TWI746854B - High electron mobility transistor and method for forming the same - Google Patents
High electron mobility transistor and method for forming the same Download PDFInfo
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Abstract
Description
本發明實施例係有關於一種半導體技術,特別是有關於一種高電子移動率電晶體。 The embodiment of the present invention relates to a semiconductor technology, in particular to a high electron mobility transistor.
高電子移動率電晶體(High Electron Mobility Transistor,HEMT)因具有高崩潰電壓、高輸出電壓等優點,廣泛應用於高功率半導體裝置當中。 High Electron Mobility Transistor (HEMT) is widely used in high power semiconductor devices due to its advantages of high breakdown voltage and high output voltage.
傳統上,高電子移動率電晶體利用三五族半導體堆疊而形成。然而,源極/汲極電極與三五族半導體之間形成的異質接面(heterojunction)阻值極高,需利用高溫熱製程使金屬擴散,形成歐姆接觸(ohmic contact)以降低接觸電阻(contact resistance,Rc)阻值。然而,當三五族半導體及基板均為透光材料時,易使溫度感應器偵測異常,而使歐姆接觸形成失敗,導致無法有效降低阻值。 Traditionally, high electron mobility transistors are formed by stacking three or five group semiconductors. However, the heterojunction formed between the source/drain electrode and the third and fifth group semiconductor has a very high resistance value. A high-temperature thermal process is required to diffuse the metal to form an ohmic contact to reduce the contact resistance ( contact resistance, Rc) resistance value. However, when the third and fifth group semiconductors and the substrate are both light-transmitting materials, it is easy to make the temperature sensor detect abnormalities, and the ohmic contact formation fails, which makes it impossible to effectively reduce the resistance.
雖然現有的高電子移動率電晶體大致符合需求,但並非各方面皆令人滿意,特別是形成高電子移動率電晶體良好的歐姆接觸仍需進一步改善。 Although the existing high electron mobility transistors generally meet the requirements, they are not satisfactory in all aspects. In particular, the formation of good ohmic contacts for high electron mobility transistors still needs further improvement.
根據一實施例,本發明提供一種高電子移動率電晶體的形成方法,包括:形成緩衝層於透光基板上;形成阻障 層於緩衝層上,通道區位於緩衝層中,鄰近緩衝層與阻障層之介面;形成介電層於阻障層上;形成源極/汲極電極,穿過介電層及阻障層,設於緩衝層上;形成遮光層順應性地覆蓋於介電層及源極/汲極電極上;及對源極/汲極電極進行熱製程。 According to one embodiment, the present invention provides a method for forming a high electron mobility transistor, including: forming a buffer layer on a light-transmitting substrate; forming a barrier layer on the buffer layer, and the channel region is located in the buffer layer, adjacent to the buffer layer and The interface of the barrier layer; the formation of a dielectric layer on the barrier layer; the formation of source/drain electrodes, which pass through the dielectric layer and the barrier layer, and are placed on the buffer layer; the formation of a light-shielding layer that conforms to the dielectric Layer and source/drain electrodes; and thermally process the source/drain electrodes.
根據另一實施例,本發明提供一種高電子移動率電晶體包括:緩衝層,位於透光基板上;阻障層,位於緩衝層上,其中通道區位於緩衝層中,鄰近緩衝層與阻障層之介面;介電層,位於阻障層上;源極/汲極電極,穿過介電層及阻障層,設於緩衝層上;遮光層,覆蓋於源極/汲極電極上。 According to another embodiment, the present invention provides a high electron mobility transistor including: a buffer layer located on a light-transmitting substrate; a barrier layer located on the buffer layer, wherein the channel region is located in the buffer layer and is adjacent to the buffer layer and the barrier layer. The interface of the layer; the dielectric layer is located on the barrier layer; the source/drain electrode passes through the dielectric layer and the barrier layer and is located on the buffer layer; the light shielding layer covers the source/drain electrode.
為讓本發明之上述目的、特徵及優點能更明顯易懂,下文特舉數個實施例,並配合所附圖式,作詳細說明如下。 In order to make the above-mentioned objects, features and advantages of the present invention more obvious and understandable, several embodiments are cited below in conjunction with the accompanying drawings, which are described in detail as follows.
10‧‧‧晶圓 10‧‧‧wafer
12‧‧‧溫度感測器 12‧‧‧Temperature sensor
16‧‧‧光源 16‧‧‧Light source
100、200、300、400‧‧‧高電子移動率電晶體 100, 200, 300, 400‧‧‧High electron mobility transistor
102‧‧‧基板 102‧‧‧Substrate
104‧‧‧緩衝層 104‧‧‧Buffer layer
106‧‧‧阻障層 106‧‧‧Barrier layer
108‧‧‧通道區 108‧‧‧Passage Area
110‧‧‧介電層 110‧‧‧Dielectric layer
112‧‧‧源極/汲極電極 112‧‧‧Source/Drain electrode
112i‧‧‧界面 112i‧‧‧Interface
114、114a、114b‧‧‧遮光層 114, 114a, 114b‧‧‧shading layer
116‧‧‧熱製程 116‧‧‧Heat process
118‧‧‧蝕刻製程 118‧‧‧Etching process
120‧‧‧閘極電極 120‧‧‧Gate electrode
224‧‧‧蝕刻停止層 224‧‧‧Etching stop layer
318‧‧‧蝕刻製程 318‧‧‧Etching process
426‧‧‧能帶調整層 426‧‧‧Energy Band Adjustment Layer
以下將配合所附圖式詳述本發明實施例。應注意的是,依據在業界的標準做法,各種特徵並未按照比例繪製且僅用以說明例示。事實上,可能任意地放大或縮小元件的尺寸,以清楚地表現出本發明實施例的特徵。 The embodiments of the present invention will be described in detail below in conjunction with the accompanying drawings. It should be noted that, according to standard practices in the industry, the various features are not drawn to scale and are only used for illustration and illustration. In fact, it is possible to arbitrarily enlarge or reduce the size of the element to clearly show the characteristics of the embodiment of the present invention.
