TWI310233B - Trap memory with a modified drain/source voltage and the method for making the same - Google Patents

Trap memory with a modified drain/source voltage and the method for making the same Download PDF

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TWI310233B
TWI310233B TW95127761A TW95127761A TWI310233B TW I310233 B TWI310233 B TW I310233B TW 95127761 A TW95127761 A TW 95127761A TW 95127761 A TW95127761 A TW 95127761A TW I310233 B TWI310233 B TW I310233B
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layer
substrate
recess
electron
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TW200807628A (en
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Jyi Tsong Lin
Wei Ching Lin
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Univ Nat Sun Yat Sen
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Ι3Ί0233 九、發明說明: 【發明所屬之技術領域】 本發明係關於一種能陷記憶體(Trap Mem〇ry)及其製造 方法,特別是一種調變源/汲極電壓的新型能陷記憶體及 其製造方法。 【先前技術】 由快閃記憶體(FLASH)及電子抹除式唯讀記憶體 (EEPROM)技術衍生而出的石夕_氧化物_氮化物_氧化物·基板 (SONOS)記憶體架構,最早由施敏博士等人提出,集合美 =、歐洲、臺灣、日本及韓國的半導體業界及學界廣泛研 究及討論,但此種S0N0S仍有不少缺點,如建造於閉極端 的多層架構需消耗較大電壓,以在其下方導引感應出通道 層;儲存的電荷易逸散,對於沒有多層架構,尤其無絕緣 ^體的儲存媒介,電荷㈣逸散;另外對於將儲存機構建 造於下方的水平式氧化物.氮化物·氧化物(⑽〇)結構以改 善高操作電麼之元件,在製作上易會產生因多個光罩使用 下,上下層結構無法正確對齊的缺點,此外水平式的儲存 、’Ό構’易造成元件無法持續縮小的限^ (因 度和通道長度相關)。 構長 =於:位元的其㈣N〇s元件,除了需有較高的操 =卜:在兩電荷餘存區間若無有效隔離,會使儲存的 了逐無攸南密度電荷區擴散至低密度 的困難,芒I』 &成位疋判讀 力要做成隔離,除無法實現自我對齊的缺失外, ,驟亦嫌繁複;另外,建造於閘極端的多層架構需消 i 11758.doc 1310233 耗較大電壓,以在其下方導引感應出通道層,即便在讀取 模式時仍需有較大電壓操作,亦會有少數衝擊離子化產 生,並影響元件可信賴度及儲存有效時間;最後,對於水 平式ΟΝΟ結構,電荷分布過於分散,無法感應強電場以對 臨界電壓產生較大改變,使其判讀不易。 論文[Wen-Jer Tsai, Chih-Chieh Yeh, Nian-Kai Zous, Chen-Chin Liu, Shih-Keng Cho, Tahui Wang, Samuel C. Pan, Chih-Yuan Lu, "Positive Oxide Charge-Enhanced Read Disturb in a Localized Trapping Storage Flash Memory Cell" in IEEE TRANSACTIONS ON ELELCTRON DEVICES,VOL. 51, NO. 3, MARCH 20 04]揭示一種將水平 ΟΝΟ結構做至閘極端下方的SONOS元件,在水平結構夠長 時,在源極或汲極的高電壓寫入操作會導致電子碰撞游離 現象產生的區域不同,而使穿邃過閘極氧化層爾後陷入儲 存區的電子出現局部化的現象,但此種結構雖有上方ΟΝΟ 和通道完全切合的自我對齊特徵,惟元件在做微縮時,局 部化現象會逐漸消失,位元判讀視窗被壓縮,雙位元的功 能逸失;另外,因在閘極使用多層結構,會使寫入或抹除 的操作電壓過高,可能無法符合主流積體電路電氣要求。 論文[Rossella Ranica, Alexandre Villaret, Pascale Mazoyer, Stephane Monfray, Daniel Chanemougame, Pascal Masson, Arnaud Regnier, Cyrille N. Dray, Roberto Bez, and Thomas Skotnicki, "A New 40-nm SONOS Structure Based on Backside Trapping for Nano-scale Memories”]揭示一種 111758.doc 1310233 將水平麵結構做至間極端下方的s〇N〇s元件,此結構在 操作電壓上有效改善上篇論文所提及的元件結構,因上方 閘極並非使用多層結構’寫入或抹除的操作電屋不會過 而,但’如同上篇論文提及,在水平結構夠長時,在源極 或汲極的高電壓寫人操作會導致電子碰撞游離現象產生的 區域不同’而使穿邃過下方_的上部氧化層爾後陷入儲 存區的電子出現局部化的現象,惟元件在做微縮時,局部 化現象會因無有效隔離而互㈣散或干擾而_,位元判 讀視窗被㈣,雙位元的功能逸失n該結構在完成 下方水平ΟΝΟ結構後,欲建構出上方的閘極,會有自我對 準的問題,若閘極無法置於相對下方水平〇Ν〇結構的中央 位置’會使從源極及從汲極操作寫入時,局部化的現象不 對稱’位元判讀視窗被壓縮’此外’在一段長時間不做覆 寫(refresh)時,會因電荷逐漸擴散至另一端使在做單端抹 除時,不易完全抹除(under-erase)的缺點。 論文[Laurent Bqreuil,Luc Haspeslagh,Pieter BlommeΙ3Ί0233 IX. Description of the Invention: [Technical Field] The present invention relates to a trapable memory (Trap Mem〇ry) and a method of fabricating the same, and more particularly to a novel energy trapping source for a modulated source/drain voltage and Its manufacturing method. [Prior Art] The Xixia_Oxide_Nitrate_Oxide/Substrate (SONOS) memory structure derived from flash memory (FLASH) and electronic erasing read-only memory (EEPROM) technology, the earliest According to Dr. Shi Min and others, the semiconductor industry and academic circles in the United States, Europe, Taiwan, Japan, and South Korea have extensively studied and discussed, but such S0N0S still has many shortcomings, such as the multi-layer architecture built on closed extremes. Large voltage to guide the channel layer underneath; the stored charge is easily dissipated, for a storage medium without a multi-layer structure, especially without insulation, the charge (4) is dissipated; in addition, the storage mechanism is built below the level The structure of the oxide, the oxide and the oxide ((10) 〇) is used to improve the high-operational components. In the fabrication, it is easy to produce the disadvantage that the upper and lower layers cannot be properly aligned due to the use of multiple masks. Storage, 'Ό' is a limitation that can cause the component to continue to shrink (depending on the length of the channel). The length of the structure = in: the (four) N〇s component of the bit, in addition to the higher operation = Bu: if there is no effective isolation in the remaining interval of the two charges, the stored density-free region of the south of the charge will be diffused to a low The difficulty of density, Mang I』 & 成 疋 疋 疋 疋 疋 疋 疋 疋 , 疋 , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , 11 11 11 11 A large voltage is consumed to guide the channel layer underneath, even if a large voltage operation is required in the read mode, a small amount of impact ionization is generated, which affects component reliability and storage effective time; Finally, for the horizontal ΟΝΟ structure, the charge distribution is too scattered, and it is impossible to induce a strong electric field to make a large change to the threshold voltage, making it difficult to interpret. Paper [Wen-Jer Tsai, Chih-Chieh Yeh, Nian-Kai Zous, Chen-Chin Liu, Shih-Keng Cho, Tahui Wang, Samuel C. Pan, Chih-Yuan Lu, "Positive Oxide Charge-Enhanced Read Disturb in a Localized Trapping Storage Flash Memory Cell" in IEEE TRANSACTIONS ON ELELCTRON DEVICES, VOL. 51, NO. 3, MARCH 20 04] reveals a SONOS component that uses a horizontal ΟΝΟ structure to the bottom of the gate. When the horizontal structure is long enough, The high-voltage writing operation of the source or the drain causes the area of the electron collision free phenomenon to be different, and the electrons that have entered the storage area after passing through the gate oxide layer are localized, but the structure has the above自我 Self-alignment features that are completely compatible with the channel. However, when the component is miniaturized, the localization phenomenon will gradually disappear, the bit interpretation window is compressed, and the double-bit function is lost. In addition, because the gate structure is used in the gate, The write or erase operation voltage is too high and may not meet the electrical requirements of the mainstream integrated circuit. Papers [Rossella Ranica, Alexandre Villaret, Pascale Mazoyer, Stephane Monfray, Daniel Chanemougame, Pascal Masson, Arnaud Regnier, Cyrille N. Dray, Roberto Bez, and Thomas Skotnicki, "A New 40-nm SONOS Structure Based on Backside Trapping for Nano -scale Memories"] reveals a 111758.doc 1310233 s〇N〇s element that makes the horizontal structure below the extreme. This structure effectively improves the component structure mentioned in the previous paper in terms of operating voltage, due to the upper gate It is not the use of a multi-layer structure to write or erase the operation of the electric house will not pass, but as mentioned in the previous paper, when the horizontal structure is long enough, the high voltage writing operation at the source or the bungee will lead to electronics. The area generated by the collision free phenomenon is different, and the electrons that have penetrated into the storage area after the upper oxide layer of the lower layer are localized. However, when the components are miniaturized, the localization phenomenon may be due to the absence of effective isolation. Or interfere with _, the bit interpretation window is (four), the function of the double bit is lost n. After the structure is completed, the structure is to be constructed. The gate has self-alignment problems. If the gate cannot be placed in the center of the horizontal 〇Ν〇 structure, it will make the localization phenomenon asymmetrical when writing from the source and the drain. The bit interpretation window is compressed 'when' is not overwritten for a long time, it will spread to the other end due to the charge, so it is not easy to completely erase (under-erase) when doing single-ended erasure. Paper [Laurent Bqreuil, Luc Haspeslagh, Pieter Blomme

