配置之k個導電體碟150中之第n個導電體碟150彎曲前之尺寸(參照圖1)。Dn1係於正交於Y軸方向之剖面中,第n個導電體碟150之未彎曲之上表面之長度。Dn2表示第n個導電體碟150之彎曲後之尺寸(參照圖4)。Dn2係於正交於中心軸CN之剖面中,第n個導電體碟150之彎曲之上表面之長度。k係2以上之自然數。n係自然數。於圖2及圖3之例中,k係9。第n個導電體碟150之例係具有最小直徑(0.9 μm)之第1導電體碟150a。於以上表面110凸出之方式彎曲可撓性膜110之情形時,尺寸變化率RT1(%)為正值。另一方面,於上表面110b以凹窪之方式彎曲可撓性膜110之情形時,尺寸變化率RT1(%)為負值。 The dimensional change rate RT1 (%) of each of the plurality of conductive disks 150 can be calculated by the following formula.
Figure 02_image001
Dn1 represents the dimension before bending of the n-th conductor disk 150 among the k conductor disks 150 arranged in the unit configuration region R (refer to FIG. 1 ). Dn1 is the length of the unbent upper surface of the n-th conductor disk 150 in a cross-section perpendicular to the Y-axis direction. Dn2 represents the dimension of the n-th conductor disk 150 after bending (refer to FIG. 4 ). Dn2 is the length of the curved upper surface of the n-th conductor disk 150 in a section orthogonal to the central axis CN. k is a natural number greater than or equal to 2. n is a natural number. In the example of FIG. 2 and FIG. 3 , k is 9. An example of the nth conductor disk 150 is the first conductor disk 150a having the smallest diameter (0.9 μm). In the case where the flexible film 110 is bent in such a manner that the upper surface 110 protrudes, the dimensional change rate RT1 (%) is a positive value. On the other hand, in the case where the upper surface 110b bends the flexible film 110 in a concave manner, the dimensional change rate RT1 (%) is a negative value.

相鄰之複數個導電體碟150間之間隔之尺寸變化率RT2(%)可藉由以下計算式算出。

Figure 02_image003
Gn1表示單位構成區域R內之m個間隔中之第n個間隔之彎曲前之尺寸(參照圖1)。Gn1係於正交於Y軸方向之剖面中,相鄰之複數個導電體碟150之未彎曲之上表面間之間隔。Gn2表示第n個間隔之彎曲後之尺寸(參照圖4)。Gn2係於正交於中心軸CN之剖面中,相鄰之複數個導電體碟150之彎曲之上表面間之間隔。m及n係自然數。於圖2及圖3之例中,m係6。第n個間隔之例係m個間隔中最小之間隔。於以上表面110b凸出之方式彎曲可撓性膜110之情形時,尺寸變化率RT2(%)為正值。另一方面,於以上表面110b凹窪之方式彎曲可撓性膜110之情形時,尺寸變化率RT2(%)為負值。 The dimensional change rate RT2 (%) of the interval between the adjacent plurality of conductive disks 150 can be calculated by the following formula.
Figure 02_image003
Gn1 represents the dimension before bending of the n-th space among the m spaces in the unit configuration region R (refer to FIG. 1 ). Gn1 is the interval between the unbent upper surfaces of the plurality of adjacent conductive disks 150 in the cross section orthogonal to the Y-axis direction. Gn2 represents the dimension after bending of the n-th interval (refer to FIG. 4 ). Gn2 is the interval between the curved upper surfaces of the adjacent plurality of conductor disks 150 in the section orthogonal to the central axis CN. m and n are natural numbers. In the example of FIG. 2 and FIG. 3, m is 6. FIG. The example of the nth interval is the smallest interval among the m intervals. In the case where the flexible film 110 is bent in such a manner that the upper surface 110b protrudes, the dimensional change rate RT2 (%) is a positive value. On the other hand, when the flexible film 110 is bent so that the upper surface 110b is concave, the dimensional change rate RT2 (%) is a negative value.