第1~6、7A、7B、8、9圖係根據一些實施例繪示出形成高電子移動率電晶體不同階段的剖面示意圖。 Figures 1 to 6, 7A, 7B, 8, and 9 are schematic cross-sectional diagrams illustrating different stages of forming a high electron mobility transistor according to some embodiments.
第10至12圖係根據另一些實施例繪示出形成高電子移動率電晶體不同階段的剖面示意圖。 10 to 12 are schematic cross-sectional diagrams illustrating different stages of forming a high electron mobility transistor according to other embodiments.
第13至14圖係根據又一些實施例繪示出形成高電子移動率電晶體不同階段的剖面示意圖。 13 to 14 are schematic cross-sectional diagrams illustrating different stages of forming a high electron mobility transistor according to still other embodiments.
第15至16圖係根據再一些實施例所繪示之高電子移動率電晶體的剖面示意圖。 15 to 16 are schematic cross-sectional diagrams of high electron mobility transistors drawn according to still other embodiments.
第17圖係根據一些實施例繪示出形成高電子移動率電晶體的升溫曲線圖。 FIG. 17 is a graph showing the temperature rise curve for forming a high electron mobility transistor according to some embodiments.
以下公開許多不同的實施方法或是例子來實行本發明實施例之不同特徵,以下描述具體的元件及其排列的實施例以闡述本發明實施例。當然這些實施例僅用以例示,且不該以此限定本發明實施例的範圍。例如,在說明書中提到第一特徵形成於第二特徵之上,其包括第一特徵與第二特徵是直接接觸的實施例,另外也包括於第一特徵與第二特徵之間另外有其他特徵的實施例,亦即,第一特徵與第二特徵並非直接接觸。此外,在不同實施例中可能使用重複的標號或標示,這些重複僅為了簡單清楚地敘述本發明實施例,不代表所討論的不同實施例及/或結構之間有特定的關係。 Many different implementation methods or examples are disclosed below to implement the different features of the embodiments of the present invention. The following describes specific elements and their arrangement embodiments to illustrate the embodiments of the present invention. Of course, these embodiments are only for illustration, and should not be used to limit the scope of the embodiments of the present invention. For example, in the specification, it is mentioned that the first feature is formed on the second feature, which includes the embodiment in which the first feature and the second feature are in direct contact, and it also includes the embodiments between the first feature and the second feature. The embodiment of the feature, that is, the first feature and the second feature are not in direct contact. In addition, repeated reference numerals or labels may be used in different embodiments, and these repetitions are only used to briefly and clearly describe the embodiments of the present invention, and do not represent a specific relationship between the different embodiments and/or structures discussed.
此外,其中可能用到與空間相對用詞,例如「在...下方」、「下方」、「較低的」、「上方」、「較高的」及類似的用詞,這些空間相對用詞係為了便於描述圖示中一個(些)元件或特徵與另一個(些)元件或特徵之間的關係,這些空間相對用詞包括使用中或操作中的裝置之不同方位,以及圖式中所描述的方位。當裝置被轉向不同方位時(旋轉90度或其他方位),則其中所使用的空間相對形容詞也將依轉向後的方位來解釋。 In addition, terms that are relative to space may be used, such as "below", "below", "lower", "above", "higher" and similar terms. These spaces are relatively used In order to facilitate the description of the relationship between one element(s) or feature and another element(s) or feature in the illustration, the relative terms in space include the different orientations of the device in use or operation, as well as in the drawings. The orientation described. When the device is turned to different directions (rotated by 90 degrees or other directions), the spatially relative adjectives used therein will also be interpreted according to the turned position.
在此,「約」、「大約」、「大抵」之用語通常表示在一給定值或範圍的20%之內,較佳是10%之內,且更佳是5%之內,或3%之內,或2%之內,或1%之內,或0.5%之內。應注意的是,說明書中所提供的數量為大約的數量,亦即在沒有特定 說明「約」、「大約」、「大抵」的情況下,仍可隱含「約」、「大約」、「大抵」之含義。 Here, the terms "about", "approximately", and "approximately" usually mean within 20% of a given value or range, preferably within 10%, and more preferably within 5%, or 3 Within %, or within 2%, or within 1%, or within 0.5%. It should be noted that the quantity provided in the manual is an approximate quantity, that is, if there is no specific description of "about", "approximately" or "approximately", "about", "approximately", and "approximately" can still be implied. The meaning of "probably".