Dirk Wellekens, Joeri De Vos, Martino Lorenzini, and Jan Van Houdt, "A New scalable Self-Aligned Dual-Bit Split-Gate Charge-Trapping Memory Device" in IEEEDirk Wellekens, Joeri De Vos, Martino Lorenzini, and Jan Van Houdt, "A New scalable Self-Aligned Dual-Bit Split-Gate Charge-Trapping Memory Device" in IEEE

TRANSACTIONS ON ELECTRON DEVICES,VOL. 52, NO 1 0,OCTOBER 2005.]揭示一種將水平〇NO結構做至閘極端 下方的SONOS元件’惟此結構用隔離技術’確保不同區域 儲存的電荷不會因濃度不同而擴散或因電場交越而形成位 元間干擾,使閘極的長度恰巧和通道長度相等,亦即控制 111758.doc 1310233 閘極兩端和源/汲極定義區的盡頭恰好對齊 ,A ^ 4一社要做出 °立於閘控端的兩側,每個位元的儲存區時,勢必要使 用另一層光罩定義,這樣會造成兩個位元的儲存區長度不 同,甚至在閘控端進一步微縮時,有可能因光罩偏移稍 大,使某一位元的儲存區完全消失,此外,閑極長度是特 徵長度,勢必使此結構在微小化時受到較大限制,再者, 此結構仍有要使用多層結構,會使寫入或抹除的操作電壓 過高’可能無法符合主流積體電路電氣要求。 論文[HWan Ch0, Tai-su Parki, Si Y〇ung Choi,J〇ng DukTRANSACTIONS ON ELECTRON DEVICES, VOL. 52, NO 1 0, OCTOBER 2005.] Reveals a SONOS component that uses a horizontal 〇NO structure below the gate terminal. 'This structure uses isolation technology' to ensure that the charge stored in different regions is not concentrated. Diffusion or inter-bit interference due to electric field crossover, so that the length of the gate coincides with the length of the channel, that is, control 111758.doc 1310233 The end of the gate and the end of the source/drain definition area are just aligned, A ^ 4 a community to make ° stand on both sides of the gate, the storage area of each bit, it is necessary to use another layer of mask definition, which will result in different storage areas of two bits, even in the gate When the controller is further reduced, there may be a slight deviation of the mask, so that the storage area of a certain bit completely disappears. In addition, the length of the idle pole is the characteristic length, which is bound to make the structure more limited when miniaturized. However, this structure still has to use a multi-layer structure, which will make the writing or erasing operation voltage too high 'may not meet the electrical requirements of the mainstream integrated circuit. Paper [HWan Ch0, Tai-su Parki, Si Y〇ung Choi, J〇ng Duk

Lee, and Jong-Ho Lee'"Body-Tied Double-Gate SONOS Flash (Omega Flash) Memory Device Built 〇n Bulk Si Wafer", in Semiconductor R&D Center, SamsungLee, and Jong-Ho Lee'"Body-Tied Double-Gate SONOS Flash (Omega Flash) Memory Device Built 〇n Bulk Si Wafer", in Semiconductor R&D Center, Samsung

Electronics Co.,Ltd ]欲利用雙邊閘極,甚至多邊閘極來增 加驅動電流,加強通道末端的空乏區内產生的高速碰撞解 離效果’此立意頗佳,但欲形成雙邊閘極,甚至多邊閘極 時’或其他較複雜的閘極結構,不同面的閘極間產生自我 對齊的問題’此問題在元件微縮後更加嚴重,不同面的閘 極的相對幾何位置往往不能因設計者之要求精確達成,此 係因光罩在小刻度的對準時無法達到絕對精準的原因,這 樣會造成不必要的加熱效應,甚至使同一晶圓内的不同 SONOS元件會有不同的臨界電壓,而大大降低該創意的價 值’此在製做出雙邊閘極,甚至多邊閘極的SONOS嘗試中 會碰到的自我對齊問題。 論文[Rob van Schaijk,Michiel van Duuren, Pierre 111758.doc .10· 1310233Electronics Co., Ltd. wants to use bilateral gates and even multilateral gates to increase the drive current and enhance the high-speed collision dissociation effect in the depletion zone at the end of the channel. This is a good idea, but it is necessary to form a bilateral gate or even a multilateral gate. Extremely 'or other more complex gate structures, self-alignment between the gates of different faces'. This problem is more serious after the components are miniature, and the relative geometrical positions of the gates of different faces are often not precisely determined by the designer. This is achieved because the reticle cannot be absolutely accurate due to the alignment of the small scale, which will cause unnecessary heating effects, and even different threshold voltages in different SONOS components in the same wafer will greatly reduce the The value of creativity 'this is the self-alignment problem that will be encountered in the SONOS attempt of bilateral gates and even multilateral gates. Paper [Rob van Schaijk, Michiel van Duuren, Pierre 111758.doc .10· 1310233

Goarin, Wan Yuet Mei, Kees van der Jeugd, "Reliability of embedded SONOS memories", in IEEE 2004.]揭示於閘極下 方形成一儲存區域的SONOS元件,此為SONOS元件的離 形’沒有自我對齊的問題,無論是閘極對通道,或閘極對 做為儲存區的ΟΝΟ結構而言,但此元件僅能做為一位元的 儲存記憶體。Goarin, Wan Yuet Mei, Kees van der Jeugd, "Reliability of embedded SONOS memories", in IEEE 2004.] reveals a SONOS component that forms a storage region under the gate, which is the off-shape of the SONOS component. The problem, whether it is the gate-to-channel, or the gate pair, is the storage structure of the storage area, but this component can only be used as a one-dimensional memory.

