TWI711348B - 具有低介電性質之玻璃基板組件、電子組件及製造玻璃基板組件的方法 - Google Patents
具有低介電性質之玻璃基板組件、電子組件及製造玻璃基板組件的方法 Download PDFInfo
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- TWI711348B TWI711348B TW105126522A TW105126522A TWI711348B TW I711348 B TWI711348 B TW I711348B TW 105126522 A TW105126522 A TW 105126522A TW 105126522 A TW105126522 A TW 105126522A TW I711348 B TWI711348 B TW I711348B
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Abstract
本發明揭示了具有低介電屬性的玻璃基板組件、包含玻璃基板組件的電子組件及製造玻璃基板組件的方法。在一實施例中,基板組件包括具有第一表面和第二表面且厚度小於約300μm的的玻璃層。該基板組件進一步包括設置於該玻璃層的該第一表面和第二表面中至少一個上的介電層。該介電層回應於具有10GHz頻率的電磁輻射而具有小於約3.0的介電常數值。在一些實施例中,該玻璃層由退火玻璃製成,從而該玻璃層回應於具有10GHz頻率的電磁輻射而具有小於約5.0的介電常數值和小於約0.003的散逸因數值。
Description
本申請要求於2015年8月21日遞交的美國臨時專利第62/208,282號,於2015年9月24日遞交的第62/232,076號的優先權,以其內容為依據並且透過引用以整體納入本文。
本說明書大致上涉及用於電子設備應用的基板,且更具體地涉及回應於高頻電子信號而具有低介電屬性的玻璃基板組件。
隨著電子技術的進步,無線通信、微型通信和高速數據傳輸應用領域需要更高頻的裝置。然而,由於高速應用(例如,10GHz或更高)中的柔性印刷電路板(FPC)或印刷電路板(PCB)的介電屬性,存在關於電損耗的顧慮。目前的FPC基板,例如聚合物、聚合物/玻璃纖維複合物,難以勝任未來的高頻裝置應用。因此,需要低介電常數(例如,低於約3.0)和低散逸因數值(例如,低於約0.003)的基板。儘管一些薄玻璃基板可滿足
所需散逸因數目標,但在一些高頻應用中這種玻璃基板的介電常數過高。
因此,存在對回應於高頻電信號而具有低介電常數和散逸因數屬性的基板的需求。
在一實施例中,基板組件包括具有第一表面和第二表面的玻璃層。該基板組件進一步包括設置於該玻璃層的該第一表面和第二表面中至少一個上的介電層。該介電層回應於具有10GHz頻率的電磁輻射而具有小於約3.0的介電常數值。
在另一實施例中,電子組件包括玻璃層,該玻璃層包括第一表面和第二表面,設置於該玻璃層的該第一表面或該第二表面中的至少一個上的介電層,複數個設置於該介電層內、該介電層的下方或該介電層的表面上的導電跡線,和設置於該介電層的該表面上且電耦合至該複數個導電跡線的一個或多個導電跡線的積體電路元件。該介電層回應於具有10GHz頻率的電磁輻射而具有小於約3.0的介電常數值,且該積體電路元件組態用以進行無線通信信號的傳送或接收中的至少一個。
在另一實施例中,製造玻璃基板組件的方法包括將玻璃基板加熱至高於該玻璃基板的應變點且低於該玻璃基板的軟化點的第一溫度,且將該玻璃基板保持在該第一溫度的約10%的變化內長達第一時間段。該方法進一步包括將該玻璃基板冷卻至第二溫度超過第二時間
段,從而在冷卻該玻璃基板之後,該玻璃基板回應於具有10GHz頻率的電磁輻射而具有小於約5.0的介電常數值。將介電層施加於該玻璃基板的至少一個表面上,其中,該介電層回應於具有10GHz頻率的電磁輻射而具有小於約2.5的介電常數值。
100:玻璃基板組件
101:初始線軸
103:第二線軸
110:玻璃層
110A:交替玻璃層
110B:交替玻璃層
110C:交替玻璃層
111:玻璃網
112:第一表面
113:第二表面
120:介電層
120A:介電層
120B:介電層
120C:介電層
