TWI462286B - A epitaxial substrate for electronic components and a method for manufacturing the same - Google Patents

A epitaxial substrate for electronic components and a method for manufacturing the same Download PDF

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TWI462286B
TWI462286B TW099115374A TW99115374A TWI462286B TW I462286 B TWI462286 B TW I462286B TW 099115374 A TW099115374 A TW 099115374A TW 99115374 A TW99115374 A TW 99115374A TW I462286 B TWI462286 B TW I462286B
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TW201121039A (en
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生田哲也
清水成
柴田智彥
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同和電子科技股份有限公司
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電子元件用磊晶基板及其製造方法Epitaxial substrate for electronic component and method of manufacturing the same

本發明係有關電子元件用磊晶基板及其製造方法,特別是HEMT用電子元件用磊晶基板及其製造方法。The present invention relates to an epitaxial substrate for an electronic component and a method of manufacturing the same, and more particularly to an epitaxial substrate for an electronic component for HEMT and a method of manufacturing the same.

近年來,隨著IC用元件等之高速化,高電子遷移率電晶體(HEMT:High electron mobility transistor)被廣泛地用作高速之場效電晶體(FET:Field effect transistor)。該種場效型電晶體,例如圖1之示意圖所示般,在基板21上積層通道層22及電子供應層23,在該電子供應層23的表面配設源極(source electrode)24、汲極(drain electrode)25、及閘極(gate electrode)26而形成。在元件運作時,電子依照源極24、電子供應層23、通道層22、電子供應層23及汲極25的順序遷移,並以橫向作為電流導通方向,該橫向之電子遷移,係受到施加於閘極26之電壓所控制。在HEMT中,於帶隙相異之電子供應層23及通道層22的接合界面所產生之電子,與一般之半導體內相較,能高速遷移。In recent years, high electron mobility transistors (HEMTs) have been widely used as high-speed field effect transistors (FETs) in order to increase the speed of IC devices and the like. In the field effect type transistor, as shown in the schematic diagram of FIG. 1, a channel layer 22 and an electron supply layer 23 are laminated on a substrate 21, and a source electrode 24 is disposed on the surface of the electron supply layer 23. A drain electrode 25 and a gate electrode 26 are formed. When the device is in operation, the electrons migrate in the order of the source 24, the electron supply layer 23, the channel layer 22, the electron supply layer 23, and the drain 25, and the lateral direction is the current conduction direction, and the lateral electron transfer is applied to The voltage of the gate 26 is controlled. In the HEMT, electrons generated at the junction interface of the electron supply layer 23 and the channel layer 22 having different band gaps can migrate at a high speed as compared with a general semiconductor.

如上述,橫向之電子遷移,亦即電流,係藉由閘電壓而控制,然而,即使關閉閘電壓,電流一般並不會成為0。此種在閘電壓關閉時流動之電流稱為洩漏電流,若洩漏電流增加會使消耗電力增加,其結果會造成發熱等問題。上述洩漏電流一般被分成橫向洩漏電流與縱向洩漏電流,橫向洩漏電流係指,配置在電子供應層23側表面之2電極間(例如源極24與汲極25之間)流動之洩漏電流;縱向洩漏電流係指,在分別配置於電子供應層23側表面與基板21側表面之2電極間流動之洩漏電流。As described above, the lateral electron transfer, that is, the current, is controlled by the gate voltage, however, even if the gate voltage is turned off, the current generally does not become zero. Such a current flowing when the gate voltage is turned off is called a leakage current, and if the leakage current is increased, the power consumption is increased, and as a result, heat generation and the like are caused. The leakage current is generally divided into a lateral leakage current and a longitudinal leakage current, and the lateral leakage current refers to a leakage current flowing between two electrodes (for example, between the source 24 and the drain 25) disposed on the side surface of the electron supply layer 23; The leakage current refers to a leakage current that flows between the electrodes on the side surface of the electron supply layer 23 and the side surface of the substrate 21, respectively.

在專利文獻1中揭示有以下之技術:在基板上具備緩衝層、碳濃度遷移層、通道層、及電子供應層之HEMT中,以碳濃度由通道層朝緩衝層增加之方式形成,藉此降低在緩衝層及碳濃度遷移層中產生之橫向洩漏電流,並提升橫向耐壓。Patent Document 1 discloses a technique in which a HEMT including a buffer layer, a carbon concentration transition layer, a channel layer, and an electron supply layer on a substrate is formed such that a carbon concentration increases from a channel layer toward a buffer layer, whereby Reduce the lateral leakage current generated in the buffer layer and the carbon concentration migration layer, and increase the lateral withstand voltage.

又,在專利文獻2中揭示有以下之技術:在基板上具備超晶格緩衝層、通道層、及電子供應層之半導體元件中,以使超晶格緩衝層含碳之方式,來抑制半導體元件之橫向洩漏電流及提升橫向耐壓。Further, Patent Document 2 discloses a technique of suppressing a semiconductor in a semiconductor element including a superlattice buffer layer, a channel layer, and an electron supply layer on a substrate so that the superlattice buffer layer contains carbon. The lateral leakage current of the component and the lateral withstand voltage.

再者,在專利文獻3中揭示有以下之技術:在單晶基板上形成之第1Ⅲ族氮化物基底層,與在該第1Ⅲ族氮化物基底層上形成之第2Ⅲ族氮化物基底層之界面間,含有受體雜質,於該界面起至第2Ⅲ族氮化物基底層之厚度方向,使該受體雜質的濃度減少,藉此來抑制半導體元件之橫向洩漏電流。Further, Patent Document 3 discloses a technique of forming a first group III nitride underlayer formed on a single crystal substrate and a second group III nitride underlayer formed on the first group III nitride underlayer. The interface contains an acceptor impurity, and the interface is in the thickness direction of the second group III nitride underlayer, and the concentration of the acceptor impurity is reduced, thereby suppressing the lateral leakage current of the semiconductor element.

然而,在使HEMT以高頻運作時,除降低該洩漏電流外,亦須降低高頻信號施加時的損失。該種損失,當基板或其上之磊晶膜存在電荷時,係因為耗竭層(depletion layer)不能有效率地擴張,引起配置在基板表面之電極與電容性或電感性之相互作用而產生。However, when the HEMT is operated at a high frequency, in addition to reducing the leakage current, it is also necessary to reduce the loss when the high frequency signal is applied. Such a loss occurs when a charge is present on the substrate or the epitaxial film thereon because the depletion layer cannot be efficiently expanded, causing the interaction of the electrodes disposed on the surface of the substrate with capacitive or inductive properties.

又,在專利文獻4中揭示有以下之技術:提高Si單晶基板之比電阻來防止雜質混入,藉以減少載子,以抑制高頻區域之半導體電子元件的損失。Further, Patent Document 4 discloses a technique of increasing the specific resistance of a Si single crystal substrate to prevent impurities from being mixed, thereby reducing carriers to suppress loss of semiconductor electronic components in a high frequency region.

然而,在專利文獻1所載的發明中,在基板上生長Ⅲ族氮化物層之際,由於使用GaN系低溫緩衝層,因此,在基板使用Si之情形下會因為與Ga之反應而產生坑等穿孔缺陷,而有惡化縱向耐壓的問題。又,專利文獻2所載之發明,雖然可抑制超晶格緩衝層內之洩漏電流,但未能充份抑制在通道層與超晶格緩衝層界面之洩漏電流,結果成為導致縱向及橫向耐壓一併惡化之原因。再者,專利文獻3、4並未考慮縱向耐壓,對緩衝層之耐壓全然未予探究,因此,用在如Si基板之類的半導體基板時,無法確保縱向耐壓。However, in the invention described in Patent Document 1, when the group III nitride layer is grown on the substrate, since the GaN-based low-temperature buffer layer is used, pits are generated due to the reaction with Ga in the case where Si is used as the substrate. The perforation defect is a problem, and there is a problem that the longitudinal withstand voltage is deteriorated. Further, in the invention disclosed in Patent Document 2, although the leakage current in the superlattice buffer layer can be suppressed, the leakage current at the interface between the channel layer and the superlattice buffer layer is not sufficiently suppressed, resulting in resistance to longitudinal and lateral directions. The reason for the pressure to deteriorate. Further, Patent Documents 3 and 4 do not consider the longitudinal withstand voltage, and the withstand voltage of the buffer layer is not investigated at all. Therefore, when used in a semiconductor substrate such as a Si substrate, longitudinal withstand voltage cannot be ensured.

專利文獻1:日本特開2007-251144號公報Patent Document 1: Japanese Laid-Open Patent Publication No. 2007-251144

專利文獻2:日本特開2005-85852號公報Patent Document 2: Japanese Laid-Open Patent Publication No. 2005-85852

專利文獻3:日本特開2003-282598號公報Patent Document 3: Japanese Laid-Open Patent Publication No. 2003-282598

專利文獻4:日本特表2008-522447號公報Patent Document 4: Japanese Patent Publication No. 2008-522447

本發明之目的在於,提供能良好地兼顧橫向洩漏電流之降低及橫向耐壓特性,且能提升縱向耐壓之電子元件用磊晶基板,以及其製造方法。An object of the present invention is to provide an epitaxial substrate for an electronic component which can achieve both a reduction in lateral leakage current and a lateral withstand voltage characteristic and which can improve longitudinal withstand voltage, and a method for producing the same.

為達成上述目的,本發明之構成要旨如以下所述。In order to achieve the above object, the constitution of the present invention is as follows.

