TW575960B - Memory cell with trench transistor - Google Patents
Memory cell with trench transistor Download PDFInfo
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- TW575960B TW575960B TW91135418A TW91135418A TW575960B TW 575960 B TW575960 B TW 575960B TW 91135418 A TW91135418 A TW 91135418A TW 91135418 A TW91135418 A TW 91135418A TW 575960 B TW575960 B TW 575960B
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- 239000004065 semiconductor Substances 0.000 claims description 52
- 239000000463 material Substances 0.000 claims description 30
- 239000002800 charge carrier Substances 0.000 claims description 7
- 239000013078 crystal Substances 0.000 claims description 2
- 230000004888 barrier function Effects 0.000 claims 1
- 210000004027 cell Anatomy 0.000 claims 1
- 238000005253 cladding Methods 0.000 claims 1
- 239000004020 conductor Substances 0.000 claims 1
- 210000004508 polar body Anatomy 0.000 claims 1
- 238000002347 injection Methods 0.000 description 13
- 239000007924 injection Substances 0.000 description 13
- 230000005684 electric field Effects 0.000 description 8
- 239000000758 substrate Substances 0.000 description 4
- 230000000694 effects Effects 0.000 description 3
- 239000012535 impurity Substances 0.000 description 3
- 238000013459 approach Methods 0.000 description 2
- 238000005452 bending Methods 0.000 description 2
- 238000002513 implantation Methods 0.000 description 2
- 230000000739 chaotic effect Effects 0.000 description 1
- 150000001875 compounds Chemical class 0.000 description 1
- 238000010586 diagram Methods 0.000 description 1
- 239000002019 doping agent Substances 0.000 description 1
- 239000012634 fragment Substances 0.000 description 1
- 238000004519 manufacturing process Methods 0.000 description 1
- 238000005259 measurement Methods 0.000 description 1
- 238000012821 model calculation Methods 0.000 description 1
- 150000004767 nitrides Chemical class 0.000 description 1
- 239000004575 stone Substances 0.000 description 1
Classifications
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- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01L—SEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
- H01L29/00—Semiconductor devices specially adapted for rectifying, amplifying, oscillating or switching and having potential barriers; Capacitors or resistors having potential barriers, e.g. a PN-junction depletion layer or carrier concentration layer; Details of semiconductor bodies or of electrodes thereof ; Multistep manufacturing processes therefor
- H01L29/66—Types of semiconductor device ; Multistep manufacturing processes therefor
- H01L29/68—Types of semiconductor device ; Multistep manufacturing processes therefor controllable by only the electric current supplied, or only the electric potential applied, to an electrode which does not carry the current to be rectified, amplified or switched
- H01L29/76—Unipolar devices, e.g. field effect transistors
- H01L29/772—Field effect transistors
- H01L29/78—Field effect transistors with field effect produced by an insulated gate
- H01L29/792—Field effect transistors with field effect produced by an insulated gate with charge trapping gate insulator, e.g. MNOS-memory transistors
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01L—SEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
- H01L21/00—Processes or apparatus adapted for the manufacture or treatment of semiconductor or solid state devices or of parts thereof
- H01L21/02—Manufacture or treatment of semiconductor devices or of parts thereof
- H01L21/04—Manufacture or treatment of semiconductor devices or of parts thereof the devices having potential barriers, e.g. a PN junction, depletion layer or carrier concentration layer
- H01L21/18—Manufacture or treatment of semiconductor devices or of parts thereof the devices having potential barriers, e.g. a PN junction, depletion layer or carrier concentration layer the devices having semiconductor bodies comprising elements of Group IV of the Periodic Table or AIIIBV compounds with or without impurities, e.g. doping materials
-
- H—ELECTRICITY
- H10—SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
- H10B—ELECTRONIC MEMORY DEVICES
- H10B69/00—Erasable-and-programmable ROM [EPROM] devices not provided for in groups H10B41/00 - H10B63/00, e.g. ultraviolet erasable-and-programmable ROM [UVEPROM] devices
-
- H—ELECTRICITY
- H10—SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
- H10B—ELECTRONIC MEMORY DEVICES
- H10B99/00—Subject matter not provided for in other groups of this subclass
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- Engineering & Computer Science (AREA)
- Microelectronics & Electronic Packaging (AREA)
- Power Engineering (AREA)
- Physics & Mathematics (AREA)
- Condensed Matter Physics & Semiconductors (AREA)
- General Physics & Mathematics (AREA)
- Computer Hardware Design (AREA)
- Manufacturing & Machinery (AREA)