120D:介電層
120E:介電層
121:介電材料
122:表面
124:表面
125:通道
130:介電層沉積系統
130A:狹縫式模具塗覆系統
130B:層壓系統
134A:滾輪
134B:滾輪
140A:第一導電層
140B:第二導電層
140C:第三導電層
142:導電層
145:導電跡線
146A:第一孔
146B:第二孔
150:卷裝製程
160:堆層
160':堆層
170:爐
200:玻璃基板組件
300:基板組件
301:電子組件
310:玻璃層
320:介電層
322:表面
342:導電跡線
360:積體電路元件
362A:電子元件
362B:電子元件
362C:電子元件
前述將自以下該例示性實施例的更具體的說明變得更加清楚,如附圖中所示,相同的參考符號自始至終表示相同的元件。附圖並不必按比例繪製,重點應放在說明代表性的實施例上。
圖1示意性圖示根據本文描述並圖示的一個或多個實施例的包含耦合至玻璃層的表面的介電層的部分例示性玻璃基板組件;圖2示意性圖示根據本文描述並圖示的一個或多個實施例的施加於圖1中所示的該玻璃層的該表面的該介電層;圖3示意性圖示根據本文描述並圖示的一個或多個實施例的將一個或多個介電層施加於玻璃層的例示性卷對卷製程;圖4示意性圖示根據本文描述並圖示的一個或多個實施例的將一個或多個介電層施加於玻璃層的例示性狹縫式模具製程;
圖5示意性圖示根據本文描述並圖示的一個或多個實施例的將一個或多個介電層施加於玻璃層的例示性層壓製程;圖6A示意性圖示根據本文描述並圖示的一個或多個實施例的包括玻璃層、介電層和導電層的玻璃基板組件的側視圖;圖6B示意性圖示根據本文描述並圖示的一個或多個實施例的包括玻璃層、介電層和包括至少一個導電跡線的導電層的玻璃基板組件的部分立體圖;圖7A示意性圖示根據本文描述並圖示的一個或多個實施例的包括具有組態為通道的三維特徵的玻璃層的例示性玻璃基板組件的部分立體圖;圖7B示意性圖示根據本文描述並圖示的一個或多個實施例的包括玻璃層、介電層和在該介電層內組態為通道的三維特徵的例示性玻璃基板組件的部分側視圖;圖8A示意性圖示根據本文描述並圖示的一個或多個實施例的包括交替玻璃層和介電層的例示性玻璃基板組件的側視圖;圖8B示意性圖示根據本文描述並圖示的一個或多個實施例的包括交替玻璃層、介電層和導電層和電耦合導電層的導電孔的玻璃基板組件的橫截面圖;圖9示意性圖示根據本文描述並圖示的一個或多個實施例的包括玻璃基板組件的電子組件;且
圖10示意性圖示根據本文描述並圖示的一個或多個實施例的正在爐內被退火的玻璃基板組件。
本文揭示的該等實施例涉及回應於高頻電子信號(例如透過各種無線通信協定限制的信號)而展示滿足需要的介電屬性的玻璃基板組件。更具體地,本文描述的該玻璃基板組件回應於具有10GHz或更高頻率的電子信號而展示滿足需要的介電常數和散逸損耗值。例示性玻璃基板包含設置於薄玻璃層的一個或兩個表面上的介電層。
如以下更具體的描述,回應於具有10GHz或更高頻率的電子信號而選取該介電層的材料具有低介電常數值和低散逸因數值。該介電層的該等介電屬性降低整個複合結構的有效介電屬性,從而將玻璃用作基板用於高速電子應用中,例如高速通信應用中。該介電層不僅提供滿足需要的高頻介電屬性,還將機械保護添加至該玻璃表面。
進一步地,本文亦揭示用於回應於高頻電子信號而降低該玻璃層的該介電常數值和逸散損失值的方法。更具體地,在一些實施例中,退火製程用於減少該玻璃層的介電屬性。之後,該介電層可設置於該退火玻璃層的一個或多個表面上。
將薄玻璃用作柔性電路板應用的基板可提供優於傳統柔性印刷電路板材料的優勢,其一般由聚合物、
聚合物/玻璃纖維複合物製成。該等優勢包括但不限於優於傳統柔性印刷電路板材料的更優的熱屬性(包括熱能力和熱傳導性)、增強的光品質,例如光傳輸,增強的厚度控制、更優的表面品質、更優的尺寸穩定性和更優的氣密性。該等屬性不加限制地能夠實現熱偏離>300℃;熱傳導>0.01W/cmK;光透明或半透明應用的傳輸>50%、>70%或>90%;電子裝置結構的特徵分辨率<50μm、<20μm、<10μm或<5μm;水蒸氣傳輸速率<10-6g/m2/天;多層裝置的層-至-層定位<10μm、<5μm或<2μm;或電子頻率應用≧10GHz、≧20GHz、≧50GHz或≧100GHz。
