TW530146B - Surfaces having particle structures with broad range radiation absorptivity - Google Patents
Surfaces having particle structures with broad range radiation absorptivity Download PDFInfo
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- TW530146B TW530146B TW091105672A TW91105672A TW530146B TW 530146 B TW530146 B TW 530146B TW 091105672 A TW091105672 A TW 091105672A TW 91105672 A TW91105672 A TW 91105672A TW 530146 B TW530146 B TW 530146B
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- 239000002245 particle Substances 0.000 title claims abstract description 150
- 230000005855 radiation Effects 0.000 title claims description 21
- 239000000463 material Substances 0.000 claims abstract description 91
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- 239000000126 substance Substances 0.000 claims abstract description 11
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- BQCADISMDOOEFD-UHFFFAOYSA-N Silver Chemical compound [Ag] BQCADISMDOOEFD-UHFFFAOYSA-N 0.000 claims description 23
- 230000005670 electromagnetic radiation Effects 0.000 claims description 22
- PCHJSUWPFVWCPO-UHFFFAOYSA-N gold Chemical compound [Au] PCHJSUWPFVWCPO-UHFFFAOYSA-N 0.000 claims description 21
- 229910052709 silver Inorganic materials 0.000 claims description 18
- 239000004332 silver Substances 0.000 claims description 18
- 229910052737 gold Inorganic materials 0.000 claims description 17
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- NLJMYIDDQXHKNR-UHFFFAOYSA-K sodium citrate Chemical compound O.O.[Na+].[Na+].[Na+].[O-]C(=O)CC(O)(CC([O-])=O)C([O-])=O NLJMYIDDQXHKNR-UHFFFAOYSA-K 0.000 description 4
- 238000002834 transmittance Methods 0.000 description 4
- RYGMFSIKBFXOCR-UHFFFAOYSA-N Copper Chemical compound [Cu] RYGMFSIKBFXOCR-UHFFFAOYSA-N 0.000 description 3
- OKKJLVBELUTLKV-UHFFFAOYSA-N Methanol Chemical compound OC OKKJLVBELUTLKV-UHFFFAOYSA-N 0.000 description 3
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- VNWKTOKETHGBQD-UHFFFAOYSA-N methane Natural products C VNWKTOKETHGBQD-UHFFFAOYSA-N 0.000 description 3
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- XKRFYHLGVUSROY-UHFFFAOYSA-N Argon Chemical compound [Ar] XKRFYHLGVUSROY-UHFFFAOYSA-N 0.000 description 2
- CIWBSHSKHKDKBQ-JLAZNSOCSA-N Ascorbic acid Chemical compound OC[C@H](O)[C@H]1OC(=O)C(O)=C1O CIWBSHSKHKDKBQ-JLAZNSOCSA-N 0.000 description 2
- KRKNYBCHXYNGOX-UHFFFAOYSA-K Citrate Chemical compound [O-]C(=O)CC(O)(CC([O-])=O)C([O-])=O KRKNYBCHXYNGOX-UHFFFAOYSA-K 0.000 description 2
- KFZMGEQAYNKOFK-UHFFFAOYSA-N Isopropanol Chemical compound CC(C)O KFZMGEQAYNKOFK-UHFFFAOYSA-N 0.000 description 2
- 241000209094 Oryza Species 0.000 description 2
- 235000007164 Oryza sativa Nutrition 0.000 description 2
- KDLHZDBZIXYQEI-UHFFFAOYSA-N Palladium Chemical compound [Pd] KDLHZDBZIXYQEI-UHFFFAOYSA-N 0.000 description 2
- FAPWRFPIFSIZLT-UHFFFAOYSA-M Sodium chloride Chemical compound [Na+].[Cl-] FAPWRFPIFSIZLT-UHFFFAOYSA-M 0.000 description 2
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- 239000011888 foil Substances 0.000 description 2
- 239000003292 glue Substances 0.000 description 2
- 239000000178 monomer Substances 0.000 description 2
- 239000002114 nanocomposite Substances 0.000 description 2
- 238000003199 nucleic acid amplification method Methods 0.000 description 2
- 230000035515 penetration Effects 0.000 description 2
- 239000012071 phase Substances 0.000 description 2
- BASFCYQUMIYNBI-UHFFFAOYSA-N platinum Chemical compound [Pt] BASFCYQUMIYNBI-UHFFFAOYSA-N 0.000 description 2
- 230000010287 polarization Effects 0.000 description 2
- 235000009566 rice Nutrition 0.000 description 2
- 150000003839 salts Chemical class 0.000 description 2
- 238000002198 surface plasmon resonance spectroscopy Methods 0.000 description 2
- 125000003396 thiol group Chemical class [H]S* 0.000 description 2
- 238000005406 washing Methods 0.000 description 2
- PCGDBWLKAYKBTN-UHFFFAOYSA-N 1,2-dithiole Chemical compound C1SSC=C1 PCGDBWLKAYKBTN-UHFFFAOYSA-N 0.000 description 1
- SJECZPVISLOESU-UHFFFAOYSA-N 3-trimethoxysilylpropan-1-amine Chemical compound CO[Si](OC)(OC)CCCN SJECZPVISLOESU-UHFFFAOYSA-N 0.000 description 1
- 101710134784 Agnoprotein Proteins 0.000 description 1
- XMWRBQBLMFGWIX-UHFFFAOYSA-N C60 fullerene Chemical class C12=C3C(C4=C56)=C7C8=C5C5=C9C%10=C6C6=C4C1=C1C4=C6C6=C%10C%10=C9C9=C%11C5=C8C5=C8C7=C3C3=C7C2=C1C1=C2C4=C6C4=C%10C6=C9C9=C%11C5=C5C8=C3C3=C7C1=C1C2=C4C6=C2C9=C5C3=C12 XMWRBQBLMFGWIX-UHFFFAOYSA-N 0.000 description 1
- HZZVJAQRINQKSD-UHFFFAOYSA-N Clavulanic acid Natural products OC(=O)C1C(=CCO)OC2CC(=O)N21 HZZVJAQRINQKSD-UHFFFAOYSA-N 0.000 description 1
- 206010011878 Deafness Diseases 0.000 description 1
- LFQSCWFLJHTTHZ-UHFFFAOYSA-N Ethanol Chemical compound CCO LFQSCWFLJHTTHZ-UHFFFAOYSA-N 0.000 description 1
- 108010068370 Glutens Proteins 0.000 description 1
- GRYLNZFGIOXLOG-UHFFFAOYSA-N Nitric acid Chemical compound O[N+]([O-])=O GRYLNZFGIOXLOG-UHFFFAOYSA-N 0.000 description 1
- 241001494479 Pecora Species 0.000 description 1
- 239000004372 Polyvinyl alcohol Substances 0.000 description 1
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- 229920002472 Starch Polymers 0.000 description 1
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- 125000003636 chemical group Chemical group 0.000 description 1
- HZZVJAQRINQKSD-PBFISZAISA-N clavulanic acid Chemical compound OC(=O)[C@H]1C(=C/CO)/O[C@@H]2CC(=O)N21 HZZVJAQRINQKSD-PBFISZAISA-N 0.000 description 1
- 229960003324 clavulanic acid Drugs 0.000 description 1
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- ORTYMGHCFWKXHO-UHFFFAOYSA-N diethadione Chemical compound CCC1(CC)COC(=O)NC1=O ORTYMGHCFWKXHO-UHFFFAOYSA-N 0.000 description 1
- 238000004821 distillation Methods 0.000 description 1
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- 230000007613 environmental effect Effects 0.000 description 1
- 239000004744 fabric Substances 0.000 description 1
- 238000001914 filtration Methods 0.000 description 1
- 239000010419 fine particle Substances 0.000 description 1
- 239000005357 flat glass Substances 0.000 description 1
- 239000012634 fragment Substances 0.000 description 1
- 229910003472 fullerene Inorganic materials 0.000 description 1
- 239000007789 gas Substances 0.000 description 1
- 235000021312 gluten Nutrition 0.000 description 1
- 150000002343 gold Chemical class 0.000 description 1
- 208000016354 hearing loss disease Diseases 0.000 description 1
- 239000001307 helium Substances 0.000 description 1
- 229910052734 helium Inorganic materials 0.000 description 1
- SWQJXJOGLNCZEY-UHFFFAOYSA-N helium atom Chemical compound [He] SWQJXJOGLNCZEY-UHFFFAOYSA-N 0.000 description 1
- 239000001257 hydrogen Substances 0.000 description 1
- 229910052739 hydrogen Inorganic materials 0.000 description 1
- 125000004435 hydrogen atom Chemical class [H]* 0.000 description 1
- 238000005286 illumination Methods 0.000 description 1
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- 125000001449 isopropyl group Chemical group [H]C([H])([H])C([H])(*)C([H])([H])[H] 0.000 description 1
- 229910052743 krypton Inorganic materials 0.000 description 1
- DNNSSWSSYDEUBZ-UHFFFAOYSA-N krypton atom Chemical compound [Kr] DNNSSWSSYDEUBZ-UHFFFAOYSA-N 0.000 description 1
- 239000007791 liquid phase Substances 0.000 description 1
- 238000001459 lithography Methods 0.000 description 1
- 230000007246 mechanism Effects 0.000 description 1
- 238000002844 melting Methods 0.000 description 1
- 230000008018 melting Effects 0.000 description 1
- 230000005405 multipole Effects 0.000 description 1
- 229910052754 neon Inorganic materials 0.000 description 1
- GKAOGPIIYCISHV-UHFFFAOYSA-N neon atom Chemical compound [Ne] GKAOGPIIYCISHV-UHFFFAOYSA-N 0.000 description 1
- 230000004297 night vision Effects 0.000 description 1
- 229910017604 nitric acid Inorganic materials 0.000 description 1
- 238000010899 nucleation Methods 0.000 description 1
- 150000007523 nucleic acids Chemical class 0.000 description 1
- 102000039446 nucleic acids Human genes 0.000 description 1
- 108020004707 nucleic acids Proteins 0.000 description 1
- 238000012856 packing Methods 0.000 description 1
- 229910052763 palladium Inorganic materials 0.000 description 1
- 239000008188 pellet Substances 0.000 description 1
- 230000002085 persistent effect Effects 0.000 description 1
- 229910052697 platinum Inorganic materials 0.000 description 1
- 229920002451 polyvinyl alcohol Polymers 0.000 description 1
- 239000010970 precious metal Substances 0.000 description 1
- 230000000750 progressive effect Effects 0.000 description 1
- 238000000746 purification Methods 0.000 description 1
- 238000006722 reduction reaction Methods 0.000 description 1
- 229910052702 rhenium Inorganic materials 0.000 description 1
- WUAPFZMCVAUBPE-UHFFFAOYSA-N rhenium atom Chemical compound [Re] WUAPFZMCVAUBPE-UHFFFAOYSA-N 0.000 description 1
- 235000015170 shellfish Nutrition 0.000 description 1
- 229910052710 silicon Inorganic materials 0.000 description 1
- 239000010703 silicon Substances 0.000 description 1
- 239000011780 sodium chloride Substances 0.000 description 1
- 239000002689 soil Substances 0.000 description 1
- 241000894007 species Species 0.000 description 1
- 238000012306 spectroscopic technique Methods 0.000 description 1
- 238000001228 spectrum Methods 0.000 description 1
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- 235000019698 starch Nutrition 0.000 description 1
- 239000008107 starch Substances 0.000 description 1
- 238000004416 surface enhanced Raman spectroscopy Methods 0.000 description 1
- 238000004415 surface enhanced infrared absorption spectroscopy Methods 0.000 description 1
- 239000000725 suspension Substances 0.000 description 1
- 238000003786 synthesis reaction Methods 0.000 description 1
- 239000008399 tap water Substances 0.000 description 1
- 235000020679 tap water Nutrition 0.000 description 1
- 238000012360 testing method Methods 0.000 description 1
- 239000010409 thin film Substances 0.000 description 1
- WFKWXMTUELFFGS-UHFFFAOYSA-N tungsten Chemical compound [W] WFKWXMTUELFFGS-UHFFFAOYSA-N 0.000 description 1
- 229910052721 tungsten Inorganic materials 0.000 description 1
- 239000010937 tungsten Substances 0.000 description 1
- 229910052724 xenon Inorganic materials 0.000 description 1
- FHNFHKCVQCLJFQ-UHFFFAOYSA-N xenon atom Chemical compound [Xe] FHNFHKCVQCLJFQ-UHFFFAOYSA-N 0.000 description 1
Classifications
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01N—INVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
- G01N33/00—Investigating or analysing materials by specific methods not covered by groups G01N1/00 - G01N31/00
- G01N33/48—Biological material, e.g. blood, urine; Haemocytometers
- G01N33/50—Chemical analysis of biological material, e.g. blood, urine; Testing involving biospecific ligand binding methods; Immunological testing
- G01N33/53—Immunoassay; Biospecific binding assay; Materials therefor
- G01N33/543—Immunoassay; Biospecific binding assay; Materials therefor with an insoluble carrier for immobilising immunochemicals
- G01N33/54313—Immunoassay; Biospecific binding assay; Materials therefor with an insoluble carrier for immobilising immunochemicals the carrier being characterised by its particulate form
- G01N33/54346—Nanoparticles