美國專利公開第2006/0,068,546號揭示一種每位元皆能 完全隔離的SONOS元件,利用先將0Ν0堆疊而成,再以一 光罩定義挖出一井,於井兩侧做出電子能陷區(spacer), 再依次以閘極氧化層,閘極矽化層依次水平填滿該井,如 此的確可以使每位元皆能完全隔離,但在以一光罩定義挖 出一井以分隔兩個位元儲存區時,會發生儲存區大小不 均’此在元件微縮時會益加嚴重,甚至在光罩偏移過大 時’會造成某一位元儲存區完全消失的可能,另外,若填 井過程中強調水平,則會增加製程難度,此外,該井在電 子能陷區完成後’形成一倒三㈣,若有少數碰接游離電 何:動至此井下方尖端’易形成尖端放電,此非預期中之 電何累積可能會比兩側電荷儲存區電荷改變臨界電U.S. Patent Publication No. 2006/0,068,546 discloses a SONOS component that can be completely isolated per bit, by first stacking 0Ν0, and then dug a well with a mask definition to make electron energy on both sides of the well. The trap, in turn, the gate oxide layer and the gate deuteration layer fill the well horizontally, so that each bit can be completely isolated, but a well is dug out by a mask definition to separate In the case of two bit storage areas, the size of the storage area will be uneven. 'This will be more serious when the component is miniature, and even when the mask is too large, it will cause a certain bit storage area to completely disappear. In addition, If the level is emphasized during the filling process, it will increase the difficulty of the process. In addition, after the completion of the electron energy trapping area, the well will form a three-to-three (four). If there is a small amount of contact with the free electricity, move to the lower tip of the well. Discharge, the accumulation of this unexpected electricity may change the critical charge of the charge in the charge storage area on both sides.

有影響力,此外,M e A 閘極長度是特徵長度,勢必使此結構在 =、化時受到較大限制,再者,此結構仍有要使用多層結 會使寫入或抹除的操作電壓過高,可能無法符合主流 積體電路電氣要求。 寸。微 美國專利公開第2〇〇4/〇,2〇7,_號亦揭示 齊功能的FLASH元件 ,、自我對 丁 ,、马—皁一位7L之FLASH元件外, 111758.doc 1310233 但具有自我對齊的效果’惟此種架構無法在幾近相同的光 罩使用數目上而能完成較為複雜的結構,以達成多位元儲 存,而增進效能及位元集積度的功效。 美國專利公開第2002/0,004,291號揭示一種每位元皆能 完全隔離的S0N0S元件,和美國專利公開第 2006/M6M46號相似’不同是它先以光罩形成閘極,再 用閘極田做光罩功旎去切隔出使每位元皆能完全隔離的Influential, in addition, the length of the gate of the Me A is the characteristic length, which is bound to make the structure more restricted in the =, and the structure still has to use multiple layers of junctions to cause writing or erasing operations. If the voltage is too high, it may not meet the electrical requirements of the mainstream integrated circuit. Inch. Micro-US Patent Publication No. 2〇〇4/〇, 2〇7,__ also reveals the functional FLASH component, self-pairing, and horse-soap one 7L FLASH component, 111758.doc 1310233 but with self The effect of alignment 'only this architecture can not complete the more complex structure in the same number of reticle use, to achieve multi-bit storage, and improve the efficiency and the efficiency of the bit accumulation. U.S. Patent Publication No. 2002/0,004,291 discloses a SONOS component that can be completely isolated per bit, similar to U.S. Patent Publication No. 2006/M6M46, which differs in that it first forms a gate with a photomask and then uses a gate field to make light. The cover is cut and separated so that each bit can be completely isolated.

SONOS元件’惟始之光罩形成μ極就必須確保能置於 遠ΟΝΟ架構中纟,否則接下來欲形成兩個位元儲存區時, 會發生儲存區大小不均,此在元件微料會益加嚴重,甚 至,光罩偏移過大時,會造成某—位_存區完全消失的 可能’此外’閘極長度是特徵長度’勢必使此結構在微小 化時受到較大限製’再者,&結構仍有要使用多層結構, 會使寫人或抹除的操作電壓過高,可能無法符合主流積體 電路電氣要求。 美國專利公開第2〇〇5/〇,1〇6,793號亦為一單一位元之 FLASH元件,此結構大致上和傳統FLASH元件雛形相同, 利料閘極氧化層、FLA_、上方阻絕氧化層、問控層 一次堆積完成’再以光罩定義㈣,雖有良好自我對齊的 效果,惟此種架構無法在幾近相同的光罩使用數目上而能 元成較為複雜的結構,以達成多位元儲存,而增進效能, 位元集積度的功效。 參考中華民國專利公告第237349號及中華民國專利公告 第239073號,皆為揭*二位元的s〇N〇s元件,都屬水平式 H1758.doc -12· 1310233 的三層結構’並有效隔離’此將水平式儲存機構設於閉極 T方的元件,仍有二位元儲存區長度在光罩定義時不均, 操作電壓過大’及對元件微縮造成限制。The SONOS component 'the beginning of the mask to form the μ pole must ensure that it can be placed in the remote structure. Otherwise, if the next two bit storage areas are to be formed, the storage area will be unevenly sized. It is serious, even if the reticle offset is too large, it will cause the _ _ storage area to completely disappear. The 'other' gate length is the characteristic length', which is bound to make the structure more restricted when miniaturized. The & structure still has to use a multi-layer structure, which will make the write or erase operation voltage too high, and may not meet the electrical requirements of the mainstream integrated circuit. U.S. Patent Publication No. 2/5/1,6,793 is also a single-bit FLASH component. This structure is substantially the same as the conventional FLASH component, and the gate oxide layer, FLA_, upper blocking oxide layer, The control layer is stacked once and finished. 'With the mask definition (4), although there is a good self-aligning effect, this architecture cannot be used in a relatively complicated structure in the same number of masks to achieve multiple positions. Meta-storage, while improving performance, the effect of bit-integration. Refer to the Republic of China Patent Bulletin No. 237349 and the Republic of China Patent Bulletin No. 239073, both of which are s*N〇s components of the two-dimensional, all of which are of the three-layer structure of horizontal H1758.doc -12· 1310233 and effective Isolation 'This is a component with a horizontal storage mechanism set on the closed-pole T side. There are still two-dimensional storage area lengths that are uneven when the mask is defined, the operating voltage is too large' and the component shrinkage is limited.