以下詳細描述各種玻璃基板組件、電子組件和製造玻璃基板組件的方法。
現在參考圖1和2,示意性圖示部分例示性玻璃基板組件100。該所示實施例的該玻璃基板組件100包括由玻璃基板製成的玻璃層110和設置於該玻璃層110的第一表面112上的介電層120。儘管圖1和2中將該玻璃基板組件100示為僅具有設置於該玻璃層110的該第一表面112上的介電層120,應當理解,在其他實施例中,另一介電層可設置於該玻璃層110的該第二表面113上。進一步地,相同或不同材料的多個介電層可彼此堆疊。如以下更具體地描述,該玻璃基板組件100可用作電子應用中的柔性印刷電路板,例如高速無線通信應用。
在實施例中,該玻璃層110具有厚度,從而為柔性。例示性的厚度包括但不限於小於約300μm小於約200μm、小於約100μm、小於約50μm和小於約25μm。此外或作為選擇性地,例示性厚度包括但不限於大於約10μm、大於約25μm、大於約50μm、大於約75μm、大於約100μm、大於約125μm,或大於約150um。例示性柔性的玻璃基板能夠以低於300mm的半徑或低於200mm的半徑或低於100mm半徑彎曲。應當注意,在高頻無線通信應用中,該玻璃層110越薄越好,從而該玻璃基板組件100的有效介電屬性透過該介電層120相比於該玻璃層110更佔據主導。應當理解,在其他實施例中,該玻璃層110不為柔性且可具有大於約200um的厚度。在實施例中,該玻璃層110包含基本上由或由玻璃材料、陶瓷材料、玻璃-陶瓷材料或其組合組成。作為非限制性實例,該玻璃層110可為硼矽酸鹽玻璃(康寧股份有限公司製造的品牌名為Willow®Glass的玻璃)、鹼土硼-鋁矽酸鹽玻璃(例如,康寧股份有限公司製造的品牌名為EAGLE XG®的玻璃)、鹼土硼-鋁矽酸鹽玻璃(例如,康寧股份有限公司製造的品牌名為Contego Glass的玻璃)。應當理解,亦可使用其他玻璃、玻璃陶瓷、陶瓷、多層或複合組合物。
該介電層120可為能夠固定至該玻璃層110的一個或多個表面的任意材料,且任意材料具有介電常數值和散逸因數值,從而該玻璃基板組件100的該有效介電
常數值和有效散逸因數值回應於具有10GHz頻率的電磁輻射而分別小於或等於5.0及小於或等於0.003。應當注意,本文中的短語「電磁輻射」和「電子信號」可換用且指示根據一個或多個無線通信協定傳輸並接收或沿著裝配於該玻璃基板組件100上或內的該電子電路傳播的信號。其包括沿著限定的導體路徑自該玻璃基板組件100的一位置向另一位置傳輸的電磁輻射和向周圍環境無線傳輸或自其無線接收的電磁輻射。裝配於該玻璃基板組件100上或內的電子導體路徑能夠包括帶狀線、微帶線、共面傳輸線和電子信號和接地導體的其他組合。進一步地,該等術語「介電常數值」和「散逸因數值」回應於利用該分鋼共振器方法的10GHz指示該參考特定內建基板層或該特定內建基板層屬性。已知用於測定該等材料的複介電常數的該分鋼共振器方法且可購得描述為IPC標準TM-6502.5.5.13的設備。應當理解,本文揭示的玻璃基板組件100可在高於10GHz的頻率下操作且選擇10GHz僅為了樹立基準和定量。如一實例且非限制的,該介電層120回應於具有10GHz頻率的電磁輻射而具有小於約5.0的介電常數值和小於約0.003的散逸因數值。如另一非限制性實例,該介電層120回應於具有10GHz頻率的電磁輻射而具有約2.2至約2.5之範圍的介電常數值和小於約0.003的散逸因數值。該等術語「有效介電常數值」和「有效散逸因數值」指示沿著該玻璃基板組件100上的限定的傳輸線或導體路徑的該電磁傳播
的回應。在這種情況下,該電子信號以相同的速度和損失在裝配於該玻璃基板組件100上的該傳輸線或導體路徑傳播,似乎其嵌入帶有「有效介電常數值」和「有效散逸因數值」的非均勻材料中。
用於該介電層120的例示性材料包括但不限於例如二氧化矽和低介電常數(低k)聚合物材料等無機材料。例示性低k聚合物材料包括但不限於聚醯亞胺、芳香族聚合物、聚對二甲苯、方向聚酰胺、聚酯、聚四氟乙烯®和聚四氟乙烯。附加的低k材料包括干凝膠和氣凝膠氧化物。包括多孔結構的其他材料亦是可能的。應當注意,亦可利用在10GHz的頻率下能夠沉積於該玻璃層110的一個或多個表面上的帶有小於5.0的介電常數的任意材料。