-
- F—MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
- F28—HEAT EXCHANGE IN GENERAL
- F28D—HEAT-EXCHANGE APPARATUS, NOT PROVIDED FOR IN ANOTHER SUBCLASS, IN WHICH THE HEAT-EXCHANGE MEDIA DO NOT COME INTO DIRECT CONTACT
- F28D15/00—Heat-exchange apparatus with the intermediate heat-transfer medium in closed tubes passing into or through the conduit walls ; Heat-exchange apparatus employing intermediate heat-transfer medium or bodies
- F28D15/02—Heat-exchange apparatus with the intermediate heat-transfer medium in closed tubes passing into or through the conduit walls ; Heat-exchange apparatus employing intermediate heat-transfer medium or bodies in which the medium condenses and evaporates, e.g. heat pipes
-
- F—MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
- F28—HEAT EXCHANGE IN GENERAL
- F28F—DETAILS OF HEAT-EXCHANGE AND HEAT-TRANSFER APPARATUS, OF GENERAL APPLICATION
- F28F13/00—Arrangements for modifying heat-transfer, e.g. increasing, decreasing
- F28F13/18—Arrangements for modifying heat-transfer, e.g. increasing, decreasing by applying coatings, e.g. radiation-absorbing, radiation-reflecting; by surface treatment, e.g. polishing
-
- F—MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
- F28—HEAT EXCHANGE IN GENERAL
- F28F—DETAILS OF HEAT-EXCHANGE AND HEAT-TRANSFER APPARATUS, OF GENERAL APPLICATION
- F28F2245/00—Coatings; Surface treatments
- F28F2245/06—Coatings; Surface treatments having particular radiating, reflecting or absorbing features, e.g. for improving heat transfer by radiation
Landscapes
- Engineering & Computer Science (AREA)
- Health & Medical Sciences (AREA)
- Life Sciences & Earth Sciences (AREA)
- Immunology (AREA)
- Physics & Mathematics (AREA)
- Chemical & Material Sciences (AREA)
- Mechanical Engineering (AREA)
- Urology & Nephrology (AREA)
- General Engineering & Computer Science (AREA)
- Hematology (AREA)
- Biomedical Technology (AREA)
- Molecular Biology (AREA)
- Thermal Sciences (AREA)
- Microbiology (AREA)
- Biochemistry (AREA)
- Biotechnology (AREA)
- Nanotechnology (AREA)
- Food Science & Technology (AREA)
- Medicinal Chemistry (AREA)
- Analytical Chemistry (AREA)
- Cell Biology (AREA)
- General Health & Medical Sciences (AREA)
- General Physics & Mathematics (AREA)
- Pathology (AREA)
- Sustainable Development (AREA)
- Laminated Bodies (AREA)
- Investigating Or Analysing Materials By Optical Means (AREA)
- Optical Modulation, Optical Deflection, Nonlinear Optics, Optical Demodulation, Optical Logic Elements (AREA)
Abstract
Description
530146 A7 B7 五、發明説明(1 相關申請案 本案主張在2000年9月26申請的美國實用專利申請案第 09/669,796號之35 U.S.C. § 120下之權利,而後者主張現已 放棄的美國臨時專利申請案第60/156,471號之35 U.S.C. § 1 19下之權利。本案亦相關於2〇〇〇年9月26申請的美國實用 專利申請案第09/670,453號、2000年9月26申請的美國實用 專利申請案第09/669,369號以及2001年3月23日申請的美國 實用專利申請案(其標題,,用感受器藉由具有顆粒結構 之基材增大分析物檢測"(Amplification 〇f Anaiyte530146 A7 B7 V. Description of the invention (1 Related applications This application claims rights under 35 USC § 120 of U.S. Utility Patent Application No. 09 / 669,796, filed on September 26, 2000, while the latter claims the United States provisional Patent Application No. 60 / 156,471 under 35 USC § 1 19. This case is also related to U.S. Utility Patent Application No. 09 / 670,453 filed on September 26, 2000, and filed on September 26, 2000 U.S. Utility Patent Application No. 09 / 669,369 and U.S. Utility Patent Application filed on March 23, 2001 (the title of which is to use a susceptor to increase the detection of an analyte by a substrate with a particulate structure " (Amplification 〇f Anaiyte
Detection by Substrates Having Particle Structures With Receptors),發明者,大衛][.克瑞邁爾(David j Kreimer)、 奥立格Α·依文(Oleg a. Yevin)和托馬斯H奴弗(Th〇mas hDetection by Substrates Having Particle Structures With Receptors), inventor, David] [. David J Kreimer, Oleg a. Yevin, and Thomas H. Nuffer h
Nufert)),所有此等專利申請案均全文以引用之方式併入 本文中。 發明範疇 本發明係關於製造具有熱輻射吸收性改良之表面。更確 切而言,本發明係關於製造具有由輕射傳吸熱及輕射教量 (表面及熱管。更確切而言,本發明係關於製造具有 以奈未顆粒結構覆蓋表面用於吸收寬帶電磁輻 窗及窗材料。 …I' 相關技藝說明 結構内的很多有用機械及電過程以熱形 P 、 熱量常不合乎需要,因為其導致結構;把f。该 再1如建築)溫度增加 -5-Nufert)), all of which are incorporated herein by reference in their entirety. Field of the Invention The present invention relates to the production of a surface having improved heat radiation absorption. More specifically, the present invention relates to the manufacture of heat-absorbing and light-radiating heat transfer surfaces (surfaces and heat pipes). More precisely, the present invention relates to the manufacture of windows with a nano-grain structure covering the surface for absorbing broadband electromagnetic radiation windows. And window materials.… I 'related techniques explain that many useful mechanical and electrical processes in the structure to form P, the heat is often not desirable, because it leads to the structure; increase f. This is like a building) temperature increase -5-
530146530146
及敏感设備溫度增加。此外,在用太陽輻射作為能源時, 加熱太陽輻射吸收元件為能量轉化中的第一步驟。下一 y ^用漓言使熱自太陽輪射吸收元件迅速傳遞到此等系 統中的其他元件。And the temperature of sensitive equipment increases. In addition, when using solar radiation as an energy source, heating the solar radiation absorbing element is the first step in energy conversion. The next step is to quickly transfer heat from the sun-radiation absorbing element to other elements in these systems.
裝〜 通吊,熱官比相同直徑的固體銅棒傳熱快。熱管傳熱損 ==、,且不需要投入額外能源,如,壓縮機。這一不需要 旎:輸入之傳熱能力有利於熱管的寬範圍技術應用。為防 止將結構加熱,已將窗及窗材料用於窗,以允許或阻止輻 射自窗一側向另一側傳遞。 此外在用太陽輻射作為結構加熱源時,輻射能量通過 窗傳入-種結構為第-步驟。在此結構内,輻射能量可由 $内的元件吸收,並由增溫顯示轉化成熱能。一些熱能可 月匕作為較長波長輻射耗散,包括紅外範圍輻射.。為促進有 放加熱’可理想使人射輻射易於通過’但阻止長波輕射離 開。Equipped ~ Through hanging, the heat official transfers heat faster than solid copper rods of the same diameter. Heat pipe heat loss ==, and does not require additional energy input, such as a compressor. This is not necessary 旎: the heat transfer capacity of the input is beneficial to the wide range of technical applications of the heat pipe. To prevent the structure from heating, windows and window materials have been used for windows to allow or prevent radiation from passing from one side of the window to the other. In addition, when solar radiation is used as a structural heating source, radiant energy is introduced into the structure through a window as a first step. In this structure, the radiant energy can be absorbed by the components inside the $ and converted into thermal energy by the temperature increase display. Some thermal energy is dissipated as longer wavelength radiation, including radiation in the infrared range. In order to promote the heating with radiation, it may be desirable to make it easy for human radiation to pass through, but to prevent light from being emitted by long waves.
未處理的玻璃或塑膠可顯示理想輻射傳遞性能,且廣泛 用於溫室中。玻璃廣泛用於窗子。然而破璃導熱,且能夠 傳導電磁輕射。由於電磁#射通路能夠使相當㈣熱通過 破璃窗敎’所以,理想提供對某電磁輻射波長具有低透 射性之窗用玻璃。Untreated glass or plastic shows ideal radiation transmission properties and is widely used in greenhouses. Glass is widely used in windows. However, broken glass conducts heat and can conduct electromagnetic light emission. Since the electromagnetic #radiation path can pass a considerable amount of heat through the broken glass window, it is desirable to provide a window glass having a low transmittance to a certain electromagnetic radiation wavelength.
I·熱管 圖1圖示一般熱管1〇〇之工作原理,該熱管為一種兩端封 閉的空心金屬管1〇5’芯135覆蓋該管的内表面。該管用揮 發性流體140填充。在將管一端11〇加熱時,如^所示,揮 -6 - 530146 A7 ---~------ B7 五、發明説明(3 ) "一"" ----- 發性流體140在該管端蒸發。蒸氣膨服,並移到該管的另 —較冷端120(彎箭頭),在此,揮發性流體冷凝,將散量放 = 二由於毛細管力作用,冷凝液由芯路徑135移回到 S 2煞%。因此,在溫熱端自環境吸收熱能蒸發,在冷端 々叛4r ,4 f釋放到環境,蒸發和冷凝迴圈為 基礎。 于…< 、、通常,外管由具有高導熱性之材料製成,例如,銅。在 接觸及對流傳熱條件下,此等材料吸收及/或發射執量。 但在包括籍射傳熱機制時,高導熱性本身不足以理想高效 傳^,而其他因素能夠改民此過程之效率。此等需要為: 2 5的外表面應吸收及/或發射寬波長範圍電磁輻射丨及2) “才料本體及外表面間的傳熱應有效。控制表面吸收及/ 或發射特性的一種方法為,使用具有微米大小幾何孔之結 構,亚用具有理想光譜發射之材料塗覆該管,如用鎢塗覆 (斯同(Stone)等人的美國專利第5,932,〇29號,其全文係以 引用方式併入本文中)。 玻璃及塑膠廣泛用於窗及窗覆蓋材料。然而,未經處理 $破璃及塑膠可能傳導電磁輻射。由於相當輻射熱可能由 電磁輻射通道通過玻璃窗損失,所以,理想提供對某電磁 私射波長具有低透射性而對其他波長保持透射性之窗用材 料。 發明概要 因此,本發明一個目的為研究在寬光譜範圍具有優良吸 收及發射電磁輻射能力之表面,此係藉助於材料内或施加I. Heat pipe Fig. 1 illustrates the working principle of a general heat pipe 100, which is a hollow metal pipe 105 ' core 135 closed at both ends to cover the inner surface of the pipe. The tube is filled with a volatile fluid 140. When heating one end of the tube 110, as shown by ^, wave -6-530146 A7 --- ~ ------ B7 V. Description of the invention (3) " 一 " " ----- The evaporative fluid 140 evaporates at the end of the tube. The steam is expanded and moved to the other-cold end 120 (curved arrow) of the tube, where the volatile fluid condenses, and the bulk is released = two. Due to the capillary force, the condensate moves from the core path 135 back to S 2%. Therefore, at the warm end, heat energy is absorbed from the environment to evaporate, and at the cold end, 4r and 4f are released to the environment, based on evaporation and condensation loops. In ... < Generally, the outer tube is made of a material having high thermal conductivity, for example, copper. Under contact and convective heat transfer conditions, these materials absorb and / or emit energy. However, when including the heat transfer mechanism, the high thermal conductivity is not sufficient for ideal and efficient heat transfer, and other factors can improve the efficiency of this process. These requirements are: 2 5 The outer surface should absorb and / or emit electromagnetic radiation in a wide wavelength range 丨 and 2) "The heat transfer between the material body and the outer surface should be effective. A method to control the absorption and / or emission characteristics of the surface In order to use a structure with micrometer-sized geometric holes, the tube is sub-coated with a material having ideal spectral emission, such as coating with tungsten (Stone et al., US Patent No. 5,932, 〇29, the entire text of which is (Incorporated by reference herein.) Glass and plastic are widely used in windows and window covering materials. However, untreated glass and plastic may conduct electromagnetic radiation. Since considerable radiant heat may be lost by electromagnetic radiation channels through glass windows, It is ideal to provide a window material that has low transmission to certain electromagnetic private emission wavelengths and maintains transmission to other wavelengths. SUMMARY OF THE INVENTION Therefore, an object of the present invention is to study a surface that has excellent absorption and emission of electromagnetic radiation in a wide spectral range. By means of material
