CN101241966B - 电阻随机存取存储单元装置 - Google Patents
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Abstract
本发明涉及电阻随机存取存储单元装置。一种存储单元装置其具有一底电极与一顶电极,一存储材料栓塞接触至底电极,以及一杯状导电构件其具有一周缘接触至顶电极、以及在底部具有一开口接触至存储材料。因此,在存储单元中的导电路径是从顶电极穿过导电杯状构件,并穿过相变化材料栓塞而到达底电极。同时,用以制造此存储单元装置的方法包括:形成一岛状底电极、其包括一绝缘构件以及一停止构件于一底电极之上,形成一分隔层其环绕此岛状底电极,移除停止构件以形成一空洞于分隔层中的绝缘构件之上,形成一导电薄膜于此空洞中、并形成一绝缘衬底于导电薄膜之上,蚀刻以形成一杯状导电薄膜其具有一周缘并形成一开口穿过绝缘衬底与杯状导电薄膜的底部、而到达底电极的表面,形成一相变化存储材料栓塞于此开口中,并形成一顶电极接触至杯状导电薄膜的周缘。
Description
技术领域
本发明涉及以相变化存储材料为基础的高密度存储装置,以及用以制造这种装置的方法,其中相变化存储材料包括硫属化物材料与其他材料。
背景技术
相变化存储材料广泛地用于读写光碟中。这些材料包括有至少两种固态相,包括如一大部分为非晶态的固态相,以及一大体上为结晶态的固态相。激光脉冲被用于读写光碟片中,以在二种相中切换,并读取此种材料子相变化之后的光学性质。
如硫属化物及类似材料的这种相变化存储材料,可通过施加其幅度适用于集成电路中的电流,而致使晶相变化。大致非晶态的特征是其电阻高于结晶态,此电阻值可轻易测量得到而用以作为指示。这种特性则引发使用可编程电阻材料以形成非挥发性存储器电路等兴趣,此电路可用于随机存取读写。
从非晶态转变至结晶态一般为一低电流步骤。从结晶态转变至非晶态(以下指称为重置(reset))一般为一高电流步骤,其包括一短暂的高电流密度脉冲以熔化或破坏结晶结构,其后此相变化材料会快速冷却,抑制相变化的过程,使得至少部份相变化结构得以维持在非晶态。理想状态下,致使相变化材料从结晶态转变至非晶态的重置电流幅度应越低越好。欲降低重置所需的重置电流幅度,可通过减低在存储器中的相变化材料元件的尺寸、以及减少电极与此相变化材料的接触面积而达成,因此可针对此相变化材料元件施加较小的绝对电流值而达成较高的电流密度。
此领域发展的一种方法是致力于在一集成电路结构上形成微小孔洞,并使用微量可编程的电阻材料填充这些微小孔洞。致力于这种微小孔洞的专利包括:于1997年11月11日公告的美国专利第5,687,112号“Multibit Single Cell Memory Element Having TaperedContact”、发明人为Ovshinky;于1998年8月4日公告的美国专利第5,789,277号“Method of Making Chalogenide[sic]MemoryDevice”、发明人为Zahorik等;于2000年11月21日公告的美国专利第6,150,253号“Controllable Ovonic Phase-Change SemiconductorMemory Device and Methods of Fabricating the Same”、发明人为Doan等。
当以非常微小尺寸制造这种装置且工艺变数必须符合大尺寸存储装置所要求的严格工艺规范时,会遭遇到问题。因此,较佳是能提供一种存储单元结构与制造这种结构的方法,其具有微小尺寸与低重置电流。
发明内容
本发明的一目的涉及相变化存储装置,其包括一存储材料,可通过能量的应用而在电性状态间交替。此存储单元装置具有一底电极与一顶电极,一存储材料栓塞接触至底电极,以及一杯状导电构件其具有一周缘接触至顶电极且在底部具有一开口接触至存储材料。藉此,存储单元中的导电路径是从顶电极穿过杯状导电构件,并穿过相变化材料栓塞到达底电极。
