TW510022B - High-speed level shifter device with zero threshold voltage components - Google Patents

High-speed level shifter device with zero threshold voltage components Download PDF

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TW510022B
TW510022B TW90116065A TW90116065A TW510022B TW 510022 B TW510022 B TW 510022B TW 90116065 A TW90116065 A TW 90116065A TW 90116065 A TW90116065 A TW 90116065A TW 510022 B TW510022 B TW 510022B
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pair
transistors
type
transistor
type transistors
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TW90116065A
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Wen-Tai Wang
Jung-Huei Chen
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Taiwan Semiconductor Mfg
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Abstract

The present invention provides a high-speed level shifter device with zero threshold voltage components. The device includes: an inverter and a shift latch. The inverter is composed of two pairs of N-type transistors and two pairs of P-type transistors, wherein the transistors have relatively thin gate oxide layers. The shift latch includes a pair of crossed-coupled P-type transistors, a pair of N-type transistors and a pair of N-type transistors with zero threshold voltage, wherein the crosses-coupled P-type transistors have relatively thick gate oxide layer, the N-type transistors have relatively thin gate oxide layers, and the N-type transistors with zero threshold voltages have relatively thick gate oxide layers.

Description

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發明領域: 本發明與一種電平位移(level shifter)裝置有關, 特別是一種具有零臨界電壓金氧半場效電晶體之電平位 裝置’可應用於超深次微米(ultra sub-micr〇n)半導體技 發明背景: 基於積體電路技術之快速進展,積體電路之線寬已經 可以達到深次微米甚至超深次微米之程度,在進入線寬小 於0 · 1 8微米之世代時,各種製程之條件較以往更為嚴格。 在元件縮小化之前提下,製作元件之空間亦相對減少,因 此,在(超)深次微米技術中製作高性能之元件或裝置是一 項具挑戰性之工作。由穩定製作JFET的技術,導致更重要 之元件金氧半場效電晶體(M〇SFET)之發展,m〇sfet的結構 在二氧化矽上建立閘極,位於半導體之汲極與源極之間。 在閘極與半導體之間加上適當之電壓,即可控制源極與汲 極間之通道電流。 $平位移裝置使用兩種不同型態之金氧半場效電晶 ,丄,、包含核心元件以及作為輸入/輸出元件。核心元件 具有較低之臨界電壓(thresh〇ld v〇u 一 "到。.35伏之間,其間極氧化層厚度較薄,係用來增般加為FIELD OF THE INVENTION The present invention relates to a level shifter device, in particular to a level-bit device with zero critical voltage metal-oxygen half field effect transistor, which can be applied to ultra deep sub-micron (ultra sub-micr) ) Background of semiconductor technology invention: Based on the rapid progress of integrated circuit technology, the line width of integrated circuits can reach the depth of sub-micron or even ultra-deep sub-micron. When entering the generation with line width less than 0 · 18 microns, various The process conditions are stricter than before. Before the components are reduced, the space for making components is also relatively reduced. Therefore, it is a challenging task to make high-performance components or devices in (ultra-deep) sub-micron technology. The stable production of JFET technology has led to the development of the more important element metal-oxide-semiconductor field-effect transistor (MOSFET). The structure of mfsfet builds a gate on silicon dioxide, located between the drain and source of the semiconductor. . By applying an appropriate voltage between the gate and the semiconductor, the channel current between the source and the drain can be controlled. The flat displacement device uses two different types of metal-oxide half-field-effect transistors, 丄, containing core components and as input / output components. The core component has a lower threshold voltage (thresh〇ld v〇u -1 to .35 volts, during which the thickness of the polar oxide layer is thinner, which is used to increase the