在2.986GHz和10GHz的電磁輻射頻率下評估一些例示性紫外光(「UV」)固化介電塗覆的介電常數值(Dk)和散逸損失因數值(Df)。下表1圖示利用該分鋼共振器方法在2.986GHz和10GHz下評估的該例示性UV固化介電塗覆的Dk和Df。該等材料適用於本文描述的該介電層120。
表1中的各介電塗覆包括配製參考號。各介電塗覆的配製透過其配製參考號在表2A和表2B中提供。表2A和表2B中揭示的該等值是在該等各配製中各材料的重量的代表性部分。在各種實施例中,該介電塗覆配製包括在一個或多個材料,例如選自丙烯酸異冰片酯、丙烯酸二環戊酯、甲基丙烯酸金剛烷酯、苯氧基丙烯酸芐酯(自
南韓的Miwon Specialty Chemical公司購得的Miramer M1120)、三環葵烷二甲醇二丙稀酸酯(自法國的阿科瑪購得的SR833 S)和/或二茂鐵甲基丙烯酸酯(自法國的阿科瑪購得的CD535)中的丙烯酸酯單體;選自雙酚芴二丙烯酸酯(自南韓的Miwon Specialty Chemical公司購得的Miramer HR6060)和/或全氟聚醚(PFPE)-尿烷丙烯酸酯(自比利時的索爾維基團購得的Fluorolink® AD1700)中的氟化丙烯酸酯材料;和選自1-羥基-環己基-苯基酮(自德國的巴斯夫股份公司購得的Irgacure® 184)和/或二(2,4,6-三甲基苯甲酰)-苯基-氧化磷(自德國的巴斯夫股份公司購得的Irgacure® 819)中的光引發劑。
應當注意,包括在該等配製中的光引發劑的量適用於玻璃之間的塗覆。若其固化有一曝露的表面,該等水平不產生具有足夠表面固化的樣本。
該介電層120可透過任意適用的製程施加於該玻璃層110的表面。當該玻璃層110為柔性材料時,該介電層120可透過卷對卷製程施加於該玻璃層110。該介電層120亦可施加於玻璃的單個板,但不是在卷對卷製程中。
現在參考圖3,示意性圖示用於將介電材料121沉積於玻璃網111上的卷對卷製程150。應當注意,當切割為形成該玻璃基板組件100的尺寸時,該介電材料121和該玻璃網111分別形成該介電層120和該玻璃層110。在所示實施例中,該玻璃網111為初始線軸101的形式。例如,該柔性玻璃網111可環繞核心捲繞。之後,該玻璃網111朝向並透過介電層沉積系統130退繞。該介電層沉積系統130將該介電材料121沉積於該玻璃網111的一個或兩個表面上。在一些實施例中,在接收該介電材料121之後,該玻璃網111可捲繞至第二線軸103。之後,例如,非限制性地,透過成形(例如,透過雷射鑚
磨)、電鍍(例如,以形成導電跡線和平面)、附加塗覆、切割和電子元件安裝,該第二線軸103的該塗覆的玻璃網111被運輸至一個或多個下游製程。相似地,該玻璃網111(或片材製程中的玻璃板)在沉積介電材料121之前可經受一個或多個上游製程。相似地,該等上游製程能夠非限制性地包括透過成形(例如,透過雷射鑚磨)、電鍍(例如,以形成導電跡線和平面)、附加塗覆、切割和電子元件安裝。而且,若該介電材料121沉積於該玻璃網111或玻璃板的兩個表面上,其無需對稱。該玻璃網111或玻璃板的一表面上的該介電材料121組成物、圖案、厚度和其他屬性與該玻璃網或基板的另一表面上的該介電材料屬性不同。
該介電層沉積系統130可為任意能夠將該介電材料121沉積於該玻璃網111上的組件或系統。如一實例且非限制的,圖4示意性圖示用於在例如卷對卷製程中將介電材料121沉積於柔性玻璃網111上的例示性狹縫式模具塗覆系統130A。應當理解,儘管圖1中僅示出一個表面,該介電材料121可塗覆至該玻璃網111的兩個表面上。該系統130A包括連續將該介電材料121沉積於該玻璃網111上的狹縫式模具。應當理解,在實施例中,該玻璃網111的兩個表面塗覆有該介電材料121,提供另一狹縫式模具用以塗覆該第二表面。進一步地,亦可提供附加的處理組件或系統,其在圖4中未圖示,例如固化組件(熱固化、UV固化等類似組件)。應當理解,可利用除
