TW415065B - Electrostatic discharge protection circuit for preventing melting of the gate structure - Google Patents
Electrostatic discharge protection circuit for preventing melting of the gate structure Download PDFInfo
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415065 五、發明説明(1) 5 _ 1發明領域 本發明是有關於一種靜電放電保護(electr〇static discharge ; ESD )電路’特別是有關於任何一種汲極( drain)導通至墊(Pad)以及電晶體〇xide semiconductor ; MOS )的閘極係直接導通至源極的靜電放 電保護電路。 5-2發明背景 積體電路對於靜電放電所導致的影響是相當敏感的, 典型的靜電放電常是由碰觸到積體電路的接腳(pin)所導 致的短暫與瞬間的高電壓放電。假如未事先做預防的話, 靜電放電會損害或是完全破壞積體電路。因此,靜電放電 保護電路被廣泛地應用於積體電路中以防治靜電放電效應 。在此’靜電放電保護電路係位於積體電路的接腳與晶粒 (d i e )之間。 再者,一個良好的靜電放電保護裝置必需能夠在靜電 放電引發的熱效應下正常工作、防止大量電流影響到積體 電路以及不受突然的高電壓所損害。這些能力主要係取決 於靜電保護裝置的設計與佈局。因此,有許多種的靜電放 電保護電路可使用,而選用哪一種的靜電放電保護電路則 取決於靜電放電保護裴置的工作範圍。415065 V. Description of the invention (1) 5 _ 1 Field of the invention The present invention relates to an electrostatic discharge protection (ESD) circuit, and in particular to any kind of drain (Pad) conduction to a pad and The gate of the transistor (Oxide semiconductor; MOS) is an electrostatic discharge protection circuit that is directly conducted to the source. 5-2 Background of the Invention Integrated circuits are very sensitive to the effects of electrostatic discharge. Typical electrostatic discharges are usually short-term and transient high-voltage discharges caused by touching the pins of integrated circuits. If not prevented in advance, electrostatic discharge can damage or completely destroy the integrated circuit. Therefore, electrostatic discharge protection circuits are widely used in integrated circuits to prevent electrostatic discharge effects. Here, the ESD protection circuit is located between the pins of the integrated circuit and the die (d i e). Furthermore, a good electrostatic discharge protection device must be able to work normally under the thermal effects caused by electrostatic discharge, prevent a large amount of current from affecting the integrated circuit, and not be damaged by sudden high voltage. These capabilities mainly depend on the design and layout of the electrostatic protection device. Therefore, there are many types of electrostatic discharge protection circuits that can be used, and which type of electrostatic discharge protection circuit to use depends on the operating range of the electrostatic discharge protection device.
415065 五、發明說明(2) ' 一種有用的輸入靜電放電保護電路為接地閘極( grounded-gate)電晶體型靜電放電保護電路,其包括多數 個被保護環(Guard ring)所圍繞且通常為關閉(turn 0ff) 的電晶體。這些電晶體的尺寸明顯地大於積體電路中晶粒 之電晶體的尺寸,以降低電流密度與電壓。參照第一圖, 每個電晶體的汲極1 0係導通至墊11,而且源極1 2係接地。 其中,墊11再導通至積體電路的接腳,而且電晶體的閘極 13係接地並導通至接觸(contact)i4。在此,保護環15是 用來隔離這些電晶體與積體電路之晶粒,保護環15導通到 電位零點16。當高電壓產生於墊η時,這些電晶體就會導 通(turn 〇n),藉以將墊丨丨上的高電壓經由電晶體而接地 ,以防止積體電路之晶粒受到高電壓的影響。明顯地,對 於任何電晶體而言,電流都是經由汲極1〇直接流至源極12 ,。明顯的這些電晶體可分成數群,在每一群内電晶體都 是呈並聯(in sequence)排列,而且任何一個電晶體的 壓都相同於其他電晶體的電壓,所以電流所產生的隹耳熱 (joule heat)並不會聚集於任何一個電晶體。 … 隨著現代超大型積體電路(very iarge scale ⑴因:的發展’ ·導體電路的尺寸逐漸縮小 因此,閘極氧化層的厚度也相對應地減少,又 層的厚度會明顯地影響崩潰(breakd〇wn)電壓,所以 流會直接經由閘極氧化層而流至閘極的導體層(所的^ 第二圖所示,t高電壓產生於墊20時,在汲㈣週圍會出。415065 V. Description of the invention (2) '' A useful input electrostatic discharge protection circuit is a grounded-gate transistor-type electrostatic discharge protection circuit, which includes a plurality of guard rings and is usually Turn off (turn 0ff) the transistor. The size of these transistors is significantly larger than the size of the crystals in the integrated circuit to reduce the current density and voltage. Referring to the first figure, the drain 10 of each transistor is turned on to the pad 11, and the source 12 is grounded. Among them, the pad 11 is further conducted to the pins of the integrated circuit, and the gate electrode 13 of the transistor is grounded and conducted to the contact i4. Here, the guard ring 15 is used to isolate the crystals from the crystals of the integrated circuit, and the guard ring 15 is turned on to the potential zero 16. When a high voltage is generated in the pad η, these transistors will turn on, thereby grounding