圖5係顯示一實施形態之放射冷卻裝置之概略構成之圖。圖5所示之放射冷卻裝置10係例如天空散熱器。放射冷卻裝置10具備本實施形態之輻射裝置100與構件300。構件300具有彎曲表面300a。輻射裝置100以可撓性膜110面向彎曲表面300a之方式,設置於構件300上。放射冷卻裝置10亦可為於大氣之窗口波長帶中具有具備高輻射率之光譜之輻射面板等。放射冷卻裝置10具有釋放特定波長域之電磁波之表面10a、及與表面10a為相反側之背面10b。位於表面10a之輻射裝置100遠離建築物200而配置。另一方面,位於背面10b之構件300配置於建築物200之附近。放射冷卻裝置10可配置為,於建築物200內與因熱源210而升溫之空氣直接或間接地相接。FIG. 5 is a diagram showing a schematic configuration of a radiation cooling apparatus according to an embodiment. The radiation cooling device 10 shown in FIG. 5 is, for example, a sky radiator. The radiation cooling device 10 includes the radiation device 100 and the member 300 of the present embodiment. The member 300 has a curved surface 300a. The radiation device 100 is disposed on the member 300 in such a manner that the flexible film 110 faces the curved surface 300a. The radiation cooling device 10 may also be a radiation panel or the like having a spectrum with a high emissivity in the window wavelength band of the atmosphere. The radiation cooling device 10 has a surface 10a that emits electromagnetic waves in a specific wavelength range, and a back surface 10b that is opposite to the surface 10a. The radiation device 100 on the surface 10a is arranged away from the building 200 . On the other hand, the member 300 located in the back surface 10b is arrange|positioned in the vicinity of the building 200. Radiative cooling device 10 may be configured to be in direct or indirect contact with air heated by heat source 210 within building 200 .

放射冷卻裝置10可吸收建築物200內因熱源210而升溫之空氣之熱量,將熱量轉換為大氣之窗口波長域之電磁波230,且向建築物200之外部放出。因通過大氣之窗波長域進行放射冷卻裝置10與宇宙之間之熱平衡,故放射冷卻裝置10損失熱能。藉此,放射冷卻裝置10之溫度下降。建築物200內之升溫之空氣與放射冷卻裝置10之背面10b相接。因此,升溫之空氣藉由將暫時累積之熱能向放射冷卻裝置10轉移而冷卻。冷卻之空氣藉由建築物200內之自然對流220或強制循環而回流至屋內。因此,本實施形態之放射冷卻裝置10可作為製冷機發揮功能。The radiation cooling device 10 can absorb the heat of the air heated by the heat source 210 in the building 200 , convert the heat into electromagnetic waves 230 in the window wavelength region of the atmosphere, and release the heat to the outside of the building 200 . The radiation cooling device 10 loses thermal energy because the thermal balance between the radiation cooling device 10 and the universe is performed through the atmospheric window wavelength region. Thereby, the temperature of the radiation cooling apparatus 10 falls. The heated air in the building 200 is in contact with the back surface 10b of the radiation cooling device 10 . Therefore, the heated air is cooled by transferring the temporarily accumulated thermal energy to the radiation cooling device 10 . The cooled air is returned to the house by natural convection 220 or forced circulation in the building 200 . Therefore, the radiation cooling device 10 of the present embodiment can function as a refrigerator.

圖6係顯示一實施形態之輻射裝置之吸收光譜之例之圖表。於圖6中,橫軸顯示波長(μm)。縱軸顯示吸收率。縱軸之吸收率之值係最大值正規化為1。圖6之圖表顯示具有以下之構造之輻射裝置之例相關之吸收光譜之計算結果。本例之輻射裝置包含依序積層於聚醯亞胺膜上之厚度100 nm之鋁層、厚度500 nm之矽層及厚度50 nm之複數個導電體碟。複數個導電體碟之配置圖案與圖2及圖3之例之配置圖案相同。根據圖6可知,可於相當於8 μm以上13 μm以下之波長域之「大氣窗口」中獲得高吸收率。FIG. 6 is a graph showing an example of the absorption spectrum of the radiation device of one embodiment. In FIG. 6 , the horizontal axis shows the wavelength (μm). The vertical axis shows the absorption rate. The value of the absorptivity on the vertical axis is the maximum value normalized to 1. The graph of FIG. 6 shows the calculated results of absorption spectra associated with an example of a radiation device having the following configuration. The radiation device of this example includes an aluminum layer with a thickness of 100 nm, a silicon layer with a thickness of 500 nm, and a plurality of conductive disks with a thickness of 50 nm, which are sequentially laminated on the polyimide film. The arrangement pattern of the plurality of conductor disks is the same as the arrangement pattern of the example of FIG. 2 and FIG. 3 . It can be seen from Fig. 6 that a high absorption rate can be obtained in the "atmospheric window" corresponding to the wavelength range of 8 μm to 13 μm.