本发明的一目的,是提供一存储单元装置,其包括一底电极与一顶电极,一相变化存储材料栓塞接触至底电极,以及一杯状导电构件其具有一周缘与一底部,该底部具有一开口,其中,该导电构件在所述周缘处接触至顶电极,以及该导电构件在所述开口处接触至存储材料,以使存储单元中的导电路径是从顶电极穿过杯状导电构件,并穿过相变化材料栓塞到达底电极。
本发明的另一目的,是提供制造一存储单元装置的方法,通过提供一基板其在一表面具有一介金属介电质,形成一第一电极层于介金属介电质之上,形成一电绝缘层于第一电极层之上,形成一停止层于电绝缘层之上,以及图案化各层以形成岛状底电极,每个岛状底电极包括一电绝缘元件与一停止元件;沉积一填充材料于介金属介电质及这种岛状底电极之上;移除填充材料至停止元件;移除停止元件,形成一空洞,空洞由分隔层的一侧壁与电绝缘元件的一外露表面所定义;沉积一导电材料以形成一导电薄膜于填充材料、分隔层的侧壁与电绝缘元件的外露表面之上;沉积一电绝缘衬底材料于导电薄膜之上;进行一非等向性蚀刻,以从分隔层的表面移除电绝缘衬底材料及导电薄膜,并形成一开口穿过电绝缘衬底材料、且穿过导电薄膜和电绝缘层;沉积一相变化存储材料于开口中;形成一氧化物覆盖层于相变化存储材料之上;以及形成一顶电极于氧化物覆盖层以及分隔层的表面上等步骤达成。
本发明的方法直接采用自对准工艺,且可改变其大小。
在所生成的存储单元构件下,存储材料与底电极电性接触。一导电构件包括具有一周缘的一侧壁、以及带有一开口的一底部。存储材料接触底电极并于其开口接触导电构件;以及杯状构件的周缘接触顶电极。
附图说明
图1示出了本发明的一实施例的存储单元装置的剖面图;
图2A及图2B分别示出了一带图样的底电极堆叠位于介金属介电质的表面的平面及剖面图,其中堆叠包括底电极、氧化物、以及氮化硅层;
图3A及图3B分别示出了沉积与研磨如图2A及图2B所示的堆叠旁的填充层的结果的平面及剖面图;
图4A及图4B分别示出了从堆叠移除氮化硅层的结果的平面及剖面图;
图5A及图5B分别示出了沉积一层氮化钛于图4A、图4B的结构以及形成二氧化硅的衬底层于氮化钛层上的结果的平面及剖面图;
图6A及图6B分别示出了非等向性蚀刻穿过二氧化硅及氮化钛以外露底电极的一区域的结果的平面及剖面图;
图7A及图7B分别示出了沉积一锗锑碲(GST)于图6A、图6B的结构上以及回蚀该层以形成GST栓塞的结果的平面及剖面图;
图8A及图8B分别示出了沉积覆盖氧化物于图7A、图7B的结构以及平面化的结果的平面及剖面图;
图9A及图9B分别示出了形成顶电极于图8A、图8B的结构上的结果以及标示以显示完成的存储单元的某些特征的大小的平面及剖面图;
图9C示出了图9A的顶电极的另一形态的平面图;
图10示出了包括相变化存储构件的存储阵列的示意图。
【主要元件符号说明】
10 存储单元结构
11 分隔层
12 底电极
13 周缘
14 顶电极
16 电绝缘层
17 电绝缘衬底
18 杯状导电衬底
19 箭头
20 相变化材料栓塞
21 表面
22 非晶态
23 小区域
26 覆盖氧化物
27 底部
28 开口
29 侧壁
92 分隔层的空洞宽度
94 杯状导电薄膜侧壁部分的厚度
95 杯状薄膜的底部厚度
98 栓塞与底电极接触的区域的宽度
99 栓塞高度
123、124 字线
128 共同源极线
132、133 底电极构件
134 顶电极构件
135、136 存储单元
141、142 位线
145 Y解码器与字线驱动器
146 X解码器与感测放大器
150、151、152 存取晶体管
210 底电极堆叠或岛
212 底电极
216 绝缘层
221 表面介金属介电质层
230 蚀刻停止层
311 填充层
421 绝缘层表面
422 空洞
427 绝缘层表面
512 分隔层表面