(1)一種電子元件用磊晶基板,其具備Si單晶基板、形成於該Si單晶基板上之作為絕緣層之緩衝層、及在該緩衝層上磊晶生長複數層之Ⅲ族氮化物層所形成之主積層體,並以橫向作為電流導通方向,其特徵在於:該緩衝層至少具有與該Si單晶基板連接之初期生長層、以及在該初期生長層上之由超晶格多層結構所構成之超晶格積層體;該初期生長層由AlN材料構成,且,該超晶格積層體係交互積層由Ba1 Alb1 Gac1 Ind1 N(0≦a1 ≦1,0≦b1 ≦1,0≦c1 ≦1,0≦d1 ≦1,a1 +b1 +c1 +d1 =1)材料所構成之第1層、以及由帶隙不同於該第1層之Ba2 Alb2 Gac2 Ind2 N(0≦a2 ≦1,0≦b2 ≦1,0≦c2 ≦1,0≦d2 ≦1,a2 +b2 +c2 +d2 =1)材料所構成之第2層而成;該超晶格積層體、或該主積層體之該緩衝層側之部分的至少一方,C濃度為1×1018 /cm3 以上。(1) An epitaxial substrate for an electronic component comprising: a Si single crystal substrate; a buffer layer as an insulating layer formed on the Si single crystal substrate; and a group III nitride epitaxially grown on the buffer layer a main laminate formed by a layer and having a lateral direction as a current conduction direction, wherein the buffer layer has at least an initial growth layer connected to the Si single crystal substrate, and a superlattice multilayer on the initial growth layer a superlattice laminate composed of a structure; the initial growth layer is composed of an AlN material, and the superlattice layer system is alternately layered by B a1 Al b1 Ga c1 In d1 N(0≦a 1 ≦1,0≦b 1 ≦1,0≦c 1 ≦1,0≦d 1 ≦1, a 1 +b 1 +c 1 +d 1 =1) the first layer of the material, and the band gap is different from the first layer B a2 Al b2 Ga c2 In d2 N(0≦a 2 ≦1,0≦b 2 ≦1,0≦c 2 ≦1,0≦d 2 ≦1, a 2 +b 2 +c 2 +d 2 =1) The second layer composed of the material; at least one of the superlattice laminate or the portion of the main laminate on the buffer layer side has a C concentration of 1 × 10 18 /cm 3 or more.

(2)如上述第1項之電子元件用磊晶基板,其中,該超晶格積層體及該主積層體之該緩衝層側部分之至少一方,C濃度均為1×1018 /cm3 以上。(2) The epitaxial substrate for an electronic component according to the above aspect, wherein at least one of the superlattice laminate and the buffer layer side portion of the main laminate has a C concentration of 1 × 10 18 /cm 3 the above.

(3)如上述第1或2項之電子元件用磊晶基板,其中,該第1層由AlN材料構成,該第2層由Alb2 Gac2 N(a2 =0,0≦b2 ≦0.5,0.5≦c2 <1,d2 =0)材料構成。(3) The epitaxial substrate for an electronic component according to the above item 1, wherein the first layer is made of an AlN material, and the second layer is made of Al b2 Ga c2 N (a 2 =0, 0 ≦ b 2 ≦ 0.5, 0.5 ≦ c 2 <1, d 2 =0) material composition.

(4)如上述第1、2、或3項之電子元件用磊晶基板,其中,該Si單晶基板之比電阻為1000Ω‧cm以上,由該初期生長層起至0.1μm深度之Ⅲ族原子之合計最大濃度為1×1016 /cm3 以下,且,在由該初期生長層起0.3μm深度位置之Ⅲ族原子之合計濃度為1×1015 /cm3 以下。(4) The epitaxial substrate for an electronic component according to the above 1, 2, or 3, wherein the Si single crystal substrate has a specific resistance of 1000 Ω ‧ cm or more, and the III group from the initial growth layer to a depth of 0.1 μm The total concentration of the atoms is 1 × 10 16 /cm 3 or less, and the total concentration of the group III atoms at a depth of 0.3 μm from the initial growth layer is 1 × 10 15 /cm 3 or less.

(5)一種電子元件用磊晶基板之製造方法,其依序在Si單晶基板上形成作為絕緣層之緩衝層、及在該緩衝層上磊晶生長複數層之Ⅲ族氮化物層而成之主積層體,並以橫向作為電流導通方向,其特徵在於:該緩衝層至少具有與該Si單晶基板連接之初期生長層、以及在該初期生長層上之由超晶格多層結構所構成之超晶格積層體;該初期生長層由AlN材料構成,且,該超晶格積層體係交互積層由Ba1 Alb1 Gac1 Ind1 N(0≦a1 ≦1,0≦b1 ≦1,0≦c1 ≦1,0≦d1 ≦1,a1 +b1 +c1 +d1 =1)材料所構成之第1層、以及由帶隙不同於該第1層之Ba2 Alb2 Gac2 Ind2 N(0≦a2 ≦1,0≦b2 ≦1,0≦c2 ≦1,0≦d2 ≦1,a2 +b2 +c2 +d2 =1)材料所構成之第2層而成;該超晶格積層體、或該主積層體之該緩衝層側之部分的至少一方,C濃度為1×1018 /cm3 以上。(5) A method for producing an epitaxial substrate for an electronic component, comprising sequentially forming a buffer layer as an insulating layer on a Si single crystal substrate, and epitaxially growing a plurality of group III nitride layers on the buffer layer The main laminate body has a lateral direction as a current conduction direction, and the buffer layer has at least an initial growth layer connected to the Si single crystal substrate and a superlattice multilayer structure on the initial growth layer. a superlattice laminate; the initial growth layer is composed of an AlN material, and the superlattice laminated system is alternately layered by B a1 Al b1 Ga c1 In d1 N(0≦a 1 ≦1,0≦b 1 ≦1 , 0≦c 1 ≦1,0≦d 1 ≦1, a 1 +b 1 +c 1 +d 1 =1) the first layer composed of the material, and the B a2 different from the first layer by the band gap Al b2 Ga c2 In d2 N(0≦a 2 ≦1,0≦b 2 ≦1,0≦c 2 ≦1,0≦d 2 ≦1, a 2 +b 2 +c 2 +d 2 =1) The second layer formed of the material is formed; and at least one of the superlattice laminate or the portion of the main laminate on the buffer layer side has a C concentration of 1 × 10 18 /cm 3 or more.

(6)如上述第5項之電子元件用磊晶基板之製造方法,其中,該超晶格積層體及該主積層體之該緩衝層側部分之至少一方,C濃度均為1×1018 /cm3 以上。(6) The method for producing an epitaxial substrate for an electronic component according to the item 5, wherein at least one of the superlattice laminate and the buffer layer side portion of the main laminate has a C concentration of 1 × 10 18 /cm 3 or more.

(7)如上述第5或6項之電子元件用磊晶基板之製造方法,其中,該Si單晶基板係形成為比電阻為1000Ω‧cm以上,由該初期生長層起至0.1μm深度之Ⅲ族原子之合計最大濃度為1×1016 /cm3 以下,且,在由該初期生長層起0.3μm深度位置之Ⅲ族原子之合計濃度為1×1015 /cm3 以下。(7) The method for producing an epitaxial substrate for an electronic component according to the fifth or sixth aspect, wherein the Si single crystal substrate is formed to have a specific resistance of 1000 Ω ‧ cm or more, and from the initial growth layer to a depth of 0.1 μm The total concentration of the group III atoms is 1 × 10 16 /cm 3 or less, and the total concentration of the group III atoms at a depth of 0.3 μm from the initial growth layer is 1 × 10 15 /cm 3 or less.

本發明之電子元件用磊晶基板,具備:緩衝層及既定之主積層體,該緩衝層含有由AlN材料構成之初期生長層及既定之超晶格積層體;其等超晶格積層體、或主積層體之緩衝層側部分之至少一方,具有1×1018 /cm3 以上的C濃度,藉此,不僅能良好地兼顧橫向洩漏電流之降低及橫向耐壓特性,亦能提升縱向耐壓。An epitaxial substrate for an electronic component according to the present invention includes: a buffer layer and a predetermined main laminate; the buffer layer includes an initial growth layer made of an AlN material and a predetermined superlattice laminate; and a superlattice laminate, Or at least one of the buffer layer side portions of the main laminate has a C concentration of 1 × 10 18 /cm 3 or more, whereby not only the lateral leakage current reduction and the lateral withstand voltage characteristics but also the longitudinal resistance can be improved. Pressure.

又,本發明可製得之電子元件用磊晶基板,其具有緩衝層及既定之主積層體,該緩衝層含有由AlN材料構成之初期生長層及既定之超晶格積層體;其等超晶格積層體、或主積層體之緩衝層側部分之至少一方,具有1×1018 /cm3 以上的C濃度,藉此,不僅能良好地兼顧橫向洩漏電流之降低及橫向耐壓特性,亦能提升縱向耐壓。Moreover, the epitaxial substrate for an electronic component which can be obtained by the present invention has a buffer layer and a predetermined main laminate, the buffer layer comprising an initial growth layer composed of an AlN material and a predetermined superlattice laminate; At least one of the lattice layer body or the buffer layer side portion of the main laminate has a C concentration of 1 × 10 18 /cm 3 or more, whereby not only the lateral leakage current reduction but also the lateral withstand voltage characteristics can be satisfactorily balanced. It can also increase the longitudinal withstand voltage.

再者,本發明之電子元件用磊晶基板,Si單晶基板具有1000Ω‧cm以上的比電阻,由初期生長層起至0.1μm深度之Ⅲ族原子之合計最大濃度設在1×1016 /cm3 以下,且,由初期生長層起0.3μm深度位置之Ⅲ族原子的合計濃度在1×1015 /cm3 以下,藉此方式,除了上述效果之外,亦能降低高頻運作時的損失。Further, in the epitaxial substrate for an electronic component of the present invention, the Si single crystal substrate has a specific resistance of 1000 Ω ‧ or more, and the total concentration of the group III atoms from the initial growth layer to a depth of 0.1 μm is set at 1 × 10 16 / In the case of cm 3 or less, the total concentration of the group III atoms at the depth of 0.3 μm from the initial growth layer is 1 × 10 15 /cm 3 or less, and in addition to the above effects, the high frequency operation can be reduced. loss.

又,本發明,藉由將Si單晶基板形成為比電阻在1000Ω‧cm以上,由初期生長層起至0.1μm深度之Ⅲ族原子之合計最大濃度設在1×1016 /cm3 以下,且由初期生長層起0.3μm深度位置之Ⅲ族原子的合計濃度在1×1015 /cm3 以下,可製得除了上述效果之外,亦能降低高頻運作時之損失的電子元件用磊晶基板。Further, in the present invention, when the Si single crystal substrate is formed to have a specific resistance of 1000 Ω ‧ cm or more, the total concentration of the group III atoms from the initial growth layer to the depth of 0.1 μm is set to be 1 × 10 16 /cm 3 or less. Further, the total concentration of the group III atoms at a depth of 0.3 μm from the initial growth layer is 1 × 10 15 /cm 3 or less, and the electronic component can be reduced in addition to the above effects. Crystal substrate.

繼而,邊參照圖式邊說明本發明之電子元件用磊晶基板之實施形態。圖2係本發明之電子元件用磊晶基板之截面構造之示意圖。再者,為說明方便起見,圖2之厚度方向畫得較為誇張。Next, an embodiment of the epitaxial substrate for an electronic component of the present invention will be described with reference to the drawings. 2 is a schematic view showing a cross-sectional structure of an epitaxial substrate for an electronic component of the present invention. Moreover, for convenience of description, the thickness direction of FIG. 2 is more exaggerated.