根據本實施形態之輻射裝置100,藉由如圖4所示使可撓性膜110彎曲,可使輻射裝置100彎曲。因此,根據本實施形態之放射冷卻裝置10,例如圖5所示,可彎曲可撓性膜110,追隨構件300之彎曲表面300a。According to the radiation device 100 of the present embodiment, the radiation device 100 can be bent by bending the flexible film 110 as shown in FIG. 4 . Therefore, according to the radiation cooling device 10 of the present embodiment, for example, as shown in FIG.

於可撓性膜110可以上表面110b具有60 mm以下之曲率半徑CR之方式彎曲之情形,可使輻射裝置100較大地彎曲。In the case where the flexible film 110 can be bent in such a manner that the upper surface 110b has a curvature radius CR of 60 mm or less, the radiation device 100 can be greatly bent.

於可撓性膜110以上表面110b具有60 mm之曲率半徑CR之方式彎曲之情形,複數個導電體碟150之各者之尺寸變化率RT1之絕對值、與相鄰之複數個導電體碟150間之間隔之尺寸變化率RT2之絕對值亦可為10%以下。於該情形時,即使將輻射裝置100較大地彎曲,亦可使各導電體碟150及各間隔之尺寸變化率變小。藉此,可將尺寸變化引起之吸收波長之偏差之絕對值例如變小至0.5 μm以下。因此,只要以吸收波長為5 μm之方式設定各導電體碟150及各間隔,即使可撓性膜110彎曲,亦可獲得4.5 μm以上5.5 μm以下之波長域內之吸收波長。In the case where the upper surface 110b of the flexible film 110 is bent in such a way that the radius of curvature CR of 60 mm, the absolute value of the dimensional change rate RT1 of each of the plurality of conductive disks 150 and the adjacent plurality of conductive disks 150 The absolute value of the dimensional change rate RT2 of the interval may be 10% or less. In this case, even if the radiation device 100 is greatly bent, the dimensional change rate of each conductor disk 150 and each space can be reduced. Thereby, the absolute value of the deviation of the absorption wavelength due to the dimensional change can be reduced to, for example, 0.5 μm or less. Therefore, as long as each conductor disk 150 and each space are set so that the absorption wavelength is 5 μm, even if the flexible film 110 is bent, the absorption wavelength in the wavelength range of 4.5 μm or more and 5.5 μm or less can be obtained.

於複數個單位構成區域R之各者具有具備4.5 μm以上5.5 μm以下之長度之各邊之矩形形狀之情形,輻射裝置100可將相當於4.5 μm以上5.5 μm以下之波長域之「大氣窗口」之電磁波選擇性地放出。In the case where each of the plurality of unit constituting regions R has a rectangular shape with each side having a length of 4.5 μm or more and 5.5 μm or less, the radiation device 100 can emit an “atmospheric window” equivalent to a wavelength range of 4.5 μm or more and 5.5 μm or less. The electromagnetic waves are selectively emitted.

9個導電體碟150包含以對應於3×3之矩陣之方式配置,且具有彼此不同之直徑之4種以上之導電體碟150之情形,可將9個導電體碟150適當地配置於具有4.5 μm以上5.5 μm以下之長度之各邊之矩形形狀內。In the case where the nine conductor disks 150 include four or more types of conductor disks 150 which are arranged in a manner corresponding to a 3×3 matrix and have mutually different diameters, the nine conductor disks 150 can be appropriately arranged to have Within the rectangular shape of each side with a length of 4.5 μm or more and 5.5 μm or less.

圖7A及圖7B之各者係模式性顯示製造一實施形態之輻射裝置之方法之一步驟之剖視圖。本實施形態之輻射裝置100可以如下之方式製造。Each of FIGS. 7A and 7B is a cross-sectional view schematically showing a step of a method of making a radiation device of one embodiment. The radiation device 100 of this embodiment can be manufactured as follows.