雖然所述的一些實施例中的步驟以特定順序進行,這些步驟亦可以其他合邏輯的順序進行。在不同實施例中,可替換或省略一些所述的步驟,亦可於本發明實施例所述的步驟之前、之中、及/或之後進行一些其他操作。本發明實施例中的高電子移動率電晶體可加入其他的特徵。在不同實施例中,可替換或省略一些特徵。 Although the steps in some of the described embodiments are performed in a specific order, these steps can also be performed in other logical orders. In different embodiments, some of the steps described may be replaced or omitted, and some other operations may be performed before, during, and/or after the steps described in the embodiments of the present invention. Other features can be added to the high electron mobility transistor in the embodiment of the present invention. In different embodiments, some features may be replaced or omitted.
本發明實施例提供一種高電子移動率電晶體(high electron mobility transistor,HEMT)的形成方法,在以高溫熱製程形成源極/汲極電極與通道層之間的歐姆接觸時,於元件上形成遮光層,以避免高溫光線透過透光三五族半導體及透光基板,而使基板下方的溫度感應器偵測異常,以致無法形成良好的歐姆接觸,因而無法降低阻值。 The embodiment of the present invention provides a method for forming a high electron mobility transistor (HEMT). When the ohmic contact between the source/drain electrode and the channel layer is formed by a high temperature thermal process, the device is The light-shielding layer is formed to prevent high-temperature light from passing through the light-transmitting Group III or 5 semiconductors and the light-transmitting substrate, and the temperature sensor under the substrate detects abnormality, so that a good ohmic contact cannot be formed, and the resistance cannot be reduced.
第1至9圖係根據一些實施例繪示出形成高電子移動率電晶體100不同階段的剖面示意圖。如第1圖所繪示,提供一基板102。在一些實施例中,此基板102可為Al2O3(藍寶石(sapphire))基板。此外,上述半導體基板亦可為元素半導體,包括矽(silicon)或鍺(germanium);化合物半導體,包括氮化鎵(gallium nitride,GaN)、碳化矽(silicon carbide)、砷化鎵(gallium arsenide)、磷化鎵(gallium phosphide)、磷化銦(indium phosphide)、砷化銦(indium arsenide)及/或銻化銦(indium antimonide);合金半導體,包括矽鍺合金(SiGe)、磷砷鎵合金(GaAsP)、砷鋁銦合金(AlInAs)、砷鋁鎵合金(AlGaAs)、砷銦鎵 合金(GaInAs)、磷銦鎵合金(GaInP)及/或磷砷銦鎵合金(GaInAsP)、或上述材料之組合。在一些實施例中,基板102可為單晶基板、多層基板(multi-layer substrate)、梯度基板(gradient substrate)、其他適當之基板、或上述之組合。此外,基板102也可以是絕緣層上覆半導體(semiconductor on insulator,SOI)基板,上述絕緣層覆半導體基板可包括底板、設置於底板上之埋藏氧化層、或設置於埋藏氧化層上之半導體層。在一些實施例中,基板102為透光基板。在本文中,透光基板102係指對波長300nm至2500nm的光源下穿透率在10%以上,例如穿透率10%至99%的基板102。 FIGS. 1-9 are schematic cross-sectional diagrams illustrating different stages of forming the high
接著,如第2圖所繪示,在基板102上形成緩衝層104。在一些實施例中,緩衝層104包括III-V族半導體,例如GaN。緩衝層104亦可包括AlGaN、AlN、GaAs、GaInP、AlGaAs、InP、InAlAs、InGaAs、其他適當的III-V族半導體材料、或上述之組合。在一些實施例中,可使用分子束磊晶法(molecular-beam epitaxy,MBE)、有機金屬氣相沉積法(metalorganic chemical vapor deposition,MOCVD)、氫化物氣相磊晶法(hydride vapor phase epitaxy,HVPE)、其他適當之方法、或上述之組合在基板102上形成緩衝層104。 Next, as shown in FIG. 2, a