如圖2所示,本發明之電子元件用磊晶基板1,係以橫向作為電流導通方向之電子元件用磊晶基板,其具備Si單晶基板2、於Si單晶基板2上形成之作為絕緣層的緩衝層3、及在緩衝層3上磊晶生長複數層之Ⅲ族氮化物層而形成的主積層體4,其特徵在於:緩衝層3至少具有與Si單晶基板2連接之初期生長層5、以及在初期生長層5上之由超晶格多層結構構成之超晶格積層體6:初期生長層5由AlN材料所構成,且,超晶格積層體6係交互積層由Ba1 Alb1 Gac1 Ind1 N(0≦a1 ≦1,0≦b1 ≦1,0≦c1 ≦1,0≦d1 ≦1,a1 +b1 +c1 +d1 =1)所構成之第1層6a,以及由帶隙不同於該第1層6a之Ba2 Alb2 Gac2 Ind2 N(0≦a2 ≦1,0≦b2 ≦1,0≦c2 ≦1,0≦d2 ≦1,a2 +b2 +c2 +d2 =1)材料所構成之第2層6b而成;超晶格積層體6或主積層體4之緩衝層3側之部分4'之至少一方,C濃度為1×1018 /cm3 以上,由於具有上述構成,不僅能良好地兼顧橫向洩漏電流的降低及橫向耐壓特性,亦能提升縱向耐壓。As shown in FIG. 2, the epitaxial substrate 1 for an electronic component of the present invention is an epitaxial substrate for an electronic component having a lateral direction as a current conduction direction, and the Si single crystal substrate 2 is formed on the Si single crystal substrate 2. The buffer layer 3 of the insulating layer and the main layer body 4 formed by epitaxially growing the group III nitride layer of the plurality of layers on the buffer layer 3 are characterized in that the buffer layer 3 has at least an initial connection with the Si single crystal substrate 2 The growth layer 5 and the superlattice laminate 6 composed of a superlattice multilayer structure on the initial growth layer 5: the initial growth layer 5 is composed of an AlN material, and the superlattice laminate 6 is an interactive laminate by B A1 Al b1 Ga c1 In d1 N(0≦a 1 ≦1,0≦b 1 ≦1,0≦c 1 ≦1,0≦d 1 ≦1, a 1 +b 1 +c 1 +d 1 =1 The first layer 6a is composed of B a2 Al b2 Ga c2 In d2 N (0≦a 2 ≦1,0≦b 2 ≦1,0≦c 2 ≦ different from the first layer 6a) 1,0≦d 2 ≦1, a 2 +b 2 +c 2 +d 2 =1) The second layer 6b composed of the material; the superlattice laminate 6 or the buffer layer 3 side of the main laminate 4 the portion 4 'of at least one, C is a concentration of 1 × 10 18 / cm 3 or more, since Components described above, not only a good balance between reducing the lateral leakage current and breakdown voltage characteristic of a lateral, longitudinal also enhance the breakdown voltage.

Si單晶基板2之面方位並無特別限定,(111)、(100)、(110)面等皆可使用,但為了使Ⅲ族氮化物之(0001)面在表面平坦性良好之情況下生長,使用(111)面較佳。又,p型或n型之傳導型皆可。至於Si單晶基板2之導電性,由10000Ω‧cm以上之高絕緣性的高比電阻基板,到低至0.001Ω‧cm左右之低比電阻基板,能依用途而妥為應用。該種Si單晶基板2之製造方法,可使用CZ法、FZ法等各種方法,在基板表面磊晶生長Si、SiC等亦可。又,亦可使用在基板表面形成由氧化膜、氮化膜、碳化膜構成之薄膜者。The plane orientation of the Si single crystal substrate 2 is not particularly limited, and any of the (111), (100), and (110) planes may be used, but in order to make the (0001) plane of the group III nitride have good surface flatness. For growth, it is preferred to use the (111) face. Also, a p-type or an n-type conduction type is acceptable. As for the conductivity of the Si single crystal substrate 2, a high specific resistance substrate having a high insulating property of 10000 Ω ‧ cm or more can be suitably applied depending on the application to a low specific resistance substrate as low as 0.001 Ω ‧ cm. In the method for producing the Si single crystal substrate 2, Si, SiC, or the like may be epitaxially grown on the surface of the substrate by various methods such as a CZ method or an FZ method. Further, a film formed of an oxide film, a nitride film, or a carbonized film may be formed on the surface of the substrate.

特別是,在製作高頻特性優異之電子元件用磊晶基板之際,以使用具有1000Ω‧cm以上比電阻之基板為佳。該種基板,較佳係以易於達到Si結晶之高純度化之FZ法來製作。In particular, when an epitaxial substrate for an electronic component having excellent high-frequency characteristics is produced, a substrate having a specific resistance of 1000 Ω‧cm or more is preferably used. Such a substrate is preferably produced by an FZ method which is easy to achieve high purity of Si crystal.

又,藉由以AlN材料來形成初期生長層5,可抑制與Si單晶基板2之反應,提升縱向耐壓。其目的在於,以含有Ga、In之Ⅲ族氮化物材料來形成初期生長層5時,抑制Ga、In與基板之Si反應而產生缺陷,而在磊晶膜內引起穿孔缺陷以致降低縱向耐壓之情形。然而,此處所謂之AlN材料,亦可含有1%以下之微量雜質(無論有意為之,或是無心造成),例如,可含有上述Ga、In乃至Si、H、O、C、B、Mg、As、P等雜質。Further, by forming the initial growth layer 5 with an AlN material, the reaction with the Si single crystal substrate 2 can be suppressed, and the longitudinal withstand voltage can be improved. When the initial growth layer 5 is formed of a group III nitride material containing Ga or In, it is suppressed that Ga and In react with Si of the substrate to cause defects, and perforation defects are caused in the epitaxial film to lower the longitudinal withstand voltage. The situation. However, the AlN material referred to herein may also contain less than 1% of trace impurities (whether intentional or unintentional), for example, may contain the above Ga, In or Si, H, O, C, B, Mg. , As, P and other impurities.

特別是,在製作高頻特性優異之電子元件用磊晶基板之際,較佳係使Si單晶基板具有1000Ω‧cm以上的比電阻,由初期生長層起至0.1μm深度之Ⅲ族原子之合計最大濃度在1×1016 /cm3 以下,且,由初期生長層起0.3μm深度位置之Ⅲ族原子的合計濃度在1×1015 /cm3 以下。藉由使用高比電阻之基板,能有效擴展耗竭層,可抑制於基板表面形成之載子與存在於基板之電荷之電容性或電感性的結合而造成之電子元件在高頻運作時的損失。特別是,Si單晶基板之比電阻值在5000Ω‧cm以上時較佳,高頻運作時之損失傾向飽和。又,由於Ⅲ族原子在Si單晶基板內係作為p型雜質而發揮功能,因此,以設成上述濃度範圍之方式,可抑制於基板表面形成之電極與該p型雜質之電容性或電感性之結合而造成之電子元件在高頻運作時的損失。再者,雜質濃度係使用SIMS分析來測定。在此情形,係從內面側(基板側)邊進行蝕刻,邊測定深度方向之雜質濃度分布。此際,Al之雜質濃度宜小於Ga之雜質濃度。原因在於,Al之活化能較Ga小,較易產生p型載子。In particular, when an epitaxial substrate for an electronic component having excellent high-frequency characteristics is produced, it is preferable that the Si single crystal substrate has a specific resistance of 1000 Ω·cm or more, and a group III atom having a depth of 0.1 μm from the initial growth layer. The total concentration is 1 × 10 16 /cm 3 or less, and the total concentration of the group III atoms at a depth of 0.3 μm from the initial growth layer is 1 × 10 15 /cm 3 or less. By using a substrate with a high specific resistance, the depletion layer can be effectively expanded, and the loss of the electronic component during high frequency operation caused by the combination of the carrier formed on the surface of the substrate and the capacitive or inductive charge of the charge existing on the substrate can be suppressed. . In particular, the specific resistance of the Si single crystal substrate is preferably 5,000 Ω ‧ cm or more, and the loss at the time of high frequency operation tends to be saturated. Further, since the group III atom functions as a p-type impurity in the Si single crystal substrate, it is possible to suppress the capacitance or electric power of the electrode formed on the surface of the substrate and the p-type impurity so as to have the above-described concentration range. The loss of electronic components caused by the combination of sensibility and high frequency operation. Further, the impurity concentration was measured using SIMS analysis. In this case, the impurity concentration distribution in the depth direction was measured while etching from the inner surface side (substrate side). At this time, the impurity concentration of Al is preferably smaller than the impurity concentration of Ga. The reason is that the activation energy of Al is smaller than that of Ga, and it is easier to generate a p-type carrier.

如所示,以製作高頻特性優異之電子元件用磊晶基板為目的,在磊晶生長時,為防止雜質混入Si單晶基板,所著重的是:As shown in the figure, in order to produce an epitaxial substrate for an electronic component having excellent high-frequency characteristics, in order to prevent impurities from being mixed into the Si single crystal substrate during epitaxial growth, it is important to:

(1)降低成膜溫度,以及(2)抑制初期生長層AlN之島狀生長,促進二維生長。為實現上述第2點,宜抑制Si多晶基板表面之過度氮化,使氮化膜厚小於1nm,或是不予氮化。原因基於以下推測:若過度氮化Si單晶基板表面,在基板最表面之原料擴散速度變快,AlN呈島狀生長的結果,因初期生長時之基板外露部分造成Al、Ga等Ⅲ族原料的擴散。(1) lowering the film formation temperature, and (2) suppressing the island-like growth of the initial growth layer AlN to promote two-dimensional growth. In order to achieve the second point described above, it is preferable to suppress excessive nitridation on the surface of the Si polycrystalline substrate to make the nitride film thickness less than 1 nm or not to be nitrided. The reason is based on the following assumptions: if the surface of the Si single crystal substrate is excessively nitrided, the diffusion rate of the raw material on the outermost surface of the substrate becomes faster, and AlN is grown as an island. As a result, the exposed portion of the substrate during initial growth causes a group III material such as Al or Ga. The spread.

