CN108321082A - 半导体装置的制造方法 - Google Patents
半导体装置的制造方法 Download PDFInfo
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Abstract
本发明提供一种半导体装置的制造方法,抑制在向半导体基板的表面照射光来激活杂质时半导体基板背面的温度上升。在光吸收层形成工序中,在具有表面和背面的半导体基板的表面上或内部形成光吸收率高于相邻半导体层的光吸收率的光吸收层。在此,以使光吸收层分布在比背面接近表面的范围内的方式形成光吸收层。在高浓度层形成工序中,通过向半导体基板注入杂质而形成杂质浓度上升的高浓度层。在加热工序中,通过对高浓度层进行加热而激活高浓度层内的杂质。光吸收层形成工序和高浓度层形成工序以使光吸收层与高浓度层至少局部重叠的方式实施。在对高浓度层进行加热的工序中,通过从表面侧朝着高浓度层照射光而对高浓度层进行加热。
Description
技术领域
本说明书公开的技术涉及半导体装置的制造方法。
背景技术
专利文献1公开了一种技术,向半导体基板的表面注入杂质,然后向该表面照射激光,由此激活注入到半导体基板上的杂质。而且,在该技术中,通过向半导体基板的表面照射脉冲宽度不同的两种激光,来抑制半导体基板的背面(被照射光的半导体基板的与表面相反一侧的面)的温度上升。
在先技术文献
专利文献1:日本特开2014-036110号公报
发明内容
发明要解决的课题
近年来,半导体基板越发薄型化。因此,在通过照射光来激活半导体基板内的杂质时,背面的温度容易上升。因此,在本说明书中,提供另一种技术,在向半导体基板的表面照射光来激活杂质时,能够良好地抑制半导体基板的背面的温度上升。
用于解决课题的方案
本说明书公开的半导体装置的制造方法具有光吸收层形成工序、高浓度层形成工序及加热工序。在上述光吸收层形成工序中,在具有表面和背面的半导体基板的上述表面上或内部形成光吸收率高于相邻半导体层的光吸收率的光吸收层。在此,以在形成了上述光吸收层之后的上述半导体基板中上述光吸收层分布在比上述背面接近上述表面的范围内的方式来形成上述光吸收层。在上述高浓度层形成工序中,通过向上述半导体基板注入杂质而形成杂质浓度上升的高浓度层。在上述加热工序中,通过对上述高浓度层进行加热而激活上述高浓度层内的杂质。上述光吸收层形成工序和上述高浓度层形成工序以使上述光吸收层与上述高浓度层至少局部重叠的方式实施。在对上述高浓度层进行加热的工序中,通过从上述表面侧朝着上述高浓度层照射光而对上述高浓度层进行加热。
另外,光吸收层可以形成在原来的半导体基板(形成光吸收层之前的半导体基板)的表面上,也可以形成在原来的半导体基板的内部。在原来的半导体基板的表面上形成光吸收层的情况下,将光吸收层和原来的半导体基板整体称为形成了光吸收层之后的半导体基板。即,形成了光吸收层之后的半导体基板包含光吸收层。
另外,光吸收层形成工序和高浓度层形成工序哪个先实施均可。在光吸收层形成工序之后实施高浓度层形成工序的情况下,高浓度层只要是与光吸收层至少局部重叠的范围即可,可以形成于任意范围。例如,高浓度层可以仅形成于光吸收层的内部,高浓度层也可以横跨光吸收层的内部和外部地形成。而且,在高浓度层形成工序之后实施光吸收层形成工序的情况下,光吸收层只要是与高浓度层至少局部重叠的范围即可,可以形成于任意范围。例如,光吸收层可以仅形成于高浓度层的内部,光吸收层也可以横跨高浓度层的内部和外部地形成。
在该制造方法中,在加热工序中,从半导体基板的表面侧朝着高浓度层照射光。照射的光在光吸收层中被高效地吸收,光吸收层被高效地加热。由于光吸收层与高浓度层至少局部重叠,因此高浓度层也被高效地加热。这样,高浓度层被高效地加热,激活了高浓度层内的杂质。而且,光吸收层中的光的吸收率高,因此到达比光吸收层靠背面侧的位置的光较少。因此,抑制了比光吸收层靠背面侧的位置的温度上升。因此,能抑制半导体基板的背面的温度上升。因此,根据该制造方法,能够在抑制背面的温度上升的同时,激活高浓度层内的杂质。
附图说明
图1是半导体装置的剖视图。
图2是形成了上表面侧的构造之后的半导体基板的剖视图。
图3是高浓度层形成工序的说明图(下表面附近的放大剖视图。)。
图4是表示高浓度层内的n型杂质浓度分布的曲线图。
图5是非晶层形成工序的说明图(下表面附近的放大剖视图)。
图6是非晶层形成工序的说明图(下表面附近的放大剖视图)。