the high voltage on the pad through the transistor to prevent the crystals of the integrated circuit from being affected by the high voltage. Obviously, for any transistor, the current flows directly to the source 12 via the drain 10. Obviously, these transistors can be divided into several groups. In each group, the transistors are arranged in parallel, and the voltage of any one transistor is the same as the voltage of other transistors, so the ear heat generated by the current ( joule heat) does not accumulate in any transistor. … With modern very large scale circuits (the development of very iarge scale factors: · the size of the conductor circuit is gradually shrinking, the thickness of the oxide layer of the gate is correspondingly reduced, and the thickness of the layer will significantly affect the collapse ( breakdwn) voltage, so the current will flow directly through the gate oxide layer to the gate conductor layer (as shown in the second figure, when the t high voltage is generated on the pad 20, it will flow out around the drain.
415065 五、發明說明(3) ' 現S乏區27(depIetion region),此時電流不只會受側面 電場(lateral field, Eh)作用而從汲極21流至源極22, 而且會受垂直電場(vertical field,Εν)的作用而從;及極 21經由閘極氧化層23而流至閘極傳導層24。流經閘極的電 流包括(1)由能帶-能帶(band to band)穿隧電洞25穿透氣 化層所形成的電流和(2)由F-N (Fowler-Nordheim)穿隨電 子2 6穿透氧化層所形成的電流。因此,參照第三圖其中通 過閘極的電流33以Ig表示,可以清楚看出此時所有分享同 一個閘極的電晶體彼此間形成一串聯電路。 參照第三圖,第三圖顯示電流從墊3 〇經由電晶體的閑 極31而流至電位零點32(circuit ground)的電路示意圖。 很明顯地’每一個閘極3 1的電壓都不同於其他閘極31,且 越遠離電位零點32則電壓越高。由於高電壓會產生高能量 ,而且這些能量係不均句的分佈在這些閘極3丨中,所以遠 離電位零點3 2的閘極31會被大量的焦耳熱所融化。明顯地 ’當靜電放電產生於輸入保護電路時,某些輸入保護電路 的電晶體可能因閘極31融化而失效。換句話說,當靜電放 電產生於輸入保護電路時,接地型閘極靜電放電保護電路 之閘極31可能會被融化,使得輸入靜電保護電路失去防治 靜電放電效應的能力。 σ 因此依據先前的敛述可知,需要提供一種適用於超大 型積體電路的靜電放電保護電路。特別是需要提供一種可 防止閘極融化之輸入保護電路,藉以確保保護電路之正 操作。415065 V. Description of the invention (3) 'Now the depletion region 27 (depIetion region), the current will not only be affected by the lateral field (Eh) from the drain 21 to the source 22, but also subject to the vertical electric field (Vertical field, Ev); and the electrode 21 flows through the gate oxide layer 23 to the gate conductive layer 24. The current flowing through the gate includes (1) the current formed by the band-to-band tunneling hole 25 penetrating the vaporized layer and (2) the FN (Fowler-Nordheim) penetrating electron 2 6 The current formed by penetrating the oxide layer. Therefore, referring to the third figure in which the current 33 passing through the gate is represented by Ig, it can be clearly seen that all the transistors sharing the same gate form a series circuit with each other at this time. Referring to the third figure, the third figure shows a schematic circuit diagram of a current flowing from the pad 30 to the potential ground 32 (circuit ground) through the free terminal 31 of the transistor. Obviously, the voltage of each gate 31 is different from that of the other gates 31, and the farther away from the potential zero 32, the higher the voltage. Since high voltage generates high energy, and these energy systems are unevenly distributed in the gates 3, the gates 31 far from the potential zero 3 2 will be melted by a large amount of Joule heat. Obviously, when the electrostatic discharge is generated in the input protection circuit, the transistor of some input protection circuit may fail due to the melting of the gate electrode 31. In other words, when the electrostatic discharge is generated in the input protection circuit, the gate 31 of the grounded gate electrostatic discharge protection circuit may be melted, so that the input electrostatic protection circuit loses its ability to prevent the electrostatic discharge effect. σ Therefore, according to the previous summary, it is known that it is necessary to provide an electrostatic discharge protection circuit suitable for an oversized integrated circuit. In particular, there is a need to provide an input protection circuit that prevents the gate from melting, thereby ensuring the correct operation of the protection circuit.
