TWI470833B - 半導體裝置及其製造方法 - Google Patents

半導體裝置及其製造方法 Download PDF

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TWI470833B
TWI470833B TW101119907A TW101119907A TWI470833B TW I470833 B TWI470833 B TW I470833B TW 101119907 A TW101119907 A TW 101119907A TW 101119907 A TW101119907 A TW 101119907A TW I470833 B TWI470833 B TW I470833B
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substrate
semiconductor device
epitaxial structure
doped layer
optical band
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Yuan Hsiao Chang
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Phostek Inc
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Description

半導體裝置及其製造方法
本發明係有關一種半導體裝置,特別是關於一種垂直式半導體裝置。
第一圖顯示傳統半導體裝置100的立體示意圖,其結構由下而上依序為藍寶石基板11、n型摻雜層12、主動層13、p型摻雜層14、透明接觸層15、負電極16及正電極17。此種結構之發光二極體又稱為水平式發光二極體,因為其電流由正電極17至負電極16的流向為水平流向。電流容易在負電極16下方產生電流擁擠現象,因而造成操作電壓上升及動態電阻的增加,因而升高元件的溫度。
因此亟需提出一種新穎的半導體裝置,用以解決上述電流擁擠及溫度升高的問題。
鑑於上述,本發明實施例提出一種垂直式半導體裝置及其製造方法,其結構可降低或避免傳統水平式半導體裝置的電流擁擠現象,及其所造成的操作電壓上升、動態電阻增加及溫度升高等問題。
根據本發明實施例,首先提供一基板,且形成至少一磊晶 結構於上。接著,切割並剝離基板的一部分,以曝露磊晶結構的部分表面。形成第一電極於磊晶結構的曝露表面,因而形成垂直式半導體裝置。在一實施例中,提供一導電基板,且耦接導電基板於至少一磊晶結構相對於基板的另一側,因而形成覆晶式半導體裝置。
100‧‧‧半導體裝置
11‧‧‧藍寶石基板
12‧‧‧n型摻雜層
13‧‧‧主動層
14‧‧‧p型摻雜層
15‧‧‧透明接觸層
16‧‧‧負電極
17‧‧‧正電極
200‧‧‧半導體裝置
300‧‧‧半導體裝置
21‧‧‧基板
211‧‧‧空缺區
22‧‧‧磊晶結構
221‧‧‧第一摻雜層
222‧‧‧主動層
223‧‧‧第二摻雜層
224‧‧‧穿隧接面
22’‧‧‧磊晶結構
225‧‧‧第一摻雜層
226‧‧‧主動層
227‧‧‧第二摻雜層
23‧‧‧第一電極
24‧‧‧第二電極
25‧‧‧透明導電層
26‧‧‧導電基板
28‧‧‧阻隔層
第一圖顯示傳統發光二極體的立體示意圖。
第二A圖至第二F圖顯示本發明第一實施例之半導體裝置的製程剖面或立體圖。
第三A圖至第三E圖顯示本發明第二實施例之半導體裝置的製程剖面或立體圖。
第二A圖至第二F圖顯示本發明第一實施例之半導體裝置200的製程剖面或立體圖。本實施例雖以發光二極體(LED)及光伏電池(photovoltaic cell)作為例示,然而本發明也可適用於其他半導體裝置,例如電晶體(transistor)或其他二極體(diode)。
首先,如第二A圖所示,提供一基板21。在本實施例中,基板21的材質可吸收第一光波段,並供第二光波段穿透,其中第一光波段與第二光波段相異。此外,基板21為非導體,例如藍寶石(sapphire),然而也可以使用其他材質,例如玻璃或石英,但不限定於此。本實施例若以發光二極體(LED)作為例示,則第二光波段可介於400奈米至1600奈米。若本實施例以光伏電池作為例示,則第二光波 段可介於200奈米至2000奈米。此外,基板21包括極化(polar)基板、半極化(semi-polar)基板或非極化(non-polar)基板。
接著,以磊晶製程技術形成至少一磊晶結構22於基板21上。在本實施例中,磊晶結構22依序包含第一摻雜層221、主動層222及第二摻雜層223,其中第一摻雜層221靠近基板21,第二摻雜層223遠離基板21,且主動層222位於第一摻雜層221與第二摻雜層223之間。此外,第一摻雜層221的電性相反於第二摻雜層223的電性。例如,第一摻雜層221為n型摻雜,且第二摻雜層223為p型摻雜。主動層222可以是單一量子井(SQW)層或多重量子井(MQW)層,但不限定於此。本實施例之磊晶結構22的材質可為三族氮化物,例如氮化銦(InN)、氮化鎵(GaN)、氮化鋁(AlN)、氮化銦鎵(InGaN)、氮化銦鋁鎵(InAlGaN)等,但不限定於上述。