图7是高浓度层形成工序的说明图(下表面附近的放大剖视图)。
具体实施方式
【实施例】
图1示出通过后述的实施例1、2的制造方法制造的半导体装置10。半导体装置10具有:半导体基板12、上部电极14及下部电极16。半导体基板12由单晶硅构成。上部电极14与半导体基板12的上表面12a相接。下部电极16与半导体基板12的下表面12b相接。半导体基板12具有作为IGBT(绝缘栅双极型晶体管)进行动作的IGBT区域20和作为二极管进行动作的二极管区域40。在IGBT区域20内的IGBT进行动作时,上部电极14作为发射极发挥作用,下部电极16作为集电极发挥作用。在二极管区域40内的二极管进行动作时,上部电极14作为阳极发挥作用,下部电极16作为阴极发挥作用。在IGBT区域20的内部的上表面12a侧的范围设有n型的源区、p型的体区、沟槽栅电极等。在二极管区域40的内部的上表面12a侧的范围设有p型的阳极区等。IGBT区域20和二极管区域40的上表面12a侧的构造是以往公知的,因此省略详细的说明。
在半导体基板12的内部的下表面12b侧的范围设有漂移层27、缓冲层28、集电层30及阴极层44。漂移层27是n型杂质浓度低的n型层。漂移层27横跨IGBT区域20和二极管区域40地分布。缓冲层28是n型杂质浓度高于漂移层27的n型层。缓冲层28配置在漂移层27的下侧。缓冲层28横跨IGBT区域20和二极管区域40地分布。集电层30是p型层。集电层30配置在IGBT区域20内的缓冲层28的下侧。集电层30在下表面12b与下部电极16进行欧姆接触。阴极层44是n型杂质浓度高于缓冲层28的n型层。阴极层44配置在二极管区域40内的缓冲层28的下侧。阴极层44在下表面12b与下部电极16进行欧姆接触。
【实施例1】
接下来,说明实施例1的制造方法。首先,准备由n型的单晶硅构成的半导体基板12。接下来,如图2所示,通过以往公知的方法,形成半导体装置10的上表面12a侧的构造。接下来,在上部电极14的表面粘贴保护带60。接下来,通过对半导体基板12的下表面12b进行研磨而使半导体基板12薄型化。在该阶段,半导体基板12的厚度成为140μm以下。而且,在该阶段,漂移层27露出于半导体基板12的下表面12b。
接下来,如图3所示,将n型杂质(在本实施方式中为磷)从下表面12b向半导体基板12的内部进行离子注入。在此,以使n型杂质的平均停止位置为距下表面12b约2μm的深度的方式注入n型杂质。由此,在半导体基板12的内部形成n型杂质浓度比注入前上升的高浓度层70。图4示出高浓度层70的内部及其周边的n型杂质浓度分布。图4的纵轴所示的n型杂质浓度与通过n型杂质注入而上升的n型杂质的上升量大致相等。如图4所示,以深度约2μm的位置为中心,在从深度约1μm至深度约3μm的范围内形成高浓度层70。而且,在深度约2μm的位置形成高浓度层70的n型杂质浓度的峰值P1。以下,将高浓度层70中的具有峰值P1的10%以上的n型杂质浓度的层称为主要层72。
接下来,如图5所示,从下表面12b向半导体基板12的内部注入非活性离子(在本实施例中为硅)。在此,以使注入的非活性离子的平均停止位置为距下表面12b约2μm的深度的方式注入非活性离子。在非活性离子的停止位置形成晶体缺陷。在此,以8×1014cm-2以上的剂量注入非活性离子。当这样以高剂量注入非活性离子时,在该平均停止位置周边,半导体基板(即,单晶硅)的晶体性被破坏,而形成非晶层76(即,非晶硅)。非晶层76具有比与非晶层76相邻的半导体层(具有晶体性的半导体层)高的光吸收率。而且,非晶层76具有比与非晶层76相邻的半导体层(具有晶体性的半导体层)低的导热率。如图4、5所示,非晶层76以与n型杂质浓度的峰值P1的深度重叠的方式形成。而且,非晶层76以其整体包含于高浓度层70的主要层72的方式形成。
接下来,向相当于阴极层44的范围内注入n型杂质(在本实施例中为硼),向相当于集电层30的范围内注入p型杂质(在本实施例中为磷)。
接下来,向半导体基板12的下表面12b照射IR激光(红外线激光)。IR激光是波长为约808nm的激光。室温下的IR激光对于单晶硅的穿透深度为约10.7μm。另外,穿透深度是当将表面的激光的能量设为1时,激光的能量衰减至1/e(e≈2.718)的深度。IR激光的穿透深度比非晶层76的深度(约2μm)长,因此向下表面12b照射的激光到达非晶层76。