了狹縫式模具塗覆以外的塗覆系統。該附加的塗覆系統可非限制性地包括基於溶液的製程,例如列印方法或其他塗覆方法。該塗覆系統亦能夠包括無機薄膜沉積技術,例如噴射、PECVD、ALD和其他製程。該等方法可用於將介電材料121的連續層沉積至該玻璃基板。該等方法亦能夠用於沉積包括該玻璃基板區域的圖案化介電材料層,其塗覆且未塗覆包括3D形狀、垂直輪廓或複雜3D輪廓(例如不同厚度、通道、孔、立體浮凸或柱狀結構)的該介電材料區域。
現在參考圖5,示意性圖示用於將介電材料121施加於玻璃網111的層壓系統130B。該層壓系統130B包括至少兩個滾輪134A、134B。在該等滾輪134A、134B之間給進該介電材料121和該柔性玻璃網111,以將該介電材料121層壓至該柔性玻璃網111。在一些實施例中,之後,將該層壓的柔性玻璃網111軋製成線軸。亦可利用已知的或將要研製的層壓製程。
如上述,該介電材料121可施加於該玻璃基板111的單個板,但不是在卷對卷製程中。
在將該介電材料121施加於該玻璃基板或網111之後,該塗覆的玻璃基板/網111被切割成複數個具有一個或多個所需形狀的玻璃基板組件。對於在相對高的電磁輻射的頻率下的該玻璃基板組件100的該低介電常數值和散逸因數值用作無線通信應用中的柔性印刷電路板而言是理想的。
現在參考圖6A,導電層142設置於該介電層120上、下方或內。圖6A是包括設置於介電層120上的導電層142的例示性玻璃基板組件200的側視圖。根據電子組件的圖解,該導電層142可包括或組態為複數個導電跡線和/或導電襯墊。圖6B是圖6A中的該例示性玻璃基板組件200的俯視圖,其中,該導電層142包括該介電層120的表面122上的導電跡線145。例如,根據電子電路,該導電跡線145可電耦合兩個或更多電子元件。例如,該導電層142亦可組態為接地平面。因此,該導電層142可呈現任意組態。如所需產生所需的電子電路、傳輸線或傳導路徑,該導電層142和導電跡線145能夠形成於該介電層120的頂部上和/或該玻璃基板110(例如,該玻璃基板和該介電層之間或該介電層的下方)的頂部上。
該導電層142可由能夠傳播電信號的導電材料(例如銅、錫、銀、金、鎳等類似材料)製成。應當理解,其他材料或材料組合物可用於該導電層142。該導電層142可透過例如電鍍製程或列印製程設置於該介電層120上。應當理解,任意已知或將要研製的製程可用於將該導電層142施加於該介電層120。
在一些實施例中,該介電層120的表面122包括一個或多個三維特徵。如本文中使用,短語「三維特徵」指示具有長度、寬度和高度的特徵。該三維特徵可呈現任意尺寸和組態。圖7A和7B示意性圖示組態為該介電層120的表面122內的通道125的例示性三維特徵。如一實
例且非限制的,導電跡線可設置於電耦合電子元件的該通道125內。例如就在該導電跡線內傳播的電信號而言,至少部分環繞該通道125內的該導電跡線可提供電磁干擾防護。例如,這種防護在高速通信應用中有益。
該等三維特徵可透過任意已知或將要研製的製程製成。用於製造該等三維特徵的例示性製程包括但不限於光刻(例如,UV壓印光刻)和微複製製程。
在實施例中,玻璃層110的多個交替層和介電層120可設置為堆層。現在參考圖8A,示意性圖示包含交替玻璃層110A-110C和介電層120A-120C的部分例示性堆層160。介電層120B設置於玻璃層110A和110B之間且介電層120C設置於玻璃層110B和110C之間。介電層120A設置於玻璃層110A的頂部或外表面上。例如,該等單個層可在層壓製程中層壓,以形成該堆層160。然而,本文揭示的實施例不限於設置該等交替層和介電層的任意具體方法。該多層堆層能夠亦包括多個介電層或形成於帶有設置於其間的玻璃基板的其相互頂部的相同或不同的組成物。
玻璃和介電層的堆層160可用作柔性印刷電路板。例如,導電層可設置於該堆層160內的內部介電層內或上。參考圖8B,示意性圖示包含玻璃層110A-110C和介電層120A-120E的部分例示性堆層160'。在圖8B中,第一導電層140A設置於介電層120A上,第二導電層140B設置於介電層120B和介電層120C之間,且第三
導電層140C設置於介電層120D和介電層120E之間。該等介電層140A-140C可呈現任意組態,例如導電跡線、接地平面、導電襯墊和其組合。
在實施例中,導電孔可設置於電耦合至各種導電層的多層之間。圖8B示意性圖示設置於電耦合至導電層140B和140C的一個或多個特徵(例如,跡線)的介電層120C、玻璃層110B和介電層120D之間的第一和第二孔146A、146B。