第7頁 415065Page 7 415065
5-3發明目的及概述: 本發明的目的是提供一種可以防治閘極融化的靜電放 電保護電路。 本發明之一較佳實施例是一種輸入靜電放電保護電路 ,在此一保護環圍繞著多數個平常為關閉的電晶體,而且 每個電晶體的源極都是導通至電位零點,並且電晶體的汲 極是導通至墊。此外,每個電晶體的源極都是直接經由接 觸(contact)而導通至電晶體的閘極。 因此,假如閘極氧化層的厚度足夠薄以致於電流可直 接從電晶體的汲極流至電晶體的閘極,此電流也會直接由 電晶體的閘極經由接觸而流至源極。換句話說,雖然數個 電晶體共同分旱一個長的閘極,但由於接觸的電阻遠小於 般疋以夕日曰梦所形成之閘極的電阻,因此由沿閘極流動 之電流所引發的沿閘極的電位差是微小且可忽略的。除此 之外’在本發明中電流流過的途徑(Path)也遠短於習知之 靜電放電保護電路中電流流經的途徑。綜合上面的討論可 知,本發明可以有效的防治閘極融化以確保輸入靜電放電 保護電路的正常運作。 5-4圖式簡單說明: 415065 五、發明說明(5) 第一圖顯示接地型閘極之電晶體靜電放電保護電路的 簡要示意圖; 第二圖顯示接地型閘極之電晶體靜電放電保護電路中 電晶體的横戴面不意圖; 第三圖顯示在閘極氧化層薄到使電流可以直接由汲極 流到閘極時,接地型閘極之電晶體靜電放電保護電路之等 效電路; 第四圖顯示本發明之一實施例的簡要示意圖; 第五圖顯示根據本發明之一實施例的電晶體橫截面示 意圖;和 第六圖顯示根據本發明之一實施例,當閘極氧化層薄 到使電流可以直接由汲極流到閘極時的等效電路圖。 主要部份的代表符號: 10 没極 11 墊 12 源極 13 閘極 14 接觸 15 保護環 16 電位零點 20 墊 21 汲極5-3 Object and Summary of the Invention The object of the present invention is to provide an electrostatic discharge protection circuit capable of preventing the melting of the gate electrode. A preferred embodiment of the present invention is an input electrostatic discharge protection circuit, in which a protection ring surrounds a plurality of normally closed transistors, and the source of each transistor is turned on to the potential zero point, and the transistor is The drain is conductive to the pad. In addition, the source of each transistor is directly connected to the gate of the transistor via a contact. Therefore, if the thickness of the gate oxide layer is thin enough that current can flow directly from the transistor's drain to the transistor's gate, this current will also flow directly from the transistor's gate to the source through the contact. In other words, although several transistors share a long gate, the resistance of the contact is much smaller than the resistance of the gate formed by the dream, so it is caused by the current flowing along the gate. The potential difference along the gate is small and negligible. In addition, the path through which the current flows in the present invention is also much shorter than the path through which current flows in the conventional electrostatic discharge protection circuit. From the above discussion, it can be known that the present invention can effectively prevent the melting of the gate electrode to ensure the normal operation of the input electrostatic discharge protection circuit. A brief description of the 5-4 diagram: 415065 V. Description of the invention (5) The first diagram shows a schematic diagram of the electrostatic discharge protection circuit of the grounded gate transistor; The second diagram shows the electrostatic discharge protection circuit of the grounded gate transistor The cross-section of the CLP crystal is not intended; the third figure shows the equivalent circuit of a grounded gate transistor electrostatic discharge protection circuit when the gate oxide layer is thin enough to allow current to flow directly from the drain to the gate; The fourth diagram shows a schematic diagram of an embodiment of the present invention; the fifth diagram shows a schematic cross-section of a transistor according to an embodiment of the present invention; and the sixth diagram shows a gate oxide layer according to an embodiment of the present invention. An equivalent circuit diagram when thin enough to allow current to flow directly from the drain to the gate. Symbols of main parts: 10 poles 11 pads 12 sources 13 gates 14 contacts 15 guard rings 16 potential zero 20 pads 21 drain
415065 五、發明說明(6) 22 源極 23 閘極氧化層 2 4 閘極傳導層 25 電洞 26 電子 27 匱乏區 30 塾 31 閘極 32 電位零點 33 通過閉極的電流 40 保護環 41 閘極 42 源極 43 汲極 44 墊 45 電位零點 50 閘極傳導層 51 源極 52 間極氧化層 53 汲極 54 電位零點 55 墊 56 接觸 57 接地金屬線415065 V. Description of the invention (6) 22 source 23 gate oxide layer 2 4 gate conductive layer 25 electric hole 26 electron 27 deficient area 30 塾 31 gate 32 potential zero 33 current through the closed pole 40 guard ring 41 gate 42 source 43 sink 44 pad 45 potential zero 50 gate conductive layer 51 source 52 interlayer oxide layer 53 drain 54 potential zero 55 pad 56 contact 57 ground wire