接著,如第3圖所繪示,在緩衝層104上形成阻障層106,在一些實施例中,阻障層106包括與緩衝層104相異之材料。阻障層106可包括III-V族半導體,例如AlxGa1-xN,其中0<x<1。阻障層106亦可包括GaN、AlN、GaAs、GaInP、AlGaAs、InP、InAlAs、InGaAs、其他適當的III-V族材料、或上述之組合。在一些實施例中,可使用分子束磊晶法、有機金屬氣相沉積法、氫化物氣相磊晶法、其他適當之方法、或上述之組合在緩衝層104上形成阻障層106。
Next, as shown in FIG. 3, a
由於緩衝層104與阻障層106之材料相異,其能帶間隙(band gap)不同,緩衝層104與阻障層106的介面處形成異質接面(heterojunction)。異質接面處的能帶彎曲,導帶(conduction band)彎曲深處形成量子井(quantum well),將壓電效應(Piezoelectricity)所產生的電子約束於量子井中,因此在緩衝層104與阻障層106的介面處形成二維電子氣(two-dimensional electron gas,2DEG),進而形成導通電流。如第3圖所示,在緩衝層104與阻障層106的介面處形成通道區108,通道區108即為二維電子氣形成導通電流之處。
Since the materials of the
接著,如第4圖所繪示,在阻障層106上形成介電層110。在一些實施例中,介電層110為氧化物。在一些實施例中,介電層110包括SiO2、SiN3、SiON、Al2O3、MgO、Sc2O3、HfO2、HfSiO、HfSiON、HfTaO、HfTiO、HfZrO、LaO、ZrO、TiO2、ZnO2、ZrO2、AlSiN3、SiC、或Ta2O5、其他適當的介電材料、或上述之組合。在一些實施例中,可使用化學氣相沉積法(chemical vapor deposition,CVD)(如電漿強化化學氣相沉積(plasma enhanced CVD,PECVD)、高密度電漿化學氣相沉積(high density plasma CVD,HDPCVD))、原子層沉積製程(atomic layer deposition,ALD)、及/或其他合適技術沉積介電材料,以形成介電層110。在一些實施例中,可使用熱氧化製程,在含氧或含氮(例如含NO或N2O)的環境下熱成長介電層110。介電層110可降低後續形成閘極的漏電電流,提升閘極可承受的電壓範圍,進一步使通道阻值降低。 Next, as shown in FIG. 4, a
接著,如第5圖所繪示,形成源極/汲極電極112,其穿過介電層110及阻障層106,設置於緩衝層104上。在一些實施例中,源極/汲極電極112各自可包括Ti、Al、W、Au、Pd、其他適當之金屬材料、其合金、或上述之組合。在一些實施例中,可進行微影製程及蝕刻製程,於介電層110及阻障層106中形成源極/汲極電極開口,接著以化學氣相沉積法、物理氣相沉積法(例如蒸鍍或濺鍍)、電鍍、原子層沉積法、其他適當之方法、或上述之組合於介電層110上沉積導電材料並填入上述源極/汲極電極開口中,之後以蝕刻製程去除源極/汲極電極開口以外的導電材料,以形成源極/汲極電極112。 Next, as shown in FIG. 5, a source/
在一些實施例中,在形成源極/汲極電極開口後,填入導電材料以形成源極/汲極電極112之前,順應性地形成鈍化層內襯於源極/汲極電極112與介電層110及阻障層106之間(圖未示)。鈍化層可包括SiO2、SiN3、SiON、Al2O3、AlN、聚亞醯胺(polyimide,PI)、苯環丁烯(benzocyclobutene,BCB)、聚苯并噁唑(polybenzoxazole,PBO)、其他絕緣材料、或上述之組合。在一些實施例中,可使用有機金屬氣相沉積法、化學氣相沉積法、其他適當之方法、或上述之組合形成鈍化層。鈍化層可保護下方的膜層,並提供物理隔離及結構支撐。 In some embodiments, after forming the source/drain electrode openings, before filling conductive materials to form the source/
接著,如第6圖所繪示,形成遮光層114順應性地覆蓋於介電層110及源極電極/汲極電極112上。在一些實施例中,遮光層114包括TiN。遮光層114亦可包括Al、Ag、Cu、AlCu、 Pt、W、Ru、Ni、TaN、TiAlN、TiW、TiO、TiO2、其他阻光材料、或上述之組合。在一些實施例中,遮光層114可使用物理氣相沉積製程(例如蒸鍍法或濺鍍法)、原子層沉積製程、電鍍法、其他合適的製程、或上述之組合沉積遮光層材料。遮光層114可選用對於波長300nm至2500nm的光源下穿透率小於10%,例如0%至10%的材料。遮光層114的厚度可為100Å至2000Å,厚度將依選擇之材料光穿透特性而有所變動。遮光層114的厚度若太厚,則可能容易因懸突(overhang)而造成薄膜破裂或剝離,遮光層114的厚度若太薄,則可能遮光效果不足。 Next, as shown in FIG. 6, a