該等孔可貫穿各種層先於將該等層層壓成堆層形成。參考圖8B,例如,如上述,介電層120C和120D可首先施加於玻璃層110B。之後,孔(例如,第一和第二孔146A、146B)貫穿該等介電層120C、120D和該玻璃層110B形成。如一實例且非限制的,該等孔可透過雷射損壞和蝕刻製程形成,其中,一個或多個雷射光束預鑚磨該等介電層120C、120D和玻璃層110B且隨後的蝕刻製程將該等孔的直徑擴大至所需尺寸。美國專利申請第62/208,282號描述了例示性雷射鑚磨製程,以其內容為依據並且透過引用以整體納入本文。之後,在金屬化製程中用導電材料填充該等孔。可層壓該等介電層120C、120D和玻璃層110B或附接至其它層(例如導電層140A和140B)並接近介電和玻璃層。
如上述,本文揭示的該玻璃基板組件可用作電子組件(例如能夠傳輸和/或接收無線信號的無線通信電子組件)的柔性印刷電路板。圖9示意性圖示例示性電子
組件301。應當理解,僅出於說明目的提供所示電子組件301且實施例不限於此。該電子組件301包括基板組件300,該基板組件300包含至少一個玻璃層310和至少一個介電層320。積體電路元件360設置於該介電層320的表面322上(例如,該介電層320上或內的導電襯墊(未圖示)上)。附加的電子元件362A-362C亦設置於該介電層320的該表面322上且透過導電跡線342電耦合至該積體電路元件360。
該積體電路元件360可為無線傳輸器、無線接收器或無線收發器裝置。在一些實施例中,該積體電路元件360可組態用以傳輸和/或接收10GHz和以上頻率的無線信號。該基板組件300的該低介電常數和散逸因數值使該基板組件300成為柔性印刷電路板的理想基板。
在一些實施例中,先於用該介電層塗覆該玻璃層,透過退火製程降低該玻璃層的該低介電常數和散逸因數值。出乎意料地,本發明人發現相比於未經受退火製程或再成形製程的薄玻璃基板,經受退火製程或再成形製程的薄玻璃基板回應於具有10GHz的頻率的電磁輻射而具有較低的介電常數和散逸因數值。試驗數據表明經受本文描述的退火製程的該玻璃層在10GHz頻率下該介電常數值降低了10%且散逸因數值降低了75%以上。該玻璃層的該等介電屬性的降低降低了本文描述的包括玻璃層和介電層的該等基板組件的該有效介電屬性。
現在參考圖10,在爐170內將玻璃層110(例如,在單個板或線軸內)加熱至高於該玻璃層110的應變點的第一溫度(例如,最大溫度)。在一些實施例中,該第一溫度高於該玻璃層110的該退火點。此外或作為選擇性地,該第一溫度低於該玻璃層110的該軟化點。如本文使用,短語「應變點」指示該玻璃層在該溫度下具有1014.5泊的黏度的溫度。如本文使用,短語「退火點」指示該玻璃層在該溫度下具有1013泊的黏度的溫度。如本文使用,短語「軟化點」指示該玻璃層在該溫度下具有107.6泊的黏度的溫度。該爐170將該玻璃層110加熱至該第一溫度。在一些實施例中,該玻璃層110的該溫度以所需速率(例如,250℃/小時)遞增增加。之後,將該玻璃層110保持在該第一溫度下長達第一時間段,以使該玻璃層110的內應力鬆弛。例如,該玻璃層110保持在該第一溫度的約20%、約10%、約5%或約1%的變化內長達第一時間段。之後,將該玻璃層110冷卻至第二溫度(例如,室溫,或約25℃)超過第二時間段。該退火製程降低了該玻璃層110的介電屬性,從而回應於處於10GHz頻率的電磁輻射而介電常數值小於約5.0和散逸因數值小於約0.003。
以下實例闡釋退火製程如何回應於處於10GHz頻率的電磁輻射而降低薄玻璃基板的介電屬性。利用分鋼法評估薄玻璃基板的該等介電屬性。
實例1中,提供兩個0.1mm康寧® EAGLE XG®玻璃基板。一玻璃基板用作控制且不經受退火製程,而另一玻璃基板透過以250℃/小時的速率將其遞增加熱至700℃被退火。該玻璃基板被保持在700℃下長達10小時,之後將其冷卻至室溫超過10小時。於10GHz下評估這兩個樣本的介電屬性。該控制玻璃基板呈現約5.14的介電常數值和約0.0060的散逸因數值。該退火玻璃基板呈現約5.02的介電常數值和約0.0038的散逸因數值。