❿ 美國專利公開第厕/〇,285,177號,亦為閘極下方形成 一儲存區域的SONGS元件,但以中間的通道材質去分隔兩 個位元儲存區時’會發生儲存區大小不均,此在元件微縮 時會益加嚴重,甚至在光罩偏移過大時,會造成某一位元 儲存區完全消失的可能,用光罩在閘極做^義日夺,會有對 準問題,使位元儲存區在微縮時,會出現問題。 美國專利公開第2_/M23,513號,則是做出大問極, 並在大閘極挖出—井,利用側壁殘餘留下兩個位元健存 區’再利用沉積時井端上方沉陷做自動對齊閘極,此概念 在對準上確有優,點,但仍存多層閘極消耗較大電壓,另外 閘極為特徵長度,在微縮過程,因此兩位元逐漸靠近,會 壓縮微縮可能性。 美國專利公開第2005/0,255,657號揭示利用連續沉積三 層或多層的結構後’再以光罩定義,蝕刻過程中留下側 壁’但若光罩無法恰好將凸起上方之層狀結構蝕刻掉,而 剛好留下側壁欲留的多層結構,此元件效能會降低。 美國專利公開第2005/0,242,391號,如同上則揭示的專 利,亦先連續沉積三層或多層的結構後,再以光罩定義出 閘極進行切割,使在閘極下方形成一儲存區域的SONOS元 件’此為單—位元SONOS,不具擴充性,此外,如同先前 提及’多層閘極仍需要一較大操作電壓。 111758.doc •13· 1310233 由以上例子可以發現’在不同的論文和專利中,都有針 :發明人於一開始所提出的’發展8〇刪元件所面臨的困 兄及問題,如建造於閘極端的多層架構需消耗較大電壓; 儲存的電荷易逸散’對於沒有多層架構或無絕緣覆體的儲 存媒介,電荷極易逸散;對於將儲存機構建造於下方的水 平式ΟΝΟ結構以改善高操作電壓之元件的製作上需要多光 罩使用’上下層結構在微縮時會無法正確對齊;水平式的 儲存結構也造成元件縮小的限制(因此水平結構長度和通 道長度相關);另外對於兩位元的其他s〇N〇s元件,在兩 電荷儲存區間無有效隔離會使儲存的電荷擴散而造成位元 判讀視窗縮減,若要做成隔離,除無法實現自我對齊的缺 失外’製成步驟亦嫌繁複;最後’對於水平式咖結構,' 電荷分布分散,可能合成電場不對臨界電壓產生大改變或 使雙位元概念減念。 因此,有必要提供一創新且富進步性的調變源/汲極電 壓的能陷記憶體及其製造方法,以解決上述問題。 【發明内容】 本發明之主要目㈣提供一種調變源/汲極電遂的能陷 s己憶體之製造方法’包括以下步驟: (a) 提供一基板,該基板具有一表面; (b) 於該基板之該表面上形成一凹槽,該凹槽具有二側 壁及一底部; (c) 形成一電子儲存層於該基板之該表面及該凹槽上; (d) 部分移除該電子儲存層以形成二個不連續之電子能 111758.doc -14- 1310233 陷區(或電子儲存層),且暴露出該基板之該表面及該凹槽 之該底部,該等電子能陷區係分別位於該凹槽之二側壁 上,且該等電子能陷區間具有一間距; (e) 形成一導電層於該基板之該表面、該等電子能陷區及 該凹槽之該底部上’ I亥導電層之上表面具有_閘極 區; (f) 形成一閘極氧化層於該導電層上; (g) 形成一閘極矽化層於該閘極氧化層上; (h) 部分移除該閘極石夕化層以留下—殘时於該閑極凹 陷區之相對位置上; ⑴成長該殘留矽’以形成一閘極,其中該閘極之水平寬 度係小於該等電子能陷區間之該間距; (J)形成一閘極保護層於該閘極及該閘極氧化層上;及 ㈨形成一源極及一汲極’其中該源極及該汲極係位於 該導電層相對於該等電子能陷區之内側。 ▲本發明之另一目的係提供一種調變源/汲極電壓的能陷 隐體包括基板、二個不連續之電子能陷區、—導電 :二-閘極氧化層、一閘極、一源極及一汲極。該基板呈 -凹槽’該凹槽具有二側壁及一底部,該等側壁係為對 °亥等電子能陷區係用以儲存電子,且分別位於 該凹槽之側壁上’,亥等電子能陷區間具有-間距。該導電 =位於該基板之該表面、該等電子能陷區及該凹槽之該 =’料電層之上表面具有一問極凹陷區。該 化層係位於該導電層上。該閑極係位於該間極氧化層上, 111758.doc • 15 · !310233 且相對於該閘極凹陷區,該閘極之水平寬度係小於該等電 子忐陷區間之該間距。該源極及一汲極係位於該導電層, ; 且分別位於該閘極之二側,該源極及該汲極係位於該等電 , 子月b陷區之内側。 在本發明中’該等電子能陷區和上層的通道及該閘極可 產生完全的自我對齊之效果。另外,該分離垂直式之電子 能陷區結構將不會對通道長度的微縮造成侷限,又因並非 _ 在閘極端建造的多層架構,不需消耗較大閘極電壓。在操 作上,又因較小的操作電壓,對於因高電場而產生的額外 電性效果有較強抑制效用。而且,因為此對分離垂直式之 電子能陷區結構彼此間有該閘極氧化層及該導電層做有效 隔離,不會有位元間彼此互相干擾,及極佳的阻絕因電荷 分布濃度不均造成的擴散現象並導致判讀困難甚至錯誤之 It況。本發明之垂直式架構在上端有尖端電荷累積,會產 生較強電場以調變在次臨界區(sub thresh〇ld 時, _ 作用在源7汲極的電壓,構成位元間較大的判讀視窗。 、 此外,本發明係利用在該源極及該汲極外側製作出一對 稱垂直的電子儲存區(即該等電子能陷區),該電子儲存區 ^ 會依所保持的電子產生的合成電場去調變真正做用在該源 極及該沒極的電場而產生判讀性,此電子儲存區較遠離衝 撞離子化區,故可以防止讀取時的干擾,為一可靠的記憶 體元件。 【實施方式】 參考圖1至圖〗1,顯示根據本發明調變源/汲極電壓的能 111758.doc 16 1310233 陷記憶體之製造方法之示意圖。首先參考圖丨,提供 板1,該基板1具有一表面11。在本實施例中,該基板1 ( 為一石夕覆絕緣(Silicon-On-Insulator,SOI)基板,其勺括 第一晶圓12、一氧化層13及一第二晶圓14,該氧化層=係 夾設於該第一晶圓12及該第二晶圓14之間。 4 』以理解的 是,該基板1也可以是單一晶圓。 參考圖2,於該基板1之該表面11上形成-凹槽15,該凹❿ US Patent Publication No. 285/177, which also forms a storage area SONGS element under the gate, but when the middle channel material is used to separate the two bit storage areas, 'the storage area size will be uneven. This will increase the severity of the component when it is miniature. Even when the mask is too large, it will cause the loss of a certain bit storage area. The use of a photomask in the gate will result in alignment problems. There is a problem when the bit storage area is being miniaturized. U.S. Patent Publication No. 2_/M23,513, is to make a big question, and excavate the well at the gate, using the sidewall residue to leave two bit-storage areas' to reuse the sedimentation above the well end. Automatically aligning the gate, this concept is excellent in alignment, but the multi-layer gate still consumes a large voltage, and the gate is extremely characteristic length. During the miniaturization process, the two elements are gradually approaching, which will compress the possibility of miniaturization. . US Patent Publication No. 2005/0,255,657 discloses the use of a continuous deposition of three or more layers of structure, which is defined by a reticle, leaving a sidewall during etching, but if the reticle fails to etch away the layered structure above the bump, The effectiveness of this component is reduced by leaving the multilayer structure that the sidewall wants to leave. U.S. Patent Publication No. 2005/0,242,391, the entire disclosure of which is incorporated herein by reference in its entirety, the disclosure of the entire disclosure of the entire disclosure of the disclosure of the entire disclosure of the disclosure of the disclosure of the disclosure of the disclosure of the disclosure of The component 'this is a single-bit SONOS, which is not scalable. In addition, as mentioned earlier, 'multilayer gates still require a large operating voltage. 111758.doc •13· 1310233 From the above example, we can find that 'in different papers and patents, there are needles: the inventor’s initial development of the problem of developing 8 〇 deleting components and problems, such as built in The multi-layer architecture of the gate terminal consumes a large voltage; the stored charge is easily dissipated. 'For a storage medium without a multilayer structure or without an insulating body, the charge is easily dissipated; for a horizontal crucible structure in which the storage mechanism is built below The fabrication of components that improve high operating voltages requires the use of multiple masks. 