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530146 發明説明(6 圖3描績本發明熱管輕射吸收端之具體設計。 圖4描繪本發明的_種熱管,㈣^ ^ 收集電磁輻射、將此能量轉 ——曰靶圍 經冷卻端。 荇又成…里亚將此熱量傳到管的 圖5描繪本發明一種熱管所用設計,哕哉其处 射傳吸收熱量及輻射熱量。 t、、、5犯夠,,莖由輻 ΞΓ/Γ描緣其上具有顆粒結構之窗破璃所用設計。 圖7為繪一片其上具有 線圖。 料^錢破璃之光密度曲 圖8a-8b騎其中顆粒結構處於窗 性具體實施例。 門之尽I明替代 圖9a-9b描繪其中窗覆蓋材料有 體實施例。 “七、有顆虹結構之本發明具 發明詳細說明 定義 本發明使用以下單詞及術語。 ’’碎形(fractal)”在本文中指一種由 度和單位數之間具有一定關係二位组成且在觀察尺 • . ' ’、( P ’尺度不變(scale- 7_叫之結構。僅舉例說明’-條連續線為-個i-維對 個平面為-個二維對象,而體積為-個三維對象。 ,;、而,如果-條線其間有間隙且τ、為—條連續,線,則維度 、…例如’如果線的〗/2失去’則碎形維度為”。與之相 似’如果一個平面上的點失去’則平面之碎形維度在_ “。如果孩平面上的y2點失去’則碎形維度為15。另 裝~ 訂 線 -10-530146 Description of the invention (6) Figure 3 depicts the specific design of the light-emitting absorbing end of the heat pipe of the present invention. Figure 4 depicts the heat pipe of the present invention, which collects electromagnetic radiation and transfers this energy to the target through the cooling end. Figure 5 depicts the heat transfer to the tube. Figure 5 depicts the design of a heat pipe according to the present invention. The transmission and absorption of heat and radiant heat are transmitted at its place. The design of the window-breaking glass with a granular structure is depicted on the edge. Figure 7 is a drawing with a line graph on it. Material ^ The optical density curve of the broken glass is shown in Figures 8a-8b in which the granular structure is in a window-like embodiment. Door Exemplary embodiments are shown in Figs. 9a-9b. The embodiment of the window covering material is described in detail. "Seven, the invention with a rainbow structure has a detailed description of the invention. The definition of the invention uses the following words and terms." Fractal " In this article, it refers to a structure consisting of two digits with a certain relationship between the degree and the unit number, and the observation rule •. '', (P 'scale-invariant (scale- 7_ called the structure. Only an example'-continuous line is -I-dimensional to plane are two-dimensional objects, The volume is a three-dimensional object., And, if there is a gap between the lines and τ is a continuous, line, then the dimension, ... For example, if the line's / 2 is lost, the fractal dimension is "." Similarly, if the point on a plane is lost, then the fractal dimension of the plane is _ ". If the y2 point on the child plane is lost, then the fractal dimension is 15. Separately installed ~ Order -10-
530146 五、發明説明( 外’如果-個固體上的》點失去,則 度不k的結構中,不考慮所觀察面^又為2.5。在尺 似乎相似。因此’碎形結構為一種有’物件之結構 規則結構不同。 〜構’與無序的不 在本又+碎形聚集體f,或,,碎形 小結構,其包括至少约1〇〇個缔合在一起^:種有限大 在由包含碎形缔合體之單獨顆粒大小限粒,且 合體限定的上限限制的區域内顯示尺度:限及碎形缔 在本文中,”碎形維度 此’ R為觀察之面積,顆粒數,:二:度^此在 :非碎形固體中’如果觀察之半徑增加2倍 : 内觀察到的顆粒數捭 3 、〗在这肖豆積 之半;^力2拉"么。但在對應碎形中,如果觀察 丰 加倍,則所觀察顆粒數增加小於23倍。 j本又中’ Π碎形顆粒缔合體”指大量經佈置的顆粒,該 果、粒,二你^置,使每單位體積或每表面單位的顆粒數(因變 數)隨觀察尺度(自變數)非線性變化。 在本文中連接劑,指具有二或多個能夠結合到表面且 允终顆粒一起附著形成顆粒團之之化學基團之原子、分 子、部分或分子錯合物。最簡單連接劑連接兩個顆粒。分 枝連接劑可將大量顆粒連接在一起。 在本文中,”有序結構”指非不規則結構。 在本文中’’’顆粒結構”指相互以一種方式缔合以允許增 強電場回應入射電磁輻射之單獨顆粒之集團。顆粒之實例 包括金屬、經金屬塗覆之聚合物及弗樂林(fullerenes)。 -11- 本紙張尺度適/¾中國國家標準(CNS) A4規格(21〇^797公爱)530146 V. Description of the invention (outside 'if a point on a solid body is lost, the structure with degree k is not taken into account, and the observed surface is 2.5 again. It seems similar in ruler. Therefore,' fragment structure is a kind of ' The structure of the object is different from the regular structure. ~ Struct 'and the disordered absent + fragmented aggregate f, or, a fragmented small structure, which includes at least about 100 associated together The size is limited by the size of the individual particles containing the fragmented association, and the upper limit defined by the combination shows the scale: limit and fragmentation. In this article, "fragmentation dimension" R is the area of observation, the number of particles ,: Two: Degree ^ Here: in non-fragmented solids' If the radius of observation is doubled: the number of particles observed inside 捭 3, is half of this Xiaodou product; ^ force 2 pull " but in the corresponding In the fractal shape, if you observe the doubling of the abundance, the number of particles observed will increase less than 23 times. J This "zhong fractal particle association" refers to a large number of arranged particles. The number of particles per unit volume or unit per surface (dependent variable) depends on the observation scale (from Number) Non-linear change. In this context, a linking agent refers to an atom, molecule, part or molecular complex with two or more chemical groups capable of binding to the surface and allowing the final particles to attach together to form a particle group. The simplest A linking agent connects two particles. A branching linking agent can connect a large number of particles together. In this context, "ordered structure" refers to an irregular structure. In this context, "" particle structure "means to associate with each other in one way. A group of individual particles that allow an enhanced electric field to respond to incident electromagnetic radiation. Examples of particles include metals, metal-coated polymers, and fullerenes. -11- This paper is compliant with China National Standards (CNS) A4 specifications (21〇 ^ 797 public love)
五、發明説明(8 ,,顆粒結構,,意義中亦包括於介電表面上包 材料中包埋顆粒之薄膜或複合材料。 4或万… 在本文中,”滲透點”指在表面由介質中的表 聋 導檢測:不傳導增加之當時傳導表面上的點 :: ”片”傳導的-種方法為經由施加於表面上^ f面或 在以中,”無規結構,,指即非有序又非之^構。 考慮觀祭:及尺度’無規結構似乎均勻,且其中二尺: 包括至少數個顆粒。 規氣爲..度 在本又中’共据"指入射、散射及/或發射 二具=由電磁輕射激發且增加電磁輕 子之表面之相互作用。 # /又心私 在本又中,共振田壽”指在顆粒結構内或接近卿 其中入射電磁輻射電場發生增加之區域。 -』、、、。冓 在本文巾定‘直控”(scaling diameter)指巢化社槿φ 顆粒間的關係,其中不考慮顆 =中 比(定標比)。 有相冋顆粒直徑 發明之具體實施例 本發明包括在熱管之吸收及/或發射性表面上 結:。奈米顆粒結構能夠被施加於熱管之内表 可: :有效吸收或發射熱能。藉由熱管之外表面增加吸:: 广可更容易將熱能傳到熱管之内部,且因此增加二 軍發性流體之蒸發速率。揮發性流體之蒸發增加能二 致所蒸發流體流動增加,由此使熱量自熱管之匕^ 熱管之發射部分流動增加。流到發射部分的熱量增力:; -12-V. Description of the invention (8, particle structure, meaning also includes the film or composite material in which the particles are embedded in the dielectric surface. 4 or 10,000 ... In this article, "penetration point" means that the surface is covered by the medium In the table, the deafness detection: the point on the conducting surface at the time when non-conduction increases: "sheet" conduction-a method is applied on the surface ^ f surface or in the middle, "random structure, refers to non- Ordered and unstructured. Consider the viewing sacrifice: and the size of the random structure seems to be uniform, and two of them: include at least a few particles. The rules are: the degree in this book and the 'common basis' refers to incidence, Scattering and / or emission == surface interactions that are excited by electromagnetic light emission and increase the surface of electromagnetic lepton. # / 又 心 私 In this context, resonance Tianshou "refers to the incident electromagnetic radiation in or near the particle structure. The area where the electric field increases.-",,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,, ', 指', refers to the relationship between the particles of Chaohua Co., Ltd., excluding particles = medium ratio (scaling ratio) A specific embodiment of the invention of the diameter of the particles On the absorption and / or emissive surface of the heat pipe: The nano-particle structure can be applied to the inner surface of the heat pipe. It can:: effectively absorb or emit heat energy. By increasing the absorption by the outer surface of the heat pipe: The heat energy is transmitted to the inside of the heat pipe, and therefore the evaporation rate of the second fluid is increased. The increased evaporation of the volatile fluid can increase the flow of the evaporated fluid, thereby increasing the flow of heat from the heat pipe's emitting part. Force increase of the heat flowing to the emission part: -12-
本紙張尺度適巾國國家標準(CNS) Α4規格(21GX297公D 530146This paper is suitable for national standards (CNS) Α4 specifications (21GX297 male D 530146)
530146530146
進入結構物的熱量能夠減少。在外部溫度降低且需要增加 進入輻射量時,可除去塗層,藉以允許輻射進入該結構 物。 除結構物所用的窗外,本發明亦包括較小結構物所用塗 層’例如’其中需要光吸收及/或透射性能之管、載片及 其它裝置。例如,在本發明的某些具體實施例中,可提供 對可能干擾檢測電磁輻射或”寄生輻射”的某段波長具有低 透射率之光學池或樣品容器,如2〇〇〇年9月26申請的同在 申請中美國專利申請案第09/669,369號所述,其全文係以 引用之方式併入本文中。此等具體實施例亦可理想用於檢 測分析物,如2000年9月26申請的同在申請中美國專利^ 凊案第09/670,453號所述,其全文係以引用之方式併入本 文中。 理想用於本發明方法之結構包括含小顆粒之結構,此結 構包括作為子集的碎形缔合體,在此稱為顆粒結構。此等 顆粒結構可具有使電子與入射及外出電磁輻射共振的物理 及化學結構特徵。 I·製造顆粒結構 理想用於本發明之顆粒結構可包括任何其中能夠在寬波 長範圍吸收或發射電磁信號之結構。關於金屬顆粒、社構之 討論不用於限制本發明範圍,僅用於說明目的。亦可包括 其他結構’包括碎形結構。 A.製造金屬顆粒 可使用此項技藝中的已知方法製造本發明一些具體實施 -14- 本紙張尺中國國家標準(CNS) A4規格(2ιο χ 297公爱)--------The amount of heat entering the structure can be reduced. When the external temperature decreases and the amount of incoming radiation needs to be increased, the coating can be removed to allow radiation to enter the structure. In addition to windows for structures, the invention also includes coatings for smaller structures, such as tubes, slides and other devices where light absorption and / or transmission properties are required. For example, in certain embodiments of the present invention, an optical cell or sample container having a low transmittance to a certain wavelength range that may interfere with the detection of electromagnetic radiation or "parasitic radiation" may be provided, such as September 26, 2000 The co-pending application is described in US Patent Application No. 09 / 669,369, the entirety of which is incorporated herein by reference. These specific examples are also ideal for the detection of analytes, as described in US Patent Application No. 09 / 670,453, co-pending application filed on September 26, 2000, which is incorporated herein by reference in its entirety. . Desirable structures for use in the method of the present invention include structures containing small particles. This structure includes, as a subset, fractal associations and is referred to herein as a granular structure. These particle structures may have physical and chemical structural features that resonate electrons with incident and outgoing electromagnetic radiation. I. Manufacture of granular structure The granular structure ideally used in the present invention may include any structure capable of absorbing or emitting electromagnetic signals over a wide wavelength range. The discussion of metal particles and social structure is not intended to limit the scope of the present invention, but only for illustrative purposes. Other structures' may also be included including fractal structures. A. Manufacture of metal particles The known methods in this technology can be used to make some specific implementations of the present invention. -14- Chinese paper standard (CNS) A4 (2ιο χ 297)
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例所用金屬顆粒,如,塔查(Tarcha)等人的美國專利第 5, :)67, 628號,其全文係以引用之方式併入本文中。金屬膠 體可由貴金屬組成,確切為元素金或銀、銅、鉑、鈀及其 它已知用於在所需光譜範圍提供寬帶吸收及發射之金屬。 通常,為製造金屬膠體,可使含金屬鹽之稀溶液與還原劑 發生化學反應。還原劑可包括抗壞血酸鹽、擰檬酸鹽、硼 氫化物、氫氣及類似物。化學還原金屬鹽能夠在溶液中產 生單質金屬,該單質金屬結合,以生成包含可為相對球形 形狀之金屬顆粒之膠體溶液。 製造金膠體及碎形結構 在本發明-具體實施例中’為產生金核之溶液,在劇列 攪拌下製備NaAuCU溶於水之〇.〇1%溶液產生。加入i毫升 (、1” 1%檸檬酸鈉之溶液…混合】分鐘後,在劇烈攪:下 加入1毫升含0.075% NaBH4及〇.1%檸檬酸鈉之溶液。使該 反應進行5分鐘,以製備具有約2奈米平均直徑之金核。 將含金核之容液在代冷藏’直至需要。該溶液可原樣使 用’或用於製造較大大小之顆粒⑽如’至高約5〇奈米直 徑),製造時,在劇烈攪拌下快速將3〇微升含金核之 及0.4毫升1%檸檬酸鈉溶液加人在⑽毫升_中稀釋的以。 HAuCUH.W)之溶液,將該混合物煮沸15分鐘然 卻至室溫。冷卻期㈤,溶液中的顆粒能夠形成碎形結: 可將所得膠體及/或碎形顆粒結構貯存於暗色瓶中。"在包括玻璃之電介質表面上沈積增強顆粒可產生能夠增 -15-Examples of metal particles used are, for example, Tarcha et al. US Patent No. 5, :) 67, 628, the entirety of which is incorporated herein by reference. Metal colloids can be composed of precious metals, exactly the elements gold or silver, copper, platinum, palladium, and other metals known to provide broadband absorption and emission in the desired spectral range. Generally, in order to make a metal colloid, a dilute solution containing a metal salt can be chemically reacted with a reducing agent. The reducing agent may include ascorbate, citrate, borohydride, hydrogen, and the like. The chemically reduced metal salt is capable of producing elemental metals in solution, which element metals are combined to produce a colloidal solution containing metal particles which may be relatively spherical in shape. Manufacture of gold colloids and fractal structures In the present invention-specific embodiments, ′ is a solution that produces gold nuclei, and a 0.01% solution of NaAuCU dissolved in water is prepared under stirring in a column. Add 1 milliliter (, 1 "1% sodium citrate solution ... mixed) minutes, and then add 1 milliliter of a solution containing 0.075% NaBH4 and 0.1% sodium citrate under vigorous stirring. Allow the reaction to proceed for 5 minutes, To prepare gold nuclei with an average diameter of about 2 nm. Refrigerate the container containing the gold nuclei until needed. This solution can be used as is 'or used to make larger size particles such as' up to about 50 nm (Meter diameter), when manufacturing, quickly add 30 microliters of gold nucleus and 0.4 ml of 1% sodium citrate solution to a solution diluted in ⑽ml_ with vigorous stirring. HAuCUH.W) The mixture is boiled for 15 minutes and then reaches room temperature. During the cooling period, the particles in the solution can form broken knots: the resulting colloid and / or broken particle structure can be stored in dark bottles. &Quot; On a dielectric surface including glass Deposition-enhancing particles can produce -15-