第4頁 510022 五、發明說明(2) M0S之飽和電流。輸入/輸出元件(丨/〇)的臨界電壓較高, 約為0 · 4到0 · 7伏之間,其閘極氧化層厚度較厚,係用來增 加可靠度(reliability)。電平位移裝置是使訊號從低核 心電壓(low core voltage)轉換到高輸入/輸出電壓(1^以 I/O voltage)之橋樑,換句話說:電平位移是用來轉換輸 入之訊號電壓位準到一預定之訊號電壓位準,其通常可以 作為緩衝(buffer)用。積體電路之元件通常具有内部之操 作電壓(internal operating voltage),其與外部電路或 系統操作之電壓不同。電平位移裝置接收在一範圍内可變 之輸入訊號電壓,再將其偏移到另一範圍位準之電壓,一 _ 般稱做可變輸入緩衝(scalable level buffer^。 一般而言,核心元件之操作電壓低於輸入/輸出元件 之操作電壓,且輸入/輸出元件操作電壓之降低(scale down)程度遠比核心元件操作電壓下降的緩慢。通常, VDDQ約為5v-3v ’VDD約為〇·9ν-2·5ν。習知技術之前案可 以參閱美國專利US 60 1 1 421、US 5 969542等相關前案。 圖一所不為一傳統技術之電平位移器,包含^一反相器 由NM0S(N1,Ν2)及PM0S(P1,Ρ2)所組成,以及包含一偏移❿ 閂。偏移閂由一對NM0S(N3, N4)以及一相互輕合之 PM0S(P3,P4)所構成,也就是PM0S(P3)之閘極連接到 PM0S(P4)之汲極,同理,PM0S(P4)之閘極也連接到 , PM0SCP3)之汲極。NM0S對(N3, N4)之源極則連接到一電位Page 4 510022 V. Description of the invention (2) Saturation current of M0S. The threshold voltage of the input / output element (丨 / 〇) is relatively high, which is between about 0.4 volts and 0.7 volts. The thickness of the gate oxide layer is thicker, which is used to increase the reliability. The level shifter is a bridge that converts the signal from low core voltage to low input / output voltage (1 ^ to I / O voltage). In other words, the level shifter is used to convert the input signal voltage Level to a predetermined signal voltage level, which can usually be used as a buffer. Components of integrated circuits usually have an internal operating voltage, which is different from the voltage at which an external circuit or system operates. The level shifting device receives a variable input signal voltage within a range, and then shifts it to a voltage of another range level, which is generally called a variable input buffer (scalable level buffer ^. Generally speaking, the core The operating voltage of the device is lower than the operating voltage of the input / output device, and the operating voltage of the input / output device decreases much more slowly than the core device operating voltage. Generally, VDDQ is about 5v-3v 'VDD is about 〇 · 9ν-2 · 5ν. For the previous case of the conventional technology, please refer to the related cases such as US patents US 60 1 1 421, US 5 969542, etc. Fig. 1 is not a traditional technology level shifter, which includes a phase inversion The device is composed of NM0S (N1, Ν2) and PM0S (P1, P2), and contains an offset ❿ latch. The offset latch consists of a pair of NM0S (N3, N4) and a light-weight PM0S (P3, P4). The gate of PM0S (P3) is connected to the drain of PM0S (P4). Similarly, the gate of PM0S (P4) is also connected to the drain of PM0SCP3. The source of NM0S pair (N3, N4) is connected to a potential

第5頁 510022510022Page 5

ϊί入端,型電晶體(Ν4)之閘極則連接於反相器之輸 出鈿。反相盗藉由輸入端(ΙΝ)接收一輸入訊號之電壓位 準,經由偏#閃將電平位移#出一帛^圍位準之輸出訊 號。一般,輸入的低電位訊號約介於VDD_vss之間,經 電平位移裝置處理後之電位位準約介於VDDQ_vss之間。 圖二所述之電平位移裝置之操作如了,在輸人端( 輸入一較低電位訊號(如vss)時,P型電晶體(P1)開啟, 型電晶體(N1 )關閉,則將IN-bar電位提升為較高之電位 VDD,因而N型電晶體〇2)開啟,P型電晶體(p2/關閉。此 時’因為IN-bar之拉升(pull up)所以開啟1^型電晶體 (N3) ’而輸出端(OUT)下拉(pull down)至VSS,造成p型電 晶體(P4)開啟,使OUT-bar之電位為VDDQ,P型電晶體(p3) 與N型電晶體(N4)皆關閉,N型電晶體〇5)開啟,jT型電曰 體(P5)關閉’此時輸出端(0UT2)完全被下拉到電位為零曰曰或 接地(ground)。 一 同理,在輸入端(IN)從VSS轉換為輸入一較高之電位 訊號到VDD時,N型電晶體(N1)開啟,p型電晶體(ρι)關 修 閉,則將IN-bar從VDD拉為較低之電位(接地),因而p型電 晶體(P2)開啟,而N型電晶體(N2)關閉。因為IN —bar之下 拉所以開啟N型電晶體(N4),N型電晶體(N3)關閉,接著, P型電晶體(P3)開啟,P型電晶體(P4)關閉。由於n型電晶At the input terminal, the gate of the transistor N4 is connected to the output of the inverter. The anti-phase stealing receives the voltage level of an input signal through the input terminal (IN), and outputs the level shift signal by a range of # ^ through the bias #flash. Generally, the input low-potential signal is between VDD_vss, and the potential level after being processed by the level shift device is between VDDQ_vss. The operation of the level shifting device described in Fig. 2 is as follows. When a low potential signal (such as vss) is input to the input terminal, the P-type transistor (P1) is turned on and the N-type transistor (N1) is turned off. The IN-bar potential rises to a higher potential VDD, so the N-type transistor (2) is turned on, and the P-type transistor (p2 / is turned off. At this time, the 1-type is turned on because the IN-bar is pulled up) Transistor (N3) 'and the output (OUT) pulls down to VSS, causing the p-type transistor (P4) to turn on, so that the potential of OUT-bar is VDDQ, the P-type transistor (p3) and the N-type transistor The crystal (N4) is turned off, the N-type transistor (0) is turned on, and the jT-type electric body (P5) is turned off. At this time, the output terminal (OUT2) is completely pulled down to a potential of zero or ground. For the same reason, when the input terminal (IN) is converted from VSS to input a higher potential signal to VDD, the N-type transistor (N1) is turned on, and the p-type transistor (ρι) is turned off. VDD is pulled to a lower potential (ground), so the p-type transistor (P2) is turned on and the N-type transistor (N2) is turned off. Because the IN-bar is pulled down, the N-type transistor (N4) is turned on, the N-type transistor (N3) is turned off, and then the P-type transistor (P3) is turned on and the P-type transistor (P4) is turned off. As n-type transistor