'The upper and lower layers will not be properly aligned during miniaturization; the horizontal storage structure also limits the component shrinkage (and therefore the horizontal structure length and channel length); The other two s〇N〇s components have no effective isolation in the two charge storage intervals, which will cause the stored charge to spread and cause the bit reading window to be reduced. If it is to be isolated, it cannot be self-aligned. The steps are also complicated; finally, for the horizontal coffee structure, the charge distribution is dispersed, and the synthetic electric field may not change the threshold voltage. Or to study the concept of double bit Save. Therefore, it is necessary to provide an innovative and progressive modulation source/bungee voltage capable memory and its manufacturing method to solve the above problems. SUMMARY OF THE INVENTION The main object (4) of the present invention provides a method for manufacturing a modulated source/drain electrode, which comprises the following steps: (a) providing a substrate having a surface; (b) Forming a recess on the surface of the substrate, the recess having two sidewalls and a bottom; (c) forming an electron storage layer on the surface of the substrate and the recess; (d) partially removing the An electron storage layer to form two discontinuous electron energy 111758.doc -14-1310233 traps (or electron storage layers), and exposing the surface of the substrate and the bottom of the recess, the electron trapping regions Each of the two sidewalls of the recess is disposed on the sidewall of the recess, and the electron trapping region has a pitch; (e) forming a conductive layer on the surface of the substrate, the electron trapping region, and the bottom of the recess 'I has a _ gate region on the upper surface of the conductive layer; (f) a gate oxide layer is formed on the conductive layer; (g) a gate bismuth layer is formed on the gate oxide layer; (h) Removing the gate layer to leave a relative position in the recessed region; (1) growing the residual 矽' to form a gate, wherein the gate has a horizontal width smaller than the spacing of the electron energy trapping regions; (J) forming a gate protective layer on the gate and the gate oxide layer And (9) forming a source and a drain electrode, wherein the source and the drain are located inside the conductive layer relative to the electron trap. ▲ Another object of the present invention is to provide a modulated source/drain voltage capable recessed body comprising a substrate, two discontinuous electron energy trapping regions, conductive: two-gate oxide layer, one gate, one Source and a bungee. The substrate has a groove-shaped groove having two sidewalls and a bottom portion, and the sidewalls are used for storing electrons in the electron energy trapping region, and are respectively located on the sidewall of the groove. Can trap the interval with - spacing. The conductive layer is located on the surface of the substrate, the electron energy trapping region, and the surface of the recess. The layer is on the conductive layer. The idle pole is located on the interpole oxide layer, and the horizontal width of the gate is less than the spacing of the electron depression regions relative to the gate recessed region. The source and the drain are located on the conductive layer, and are respectively located on two sides of the gate, and the source and the drain are located inside the isoelectric b-zone. In the present invention, the channels of the electron energy trapping region and the upper layer and the gate electrode can produce a complete self-alignment effect. In addition, the separate vertical electron trap structure will not limit the miniaturization of the channel length, and it does not consume a large gate voltage because it is not a multi-layer structure built at the gate terminal. In operation, due to the small operating voltage, it has a strong inhibitory effect on the extra electrical effects caused by the high electric field. Moreover, since the separated vertical electron energy trap structure has the gate oxide layer and the conductive layer effectively isolated from each other, there is no bit interference between the bits, and the excellent resistance is not caused by the charge distribution concentration. The resulting diffusion phenomenon and the difficulty of interpretation or even the wrong situation of It. The vertical architecture of the present invention has a tip charge accumulation at the upper end, which generates a stronger electric field to modulate the subcritical region (sub thresh〇ld, _ the voltage acting on the source 7 drain, forming a larger interpretation between the bits In addition, the present invention utilizes a symmetric vertical electron storage region (i.e., such electron trapping regions) formed outside the source and the drain, the electron storage region being generated by the held electrons. The synthetic electric field demodulation is truly used in the source and the infinite electric field to produce readability. The electron storage area is far away from the collision ionization area, so that interference during reading can be prevented, and it is a reliable memory element. [Embodiment] Referring to FIG. 1 to FIG. 1, a schematic diagram showing a method of manufacturing a 111758.doc 16 1310233 memory of a modulated source/drain voltage according to the present invention is shown. Referring first to FIG. 1, a board 1 is provided. The substrate 1 has a surface 11. In the embodiment, the substrate 1 is a Silicon-On-Insulator (SOI) substrate, which includes a first wafer 12, an oxide layer 13, and a second Wafer 14, the oxide layer = system The substrate 1 is also sandwiched between the first wafer 12 and the second wafer 14. It is understood that the substrate 1 may also be a single wafer. Referring to FIG. 2, the surface 11 of the substrate 1 is formed. - groove 15, the concave

