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 PDFInfo
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- B32B3/14—Layered 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
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- F—MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
- F25—REFRIGERATION OR COOLING; COMBINED HEATING AND REFRIGERATION SYSTEMS; HEAT PUMP SYSTEMS; MANUFACTURE OR STORAGE OF ICE; LIQUEFACTION SOLIDIFICATION OF GASES
- F25B—REFRIGERATION MACHINES, PLANTS OR SYSTEMS; COMBINED HEATING AND REFRIGERATION SYSTEMS; HEAT PUMP SYSTEMS
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Abstract
Description
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]
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
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
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
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
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
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
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
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
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
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。
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
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。
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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:
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)
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