517 绝缘衬底
518 导电薄膜
522 空隙
622 开口
具体实施方式
下面的发明说明将参照至特定结构实施例与方法。可以理解的是,本发明的范围并非限制于特定所披露的实施例,且本发明可利用其他特征、元件、方法与实施例进行实施。在各实施例中的类似元件将以类似标号对其进行指定。
参照图1,其大体上显示本发明的一实施例的存储单元结构10。存储单元结构10包括底电极12与顶电极14。电绝缘层16覆盖于底电极12之上。杯状导电衬底18包括形成于绝缘层16上的底部27以及具有一周缘13接触顶电极14的侧壁部分29。电绝缘衬底17形成于底部27之上并位于杯状导电衬底18的侧壁部分29。相变化存储材料栓塞20穿过绝缘衬底17、杯状导电衬底18的底部27以及绝缘层16,形成于一开口内。相变化存储材料栓塞20接触底电极12的表面21的一部分23,并穿过底部27于开口28接触杯状导电衬底18。电绝缘覆盖层26填满绝缘衬底17内以及顶电极14与相变化材料栓塞20间的空间。底电极12、绝缘层14以及杯状导电衬底18与相变化材料栓塞20还有杯状衬底内所包括的其他特征,被一填充层或分隔层11所包围。填充层11及底电极12位于介金属介电质上;顶电极14位于填充层11上,并接触杯状导电衬底18的周缘13。因此,顶电极在杯状衬底的侧壁的周缘电连接杯状衬底;相变化材料栓塞于底电极的表面的一部分电连接底电极;以及杯状衬底于杯状衬底的底部开口处电连接相变化材料栓塞。如箭头19略示,导电路径从顶电极14穿过杯状导电衬底18、穿过相变化材料栓塞20到达底电极12。
本发明的存储单元结构提供许多优势特征,如图1所示。相变化材料栓塞与底电极有一小区域的接触。从顶电极到相变化材料栓塞的电流(利用杯状衬底)局限于杯状衬底的底部接触相变化材料的开口的一小区域。
图10是一存储阵列的示意图,存储阵列可依据在此所述的方法实施。在图10的示意中,共同源极线128、字线123以及字线124朝Y方向大致呈平行排列。位线141及142朝X方向大致呈平行排列。因此,方块145中的Y解码器与字线驱动器耦接字线123、124。方块146中的X解码器与一组感测放大器耦接位线141及142。共同源极线128耦接存取晶体管150、151、152及153的源极端。存取晶体管150的栅极耦接字线123。存取晶体管151的栅极耦接字线124。存取晶体管152的栅极耦接字线123。存取晶体管153的栅极耦接字线124。存取晶体管150的漏极耦接存储单元135的底电极构件132,存储单元135具有顶电极构件134。顶电极构件134耦接位线141。类似地,存取晶体管151的漏极耦接存储单元136的底电极构件133,存储单元136具有顶电极构件137。顶电极构件137耦接位线141。存取晶体管152及153亦于位线142耦接对应的存储单元。从示范配置可知,共用源极线128由两列存储单元所分享,其中一列以Y方向排列,如图所示。在其他实施例中,存取晶体管可由二级管或控制阵列中的电流流向某些特定装置以读写数据的其他结构代替。
存储单元装置的实施例,包括存储材料20的相变化存储材料,其相变化存储材料包括硫属化物材料与其他材料。相变化合金能在此单元主动通道区域内依其位置顺序于材料为一般非晶状态的第一结构状态与为一般结晶固体状态的第二结构状态之间切换。这些材料至少为双稳定态。此词汇「非晶」用以指称一相对较无次序的结构,其较之一单晶更无次序性,而带有可检测的特征如较之结晶态更高的电阻值。此词汇「结晶态」用以指称一相对较有次序的结构,其较之非晶态更有次序,因此包括有可检测的特征例如比非晶态更低的电阻值。典型地,相变化材料可电切换至完全结晶态与完全非晶态之间所有可检测的不同状态。其他受到非晶态与结晶态的改变而影响的材料特征包括,原子次序、自由电子密度、以及活化能。此材料可切换成为不同的固态、或可切换成为由两种以上固态所形成的混合物,提供从非晶态至结晶态之间的灰阶部分。此材料中的电性质亦可能随之改变。