第ίο頁 415065_ 五、發明說明(7) 60 閘極 61 墊 62 電位零點 5 - 5發明詳細說明: 為了闡明本發明之宗旨,首先提出一可以防治閘極融 化的輸入靜電放電保護電路。此靜電放電保護電路位於積 體電路的接腳與晶粒之間,藉以防止晶粒受到靜電放電的 影響。本發明所提供之靜電放電保護電路與習知接地型閘 極電晶體靜電放電保護電路的主要差異在於本發明實施例 中的每個電晶體的閘極都連通到源極的接地金屬線,也就 是說任何流至間極的電流會直接流至源極的接地金屬線。 參照第四圖,本發明所提供的靜電放電保護電路包括 保護環40、數個閘極41、源極42與汲極43、以及^4,其 中没極43導通至墊44,且源極42導通至電位零點這^ 閘極41、源極42與汲極43構成多數個被保護環之^ 晶體。 保護環40係用來隔離這些電晶體與積體電路續—美他部 份,而且係導通至靜電放電保護電路的電位零點保^ 環40的材質至少包括重摻雜的p型半導體與重摻型^ 導體。閘極41的材料至少包括多晶矽與金屬。此外, 明可適用於P型電晶體與N型電晶體。 415065 五、發明說明(8) 值付注意的是電晶體平常是.處於關閉狀態,只有當高 電壓出現於塾4 4時才會打開。 另外需要注意的一點是這些電晶體的尺寸明顯的比晶 粒中電晶體的尺寸還要大β原因是大面積的電晶體可使電 荷密度(charge density)大幅減少,所以這些電晶體可忍 受較大的電壓範圍。 ^ 除此之外’這些電晶體的詳細形狀、尺寸與數目係決 定於所提供的靜電放電保護電路的工作範圍,典型的寬度 約為10^m到100仁m,且典型的數量約為12。 參照第五圖,本發明實施例的主要特徵包括就靜電放 電保遵電路中的每一個電晶體而言’閘極傳導層5 〇都是直 接經由接觸56和接地金屬線57而導通至電位零點54,而且 閘極傳導層50與電位零點54之間的電阻值可忽略,該電阻 值至少包括接觸56的電阻值(Rcontact)與接地金屬線57的 電阻值。因此,當閘極氧化層52的厚度薄的足夠使電流直 接從沒極5 3流至閘極傳導層5 〇,電流也會直接從閘極傳導 層50流至電位零點54。換句話說,電流會從墊55直接流至 電位零點5 4。即使如第四圖所示,即使數個電晶體共同分 享一個閘極41,電流也不會沿著閘極41流動,而會從墊55 直接流至源極51。也就是說說,如第六圖所示,這些電晶 體的等效電路是成並聯(in sequence)排列。 參照第六圖顯示之本發明之一實施例的等效電路。明 顯地,墊61與電位零點62之間的閘極6〇係呈並聯排列的。 所以,任何一個閘極60的電壓都是相同於其他閘極60的電Page 415065_ V. Description of the invention (7) 60 Gate 61 Pad 62 Potential zero 5-5 Detailed description of the invention: In order to clarify the purpose of the present invention, an input electrostatic discharge protection circuit capable of preventing the melting of the gate is first proposed. This electrostatic discharge protection circuit is located between the pins of the integrated circuit and the die to prevent the die from being affected by electrostatic discharge. The main difference between the electrostatic discharge protection circuit provided by the present invention and the conventional grounded gate transistor electrostatic discharge protection circuit is that the gate of each transistor in the embodiment of the present invention is connected to the ground metal line of the source, and That is to say, any current flowing to the intermediate electrode will directly flow to the ground metal line of the source. Referring to the fourth figure, the electrostatic discharge protection circuit provided by the present invention includes a protection ring 40, a plurality of gates 41, a source 42 and a drain 43, and ^ 4, wherein the non-electrode 43 is connected to the pad 44 and the source 42 The gate 41, the source 42 and the drain 43, which are turned on to the potential zero point, constitute a plurality of protected crystals. The guard ring 40 is used to isolate these transistors from the integrated circuit, the other part, and the potential zero point conduction to the electrostatic discharge protection circuit. The material of the ring 40 includes at least a heavily doped p-type semiconductor and a heavily doped semiconductor. Type ^ Conductor. The material of the gate 41 includes at least polycrystalline silicon and metal. In addition, it is applicable to P-type transistors and N-type transistors. 415065 V. Description of the invention (8) It should be noted that the transistor is usually in the off state, and it will only turn on when high voltage appears at 塾 4 4. Another thing to note is that the size of these transistors is significantly larger than the size of the crystals in the grains. Β The reason is that large area transistors can significantly reduce the charge density, so these transistors can tolerate Large voltage range. ^ In addition to this, the detailed shape, size, and number of these transistors are determined by the working range of the ESD protection circuit provided. The typical width is about 10 ^ m to 100 in m, and the typical number is about 12 . Referring to the fifth figure, the main features of the embodiment of the present invention include that, for each transistor in the electrostatic discharge compliance circuit, the 'gate conductive layer 50' is directly conducted to the potential zero through the contact 56 and the ground metal wire 57. 