接著,如第7A圖所繪示,對源極電極/汲極電極112進行熱製程116。由於熱製程116的高溫,源極電極/汲極電極112中的金屬將擴散至通道區108,因而在源極電極/汲極電極112與通道區108之間的界面112i形成歐姆接觸,可降低源極電極/汲極電極112與通道區108之間界面112i的阻值。在一些實施例中,熱製程116使用紅外光光源,其波長介於700nm至2500nm。熱製程116之溫度介於500℃至1000℃,所持續時間介於10秒至120秒。若熱製程116的溫度過高或時間過長,則可能因高溫或長時間反應的副產物而導致元件特性劣化並形成高阻值的介面,若溫度過低或時間過短,則無法在源極電極/汲極電極112與通道區108之間的界面112i形成良好的歐姆接觸。 Then, as shown in FIG. 7A, a
第7B圖係根據一些實施例繪示出進行熱製程116時設備的剖面示意圖。在一些實施例中,在晶圓10上形成高電子移動率電晶體100,包括基板102及其上方的結構,而溫度感測器12位於晶圓10之下方。進行熱製程116時,光源16照射晶 圓10,由底部的溫度感測器12偵測晶圓10的溫度以決定光源16照射的時間長短。然而,當基板102為透光基板時,光源16可能穿透基板102,直接照射溫度感測器12,導致偵測得到的溫度升高,但此時晶圓10可能尚未吸收足夠的熱能,而使源極電極/汲極電極112與通道區108之間的界面112i無法形成歐姆接觸,導致無法有效降低阻值。 FIG. 7B is a schematic cross-sectional view of the device during the
如第7A及7B圖所示,由於在進行熱製程116前先於介電層110及源極電極/汲極電極112上形成遮光層114,熱製程116用以加熱的光源16較不易穿透基板102及其上方的結構,因此在晶圓10底部的溫度感測器較不易產生溫度偵測異常的情形,因此熱製程116可於源極電極/汲極電極112與通道區108之間的界面112i形成良好的歐姆接觸,進一步降低阻值。 As shown in FIGS. 7A and 7B, since the
值得注意的是,第7B圖繪示出晶圓10底部之溫度感測器12之數量、形狀、和配置僅為一範例,本發明實施例不以此為限。在本發明實施例中,晶圓10底部之溫度感測器12之可為任意數量、形狀、和配置,視製程需求而定。 It is worth noting that the number, shape, and configuration of the
接著,如第8圖所繪示,以蝕刻製程118去除遮光層114。在一些實施例中,蝕刻製程118可包括乾蝕刻、濕蝕刻、反應離子蝕刻(reactive ion etching,RIE)、及/或其他適合的製程。舉例來說,乾蝕刻製程可以含氧氣體、含氟氣體(例如CF4、SF6、CH2F2、CHF3、及/或C2F6)、含氯氣體(例如Cl2、CHCl3、CCl4、及/或BCl3)、含溴氣體(例如HBr及/或CHBR3)、含碘氣體、其他適合的氣體及/或電漿、及/或上述之組合實施。舉例來說,濕蝕刻製程可包括在稀氫氟酸(diluted hydrofluoric acid,DHF)、 氫氧化鉀(potassium hydroxide,KOH)溶液、氨水(ammonia)、含氫氟酸(hydrofluoric acid,HF)溶液、硝酸(nitric acid,HNO3)、及/或醋酸(acetic acid,CH3COOH)、或其他適合的濕蝕刻劑中蝕刻。在一些實施例中,蝕刻製程118完全去除遮光層114。殘留於源極電極/汲極電極112之間並接觸不同源極電極/汲極電極112的遮光層114可能引起不想要的短路。 Then, as shown in FIG. 8, the light-
接著,如第9圖所繪示,形成閘極電極120於阻障層106上。在一些實施例中,閘極電極120可包括多晶矽、金屬(例如鎢、鈦、鋁、銅、鉬、鎳、鉑、其相似物、或以上之組合)、金屬合金、金屬氮化物(例如氮化鎢、氮化鉬、氮化鈦、氮化鉭、其相似物、或以上之組合)、金屬矽化物(例如矽化鎢、矽化鈦、矽化鈷、矽化鎳、矽化鉑、矽化鉺、其相似物、或以上之組合)、金屬氧化物(氧化釕、氧化銦錫、其相似物、或以上之組合)、其他適用的導電材料、或上述之組合。在一些實施例中,可進行微影製程及蝕刻製程,以於介電層110中形成閘極開口,接著使用化學氣相沉積製程(例如低壓氣相沉積製程或電漿輔助化學氣相沉積製程)、物理氣相沉積製程(例如電阻加熱蒸鍍法、電子束蒸鍍法、或濺鍍法)、電鍍法、原子層沉積製程、其他合適的製程、或上述之組合於介電層110上沉積導電材料並填入上述閘極開口中,之後以蝕刻去除閘極開口以外的導電材料,以形成閘極電極120。 Next, as shown in FIG. 9, a gate electrode 120 is formed on the
如上所述,在進行熱製程之前,於高電子移動率電晶體上覆蓋遮光層,以避免熱製程的加熱光線穿透高電子移動率電晶體,造成溫度偵測異常的現象。熱製程正常加熱可在 源極電極/汲極電極與通道區之間的界面形成良好的歐姆接觸,降低接觸電阻阻值。 As mentioned above, before the thermal process, the high electron mobility transistor is covered with a light shielding layer to prevent the heating light of the thermal process from penetrating the high electron mobility transistor, which may cause abnormal temperature detection. The normal heating of the thermal process can form a good ohmic contact at the interface between the source electrode/drain electrode and the channel area, reducing the contact resistance.