- Ceramic Engineering (AREA)
- Non-Volatile Memory (AREA)
- Semiconductor Memories (AREA)
Description
575960 ⑴ 坎、發明說明575960 ⑴ bump, invention description
(發明說明應敘明:發明所屬之技術領域、先前技術、内容、實施方式及圖式簡單說明) 本發明係關於一種具儲存電晶體之記憶體單元,其包括 在一半導體主體或半導體層頂部表面上的一閘極電極,該 電極位於一源極區與一汲極區之間的一溝渠中,該溝渠構 造在該半導體主體或層的半導體材料中》並在橫向於一縱 向方向、至少斷面對斷面呈現相同的斷面,其中一介電質 層(最好是一 ΟΝΟ層)作為儲存媒體位於該閘極電極與該半 導體材料之間。 ~(Explanation of the invention should state: the technical field to which the invention belongs, the prior art, the content, the embodiments, and the drawings are briefly explained) The present invention relates to a memory cell with a storage transistor, which includes a semiconductor body or a semiconductor layer on top A gate electrode on the surface, the electrode being located in a trench between a source region and a drain region, the trench being constructed in the semiconductor material of the semiconductor body or layer, and transverse to a longitudinal direction, at least The cross-section shows the same cross-section, and a dielectric layer (preferably a 10NO layer) is used as a storage medium between the gate electrode and the semiconductor material. ~
DE 100 39 441 Α1說明一種具溝渠電晶體之記憶體單元, 該溝渠電晶體位於構造在一半導體主體頂部表面的一溝 渠中。配置在該安裝在溝渠中的閘極電極、橫向鄰接源極 區及另一側的鄰接沒極區之間的是一氧化-氮化-氧化層 序列,其係用來在該源極和汲極捕獲電荷載子。該類電晶 體尤其適合於非揮發性記憶體(Non-Volatile Memory ; NVM)之 記憶體單元配置。具有程式化和抹除所需要之電場強度的 區域一般位於這些電晶體中的不同位置。因此,一旦電荷 在氮化物上程式化,要完全抹除它們是相當困難的。程式 化操作需要一電子注入。電子必須穿透氧化邊界層以達到 作為儲存層的氮化層。因此,電子必須是具有高動能的所 謂「熱電子」。該類電子只存在於該半導體材料表面閘極 電極之下的通道中電場強度非常強的地方。 - 附圖5從左到右顯示閘極電極4、閘極介電質9 (具體而言, 其可以是一 ΟΝΟ儲存層)以及具有通道區域5的鄰接半導 體材料。能量由在垂直方向繪製的一箭頭表示,並以該 575960 (2) 發明嬈明績頁DE 100 39 441 A1 describes a memory cell with a trench transistor, which is located in a trench formed on the top surface of a semiconductor body. Arranged between the gate electrode installed in the trench, the laterally adjacent source region, and the adjacent non-electrode region on the other side is an oxide-nitridation-oxide layer sequence, which is used between the source and drain The pole captures charge carriers. This type of electric crystal is particularly suitable for the memory cell configuration of non-volatile memory (NVM). Areas with the electric field strength required for stylization and erasure are typically located at different locations in these transistors. Therefore, once the charges are programmed on the nitride, it is quite difficult to completely erase them. The programming operation requires an electron injection. The electrons must penetrate the oxidized boundary layer to reach the nitrided layer as a storage layer. Therefore, the electron must be a so-called "thermoelectron" with high kinetic energy. This type of electron exists only where the electric field strength is very strong in the channel below the gate electrode on the surface of the semiconductor material. -Figure 5 shows from left to right the gate electrode 4, the gate dielectric 9 (specifically, it may be a 100N storage layer), and the adjacent semiconductor material with the channel region 5. Energy is represented by an arrow drawn in the vertical direction, and the 575960 (2) invention page
箭頭的方向增加。繪製的曲線a和b分別表示價帶的上限和 導電帶的下限。有兩種Fermi能量水準Efl和Ef2。上至這些能 量水準,依據Pauli原理只可單獨佔用的狀態充滿了電子。 如圖5所示之陰影區域,當Fermi能量水準Efl較低時,只有 少許電子位於該半導體材料邊界的導電帶中。可發現在一 較高Fermi能量水準Ef2的情形中,更多電子、且是更高能量 電子存在於該導電帶中。因此,較高能量電子更容易穿透 鄰接氮化儲存層的氧化層。 一The direction of the arrow increases. The drawn curves a and b represent the upper limit of the valence band and the lower limit of the conductive band, respectively. There are two Fermi energy levels Efl and Ef2. Up to these energy levels, the states that can only be occupied by Pauli's principle are filled with electrons. In the shaded area shown in Fig. 5, when the Fermi energy level Efl is low, only a few electrons are located in the conductive band at the boundary of the semiconductor material. It can be found that in the case of a higher Fermi energy level Ef2, more electrons and higher energy electrons are present in the conductive band. Therefore, higher energy electrons are more likely to penetrate the oxide layer adjacent to the nitrided storage layer. One
圖6顯示一典型電晶體結構的一斷面,其包括一源極區2 、一汲極區3、一閘極電極4、一閘極介電質9及通道區域5 。虛線表示該通道一電荷形成空間區的邊界。當施加程式 化該種電晶體所需要的電壓時,通過該通道區域的電子以 箭頭方向加速。箭頭的長度(不按比例繪製)表示電子的平 均動能。很明顯,電子的平均動能在向汲極區3靠近時迅 速增長。由於在向汲極區3靠近時電場強度迅速增長直到 恰好在汲極區之前的一點,該增長係極端超比例。當電子 到達通道區域5的末端時,它們的能量已足夠高以進入儲 存層。 在安置於一溝渠中的儲存電晶體例子中,具有適合於程 式化能量之電子所在的區域同樣位於該通道區域的末端 ,在此例中係結束於該溝渠底部的一側,其直接位於p f 電摻雜基板與導電摻雜汲極區域連接處之下。在源極區 在左和汲極區在右的一斷面中,該適合程式化區域位於溝 渠底部,大約在底部的右手側。 575960 (3) 發明說明績頁 對於抹除操作,需要一電洞注入(具有相反符號的電荷 載子),其唯有藉著閘極感應汲極洩漏(Gate Induced Drain Leakage ; GIDL)效應在一 n-MOSFET中獲得。該效應只發生在 汲極區的附近。因此,電子注入和電洞注入發生的位置未 必一致。在任何情形中,可使用一高電壓及/或非常長之 抹除時間來抹除該類記憶體單元。