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體(N4)的開啟,則拉下0UT_bar電位到vss, 體(N5)關閉,而p型電晶體(p5)則開啟,因 =電晶 (0UT2)之電位為VDDQ。 彌®知 利用上述之電平位移電路可以將一般為較低When the body (N4) is turned on, the OUT_bar potential is pulled down to vss, the body (N5) is turned off, and the p-type transistor (p5) is turned on, because the potential of the transistor (0UT2) is VDDQ. Mi® knows that using the above-mentioned level shift circuit can generally lower

元:將其電位偏移位準到較高電_Q 二:右ΐϊ! :操作。上述之設計對輸入訊號而 吕》又有DC漏電流。在偏移閃的設計上由於只 到VDD間沒有短路電流產生。此外,對偏移閃而言,口 電晶體(P4、N3)或電晶體(P3、N4)之一同時開啟 於VDDQ到VSS之間也沒有短路電流之路徑。 匕厂 從輸入端輸入的訊號之電位介於vss到VDD,隨著半導 體技術縮小之趨勢,VDD將變的越來越小。因為電晶體 (N3、N4)仍具有相同之臨界電壓,電晶體(N4)的飽合電流 將變的越來越小。如上所述電晶體(N4)從開啟到關閉時, 電晶體(P3)仍為開啟的狀態時,以及VDDQ經由電晶體 (P3、N3)短路,造成電流一直流通,必須將〇UT_bar節點 下拉到接地,才可將p型電晶體(p3)完全關閉。此電路在_ VDD很低或VDDQ很高之狀態下,將會失效。假如電晶體 (N3)的飽合電流不大於電晶體(p3)的飽合電流,則訊號傳 送的速率會十分緩慢而需消耗較長之時間。在深次微米的· 應用中’會造成嚴重的延遲。Yuan: shift its potential to a higher level. Q: Right ΐϊ !: Operation. The above design has DC leakage current to the input signal. In the design of offset flash, there is no short-circuit current to VDD. In addition, for offset flash, there is no short-circuit current path between one of the transistor (P4, N3) or transistor (P3, N4) is turned on from VDDQ to VSS at the same time. The potential of the signal input from the input terminal is between vss to VDD. With the shrinking trend of semiconductor technology, VDD will become smaller and smaller. Because the transistors (N3, N4) still have the same threshold voltage, the saturation current of the transistor (N4) will become smaller and smaller. As mentioned above, when the transistor (N4) is turned from on to off, when the transistor (P3) is still on, and VDDQ is short-circuited through the transistor (P3, N3), the current always flows, and the UT_bar node must be pulled down to Grounding can completely turn off the p-type transistor (p3). This circuit will fail when _ VDD is low or VDDQ is high. If the saturation current of the transistor (N3) is not greater than the saturation current of the transistor (p3), the signal transmission rate will be very slow and it will take a long time. In deep submicron applications, it can cause severe delays.