相变化合金可通过施加一电脉冲而从一种相态切换至另一相态。先前观察指出,一较短、较大幅度的脉冲倾向于将相变化材料的相态改变成大体为非晶态。一较长、较低幅度的脉冲倾向于将相变化材料的相态改变成大体为结晶态。在较短、较大幅度脉冲中的能量够大,因此足以破坏结晶结构的键结,同时够短因此可以防止原子再次排列成结晶态。在没有不适当实验的情形下,可以利用实验方法决定特别适用于一特定相变化合金的适当脉冲量变曲线。在本发明中,相变化材料指GST,且需要知道的是,本发明亦可使用其他类形的相变化材料。适用于实施在此所述的存储装置的材料为Ge2Sb2Te5。
参照图1,如图10所述的存取电路可以许多方法配置,以接触第一电极12与第二电极14,供控制存储单元的操作,使相变化材料20得以编程设定为可利用存储材料反向实作的两种固态相的其中一种。举例而言,利用硫属化物材料为主的相变化材料,可将存储单元设定为较高电阻状态以及较低电阻状态,其中在较高电阻状态下电流路径中的导桥的至少一部份是非晶态,而在较低电阻状态下电流路径中的导桥的至少一部份是结晶态。举例而言,带有适当的较短、高振幅的电脉冲的应用将导致相变化材料20局部变成大体上为非晶态,如图1中的22所示。
存储单元装置10的制造将参考图2A-9C进行描述,其中一示范工艺的许多阶段以平面图(2A、3A等;显示四个存储单元的阵列)以及剖面图(2B、3B等;显示一个存储单元)显示。存取电路位于具有一表面介金属介电质层221的基板上。适用于底电极的导电材料的导电层沉积于介金属介电质层221的表面,适用于底电极的导电材料例如有金属或以金属为主或非金属的材料,比方铜;铝;钛(Ti)及例如氮化钛(TiN)、氮氧化钛(Ton)等以钛为主的材料;钽(Ta)及例如氮化钽(Tan)的以钽为主的材料;多晶硅、例如硅化钨(WSix)的以钨为主的材料;以及针对低热传导电极,例如LNO(LaNiO3)和LSMO(LaSrMnO3)等材料;如氧化物(比如二氧化硅)的电绝缘层沉积于底电极层之上;以及例如氮氧化硅或氮化硅的材料的蚀刻停止层,沉积于绝缘层上。
底电极层可具有例如介于约200埃到约3000埃之间的厚度,通常在约500埃。举例而言,氧化物绝缘层可具有介于约50埃到2000埃之间的厚度,二氧化硅层通常在约200埃。举例说明,氮化硅蚀刻停止层可具有介于约200埃到3000埃之间的厚度,通常在约1000埃。这些层接着被图样化并被蚀刻,以形成底电极堆叠或岛状底电极210,每个底电极堆叠或岛状底电极210包括底电极212、绝缘层(氧化物,比方二氧化硅)216以及蚀刻停止层230,如图2A、2B中的范例所示。层230是根据绝缘层216及填充层311(参考下图)的材料所选的材料的牺牲层;通常适用于层230的材料对于绝缘层216有较高的蚀刻选择性且对层311有较高的CMP选择性。藉此,多晶硅或钨材料大多适用于绝缘层材料及导电层。在平面图(图2A)中,所示的底电极堆叠已被图样化为一圆柱岛;其他形状亦可通过不同配置的图样而形成。或者,本发明亦可以图10所示出的交叉点的配置(位线/字线)实施。
接着,将填充材料沉积于图2A及图2B的结构上,并将此材料移除到蚀刻停止层230的表面,以形成一填充层(或分隔层)311。适当的填充材料包括例如氧化物(例如二氧化硅、BPSG、FSG低介电常数、或对层230有较高的蚀刻选择性的其他材料),以及氮化物(例如氮化硅、多晶硅氮氧化硅、钨、或对层216具有较高的蚀刻选择性)。填充材料围绕底电极堆叠,且较佳地提供较良好的电与热绝缘,为存储单元提供热与电隔离。填充材料可利用化学机械研磨方法或例如回蚀,使之平面化,而检测到蚀刻停止层230表面的外露时,即停止研磨或蚀刻。填充材料可通过例如高密度等离子化学气相沉积进行沉积,在此工艺中蚀刻停止层会受到保护。适当的蚀刻停止材料包括例如氮氧化硅(SiON)、钨(W)、多晶硅、或对绝缘层216有较高的蚀刻选择性以及对层311有较高CMP率的其他材料;蚀刻停止层具有介于约200埃到约3000埃之间的厚度,通常约1000埃。