將超晶格積層體6之C濃度設定在1×1018 /cm3 以上,可藉此提升縱向耐壓,將主積層體4在緩衝層5側之部分4'的C濃度設為1×1018 /cm3 以上,可藉此提升橫向耐壓,且能抑制橫向洩漏電流。再者,為了防止因過度增加雜質導致產生坑,宜使其等之C濃度未滿1×1020 /cm3 。至於其他之雜質量雖無特別限定,但最好能抑制雜質等級較淺之施體雜質(Si,O,Ge)之混入為佳,儘管如此,若含有其程度可補償上述施體等級之碳,則能容許某種程度的混入。再者,雜質濃度係使用SIMS分析,由表面側邊進行蝕刻邊測定深度方向之雜質濃度分布。When the C concentration of the superlattice laminate 6 is set to 1 × 10 18 /cm 3 or more, the longitudinal withstand voltage can be increased, and the C concentration of the portion 4' of the main laminate 4 on the buffer layer 5 side is set to 1 × 10 18 /cm 3 or more, which can increase the lateral withstand voltage and suppress the lateral leakage current. Further, in order to prevent pits from being generated by excessively increasing impurities, it is preferable to make the C concentration of the liquid or the like less than 1 × 10 20 /cm 3 . As for the other impurity qualities, although it is not particularly limited, it is preferable to suppress the mixing of the donor impurities (Si, O, Ge) having a shallow impurity level, but if it is contained, the carbon of the above-mentioned donor grade can be compensated. , can tolerate some degree of mixing. Further, the impurity concentration was analyzed by SIMS, and the impurity concentration distribution in the depth direction was measured by etching from the side of the surface.

此處所謂「以橫向作為電流導通方向」,如圖1所示,係指電流係由源極24朝汲極25,主要於積層體之寬度方向流動,其與例如以一對電極夾住半導體之構造,電流主要在縱向(即積層體之厚度方向)流動,具有不同的意涵。Here, "the lateral direction is the current conduction direction", as shown in FIG. 1, means that the current flows from the source 24 to the drain 25, mainly in the width direction of the laminated body, and sandwiches the semiconductor with, for example, a pair of electrodes. In the configuration, the current flows mainly in the longitudinal direction (ie, the thickness direction of the laminated body), and has different meanings.

又,此處所謂交互積層超晶格積層體,意指以周期性地含有第1層6a與第2層6b之方式進行積層。亦可含有第1層6a與第2層6b以外之層(例如組成遷移層)。Here, the term "interlayer laminated superlattice laminate" means that the first layer 6a and the second layer 6b are periodically laminated. It is also possible to include a layer other than the first layer 6a and the second layer 6b (for example, a composition migration layer).

主積層體4之緩衝層3側之部分4'的C濃度,宜較超晶格積層體6之C濃度為高。在部分4'中,由於受到緩衝層3與主積層體4之晶格常數差異的影響,可見差排朝橫向或斜向彎曲的現象,形成洩漏電流容易流經的路徑。因此,部分4'較緩衝層3易有洩漏電流流經,為了抑制該洩漏電流,較佳係設成如上述之C濃度。又,若是該主積層體4之緩衝層3側的部分4'之厚度未滿0.1μm,由於有連C濃度較少的部分亦存在明顯差排彎曲之虞,因此,設定成0.1μm以上的厚度較佳。至於部分4'之厚度上限,由耐壓之提升與降低洩漏電流之觀點而言,並無特別指定,可由抑制基板之彎曲、裂縫之觀點而妥為設定。此際,僅是改變部分4'之Ⅲ族元素的組成,或是改變從部分4'起通道層4a之與緩衝層位於相反側之部分之C濃度或III族元素組成時,可採使之急速變化的方式,亦可採連續性變化之方式。The C concentration of the portion 4' on the buffer layer 3 side of the main laminate 4 is preferably higher than the C concentration of the superlattice laminate 6. In the portion 4', due to the influence of the difference in lattice constant between the buffer layer 3 and the main laminate 4, it is seen that the difference is curved in the lateral direction or obliquely, forming a path through which leakage current easily flows. Therefore, the portion 4' is more likely to have a leakage current flowing through the buffer layer 3. In order to suppress the leakage current, it is preferable to set the concentration to C as described above. In addition, if the thickness of the portion 4' on the side of the buffer layer 3 of the main laminate 4 is less than 0.1 μm, the portion having a small C concentration may have a sharp difference in bending, and therefore, it is set to be 0.1 μm or more. The thickness is preferred. The upper limit of the thickness of the portion 4' is not particularly specified from the viewpoint of improvement in withstand voltage and reduction in leakage current, and can be appropriately set from the viewpoint of suppressing bending and cracking of the substrate. In this case, only the composition of the group III element of the portion 4' is changed, or the C concentration or the composition of the group III element of the portion of the channel layer 4a opposite to the buffer layer from the portion 4' is changed. The way of rapid change can also take the form of continuous change.

構成超晶格積層體6之第1層6a較佳為由AlN材料構成,第2層6b較佳為由Alb2 Gac2 N(a2 =0,0<b2 ≦0.5,0.5≦c2 <1,d2 =0)材料構成。由於第1層6a與第2層6b之帶隙差提高縱向耐壓,故較佳為盡可能地加大組成差而盡可能取較大帶隙差。以Ⅲ族氮化物半導體材料來製作混晶時,由於帶隙差最大者乃是AlN(6.2eV)與GaN(3.5eV),因此較佳為以AlGaN材料來製作超晶格構造。至於組成差的下限,若是小於0.5,因為由Si單晶與Ⅲ族氮化物之晶格常數差帶來之應力鬆弛變得不充分而產生裂縫,因此組成差設為0.5以上較佳。又,就組成差的上限而言,雖說較大的組成差較理想,但由於AlGaN層本身的絕緣化進展而提升耐壓,因此較佳為以帶隙較小的第2層至少含有Al之方式,使Al之組成差小於1。原因在於,至少含有Al時,能有效率地取入C。若超晶格之對數至少在40對以上時,因為可降低耐壓的不一致性故較佳。The first layer 6a constituting the superlattice laminate 6 is preferably made of an AlN material, and the second layer 6b is preferably made of Al b2 Ga c2 N (a 2 =0, 0 < b 2 ≦ 0.5, 0.5 ≦ c 2 <1, d 2 =0) material composition. Since the band gap difference between the first layer 6a and the second layer 6b increases the longitudinal withstand voltage, it is preferable to increase the composition difference as much as possible and take a larger band gap as much as possible. When a mixed crystal is produced from a group III nitride semiconductor material, since the difference in band gap is the largest among AlN (6.2 eV) and GaN (3.5 eV), it is preferable to form a superlattice structure using an AlGaN material. When the lower limit of the composition difference is less than 0.5, since the stress relaxation due to the difference in lattice constant between the Si single crystal and the group III nitride is insufficient, cracks are formed, so that the composition difference is preferably 0.5 or more. Further, in terms of the upper limit of the composition difference, although a large composition difference is preferable, since the withstand voltage of the AlGaN layer itself progresses to increase the withstand voltage, it is preferable that the second layer having a small band gap contains at least Al. In a way, the composition difference of Al is less than 1. The reason is that C can be taken in efficiently when at least Al is contained. If the logarithm of the superlattice is at least 40 pairs or more, it is preferable because the pressure inconsistency can be reduced.

關於各層之厚度,若由耐壓提升之觀點來看,帶隙較大之第1層6a之厚度,較佳係能抑制通道電流程度之厚度以上,且為不產生裂縫之膜厚以下。例如,在使用AlN之情形時,設定成2~10nm較佳。關於第2層6b之厚度,係由抑制裂縫、控制彎曲的觀點來適當地設定,但為了要有效發揮超晶格積層構造的應變緩衝效果以抑制裂縫的產生,較佳為帶隙較小之層之厚度較帶隙較大之層為厚,並設在40nm以下。又,在超晶格積層體內不一定須要皆以相同膜厚、相同組成來進行積層。With respect to the thickness of each layer, the thickness of the first layer 6a having a large band gap is preferably greater than or equal to the thickness of the channel current, and is not less than the film thickness at which cracks are generated. For example, in the case of using AlN, it is preferably set to 2 to 10 nm. The thickness of the second layer 6b is appropriately set from the viewpoint of suppressing cracks and controlling bending. However, in order to effectively exhibit the strain buffering effect of the superlattice laminate structure to suppress the occurrence of cracks, it is preferable that the band gap is small. The thickness of the layer is thicker than the layer with a larger band gap and is set below 40 nm. Further, it is not always necessary to laminate the layers in the superlattice layer with the same film thickness and the same composition.

電子元件用磊晶基板1,用於HEMT較佳。圖2所示之磊晶基板1之主積層體4,可具有由Ba3 Alb3 Gac3 Ind3 N(0≦a3 ≦1,0≦b3 ≦1,0≦c3 ≦1,0≦d3 ≦1,a3 +b3 +c3 +d3 =1)所構成之通道層4a,以及由帶隙大於通道層4a之Ba4 Alb4 Gac4 Ind4 N(0≦a4 ≦1,0≦b4 ≦1,0≦c4 ≦1,0≦d4 ≦1,a4 +b4 +c4 +d4 =1)材料所構成之電子供應層4b。此際,兩層皆可由單一或複數之組成來構成。特別是,為了要避免合金散射、降低電流導通部分之比電阻,通道層4a之至少與電子供應層4b連接的部分以GaN材料為佳。The epitaxial substrate 1 for electronic components is preferably used for HEMT. The main laminate 4 of the epitaxial substrate 1 shown in FIG. 2 may have B a3 Al b3 Ga c3 In d3 N(0≦a 3 ≦1, 0≦b 3 ≦1, 0≦c 3 ≦1, 0通道d 3 ≦1, a 3 +b 3 +c 3 +d 3 =1) the channel layer 4a formed, and the B a4 Al b4 Ga c4 In d4 N (0≦a 4) with a band gap larger than the channel layer 4a ≦1,0≦b 4 ≦1,0≦c 4 ≦1,0≦d 4 ≦1, a 4 +b 4 +c 4 +d 4 =1) The electron supply layer 4b composed of the material. In this case, both layers can be composed of a single or a complex number. In particular, in order to avoid scattering of the alloy and lower the specific resistance of the current conducting portion, at least the portion of the channel layer 4a to be connected to the electron supply layer 4b is preferably a GaN material.