第二B圖顯示第二A圖的另一變化態樣。在本實施例中,形成多個磊晶結構於基板21上,例如依序形成磊晶結構22及磊晶結構22’,以形成堆疊磊晶結構於基板21上。其中,磊晶結構22’藉由穿隧接面224而堆疊於磊晶結構22上。本實施例之磊晶結構22’依序包含第一摻雜層225、主動層226及第二摻雜層227,其中第一摻雜層225靠近穿隧接面224,第二摻雜層227遠離穿隧接面224,且主動層226位於第一摻雜層225與第二摻雜層227之間。此外,第一摻雜層225的電性相反於第二摻雜層227的電性。例如,第一摻雜層225為n型摻雜,且第二摻雜層227為p型摻雜。主動層226可以是單一量子井(SQW)層或多重量子井(MQW)層,但不限定於此。本實施例之磊晶結構22’的材質可為三族氮化物,例如氮化銦(InN)、氮化鎵(GaN)、氮化鋁(AlN)、氮化銦鎵(InGaN)、氮化銦鋁鎵(InAlGaN)等,但不限定於上述。
上述形成磊晶結構22於基板21之前,還可額外圖形化(pattern)基板21的表面,如第二C圖所示。具圖形化表面的基板21可加強光的散射,因而增加光的射出量。若本實施例以光伏電池作為例示,則圖形化表面的基板21可使得光於磊晶結構22中來回通過,而增加光吸收量,有利於光電轉換。
接下來,如第二D圖所示的剖面圖或第二E圖所示的立體圖,切割(cut)並剝離(lift off)基板21的一部分,以曝露第一摻雜層221的部分表面,因而於基板21形成一空缺區211。本實施例使用雷射光剝離技術以進行基板21的切割與剝離,但不限定於此。上述雷射光剝離技術所使用之雷射光之光波長介於第一光波段中,由於基板21的材質可吸收第一光波段,因此基板21吸收雷射光而被加熱部分剝離消除,因而形成空缺區211。
上述空缺區211的形狀及位置不限定於第二D/二E圖所示。在一實施例中,於進行基板21的切割及剝離製程之前,還可額外拋光研磨(polish)基板21,使其厚度變薄,使得供第二光波段穿透之光穿透率效果更佳,且有利於切割及剝離製程的進行。接著,形成第一電極23於空缺區211中第一摻雜層221的曝露表面。第一電極23的材質為導體,例如金屬。
如第二F圖所示,形成第二電極24於磊晶結構22相對於基板21的另一側(例如圖示中的第二摻雜層223)。第二電極24的材質為導體,例如金屬。藉此,形成一種垂直式半導體裝置,電流由第二電極24至第一電極23的流向為垂直流向。本實施例所形成的結構不會有傳統水平式半導體裝置(如第一圖所示)的電流擁擠現象。在一實施例中,第二電極24與磊晶結構22之間更形成透明導電層(或透明接觸 層)25,用以增強電流的分散(spreading)。透明導電層25的材質可為銻錫氧化物(Antimony Tin Oxide,ATO)、銦錫氧化物(Indium Tin Oxide,ITO)、氧化錫(Tin Oxide,SnO2)、氧化鋅摻雜鋁(aluminum doped zinc oxide,AZO)、氧化鋅摻雜鎵(Gallium doped zinc oxide,GZO)和氧化鋅摻雜銦(Indium doped zinc oxide,IZO),但不以上述為限。
第三A圖至第三E圖顯示本發明第二實施例之半導體裝置300的製程剖面或立體圖。如第三A圖所示,形成磊晶結構22於基板21上,且形成第一電極23於空缺區211中第一摻雜層221的曝露表面。相關細節可參考第一實施例之第二A圖至第二E圖所示,不再贅述。
接著,如第三B圖所示,提供導電基板26並耦接於磊晶結構22相對於基板21的另一側(例如圖示中的第二摻雜層223),用以作為電極之用。將第三B圖的結構上下翻轉後得到一種覆晶式的半導體裝置,如第三C圖所示的立體圖。於本實施例中半導體裝置以發光二極體作為例示,基板21係作為視窗(window)層,其不但具有保護作用,且可供由磊晶結構22出射介於400奈米至1600奈米之第二光波段,以增加側面光線的射出量。若本實施例以光伏電池作為例示,則基板21可供介於200奈米至2000奈米之第二光波段入射至磊晶結構22,可增加側面光線的入射量,以提高光伏電池的光電轉換量。
上述導電基板26與磊晶結構22之間還可額外形成透明導電層25,用以增強電流的分散,如第三D圖所示。導電基板26為金屬等可導電且具有良好反射之材質,因此可增強光線的射出,或反射回收利用。
第三E圖顯示於導電基板26耦接有多個覆晶式半導體裝置 (圖式以兩個為例)。該些覆晶式半導體裝置可使用前述第三A圖至第三D圖所示製程,先形成一整體結構,再以蝕刻製程除去部分基板21與磊晶結構22,直到曝露出導電基板26,因而形成互為並聯的多個覆晶式半導體裝置,其形成一半導體裝置陣列。在另一實施例中,也可使用第三A圖所示製程,先形成多個覆晶式半導體裝置,再將其耦接至同一個導電基板26,因而形成互為並聯或串聯的多個覆晶式半導體裝置,其形成一半導體裝置陣列。為了避免相鄰覆晶式半導體裝置之間光線的干擾,可於磊晶結構22的側壁額外形成阻隔(passivation)層28。
以上所述僅為本發明之較佳實施例而已,並非用以限定本發明之申請專利範圍;凡其它未脫離發明所揭示之精神下所完成之等效改變或修飾,均應包含在下述之申請專利範圍內。
200‧‧‧半導體裝置
21‧‧‧基板
22‧‧‧磊晶結構
221‧‧‧第一摻雜層
222‧‧‧主動層
223‧‧‧第二摻雜層
23‧‧‧第一電極