首先,如圖7A所示,於基板400上設置可撓性膜110。基板400係例如矽基板。可撓性膜110以下表面110a面向基板400之方式設置。可撓性膜110亦可藉由接著劑層410接著於基板400。於該情形時,可抑制可撓性膜110相對於基板400之位置偏移。接著劑層410例如亦可具有300℃以上之耐熱性。接著劑層410亦可具有對於有機溶劑及強酸之高耐性。接著劑層410例如亦可包含矽系黏著劑(感壓接著劑)。設置有接著劑層410之可撓性膜110之例係黏著膠帶(寺岡製作所股份有限公司製之KAPTON(註冊商標)黏著膠帶)。自可撓性膜110之厚度方向觀察,可撓性膜110例如具有矩形形狀。First, as shown in FIG. 7A , the flexible film 110 is provided on the substrate 400 . The substrate 400 is, for example, a silicon substrate. The flexible film 110 is disposed in such a manner that the lower surface 110 a faces the substrate 400 . The flexible film 110 can also be adhered to the substrate 400 through the adhesive layer 410 . In this case, the positional displacement of the flexible film 110 with respect to the substrate 400 can be suppressed. The adhesive layer 410 may have, for example, a heat resistance of 300° C. or higher. The adhesive layer 410 may also have high resistance to organic solvents and strong acids. The adhesive layer 410 may also contain, for example, a silicon-based adhesive (pressure-sensitive adhesive). An example of the flexible film 110 provided with the adhesive layer 410 is an adhesive tape (KAPTON (registered trademark) adhesive tape by Teraoka Seisakusho Co., Ltd.). The flexible film 110 has, for example, a rectangular shape when viewed from the thickness direction of the flexible film 110 .

於基板400上設置可撓性膜110後,亦可藉由醇系洗淨液將可撓性膜110之上表面110b洗淨。藉此,去除上表面110b上之有機物。其後,亦可對上表面110b進行氧電漿處理。藉此,去除上表面110b之針狀突起及殘留之有機物。After the flexible film 110 is provided on the substrate 400, the upper surface 110b of the flexible film 110 may also be cleaned with an alcohol-based cleaning solution. Thereby, the organic matter on the upper surface 110b is removed. Thereafter, oxygen plasma treatment may also be performed on the upper surface 110b. Thereby, the needle-like protrusions on the upper surface 110b and the remaining organic matter are removed.

接著,如圖7B所示,於可撓性膜110上,依序形成導電體層120、半導體層130、與彼此隔開配置之複數個導電體碟150。複數個導電體碟150可藉由光微影及蝕刻而形成。首先,於可撓性膜110上,例如藉由磁控濺鍍將導電體層120(例如厚度100 nm)及半導體層130(例如厚度500 nm)連續堆積。亦可將基板400之溫度於150℃以上300℃以下之範圍內調整且進行堆積。藉此,可獲得導電體層120及半導體層130之緻密化及表面之平坦化之效果。其後,於半導體層130之上表面130b形成抗蝕劑膜後,進行步進機曝光及顯影,藉此於抗蝕劑膜形成開口圖案。其後,於抗蝕劑膜上及開口圖案內,例如藉由磁控濺鍍,堆積導電體層(例如厚度50 nm)。其後,藉由使用有機溶媒去除抗蝕劑膜及抗蝕劑膜上之導電體層,可獲得複數個導電體碟150。Next, as shown in FIG. 7B , on the flexible film 110 , a conductor layer 120 , a semiconductor layer 130 , and a plurality of conductor disks 150 arranged to be spaced apart from each other are sequentially formed. The plurality of conductor disks 150 may be formed by photolithography and etching. First, on the flexible film 110, the conductor layer 120 (for example, the thickness of 100 nm) and the semiconductor layer 130 (for example, the thickness of 500 nm) are successively deposited, for example, by magnetron sputtering. The temperature of the substrate 400 may be adjusted within a range of 150° C. or higher and 300° C. or lower, and the deposition may be performed. Thereby, the effects of densification of the conductor layer 120 and the semiconductor layer 130 and flattening of the surface can be obtained. After that, after forming a resist film on the upper surface 130b of the semiconductor layer 130, stepper exposure and development are performed, thereby forming an opening pattern in the resist film. Thereafter, a conductor layer (eg, thickness 50 nm) is deposited on the resist film and in the opening pattern, for example, by magnetron sputtering. After that, by using an organic solvent to remove the resist film and the conductor layer on the resist film, a plurality of conductor disks 150 can be obtained.