通道層4a之與緩衝層位於相反側的部分,較佳為C濃度低,設定成4×1016 /cm3 以下為佳。原因係由於該部分相當於電子元件之電流導通部分,因此不含會妨礙導電性、或產生電流崩塌(current collapse)的雜質較理想。又,為了抑制來自n型雜質之殘留載子造成的洩漏電流,以存在1×1015 /cm3 以上為佳。The portion of the channel layer 4a on the opposite side to the buffer layer preferably has a low C concentration, and is preferably set to 4 × 10 16 /cm 3 or less. The reason is that since this portion corresponds to the current conducting portion of the electronic component, it is preferable that impurities are not contained which may impede conductivity or cause current collapse. Further, in order to suppress leakage current caused by residual carriers from the n-type impurities, it is preferable that 1 × 10 15 /cm 3 or more is present.

接著,邊參照圖式邊說明本發明之電子元件用磊晶基板之製造方法的實施形態。Next, an embodiment of a method of manufacturing an epitaxial substrate for an electronic component according to the present invention will be described with reference to the drawings.

如圖2所示,係在Si單晶基板2上,依序形成作為絕緣層之緩衝層3、在緩衝層3上磊晶生長複數層Ⅲ族氮化物層之HEMT構造的主積層體4,並以橫向作為電流導通方向之電子元件用磊晶基板1的製造方法,其特徵在於:緩衝層3具有與Si單晶基板2連接之初期生長層5以及在初期生長層5上之由超晶格多層結構構成的超晶格積層體6;初期生長層5係由AlN材料所構成,且,超晶格積層體6係交互積層由Ba1 Alb1 Gac1 Ind1 N(0≦a1 ≦1,0≦b1 ≦1,0≦c1 ≦1,0≦d1 ≦1,a1 +b1 +c1 +d1 =1)所構成之第1層6a、以及由帶隙不同於第1層6a之Ba2 Alb2 Gac2 Ind2 N(0≦a2 ≦1,0≦b2 ≦1,0≦c2 ≦1,0≦d2 ≦1,a2 +b2 +c2 +d2 =1)材料所構成之第2層6b而成;超晶格積層體6、或主積層體4之緩衝層3側的部分4'之至少一方,形成為C濃度在1×1018 /cm3 以上,由於具有上述構成,故能製造良好地兼顧縱向耐壓特性及橫向耐壓特性、且能降低橫向洩漏電流之電子元件用磊晶基板,。As shown in FIG. 2, on the Si single crystal substrate 2, a buffer layer 3 as an insulating layer, and a main layer body 4 of a HEMT structure in which a plurality of layers of a group III nitride layer are epitaxially grown on the buffer layer 3 are sequentially formed, A method for manufacturing an epitaxial substrate 1 for an electronic component having a lateral direction as a current conduction direction, characterized in that the buffer layer 3 has an initial growth layer 5 connected to the Si single crystal substrate 2 and a supercrystal on the initial growth layer 5 a superlattice laminate 6 composed of a multi-layer structure; the initial growth layer 5 is composed of an AlN material, and the superlattice laminate 6 is an alternating layer of B a1 Al b1 Ga c1 In d1 N (0≦a 1 ≦ 1,0≦b 1 ≦1,0≦c 1 ≦1,0≦d 1 ≦1, a 1 +b 1 +c 1 +d 1 =1) The first layer 6a is formed, and the band gap is different B a2 Al b2 Ga c2 In d2 N in the first layer 6a (0≦a 2 ≦1,0≦b 2 ≦1,0≦c 2 ≦1,0≦d 2 ≦1, a 2 +b 2 + c 2 +d 2 =1) the second layer 6b composed of the material; at least one of the superlattice laminate 6 or the portion 4' of the buffer layer 3 side of the main laminate 4 is formed to have a C concentration of 1 × 10 18 / cm 3 or more, since the above-described configuration, it can be manufactured with good longitudinal balance Lateral breakdown voltage characteristics and breakdown voltage characteristics, and can reduce the lateral leakage current of the electronic component by epitaxial substrate.

使用CVD法來生長時,添加於超晶格積層體6與主積層體4之緩衝層3側之部分4'的C,可使用以下所示之數種方法來添加。When growing by the CVD method, C added to the portion 4' of the superlattice laminate 6 and the buffer layer 3 side of the main laminate 4 can be added by several methods as described below.

第1種方法:將含有C之原料氣體,在Ⅲ族氮化物生長中另行添加。例如甲烷、乙烷、乙烯、乙炔、苯、環戊烷等。The first method: a raw material gas containing C is separately added in the growth of the group III nitride. For example, methane, ethane, ethylene, acetylene, benzene, cyclopentane, and the like.

第2種方法:將有機金屬中的甲基、乙基等,藉由生長Ⅲ族氮化物之生長條件混入磊晶生長層。適當地設定生長溫度、生長壓力、生長速度、生長時的氨流量、氫流量、氮流量等,以抑制有機金屬的分解,藉此可調整添加至磊晶生長層的C濃度。The second method: a methyl group, an ethyl group or the like in the organic metal is mixed into the epitaxial growth layer by growing the growth conditions of the group III nitride. The growth temperature, the growth pressure, the growth rate, the ammonia flow rate during growth, the hydrogen flow rate, the nitrogen flow rate, and the like are appropriately set to suppress the decomposition of the organic metal, whereby the C concentration added to the epitaxial growth layer can be adjusted.

再者,在本申請中,超晶格積層體6的C濃度,係利用SIMS在去除超晶格積層體6之1/2厚度後之處之測定值。主積層體4之緩衝層3側之部分4'的C濃度,係利用SIMS在去除上述部分4'之1/2厚度後之處之測定值。Further, in the present application, the C concentration of the superlattice laminate 6 is measured by the SIMS after removing the thickness of the superlattice laminate 6. The C concentration of the portion 4' on the buffer layer 3 side of the main laminate 4 is measured by SIMS after removing the thickness of 1/2 of the above portion 4'.

再者,圖1及圖2係表示代表性的實施形態之例,本發明並不侷限於此等實施形態。例如,可在各層之間插入不會對本發明之效果造成不良影響的中間層,或是插入其他超晶格層,或是在組成中加上梯度。又,亦可在Si單晶的表面形成氮化膜、碳化膜、Al層等。1 and 2 show examples of representative embodiments, and the present invention is not limited to these embodiments. For example, an intermediate layer that does not adversely affect the effects of the present invention may be interposed between the layers, or other superlattice layers may be inserted, or a gradient may be added to the composition. Further, a nitride film, a carbonized film, an Al layer, or the like may be formed on the surface of the Si single crystal.

(實驗例1)(Experimental Example 1)

在比電阻分別為1×10-1 Ω‧cm、1×10Ω‧cm、2×103 Ω‧cm、及1×104 Ω‧cm的600μm厚的(111)面4吋Si單晶基板上,生長初期生長層(AlN材料:厚度100nm)及超晶格積層體(AlN:膜厚4nm與Al0.15 Ga0.85 N:膜厚25nm,合計85層)以形成緩衝層,在該超晶格積層體上磊晶生長通道層(GaN材料:厚1.5μm)及電子供應層(Al0.25 Ga0.75 材料:厚20nm)而形成HEMT構造的主積層體,得到試料1~4。改變超晶格積層體的C濃度,主積層體之緩衝層側部分的C濃度之任一結果均在1.5~2.0×1018 /cm3 的範圍。又,通道層之電子供應層側的部分,C濃度在0.8~3.5×1016 /cm3 的範圍。各層之生長溫度及壓力示於表1。透過調整表中P1 來調整C濃度,透過降低成膜壓力來增加C濃度。使用MOCVD法來作為生長方法,以TMA(三甲基鋁)、TMG(三甲基鎵)來作為Ⅲ族原料,以氨作為V族原料,使用氫及氮氣作為載子氣體。此處所謂成膜溫度,係指在生長中使用輻射溫度計測定之基板本身的溫度。再者,C濃度之SIMS測定,係由磊晶層側開始進行蝕刻,以Cameca製之測定裝置,使用Cs- 作為離子源,以8keV的離子能量來進行。600 μm thick (111) face 4 吋 Si single crystal substrate with specific resistance of 1×10 -1 Ω··cm, 1×10 Ω·cm, 2×10 3 Ω··cm, and 1×10 4 Ω·cm Upper growth layer (AlN material: thickness: 100 nm) and superlattice laminate (AlN: film thickness: 4 nm and Al 0.15 Ga 0.85 N: film thickness: 25 nm, total of 85 layers) to form a buffer layer in the superlattice The epitaxial growth channel layer (GaN material: 1.5 μm thick) and the electron supply layer (Al 0.25 Ga 0.75 material: thickness: 20 nm) were formed on the laminate to form a main laminate of the HEMT structure, and samples 1 to 4 were obtained. The C concentration of the superlattice laminate is changed, and any of the C concentrations of the buffer layer side portion of the main laminate is in the range of 1.5 to 2.0 × 10 18 /cm 3 . Further, the portion of the channel layer on the electron supply layer side has a C concentration in the range of 0.8 to 3.5 × 10 16 /cm 3 . The growth temperatures and pressures of the respective layers are shown in Table 1. The C concentration is adjusted by adjusting P 1 in the table, and the C concentration is increased by decreasing the film forming pressure. The MOCVD method was used as a growth method, and TMA (trimethylaluminum) and TMG (trimethylgallium) were used as the group III raw materials, ammonia was used as the group V raw material, and hydrogen and nitrogen were used as the carrier gas. The film formation temperature herein refers to the temperature of the substrate itself measured by using a radiation thermometer during growth. Furthermore, the C concentration of the SIMS measurement, the system begins by etching the epitaxial layer side to the measuring apparatus manufactured by Cameca, using Cs - as an ion source, the ion energy to 8keV.

(實驗例2)(Experimental Example 2)

以在700℃生長之GaN材料(厚度:20nm)形成初期生長層,各層之生長溫度、壓力以表2所示之條件來進行,除此之外則以與實驗例1之試料2相同的方法來製作試料5。An initial growth layer was formed of a GaN material (thickness: 20 nm) grown at 700 ° C, and the growth temperature and pressure of each layer were carried out under the conditions shown in Table 2, except that the same method as that of the sample 2 of Experimental Example 1 was carried out. To make sample 5.

圖3(a)、圖3(b)及圖3(c)中,表示試料2及試料5之橫向耐壓、橫向洩漏電流及縱向耐壓的測定結果。測定以下述方式進行。3(a), 3(b), and 3(c) show the measurement results of the lateral withstand voltage, the lateral leakage current, and the longitudinal withstand voltage of the sample 2 and the sample 5. The measurement was carried out in the following manner.