第10至12圖繪示出本發明另一些實施例繪示出形成高電子移動率電晶體200不同階段的剖面示意圖。其中與前述實施例相同或相似的製程或元件將沿用相同的元件符號,其詳細內容將不再贅述。與前述實施例的差別在於,如第10圖所示,在形成遮光層114之前,形成蝕刻停止層224順應性地覆蓋於介電層110及源極電極/汲極電極112上。 FIGS. 10 to 12 show schematic cross-sectional views showing different stages of forming the high
在一些實施例中,蝕刻停止層224為氧化物。在一些實施例中,蝕刻停止層224包括SiO2、Si3N4、SiON、Al2O3、MgO、Sc2O3、HfO2、HfSiO、HfSiON、HfTaO、HfTiO、HfZrO、LaO、ZrO、TiO2、ZnO2、ZrO2、或Ta2O5、類似的材料、或上述之組合。在一些實施例中,可使用化學氣相沉積法(如電漿強化化學氣相沉積、高密度電漿化學氣相沉積)、原子層沉積製程、及/或其他合適技術沉積介電材料,以形成蝕刻停止層224。在一些實施例中,蝕刻停止層224的厚度可為100Å至2000Å。蝕刻停止層224的厚度若太厚,則可能因懸突(overhang)而造成孔洞或者應力過大造成薄膜破裂,蝕刻停止層224的厚度若太薄,則可能不足以使後續蝕刻製程停止於該層之上。 In some embodiments, the
接著,如第11圖所繪示,對源極電極/汲極電極112進行熱製程116。由於熱製程116的高溫,源極電極/汲極電極112中的金屬將擴散至通道區108,因而在源極電極/汲極電極112與通道區108之間的界面112i形成歐姆接觸。由於在進行熱製程116前先於介電層110及源極電極/汲極電極112上形成了遮光 層114,熱製程116用以加熱的光線較不易穿透高電子移動率電晶體100,因此較不易產生溫度偵測異常的情形,因此熱製程116可於源極電極/汲極電極112與通道區108之間的界面112i形成良好的歐姆接觸,進一步降低阻值。 Next, as shown in FIG. 11, a
接著,如第12圖所繪示,以蝕刻製程118去除遮光層114。在一些實施例中,蝕刻製程118去除遮光層114後,留下的蝕刻停止層224覆蓋源極電極/汲極電極112。因此,源極電極/汲極電極112的厚度可不因蝕刻製程118而改變,使得在蝕刻製程118後,源極電極/汲極電極112的厚度均勻。在一些實施例中,介電層110與蝕刻停止層224均為氧化物。在一些實施例中,蝕刻停止層224與介電層110在蝕刻製程118時的蝕刻速率遠小於遮光層114,例如蝕刻速率比為1:3,以避免蝕刻製程118時過度蝕刻源極電極/汲極電極112。在一些實施例中,蝕刻停止層224與介電層110在蝕刻製程118時的蝕刻速率不同,以避免蝕刻製程118時過度蝕刻介電層110。 Then, as shown in FIG. 12, the light-
在一些實施例中,在蝕刻製程118之後,可進一步以沉積製程或熱氧化製程順應性地覆蓋氧化物層於蝕刻停止層224之上(圖未示)。然而,即使在蝕刻停止層224為氧化物的情形之下,由於蝕刻停止層224經受熱製程116,而氧化物層並未經受熱製程116,蝕刻停止層224與氧化物層在後續蝕刻製程的蝕刻率亦不同,而可避免後續蝕刻製程過度蝕刻蝕刻停止層224。 In some embodiments, after the
在如第10至12圖所示的實施例中,在進行熱製程之前,於高電子移動率電晶體上覆蓋蝕刻停止層及遮光層,以 避免加熱光線穿透高電子移動率電晶體,造成溫度偵測異常的現象,熱製程正常加熱可在源極電極/汲極電極與通道區之間的界面形成良好的歐姆接觸,進一步降低接觸電阻。蝕刻停止層更可避免在移除遮光層時過度蝕刻下方的源極電極/汲極電極及介電層,而使源極電極/汲極電極厚度均勻。 In the embodiment shown in Figures 10 to 12, before the thermal process, the high electron mobility transistor is covered with an etching stop layer and a light shielding layer to prevent heating light from penetrating the high electron mobility transistor, causing The abnormal temperature detection phenomenon, the normal heating of the thermal process can form a good ohmic contact at the interface between the source electrode/drain electrode and the channel area, further reducing the contact resistance. The etching stop layer can also avoid excessive etching of the source electrode/drain electrode and the dielectric layer underneath when the light shielding layer is removed, so that the thickness of the source electrode/drain electrode is uniform.
第13至14圖繪示出本發明另一些實施例繪示出形成高電子移動率電晶體300不同階段的剖面示意圖。其中與前述實施例相同或相似的製程或元件將沿用相同的元件符號,其詳細內容將不再贅述。與前述實施例的差別在於,如第13圖所示,在進行熱製程116之後,以蝕刻製程318選擇性地去除遮光層114。在一些實施例中,以圖案化製程選擇性去除遮光層114。圖案化製程可包括光阻塗佈(例如旋轉塗佈)、軟烤(soft baking)、罩幕對準、曝光圖案、曝光後烘烤、光阻顯影、清洗及乾燥(例如硬烤(hard baking))、其他合適的技術、或上述之組合。蝕刻製程可包括乾蝕刻製程(例如反應離子蝕刻、非等向性電漿蝕刻)、濕蝕刻製程、或上述之組合。去除遮光層114後,殘餘的遮光層114分別包括覆蓋源極電極/汲極電極112兩側壁的遮光層114a及僅覆蓋於介電層110上的遮光層114b。 FIGS. 13 to 14 show schematic cross-sectional views showing different stages of forming the high
接著,如第14圖所示,形成閘極電極120於阻障層106上。在一些實施例中,殘餘的遮光層114a及114b並未接觸閘極電極120。若殘餘的遮光層114a及114b殘留於源極電極/汲極電極112與閘極電極120之間,並接觸不同的源極電極/汲極電極112與閘極電極120,則可能引起不想要的短路。遮光層114除了在熱製程116時作為遮蔽光線之外,殘餘的遮光層114b亦 可後續作為其他繞線用途。 Next, as shown in FIG. 14, a gate electrode 120 is formed on the
在如第13至14圖所示的實施例中,在進行熱製程之前,於高電子移動率電晶體上覆蓋遮光層,以避免加熱光線穿透高電子移動率電晶體,造成溫度偵測異常的現象,熱製程正常加熱可在源極電極/汲極電極與通道區之間的界面形成良好的歐姆接觸,降低接觸電阻。接著,選擇性去除遮光層,殘餘的部分遮光層可於後續作為其他繞線用途,節省製程成本及時間。 In the embodiment shown in Figures 13 to 14, before the thermal process, the high electron mobility transistor is covered with a light-shielding layer to prevent heating light from penetrating the high electron mobility transistor, causing abnormal temperature detection The phenomenon of normal heating in the thermal process can form a good ohmic contact at the interface between the source electrode/drain electrode and the channel area, reducing the contact resistance. Then, the light-shielding layer is selectively removed, and the remaining part of the light-shielding layer can be used for other winding purposes later, saving process cost and time.