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530146 A7 B7 五、發明説明(12 ) 強電磁信號之薄膜。此等薄膜可薄約10奈米。特別是,電 場增強在此等薄膜上之分佈可能不均勾。此等增強區域為 共振疇。此等區域可特別用於對分析物結合及檢測所有受 體定位。對於包埋於介電材料之薄膜或顆粒結構,製造增 強結構的一種方法為處理該表面,直至出現滲透點。檢測 片阻抗及體阻抗所用方法為技藝上所熟悉。 實例2 用雷射燒蝕製造金屬顆粒及碎形結構 除上述液相合成外,可用雷射燒姓製造金屬顆粒。將金 屬箔片置於含低濃度稀有氣體之室中,稀有氣體如氦、 氖、氬、氙或氪。使箔片暴露於雷射光或其他熱源可導致 金屬原子蒸發,此等原子在室中的懸浮系中可由無規擴散 自發聚集成碎形或其他顆粒結構。此等方法為技藝上所熟 悉。 B.製造含顆粒之薄膜 為製造含本發明一具體實施例之金屬膠體顆粒之基材, 可將實例1或2所述之金屬膠體顆粒沈積於石英載片上。可 以類似方式製造其他結合無規結構、非碎形有序結構及/ 或碎形聚集體之薄膜。 實例3 製造含金碎形結構之石英載片 將石英載片(2.5釐米χ〇.8釐米χ〇.1釐米)在一種HC1:HN〇3 (3: 1)之混合物中清洗數小時。然後用去離子H2〇 (Millipore Corporation)將載片清洗至約18兆歐姆電阻,隨 16- 本紙張尺度適用中國國家標準(CNS) A4規格(210 X 297公釐) 530146 A7 B7 五、發明説明(13 ) 後用CH3〇H清洗。將載片浸在1: 5胺丙基三甲氧基矽烷稀 釋於CH3〇H之溶液。在浸入上述膠體金溶液之前,將載片 徹底用CH3OH(分光光度級)及去離子&0清洗。接著將載 片浸入以上金膠體溶液。在此期間,金膠體顆粒可能沈積 並附著石英載片表面。24小時後,膠體衍生完成。一旦經 附著,金膠體奈米複合材料對石英表面的結合力就很強, 且基本上不可逆。在進行步騾期間,用此等經衍生載片之 紫外及/或可見光吸收光譜評估衍生步騾品質及再現性。 用電子顯微法監測該製程,以估定膠體塗覆密度、表面上 的金膠體顆粒分佈及金膠體顆粒之大小。 C.顆粒聚集成顆粒結構 根據本發明之其他具體實施例,可用數種方法形成顆粒 結構。已知金屬膠體能夠在表面上沈積,且在聚集時形成 約1.8之碎形維度之碎形結構,薩分諾(Safonov)等人,膠 體顆粒之碎形聚集體中的選擇性光學修飾之光譜關係 (Spectral Dependence of Selective Photomodification in Fractal Aggregates of Colloidal Particles),Physical Review Letters 80(5): 1102-1 105 (1998),其全文係以引用方式併 入本文中。圖1描繪適合本發明所用方法之顆粒結構。其 顆粒係以尺度不變之方式佈置,這將促進雷射光照明時共、 振疇生成。 除碎形結構外,可產生有序非碎形結構及無規結構。此 等不同類型結構可具有與用電磁輻射檢測分析物有關的增 強信號所需之性能。 -17- 本紙張尺度適用中國國家標準(CNS) A4規格(210 X 297公釐) 零 裝 訂530146 A7 B7 V. Description of the invention (12) Film with strong electromagnetic signal. These films can be as thin as about 10 nm. In particular, the distribution of electric field enhancement on these films may be uneven. These enhancement regions are resonance domains. These areas are particularly useful for binding analytes and detecting all receptors. For thin film or granular structures embedded in a dielectric material, one way to make a reinforced structure is to treat the surface until a penetration point appears. The methods used to measure the impedance of the sheet and body impedance are technically familiar. Example 2 Manufacturing of metal particles and fractal structures by laser ablation In addition to the liquid phase synthesis described above, metal particles can be manufactured by laser ablation. The metal foil is placed in a chamber containing a low concentration of a rare gas such as helium, neon, argon, xenon or krypton. Exposure of the foil to laser light or other heat sources can cause the metal atoms to evaporate, and these atoms can spontaneously diffuse into a fractal or other granular structure in the suspension system in the chamber. These methods are well known in the art. B. Manufacture of Particle-Containing Films In order to produce a substrate containing metal colloid particles according to a specific embodiment of the present invention, the metal colloid particles described in Example 1 or 2 can be deposited on a quartz slide. Other films incorporating random structures, non-fragmented ordered structures and / or fragmented aggregates can be made in a similar manner. Example 3 Manufacture of a quartz slide with a gold fractal structure A quartz slide (2.5 cm x 0.8 cm x 0.1 cm) was washed in a mixture of HC1: HNO3 (3: 1) for several hours. Then use deionized H2O (Millipore Corporation) to clean the slide to about 18 megaohm resistance. With 16- this paper size applies Chinese National Standard (CNS) A4 specification (210 X 297 mm) 530146 A7 B7 V. Description of the invention (13) After washing with CH3OH. The slide was immersed in a solution of 1: 5 aminopropyltrimethoxysilane diluted in CH3OH. Before immersing in the above colloidal gold solution, the slide was thoroughly washed with CH3OH (spectrophotometric grade) and deionized & 0. The slide was then immersed in the above gold colloid solution. During this time, gold colloidal particles may deposit and adhere to the surface of the quartz slide. After 24 hours, colloid derivatization was complete. Once attached, the gold-colloidal nanocomposite has a strong bond to the quartz surface and is essentially irreversible. The UV and / or visible absorption spectra of these derivatized slides were used to evaluate the quality and reproducibility of the derivatized steps during the steps. The process was monitored by electron microscopy to estimate the colloidal coating density, the distribution of gold colloidal particles on the surface, and the size of the gold colloidal particles. C. Particle Aggregation into Particle Structure According to other embodiments of the present invention, the particle structure can be formed in several ways. It is known that metal colloids can be deposited on the surface and form a fractal structure with a fractal dimension of about 1.8 when aggregated. Safonov et al., Spectra of selective optical modification in fractal aggregates of colloidal particles Relationship (Spectral Dependence of Selective Photomodification in Fractal Aggregates of Colloidal Particles), Physical Review Letters 80 (5): 1102-1 105 (1998), the full text of which is incorporated herein by reference. Figure 1 depicts the particle structure suitable for the method used in the present invention. The particles are arranged in a scale-invariant manner, which will promote the generation of common and vibrating domains during laser light illumination. In addition to fractal structures, ordered non-fractal structures and random structures can be produced. These different types of structures may have the performance required to enhance signals associated with detecting analytes with electromagnetic radiation. -17- This paper size is in accordance with Chinese National Standard (CNS) A4 (210 X 297 mm) Zero binding
530146 A7 B7 五、發明説明(14 ) 為製造有序非碎形結構,可使用具有不同長度之化學連 接劑,如以下順序詳述。此外,用相同大小之^接劑可產 生有序結構,這可能對某些應用有用。 在本發明的某些具體實施例中,可使顆粒一起結合,以 形成具有共振性能之結構。通常,具有球形、橢球形或棒 形之顆粒可能較為理想。對於橢球形顆粒,顆粒具有長軸 (x)、另一軸(y)及第三軸(z)可能合乎需要。通常,可能需 要其具有所要使用入射電磁輻射波長(λ )約〇 〇5至約i倍之 X。對棒而言,X可理想小於約4又,或小於約3又,戋小於 約2又,在其他具體實施例中小於約1λ,&在另外的具體 實施例中小於約% λ。棒端可為平、錐狀或長方形(長橢圓 形)’或具有能夠促進共振的其他形狀。530146 A7 B7 V. Description of the invention (14) In order to manufacture an ordered non-fragmented structure, chemical linkers with different lengths can be used, as detailed in the following sequence. In addition, using the same size of the coupling agent can produce an ordered structure, which may be useful for some applications. In some embodiments of the present invention, the particles can be combined together to form a structure having resonance properties. In general, particles with a spherical, ellipsoidal or rod shape may be desirable. For ellipsoidal particles, it may be desirable for the particles to have a major axis (x), another axis (y), and a third axis (z). Generally, it may be necessary to have X of about 0.05 to about i times the wavelength (λ) of the incident electromagnetic radiation to be used. For rods, X may ideally be less than about 4, or less than about 3, 戋 less than about 2, and less than about 1λ in other embodiments, and less than about% λ in other embodiments. The rod end may be flat, tapered, or rectangular (oblong) 'or have other shapes that promote resonance.
尺度之分佈密度。 起,以形成提 在其他具體實施例中,棒可端_端連在一起 供共振性能增強之長結構。The distribution density of the scale. In other embodiments, the rods can be connected end-to-end to provide long structures with enhanced resonance performance.
序巢化陣列中 ,可理想使用 所懸浮顆粒可 本紙張尺度適用巾s a家標準(CNS) μ規格 530146 A7In the nested array, it can be used ideally. The suspended particles can be used in this paper. Standards (CNS) μ size 530146 A7
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530146 A7 B7 五、發明説明(16 ) 頻率可能比與表面電漿激元共振有關的單體吸收帶寬跨越 更寬光譜範圍。儘管如此,其他理論亦可解釋碎形結構之 光學修飾效應,但本發明不受任何特定操作理論限制。 銀碎形聚集體之光學修飾可在小約24X 24X 48奈米3之疇 中發生(薩分諾等人,Physical Review letters 1102- 1 105 (199 8),其全文係以引用方式併入本文中)。在雷射 波長增加時,由碎形介質吸收的能量可能位於漸進性較少 數單體中。在吸入共振轉的能量增加時,在此等位置的溫 度可能增加。在11毫焦耳/釐米2之功率時,具有550奈米波 長的光可能產生約600 K之溫度(薩分諾等人,Physical Review Letters 80i5V· 1 1 02-1 1 05 (1 99 8),其全文係以引用 方式併入本文中)。在此溫度(為銀熔化溫度的約一半溫 度),膠體可能熔結(薩分諾等人,M·),其全文係以引用方 式併入本文中),藉以形成穩定碎形奈米複合材料。 如本文中所使用,為完成光聚集,可使表面上的金屬膠 體暴露於具有在約400奈米至約2000奈米範圍波長之入射 光脈衝。在選擇性具體實施例中,該波長可在約450奈米 至約1079奈米之範圍内。入射光強度可在約5毫焦耳/釐米2 至約20毫焦耳/釐米2之範圍内。在選擇性具體實施例中, 入射光可在11毫焦耳/釐米2強度具有1079奈米之波長。 尤其用於本發明之碎形聚集體可用具有在約10奈米至約 100奈米直徑範圍大小之金屬顆粒製成,在選擇性具體實 施例中,可具有約50奈米直徑。本發明之典型碎形結構由 至高約1000個顆粒組成。 -20- 本紙張尺度適用中國國家標準(CNS) A4規格(210 X 297公釐)530146 A7 B7 V. Description of the invention (16) The frequency may span a wider spectral range than the monomer absorption bandwidth related to the surface plasmon resonance. Nevertheless, other theories can also explain the optical modification effect of the fractal structure, but the present invention is not limited by any particular theory of operation. Optical modification of silver fractal aggregates can occur in domains as small as about 24X 24X 48 nm 3 (Safano et al., Physical Review letters 1102- 1 105 (199 8), the entirety of which is incorporated herein by reference) in). As the laser wavelength increases, the energy absorbed by the fractal medium may be located in a less progressive monomer. As the energy of the suction resonance revolution increases, the temperature at these locations may increase. At a power of 11 mJ / cm2, light with a wavelength of 550 nm may produce a temperature of about 600 K (Safano et al., Physical Review Letters 80i5V · 1 1 02-1 1 05 (1 99 8), Its entirety is incorporated herein by reference). At this temperature (which is about half the temperature at which silver is melted), the colloid may sinter (Safano et al., M.), which is incorporated herein by reference in its entirety), thereby forming a stable broken nanocomposite . As used herein, to complete light gathering, the metal colloid on the surface may be exposed to an incident light pulse having a wavelength in the range of about 400 nanometers to about 2000 nanometers. In alternative embodiments, the wavelength may be in the range of about 450 nm to about 1079 nm. The intensity of the incident light may range from about 5 mJ / cm2 to about 20 mJ / cm2. In an alternative embodiment, the incident light may have a wavelength of 1079 nm at an intensity of 11 mJ / cm2. The fractal aggregates particularly useful in the present invention can be made of metal particles having a size in the range of from about 10 nanometers to about 100 nanometers, and in selective embodiments may have a diameter of about 50 nanometers. The typical fractal structure of the present invention consists of up to about 1000 particles. -20- This paper size applies to China National Standard (CNS) A4 (210 X 297 mm)