縱向:在基板表面形成由80μmΦ構成之Ti/Al積層構造之歐姆電極,對歐姆電極外側以50nm的厚度進行蝕刻之後,將基板內面接地於金屬板,對電壓測定流經兩電極間之電流值。Longitudinal: an ohmic electrode having a Ti/Al laminated structure composed of 80 μm Φ is formed on the surface of the substrate, and the outer surface of the ohmic electrode is etched to a thickness of 50 nm, and then the inner surface of the substrate is grounded to a metal plate, and the voltage is measured to flow between the electrodes. value.

橫向:以離開各邊10μm距離之方式,配置形成了由200μm□(四角)構成之Ti/Al積層構造之歐姆電極,對該歐姆電極周圍以150nm厚度進行蝕刻後,對電壓測定流經兩電極間的電流值。此際,為了要抑制空氣中的放電,以絕緣油使兩電極間絕緣。又,為了消除洩漏電流對基板內面的影響,在基板下配置有絕緣板。Lateral direction: an ohmic electrode having a Ti/Al laminated structure composed of 200 μm □ (four corners) was disposed so as to be separated by a distance of 10 μm from each side, and after etching the thickness of the ohmic electrode at a thickness of 150 nm, the voltage was measured and passed through the two electrodes. Current value between. In this case, in order to suppress the discharge in the air, the electrodes are insulated by insulating oil. Further, in order to eliminate the influence of the leakage current on the inner surface of the substrate, an insulating plate is disposed under the substrate.

本實驗例中,縱向耐壓的定義為:將縱向電流值以上述電極面積換算為每單位面積之值達到10-4 A/cm2 時之電壓值;對橫向耐壓的定義為:將橫向電流值換算成上述電極之每單邊長之值達到10-4 A/cm時之電壓值;對橫向洩漏電流之定義為:橫向在100V時之電流值。In the experimental example, the longitudinal withstand voltage is defined as a voltage value obtained by converting the longitudinal current value into the above-mentioned electrode area to a value of 10 -4 A/cm 2 per unit area; the lateral withstand voltage is defined as: The current value is converted into a voltage value when the value of each side of the above electrode reaches 10 -4 A/cm; the lateral leakage current is defined as a current value at a lateral direction of 100V.

超晶格積層體6之C濃度,係利用SIMS,對於將超晶格積層體6之去除1/2厚度之處進行測而得。主積層體4之緩衝層3側的部分4'的C濃度,係利用SIMS,對於該部分4'之去除1/2厚度之處進行測定而得。The C concentration of the superlattice laminate 6 was measured by using SIMS to remove the 1/2 thickness of the superlattice laminate 6. The C concentration of the portion 4' on the buffer layer 3 side of the main laminate 4 was measured by SIMS and the thickness of the portion 4' was removed by 1/2.

改變超晶格積層體之C濃度的結果,可確認橫向耐壓、橫向洩漏電流皆是幾乎沒有變化,相對於此,試料2的縱向耐壓,在超晶格積層體的C濃度超過1×1018 /cm3 後,則特別急遽上升。又,此現象在參照試料5後亦可確認得知,係以初期生長層作為AlN時之固有現象。又,對於試料1、3、及4,可獲得與試料2相同的結果。As a result of changing the C concentration of the superlattice laminate, it was confirmed that the lateral withstand voltage and the lateral leakage current were hardly changed. On the other hand, the longitudinal withstand voltage of the sample 2 exceeded the C concentration of the superlattice laminate by more than 1×. After 10 18 /cm 3 , it is particularly eager to rise. Moreover, this phenomenon was confirmed after referring to the sample 5, and it was an inherent phenomenon when the initial growth layer was used as AlN. Further, with respect to the samples 1, 3, and 4, the same results as those of the sample 2 were obtained.

由以上之實驗例1及2得知,將超晶格積層體之C濃度、或主積層體之緩衝層側部分之C濃度之至少一方設為1×1018 /cm3 以上,藉此可有效地強化縱向耐壓。According to the above Experimental Examples 1 and 2, at least one of the C concentration of the superlattice laminate or the C concentration of the buffer layer side portion of the main laminate is 1 × 10 18 /cm 3 or more. Effectively strengthen the longitudinal withstand voltage.

(實驗例3)(Experimental Example 3)

將超晶格積層體之生長壓力設為10kPa,改變主積層體之緩衝層側的部分之C濃度,各層之生長溫度及壓力以表3所示的條件來進行,除此之外,則是以與實驗例1之試料1~4相同的方法來製作試料6~9。透過調整表中P2 來調整C濃度,透過降低成膜壓力來增加C濃度。超晶格積層體之C濃度之任一結果均在1.5~2.5×1018 /cm3 的範圍。The growth pressure of the superlattice laminate was set to 10 kPa, and the C concentration of the portion on the buffer layer side of the main laminate was changed, and the growth temperature and pressure of each layer were carried out under the conditions shown in Table 3, except that Samples 6 to 9 were prepared in the same manner as Samples 1 to 4 of Experimental Example 1. The C concentration is adjusted by adjusting P 2 in the table, and the C concentration is increased by decreasing the film forming pressure. Any of the C concentrations of the superlattice laminates is in the range of 1.5 to 2.5 × 10 18 /cm 3 .

圖4(a)、圖4(b)、及圖4(c),表示試料6之橫向耐壓、橫向洩漏電流、及縱向耐壓的測定結果。改變主積層體的C濃度的結果是,可確認橫向耐壓、橫向洩漏電流幾乎沒有變化,相對於此,試料6的縱向耐壓則是,當主積層體之緩衝層側部分之C濃度超過1×1018 /cm3 時,則特別急遽上升。又,與實驗例1相同地,針對所使用之Si單晶基板比電阻相異之試料7~9,未確認與圖4(a)~圖4(c)所示結果有大的差異。4(a), 4(b), and 4(c) show the measurement results of the lateral withstand voltage, the lateral leakage current, and the longitudinal withstand voltage of the sample 6. As a result of changing the C concentration of the main laminate, it was confirmed that the lateral withstand voltage and the lateral leakage current hardly changed. On the other hand, the longitudinal withstand voltage of the sample 6 was such that the C concentration of the buffer layer side portion of the main laminate exceeded When 1 × 10 18 /cm 3 , it is particularly sharply rising. Further, in the same manner as in Experimental Example 1, the samples 7 to 9 having different specific resistances to the Si single crystal substrate used were not significantly different from the results shown in FIGS. 4(a) to 4(c).

實驗例1~3中,可以確認,為了提升縱向耐壓,將超晶格積層體及通道層之緩衝層側之C濃度設在既定值以上,藉此可提升縱向耐壓。在之後的實驗例4中,對於上述緩衝層C濃度,係設成在實驗例1~3經確認為較佳之既定值以上,嘗試高頻特性的改善。In the first to third examples, it was confirmed that the C-concentration on the buffer layer side of the superlattice laminate and the channel layer was set to a predetermined value or more in order to increase the longitudinal withstand voltage, whereby the longitudinal withstand voltage can be increased. In the following Experimental Example 4, the buffer layer C concentration was determined to be better than the predetermined values confirmed in Experimental Examples 1 to 3, and the improvement of the high-frequency characteristics was attempted.

(實驗例4)(Experimental Example 4)

在比電阻6×103 Ω‧cm之600μm厚之(111)面4吋Si單晶基板上,邊抑制初期氮化層的形成,邊使初期生長層(AlN材料:厚100nm)及超晶格積層體(AlN:膜厚4nm與Al0.15 Ga0.85 N:膜厚25nm,合計85層)生長以形成緩衝層,在該超晶格積層體上以表4之生長壓力、生長溫度條件,磊晶生長通道層(GaN材料:厚1.5μm)及電子供應層(Al0.25 Ga0.75 N材料:厚20nm),形成HEMT構造之主積層體而得到試料10。超晶格積層體之C濃度為2.0×1018 /cm3 ,主積層體之緩衝層側之0.2μm厚的部分之C濃度為3.0×1018 /cm3 。又,通道層之電子供應層之部分的C濃度為1×1016 /cm3On the (111)-face 4吋 Si single crystal substrate having a specific resistance of 6 × 10 3 Ω·cm and a thickness of 6 × 10 3 Ω·cm, the initial growth layer (AlN material: 100 nm thick) and supercrystal were formed while suppressing the formation of the initial nitride layer. A laminate layer (AlN: film thickness: 4 nm and Al 0.15 Ga 0.85 N: film thickness: 25 nm, total of 85 layers) was grown to form a buffer layer, and the growth pressure and growth temperature conditions of Table 4 were observed on the superlattice laminate. A crystal growth channel layer (GaN material: 1.5 μm thick) and an electron supply layer (Al 0.25 Ga 0.75 N material: 20 nm thick) were formed to form a main laminate of a HEMT structure to obtain a sample 10. The C concentration of the superlattice laminate was 2.0 × 10 18 /cm 3 , and the C concentration of the 0.2 μm thick portion on the buffer layer side of the main laminate was 3.0 × 10 18 /cm 3 . Further, the C concentration of the portion of the electron supply layer of the channel layer was 1 × 10 16 /cm 3 .

以SIMS來觀察Si單晶基板內之雜質時,如圖5(a)所示,無法確認Al、Ga以外之Ⅲ族元素之雜質,Al、Ga均在1×1016 /cm3 以下,存在1×1015 /cm3 以上之區域,係由Si單晶與初期生長層之界面起之0.2μm以內的區域。以TEM來確認Si單晶基板與初期生長層之界面,未發現有1nm以上厚度之SiNx膜的存在。又,已確認由Si單晶基板與初期生長層之界面起0.2μm以內之區域內,平均而言Al濃度較Ga濃度為低。再者,Al、Ga之SIMS測定,係由Si單晶側開始進行蝕刻,以Cameca製之測定裝置,使用O2 + 作為離子源,以3keV之離子能量來進行。When the impurities in the Si single crystal substrate are observed by SIMS, as shown in Fig. 5 (a), impurities of the group III elements other than Al and Ga cannot be confirmed, and both Al and Ga are present at 1 × 10 16 /cm 3 or less. A region of 1 × 10 15 /cm 3 or more is a region within 0.2 μm from the interface between the Si single crystal and the initial growth layer. The interface between the Si single crystal substrate and the initial growth layer was confirmed by TEM, and the presence of a SiNx film having a thickness of 1 nm or more was not observed. Further, it has been confirmed that the Al concentration is lower than the Ga concentration in a region within 0.2 μm from the interface between the Si single crystal substrate and the initial growth layer. Further, the SIMS measurement of Al and Ga was carried out by etching from the side of the Si single crystal, and was carried out by a measuring device manufactured by Cameca using O 2 + as an ion source at an ion energy of 3 keV.