Claims (21)

  1. 一種半導體裝置的製造方法,包含:提供一基板;形成至少一磊晶結構於該基板上;切割並剝離該基板的一部分,以曝露該磊晶結構的一部分表面;及形成一第一電極於該部份表面。
  2. 如申請專利範圍第1項所述半導體裝置的製造方法,其中該基板的切割與剝離係使用一雷射光剝離技術,其中該雷射光之光波長介於一第一光波段。
  3. 如申請專利範圍第2項所述半導體裝置的製造方法,其中該基板的材質可吸收該第一光波段,並供一第二光波段穿透,且該第一光波段與該第二光波段相異。
  4. 如申請專利範圍第1項所述半導體裝置的製造方法,其中該基板的材質為非導體。
  5. 如申請專利範圍第1項所述半導體裝置的製造方法,其中該磊晶結構之材質包含三族氮化物。
  6. 如申請專利範圍第1項所述半導體裝置的製造方法,其中該至少一磊晶結構包含複數磊晶結構,相鄰的該些磊晶結構藉由一穿隧接面而形成一堆疊磊晶結構。
  7. 如申請專利範圍第1項所述半導體裝置的製造方法,於形成該磊晶結構之前,更包含:圖形化(pattern)該基板面向該磊晶結構的表面。
  8. 如申請專利範圍第1項所述半導體裝置的製造方法,於切割及剝離該基板之前,更包含拋光研磨(polish)該基板使其厚度變薄。
  9. 如申請專利範圍第1項所述半導體裝置的製造方法,更包含形成一 第二電極於該磊晶結構相對於該基板的另一側。
  10. 如申請專利範圍第1項所述半導體裝置的製造方法,更包含:提供一導電基板;及耦接該導電基板於該至少一磊晶結構相對於該基板的另一側。
  11. 一種半導體裝置,包含:一基板,具有一空缺區,其中該基板的材質可吸收一第一光波段而被部分剝離,形成該空缺區,並供一第二光波段穿透,且該第一光波段與該第二光波段相異;至少一磊晶結構,形成於該基板上,該空缺區曝露該磊晶結構的一部分表面;及一第一電極,形成於該部分表面。
  12. 如申請專利範圍第11項所述半導體裝置,其中該基板的材質為非導體。
  13. 如申請專利範圍第11項所述半導體裝置,其中該磊晶結構之材質包含三族氮化物。
  14. 如申請專利範圍第11項所述半導體裝置,其中該磊晶結構包含一第一摻雜層、一主動層及一第二摻雜層,該第一摻雜層靠近該基板,該空缺區曝露該第一摻雜層的該部分表面,該第二摻雜層遠離該基板,該主動層位於該第一摻雜層與該第二摻雜層之間,且該第一摻雜層的電性相反於該第二摻雜層的電性。
  15. 如申請專利範圍第11項所述半導體裝置包括一發光裝置,其中該第二光波段係介於400奈米至1600奈米。
  16. 如申請專利範圍第11項所述半導體裝置包括一光伏電池,其中該 第二光波段係介於200奈米至2000奈米。
  17. 如申請專利範圍第11項所述半導體裝置,其中該至少一磊晶結構包含複數磊晶結構,相鄰的該些磊晶結構藉由一穿隧接面而形成一堆疊磊晶結構。
  18. 如申請專利範圍第11項所述半導體裝置,其中該基板具有一圖形化表面,該圖形化表面朝向該磊晶結構。
  19. 如申請專利範圍第11項所述半導體裝置,更包含一第二電極,形成於該磊晶結構相對於該基板的另一側。
  20. 如申請專利範圍第11項所述半導體裝置,更包含一導電基板,其耦接於該至少一磊晶結構相對於該基板的另一側。
  21. 如申請專利範圍第20項所述半導體裝置,其中耦接於該導電基板的該至少一磊晶結構包含複數磊晶結構,其互為並聯或串聯以形成一半導體裝置陣列。
TW101119907A 2012-06-04 2012-06-04 半導體裝置及其製造方法 TWI470833B (zh)

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