槽15具有二側壁151及一底部152。在本實施例中,在完成 標準清洗步驟後與完成光罩製程後,卩隔離:術 (LOCOS,STI)配合-光罩定義該凹㈣,且利用活性離子 蝕刻該第二晶圓14以形成該凹槽15。該凹槽15即為一元件 主動區。要注意的是,在本發明中,該凹槽15之深度及形 狀並沒有特別的限制,該等侧壁151可以垂直該底部Μ或 是與該底部152間具有大於或小於9〇之傾斜角度,且該等 侧壁1 5 1也可以是弧形。 參考圖3,形成一電子儲存層16於該基板1之該表面11及 該凹槽15上。在本實施例中’該電子儲存層16之材質係為 氮化物。在本實施例中,係、利用低壓化學氣相沈積法 (LPCVD)形成該電子儲存層16。 參考圖4 ’部分移除該電子儲存層16以形成二個不連續 之電子能陷區17,且暴露出該基板1之該表面U及該凹槽 15之”玄底σ”52 ’該二個電子能陷區17係為利用側壁殘留 技術所留下之側邊俾_ s 、 透保4層(Spaeer),且係分別位於該四槽 1 5之一側土 1 5 1上,且該等電子能陷區1 7間具有一間距。 111758.doc 17 1310233 在本實施例中’係利用活性離子钱刻該電子儲存層16,形 成後之該等電子能㈣17具有均—之厚度,其與該等侧壁 151—樣皆垂直該凹槽15之底部152。 參考圖5,形成一導電層18於該基板1之該表面^、該等 電子能陷區17及該凹槽15之該底部⑸上。該導電層獻 上表面具有―閉極凹陷區181’該閉極凹陷區⑻係位於該 等電子能Μ 17之Μ之相社置。在本實施射,該導 電層18之材質係為多晶碎,且係利用低壓化學氣相沈積法 形成該導電層之後再_料電層此上表面,經過多 次之成長及蝕刻後,可形成較圓滑陷入之閘極凹陷區 18卜 參考圖6,形成一閘極氧化層19於該導電層18上。 參考圖7,形成-閘極矽化層2〇於該閉極氧化層19上。 在本實施例中,該閘極魏層2G之材f係為多晶妙,且係 利用低壓化學氣相沈積法形成該閘極矽化層2 〇。 參考圖8,冑分移除該閘極硬化層2〇以冑下一殘留矽 2〇卜在本實施例巾,係利用活性離子钱刻該閘極石夕化層 20。該殘留矽201係位於該閘極凹陷區181之相對位置。 參考圖9,成長該殘留石夕201,以形成一閉㈣。該閉極 21之水平寬度係小於該等電子能陷區17間之該間距。在本 實施例中,係利用選擇性蟲晶成長方法成長該殘留石夕 2〇丨。由於該殘留石夕201係位於該問極凹陷區i8i之相對位 置’因此該閘極21在成長過程中會有自我對齊之效果,亦 即該閘極21成長後會位於該等電子能陷區丨了之中間。 111758.doc 1310233 參考圖10,形成一閘極保護層22於該閘極21及該閘極氧 化層19上。在本實施例中,該閘極保護層22亦為一氧化 層’其材質與該閘極氧化層19相同。接著,利用離子佈植 技術於該導電層18形成參雜之源極23及汲極24,該源極23 及該汲極24係位於該導電層18相對於該等電子能陷區丨7之 内側。The slot 15 has two side walls 151 and a bottom 152. In this embodiment, after the completion of the standard cleaning step and after the completion of the mask process, the LOCOS (STI) mating-mask defines the recess (4), and the second wafer 14 is etched by the active ions to form The groove 15. The groove 15 is an element active area. It should be noted that, in the present invention, the depth and shape of the groove 15 are not particularly limited, and the side walls 151 may be perpendicular to the bottom Μ or may have an inclination angle greater than or equal to 9 间 between the bottom 152. And the side walls 151 may also be curved. Referring to FIG. 3, an electron storage layer 16 is formed on the surface 11 of the substrate 1 and the recess 15. In the present embodiment, the material of the electron storage layer 16 is nitride. In the present embodiment, the electron storage layer 16 is formed by low pressure chemical vapor deposition (LPCVD). Referring to FIG. 4, the electronic storage layer 16 is partially removed to form two discontinuous electron energy trap regions 17, and the surface U of the substrate 1 and the "bottom σ" 52 ' of the recess 15 are exposed. The electron energy trapping zone 17 is a side 俾 _ s and a permeable layer 4 layer (Spaeer) which are left by the side wall residual technology, and are respectively located on the side soil 1 51 of the four slots 15 5 , and the The isoelectronic energy trap has a distance of 17 between them. 111758.doc 17 1310233 In the present embodiment, the electronic storage layer 16 is engraved with active ions, and the formed electron energy (4) 17 has a thickness of uniform, which is perpendicular to the sidewalls 151. The bottom 152 of the slot 15. Referring to FIG. 5, a conductive layer 18 is formed on the surface of the substrate 1, the electron trapping regions 17 and the bottom portion (5) of the recess 15. The conductive layer has a "closed-pole recessed region 181' on the surface, and the closed-pole recessed region (8) is located at the opposite of the electron energy. In the present embodiment, the material of the conductive layer 18 is polycrystalline, and the conductive layer is formed by low-pressure chemical vapor deposition, and then the upper surface of the electrical layer is subjected to multiple growth and etching. A gate recessed region 18 is formed which is relatively rounded. Referring to FIG. 6, a gate oxide layer 19 is formed on the conductive layer 18. Referring to FIG. 7, a gate-deuterated layer 2 is formed on the gate oxide layer 19. In the present embodiment, the material f of the gate electrode layer 2G is polycrystalline, and the gate vaporization layer 2 is formed by a low pressure chemical vapor deposition method. Referring to Fig. 8, the gate hardened layer 2 is removed by enthalpy to remove the remaining layer 〇2. In the embodiment of the present invention, the gate electrode layer 20 is engraved with active ions. The residual crucible 201 is located at a relative position of the gate recess region 181. Referring to Fig. 9, the residual stone eve 201 is grown to form a closed (four). The horizontal width of the closed pole 21 is less than the spacing between the electron trapping regions 17. In the present embodiment, the residual crystal growth method is used to grow the residual stone. Since the residual Shixi 201 is located at the relative position of the pole depression region i8i, the gate 21 has a self-aligning effect during the growth process, that is, the gate 21 is located in the electron energy trapped region after being grown. In the middle of it. 111758.doc 1310233 Referring to Figure 10, a gate protection layer 22 is formed over the gate 21 and the gate oxide layer 19. In the present embodiment, the gate protection layer 22 is also an oxide layer' having the same material as the gate oxide layer 19. Next, a source electrode 23 and a drain electrode 24 are formed on the conductive layer 18 by using an ion implantation technique, and the source electrode 23 and the drain electrode 24 are located in the conductive layer 18 opposite to the electron energy trap region 7 Inside.