實例2中,提供三個0.7mm由康寧股份有限公司製造的EAGLE XG®玻璃基板。一玻璃基板用作控制且不經受退火製程。透過該第二玻璃基板以250℃/小時的速率將其遞增加熱至600℃被退火。該第二玻璃基板被保持在600℃下長達10小時,之後將其冷卻至室溫超過10小時。透過該第三玻璃基板以250℃/小時的速率將其遞增加熱至650℃被退火。該第三玻璃基板被保持在650℃下長達10小時,之後將其冷卻至室溫超過10小時。於10GHz下評估這三個樣本的介電屬性。該控制玻璃基板呈現約5.21的介電常數值和約0.0036的散逸因數值。於600℃溫度下退火的該第二玻璃基板呈現約5.18的介電常數值和約0.0029的散逸因數值。於
650℃溫度下退火的該第三玻璃基板呈現約5.18的介電常數值和約0.0026的散逸因數值。
實例3中,提供兩個個0.7mm由康寧股份有限公司製造的Contego玻璃基板。一玻璃基板用作控制且不經受退火製程。透過該第二玻璃基板以250℃/小時的速率將其遞增加熱至600℃被退火。該第二玻璃基板被保持在600℃下長達10小時,之後將其冷卻至室溫超過10小時。該控制玻璃基板呈現約4.70的介電常數值和約0.0033的散逸因數值。於600℃溫度下退火的該第二玻璃基板呈現約4.68的介電常數值和約0.0027的散逸因數值。
現在應當理解,本揭露的實施例提供回應於高頻無線信號而呈現所需介電屬性的玻璃基板組件。該等玻璃基板組件可用作電子組件(例如,無線收發器)內的柔性印刷電路板。更具體地,本文描述的該玻璃基板組件回應於具有10GHz或更高頻率的電子信號而展示滿足需要的介電常數和散逸損耗值。例示性玻璃基板包含設置於薄玻璃層的一個或兩個表面上的介電層。在一些實施例中,退火製程用於減少該玻璃層的介電屬性。
儘管本文已描述例示性實施例,所屬技術領域具有通常知識者應當理解,可在形式和細節上作出各種改變而不脫離所附申請專利範圍包含的範圍。
110:玻璃層
120:介電層
142:導電層
200:玻璃基板組件
Claims (22)
- 一種基板組件,其包含:一經退火的玻璃層,其包含一第一表面及一第二表面;及一介電層,其設置於該經退火的玻璃層的該第一表面或該第二表面中的至少一個上,該介電層回應於具有10GHz的一頻率的電磁輻射而具有小於3.0的一介電常數值;其中該經退火的玻璃層回應於具有10GHz的一頻率的電磁輻射而具有小於約5.0的一介電常數值。
- 如請求項1所述之基板組件,其中,該經退火的玻璃層具有小於約300μm的一厚度。
- 如請求項1所述之基板組件,其中,該介電層回應於具有10GHz一頻率的電磁輻射而具有小於約0.003的一散逸因數值。
- 如請求項1所述之基板組件,其中,該介電層的介電常數值回應於具有10GHz一頻率的電磁輻射而在約2.2至約2.5之一範圍內。
- 如請求項1至4中任意一項所述之基板組件,其中,該經退火的玻璃層回應於具有10GHz一頻率的電磁輻射而具有小於約0.003的一散逸因數值。
- 如請求項5所述之基板組件,其中,該經退 火的玻璃層的介電常數值回應於具有10GHz一頻率的電磁輻射而在約4.7至約5.0之一範圍內,且該經退火的玻璃層的散逸因數值在約0.000至約0.003之一範圍內。
- 如請求項1至4中任意一項所述之基板組件,其中,該介電層包含一聚合物。
- 如請求項1至4中任意一項所述之基板組件,其進一步包含設置於該介電層內、該介電層下方或該介電層一表面上的一導電層。
- 如請求項8所述之基板組件,其中,該導電層包含複數個導電跡線。
- 如請求項1至4中任意一項所述之基板組件,其中,該介電層的一表面包含至少一個三維特徵。
- 如請求項10所述之基板組件,其中:該至少一個三維特徵包含該介電層的表面內的一通道;及該基板組件包含設置於該通道內的一導電跡線。
- 如請求項10所述之基板組件,其中,該至少一個三維特徵進一步包含該介電層內的一通孔。
- 如請求項1至4中任意一項所述之基板組件,其進一步包含: 一第二玻璃層,其包含一第一表面和一第二表面,該介電層設置於該經退火的玻璃層的該第二表面和該第二玻璃層的該第一表面之間;及一第二介電層,其設置於該第二玻璃層的該第二表面上。