如上所述,非晶层76的光吸收率高。因此,在非晶层76中高效地吸收激光,非晶层76被高效地加热。因此,与非晶层76重叠的范围中的高浓度层70被高效地加热。而且,与非晶层76相邻的范围中的高浓度层70也由于来自非晶层76的导热或激光的吸收而被加热。因此,高浓度层70整体被加热至高温。
另外,由于在非晶层76内激光被吸收,因此在非晶层76内激光急剧衰减。因此,激光几乎不会到达比非晶层76靠上表面12a侧的位置。而且,由于非晶层76的导热率低,因此热量难以传递到比非晶层76靠上表面12a侧的位置。因此,抑制了上表面12a的温度上升。
这样,通过设置非晶层76,能够抑制上表面12a的温度上升,并且能够有效地对非晶层76及高浓度层70进行加热。通过抑制上表面12a的温度上升,能抑制保护带60和上部电极14的劣化。而且,通过抑制上表面12a的温度上升,能抑制上表面12a侧的范围的半导体层内的杂质扩散,能够以稳定的特性制造半导体装置10。而且,当非晶层76被加热时,非晶层76进行结晶。非晶层76的大致整体在IR激光的照射中进行结晶。而且,在高浓度层70内,通过加热而在电学性质上激活n型杂质。由此,形成n型的缓冲层28。
接下来,通过向半导体基板12的下表面12b照射绿色激光而对半导体基板12的下表面12b附近的范围进行加热。绿色激光是波长为约532nm的激光。室温下的绿色激光对于单晶硅的穿透深度为约0.96μm。绿色激光对于单晶硅的穿透深度较短,因此下表面12b附近的表层部被高效地加热。由此,激活被注入到该表层部的p型杂质和n型杂质。由此,形成集电层30和阴极层44。
然后,以覆盖下表面12b的方式形成下部电极16,并去除保护带60从而完成图1的半导体装置10。由于保护带60未曝露在高温下,因此保护带60未产生性质变化。因此,能够良好地去除保护带60。
另外,在上述实施例1中,以使n型杂质浓度的峰值P1的位置与非晶层76的位置重叠且非晶层76包含于高浓度层70的主要层72的方式形成了非晶层76。然而,只要形成为非晶层76的至少一部分与高浓度层70的至少一部分重叠即可,形成非晶层76的范围可以适当变更。只要形成为非晶层76的至少一部分与高浓度层70的至少一部分重叠,就能够高效地对高浓度层70进行加热,并能够抑制上表面12a的温度上升。例如,可以将非晶层76设置在主要层72的外部的高浓度层70的内部。而且,例如,非晶层76也可以横跨高浓度层70的内部和高浓度层70的外部地设置。但是,当如实施例1那样以使n型杂质浓度的峰值P1的位置与非晶层76的位置重叠且非晶层76包含于高浓度层70的主要层72的方式形成非晶层76时,能够更高效地对高浓度层70进行加热。因此,能够以较少的能量加热高浓度层70,可以减少向半导体基板12赋予的热量,因此能够进一步抑制上表面12a的温度上升。
另外,在上述实施例1中,在形成了高浓度层70之后形成非晶层76,但也可以在形成了非晶层76之后形成高浓度层70。
【实施例2】
接下来,说明实施例2的制造方法。在实施例2的制造方法中,与实施例1的制造方法相同,得到图2的构造。接下来,如图6所示,在半导体基板12的下表面12b上生长由非晶硅构成的非晶层76。例如,能够通过LPCVD(Low Pressure Chemical Vapor Deposition:低压化学气相沉积法)、等离子体CVD或光CVD等生长非晶层76。在此,形成3μm以下厚度的非晶层76。另外,以下,将形成非晶层76前的半导体基板12和非晶层76一并称为半导体基板12。因此,将非晶层76的表面称为半导体基板12的下表面12b。
接下来,如图7所示,从下表面12b向非晶层76的内部注入n型杂质(在本实施方式中为磷)。在此,以使n型杂质的平均停止位置为距下表面12b约2μm的深度的方式注入n型杂质。由此,在非晶层76的内部形成n型杂质浓度高于注入前的高浓度层70。如图7所示,高浓度层70整体包含于非晶层76。
接下来,向非晶层76的表层部中的相当于阴极层44的范围注入n型杂质(在本实施例中为硼),向非晶层76的表层部中的相当于集电层30的范围注入p型杂质(在本实施例中为磷)。
接下来,向半导体基板12的下表面12b照射IR激光(红外线激光)。在实施例2中,非晶层76露出于下表面12b,因此IR激光照射于非晶层76。由于非晶层76的光吸收率高,因此在非晶层76中激光被高效地吸收,非晶层76被高效地加热。因此,与非晶层76重叠的高浓度层70整体被高效地加热。