第15至16圖係根據本發明再一些實施例繪示出形成高電子移動率電晶體400的剖面示意圖。其中與前述實施例相同或相似的製程或元件將沿用相同的元件符號,其詳細內容將不再贅述。與前述實施例的差別在於,前述的高電子移動率電晶體不須外加閘極電壓,高電子移動率電晶體便為導通狀態,亦即為空乏型(depletion mode,D-mode)高電子移動率電晶體。然而,如第15圖所示,在形成介電層110之前,形成能帶調整層426於阻障層106上,且位於後續形成的閘極電極120預定區之下方。能帶調整層426為P型摻雜三五族半導體,包括P型摻雜之GaN、AlGaN、AlN、GaAs、AlGaAs、InP、InAlAs、或InGaAs,其P型摻雜濃度介於1e17/cm3至1e20/cm3之間。在一些實施例中,可使用分子束磊晶法、有機金屬氣相沉積法、化學氣相沉積法、氫化物氣相磊晶法沉積P型摻雜三五族半導體,再經由例如微影製程與蝕刻製程,將之圖案化形成能帶調整層426。 FIGS. 15 to 16 are schematic cross-sectional diagrams illustrating the formation of a high
接著,如第15圖所示,於高電子移動率電晶體400上覆蓋遮光層114,接著進行熱製程116。由於熱製程116的高 溫,源極電極/汲極電極112中的金屬將擴散至通道區108,因而在源極電極/汲極電極112與通道區108之間的界面112i形成歐姆接觸。由於在進行熱製程116前先於介電層110及源極電極/汲極電極112上形成了遮光層114,熱製程116用以加熱的光線較不易穿透高電子移動率電晶體400,因此較不易產生溫度偵測異常的情形,因此熱製程116可於源極電極/汲極電極112與通道區108之間的界面112i形成良好的歐姆接觸,進一步降低阻值。 Next, as shown in FIG. 15, the
接著,如第16圖所示,去除遮光層114後,在能帶調整層426上形成閘極電極120,使兩者電性連接。由於能帶調整層426為P型摻雜三五族半導體,P型摻雜可提高能帶,因此緩衝層104與阻障層106的介面處量子井能量可高於費米能階,導致通道層108中可能無二維電子氣產生,因而可能無導通電流。上述實施例中,由於能帶調整層426可拉高能帶,未外加閘極電壓時,高電子移動率電晶體400可為截止狀態,亦即高電子移動率電晶體400可為增強型(enhancement mode,E-mode)高電子移動率電晶體。與空乏型(D-mode)高電子移動率電晶體相較之下,增強型(E-mode)高電子移動率電晶體較為安全,待機功耗(standby power dissipation)較低,且由於不須供給負偏壓,亦可降低電路複雜性以及製作成本。 Next, as shown in FIG. 16, after removing the
在如第15至16圖所示的實施例中,在進行熱製程之前,於高電子移動率電晶體上覆蓋遮光層,以避免加熱光源穿透高電子移動率電晶體,造成溫度偵測異常的現象,熱製程正常加熱可使源極電極/汲極電極與通道區之間的界面形成良 好的歐姆接觸,進一步降低接觸電阻。藉由在閘極電極下方形成能帶調整層調整能帶,形成未外加閘極電壓時即為截止狀態的增強型高電子移動率電晶體。 In the embodiment shown in Figures 15 to 16, before the thermal process, the high electron mobility transistor is covered with a light-shielding layer to prevent the heating light source from penetrating the high electron mobility transistor, causing abnormal temperature detection The normal heating of the thermal process can make the interface between the source electrode/drain electrode and the channel area form a good ohmic contact, further reducing the contact resistance. By forming an energy band adjustment layer under the gate electrode to adjust the energy band, an enhanced high electron mobility transistor is formed that is in an off state when no gate voltage is applied.