又,對於本基板使用水銀探針(MSI electronic製)及阻抗分析儀(HP4284A)來進行CV測定的結果,如圖5(b)所示,確認耗竭層換算膜厚擴展至8μm左右。CV測定時之交流成分之頻率及振幅分別為100kHz、10mV。再者,為求方便,Si單晶與初期生長層之界面位置,在SIMS測定中,係Si濃度在1/5以下之位置往基板側位移0.05μm之位置。其原因在於避免SIMS測定時之蝕刻粗化,結果造成Si單晶與磊晶生長層混合外露而導致Ⅲ族元素外觀上的增加。In addition, as a result of performing CV measurement on the substrate using a mercury probe (manufactured by MSI Electronic Co., Ltd.) and an impedance analyzer (HP4284A), as shown in FIG. 5(b), it was confirmed that the film thickness of the depletion layer was expanded to about 8 μm. The frequency and amplitude of the AC component at the time of CV measurement were 100 kHz and 10 mV, respectively. Further, for the sake of convenience, the position of the interface between the Si single crystal and the initial growth layer was shifted to the substrate side by 0.05 μm at a position where the Si concentration was 1/5 or less in the SIMS measurement. The reason for this is to avoid etching roughening in the measurement of SIMS, and as a result, the Si single crystal and the epitaxial growth layer are mixed and exposed to cause an increase in the appearance of the group III element.

又,將所使用之4吋Si單晶基板之電阻率設成2×103 Ω‧cm、8×103 Ω‧cm、12×103 Ω‧cm,對於除此之外以相同於試料10之方法而製得之試料11、12、13亦進行同樣的試驗。這2個試驗之任一者亦與上述相同地,以SIMS觀察Si單晶基板內之雜質的結果,未確認Al、Ga以外的Ⅲ族元素,Al、Ga均在1×1016 /cm3 以下,存在1×1015 /cm3 以上之區域,係從Si單晶與初期生長層之界面起之0.2μm以下的區域。以TEM來確認Si單晶基板與初期生長層之界面,未能確認1nm以上厚度之SiNx膜的存在。又,由Si單晶基板與初期生長層之界面起之0.2μm以下的區域,亦可確認平均而言Al濃度較Ga濃度為低。又,確認耗竭層換算膜厚分別擴展至6μm、8μm、8μm左右。Further, the resistivity of the 4吋 Si single crystal substrate used was set to 2 × 10 3 Ω ‧ cm, 8 × 10 3 Ω ‧ cm, 12 × 10 3 Ω ‧ cm, and the same as the sample The same test was also carried out on the samples 11, 12, and 13 prepared by the method of 10. In the same manner as described above, the impurities in the Si single crystal substrate were observed by SIMS, and the group III elements other than Al and Ga were not confirmed, and both Al and Ga were 1 × 10 16 /cm 3 or less. The region of 1 × 10 15 /cm 3 or more is a region of 0.2 μm or less from the interface between the Si single crystal and the initial growth layer. The interface between the Si single crystal substrate and the initial growth layer was confirmed by TEM, and the presence of a SiNx film having a thickness of 1 nm or more was not confirmed. Further, in the region of 0.2 μm or less from the interface between the Si single crystal substrate and the initial growth layer, it was confirmed that the Al concentration was lower than the Ga concentration on average. Further, it was confirmed that the film thickness of the depletion layer was expanded to about 6 μm, 8 μm, and 8 μm, respectively.

(實驗例5)(Experimental Example 5)

在比電阻5×103 Ω‧cm之600μm厚之(111)面4吋Si單晶基板上,在初期生長層開始生長之前,相對於作為載子氣體之氫氣,僅使含有10%氨氣之氣體在1050℃下流動5分鐘,刻意形成初期氮化層,除此之外則以相同於試料2之方式製作試料14。On a (111)-face 4吋 Si single crystal substrate having a specific resistance of 5 × 10 3 Ω·cm and a thickness of 5 × 10 3 Ω·cm, only 10% of ammonia gas is contained with respect to hydrogen as a carrier gas before the initial growth layer starts to grow. The gas was flowed at 1050 ° C for 5 minutes to form an initial nitride layer, and the sample 14 was prepared in the same manner as the sample 2 except for the sample.

以SIMS來觀察Si單晶基板內之雜質的結果,如圖6(a)所示,雖然Al、Ga均在1×1016 /cm3 以下,但Al或Ga存在1×1015 /cm3 以上之區域,則有1μm以上。以TEM來確認Si單晶基板與初期生長層之界面的結果,確認SiNx膜存在1.5nm左右。又,確認Al濃度較Ga濃度為高。又,對本基板進行使用水銀探針之CV測定的結果,如圖6(b)所示,確認耗竭層換算膜厚只擴展至2μm左右。As a result of observing the impurities in the Si single crystal substrate by SIMS, as shown in Fig. 6(a), although Al and Ga are both 1 × 10 16 /cm 3 or less, Al or Ga is present at 1 × 10 15 /cm 3 . The above area is 1 μm or more. As a result of confirming the interface between the Si single crystal substrate and the initial growth layer by TEM, it was confirmed that the SiNx film was present at about 1.5 nm. Further, it was confirmed that the Al concentration was higher than the Ga concentration. In addition, as a result of CV measurement using a mercury probe on the substrate, as shown in FIG. 6(b), it was confirmed that the thickness of the depletion layer was expanded to only about 2 μm.

(實驗例6)(Experimental Example 6)

以表5所示之條件,使初期生長層至通道層之生長溫度上升,除此之外則以相同於試料10之方法來製作試料15。The sample 15 was prepared in the same manner as the sample 10 except that the growth temperature of the initial growth layer to the channel layer was raised under the conditions shown in Table 5.

以SIMS來觀察Si單晶基板內之雜質的結果,如圖7(a)所示,Ga的濃度,存在1×1016 /cm3 以上的部分,存在1×1015 /cm3 以上之區域在0.3μm以下。以TEM來確認Si單晶基板與初期生長層之界面,未能確認1nm以上厚度之SiNx膜的存在。又,亦確認Al濃度較Ga濃度為低。又,如圖7(b)所示,對本基板進行使用水銀探針之CV測定的結果,確認耗竭層換算膜厚僅擴展至2μm左右。As a result of observing the impurities in the Si single crystal substrate by SIMS, as shown in Fig. 7(a), the concentration of Ga is 1 × 10 16 /cm 3 or more, and the region of 1 × 10 15 /cm 3 or more exists. Below 0.3 μm. The interface between the Si single crystal substrate and the initial growth layer was confirmed by TEM, and the presence of a SiNx film having a thickness of 1 nm or more was not confirmed. Further, it was also confirmed that the Al concentration was lower than the Ga concentration. Furthermore, as shown in FIG. 7(b), the CV measurement using the mercury probe on the substrate was carried out, and it was confirmed that the thickness of the depletion layer was expanded to only about 2 μm.

比較試料1~13與試料14、15後可確認,抑制Al、Ga混入Si單晶,與有效擴展耗竭層相關。能夠有效率的擴展耗竭層,與能夠減少磊晶層內及Si單晶基板內之載子具有相同意義,即意味能夠抑制於基板表面形成之電極、與上述p型雜質之電容性或電感性之結合所造成之電子元件在高頻運作時的損失。特別是,比較試料2與試料14後而能推衍出經氮化膜之薄化,以及比較試料2與試料15後而能推衍出經磊晶層之成膜溫度降低,能帶來上述效果。Comparing Samples 1 to 13 with Samples 14 and 15, it was confirmed that Al and Ga were prevented from being mixed into the Si single crystal, and it was associated with the effective expansion of the exhausted layer. The ability to efficiently expand the depletion layer has the same meaning as to reduce the carrier in the epitaxial layer and in the Si single crystal substrate, that is, the electrode capable of suppressing formation on the surface of the substrate, and the capacitive or inductive property of the p-type impurity described above. The combination of the electronic components caused by the loss of high frequency operation. In particular, after the comparison of the sample 2 and the sample 14, the thinning of the nitride film can be derived, and after the comparison of the sample 2 and the sample 15, the film formation temperature of the epitaxial layer can be deduced, which can bring about the above. effect.

再者,所有之實驗例所製得之磊晶基板中,藉霍爾效應測定法評估通道層部分之電氣特性的結果,確認顯示出薄片電阻值在450Ω/□以下(四角),遷移率在1550cm2 /Vs以上之良好特性。Furthermore, in all the epitaxial substrates prepared in the experimental examples, the results of evaluating the electrical characteristics of the channel layer portion by the Hall effect measurement method confirmed that the sheet resistance value was below 450 Ω/□ (four corners), and the mobility was Good characteristics above 1550cm 2 /Vs.

[產業上之可利用性][Industrial availability]

依本發明之電子元件用磊晶基板,其具備緩衝層(具有由AlN材料構成之初期生長層及既定之超晶格積層體)及既定之主積層體,該等超晶格積層體、或主積層體之緩衝層側之部分之至少一方具有1×1018 /cm3 以上的C濃度,藉此,能良好地兼顧橫向洩漏電流之降低及橫向耐壓特性,且能提升縱向耐壓。進一步,除了上述特性之外,將該Si單晶基板之比電阻設為1000Ω‧cm以上,將上述Si單晶基板之初期生長層側之Ⅲ族原子的合計最大濃度設在1×1016 /cm3 以下,且,將在0.3μm深度位置之Ⅲ族原子的合計濃度設在1×1015 /cm3 以下,藉此,可降低高頻信號施加時的損失。An epitaxial substrate for an electronic component according to the present invention, comprising: a buffer layer (having an initial growth layer made of an AlN material and a predetermined superlattice laminate) and a predetermined main laminate, the superlattice laminate, or At least one of the portions on the buffer layer side of the main laminate has a C concentration of 1 × 10 18 /cm 3 or more, whereby the lateral leakage current and the lateral withstand voltage characteristics can be satisfactorily balanced, and the longitudinal withstand voltage can be improved. Further, in addition to the above characteristics, the specific resistance of the Si single crystal substrate is set to 1000 Ω ‧ cm or more, and the total concentration of the group III atoms on the initial growth layer side of the Si single crystal substrate is set to 1 × 10 16 / In the case of cm 3 or less, the total concentration of the group III atoms at the depth of 0.3 μm is set to 1 × 10 15 /cm 3 or less, whereby the loss at the time of application of the high-frequency signal can be reduced.