FIG. 6 shows a cross section of a typical transistor structure, which includes a source region 2, a drain region 3, a gate electrode 4, a gate dielectric 9 and a channel region 5. The dashed line indicates the boundary of a channel-forming space region of the channel. When the voltage required to program the transistor is applied, the electrons passing through the channel region are accelerated in the direction of the arrow. The length of the arrow (not drawn to scale) indicates the average kinetic energy of the electron. Obviously, the average kinetic energy of the electron increases rapidly as it approaches the drain region 3. Since the electric field strength rapidly increases as it approaches the drain region 3 to a point just before the drain region, the increase is extremely excessive. When the electrons reach the end of the channel region 5, their energy is high enough to enter the storage layer. In the example of a storage transistor placed in a trench, the region with the electrons suitable for stylized energy is also located at the end of the channel region. In this example, it ends on the side of the bottom of the trench, which is directly at pf. Below the connection between the electrically doped substrate and the conductive doped drain region. In the cross section of the source region on the left and the drain region on the right, the stylized region is located at the bottom of the trench, approximately on the right-hand side of the bottom. 575960 (3) Invention description For erasing operation, a hole injection (charge carrier with opposite sign) is required. It only has the effect of Gate Induced Drain Leakage (GIDL) effect. n-MOSFET. This effect occurs only near the drain region. Therefore, the positions where electron injection and hole injection occur may not be the same. In any case, a high voltage and / or a very long erase time can be used to erase such memory cells.
本發明的目標係構造一種具溝渠電晶體之記憶體單元 ,其程式化和抹除時間比該類型之傳統記憶體單元要顯· 著減少。 藉著具有如申請專利範圍第1、3、7和8項特徵之記憶體 單元可達成此項目標。The object of the present invention is to construct a memory cell with a trench transistor, the programming and erasing time of which is significantly less than that of a conventional memory cell of this type. This can be achieved by a memory unit with features such as patent application scope 1, 3, 7 and 8.
依據本發明,選擇相對於一區域(其中儲存層的電荷載 子在一抹除操作中被中性化)的溝渠深度,使得在一程式 化操作中,作用在電荷載子上的一電場成分在該相同區域 具有一最大值(該成分平行對準於該溝渠一壁面或底部的 切線並垂直於該溝渠的縱向方向)。這樣,該溝渠深度的 最佳化使得電子和電洞注入的位置相一致。源極區和汲極 區摻雜變化至相反符號(即基板或半導體主體導電類型的 符號)處的連接鄰接溝渠底部一彎曲區域或溝渠側壁一較 低彎曲區域。 圖1顯示二溝渠的一斷面,其產生在作為基板的一半躉 體主體1中或一基板上的一半導體層中。至少斷面對斷面 ,在溝渠縱向方向的溝渠斷面是相等的。因此,對於注入 平面正面的斷面和注入平面後面的斷面,圖1的顯示將是 575960 (4) 發明說明續頁 相同的。在本說明和申請專利範圍中,縱向方向指一垂直 斷面沿著該方向不改變。 - 在半導體主體1或半導體層相應頂部表面的一區域中, . 藉著混合一雜質形成一源極區2和一汲極區3 (此處作為左 手溝渠電晶體的一範例)。若半導體主體1是摻雜p導電, 則源極區2和 >及極區3相應形成為η +導電。相反播雜區域之 間的邊界(通常清楚表示)此處稱為連接1 4,它們在該半導 體材料中的位置係可偵測(例如使用SIMS)。在每個溝渠笮· · 安裝有一閘極電極4 (例如一多晶石夕電極)。在源極和沒極 區之下形成一通道區域5,與該半導體材料邊界表面上的 閘極電極相對。According to the present invention, the trench depth is selected relative to a region where the charge carriers of the storage layer are neutralized in an erase operation, so that in a stylized operation, an electric field component acting on the charge carriers is The same region has a maximum value (the component is aligned parallel to a tangent to a wall or bottom of the trench and perpendicular to the longitudinal direction of the trench). In this way, the trench depth is optimized so that the locations of electron and hole injection are consistent. The connection at the source and drain regions doped to opposite signs (ie, the sign of the substrate or semiconductor body conductivity type) adjoins a curved area at the bottom of the trench or a lower curved area at the sidewall of the trench. Fig. 1 shows a cross section of two trenches, which is generated in a half body body 1 as a substrate or in a semiconductor layer on a substrate. At least the cross section of the trench is equal to the cross section of the trench in the longitudinal direction of the trench. Therefore, for the section on the front of the injection plane and the section behind the injection plane, the display in Figure 1 will be the same as in 575960 (4) Invention Description Continued. In the scope of this description and patent application, the longitudinal direction means that a vertical section does not change along that direction. -In a region of the corresponding top surface of the semiconductor body 1 or the semiconductor layer, a source region 2 and a drain region 3 are formed by mixing an impurity (here, as an example of a left-hand trench transistor). If the semiconductor body 1 is doped with p-conductivity, the source regions 2 and > and the electrode region 3 are formed to be η + conductive, respectively. On the contrary, the boundaries between the dopant areas (usually clearly indicated) are referred to here as connections 1 4 and their position in the semiconductor material is detectable (for example using SIMS). A gate electrode 4 (for example, a polycrystalline stone electrode) is installed in each trench. A channel region 5 is formed below the source and gate regions, opposite the gate electrode on the boundary surface of the semiconductor material.