接著,將可撓性膜110自基板400剝離。藉由自可撓性膜110之角部機械地拉拔,可自基板400剝離可撓性膜110。如此,可獲得輻射裝置100。Next, the flexible film 110 is peeled off from the substrate 400 . The flexible film 110 can be peeled off from the substrate 400 by mechanically pulling from the corners of the flexible film 110 . In this way, the radiation device 100 can be obtained.

根據製造本實施形態之輻射裝置100之方法,可獲得具備可撓性膜110之輻射裝置100(參照圖1)。於形成複數個導電體碟150時,因由基板400支持複數個導電體碟150,故可提高各導電體碟150之尺寸精度。於可撓性膜110藉由接著劑層410接著於基板400之情形,可抑制可撓性膜110相對於基板400之位置偏移。因此,各導電體碟150之尺寸精度進一步提高。According to the method of manufacturing the radiation device 100 of the present embodiment, the radiation device 100 provided with the flexible film 110 can be obtained (see FIG. 1 ). When the plurality of conductor disks 150 are formed, since the plurality of conductor disks 150 are supported by the substrate 400 , the dimensional accuracy of each conductor disk 150 can be improved. When the flexible film 110 is adhered to the substrate 400 by the adhesive layer 410 , the positional displacement of the flexible film 110 relative to the substrate 400 can be suppressed. Therefore, the dimensional accuracy of each conductor disk 150 is further improved.

以上,對本揭示之較佳之實施形態進行詳細說明,但本揭示並非限定於上述實施形態。The preferred embodiment of the present disclosure has been described above in detail, but the present disclosure is not limited to the above-described embodiment.

例如,於上述實施形態中,各單位構成區域R具有相同配置圖案,但複數個單位構成區域R亦可具有彼此不同之配置圖案。例如,第1單位構成區域R亦可具有第1配置圖案。第2單位構成區域R亦可具有將第1配置圖案旋轉90°而獲得之第2配置圖案。For example, in the above-described embodiment, each unit configuration region R has the same arrangement pattern, but a plurality of unit configuration regions R may have mutually different arrangement patterns. For example, the first unit configuration region R may have a first arrangement pattern. The second unit configuration region R may have a second arrangement pattern obtained by rotating the first arrangement pattern by 90°.

於上述實施形態中,各單位構成區域R之配置圖案藉由以對應於3×3之矩陣之方式配置之9個導電體碟150而構成。各單位構成區域R之配置圖案亦可藉由以對應於4×4之矩陣之方式配置之16個導電體碟150構成,又可藉由以對應於5×5之矩陣之方式配置之25個導電體碟150構成,還可藉由以對應於10×10之矩陣之方式配置之100個導電體碟150構成。若各單位構成區域R內之導電體碟150之數量增加,則可將吸收光譜之特性高精度地控制。In the above-described embodiment, the arrangement pattern of each unit configuration region R is constituted by nine conductor disks 150 arranged in a manner corresponding to a 3×3 matrix. The arrangement pattern of each unit constituting region R can also be formed by 16 conductor disks 150 arranged in a matrix corresponding to 4×4, or by 25 conductive disks 150 arranged in a matrix corresponding to 5×5. The conductor disks 150 may be formed by 100 conductor disks 150 arranged in a matrix corresponding to 10×10. If the number of the conductor disks 150 in each unit constituting region R is increased, the characteristics of the absorption spectrum can be controlled with high precision.

應理解本次揭示之實施形態係所有點皆為例示而非限制性者。本發明之範圍並非意指上述者,而由申請專利範圍所示,且意欲涵蓋與申請專利範圍均等之意義及範圍內之所有變更。It should be understood that the embodiments disclosed herein are all illustrative and not restrictive. The scope of the present invention does not mean the above, but is shown by the scope of the patent application, and is intended to cover all changes within the meaning and scope equivalent to the scope of the patent application.