另外,在非晶层76内激光被吸收,因此在非晶层76内激光急剧衰减。因此,激光几乎不会到达比非晶层76靠上表面12a侧的位置。而且,由于非晶层76的导热率低,因此热量难以传递到比非晶层76靠上表面12a侧的位置。因此,能抑制上表面12a的温度上升。
这样,通过设置非晶层76,能够抑制上表面12a的温度上升,并能够高效地对非晶层76及高浓度层70进行加热。当非晶层76被加热时,非晶层76结晶化。而且,在高浓度层70内,通过加热而激活n型杂质。由此,形成n型的缓冲层28。
接下来,向半导体基板12的下表面12b照射绿色激光,由此对半导体基板12的下表面12b附近的范围进行加热。绿色激光对于单晶硅的穿透深度短,因此下表面12b附近的表层部被高效地加热。由此,激活注入到该表层部中的p型杂质和n型杂质。由此,形成集电层30和阴极层44。
然后,以覆盖下表面12b的方式形成下部电极16,并将保护带60去除,从而完成图1的半导体装置10。由于保护带60未曝露在高温下,因此保护带60未产生性质变化。因此,能够良好地去除保护带60。
另外,在上述实施例2中,高浓度层70整体包含于非晶层76的内部,但是高浓度层70也可以横跨非晶层70的内部和外部地分布。
另外,在上述实施例1、2中,通过激光对高浓度层70进行加热,但也可以通过激光以外的光对高浓度层70进行加热。
说明实施例的结构要素与权利要求的结构要素之间的关系。实施例中的半导体基板12的下表面12b是权利要求中的半导体基板的表面的一例。实施例中的半导体基板12的上表面12a是权利要求中的半导体基板的背面的一例。实施例中的非晶层76是权利要求中的光吸收层的一例。
以下列举本说明书公开的技术要素。另外,以下的各技术要素分别是独立地有用的要素。
在本说明书公开的一例的制造方法中,高浓度层具有主要层,该主要层具有高浓度层的杂质浓度上升量的峰值的10%以上的杂质浓度上升量。在此,可以是,形成光吸收层的工序和形成高浓度层的工序以使光吸收层与主要层至少局部地重叠的方式实施。
根据该结构,能够高效地对高浓度层的主要层进行加热。
在本说明书公开的一例的制造方法中,可以是,成光吸收层的工序和形成高浓度层的工序以使光吸收层的整体位于主要层内的方式实施。
根据该结构,能够更高效地对高浓度层的主要层进行加热。
在本说明书公开的一例的制造方法中,可以是,形成光吸收层的工序和形成高浓度层的工序以使高浓度层的杂质浓度上升量的峰值位置与光吸收层重叠的方式实施。
根据该结构,能够高效地对高浓度层的上述峰值的位置进行加热。
在本说明书公开的一例的制造方法中,可以是,光吸收层是通过向半导体基板注入非活性离子而使晶体缺陷密度上升的区域。
另外,作为非活性离子,可以使用例如硅、氦、氖、氩等。
在本说明书公开的一例的制造方法中,可以是,在对高浓度层进行加热的工序中,使光吸收层结晶。
根据该结构,能够制造出具有更良好的特性的半导体装置。
以上,详细地说明了实施方式,但是它们只不过是例示,对权利要求书没有限定作用。权利要求书记载的技术包括对以上例示的具体例进行了各种变形、变更的技术。本说明书或附图说明的技术要素是单独或者通过各种组合而发挥技术有用性的要素,不限定为申请时权利要求记载的组合。另外,本说明书或附图例示的技术是同时实现多个目的的技术,并且通过实现这些目的当中之一而具有技术有用性。
附图标记说明
10:半导体装置
12:半导体基板
14:上部电极
16:下部电极
20:IGBT区域
27:漂移层
28:缓冲层
30:集电层
40:二极管区域
44:阴极层
60:保护带
70:高浓度层
72:主要层
76:非晶层
Claims (8)
1.一种半导体装置的制造方法,包括:
在具有表面和背面的半导体基板的所述表面上或内部形成光吸收率高于相邻半导体层的光吸收率的光吸收层的工序,以在形成了所述光吸收层之后的所述半导体基板中所述光吸收层分布在比所述背面靠近所述表面的范围内的方式来形成所述光吸收层;
通过向所述半导体基板注入杂质而形成杂质浓度上升的高浓度层的工序;及
通过对所述高浓度层进行加热而激活所述高浓度层内的杂质的工序,
形成所述光吸收层的工序和形成所述高浓度层的工序以使所述光吸收层与所述高浓度层至少局部重叠的方式实施,
在对所述高浓度层进行加热的工序中,通过从所述表面侧朝着所述高浓度层照射光而对所述高浓度层进行加热。
2.根据权利要求1所述的半导体装置的制造方法,其中,
所述高浓度层具有主要层,所述主要层具有所述高浓度层的杂质浓度上升量的峰值的10%以上的杂质浓度上升量,