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530146 五、發明説明(17 ) 圖2描緣經聚集且適用於本發明方法之顆粒結構。金屬 顆粒之融化局部區域可以觀察到(圓)。 π·顆粒結構 在本發明的某些具體實施例中,本發明之顆粒結構可具 有碎形結構性能。碎形結構可為顯示自相似性模型之結 構。自相似性指其全部結構為尺度不變數,因為該結構在 I放大範圍似乎相似。碎形結構在自然中廣泛存在,舉例 說明,:雲。碎形物體亦可人工產生。例如,在將金屬表 面之景觀以自相似三角形或其他形狀佈置時,此等碎形物 體可充當所謂,,碎形天線”。此等天線可比具有更規則結 之天線允許更寬範圍的無線電接收及發射。 類似當具有入射光波長約直徑之金屬顆粒在表面上以 類碎形結構形式佈置時,此等碎形表面可在寬光學範圍顧 示吸收(沙雷(shalaev) ν·Μ.等人, 131-152 (1998),其全文仿以 a 用方式併入本文中)。在此情況下,類碎形結構可歸因於 當f面區域尺度增加時在此區域每表面面積顆粒數降低之 事貫。解釋此等碎形表面吸收的一種理論為干擾由單獨顆 粒中電磁波誘導的偶極矩振動。根據一種理論,入射光子' 跨顆粒誘導一個場,並由此使金屬中的流動電子以入射電 磁場之頻率移動。此集體性移動稱為,,電漿激元波,,。根^ 一種理論,電子集體性振動應歸於碎形結構内金屬顆粒中 的電漿激元波之強偶極與多極相互作用。由於金屬顆㈣ 構的幾乎任何距離及定向能夠在此碎形結構系統中存在 -21· 本紙張尺度適用中國國家標準(CNS) A4規格(210X297公釐) 五、發明説明(18 ::在此結構内形成大量可能的"共振空腔”。"共振空腔,, 才曰美供入射光波長所用 別在特定波長組吸收及/或二;::佈门置::…分 結構可存在很多不同共振空:二;皮。因為在奈米顆粒 或發射很多不同科。因此 結構吸收及/ h丑 /、羊Q此,所有此寺空腔在寬範圍波長 ”振芡本fa能力產生此碎形結構之寬吸收帶。 化學還原金屬膠體溶液、雷射燒姓表面、表面触刻、薄 艇退火(僅舉例說明)用於產生類碎形結構(测年9月㈣ 凊的吴國專利中請案㈣/67M53號、2_年9月%申請的 吴國專利申請案第嶋69,369號、2〇〇1年3月23日申請的美 國貫用專”請案(其標題H感受^料具㈣粒結構 裝- <基材增大分析物檢測”,發明者,大衛z•克瑞邁爾、奥立 格A_依又和托馬斯H奴弗)以及沙雷⑽心叫等人(1998), 所有此等專利均全文以引用之方式併入本文中)。典型類 訂 碎形結構可藉由使遠離平衡系統達到低能量態獲得。類碎 形結構可在此系統中自發性生成。 除砰形結構外,其他顆粒結構亦可導致本發明之吸收及 /或發射性能增強。 以下描述製造能夠用於熱管或窗材料表面之顆粒結構。 Α·化學定向合成顆粒結構 在本發明的某些具體實施例中,可用化學方法製造奈米 顆粒結構。首先,可根據上述方法製造金屬顆粒,或者, 可自供應處豕購貝(加利福尼亞,弗瑞蒙特,奈格公司 (NanoGiram Inc·,Fremont California))。第二,可使顆粒一 -22-530146 V. Description of the invention (17) Figure 2 depicts the structure of particles that are aggregated and suitable for the method of the present invention. A localized area of melting of the metal particles can be observed (round). π. Particle structure In some embodiments of the present invention, the particle structure of the present invention may have a fractal structure property. The fractal structure may be a structure showing a self-similarity model. Self-similarity means that all of its structures are scale-invariant, because the structures appear to be similar in the I magnification range. Fragmented structures are widespread in nature, for example: clouds. Fragmented objects can also be created artificially. For example, when the landscape of a metal surface is arranged in a self-similar triangle or other shape, these fractal objects can serve as so-called, fractal antennas. "These antennas can allow a wider range of radio reception than antennas with more regular knots Similar to when metal particles with an approximate diameter of incident light are arranged on the surface in a fractal-like structure, these fractal surfaces can absorb absorption over a wide optical range (shalaev ν · M., Etc. Human, 131-152 (1998), the full text of which is incorporated herein as a). In this case, the fractal-like structure can be attributed to the number of particles per surface area in this area as the scale of the f-plane area increases. Decreasing consistency. One theory to explain the absorption of these fractal surfaces is to interfere with the dipole moment vibration induced by electromagnetic waves in individual particles. According to a theory, incident photons' induce a field across the particles and thereby cause the flow in the metal The electrons move at the frequency of the incident electromagnetic field. This collective movement is called, plasmon exciter wave, .... A theory is that the collective vibration of electrons should be attributed to the metal particles in the fractal structure. The strong dipole and multipole interaction of the plasma exciton waves in the medium. Because almost any distance and orientation of the metal particle structure can exist in this fractal structure system. -21 · This paper applies the Chinese National Standard (CNS) A4 specification (210X297 mm) 5. Description of the invention (18: A large number of possible " resonant cavities " are formed in this structure. &Quot; Resonant cavities are only used in the specific wavelength group for the incident light wavelength Absorption and / or two; :: cloth door set :: ... substructure can have many different resonance spaces: two; skin. Because nano particles or many different families of emission. So the structure absorption and / hug /, sheep Q this All the temple cavities have the ability to oscillate this fractal structure in a wide range of wavelengths to generate a wide absorption band of this fractal structure. Chemical reduction metal colloid solution, laser burning surface, surface contact engraving, thin boat annealing (only for illustration) Used to generate a fractal-like structure (Wu Guo Patent Application No. / 67M53 in September 测 ㈣ 测 67 67 / 67M53, 2% in September _ Wu Guo Patent Application No. 嶋 69,369, 2001 3 Application for U.S. General Application for Application on March 23 (the title H feels ^ data Pellets Structure Pack-< Substrate Enlargement Analyte Detection ", the inventors, David Z. Kremmer, Olig A_Yi, and Thomas H. Nuffer), and Shale Mining, et al. ( 1998), all of these patents are incorporated herein by reference in their entirety). Typical fractal structures can be obtained by moving away from the equilibrium system to a low energy state. Fractal structures can be generated spontaneously in this system In addition to the bang structure, other particle structures can also lead to enhanced absorption and / or emission properties of the present invention. The following describes the manufacture of particle structures that can be used on the surface of heat pipes or window materials. A. Chemically oriented synthetic particle structures in the present invention In some embodiments, the nanoparticle structure can be manufactured chemically. First, metal particles can be manufactured according to the above method, or shellfish can be purchased from a supplier (NanoGiram Inc., California, Fremont, Fremont California)). Second, it makes the particles a -22-
五、發明説明(19 ) 起結合成第一級結構’例如’顆粒對。然 ㈣一,结合成第二級結構,例如,對顆粒對。 猎由使弟—級結構一起結合產i第三級碎形結#。 了 在本發明之替代性具體實施例中,生 :可用:學方法進行。-旦已製造金屬膠體顆1列 由硫羥或其他類型適用化學鍵使各顆粒結合到連接^ :在然:可使連接劑分子相互結合’以將相鄰膠體顆 接在-起。顆粒間之距“連接射子總長度之函數 能需要選擇顆粒對連接劑分子之化學計量比。如果使用連 接劑分子太少,則顆粒陣列太鬆,或根本不能生成。相 反,如果連接劑分子對顆粒之比太高,則陣列可能變得太 二緊,甚至可能生成非不規晶體結構,因此,沒有促進喇 曼(Raman)共振趨向。 通常,可能需要順序進行連接步驟,其中該第一步驟包 括將連接劑分子在不允許顆粒一起交聯之條件下加入單獨 顆粒。僅舉例說明,此等連接劑可只在一端包括具有反應 基團之低聚核菩酸。在第一步驟期間,低聚核甞酸之反應 端可與金屬顆粒結合,由此生成第一顆粒-連接劑種類, 並具有連接^ι1】之游離。可依賴將要結合到顆粒的連接劑 分子數目選擇連接劑分子對顆粒之比。可在不同反應室中 再次用具有游離端之連接劑使第二連接劑結合到顆粒的另 外基團,藉以產生第二連接劑-顆粒種類。 在那些反應進行後,可將不同連接劑-顆粒種類混合, 且連接劑能夠一起結合,以生成由連接劑分子連接的,1顆 530146 五、發明説明(2〇 A7 B7Fifth, the invention description (19) is combined into a first-order structure, for example, a particle pair. However, at first, they are combined into a secondary structure, for example, a pair of particles. Hunting by the brother-level structure together to produce a third-level broken knot #. In alternative embodiments of the present invention, students can use: learn methods. -Once a row of metal colloidal particles has been manufactured, each particle is bound to the link by a thiol or other type of suitable chemical bond ^: Of course: the linker molecules can be bound to each other 'to link adjacent colloidal particles together. As a function of the distance between particles, the total length of the connected emitters, the stoichiometry of the particles to the linker molecules needs to be selected. If too few linker molecules are used, the particle array is too loose, or cannot be generated at all. Conversely, if the linker molecules The ratio of particles is too high, the array may become too tight, and even non-random crystal structures may be generated. Therefore, the Raman resonance trend is not promoted. Generally, the connection step may be performed sequentially, where the first The steps include adding linker molecules to individual particles under conditions that do not allow the particles to be crosslinked together. By way of example only, these linkers may include oligonuclear acids with reactive groups at one end only. During the first step, The reactive end of the oligomeric acid can be combined with the metal particles, thereby generating the first particle-linker species, and having the freeness of the linker. The linker molecule pair can be selected depending on the number of linker molecules to be bound to the particles. Ratio of particles. A second linker can be bound to another group of particles in a different reaction chamber using a linker with a free end again. A second linker-particle type is generated. After those reactions, different linker-particle types can be mixed, and the linker can be combined together to produce a linker molecule connected by the linker molecule. 530146 V. Description of the invention (2 〇A7 B7
粒對”。 舉例說明,圖2a至2c圖解製造本發明碎形結構之方法。 在圖2a中’金屬顆粒10用前述方法生成。短連接劑2〇具有 也夠結合到金屬顆粒1 0之化學活性端。例如,連接劑在 該連接劑20各端具有硫氫基(〃SH〃)。在化合時,金屬顆粒 10與連接劑20之SH端結合,以生成顆粒對3〇。 圖2b圖示能夠用於生成顆粒對簇之步驟。顆粒對3〇與中 等長度的連接劑40反應,以形成簇50。 圖2c圖示能夠用於生成本發明奈米尺度碎形結構之步 驟。簇50與長連接劑60反應,以形成奈米尺度碎形結構 70 ° 可選擇連接劑分子,以提供所需長度。一般使用有機部 分之聚合物。例如’可用芳基二-硫醇或二-異腈分子連 接。或者可使用能夠用於使連接劑結合到金屬顆粒之活性 部分。理想使用以上類型具有核酸之芳基連接劑或其他類 型連接劑分子。該連接劑可具有具乙基苯部分之中央區 域,在此,η為在1和10, 〇〇〇間之數位。 通常,各後續連接劑對之長度比可在約2至約2 0之範圍 内。或者,後續連接劑對之長度比可在約3至約1〇之範圍 内,而在其他具體實施例中,約為5。 例如,對於包括連接劑1、2及3(分別為LI、L2及L3)之 三級製程,1^1丄2丄3之比例可理想在約1:2:4之範圍内。 或者,該比例可為約1: 5 : 25,在另外其他具體實施例中, 該比例可為約1: 20: 400。在其他具體實施例中,l 1和L2之 -24- 本紙張尺度適用中國國家標準(CNS) Α4規格(21〇 X 297公釐)Particle pairs ". For example, Figures 2a to 2c illustrate a method for making the fractal structure of the present invention. In Figure 2a, the 'metal particles 10 are produced by the aforementioned method. The short linker 20 has a chemistry that is also sufficient to bind to the metal particles 10 Active end. For example, the linker has a sulfhydryl group (〃SH〃) at each end of the linker 20. When compounded, the metal particles 10 are combined with the SH end of the linker 20 to form a particle pair 30. Figure 2b The steps that can be used to generate particle-to-cluster. The particle pair 30 reacts with a medium-length linker 40 to form clusters 50. Figure 2c illustrates the steps that can be used to generate nanoscale fractal structures of the present invention. Clusters 50 Reacts with long linker 60 to form nano-scale fractal structures 70 ° Linker molecules can be selected to provide the desired length. Polymers with organic moieties are commonly used. For example, 'Arylic di-thiol or di-iso Nitrile molecules are linked. Alternatively, active moieties that can be used to bind the linker to the metal particles may be used. Ideally, the above types of aryl linkers with nucleic acids or other types of linker molecules are used. The linker may have Central region, where η is a number between 1 and 10,000. Generally, the length ratio of each subsequent linker pair may be in the range of about 2 to about 20. Alternatively, the length of the subsequent linker pair The ratio may be in the range of about 3 to about 10, and in other specific embodiments, about 5. For example, for a three-level process including linking agents 1, 2 and 3 (LI, L2 and L3, respectively), The ratio of 1 ^ 1 丄 2 丄 3 may desirably be in the range of about 1: 2: 4. Alternatively, the ratio may be about 1: 5: 25, and in other specific embodiments, the ratio may be about 1: 20: 400. In other specific embodiments, l 1 and L2 of -24- This paper size applies the Chinese National Standard (CNS) A4 specification (21〇X 297 mm)