接着,蚀刻停止层可以通过例如选择性离子蚀刻或湿蚀刻(「浸沾」)的方式做移除。图4A及图4B显示其结构的结果。分隔层311包围底电极212与绝缘(氧化)层216,大体上如先前图式所示。只是目前绝缘(氧化)层216的表面421外露于分隔层的周壁421所定义的空洞422的底部。
接着,导电材料沉积于图4A、图4B所示的结构上,在分隔层上表面、绝缘(氧化)层216表面427、以及周壁421表面形成导电薄膜518。接着,电绝缘材料沉积于此结构上,在导电薄膜518的表面上形成衬底层517。图5A及图5B显示这些步骤的结果。衬底层的厚度不会填满空洞的整个空间,而会留下一个空隙522。适用于导电薄膜的材料包括例如氮化钛、钛、钨、铜、多晶硅;由于较薄的氮化钛比较有效,因此氮化钛较佳作为衬底材料。适用于绝缘(氧化)衬底层的材料包括例如氮氧化硅(SiON)及氮化硅(SiN)。
接着进行非等向性蚀刻,从分隔层的表面移除绝缘衬底材料及导电薄膜材料,以及蚀刻穿过空洞底部的绝缘(氧化)衬底材料以及导电薄膜。如图6A、图6B所示,这导致导电薄膜518形成杯状导电衬底18,此亦形成穿过底电极12的开口622,并外露许多特征,其包括:分隔层311的表面512、杯状衬底18的周缘13、底电极12表面21的一小区域23、以及穿过杯状衬底18的底部27的开口28。绝缘衬底材料的一部份留在底部27并在杯状衬底18的侧壁部分29内。
适当的非等向性蚀刻可包括许多步骤,一范例包括以下三个步骤。在此范例中,绝缘衬底517(17)为SiN,导电薄膜518(18)为如铜的金属,以及绝缘层216(16)为氧化硅。在第一步骤中,对于SiN,利用例如80-200W的高底功率以及比方CH3F或CHF3化合物或其混合物,选择性地与氩、氮及氧等其中之一、或两个或所有的混合物组合,进行反应性离子蚀刻(RIE)。在第二步骤中,对于金属进行含氯的蚀刻,例如利用BCl3或Cl2的化合物或其混合物,选择性与氩或氮其中之一、或其混合物组合,进行RIE。如同第一步骤,在第二步骤中底功率的强度足够进行非等向性蚀刻,例如就一8寸晶圆工艺而言是利用高于100W的底功率。第二步骤蚀刻可通过时间控制或利用终点检测而停止;关于终点检测,C-N信号降低可用以检测TiN蚀刻的工艺。在第三步骤中,对于SiO2,利用例如C4F8或CF 4或CHF3或C4F6化合物或其一或多个混合物,选择性与氧或氩或其混合物组合,进行RIE。第三层(在此为SiO2)对第一层(在此为SiN)的选择性为高选择性,以避免在第三蚀刻步骤期间毁损SiN层;蚀刻选择性可大于例如约10。蚀刻步骤的参数可以通常的设定而做调整或协调,以取得最佳性能并最佳化结果蚀刻的实体外观。第二及第三步骤之间可进行氧原子等离子剥除,以在空洞内移除聚合的残留物。选择性地,在此三个步骤的每一步骤之后以及公知的氧原子等离子剥除之后,可进行其他的干式剥除。
接着,相变化存储材料沉积于图6A、图6B所示的结构上,利用例如回蚀将沉积材料的上部分移除,以在开口622的底部留下相变化材料栓塞20,如图7A及图7B所示。相变化材料可为GexSbyTez(一种「GST」)化学式的硫属化物,其中x=0-5;y=0-5;以及z=0-10,例如其x∶y∶z=2∶2∶5的GST。或者相变化材料可为一种GST,例如掺杂N的GST、掺杂Si的GST、或掺杂Ti的GST;或可以其他元素作为掺杂物的方式实施。