10:放射冷卻裝置 10a:表面 10b:背面 100:輻射裝置 110:可撓性膜 110a:下表面 110b:上表面(主面) 120:導電體層 120a:下表面 120b:下表面 130:半導體層 130a:下表面 130b:上表面(主面) 140:表面保護層 150:導電體碟 150a:第1導電體碟 150b:第2導電體碟 150c:第3導電體碟 150d:第4導電體碟 150e:第5導電體碟 150f:第6導電體碟 150g:第7導電體碟 150h:第8導電體碟 150i:第9導電體碟 200:建築物 210:熱源 220:自然對流 230:電磁波 300:構件 300a:彎曲表面 400:基板 410:接著劑層 a1~a3:線 b1~b3:線 C:交點 CN:中心軸 CR:曲率半徑 Dn1:尺寸 Dn2:尺寸 Gn1:尺寸 Gn2:尺寸 P:週期間距 R:單位構成區域 10: Radiation cooling device 10a: Surface 10b: Back 100: Radiation Device 110: Flexible membrane 110a: Lower surface 110b: Upper surface (main surface) 120: Conductor layer 120a: lower surface 120b: lower surface 130: Semiconductor layer 130a: Lower surface 130b: Upper surface (main surface) 140: Surface protection layer 150: Conductor disc 150a: 1st conductor plate 150b: 2nd conductor plate 150c: 3rd Conductor Disc 150d: 4th Conductor Disc 150e: 5th Conductor Disc 150f: 6th Conductor Disc 150g: 7th conductor plate 150h: 8th conductor plate 150i: 9th Conductor Disc 200: Buildings 210: Heat Source 220: Natural Convection 230: Electromagnetic waves 300: Components 300a: Curved Surface 400: Substrate 410: Adhesive layer a1~a3: Line b1~b3: line C: intersection CN:Central axis CR: Radius of Curvature Dn1: size Dn2: size Gn1: size Gn2: size P: period pitch R: unit composition area

圖1係模式性顯示一實施形態之輻射裝置之剖視圖。 圖2係顯示陣列配置之複數個單位構成區域之俯視圖。 圖3係顯示各單位構成區域之導電體碟之配置圖案之俯視圖。 圖4係模式性顯示彎曲之圖1之輻射裝置之剖視圖。 圖5係顯示一實施形態之放射冷卻裝置之概略構成之圖。 圖6係顯示一實施形態之輻射裝置之吸收光譜之例之圖表。 圖7A係模式性顯示製造一實施形態之輻射裝置之方法之一步驟之剖視圖。 圖7B係模式性顯示製造一實施形態之輻射裝置之方法之一步驟之剖視圖。 FIG. 1 is a cross-sectional view schematically showing a radiation device according to an embodiment. FIG. 2 is a top view showing a plurality of unit constituent regions of an array configuration. FIG. 3 is a plan view showing the arrangement pattern of the conductor disks in each unit constituting region. FIG. 4 is a cross-sectional view of the radiation device of FIG. 1 schematically showing bending. FIG. 5 is a diagram showing a schematic configuration of a radiation cooling apparatus according to an embodiment. FIG. 6 is a graph showing an example of the absorption spectrum of the radiation device of one embodiment. 7A is a cross-sectional view schematically showing a step of a method of manufacturing a radiation device of one embodiment. 7B is a cross-sectional view schematically showing a step of a method of manufacturing a radiation device of one embodiment.

100:輻射裝置 100: Radiation Device

110:可撓性膜 110: Flexible membrane

110a:下表面 110a: Lower surface

110b:上表面(主面) 110b: Upper surface (main surface)

120:導電體層 120: Conductor layer

120a:下表面 120a: lower surface

120b:下表面 120b: lower surface

130:半導體層 130: Semiconductor layer

130a:下表面 130a: Lower surface

130b:上表面(主面) 130b: Upper surface (main surface)

140:表面保護層 140: Surface protection layer

150:導電體碟 150: Conductor disc

Dn1:尺寸 Dn1: size

Gn1:尺寸 Gn1: size

Claims (10)