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530146 A7530146 A7
間以及L2至L3之比例不必相同。因 中…咖比可為約二二 4 為 1:20:40。 :等條件下,可製造具有所需孔隙度之結構。通常, 範ί ' 結構…、應具有在約20奈米至約10,_夺米 ^平均大小。在選擇性具體實施例中,其大在 1大Λ約_奈米範^,在其他具體實施例中,在约 :未土約200奈米範圍内’在另外其他具體實施例中, 為約150奈米。 Τ 士本發明的某些應用’可理想使用具有多種不同 不未顆粒。因&,可在相同反應中用具有自約2q奈米至約 no⑽奈米直徑之顆粒開始製造材料顆粒結構。此外 改變顆粒形狀’以取得傳熱改良。例如,具有約1〇〇1至 長度對直徑之比之棒形顆粒,或者,自約5〇:1至= 5 ’ 1 ’在其他具體實施例中’約為20: 1至約1 〇: 1。 %除光譜應用外(SERS、表面電漿激元共振譜、熒光光 邊、表面增強紅外吸收光譜及其它光譜技術),可將自金 屬顆粒製備的類碎形結構用作寬波長濾光材料或天線。 另外’可將此等系統用於寬範圍熱交換方法及裝置。例 如’可用在類碎形結構中排列的金屬顆粒製備多種材料, $等材料將具有優良吸熱-發射性能。可將此等薄膜與熱 &用於除熱’且可與多種材料一起結合用於建築結構、引 擎冷卻系統、微晶片冷卻及空間技術。此外,可作為服裝 材料用於軍事目的,以模糊紅外探測(夜視)。 Β·製造巢化顆粒缔合體 -25- :297公釐)The ratio between L2 and L3 need not be the same. Because in ... the coffee ratio is about 22: 4 to 1:20:40. : Under other conditions, a structure with the required porosity can be manufactured. In general, the fan's structure ... should have an average size in the range of about 20 nanometers to about 10. In selective embodiments, it is greater than 1 Λ about _ nanometer range ^, in other specific embodiments, in the range of about: 200 nanometers' in other specific embodiments, is about 150 nm. Certain applications of the present invention ' may be ideally used with many different particles. Because of & the particle structure of the material can be made in the same reaction with particles having a diameter from about 2q nanometers to about no nanometers. In addition, the shape of the particles was changed 'to obtain improved heat transfer. For example, rod-shaped particles having a ratio of length from about 001 to length to diameter, or, from about 50: 1 to = 5 ′ 1 ′, in other embodiments, about 20: 1 to about 1 〇: 1. In addition to spectral applications (SERS, surface plasmon resonance spectroscopy, fluorescent light edges, surface-enhanced infrared absorption spectroscopy, and other spectroscopic techniques), fragment-like structures made from metal particles can be used as wide-wavelength filter materials antenna. In addition, these systems can be used in a wide range of heat exchange methods and devices. For example, a variety of materials can be prepared from metal particles arranged in a fractal-like structure. Materials such as $ will have excellent endothermic-emission properties. These films can be used with heat & for heat removal ' and can be combined with a variety of materials for building structures, engine cooling systems, microchip cooling, and space technology. In addition, it can be used as a clothing material for military purposes to blur infrared detection (night vision). Β. Manufacture of nested particle associations -25-: 297 mm)
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五、發明説明(22 可藉由選擇各自A 1 n太+ 大小金屬々:T、米、40奈米及240奈米直徑均句 …屬至果、粒〈膠體溶 , dna^1! ^f4 ° 複數個分別具有連接劑(如,幻。顆粒結合。製造 -米顆粒之混二=經I?衍生的一 接㈣互結合,以形成第-級巢化上冓互作用。DNA連 罘一級果化顆粒結構包括包 大的較大顆粒之#數個卜級兩個顆粒任一個 m , 久數個罘一級顆粒結構(如,240太夫h f 弟一級顆粒或第二級顆粒之混合物加 0'丁、未)知 溫度及然後將該混合物冷卻能狗產生更佳二?10。。。之 C製i告JL古此、 Λ生王文佳級果化顆粒。 、具有非-播規顆粒結構之表面 為製U本發明之熱管,可將經 亀導熱表面上,想用傳導:===結構 著到表面。在如此塗覆❿ 構附 射輻射由_磁輕射時,-些入 I、粒〜構吸收,並可被傳到熱管 内熱量可沿熱管傳到存在較冷環境的另一位置 ''、、後,管 管内的熱量離開熱管,進入周圍環境。置,由此使熱 ::·明的某些具體實施例中,可使用在縣 他顆粒結構。可首先使此等結構附著了然:::巢 永口为加強顆粒結構附^,以增加材 種 性。 復风材料的耐用 ΙΠ·導熱聚合物 :、裏^穩定聚合物能夠傳熱,如,以聚笨& 女或聚p比P各 530146 A7 B7 五、發明説明(23 ) 為基礎之複合材料(例如,自EEONIX公司)。能夠使金屬顆 粒附著到金屬表面之其他複合材料亦為吾等所熟悉(美國 專利第5,925,467號,其全文係以引用方式併入本文中)。 實例4 包含碎形吸熱劑之熱管 圖3描繪本發明具體實施例300的一部分1 10,其中熱管 1 05與圖1中所示相似,其係部分以一種顆粒結構覆蓋。吸 熱劑部分110包括熱管105,一種具有揮發性流體130之芯 元件135。一部分經揮發流體140顯示與芯135相鄰。在熱 管105周圍為一種導熱聚合物層145,該層具有埋於其中的 金屬顆粒150。在導熱聚合物層145周圍為包括奈米顆粒結 構之區域160。 圖4描繪本發明之具體實施例400,該具體實施例在熱管 之吸熱端110具有顆粒結構。熱管105具有芯元件135,該 芯元件.具有含於其中的揮發性流體130。熱管外部顯示具 有一導熱聚合物層145,該層具有在其上施加的顆粒結構 160區域。熱量(Q\)在熱管之吸熱劑部分110由顆粒結構 160吸收,並由聚合物層145傳到熱管105。熱量將芯區域 135中的揮發性流體130蒸發,產生經蒸發流體140,經蒸 發流體流到熱管之發射端120。在熱管之發射端120,經蒸 發流體140冷凝,釋放熱量。液體流入芯結構1 3 5,且退回 到熱管之吸熱劑部分110。 圖5描繪本發明之具體實施例500,該具體實施例在熱管 之吸熱端11 0及發射端120兩端具有顆粒結構。以上圖4中 -27- 本紙張尺度適用中國國家標準(CNS) A4規格(210 X 297公釐) 530146 A7 B7 五、發明説明(24 ) 所述之相同特徵應用於圖5。此外,一導熱聚合物層1 46在 發射端120包圍熱管105。顆粒結構層161施加於導熱聚合 物層146之外部。導熱聚合物146種類不必與導熱聚合物 145相同,而顆粒結構16 1不必與顆粒結構160相同。自熱 管5 00之吸收端1 10傳送的熱量可被運到發射端120。在發 射端120,經蒸發流體140可冷凝釋放熱量”Q〆,所釋放熱 量能夠通過導熱聚合物層146流到奈米顆粒結構16 1,藉以 輻射出去。 在本發明之其他具體實施例中,可使顆粒結構直接附著 到熱管表面,而不是導熱聚合物中間層。僅作為實例,可 用微影法附著顆粒結構。此等方法描述於200 1年3月23日 申請的美國專利申請案(其標題為”用感受器藉由具有顆粒 結構之基材增大分析物檢測”(Amplification of Analyte Detection by Substrates Having Particle Structures With Receptors),發明者,大衛 I.克瑞邁爾(David I. Kreimer)、 ?11.0.,奥立格八.依文(0168八.丫6〜丨11)?]1.0.,托馬斯11.奴弗 (Thomas H. Nufert),所有此等專利均全文以引用之方式併 入本文中。另外,可用雷射燒蝕直接在熱管上製造顆粒結 構。此等方法描述於以上引用的美國專利申請·案中。 在某些具體實施例中,理想能夠提供具有碎形聚集體之 熱管兩端,且其聚集體具有不同波長吸收/發射特徵。例 如,如果内部產生不理想高熱量,則可能需要提供一·種具 有顆粒結構或碎形聚集體之熱管端,且該顆粒結構或碎形 聚集體在空間内具有於較長波長的高熱量吸收特徵。而在 -28- 本紙張尺度適用中國國家標準(CNS) A4規格(210 X 297公釐)V. Description of the invention (22 By selecting the respective A 1 n too + size metal 々: T, rice, 40 nanometers and 240 nanometers diameter sentences ... belong to fruit, grain <colloid, dna ^ 1! ^ F4 ° Plurality of linkers (eg, magic. Granule binding. Manufacturing-Mixture of rice granules = one-to-one binding via I? Derivation to form a first-level nesting and upper-side interaction. DNA flail level one The structure of the fruiting granules includes a large number of large particles, either one of the two second-order particles, or a number of first-order particle structures (for example, a mixture of 240-degree hf first-level particles or second-level particles plus 0 ' D, Wei) Knowing the temperature and then cooling the mixture can produce better two? 10. The system of the report to JL Guzhen, Λ Sheng Wang Wen Jia grade fruit granules, surface with non-seeding particle structure In order to make the heat pipe of the present invention, the heat transfer surface of the warp can be used to conduct conduction: === structure to the surface. In this way, when the structure-attached radiation is emitted from _ magnetic light,- ~ Structure absorption, and can be transferred to the heat pipe. The heat can be transferred along the heat pipe to another location where a colder environment exists. The heat in the tube leaves the heat pipe and enters the surrounding environment. This allows the heat :: · Ming to be used in some specific embodiments of the granule structure. The structure can be attached first: :: Chao Yong The mouth is reinforced with a granular structure to increase the variety of materials. Durability of air-reinforced materials. I. Thermally conductive polymer: 里 Stable polymer capable of transferring heat, for example, with poly- & female or poly-p ratio 530146 each A7 B7 V. Invention Description (23) -based composite materials (for example, from EEONIX). Other composite materials capable of attaching metal particles to metal surfaces are also familiar to us (US Patent No. 5,925,467, the entire text of which is (Incorporated herein by reference). Example 4 Heat Pipe Containing Fragmented Heat Absorbent Figure 3 depicts a portion 10 of a specific embodiment 300 of the present invention, where the heat pipe 105 is similar to that shown in FIG. Structural coverage. The heat sink portion 110 includes a heat pipe 105, a core element 135 with a volatile fluid 130. A portion of the volatile fluid 140 is shown adjacent to the core 135. Around the heat pipe 105 is a thermally conductive polymer layer 145 This layer has metal particles 150 buried therein. Around the thermally conductive polymer layer 145 is a region 160 including a nanoparticle structure. Figure 4 depicts a specific embodiment 400 of the present invention, which has a heat-absorbing end 110 of a heat pipe with Particle structure. The heat pipe 105 has a core element 135, which has a volatile fluid 130 contained therein. The outside of the heat pipe has a thermally conductive polymer layer 145, which has a region of particle structure 160 applied on it. Heat ( Q) The heat absorber portion 110 in the heat pipe is absorbed by the particle structure 160 and is transferred to the heat pipe 105 by the polymer layer 145. The heat evaporates the volatile fluid 130 in the core region 135 to produce an evaporated fluid 140, which flows to the emitting end 120 of the heat pipe. At the emitting end 120 of the heat pipe, the evaporation fluid 140 is condensed to release heat. The liquid flows into the core structure 1 3 5 and returns to the heat-absorbing agent portion 110 of the heat pipe. FIG. 5 depicts a specific embodiment 500 of the present invention, which has a granular structure at both ends of the heat-absorbing end 110 and the emitting end 120 of the heat pipe. In the above figure -27- this paper size applies to the Chinese National Standard (CNS) A4 specification (210 X 297 mm) 530146 A7 B7 5. The same features described in the description of the invention (24) are applied to Figure 5. In addition, a thermally conductive polymer layer 146 surrounds the heat pipe 105 at the emitting end 120. The particle structure layer 161 is applied outside the thermally conductive polymer layer 146. The type of the thermally conductive polymer 146 need not be the same as that of the thermally conductive polymer 145, and the particle structure 161 need not be the same as the particle structure 160. The heat transferred from the absorption end 1 10 of the self-heating tube 5 00 can be transported to the emission end 120. At the emitting end 120, the evaporative fluid 140 can condense and release heat "Q", and the released heat can flow through the thermally conductive polymer layer 146 to the nano-particle structure 161, thereby radiating it. In other specific embodiments of the present invention, The particle structure can be attached directly to the surface of the heat pipe, rather than the thermally conductive polymer interlayer. By way of example only, the particle structure can be attached by lithography. These methods are described in the US patent application filed on March 23, 2001 (which Titled "Amplification of Analyte Detection by Substrates Having Particle Structures With Receptors", the inventor, David I. Kreimer ,? 11.0., Oleg VIII. Evan (0168 VIII. Ya 6 ~ 丨 11)?] 1.0., Thomas 11. 霍夫 (Thomas H. Nufert), all these patents are incorporated by reference in their entirety Included herein. In addition, laser ablation can be used to fabricate granular structures directly on heat pipes. These methods are described in the U.S. patent applications and applications cited above. In some specific embodiments, ideal energy Provide two ends of a heat pipe with fractal aggregates, and their aggregates have different wavelength absorption / emission characteristics. For example, if undesirably high heat is generated inside, you may need to provide a heat pipe with a granular structure or fractal aggregates End, and the granular structure or fractal aggregates have high heat absorption characteristics at longer wavelengths in the space. And at -28- this paper size applies the Chinese National Standard (CNS) A4 specification (210 X 297 mm)