- 如請求項1至4中任意一項所述之基板組件,其進一步包含:一導電層,其設置於該介電層的一表面上;一第二介電層,其設置於該導電層的一表面上;一第二玻璃層,其設置於該第二介電層的一表面上;及一第三介電層,其設置於該第二玻璃層的一表面上。
- 一種電子組件,其包含:一經退火的玻璃層,其包含一第一表面及一第二表面;一介電層,其設置於經退火的玻璃層的該第一表面或該第二表面中的至少一個上,該介電層回應於具有10GHz一頻率的電磁輻射而具有小於3.0的一介電常數值;複數個導電跡線,其設置於該介電層內、該介電層的下方或該介電層的一表面上;及 一積體電路元件,其設置於該介電層的該表面上且電耦合至該複數個導電跡線的一個或多個導電跡線,其中,該積體電路元件被組態用以進行無線通信信號的傳送或接收中的至少一個;其中該經退火的玻璃層回應於具有10GHz的一頻率的電磁輻射而具有小於約5.0的一介電常數值。
- 如請求項15所述之電子組件,其中,該經退火的玻璃層具有小於約300μm的一厚度。
- 如請求項15所述之電子組件,其中,該介電層回應於具有10GHz一頻率的電磁輻射而具有小於約0.003的一散逸因數值。
- 如請求項15所述之電子組件,其中,該介電層的介電常數值回應於具有10GHz一頻率的電磁輻射而在約2.2至約2.5之一範圍內。
- 如請求項15至18中任意一項所述之電子組件,其中,該經退火的玻璃層回應於具有10GHz一頻率的電磁輻射而具有小於約0.003的一散逸因數值。
- 如請求項19所述之電子組件,其中,該經退火的玻璃層的介電常數值回應於具有10GHz一頻率的電磁輻射而在約4.7至約5.0之一範圍內,且該經退火的玻璃層的散逸因數值在約0.000至約0.003 之一範圍內。
- 如請求項15至18中任意一項所述之電子組件,其中:該介電層的該表面包含複數個通道;且該複數個導電跡線設置於該複數個通道內。
- 一種製造一玻璃基板組件的方法,該方法包含以下步驟:將一玻璃基板加熱至高於該玻璃基板的一應變點且低於該玻璃基板的一軟化點的一第一溫度;將該玻璃基板保持在該第一溫度的約10%的變化內長達一第一時間段;將該玻璃基板冷卻至一第二溫度超過一第二時間段,從而在冷卻該玻璃基板之後,該玻璃基板回應於具有10GHz的一頻率的電磁輻射而具有小於約5.0的一介電常數值;及將一介電層施加於該玻璃基板的至少一個表面上,該介電層回應於具有10GHz的一頻率的電磁輻射而具有小於約2.5的一介電常數值。
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- 2016-08-19 JP JP2018509741A patent/JP2018525840A/ja active Pending
- 2016-08-19 TW TW105126522A patent/TWI711348B/zh not_active IP Right Cessation
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EP3338521A1 (en) | 2018-06-27 |
KR20180052646A (ko) | 2018-05-18 |
CN107926110B (zh) | 2021-04-30 |
US20180249579A1 (en) | 2018-08-30 |
WO2017034958A1 (en) | 2017-03-02 |
JP2018525840A (ja) | 2018-09-06 |
EP3338520A1 (en) | 2018-06-27 |
KR20180048723A (ko) | 2018-05-10 |
JP2018536276A (ja) | 2018-12-06 |
TW201714500A (zh) | 2017-04-16 |
CN107926111A (zh) | 2018-04-17 |
CN107926110A (zh) | 2018-04-17 |
US20180166353A1 (en) | 2018-06-14 |
WO2017034969A1 (en) | 2017-03-02 |
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