溝渠側壁6、8和底部7指面對該溝渠的半導體材料表面 。位於閘極電極4與半導體材料之間的是一介電質層9,其 作為閘極介電質並覆蓋該溝渠壁面和底部。該介電質層9 係作為儲存媒體而形成。要達到此目的,介電質層9最好 為多層,至少包括一儲存層1 1,其位於圖1所示範例中的 邊界層10、12之間。邊界層10、12係氧化物(具體而言,此 處為二氧化碎)’而儲存層1 1可以疋亂化物(此處為Si]N4)。 例如,在該半導體單元的操作中,對於程式化,在源極 區域有一 〇伏特電壓,在閘極電極4有一 9伏特電壓,而在 汲極區域3有一 6伏特電壓,對於抹除,在閘極電極有一二 8伏特電壓而在汲極區域有一 5伏特電壓。在圖式中,在溝 渠底部中的介電質層9從記憶體左溝渠中略去,其由相應 的虛線表示。為了方便以下說明,圖式中包括一水平箭頭 575960 (5) 發明說明續頁 2 2和一垂直箭頭2 3,其分別表示從源極至汲極的橫向方向 · 以及進入溝渠深度的垂直方向。此外,圖中還包括在連接 · 1 4高度處的溝渠壁面之間的間隔24,以及連接1 4高度之下 · 的溝渠深度2 5 (即從一連接1 4至溝渠最深點的整個溝渠垂 直尺寸)。 電壓分別經由附在注入平面的正面和背面的接點施加 至源極區2和汲極區3,而閘極電壓經由橫向(即在注入平 面中)延伸的字組線1 3供應。在程式化操作中,對於具# - φ 底部外形為一半圓柱的溝渠,該設定電壓產生一電場強度 分佈,其在所示斷面平面中與溝渠底部或壁面相切的成分 在連接下的右手側具有一最大值。 這些關係在圖2中重現,其顯示圖1所示斷面,用於對具 有半圓柱底部之溝渠進行模型計算。曲線分別代表該斷面The trench sidewalls 6, 8 and bottom 7 refer to the surface of the semiconductor material facing the trench. Located between the gate electrode 4 and the semiconductor material is a dielectric layer 9 which acts as a gate dielectric and covers the wall surface and bottom of the trench. The dielectric layer 9 is formed as a storage medium. To achieve this, the dielectric layer 9 is preferably multi-layered and includes at least a storage layer 11 located between the boundary layers 10, 12 in the example shown in FIG. The boundary layers 10 and 12 are oxides (specifically, they are dioxide fragments) ', and the storage layer 11 can be a chaotic compound (here, Si] N4). For example, in the operation of the semiconductor unit, for programming, there is a voltage of 10 volts in the source region, a voltage of 9 volts in the gate electrode 4, and a voltage of 6 volts in the drain region 3. The gate electrode has a voltage of 8 volts and a voltage of 5 volts in the drain region. In the figure, the dielectric layer 9 in the bottom of the trench is omitted from the left trench of the memory, which is indicated by the corresponding dashed line. In order to facilitate the following description, the drawing includes a horizontal arrow 575960 (5) Description of the invention continued on page 2 2 and a vertical arrow 23, which indicate the lateral direction from the source to the drain, and the vertical direction into the depth of the trench. In addition, the figure also includes the interval 24 between the walls of the ditch at the height of 14 and the depth of the ditch 2 5 below the height of 14 (that is, the entire ditch from a connection 14 to the deepest point of the ditch is vertical size). The voltage is applied to the source region 2 and the drain region 3 via contacts attached to the front and back sides of the implantation plane, respectively, and the gate voltage is supplied via a block line 13 extending laterally (that is, in the implantation plane). In a stylized operation, for a trench with #-φ bottom half-cylindrical shape, the set voltage generates an electric field intensity distribution that is right-handed under the connection of the components tangent to the bottom or wall of the trench in the section plane shown The side has a maximum value. These relationships are reproduced in Fig. 2, which shows the cross section shown in Fig. 1 for model calculation of a trench with a semi-cylindrical bottom. The curve represents the section
的線’在其上由前頭表不的電場成分Εγ具有相同的數值。 可從此處得出某些推論,其係關於在該斷面内延伸的分別 與溝渠壁面或底部相切之電場成分絕對值的大小。 可清楚看到在左手記憶體單元中(其在圖1中已預充電 用於使用對應電壓進行程式化),當箭頭22’之指向穿過形 成該底部之半圓柱的軸Α時,在通道縱向方向、大致在設 為向下旋轉30。之箭頭22的方向延伸的該場成分達到一最 大值。此時,發生該記憶體單元的有效程式化,而在抹 操作中的電洞注入在直接在汲極區3的連接1 4之上的區域 中發生。 圖3顯示依據本發明之該類最佳化記憶體單元,其中溝 -10- 575960 (6) 發明說明續頁 渠彎曲底部的相應區域位於汲極區3與相反摻雜半導體材 料之間的ρ η連接附近。在一相應示範性具體實施例中,不 需花很大氣力,可使用技術人士所熟悉的模型計算和模擬 及/或實驗性使用實現之結構元件而得出該最佳化記憶體 單元的準確尺寸。但對所有本發明範圍内的具體實施例不 可能都得出對應的數字資料。因此,現在將詳細解釋構成 本發明之原理。該技術指導之說明方式將使得熟悉技術人 士可製造該類記憶體單元。 一 最重要的是要明白,主要是溝渠底部的彎曲類型和溝渠 側壁的較低區域而不僅僅是通道長度決定了與溝渠壁面 相切對準的場成分的曲線。迄今為止的假設是:必須將溝 渠安裝至半導體材料足夠深使得溝渠壁面的大部分位於 源極和汲極區域之下。與之相反,在依據本發明的記憶體 單元中,一側面曲線位於溝渠的實際底部與實質上垂直的 側壁之間,其所在區域為抹除操作中電洞注入發生之處。 因此,藉著電荷載子注入來進行程式化和抹除的區域就直 接對準於該ρ η連接。要達到此目的,溝渠深度相應減小。 這顯示在圖3的斷面中,其中的參考字符具有上述圖中 參考字符的相同意義。在半導體主體1或半導體層頂部表 面與連接1 4 (其在源極區2或汲極區3與相反摻雜半導體材 料之間,但該半導體材料在實務中不必是一平面,而可A 構造成一定程度的不規則面)之間的源極區2和汲極區3之 垂直尺寸在該記憶體單元中只是比溝渠總垂直尺寸略微 小一點。使用SIMS決定該連接位置時,採用在某一面積上 575960 (7) 發明說明續頁 的平均值。 