硫属化物相变化材料利用氩、氮、氦或其类似物或这些气体的混合物作为反应气体,在介于约1mtorr到约100mtorr的气压范围内,且通常是在室温下,通过物理气相沉积溅镀或磁控溅镀进行沉积。利用具有深宽比约1比5的准直器、或利用介于约10V到约1000V的范围内(例如几十伏特到几百伏特)施加DC偏压、或同时利用准直器与DC偏压,可改进填充性能。沉积之后,硫属化物材料可进行退火以改进结晶态。后沉积退火可在真空或氮环境,温度介于约100℃到约400℃的范围内,在少于30分钟内完成。
硫属化物栓塞的厚度根据单元结构的设计而改变。大致上具有厚度大于约8nm的硫化物栓塞可显示相变化双稳定电阻态的特性。沉积的硫化物材料可利用公知金属干蚀刻技术作回蚀,即利用例如Cl2或CF4化合物或其混合物,选择性与氩或氧或其混合物的组合进行RIE。为了移除空洞外的GST,需要进行非等向性GST蚀刻。RIE需要额外的底功率,例如40-100W,形成图7B所示的结构。终点检测可用以停止GST蚀刻。
在利用溅镀方式沉积存储材料时,情况可能包括例如氮或氩气(或氩及氮的混合物);若只使用氩气,标的可能是GeSbTe;或使用氩/氮气时,标的可能是N2-GeSbTe。
控制回蚀是为了保持相变化材料与杯状衬底在开口28处的接触。相变化存储材料栓塞在小区域23接触底电极,并在开口28接触杯状导电薄膜。栓塞限制在开口622的底部,而栓塞(包括栓塞与底电极的接触区23)的形状及大小由开口622的底部的形状及大小与回蚀后的栓塞的高度进行定义。
接着,氧化材料(例如二氧化硅)沉积于图7A、图7B的结构上,填充开口622的一部份中栓塞20上所剩余的空间,而氧化材料被平面化以形成覆盖氧化层26。
接着,适合作顶电极的导电材料沉积在图8A、图8B的结构上,并被图样化以在存储单元构件上形成顶电极,如图9A、图9B及图9C所示,此导电材料可为金属或以金属为主或非金属材料,例如铜;铝;钛(Ti)和比方氮化钛(TiN)、氮氧化钛(TiON)等以钛为主的金属;钽(Ta)及例如氮化钽(TaN)的以钽为主的材料;多晶硅、如硅化钨(WSix)的以钨为主的材料;以及有关低热传导电极,例如LNO(LaNiO3)和LSMO(LaSrMnO3)。顶电极可被图样成岛状,如图9A的范例所示,或线形(带形线或位线),如图9C的范例所示。顶电极可具有例如介于约200埃到约5000埃之间的厚度,通常在约2000埃。
图9B显示形成的存储单元装置,以标记表示某些特征的尺寸。大致上本发明所制造的存储单元中其特征的剖面形状由分隔层中的空洞的形状而定义,而分隔层中的空洞的形状可根据存储堆叠或岛的形状进行定义。类似地,相变化材料栓塞的形状及大小由非等向性蚀刻所形成的开口的大小以及相变化材料回蚀的程度定义。在存储单元的许多特征的示范实施例中,显示有许多圆形剖面(在介金属介电质表面的平面上),但需要知道的是其他的剖面形状也可使用。图9B以范例显示某些可称做「宽度」的尺寸,在特征是圆形的情况下,这个尺寸是指其直径而言。
穿过分隔层的空洞的宽度92可在介于约50nm到约400nm的范围之间,通常约为100nm。杯状导电薄膜的侧壁部分的厚度94可在约25埃到约200埃的范围的内,通常约为50埃,而杯状薄膜的底部厚度95可在约25埃到约200埃的范围之内,通常约为50埃。栓塞与底电极接触的区域的宽度98可在约20nm到约260nm的范围之内,通常约为70nm,提供介于约20nm到约260nm的范围内的接触区域,通常约70nm。栓塞的高度99根据杯状导电薄膜的底部厚度95与在底电极的接触区域间绝缘氧化物的厚度等其他因素而不同;栓塞的高度99可在介于约20nm到约100nm的范围内,通常约为30nm。