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另一、,可能需要提供在此 ^ 匕寺紅件下具有通合於耗散輻射 毛射性…員粒結構或碎形聚… IV具有碎形聚集體之窗材料木^ 在本發明的某些且⑱奋、> 该 ^ _ 一 /、κ B她例中,窗材料(例如,包括玻 城、石夬、塑膠及為技蓺 用顆ρ έ士错帝 ^ L…的其他材料)可暫時性 取隹碰 k七、及/或控制輻射吸收性之碎形 ?κ集體。為製造此種窗, 心七# 了知含上述顆粒結構之溶液由噴 射或其他液體分配方法施加 、^、、 加到表面。理想提供具有接著劑 〇谷液’以促進顆粒結構對矣 口傅司·衣面又接著。如本文所述,可 用大量接著劑附著顆粒結構。 ^ 他/、拉5她例中,可用化學連接劑使顆粒結構化學 附者到窗材料之表面,如,使用石夕燒,包括叫。可由預 淨化製備細’然後施加化學連接劑(如,侧,隨後 可將顆粒結構加到經預處理之表面。 ^其中需要可見光波長透射但不需要紅外波長透射之具 體貫施例I含顆粒結構之層應相對較薄。在此項技藝之 靶圍内’應依溶液之組分決定多厚層才能提供所需光透 射。 實例5 用擰檬酸鹽製備碎形銀聚集體 知45¾克AgN〇3(西格馬公司(sigma))溶於25〇毫升三重蒸 餾、去離子水,在磁性攪拌器攪拌下使溶液滞騰。將1%檸 檬酸納溶液(5毫升)在劇烈攪拌下逐滴加入滞騰溶液。將此 溶液保持沸騰60分鐘,同時用自來水冷卻的冷凝器防止水 -29- 本紙張尺度適用中國國家標準(CNS) A4規格(210X297公釐)In addition, it may be necessary to provide under this dagger temple red piece with a property that is compatible with dissipative radiation ... a granular structure or a fragmentary aggregate ... IV a window material with fragmentary aggregates ^ In some cases, > The ^ _ a /, κ B In her example, the window material (for example, including Boseong, Shi Jie, plastic, and other materials used for technical purposes ^ L ^…). It is possible to temporarily take the bump k 七, and / or control the fragmentation of the radiation absorption? Κ collective. In order to make such a window, Xinqi # knows that the solution containing the above-mentioned particle structure is applied to the surface by spraying or other liquid distribution methods. It is desirable to provide a gluten solution with an adhesive agent 〇 to promote the particle structure to the mouthpieces and clothes. As described herein, a large number of adhesives can be used to attach the particulate structure. ^ In his case, he / she can use a chemical linking agent to make the particle structure chemically attached to the surface of the window material, for example, using Shi Xiyao, including calling. Fine particles can be prepared by pre-purification, and then a chemical linker (eg, side) can be applied, and then the particle structure can be added to the pre-treated surface. ^ Specific Embodiment 1 in which visible wavelength transmission is required but infrared wavelength transmission is not required The layer should be relatively thin. Within the target range of this technique, the thickness of the solution should be determined according to the composition of the solution to provide the required light transmission. Example 5 Preparation of broken silver aggregates using citrate. 45¾ g of AgN 〇3 (sigma) was dissolved in 250 ml of triple distillation, deionized water, and the solution was stagnate with stirring by a magnetic stirrer. The 1% sodium citrate solution (5 ml) was vigorously stirred one by one. Add the stagnation solution dropwise. Keep the solution boiled for 60 minutes while using a water-cooled condenser to prevent water -29- This paper size applies to China National Standard (CNS) A4 (210X297 mm)
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線 530146 五、發明説明 由蒸發損失。將所得銀膠體溶液在暗色玻璃瓶中於m 保持最多至少數月時間。 氣k銀顆粒之碎形聚集體時,將2 5 〇微升銀膠體溶液與 1750微升NaC丨(西格馬公司’超純)之水溶液混合,使Mi 最終濃度達到6〇毫莫耳/升。聚集體在數分鐘内生成,溶 ㈣至少達約半小時相#穩定。將碎形聚集體施加到經金 屬塗覆之基材’該碎形聚集體沈積並接著到金屬表面,形 成經碎形聚集體衍生的金屬表面。 實例6 用NaBH4製備碎形銀聚集體 將5毫莫耳/升AgN〇3(西格馬公司)溶於三重蒸餾、去離 子水之溶液(5(3毫升)在磁性攪拌器劇烈攪拌下攪掉下逐滴 加入150耄升冰冷卻、2毫莫耳/升之NaBH4(西格馬公司)溶 液。恰在其後加入1%聚乙烯醇之溶液(25毫升)。然後使該 :合物沸騰60分鐘,同時用自來水冷卻的冷凝器防止水由 洛發扣失。將銀膠體溶液在暗色玻璃瓶中於5。保持最 多至少數星期時間。 製造銀顆粒之碎形聚集體時,將25〇微升銀膠體溶液與 1750微升NaCl(西格馬公司,超純)之水溶液混合,使^ci 最終濃度達到約100毫莫耳/升。聚集體在數分鐘内生成, 溶液經至少達約半小時相當穩定。將碎形聚集體施加到經 金屬塗覆之基材,該碎形聚集體沈積並接著到金屬表面, 形成經碎形聚集體衍生的金屬表面。 實例7 -30- 本紙張尺度適用中國國家標準(CNS) A4規格(210X297公爱)Line 530146 V. Description of the invention Loss by evaporation. The resulting silver colloidal solution was kept at m for at least several months in a dark glass bottle. When gas-k silver particles are broken into aggregates, 250 microliters of silver colloidal solution is mixed with 1750 microliters of NaC 丨 (Sigma's ultrapure) aqueous solution to make the final Mi concentration reach 60 millimoles / Rise. Aggregates are formed within minutes and the phase is stable for at least about half an hour. Fractal aggregates are applied to a metal-coated substrate ' The fractal aggregates are deposited and then onto a metal surface to form a metal surface derived from the fractal aggregates. Example 6 Preparation of broken silver aggregates using NaBH4 A solution of 5 mmol / L AgNO (3 Sigma) in a triple-distilled, deionized water solution (5 (3 ml)) was stirred under vigorous stirring in a magnetic stirrer Drop dropwise and add 150 liters of ice-cooled, 2 mmol / L NaBH4 (Sigma) solution. Just after that, add 1% polyvinyl alcohol solution (25 ml). Then make the: Boil for 60 minutes, while using a water-cooled condenser to prevent water from being lost by Luofa. Place the silver colloidal solution in a dark glass bottle at 5. Keep it for at least a few weeks. When making the broken aggregates of silver particles, 25 〇µl of silver colloid solution was mixed with 1750µl of NaCl (Sigma Company, ultra-pure) aqueous solution, so that the final concentration of ^ ci reached about 100 millimolars / liter. Aggregates were formed within minutes, and the solution was at least Quite stable for about half an hour. Fractal aggregates are applied to a metal-coated substrate, and the fractal aggregates are deposited and then onto the metal surface to form a metal surface derived from the fractal aggregates. Example 7 -30- present Paper size applies to China National Standard (CNS) A4 (210X (297 public love)
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k 530146 A7k 530146 A7
川坪稼鉍鹽製備碎形金聚集髀 =。毫克财丨4(西格馬公司)溶於25〇毫;三重蒸餘、 去離子水’在磁性攪拌器檀拌下使溶液㈣。將1%棒權酸 夜(5愛升)在劇烈攪拌下逐滴加入滞騰溶液。將此溶液 ^弗騰1時用自來水冷卻的冷凝器防止水由蒸 Λ曰、失和所得金如體落液在暗色玻璃瓶中於約5〇 -8。(:保 持最多至少約數星期時間。 製造金顆粒之碎形聚集體時,將2職升金膠 1 曰750微升助(西格馬公司,超純)之水溶液混合,使Nac、丨 :終痕度達到約100毫莫耳/升。聚集體在數分鐘内生成, ’合液’.工土少達約半小時穩定。將碎形聚集體施加到噔金屬 塗覆之基材’該碎形聚集體沈積並接著I彳金屬表面,形成 經碎形聚集體衍生的金屬表面。 實例8 具有碎形吸收劑之窗 例如,圖6a描繪本發明一具體實施例6〇〇之透視圖,其 中玻璃片604具有上表面6〇8。表面6〇8上提供有具接著劑 6^6及碎形聚集體62〇之層612。圖讣描繪圖以所:具體實 施例600之橫截面圖,該具體實施例具有具上表面6〇8之玻 璃片604。表面608上提供有具接著劑616及碎形聚集體62〇 之層612。 /江- 、圖7描繪測定其上具有銀碎形聚集體之玻璃之光吸收率 ,試驗結果。在市面上購得一預淨化玻璃載片,並用異丙 "Τ ^ 步淨化。知另一塊如此處理的載片於室溫(約22°C ) -31- 530146 A7Preparation of crushed gold aggregates from Chuanping Jia bismuth salt Milligram 4 (Sigma Company) was dissolved in 250 millimeters; triple distilled residual, deionized water 'was stirred in a magnetic stirrer to make the solution ㈣. 1% clavulanic acid (5 liters) was added dropwise to the stagnation solution with vigorous stirring. This solution was used to cool the condenser with tap water at 1 o'clock to prevent water from being distilled, and the resulting gold, such as body fluid, was collected in a dark glass bottle at about 50-8. (: Keep it for at least about several weeks. When producing the fractal aggregates of gold particles, mix 2 liters of gold glue 1 ~ 750 microliters (Sigma company, ultra-pure) aqueous solution, so that Nac, 丨: final The trace reaches about 100 millimolars / liter. Aggregates are formed within a few minutes, and 'liquid'. The soil is stable for as little as about half an hour. Fragmented aggregates are applied to a rhenium-coated substrate Deformed aggregates are deposited and then adhered to the metal surface to form metal surfaces derived from fractal aggregates. Example 8 Window with fractal absorbent For example, Figure 6a depicts a perspective view of a specific embodiment of the present invention 600, where The glass sheet 604 has an upper surface 608. A surface 608 is provided with a layer 612 having an adhesive 6 ^ 6 and a fractal aggregate 62. FIG. 讣 depicts a schematic view: a cross-sectional view of a specific embodiment 600, This embodiment has a glass sheet 604 with an upper surface 608. A surface 608 is provided with a layer 612 with an adhesive 616 and a fractal aggregate 62. / Jiang-, Figure 7 depicts the determination of silver flakes on it Light absorption of glass of aggregates, test results. A pre-purified glass was purchased on the market Slide and purify it with isopropyl " T ^ step. It is known that another slide processed in this way is at room temperature (about 22 ° C) -31- 530146 A7
暴露於一種於異丙醇中含飽和二、 其表面用-紙拭輕擦。所釋二 -π洗除去。將另一塊用矽烷處理的 、 例5製備的含碎形銀顆粒之膠體溶液。在:::二上實 鐘後,用過量異丙醇清洗,然後用過量分 ,除去。在分光光度計中於約25。奈米== 長 < 範圍檢測光吸收率。 π未波 在圖7中,入射光波長(用奈米表示)呈現在橫轴上,而r 處理及未處理玻璃之吸收率(用光密度表示)呈現在縱: 上。未經處理玻璃(底部曲線)在所檢測的所有波長具 低光密度。對於高於約250奈米之大多數波長,光密, 近不變’而自250奈米至約850奈米稍微降低。具有矽:: 層〈玻璃比未處理玻璃顯示稍大光密度,但未處理及絲矽 烷處理之玻璃間的光密度差異輕微。儘管如此,同時2有 石夕坑及銀碎形|集體《玻璃纟大部分所檢測波長顯示 吸收率。 透射率增加(吸收率降低)之範圍在約28〇奈米至約35〇奈 米之波長範圍觀察到。在此範圍内,該透射率接近未處2 玻璃或經矽烷處理玻璃。 圖8a-8b描繪本發明另外其他具體實施例,其中顆粒結 構係包埋於窗材料内。圖8a描繪一個其中第一片窗材料 804具有層808之”夾層’’具體實施例800,該層808在其中具 有顆粒結構812。第二片窗材料816係於層808上提供,夢 以完成夾層結構。·可以瞭解到,為改良輻射吸收性能, -32-Expose a surface containing saturated diisopropyl alcohol, and wipe the surface with a paper wipe. The released two -π was removed by washing. Another piece of colloidal solution containing crushed silver particles prepared in Example 5 treated with silane was prepared. After 2 :: 2 hours, wash with excess isopropanol, and then remove with excess. About 25 in a spectrophotometer. Nanometer == Long < Range detection light absorption. π unwave In Fig. 7, the wavelength of incident light (expressed in nanometers) is presented on the horizontal axis, and the absorptivity (expressed as optical density) of r-treated and untreated glass is presented on the vertical axis:. Untreated glass (bottom curve) has low optical density at all wavelengths detected. For most wavelengths above about 250 nanometers, the light density is nearly constant and decreases slightly from 250 nanometers to about 850 nanometers. With silicon :: The layer <glass shows slightly higher optical density than untreated glass, but the difference in optical density between untreated and silk silane treated glass is slight. Nonetheless, at the same time there are 2 Shi Xikeng and silver fractals | collectively, most of the detected wavelengths of glass goblets show absorbance. The increase in transmittance (decrease in absorbance) was observed in the wavelength range of about 28 nm to about 35 nm. In this range, the transmittance is close to that of glass or silane-treated glass. Figures 8a-8b depict still other specific embodiments of the invention, in which the particulate structure is embedded in a window material. Fig. 8a depicts a "sandwich" embodiment 800 in which a first sheet of window material 804 has a layer 808, which has a granular structure 812 therein. A second sheet of window material 816 is provided on layer 808 and the dream is completed Sandwich structure. · It can be understood that -32-
裝- 訂Pack-order
kk