54, and the resistance value between the gate conductive layer 50 and the potential zero 54 is negligible, and the resistance value includes at least the resistance value of the contact 56 (Rcontact) and the resistance value of the ground metal line 57. Therefore, when the thickness of the gate oxide layer 52 is thin enough to allow a current to flow directly from the gate 53 to the gate conductive layer 50, the current will also flow directly from the gate conductive layer 50 to the potential zero 54. In other words, the current will flow directly from the pad 55 to the potential zero 54. Even if the gate 41 is shared by several transistors as shown in the fourth figure, the current does not flow along the gate 41 but flows directly from the pad 55 to the source 51. That is, as shown in the sixth figure, the equivalent circuits of these electric crystals are arranged in a sequence. An equivalent circuit of an embodiment of the present invention is shown with reference to the sixth figure. Obviously, the gates 60 between the pad 61 and the potential zero 62 are arranged in parallel. Therefore, the voltage of any one of the gates 60 is the same as that of the other gates 60
415065 五 、發明說明(9) 屋’而且任何一個閘極6〇的功率係相同於其他閘極的功率 。所以’不只電流所引發的焦耳熱均勻分佈在各個閘極上 ’同時由於接觸56的電阻值(RC0ntact)趨近於零所以電流 的功率(電壓與電阻值的乘積)也是趨近於零,因此焦耳熱 的影響在本發明中是以忽略不計的。 报明顯的’本發明的精神在於任何電晶體的閘極係導 通至電晶體的源極’其中閘極與源極之間的電阻可忽略。 所以即使相鄰電晶體的閘極係鄰接的,但是仍不會有電流 流經這些閘極。 以上所述僅為本發明之較佳實施例而已,並非用以限 定本發明之申請專利範圍;凡其他未脫離本發明所揭示之 精神下所完成之等效改變或修飾,均應包括在下述之申 專利範圍内。415065 V. Description of the invention (9) House 'And the power of any gate 60 is the same as the power of other gates. So 'not only the Joule heat caused by the current is evenly distributed across the gates', but because the resistance value (RC0ntact) of contact 56 approaches zero, the power of the current (the product of voltage and resistance value) also approaches zero, so Joule The effect of heat is negligible in the present invention. It is apparent that the spirit of the present invention is that the gate system of any transistor is connected to the source of the transistor, and the resistance between the gate and the source is negligible. So even if the gates of adjacent transistors are adjacent, no current will flow through them. The above descriptions are merely preferred embodiments of the present invention, and are not intended to limit the scope of patent application for the present invention; all other equivalent changes or modifications made without departing from the spirit disclosed by the present invention shall be included in the following Within the scope of patent application.
第13頁Page 13
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TW88109870A TW415065B (en) | 1999-06-14 | 1999-06-14 | Electrostatic discharge protection circuit for preventing melting of the gate structure |
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TW88109870A TW415065B (en) | 1999-06-14 | 1999-06-14 | Electrostatic discharge protection circuit for preventing melting of the gate structure |
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TW415065B true TW415065B (en) | 2000-12-11 |
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TW88109870A TW415065B (en) | 1999-06-14 | 1999-06-14 | Electrostatic discharge protection circuit for preventing melting of the gate structure |
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1999
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