一種輻射裝置,其具備: 可撓性膜; 導電體層,其設置於上述可撓性膜上; 半導體層,其設置於上述導電體層上;及 複數個導電體碟,其等設置於上述半導體層上,且彼此隔開配置。 A radiation device comprising: flexible membrane; a conductor layer, which is arranged on the above-mentioned flexible film; a semiconductor layer disposed on the above-mentioned conductor layer; and A plurality of conductor disks are arranged on the above-mentioned semiconductor layer and are arranged apart from each other. 如請求項1之輻射裝置,其中 上述導電體層設置於上述可撓性膜之主面上; 上述可撓性膜可以上述主面具有60 mm以下之曲率半徑之方式彎曲。 The radiation device of claim 1, wherein The conductor layer is arranged on the main surface of the flexible film; The flexible film may be bent so that the main surface has a radius of curvature of 60 mm or less. 如請求項2之輻射裝置,其中 於上述可撓性膜以上述主面具有60 mm之曲率半徑之方式彎曲之情形,上述複數個導電體碟之各者之尺寸變化率之絕對值、與相鄰之上述複數個導電體碟間之間隔之尺寸變化率之絕對值為10%以下。 The radiation device of claim 2, wherein In the case where the above-mentioned flexible film is bent in such a way that the above-mentioned main surface has a radius of curvature of 60 mm, the absolute value of the dimensional change rate of each of the above-mentioned plurality of conductive discs and the distance between the adjacent plurality of conductive discs The absolute value of the dimensional change rate of the interval is less than 10%. 如請求項1至3中任一項之輻射裝置,其中 上述可撓性膜包含樹脂。 The radiation device of any one of claims 1 to 3, wherein The above-mentioned flexible film contains resin. 如請求項4之輻射裝置,其中 上述可撓性膜包含聚醯亞胺。 The radiation device of claim 4, wherein The above-mentioned flexible film contains polyimide. 如請求項1至5中任一項之輻射裝置,其中 上述複數個導電體碟以於上述半導體層之主面中具有同一面積及同一形狀之複數個單位構成區域之各者具有相同之配置圖案之方式配置; 上述複數個單位構成區域之各者具有矩形形狀,該矩形形狀具有4.5 μm以上5.5 μm以下之長度之各邊; 上述複數個單位構成區域以於沿上述主面彼此正交之2個方向之各者中相鄰之單位構成區域彼此具有共通之邊之方式陣列配置。 The radiation device of any one of claims 1 to 5, wherein The plurality of conductor disks are arranged in such a manner that each of the plurality of unit constituent regions having the same area and the same shape in the main surface of the semiconductor layer has the same arrangement pattern; Each of the above-mentioned plurality of unit constituting regions has a rectangular shape, and each side of the rectangular shape has a length of not less than 4.5 μm and not more than 5.5 μm; The plurality of unit configuration regions are arranged in an array such that adjacent unit configuration regions have a common side in each of the two directions along the main surfaces orthogonal to each other. 如請求項6之輻射裝置,其中 上述配置圖案藉由以與沿上述矩形形狀之第1邊排列3個導電體碟且沿上述第1邊所正交之第2邊排列3個導電體碟之3×3之矩陣對應之方式配置之9個導電體碟構成; 上述9個導電體碟包含具有彼此不同之直徑之4種以上之導電體碟。 The radiation device of claim 6, wherein The arrangement pattern is arranged in a manner corresponding to a 3×3 matrix in which three conductor plates are arranged along the first side of the rectangular shape and three conductor plates are arranged along the second side orthogonal to the first side. It consists of 9 conductor discs; The above-mentioned nine conductor disks include four or more types of conductor disks having mutually different diameters. 一種放射冷卻裝置,其具備: 構件,其具有彎曲表面;及 如請求項1至7中任一項之輻射裝置;且 上述輻射裝置以上述可撓性膜面向上述彎曲表面之方式設置於上述構件上。 A radiation cooling device comprising: a member having a curved surface; and A radiation device as claimed in any one of claims 1 to 7; and The above-mentioned radiation device is disposed on the above-mentioned member in such a manner that the above-mentioned flexible film faces the above-mentioned curved surface. 一種製造輻射裝置之方法,其包含如下步驟: 將可撓性膜設置於基板上; 於上述可撓性膜上,依序形成導電體層、半導體層、彼此隔開配置之複數個導電體碟;及 自上述基板剝離上述可撓性膜。 A method of manufacturing a radiation device, comprising the steps of: disposing the flexible film on the substrate; On the above-mentioned flexible film, a conductor layer, a semiconductor layer, and a plurality of conductor disks spaced apart from each other are sequentially formed; and The said flexible film is peeled from the said board|substrate. 如請求項9之方法,其中 設置上述可撓性膜之步驟包含將上述可撓性膜藉由接著劑層接著於上述基板。 The method of claim 9, wherein The step of disposing the flexible film includes attaching the flexible film to the substrate through an adhesive layer.
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