又,依本發明能製造一種電子元件用磊晶基板,其具備緩衝層(具有由AlN材料構成之初期生長層及既定之超晶格積層體)及既定之主積層體,該等超晶格積層體、或主積層體之緩衝層側之部分之至少一方具有1×1018 /cm3 以上的C濃度,藉此,能良好地兼顧橫向洩漏電流之降低及橫向耐壓特性,且能提升縱向耐壓,進一步,除了上述特性之外,可降低高頻信號施加時的損失。Further, according to the present invention, it is possible to manufacture an epitaxial substrate for an electronic component comprising a buffer layer (having an initial growth layer composed of an AlN material and a predetermined superlattice laminate) and a predetermined main laminate, and the superlattice At least one of the portion of the layered body or the buffer layer side of the main layered body has a C concentration of 1 × 10 18 /cm 3 or more, whereby the lateral leakage current and the lateral withstand voltage characteristics can be satisfactorily balanced and improved. Longitudinal withstand voltage, further, in addition to the above characteristics, the loss at the time of application of a high frequency signal can be reduced.

1...電子元件用磊晶基板1. . . Epitaxial substrate for electronic components

2...Si單晶基板2. . . Si single crystal substrate

3...緩衝層3. . . The buffer layer

4...主積層體4. . . Main laminate

4a...通道層4a. . . Channel layer

4b...電子供應層4b. . . Electronic supply layer

5...初期生長層5. . . Initial growth layer

6...超晶格積層體6. . . Superlattice laminate

6a...第1層6a. . . Tier 1

6b...第2層6b. . . Level 2

圖1係表示一般場效電晶體之截面示意圖。Figure 1 is a schematic cross-sectional view showing a general field effect transistor.

圖2係本發明之電子元件用磊晶基板之截面示意圖。2 is a schematic cross-sectional view showing an epitaxial substrate for an electronic component of the present invention.

圖3之(a)、(b)、(c)係分別表示橫向耐壓、橫向洩漏電流、及縱向耐壓之測定結果之圖。(a), (b), and (c) of FIG. 3 are graphs showing measurement results of lateral withstand voltage, lateral leakage current, and longitudinal withstand voltage, respectively.

圖4之(a)、(b)、(c)係分別表示橫向耐壓、橫向洩漏電流、及縱向耐壓之測定結果之圖。(a), (b), and (c) of FIG. 4 are graphs showing measurement results of lateral withstand voltage, lateral leakage current, and longitudinal withstand voltage, respectively.

圖5之(a)、(b)係分別表示SIMS之結果及CV測定結果之圖。(a) and (b) of Fig. 5 are graphs showing the results of SIMS and the results of CV measurement, respectively.

圖6之(a)、(b)係分別表示SIMS之結果及CV測定結果之圖。(a) and (b) of Fig. 6 are graphs showing the results of SIMS and the results of CV measurement, respectively.

圖7之(a)、(b)係分別表示SIMS之結果及CV測定結果之圖。(a) and (b) of FIG. 7 are graphs showing the results of SIMS and the results of CV measurement, respectively.

1...電子元件用磊晶基板1. . . Epitaxial substrate for electronic components

2...Si單晶基板2. . . Si single crystal substrate

3...緩衝層3. . . The buffer layer

4...主積層體4. . . Main laminate

4a...通道層4a. . . Channel layer

4b...電子供應層4b. . . Electronic supply layer

5...初期生長層5. . . Initial growth layer

6...超晶格積層體6. . . Superlattice laminate

6a...第1層6a. . . Tier 1

6b...第2層6b. . . Level 2

Claims (5)

一種電子元件用磊晶基板,其具備Si單晶基板、形成於該Si單晶基板上之作為絕緣層之緩衝層、及在該緩衝層上磊晶生長複數層之Ⅲ族氮化物層所形成之主積層體,並以橫向作為電流導通方向,其特徵在於:該緩衝層至少具有與該Si單晶基板連接之初期生長層、以及在該初期生長層上之由超晶格多層結構所構成之超晶格積層體;該初期生長層由AlN材料構成,且,該超晶格積層體係交互積層由Ba1 Alb1 Gac1 Ind1 N(0≦a1 ≦1,0≦b1 ≦1,0≦c1 ≦1,0≦d1 ≦1,a1 +b1 +c1 +d1 =1)材料所構成之第1層、以及由帶隙不同於該第1層之Ba2 Alb2 Gac2 Ind2 N(0≦a2 ≦1,0≦b2 ≦1,0≦c2 ≦1,0≦d2 ≦1,a2 +b2 +c2 +d2 =1)材料所構成之第2層而成;該超晶格積層體、及該主積層體之該緩衝層側之部分,C濃度均為1×1018 /cm3 以上。An epitaxial substrate for an electronic component, comprising: a Si single crystal substrate; a buffer layer as an insulating layer formed on the Si single crystal substrate; and a group III nitride layer formed by epitaxially growing a plurality of layers on the buffer layer The main laminate body has a lateral direction as a current conduction direction, and the buffer layer has at least an initial growth layer connected to the Si single crystal substrate and a superlattice multilayer structure on the initial growth layer. a superlattice laminate; the initial growth layer is composed of an AlN material, and the superlattice laminated system is alternately layered by B a1 Al b1 Ga c1 In d1 N(0≦a 1 ≦1,0≦b 1 ≦1 , 0≦c 1 ≦1,0≦d 1 ≦1, a 1 +b 1 +c 1 +d 1 =1) the first layer composed of the material, and the B a2 different from the first layer by the band gap Al b2 Ga c2 In d2 N(0≦a 2 ≦1,0≦b 2 ≦1,0≦c 2 ≦1,0≦d 2 ≦1, a 2 +b 2 +c 2 +d 2 =1) The second layer composed of the material is formed; and the portion of the superlattice laminate and the buffer layer side of the main laminate has a C concentration of 1 × 10 18 /cm 3 or more. 如申請專利範圍第1項之電子元件用磊晶基板,其中,該第1層由AlN材料構成,該第2層由Alb2 Gac2 N(a2 =0,0≦b2 ≦0.5,0.5≦c2 <1,d2 =0)材料構成。The epitaxial substrate for an electronic component according to claim 1, wherein the first layer is composed of an AlN material, and the second layer is composed of Al b2 Ga c2 N (a 2 =0, 0 ≦ b 2 ≦ 0.5, 0.5 ≦c 2 <1, d 2 =0) material composition. 如申請專利範圍第1或2項之電子元件用磊晶基板,其中,該Si單晶基板之比電阻為1000Ω.cm以上,由該初期生長層起至0.1μm深度之Ⅲ族原子之合計最大濃度為1×1016 /cm3 以下,且,在由該初期生長層起0.3μm深度位置之Ⅲ族原子之合計濃度為1×1015 /cm3 以下。The epitaxial substrate for an electronic component according to claim 1 or 2, wherein the specific resistance of the Si single crystal substrate is 1000 Ω. The total concentration of the group III atoms from the initial growth layer to the depth of 0.1 μm is 1×10 16 /cm 3 or less, and the total of the group III atoms at a depth of 0.3 μm from the initial growth layer. The concentration is 1 × 10 15 /cm 3 or less. 一種電子元件用磊晶基板之製造方法,其依序在Si單晶基板上形成作為絕緣層之緩衝層、及在該緩衝層上磊晶生長複數層之Ⅲ族氮化物層而成之主積層體,並以橫向作為電流導通方向,其特徵在於:該緩衝層,至少具有與該Si單晶基板連接之初期生長層、以及在該初期生長層上之由超晶格多層結構所構成之超晶格積層體;該初期生長層由AlN材料構成,且,該超晶格積層體係交互積層由Ba1 Alb1 Gac1 Ind1 N(0≦a1 ≦1,0≦b1 ≦1,0≦c1 ≦1,0≦d1 ≦1,a1 +b1 +c1 +d1 =1)材料所構成之第1層、以及由帶隙不同於該第1層之Ba2 Alb2 Gac2 Ind2 N(0≦a2 ≦1,0≦b2 ≦1,0≦c2 ≦1,0≦d2 ≦1,a2 +b2 +c2 +d2 =1)材料所構成之第2層而成;該超晶格積層體、及該主積層體之該緩衝層側之部分的至少一方,C濃度均為1×1018 /cm3 以上。A method for manufacturing an epitaxial substrate for an electronic component, comprising: sequentially forming a buffer layer as an insulating layer on a Si single crystal substrate; and forming a main layer of a group III nitride layer of a plurality of layers epitaxially grown on the buffer layer And a lateral direction as a current conduction direction, wherein the buffer layer has at least an initial growth layer connected to the Si single crystal substrate, and a super-lattice multilayer structure on the initial growth layer a lattice laminate; the initial growth layer is composed of an AlN material, and the superlattice layer system is alternately layered by B a1 Al b1 Ga c1 In d1 N(0≦a 1 ≦1,0≦b 1 ≦1,0 ≦c 1 ≦1,0≦d 1 ≦1, a 1 +b 1 +c 1 +d 1 =1) the first layer composed of the material, and the B a2 Al b2 different from the first layer by the band gap Ga c2 In d2 N(0≦a 2 ≦1,0≦b 2 ≦1,0≦c 2 ≦1,0≦d 2 ≦1, a 2 +b 2 +c 2 +d 2 =1) The second layer of the structure is formed; at least one of the superlattice laminate and the portion of the main laminate on the buffer layer side has a C concentration of 1 × 10 18 /cm 3 or more. 如申請專利範圍第4項之電子元件用磊晶基板之製造方法,其中,該Si單晶基板係形成為比電阻為1000Ω.cm以上,由該初期生長層起至0.1μm深度之Ⅲ族原子之合計最大濃度為1×1016 /cm3 以下,且,在由該初期生長層起0.3μm深度位置之Ⅲ族原子之合計濃度為1×1015 /cm3 以下。The method for manufacturing an epitaxial substrate for an electronic component according to claim 4, wherein the Si single crystal substrate is formed to have a specific resistance of 1000 Ω. The total concentration of the group III atoms from the initial growth layer to the depth of 0.1 μm is 1×10 16 /cm 3 or less, and the total of the group III atoms at a depth of 0.3 μm from the initial growth layer. The concentration is 1 × 10 15 /cm 3 or less.
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US20060121682A1 (en) * 2001-12-03 2006-06-08 Cree, Inc. Strain balanced nitride heterojunction transistors and methods of fabricating strain balanced nitride heterojunction transistors
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