形成所述光吸收层的工序和形成所述高浓度层的工序以使所述光吸收层与所述主要层至少局部重叠的方式实施。
3.根据权利要求2所述的半导体装置的制造方法,其中,
形成所述光吸收层的工序和形成所述高浓度层的工序以使所述光吸收层整体位于所述主要层内的方式实施。
4.根据权利要求1~3中任一项所述的半导体装置的制造方法,其中,
形成所述光吸收层的工序和形成所述高浓度层的工序以使所述高浓度层的杂质浓度上升量的峰值的位置与所述光吸收层重叠的方式实施。
5.根据权利要求1~4中任一项所述的半导体装置的制造方法,其中,
所述光吸收层是通过向所述半导体基板注入非活性离子而使晶体缺陷密度上升的区域。
6.根据权利要求1~4中任一项所述的半导体装置的制造方法,其中,
所述光吸收层是在形成所述光吸收层之前的所述半导体基板的表面上生长而成的非晶层。
7.根据权利要求5或6所述的半导体装置的制造方法,其中,在对所述高浓度层进行加热的工序中,使所述光吸收层结晶。
8.根据权利要求1~7中任一项所述的半导体装置的制造方法,其中,
所述半导体基板是硅基板,
所述光吸收层是非晶硅层。
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CN1452223A (zh) * | 2002-04-16 | 2003-10-29 | 株式会社东芝 | 半导体装置及半导体装置的制造方法 |
JP2006344909A (ja) * | 2005-06-10 | 2006-12-21 | Sumitomo Heavy Ind Ltd | レーザ照射装置及び半導体装置の製造方法 |
US20120178223A1 (en) * | 2011-01-07 | 2012-07-12 | Kabushiki Kaisha Toshiba | Method of Manufacturing High Breakdown Voltage Semiconductor Device |
CN103283006A (zh) * | 2011-11-07 | 2013-09-04 | 松下电器产业株式会社 | 薄膜晶体管器件的制造方法、薄膜晶体管器件以及显示装置 |
JP2014195004A (ja) * | 2013-03-29 | 2014-10-09 | Sumitomo Heavy Ind Ltd | 半導体素子の製造方法及び半導体素子の製造装置 |
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JP2011243939A (ja) * | 2010-01-20 | 2011-12-01 | Panasonic Corp | 窒化物半導体レーザ装置 |
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US9679773B1 (en) * | 2016-03-14 | 2017-06-13 | Infineon Technologies Ag | Method for thermal annealing and a semiconductor device formed by the method |
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JP2006344909A (ja) * | 2005-06-10 | 2006-12-21 | Sumitomo Heavy Ind Ltd | レーザ照射装置及び半導体装置の製造方法 |
US20120178223A1 (en) * | 2011-01-07 | 2012-07-12 | Kabushiki Kaisha Toshiba | Method of Manufacturing High Breakdown Voltage Semiconductor Device |
CN103283006A (zh) * | 2011-11-07 | 2013-09-04 | 松下电器产业株式会社 | 薄膜晶体管器件的制造方法、薄膜晶体管器件以及显示装置 |
JP2014195004A (ja) * | 2013-03-29 | 2014-10-09 | Sumitomo Heavy Ind Ltd | 半導体素子の製造方法及び半導体素子の製造装置 |
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