存储单元装置10的实施例,包括了存储材料20所使用的相变化存储材料,包括硫属化物材料与其他材料。硫属化物包括下列四元素中的任一者:氧(O)、硫(S)、硒(Se)、以及碲(Te),形成元素周期表上第VI族的部分。硫属化物包括将一硫属元素与一更为正电性的元素或自由基结合而得。硫属化合物合金包括将硫属化合物与其他物质如过渡金属等结合。一硫属化合物合金通常包括一个以上选自元素周期表第六栏的元素,例如锗(Ge)以及锡(Sn)。通常,硫属化合物合金包括下列元素中一个以上的复合物:锑(Sb)、镓(Ga)、铟(In)、以及银(Ag)。许多以相变化为基础的存储材料已经被描述于技术文件中,包括下列合金:镓/锑、铟/锑、铟/硒、锑/碲、锗/碲、锗/锑/碲、铟/锑/碲、镓/硒/碲、锡/锑/碲、铟/锑/锗、银/铟/锑/碲、锗/锡/锑/碲、锗/锑/硒/碲、以及碲/锗/锑/硫。在锗/锑/碲合金家族中,可以尝试大范围的合金成分。此成分可以下列特征式表示:TeaGebSb100-(a+b)。一位研究员描述了最有用的合金为,在沉积材料中所包括的平均碲浓度远低于70%,典型地低于60%,并在一般形态合金中的碲含量范围从最低23%至最高58%,且最佳介于48%至58%的碲含量。锗的浓度高于约5%,且其在材料中的平均范围从最低8%至最高30%,一般低于50%。最佳地,锗的浓度范围介于8%至40%。在此成分中所剩下的主要成分则为锑,上述百分比是指所有组成元素的原子总计为100%的原子百分比。(Ovshinky‘112专利,栏10~11)由另一研究者所评估的特殊合金包括Ge2Sb2Te5、GeSb2Te4、以及GeSb4Te7。(Noboru Yamada,”Potential of Ge-Sb-TePhase-change Optical Disks for High-Data-Rate Recording”,SPIE v.3109,pp.28-37(1997))更一般地,过渡金属如铬(Cr)、铁(Fe)、镍(Ni)、铌(Nb)、钯(Pd)、铂(Pt)、以及上述的混合物或合金,可与锗/锑/碲结合以形成一相变化合金其包括有可编程的电阻性质。可使用的存储材料的特殊范例,如Ovshinsky‘112专利中栏11-13所述,其范例在此被列入参考。
本发明参照至相变化材料而说明。然而,亦可使用其他存储材料(有时称为可编程材料)。如本发明中所使用的,存储材料为其电气性质如电阻等,可以通过施加能量而改变者。此改变可为阶梯性改变或一连续性改变,或为二者的组合。可使用于本发明其他实施例中的其他可编程电阻存储材料,包括掺杂N2的GST、GexSby、或其他以不同结晶态转换来决定电阻的物质;PrxCayMnO3、PrSrMnO、ZrOx、或其他利用电脉冲以改变电阻状态的材料;7,7,8,8-tetracyanoquinodimethane(TCNQ)、methanofullerene 6,6-phenylC61-butyric acid methyl ester(PCBM)、TCNQ-PCBM、Cu-TCNQ、Ag-TCNQ、C60-TCNQ、以其他物质掺杂的TCNQ、或任何其他聚合物材料其包括有以一电脉冲而控制的双稳定或多稳定电阻态。可编程电阻存储材料的其他范例,包括GeSbTe、GeSb、NiO、Nb-SrTiO3、Ag-GeTe、PrCaMnO、ZnO、Nb2O5、Cr-SrTiO3。
关于相变化随机存取存储装置的制造、构件材料、使用及操作请参考2005年6月17日申请、标题为「薄膜熔断器项变化随机存取存储器及其制造方法」、申请案号为11/155,067的美国专利案,律师登录号为MXIC 1621-1。
本发明之间还包括其他实施例。
Claims (24)
1.一种存储单元装置,包括一底电极与一顶电极,一相变化存储材料栓塞接触至所述底电极,以及一杯状导电构件其具有一周缘与一底部,该底部具有一开口,其中,该导电构件在所述周缘处接触至所述顶电极,以及该导电构件在所述开口处接触至所述相变化存储材料,以使存储单元中的导电路径是从顶电极穿过杯状导电构件,并穿过相变化存储材料栓塞到达底电极。
2.如权利要求1所述的存储单元装置,其中所述导电构件在所述周缘处的厚度介于25埃至200埃之间。
3.如权利要求2所述的存储单元装置,其中所述导电构件在所述周缘处的厚度为50埃。