參考圖11,如果需要的話,移除該閘極保護層22及部分 該閘極氧化層19,以暴露出該閘極21、該源極23及該汲極 24,形成一調變源/汲極電壓的能陷記憶體2。 再參考圖11,顯不本發明調變源/汲極電壓的能陷記憶 體之示意圖。該調變源/汲極電壓的能陷記憶體2包括一基 板1 一個不連續之電子能陷區I7、一導電層18、一閘極 氧化層19、一閘極21、一源極23及一汲極24。 該基板1具有一凹槽15,該凹槽15具有二側壁ΐ5ΐ及一底 部⑴,該等側壁151係為對稱之外形。在本實施例中,該 基板i係為-矽覆絕緣基板,其包 化層13及—第二晶圓⑷該氧化㈣係纽^第-晶: 12及該第二晶圓14之間。可以理解的i,該基板i也可以 是單一晶圓。 該等電子能陷區17分別位於呤m^ 』仅於s亥凹槽1 5之側壁1 5 1上,其 係用以儲存電子,該等電子能妒p1 μ 于此£ 1 7間具有一間距。在本 實施例中,該等電子能陷區 〔7之材質係為氮化物,其具有 均-之厚度’且垂直該凹槽15之底部152。 該導電層1 8係位於該基板1 之°亥表面11、該等電子能陷 111758.doc -19· 1310233 * 區17及該凹槽15之該底部152上,該導電層i8之上表面具 有一閘極凹陷區181。該閘極氧化層19係位於該導電層U • 上。5亥閘極21係位於該閘極氧化層19上,且相對於該閘極 . 凹陷區18i,該閘極21之水平寬度係小於該等電子能陷區 17間之該間距。在本實施例中,該導電層18及該閘極21之 材質係為多晶矽。該源極23及該汲極24係位於該導電層 18,且分別位於該閘極21之二側,且該源極23及該汲極24 _ 係位於相對該等電子能陷區17之内側。 再參考圖10,在其他應用中,該閘極氧化層19係延伸於 該導電層18之上方,亦即覆蓋該源極23及該汲極24。此 外,該閘極21上更包括一閘極保護層22,以保護該閘極 2卜 在本發明中,该等電子能陷區17和上層的通道及該閘極 21可產生完全的自我對齊之效果。另外該分離垂直式之 電子此•陷區17結構將不會對通道長度的微縮造成侷限,又 • 因並非在閘極端建造的多層架構,不需消耗較大閘極電 „ 壓在操作上,又因較小的操作電壓,對於因高電場而產 生的額外電性效果有較強抑制效用。而且,因為此對分離 式電子此陷區17結構彼此間有該閘極氧化層1 9及該 導電層1 8做有效隔離,不會有位元間彼此互相干擾,及極 佳的阻絕因電荷分布濃度不均造成的擴散現象並導致判讀 困,甚至錯誤之情況。本發明之垂直式架構在上端有尖端 〃 %累積會產生較強電場以調變該元件操作在次臨界區 ( eSh〇ld reglon)時的源極/汲極電壓,構成位元間較 111758.doc 20- 1310233 大的判讀視窗。 此外,本發明係利用在該源極23及該汲極24外側製作出 一對稱垂直的電子儲存區(即該等電子能陷區17),該電子 儲存區會依所保持的電子產生的合成電場去調變真正做用 在該源極23及該汲極24的電場而產生判讀性,此電子儲存 區較遠離衝撞離子化區,故可以防止讀取時的干擾,為一 可靠的記憶體元件。 上述實施例僅為說明本發明之原理及其功效,並非限制 本發明,因此習於此技術之人士對上述實施例進行修改及 變化仍不脫本發明之精神。本發明之權利範圍應如後述之 申印專利範圍所列。 【圖式簡單說明】 圖1至圖11顯示根據本發明調變源/没極電壓的能陷記憶 體之製造方法之示意圖。 【主要元件符號說明】 1 基板 2 調變源/汲極電壓的能陷記憶體 11 基板之表面 12 第一晶圓 13 氧化層 14 第二晶圓 15 凹槽 16 電子儲存層 17 電子能陷區 111758.doc 21 1310233 18 導電層 19 閘極氧化層 20 閘極石夕化詹 21 閘極 22 閘極保護層 23 源極 24 ί及極 151 凹槽之側壁 152 凹槽之底部 181 閘極凹陷區 201 殘留矽Referring to FIG. 11, if necessary, the gate protection layer 22 and a portion of the gate oxide layer 19 are removed to expose the gate 21, the source 23, and the drain 24 to form a modulation source/汲The voltage of the pole can be trapped in the memory 2. Referring again to Fig. 11, a schematic diagram of the energy storage source of the modulated source/drain voltage of the present invention is shown. The energy storage source 2 of the modulation source/drain voltage includes a substrate 1 with a discontinuous electron energy trapping region I7, a conductive layer 18, a gate oxide layer 19, a gate 21, and a source 23; One bungee 24. The substrate 1 has a recess 15 having two side walls ΐ5ΐ and a bottom portion (1) which are symmetrical in shape. In the present embodiment, the substrate i is a germanium-covered insulating substrate, and the cladding layer 13 and the second wafer (4) are between the oxide (4) and the second wafer 14 . It can be understood that the substrate i can also be a single wafer. The electron trapping regions 17 are respectively located on the side wall 151 of the swell groove 15 and are used for storing electrons. The electron energy 妒p1 μ has a spacing. In the present embodiment, the electron trapping regions [7 are made of nitride having a uniform thickness] and perpendicular to the bottom 152 of the recess 15. The conductive layer 18 is located on the surface 11 of the substrate 1 , the electron energy trap 111758.doc -19· 1310233 * region 17 and the bottom portion 152 of the recess 15. The upper surface of the conductive layer i8 has A gate recessed area 181. The gate oxide layer 19 is located on the conductive layer U•. The 5th gate 21 is located on the gate oxide layer 19, and the horizontal width of the gate 21 is smaller than the pitch between the electron trap regions 17 with respect to the gate. In this embodiment, the conductive layer 18 and the gate 21 are made of polysilicon. The source 23 and the drain 24 are located on the conductive layer 18 and are respectively located on two sides of the gate 21, and the source 23 and the drain 24 are located on the inner side of the electron recessed area 17 . Referring again to FIG. 10, in other applications, the gate oxide layer 19 extends over the conductive layer 18, that is, over the source 23 and the drain 24. In addition, the gate 21 further includes a gate protection layer 22 for protecting the gate 2. In the present invention, the electron trapping region 17 and the upper channel and the gate 21 can be completely self-aligned. The effect. In addition, the separation of vertical electrons and the structure of the trap 17 will not limit the miniaturization of the channel length, and • because the multi-layer structure is not built at the gate extreme, it does not need to consume a large gate voltage. Moreover, due to the small operating voltage, the additional electrical effect due to the high electric field has a strong inhibitory effect. Moreover, since the separated electrons have the gate oxide layer 19 and the structure between the trapped electrons, The conductive layer 18 is effectively isolated, and there is no interference between the bits, and the diffusion phenomenon caused by the uneven distribution of the charge distribution is excellent, and the interpretation is difficult or even wrong. The vertical structure of the present invention is The upper end has a tip 〃% accumulation will generate a strong electric field to modulate the source/drain voltage of the element operating in the subcritical region (eSh〇ld reglon), which constitutes a larger interpretation between the bits than the 111758.doc 20-1310233 In addition, the present invention utilizes a symmetric vertical electron storage region (ie, the electron energy trap region 17) formed outside the source electrode 23 and the drain electrode 24, and the electron storage region is generated according to the held electrons. The synthetic electric field demodulation truly uses the electric field of the source 23 and the drain 24 to produce readability. The electronic storage area is far away from the collision ionization area, so that the interference during reading can be prevented, which is a reliable The above embodiments are merely illustrative of the principles and effects of the present invention, and are not intended to limit the present invention, and those skilled in the art can make modifications and variations to the above-described embodiments without departing from the spirit of the invention. The range should be as listed in the scope of the printed patents described later. [Simplified Schematic] FIG. 1 to FIG. 11 are schematic diagrams showing a method of manufacturing a memory capable of modulating a source/no-pole voltage according to the present invention. 】 1 substrate 2 modulation source / drain voltage can be trapped in memory 11 substrate surface 12 first wafer 13 oxide layer 14 second wafer 15 groove 16 electron storage layer 17 electron energy trapping area 111758.doc 21 1310233 18 Conductive layer 19 Gate oxide layer 20 Gate Shi Xihua Zhan 21 Gate 22 Gate protection layer 23 Source 24 ί and pole 151 Groove sidewall 152 Groove bottom 181 Gate recessed area 20 1 residual 矽