值得注意的是,前述高電子移動率電晶體100、200、300之實施例亦可適用如第15至16圖所示實施例,於閘極電極下方形成能帶調整層調整能帶,形成增強型高電子移動率電晶體。 It is worth noting that the aforementioned embodiments of high
第17圖係根據一些實施例繪示出形成高電子移動率電晶體的升溫曲線圖。實線數據表示進行熱製程116時並未使用遮光層114的升溫曲線。虛線數據表示進行熱製程116時使用了遮光層114的升溫曲線。 FIG. 17 is a graph showing the temperature rise curve for forming a high electron mobility transistor according to some embodiments. The solid line data indicates the heating curve of the
如第17圖所示,進行熱製程116時若未使用遮光層114,易造成溫度感應器偵測異常,所測得的溫度跳動而不穩定,使歐姆接觸形成失敗,無法降低阻值。相形之下,當使用遮光層114時,溫度穩定升高,因此,熱製程可正常加熱,在源極電極/汲極電極與通道區之間的界面可形成良好的歐姆接觸,進一步降低接觸電阻。 As shown in FIG. 17, if the light-
雖然在實施例中已經描述了與本技術的某些實施例相關的優點,其他實施例亦可具有這樣的優點。並非所有實施例必須具有上述優點才在本發明範圍之中。 Although the advantages related to certain embodiments of the present technology have been described in the embodiments, other embodiments may also have such advantages. Not all embodiments must have the above advantages to be within the scope of the present invention.
綜上所述,本發明實施例提供一種形成高電子移動率電晶體的方法,在進行熱製程以形成源極電極/汲極電極與通道區之間界面的歐姆接觸前,先於源極電極/汲極電極及介電層上形成遮光層,避免加熱的高溫光線穿透高電子移動率 電晶體,使得溫度偵測異常。如此一來,熱製程可正常加熱,在源極電極/汲極電極與通道區之間的界面形成良好的歐姆接觸,進一步降低接觸電阻。此外,可在形成遮光層前先形成蝕刻停止層,使源極電極/汲極電極厚度均勻。另外,若選擇性地去除遮光層,殘餘的遮光層將可用於後續繞線用途。此方法可應用於形成空乏型高電子移動率電晶體與增強型高電子移動率電晶體。 In summary, the embodiment of the present invention provides a method for forming a high electron mobility transistor. Before the thermal process is performed to form the ohmic contact at the interface between the source electrode/drain electrode and the channel region, the source electrode /A light-shielding layer is formed on the drain electrode and the dielectric layer to prevent the heated high temperature light from penetrating the high electron mobility transistor, causing abnormal temperature detection. In this way, the thermal process can be heated normally, and a good ohmic contact is formed at the interface between the source electrode/drain electrode and the channel region, which further reduces the contact resistance. In addition, an etching stop layer can be formed before the light shielding layer is formed to make the thickness of the source electrode/drain electrode uniform. In addition, if the light-shielding layer is selectively removed, the remaining light-shielding layer will be used for subsequent winding purposes. This method can be applied to form depletion high electron mobility transistors and enhanced high electron mobility transistors.
上述內容概述許多實施例的特徵,因此任何所屬技術領域中具有通常知識者,可更加理解本發明實施例之各面向。任何所屬技術領域中具有通常知識者,可能無困難地以本發明實施例為基礎,設計或修改其他製程及結構,以達到與本發明實施例相同的目的及/或得到相同的優點。任何所屬技術領域中具有通常知識者也應了解,在不脫離本發明實施例之精神和範圍內做不同改變、代替及修改,如此等效的創造並沒有超出本發明實施例的精神及範圍。 The above content summarizes the features of many embodiments, so anyone with ordinary knowledge in the technical field can better understand the aspects of the embodiments of the present invention. Anyone with ordinary knowledge in the technical field may design or modify other manufacturing processes and structures based on the embodiment of the present invention without difficulty to achieve the same purpose and/or obtain the same advantages as the embodiment of the present invention. Any person with ordinary knowledge in the technical field should also understand that various changes, substitutions and modifications can be made without departing from the spirit and scope of the embodiments of the present invention. Such equivalent creations do not exceed the spirit and scope of the embodiments of the present invention.
100‧‧‧高電子移動率電晶體 100‧‧‧High Electron Mobility Transistor
102‧‧‧基板 102‧‧‧Substrate
104‧‧‧緩衝層 104‧‧‧Buffer layer
106‧‧‧阻障層 106‧‧‧Barrier layer
108‧‧‧通道區 108‧‧‧Passage Area
110‧‧‧介電層 110‧‧‧Dielectric layer
112‧‧‧源極/汲極電極 112‧‧‧Source/Drain electrode
112i‧‧‧界面 112i‧‧‧Interface
114‧‧‧遮光層 114‧‧‧Shading layer
116‧‧‧熱製程 116‧‧‧Heat process
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JP4532574B2 (en) * | 2008-03-28 | 2010-08-25 | 古河電気工業株式会社 | Manufacturing method of semiconductor device |
US20120112202A1 (en) * | 2010-11-05 | 2012-05-10 | Samsung Electronics Co., Ltd. | E-Mode High Electron Mobility Transistors And Methods Of Manufacturing The Same |
EP2511949A1 (en) * | 2011-04-15 | 2012-10-17 | STMicroelectronics Srl | Method for manufacturing a HEMT transistor and corresponding HEMT transistor |
TW201244083A (en) * | 2011-03-04 | 2012-11-01 | Transphorm Inc | Electrode configurations for semiconductor devices |
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US20120112202A1 (en) * | 2010-11-05 | 2012-05-10 | Samsung Electronics Co., Ltd. | E-Mode High Electron Mobility Transistors And Methods Of Manufacturing The Same |
TW201244083A (en) * | 2011-03-04 | 2012-11-01 | Transphorm Inc | Electrode configurations for semiconductor devices |
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