溝渠的垂直尺寸具有超過連接14的一向下懸垂,下文中 將稱之為溝渠的深度2 5。其測量是從溝渠中的連接1 4之位 準至溝渠底部的最深點(相對於該半導體主體或半導體層 頂部主要表面之平面)以垂直方向進行,即垂直於半導體 主體或層的頂部表面平面。The electric field component Eγ on which the line 'is represented by the front has the same value. Some inferences can be drawn from this regarding the magnitude of the absolute value of the electric field component that extends within the section and is tangent to the wall or bottom of the trench, respectively. It can be clearly seen that in the left-handed memory unit (which has been precharged in Figure 1 for stylization using the corresponding voltage), when the direction of the arrow 22 'passes through the axis A forming the bottom half cylinder, the channel In the longitudinal direction, the rotation is set to approximately 30 downwards. The field component extending in the direction of the arrow 22 reaches a maximum value. At this time, effective programming of the memory cell occurs, and hole injection in the erase operation occurs in a region directly above the connection 14 of the drain region 3. FIG. 3 shows an optimized memory cell of this type according to the present invention, in which the corresponding region at the bottom of the groove of the trench -10- 960960 (6) is located between the drain region 3 and the oppositely doped semiconductor material. η is connected nearby. In a corresponding exemplary embodiment, the accuracy of the optimized memory unit can be obtained by calculating and simulating and / or experimentally using implemented structural elements using a model familiar to the skilled person without much effort. size. However, it is impossible to obtain corresponding digital data for all the specific embodiments within the scope of the present invention. Therefore, the principles constituting the present invention will now be explained in detail. This technical guide will be described in a way that will allow a person skilled in the art to manufacture such memory cells. First, it is important to understand that it is mainly the type of bend at the bottom of the ditch and the lower area of the side wall of the ditch, not just the length of the channel that determines the curve of the field component aligned tangentially to the wall of the ditch. The assumption so far is that the trench must be mounted deep enough in the semiconductor material that most of the trench wall surface lies below the source and drain regions. In contrast, in the memory cell according to the present invention, a side curve is located between the actual bottom of the trench and the substantially vertical side wall, and the region thereof is where the hole injection occurs during the erase operation. Therefore, the area programmed and erased by the charge carrier injection is directly aligned with the ρ η connection. To achieve this, the trench depth is reduced accordingly. This is shown in the section of Fig. 3, where the reference characters have the same meaning as the reference characters in the figure above. Between the top surface of the semiconductor body 1 or the semiconductor layer and the connection 1 4 (it is between the source region 2 or the drain region 3 and the oppositely doped semiconductor material, but the semiconductor material need not be a plane in practice, but can be constructed in A The vertical dimension of the source region 2 and the drain region 3 between the surface of the memory cell is only slightly smaller than the total vertical dimension of the trench in the memory cell. When using SIMS to determine the connection position, the average value of the continuation sheet of the invention description is used in a certain area. The vertical dimension of the trench has a downward overhang beyond the connection 14 and will be referred to as the depth of the trench 25 hereinafter. The measurement is performed from the level of connection 14 in the trench to the deepest point at the bottom of the trench (relative to the plane of the top surface of the semiconductor body or semiconductor layer) in a vertical direction, that is, perpendicular to the plane of the top surface of the semiconductor body or layer .