111758.doc -22111758.doc -22

Claims (1)

13102331310233 、申請專利範圍: -種調變源/汲極電壓的能陷記憶體之製造方法 包括以 (a) 提供一基板,該基板具有一表面; (b) 於該基板之該表面上形成一 辟芬一^ 珉凹槽,該凹槽具有二側 土及一底。卩,該等侧壁係為對稱之外形; :形成一電子儲存層於該基板之該表面及該凹槽上; ⑷錯移除該電子储存層㈣成:個不㈣之電子r 且暴露出該基板之該表面及該凹槽之該底 b 和该專電子能陷區係分別位於該凹槽之二側壁 上,且該等電子能陷區間具有一間距; ⑷ 形成-導電層於該基板之該表面、該等電子能陷區 及該凹槽之該底部上’該導電層之上表面具有一閘 極凹陷區; (〇形成一閘極氧化層於該導電層上; (g) 形成一閘極矽化層於該閘極氧化層上; (h) 部分移除該閘極矽化層以留下一殘留矽於該閘極凹 陷區之相對位置; (i) 成長該殘留矽,以形成一閘極,其中該閘極之水平 寬度係小於該等電子能陷區間之該間距; (j) 形成一閘極保護層於該閘極及該閘極氧化層上;及 (k) 形成一源極及一汲極,其中該源極及該汲極係位於 該導電層相對於該等電子能陷區之内側。 2.如請求項1之製造方法,其中該基板係為一矽覆絕緣 111758.doc 1310233 (Silic〇n_〇n_Insulat〇r,s〇i)基板,其包括—第一晶圓、 一氧化層及一第二晶圓’該氧化層係夾設於該第一晶圓 及該第二晶圓之間。 3·如請求項丨之製造方法,其中該基板係為一晶圓。 4·如請求項i之製造方法,其中該步驟(b)中係利用一光罩 定義該凹槽’且利用活性離子蝕刻該基板以形成該凹 槽。 5. 如清求項丨之製造方法,其中該凹槽之側壁係垂直該凹 槽之底部,且該等電子能陷區垂直該凹槽之底部。 6. 如凊求項1之製造方法,其中該步驟(C)、(e)、⑴、(§)及 (J)中之形成方法係為低壓化學氣相沈積法(LPCVD)。 7. 如清求項1之製造方法,其中該步驟⑷及(h)中之移除方 法係為活性離子蝕刻。Patent application scope: - A method for manufacturing a memory capable of modulating a source/drain voltage comprises: (a) providing a substrate having a surface; (b) forming a surface on the surface of the substrate The groove has a groove, and the groove has two sides of soil and a bottom.卩, the sidewalls are symmetrically shaped; forming an electron storage layer on the surface of the substrate and the recess; (4) erroneously removing the electron storage layer (4) into: an electron (n) that is not (d) and exposed The surface of the substrate and the bottom b of the recess and the electron-trapping region are respectively located on two sidewalls of the recess, and the electron trapping regions have a spacing; (4) forming a conductive layer on the substrate The surface, the electron energy trapping region and the bottom portion of the recess have a gate recessed surface on the upper surface of the conductive layer; (〇 forms a gate oxide layer on the conductive layer; (g) forms a gate deuterated layer on the gate oxide layer; (h) partially removing the gate deuterated layer to leave a residual position in the gate recessed region; (i) growing the residual crucible to form a gate, wherein a horizontal width of the gate is less than the spacing of the electron energy trapping regions; (j) forming a gate protection layer on the gate and the gate oxide layer; and (k) forming a gate a source and a drain, wherein the source and the drain are located in the conductive layer relative to the first 2. The manufacturing method of claim 1, wherein the substrate is a substrate insulation 111758.doc 1310233 (Silic〇n_〇n_Insulat〇r, s〇i) substrate, including - a wafer, an oxide layer and a second wafer 'the oxide layer is interposed between the first wafer and the second wafer. 3. The method for manufacturing the substrate, wherein the substrate is A wafer. The manufacturing method of claim i, wherein the step (b) defines the groove by a mask and the substrate is etched with active ions to form the groove. The manufacturing method of the crucible, wherein the sidewall of the recess is perpendicular to the bottom of the recess, and the electron trapping region is perpendicular to the bottom of the recess. 6. The manufacturing method of claim 1, wherein the step (C) The formation methods in (e), (1), (§), and (J) are low pressure chemical vapor deposition (LPCVD). 7. The manufacturing method of claim 1, wherein the steps (4) and (h) The removal method is reactive ion etching. 8·如請求項1之製造方法 為選擇性磊晶成長方法 9,如請求項1之製造方法 氮化物D 其中該步驟⑴中之成長方法係 其中該電子儲存層之材質係為 1〇·:,求項i之製造方法,丨中該導電層及該閘極矽化層 才質係為多晶碎。 11 如I含杳击 :項1之製造方法,其中該步驟(k)係利用離子佈植 式形成該源極及該汲極。 除::項1之製造方法,其中該步驟(k)之後更包括-移 13二°"3極保護層及部分該閘極氧化層之步驟。 .—種調變源/汲極電壓的能陷記憶體,包括: Hl758.do, 1310233 一基板,具有一凹槽,該凹 二個不連續之電子能陷區, 於該凹槽之側壁上 槽具有二側壁及一底部; 用以儲存電子,且分別位 該等電子能陷區間具有一間距; 一導電層,位於該基板之該表面、 該凹槽之該底部上’該導電層之上表 區; 該等電子能陷區及 面具有一閘極凹陷 且相對於該閘極凹陷 電子能陷區間之該間 一閘極氧化層,位於該導電層上 一閘極,位於該閘極氧化層上, 區,該閘極之水平寬度係小於該等 距;及 一源極及H位於該導電層,且分別位於該問極 之二側’該源極及該沒極係位於相對該等電子能陷區之 内側。 14. 15. 16. 17. 18. 如請求項13之記憶體,丨中該基板係為―⑦覆絕緣基 板’其包括-第-晶圓、一氧化層及—第二晶圓,該氧 化層係爽設於該第一晶圓及該第二晶圓之間。 如請求項13之記憶體,其中該基板係為一晶圓。 如請求項13之記憶體,其中該凹槽 θ <侧壁係垂直該凹槽 之底部’且該介電層垂直該凹槽之底部。 如請求項13之記憶體,其中該導電 守电嗜及该閘極之材質係 為多晶矽。 ’位於該閘 如請求項13之記憶體,更包括一閘極保護層 極上。 H1758.doc8. The manufacturing method of claim 1 is the selective epitaxial growth method 9, such as the manufacturing method of claim 1, wherein the growth method in the step (1) is that the material of the electron storage layer is 1〇: The manufacturing method of claim i, wherein the conductive layer and the gate deuterated layer are polycrystalline. 11 The method of claim 1, wherein the step (k) is to form the source and the drain by ion implantation. Except for: the manufacturing method of item 1, wherein the step (k) further comprises the step of shifting the three-pole protective layer and a portion of the gate oxide layer. - a variable source/drain voltage capable memory, comprising: Hl758.do, 1310233 a substrate having a recess, the recessed two discontinuous electron energy trapping regions on the sidewall of the recess The slot has two side walls and a bottom portion for storing electrons, and each of the electron energy trapping sections has a spacing; a conductive layer is located on the surface of the substrate, and the bottom of the recess is on the conductive layer The electron energy trapping region and the mask have a gate depression and a gate oxide layer between the electron recessed regions of the gate recess, and a gate on the conductive layer is located at the gate oxide a layer, a region, the horizontal width of the gate is less than the equidistance; and a source and H are located on the conductive layer and are respectively located on two sides of the question pole. The source and the pole are located opposite to each other The inside of the electron energy trap. 14. 15. 16. 17. 18. The memory of claim 13, wherein the substrate is a "7-covered insulating substrate" comprising - a wafer, an oxide layer and a second wafer, the oxidation The layer is disposed between the first wafer and the second wafer. The memory of claim 13, wherein the substrate is a wafer. The memory of claim 13, wherein the recess θ < the sidewall is perpendicular to the bottom of the recess and the dielectric layer is perpendicular to the bottom of the recess. The memory of claim 13, wherein the conductive power conservation is related to the material of the gate is polysilicon. The memory located in the gate of claim 13 further includes a gate protection layer. H1758.doc
TW95127761A 2006-07-28 2006-07-28 Trap memory with a modified drain/source voltage and the method for making the same TWI310233B (en)

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