4.如权利要求1所述的存储单元装置,其中所述导电构件与所述存储材料接触处的厚度介于25埃至200埃之间。
5.如权利要求4所述的存储单元装置,其中所述导电构件与所述存储材料接触处的厚度为50埃。
6.如权利要求1所述的存储单元装置,其中所述存储材料与所述底电极的接触区域其宽度介于20纳米至260纳米之间。
7.如权利要求6所述的存储单元装置,其中所述存储材料与所述底电极的接触区域其宽度为70纳米。
8.如权利要求1所述的存储单元装置,其中所述存储材料栓塞的高度介于20纳米至100纳米之间。
9.如权利要求8所述的存储单元装置,其中所述存储材料栓塞的高度为30纳米。
10.如权利要求1所述的存储单元装置,其中所述存储材料包括一硫属化物(Chalcogenide)材料。
11.如权利要求1所述的存储单元装置,其中所述存储材料包括一至少双稳态的合金。
12.如权利要求10所述的存储单元装置,其中所述存储材料包括一锗锑碲(GST)材料。
13.如权利要求10所述的存储单元装置,其中所述存储材料包括一由化学式GexSbyTez所表示的硫属化物,其中0≤x≤5;0≤y≤5;且0≤z≤10。
14.如权利要求13所述的存储单元装置,其中x∶y∶z=2∶2∶5。
15.如权利要求10所述的存储单元装置,其中所述存储材料包括一经掺杂的锗锑碲。
16.如权利要求15所述的存储单元装置,其中所述存储材料包括一以氮掺杂的锗锑碲。
17.如权利要求15所述的存储单元装置,其中所述存储材料包括一以硅掺杂的锗锑碲。
18.如权利要求15所述的存储单元装置,其中所述存储材料包括一以钛掺杂的锗锑碲。
19.一种用以制造一存储单元装置的方法,包括:
提供一基板其在一表面具有一介金属介电质,形成一第一电极层于所述介金属介电质之上,形成一电绝缘层于所述第一电极层之上,形成一停止层于所述电绝缘层之上,以及图案化各层以形成岛状底电极,每一所述岛状底电极包括一电绝缘元件与一停止元件;
沉积一填充材料于所述介金属介电质及所述岛状底电极之上;
移除所述填充材料至所述停止元件,剩余的所述填充材料包括一分隔层;
移除所述停止元件,形成一通孔,所述通孔由所述分隔层的一侧壁与所述电绝缘元件的一外露表面所定义;
沉积一导电材料以形成一导电薄膜于所述填充材料、所述分隔层的侧壁与所述电绝缘元件的外露表面之上;
沉积一电绝缘衬底材料于所述导电薄膜之上;
进行一非等向性蚀刻,以从所述分隔层的表面移除所述电绝缘衬底材料及所述导电薄膜,并形成一开口穿过所述电绝缘衬底材料、且穿过所述导电薄膜和所述电绝缘层;
沉积一相变化存储材料于所述开口中;
形成一氧化物覆盖层于所述相变化存储材料之上;以及
形成一顶电极于所述氧化物覆盖层以及所述分隔层的表面上。
20.如权利要求19所述的方法,其中所述填充材料沉积步骤包括沉积蚀刻选择性高于所述停止层的材料。
21.如权利要求19所述的方法,其中所述填充材料沉积步骤包括高密度等离子化学气相沉积。
22.如权利要求19所述的方法,其中所述停止层形成步骤包括沉积蚀刻选择性高于所述电绝缘层的材料。
23.如权利要求19所述的方法,其中所述停止层形成步骤包括沉积一材料,其化学机械研磨(CMP)速率高于所述填充材料。
24.如权利要求19所述的方法,其中所述非等向性蚀刻步骤包括,进行一反应性离子蚀刻以移除所述电绝缘衬底材料,利用一含氯化合物进行一化学蚀刻以形成穿过所述导电薄膜的所述开口,以及利用一含氟化合物进行一反应性离子蚀刻以形成穿过所述电绝缘层的所述开口。
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TWI324387B (en) | 2010-05-01 |
US8178405B2 (en) | 2012-05-15 |
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