在較佳示範性具體實施例中,該深度2 5最多只有在連接 14高度處的溝渠壁面間隔24(溝渠寬度)的一半大。取決於 溝渠斷面的相應幾何形狀選擇深度2 5,使得連接1 4在一區 域分別接觸到溝渠的壁面,其中橫向於一縱向方向之斷面 中的溝渠壁面的曲線具有一曲線半徑,其最多只有在連接 1 4高度處的溝渠壁面間隔2 4的三分之二大。 當溝渠底部具有一半徑為r的半圓柱外形時,連接1 4高 度處的溝渠壁面間隔24最多為該半徑的兩倍大(即最多為In a preferred exemplary embodiment, the depth 25 is at most only half of the trench wall spacing 24 (ditch width) at the height of the connection 14. The depth 2 5 is selected depending on the corresponding geometry of the trench section, so that the connections 1 4 respectively contact the wall surface of the trench in an area, wherein the curve of the trench wall surface in a cross section transverse to a longitudinal direction has a curve radius, which is at most Only two-thirds of the ditch wall surface at the height of the connection 14 is separated by 24. When the bottom of the ditch has a semi-cylindrical shape with a radius r, the distance 24 between the walls of the ditch at a height of 14 is at most twice the radius (that is, at most
2 r)。貫穿本範例,溝渠底部的曲線半徑為r,因此,深度 2 5較便利的最大值為r,儘管其最好再小一些。 當該半圓柱的半徑r為(例如)5 5奈米時,深度為5 5奈米 或更小一些。由於通道長度不能太小,可將3 0奈米的值作 為深度2 5的下限而儘量保持。設定該深度2 5為3 0奈米,溝 渠底部的弧(其可在連接14之下的斷面中看見並近似代表 通道長度)在半徑r設定為55奈米時等於120.88奈米,在f 徑r為70奈米時等於134.76奈米,在連接14高度處的溝渠壁 面間隔24在1: = 55奈米時等於97.98奈米,在1* = 70奈米時等於 114.89奈米;因此,在任何情形中,連接14鄰接溝渠壁面 -12- 575960 (8) 發明說明續頁 處該點的曲線半徑都小於在連接1 4高度處的溝渠壁面間 隔2 4的三分之二。2 r). Throughout this example, the radius of the curve at the bottom of the ditch is r, so the more convenient maximum of depth 25 is r, although it is better to be smaller. When the radius r of the semi-cylinder is, for example, 55 nm, the depth is 55 nm or less. Since the channel length cannot be too small, the value of 30 nanometers can be kept as the lower limit of the depth 2 5 as much as possible. Setting the depth 25 to 30 nm, the arc at the bottom of the ditch (which can be seen in the section below the connection 14 and approximately represents the length of the channel) has a radius r set to 55 nm and equals 120.88 nm, at f When the diameter r is 70 nm, it is equal to 134.76 nm. At the height of the connection 14, the channel wall spacing 24 is equal to 97.98 nm at 1: 55 nm and 114.89 nm at 1 * = 70 nm. Therefore, In any case, the connection 14 adjoins the trench wall surface -12- 575960 (8) Description of the invention The curve radius at this point on the following page is less than two thirds of the trench wall surface interval 24 at the height of the connection 14.
當源極區2和汲極區3的垂直尺寸為(例如)150奈米時,從 半導體主體或層的頂部表面測量的最佳總溝渠深度在半 徑r為55奈米時處於180奈米至205奈米的範圍内,在半徑I· 為70奈米時處於180奈米至220奈米的範圍内。在此範例中 ,溝渠底部不必具有一整個半圓柱的外形,溝渠側壁可直 接與彎曲底部相連或在連接上有一微小移動,使得在底部· 只有一半圓柱的一部分外形,即一中央角度小於180°的一 半圓柱的部分外形。When the vertical dimensions of source region 2 and drain region 3 are, for example, 150 nm, the optimal total trench depth measured from the top surface of the semiconductor body or layer is between 180 nm and 55 nm with a radius r of 55 nm. The range of 205 nanometers is in the range of 180 nanometers to 220 nanometers when the radius I · is 70 nanometers. In this example, the bottom of the ditch does not need to have an entire semi-cylindrical shape. The side wall of the ditch can be directly connected to the curved bottom or there is a slight movement in the connection, so that only a part of the shape of the half of the cylinder at the bottom, that is, a central angle less than 180 ° Part of the shape of a half cylinder.