530146 A7 B7 五、發明説明(29 ) 804及8 12不必為相同厚度或甚至相同; 时料。 圖8 b描 繪一選擇性具 體實施例802, 其中單片窗材料820 具有遍 及 整片材料分佈的顆粒結構 824。可很容易 瞭 解 到,此 等 ”經分佈”具體 實施例可包括 多種厚度,且在 其 他 具體實 施 例中,可使多 層π經分佈"具 體實施例組合, 以 提 供具有 所 需輻射吸收性 能之多層結構 〇 亦可 瞭 解,以上具體 實施例變化係 在本發明之範圍 内 〇 {列:¾ 口 , 可 提供顆粒結構 之混合物,且 該混合物各組分 具 有 不同吸 收 性能。使用此 等混合物能夠 提供較寬範圍輻射 吸 收性。 在某 些 具體實施例中 ,可用可溶基 質(如,膠水)使 顆 粒 結構接 考 到透明材料表面。如果基質溶於一般溶劑 1 如 水、醇 或氨清洗溶液, 則可在顆粒結 構之吸收性能不 再 需 要時除 去 顆粒結構。此 種可溶接著劑 的一個實例為澱 粉 〇 或者, 可 使用不易溶解 的基質使顆粒 結構更持久接著 到 表 面。在 另 外具體實施例 中,可用一種 或多種上述不溶 性 聚 合物使 顆 粒結構接著到 表面。 此外 1 在某些具體實 施例中,顆粒 結構可以具有能 夠 施 加於窗 材料片表面之枯 帖襯材之帶形 式在基質中提供 〇 此 等具體 實 施例在本文中 被稱為π窗覆蓋材料"。此等窗 覆 蓋 材料可 以 大批提供,例如,以具有或 不具有釋放襯墊之卷 形式提供 。在本文中, ”釋放襯墊”指 較弱接著到帶之接 著 劑之材料 片。因此,具 有顆粒結構之 帶能夠免受接著 劑 接 著到含 顆 粒基質之不適 當側面之不良後果影響。此等 釋 放 -33- 本紙張尺度適用中國國家標準(CNS) A4規格(210 x 297公釐)530146 A7 B7 V. Description of the invention (29) 804 and 8 12 need not be the same thickness or even the same; Fig. 8b depicts a selective embodiment 802 in which a single sheet of window material 820 has a granular structure 824 distributed throughout the entire sheet of material. It can be easily understood that these "distributed" specific embodiments may include various thicknesses, and in other specific embodiments, multiple layers of π distributed " specific embodiments may be combined to provide a desired radiation absorption performance. It can also be understood that the multilayer structure is within the scope of the present invention, and the variations of the above specific embodiments are within the scope of the present invention. {Column: ¾ mouth, a mixture of particle structures can be provided, and each component of the mixture has different absorption properties. The use of these mixtures can provide a wide range of radiation absorptivity. In some embodiments, a soluble substrate (eg, glue) can be used to make the particle structure accessible to the surface of the transparent material. If the matrix is dissolved in a general solvent 1 such as water, alcohol or ammonia cleaning solution, the granular structure can be removed when the absorption properties of the granular structure are no longer needed. An example of such a soluble adhesive is starch. Alternatively, a less soluble matrix can be used to make the particle structure more persistent to the surface. In another embodiment, one or more of the above insoluble polymers can be used to adhere the particle structure to the surface. In addition, in certain embodiments, the granular structure may be provided in the matrix in the form of a strip of dead lining material that can be applied to the surface of the sheet of window material. These specific embodiments are referred to herein as π window covering materials ". These window covering materials may be provided in large quantities, for example, as rolls with or without release liners. In this context, "release liner" refers to a sheet of material that is weaker and adheres to the adhesive. Therefore, a tape with a granular structure can be protected from the undesired side effects of the adhesive adhering to the inappropriate side of the granular matrix. These releases -33- This paper size applies to China National Standard (CNS) A4 (210 x 297 mm)
裝· 訂Packing
530146530146
襯墊為技藝上所熟悉。 圖9a描繪本發明一個具體實施例9〇〇,其中聚合物材料 片904具有顆粒結構9〇8及接著性襯材912層。釋放襯墊916 施加於接著性襯材912上。 在另外其他具體實施例中,本發明之窗材料包括顆粒結 構及其它吸收性材料’如染料。此等染料包括為製窗技藝 上所熟悉的染色材料,且可對窗材料給予顏色及/或極化 性能。圖9b描繪一選擇性具體實施例9〇2,該具體實施例 與實例9a相似,且具有具極化性能之額外層92〇。 所述及所描繪的具體實施例僅用於說明,不應用以限制 本發明之範圍。具有顆粒結構表面的大量變化在熟諳此蔽 者之觀察範圍内,且所有此等變化應包含在本發明之範= 内。 V ·在分析儀器中使用顆粒結構 在本發明的某些具體實施例中,可用顆粒結構製造窗材 料,以改良分析儀器所用樣品容器之性能。舉例說明1在 喇曼光譜學中,可使具有興趣分析物之基材暴露於入射電 磁輻射,則喇曼散射能夠產生喇曼光譜特徵。在装此情2 下,喇曼光譜特徵波長可由 電磁輻射掩蔽。該”寄生光” 弱喇曼光譜特徵之分析物。 自分析物以外的其他源出現的 可能為一個問題,尤其是具有 受寄生光危害的其他類型光學 檢測系統包括相光學元件、熒光光學元件及其仑 G崎型使用 電磁孝备射之檢測/分析系統。 為克服寄生光問題,可製造結合本文所述顆起 、、、。構之本 -34- 本紙張尺度適用中國國家標準(CNS) A4規格(210 X 297公釐) 530146 A7 B7 五 、發明説明( 發明裝置。藉由選擇性濾除寄生光,可改良信號識別。 工業應用The pads are technically familiar. Fig. 9a depicts a specific embodiment 900 of the present invention, in which a sheet of polymer material 904 has a granular structure 908 and a layer of adhesive 912. A release liner 916 is applied to the adhesive liner 912. In still other embodiments, the window material of the present invention includes a particulate structure and other absorbent materials ' such as dyes. These dyes include dyeing materials that are familiar in the art of window making and can impart color and / or polarization properties to the window material. Figure 9b depicts a selective embodiment 902, which is similar to Example 9a and has an additional layer 92o with polarization properties. The specific embodiments described and depicted are for illustration purposes only and should not be used to limit the scope of the invention. A large number of changes in the surface with a granular structure are within the observation range of those familiar with this mask, and all such changes should be included in the scope of the present invention. V. Use of Particle Structures in Analytical Instruments In certain embodiments of the present invention, window materials can be made with granular structures to improve the performance of sample containers used in analytical instruments. Example 1 In Raman spectroscopy, a substrate with an analyte of interest can be exposed to incident electromagnetic radiation, and Raman scattering can produce Raman spectral characteristics. In this case, the characteristic wavelength of the Raman spectrum can be masked by electromagnetic radiation. This "parasitic light" is an analyte with weak Raman spectral characteristics. It may be a problem for sources other than analytes, especially other types of optical detection systems that are endangered by parasitic light, including phase optical elements, fluorescent optical elements, and their G-type detection / analysis using electromagnetic beam preparation. system. In order to overcome the problem of parasitic light, particles can be manufactured in combination with those described herein.建 本本 -34- This paper size is in accordance with Chinese National Standard (CNS) A4 (210 X 297 mm) 530146 A7 B7 5. Description of the invention (Invention device. By selectively filtering the parasitic light, the signal recognition can be improved. Industrial applications
本發明之顆粒結構用於製造熱管及窗所用之改良吸收性 及發射性之材料。選擇通過窗材料吸收及/或透射的波長 可以對窗兩侧應用的環境條件為基礎。改良熱吸收能夠將 結構内部保持在所需溫度範圍内。具有吸熱及透射性表面 之熱管可對各種設備及空間(包括結構)保持適合操作條 件。本發明之顆粒結構應用能夠改良熱管之效率。 裝 訂 線 -35-本紙張尺度適用中國國家標準(CNS) A4規格(210 X 297公釐)The granular structure of the present invention is used to manufacture materials having improved absorptivity and emissivity for use in manufacturing heat pipes and windows. The choice of wavelengths that are absorbed and / or transmitted through the window material can be based on the environmental conditions applied on both sides of the window. Improved heat absorption keeps the interior of the structure within the required temperature range. Heat pipes with endothermic and transmissive surfaces can maintain suitable operating conditions for a variety of equipment and spaces, including structures. The particle structure application of the present invention can improve the efficiency of the heat pipe. Binding Line -35- This paper size applies to China National Standard (CNS) A4 (210 X 297 mm)
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US09/815,828 US20010054495A1 (en) | 1999-09-27 | 2001-03-23 | Surfaces having particle structures with broad range radiation absorptivity |
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CN100413061C (en) * | 2004-06-07 | 2008-08-20 | 鸿富锦精密工业(深圳)有限公司 | Thermal tube and producing method thereof |
US20060180296A1 (en) * | 2005-02-17 | 2006-08-17 | Yuh-Cheng Chemical Ltd. | Heat pipe |
FR2934709B1 (en) * | 2008-08-01 | 2010-09-10 | Commissariat Energie Atomique | THERMAL EXCHANGE STRUCTURE AND COOLING DEVICE HAVING SUCH A STRUCTURE. |
US9163883B2 (en) | 2009-03-06 | 2015-10-20 | Kevlin Thermal Technologies, Inc. | Flexible thermal ground plane and manufacturing the same |
US10041745B2 (en) | 2010-05-04 | 2018-08-07 | Fractal Heatsink Technologies LLC | Fractal heat transfer device |
CN102748737B (en) * | 2012-06-28 | 2014-06-04 | 东莞市科磊得数码光电科技有限公司 | LED (light-emitting diode) lamp and radiating pipe thereof |
US9982292B2 (en) * | 2012-09-28 | 2018-05-29 | Src, Inc. | Detecting chemical and biological agents using textile-based sensors |
JP6695803B2 (en) * | 2014-01-10 | 2020-05-20 | ブライ・エアー・アジア・ピーヴイティー・リミテッド | Hybrid adsorption device Heat exchange device manufacturing method |
US20150219406A1 (en) * | 2014-01-31 | 2015-08-06 | Asia Vital Components Co., Ltd. | Heat Dissipation Device |
US11598594B2 (en) | 2014-09-17 | 2023-03-07 | The Regents Of The University Of Colorado | Micropillar-enabled thermal ground plane |
WO2016044638A1 (en) * | 2014-09-17 | 2016-03-24 | The Regents Of The University Of Colorado, A Body Corporate | Micropillar-enabled thermal ground plane |
US11988453B2 (en) | 2014-09-17 | 2024-05-21 | Kelvin Thermal Technologies, Inc. | Thermal management planes |
US12104856B2 (en) | 2016-10-19 | 2024-10-01 | Kelvin Thermal Technologies, Inc. | Method and device for optimization of vapor transport in a thermal ground plane using void space in mobile systems |
US11208568B2 (en) * | 2017-05-17 | 2021-12-28 | Elwha Llc | Thermal signature control structures |
EP3655718A4 (en) | 2017-07-17 | 2021-03-17 | Alexander Poltorak | Multi-fractal heat sink system and method |
US20210333008A1 (en) * | 2020-04-23 | 2021-10-28 | Carrier Corporation | Advanced electric heating |
US11930621B2 (en) | 2020-06-19 | 2024-03-12 | Kelvin Thermal Technologies, Inc. | Folding thermal ground plane |
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SU905601A1 (en) * | 1980-05-30 | 1982-02-15 | Предприятие Южтехэнерго Производственного Объединения По Наладке,Совершенствованию Технологии И Эксплуатации Электростанций И Сетей "Союзтехэнерго" | Heat pipe |
US4893908A (en) * | 1988-06-27 | 1990-01-16 | Allied-Signal Inc. | Adjustable tint window with electrochromic conductive polymer |
US5099621A (en) * | 1989-05-04 | 1992-03-31 | Allied-Signal, Inc. | Thermal window glazing with conductive polymer coating to block radiative heating |
US5670742A (en) * | 1994-02-04 | 1997-09-23 | Threshold Technologies, Inc. | EMI protected aircraft |
DE4408712C2 (en) * | 1994-03-15 | 1998-01-15 | Dornier Gmbh | Double pane made of glass or plastic with controllable reflectance |
US5808784A (en) * | 1994-09-06 | 1998-09-15 | Dai Nippon Printing Co., Ltd. | Lens array sheet surface light source, and transmission type display device |
DE4433051C2 (en) * | 1994-09-16 | 1996-07-11 | Sekurit Saint Gobain Deutsch | Window pane made of silicate glass which is permeable to electromagnetic radiation |
DE4440572C2 (en) * | 1994-11-14 | 1997-05-07 | Fraunhofer Ges Forschung | Glazing element with variable transmission |
WO1998010289A1 (en) * | 1996-09-04 | 1998-03-12 | The Penn State Research Foundation | Self-assembled metal colloid monolayers |
US6429961B1 (en) * | 2000-10-03 | 2002-08-06 | Research Frontiers Incorporated | Methods for retrofitting windows with switchable and non-switchable window enhancements |
US6379589B1 (en) * | 2000-10-23 | 2002-04-30 | Fractal Systems Inc. | Super-wide band shielding materials |
US6552690B2 (en) * | 2001-08-14 | 2003-04-22 | Guardian Industries Corp. | Vehicle windshield with fractal antenna(s) |
US6727863B2 (en) * | 2001-10-26 | 2004-04-27 | The Hong Kong University Of Science And Technology | Planar band gap materials |
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- 2001-03-23 US US09/815,828 patent/US20010054495A1/en not_active Abandoned
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2002
- 2002-03-22 WO PCT/US2002/008858 patent/WO2002077558A2/en not_active Application Discontinuation
- 2002-03-22 AU AU2002255883A patent/AU2002255883A1/en not_active Abandoned
- 2002-03-22 TW TW091105672A patent/TW530146B/en active
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