溝渠深度必須相應調整以適應溝渠底部的其它曲線半 徑或溝渠底部的其它形狀。雜質濃度的水準也起一定作用 ,而且必要時可能要考慮通道區域5的額外實施方案。為 在溝渠更顯著彎曲點提高通道傳導性並減小電場的一實 施方案也使得在溝渠底部區域中提供一更彎曲曲線成為 可能,其中不發生電荷載子注入儲存層的情況。因此,提 供一有些錐形的溝渠底部以及將雜質摻雜入在下半導體 材料底部最深點區域中的一實施方案係在本發明的範圍 内。此處最好藉著選擇大於在連接14高度處的溝渠壁間隔 24—半的深度25來提供一更大通道長度。然而同樣是在此 範例中,在垂直於溝渠縱向方向的斷面中,在連接1 4鄰兔 溝渠壁的壁曲線的半徑最大為間隔2 4的三分之二。 在某些具體實施例中,溝渠深度2 5大大小於在連接1 4 高度處的溝渠壁面間隔24的一半可能是較有利的,尤其是 -13- 575960 (9) 發閱纖%績頁 當溝渠底部具有一較小彎曲或一平坦内部及十分彎曲之 側面部分,並且大部分壁面至少為大致垂直延伸,使得一 實質彎曲只存在於底部的較低側面。然而,在這些具體實 施例中,必須考慮到在一非常淺之深度2 5和一非常平坦之 溝渠底部情況下,通道長度可能不夠長,或由於該相當小 之通道長度抵消本發明部分最佳化目的。The trench depth must be adjusted accordingly to accommodate other curved radii at the bottom of the trench or other shapes at the bottom of the trench. The level of impurity concentration also plays a role, and additional implementations of channel region 5 may be considered if necessary. An embodiment to increase channel conductivity and reduce electric field at more significant bending points of the trench also makes it possible to provide a more curved curve in the bottom region of the trench, where charge carrier injection does not occur. Therefore, it is within the scope of the invention to provide an embodiment of a somewhat tapered trench bottom and doping impurities into the deepest point region of the bottom of the lower semiconductor material. It is preferred here to provide a greater channel length by selecting a depth 25 which is greater than the trench wall spacing 24-half at the height of the connection 14. However, also in this example, in a cross section perpendicular to the longitudinal direction of the ditch, the radius of the wall curve connecting the walls of the adjacent 14 ditch trenches is at most two thirds of the interval of 24. In some specific embodiments, it may be advantageous that the trench depth 25 is substantially less than half of the trench wall spacing 24 at the height of the connection 1 4, especially -13- 575960 (9) The bottom of the trench has a small curve or a flat interior and a very curved side portion, and most of the wall surface extends at least approximately vertically, so that a substantial curve exists only on the lower side of the bottom. However, in these specific embodiments, it must be taken into account that at a very shallow depth of 25 and a very flat trench bottom, the channel length may not be long enough, or because the rather small channel length offsets part of the invention best.化 purpose.
溝渠側壁可在其上部區域傾向於垂直(圖1中的箭頭2 3 ) 。圖4顯示一額外示範性具體實施例的一對應斷面,其t 溝渠側壁在其上部區域明顯傾斜,具有一相對於垂直方向 約5 ^的傾斜角。在該示範性具體實施例中,側壁6、8具有 恰好在溝渠底部7之上的狹窄區域1 5、1 7,以溝渠的縱向 方向延伸,在這些區域中,斷面内的側壁方向微微彎曲。 在側壁的較低區域1 6、1 8,在斷面内的壁面切線方向處於 一較大角度範圍,上至相對於垂直方向的10°。此處,溝 渠底部7相對略微彎曲,使得溝渠壁面的顯著較大彎曲區 域位於側壁較低區域1 6、1 8與溝渠底部7之間。 在該示範性具體實施例中,選擇溝渠深度2 5使得源極區 與相反摻雜半導體材料之間、或汲極區與相反摻雜半導體 材料之間的pn連接(連接14)大致處於該顯著彎曲的高度 或恰好在這高度之上。也可在此假設程式化發生在恰好在 具有最顯著彎曲區域之上的溝渠壁面區域中。 為說明之目的,在較低區域的介電質層9從圖4的右手溝 渠斷面中省去,其也是由虛線表示。圖中包括曲線半徑1 9 、2 0和2 1,其並非按照比例或精確繪製。這些長度只是為 -14- 575960 (ίο) 發明說明續頁 了說明在實際底部側面區域中的曲線半徑1 9非常小。側壁 的鄰接區域1 6、1 8具有一實質上較大曲線半徑2 0。底部7 的曲線半徑2 1同樣相當大。The side walls of the trench can tend to be vertical in its upper area (arrows 2 3 in Figure 1). FIG. 4 shows a corresponding cross section of an additional exemplary embodiment, the side wall of the t-ditch is obviously inclined in its upper region, and has an inclination angle of about 5 相对 with respect to the vertical direction. In this exemplary embodiment, the side walls 6, 8 have narrow areas 15, 17 just above the bottom 7 of the trench, extending in the longitudinal direction of the trench, in which the direction of the side wall in the section is slightly curved . In the lower regions 16 and 18 of the side wall, the tangent direction of the wall surface in the section is in a large angle range, up to 10 ° with respect to the vertical direction. Here, the trench bottom 7 is relatively slightly curved, so that the significantly larger curved area of the trench wall surface is located between the lower side regions 16 and 18 and the trench bottom 7. In this exemplary embodiment, the trench depth 25 is selected such that the pn connection (connection 14) between the source region and the oppositely doped semiconductor material or between the drain region and the oppositely doped semiconductor material is approximately at this significant The height of the bend may be just above this height. It can also be assumed here that stylization occurs in the area of the trench wall just above the area with the most significant bend. For illustrative purposes, the dielectric layer 9 in the lower region is omitted from the right-hand trench section of Fig. 4, which is also indicated by the dashed line. The graph includes curve radii 19, 20, and 21, which are not drawn to scale or accuracy. These lengths are just -14- 575960 (ίο) Description of the invention continued on the description that the radius of the curve 19 in the actual bottom side area is very small. Adjacent regions 16 and 18 of the side walls have a substantially larger curve radius 20. The curve radius 21 of the bottom 7 is also quite large.
觀看溝渠壁面的切線,其在橫向於溝渠縱向方向的注入 平面内延伸,由側壁形成的壁面部分可定義為較小的傾斜 角,最大為相對於垂直方向(箭頭23)的10。。如圖4所示具 體實施例的溝渠中,位於這些側壁與底部一最深點之間的 溝渠壁面部分具有圖4斷面(其與縱向方向垂直)内的一曲 線半徑,其在每一點都最多只有在連接1 4高度處的溝渠壁 面間隔2 4的一半大。連接1 4鄰接這些區域中的溝渠側壁。 假定言之,在抹除操作過程中電洞注入所發生區域至少 大致與溝渠壁面的最顯著彎曲區域相一致。因此,較有利 的是連接1 4鄰接溝渠側壁的一區域,其中彎曲半徑最多比 其在溝渠壁面具有的最小值大1 0 %。Looking at the tangent of the trench wall surface, which extends in the injection plane transverse to the longitudinal direction of the trench, the wall surface portion formed by the side wall can be defined as a small inclination angle, up to 10 relative to the vertical direction (arrow 23). . In the ditch of the specific embodiment shown in FIG. 4, the wall portion of the ditch located between these side walls and a deepest point at the bottom has a radius of a curve in the cross-section of FIG. 4 (which is perpendicular to the longitudinal direction). Only the ditch wall surface at the height of the connection 14 is half spaced by the distance 24. The connections 1 4 adjoin the trench walls in these areas. It is assumed that the area where the hole injection occurred during the erasing operation is at least approximately consistent with the most significant curved area of the trench wall surface. Therefore, it is more advantageous to connect an area adjacent to the side wall of the ditch, where the bending radius is at most 10% greater than the minimum value it has on the wall of the ditch.
記憶體單元最好具有圖中所示的鏡面對稱結構,因為在 此情形中,當施加電壓反轉時,程式化和抹除也可在位於 圖左側的儲存層區域中發生。 參考圖1至圖6,以上是該記憶體單元的詳細說明。 圖1:穿過二鄰接溝渠的一斷面示意圖。 圖2 :使用一模型來模擬圖1所示二溝渠的斷面,其具有 一向下電場成分(E-field-component)之曲線。 圖3和圖4 :依據本發明構造之記憶體單元之對應斷面。 圖5和圖6 :本說明簡介中所描述之圖式。 -15 - 575960 (ii) 式 代表 符號 說 明 1 半 導 體 主 體 2 源 極 區 3 汲 極 區 4 閘 極 電 極 5 通 道 區 域 ό、 8 溝 渠 側 壁 7 溝 渠 底 部 9 閘 極 介 電 質 10 、12 邊 界 層 11 儲 存 層 13 字 組 線 14 連 接 15 、17 狹 窄 域 16 > 18 較 低 區 域 19-21 曲 線 半 徑 22 水 平 箭 頭 22, 箭 頭 23 垂 直 箭 頭 24 間 隔 25 深 度 a、 b 曲 線 發明說明續頁The memory cell preferably has a mirror-symmetrical structure as shown in the figure, because in this case, when the applied voltage is reversed, stylization and erasure can also occur in the storage layer area on the left side of the figure. Referring to FIG. 1 to FIG. 6, the above is a detailed description of the memory unit. Figure 1: A schematic cross-section through two adjacent trenches. Figure 2: A model is used to simulate the cross section of the two trenches shown in Figure 1, which has a downward E-field-component curve. Figures 3 and 4: Corresponding sections of a memory cell constructed according to the present invention. Figures 5 and 6: The diagrams described in this introduction. -15-575960 (ii) Explanation of symbol of formula (1) Semiconductor body 2 Source region 3 Drain region 4 Gate electrode 5 Channel region, 8 Side wall of trench 7 Bottom of trench 9 Gate dielectric 10, 12 Boundary layer 11 Storage Layer 13 word line 14 connects 15 and 17 narrow area 16 > 18 lower area 19-21 curve radius 22 horizontal arrow 22, arrow 23 vertical arrow 24 interval 25 depth a, b curve invention description continued page
-16 --16-
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US10/022,654 US6661053B2 (en) | 2001-12-18 | 2001-12-18 | Memory cell with trench transistor |
DE10162261A DE10162261B4 (en) | 2001-12-18 | 2001-12-18 | Memory cell with trench transistor |
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TW575960B true TW575960B (en) | 2004-02-11 |
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JP (1) | JP4081445B2 (en) |
KR (1) | KR100554647B1 (en) |
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US7317222B2 (en) * | 2006-01-27 | 2008-01-08 | Freescale Semiconductor, Inc. | Memory cell using a dielectric having non-uniform thickness |
CN101908488B (en) * | 2009-06-08 | 2012-11-21 | 尼克森微电子股份有限公司 | Ditching type metal-oxide semiconductor assembly manufacturing method |
KR102002942B1 (en) * | 2013-04-18 | 2019-07-24 | 에스케이하이닉스 주식회사 | Nonvolatile memory device and method of fabricating the same |
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US5854501A (en) * | 1995-11-20 | 1998-12-29 | Micron Technology, Inc. | Floating gate semiconductor device having a portion formed with a recess |
DE19639026C1 (en) * | 1996-09-23 | 1998-04-09 | Siemens Ag | Self-aligned non-volatile memory cell |
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WO2003052812A3 (en) | 2003-11-06 |
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