第7頁 510022 五、發明說明(5) --------- 在超深次微米之領域範圍内,當核心元件之電位逐 下降到約1 · 〇伏時,電平位移裝置將無法運作。輸入/輸出 之臨界電壓(例如為3·3伏MOSFETs),無法與核心元件之供 應電壓VDD成比例降低之緣故。也就是說,電平位移裝置、 内的3·3伏NMOSs無法開啟(turn on)。 有二種方式可以解決習知技藝中所產生的問題,也就 是降低電平位移裝置中VDD和3· 3伏NMOSs間的電位差 (gap),第一種方式是利用核々NM0Ss代替33伏關〇^以得馨 到一個更低的臨界電壓,其中核心NMOSs臨界電壓例如為 0.5伏;第二種方式是提高(pUmp up)核心元件之供應電壓 從VDD到2VDD以得到更高的電壓來開啟3· 3伏NMOSs。雖然 第一種方式的電路結構沒有傳統習知技藝的缺點,但是它 必須花大約數十個//A的DC電流來產生偏壓(VBI AS),並且 須要額外的電路設計來關掉(turn off) DC偏壓在靜止模式 (sleep mode)情況下;而第二種方式的電路結構在 PVT(process voltage temperature)的情況不佳時運作太 慢,於數百萬Hz頻率的運用上需要花費5-ns的時間,另一 方面,若輸入訊號發生長時間不轉態(toggle)時,將由於_ 接面反偏壓電流(junction reversed-bias voltage leakage)而使得產生的電荷(PumP charges)漏電,這也將 導致有效的電壓回到VDD而不是開始的2VDD ’因此使得電 路容易受到外界干擾(noises)的影響。Page 7 510022 V. Description of the invention (5) --------- In the field of ultra-deep sub-micron, when the potential of the core component gradually drops to about 1.0 volts, the level shifter will Does not work. The input / output threshold voltage (for example, 3 · 3V MOSFETs) cannot be reduced in proportion to the supply voltage VDD of the core components. In other words, the 3 · 3 volt NMOSs inside the level shifter cannot be turned on. There are two ways to solve the problems in the conventional art, namely to reduce the potential difference (gap) between VDD and 3.3 V NMOSs in the level shift device. The first way is to use the nuclear 々NM0Ss instead of the 33 V gate. 〇 ^ Yi Dexin to a lower threshold voltage, where the core NMOSs threshold voltage is, for example, 0.5 volts; the second method is to increase (pUmp up) the supply voltage of the core components from VDD to 2VDD to get a higher voltage to turn on 3.3 V NMOSs. Although the circuit structure of the first method does not have the shortcomings of the conventional art, it must spend about tens of DC currents to generate the bias voltage (VBI AS), and it needs additional circuit design to turn off (turn off) The DC bias is in the sleep mode; while the circuit structure of the second method operates too slowly when the PVT (process voltage temperature) is not good, and it will cost millions of Hz to use 5-ns time, on the other hand, if the input signal toggles for a long time, it will cause the generated charges (PumP charges) due to _ junction reversed-bias voltage leakage Leakage, which will also cause the effective voltage to return to VDD instead of the initial 2VDD ', thus making the circuit susceptible to external noises.

第8頁 510022 五、發明說明(6) ---- - 另一個習知的具零臨界電壓金氧半場效電晶體之電平 f移裝置電路結構,其其係利用串聯(cascade)起來的電 =體去承叉南電壓,電晶體(NA1,NA2) 一直處於開啟狀 愍,而閘極連接到固定的電位VDD,參考圖三。其節點 INT1及INT2的電位接近於vdd+av,這樣的電位將導致關 掉的N1或^之閘極氧化層電崩潰(breakdown)。 因此,為了提升電路的穩定與運作速度,目前急需一 種新的電平位移裝置以取代習知技術的電平位移裝置。_ 發明目的及概述: 本發明之目的為:利用 電晶體(厚閘極氧化層)與一 取代習知技術厚閘極氧化層 裝置之操作速度。 一對零臨界電壓之金氧半場效 對N型電晶體(薄閘極氧化層) 之N型電晶體以增進電平位移 平位in為有零臨界電壓金氧半場效電晶體之電 移袭置,其係包括一反相器及一偏移閂。反 型電晶體及一隊ρ型電晶體所組成,其中上電 具有相對薄閘極氧化層,且Ρ型電晶體之 之電曰曰體 正偏壓,而Ν型電晶體之—極連接到—電 =一 而所述之偏料 1包括-對相^合之Μ電^為=型Page 8 510022 V. Description of the invention (6) -----Another conventional circuit structure of the level f shift device of a metal-oxygen half field effect transistor with zero critical voltage, which uses a cascade Electricity = body to support the south voltage, the transistors (NA1, NA2) are always on, and the gate is connected to a fixed potential VDD, refer to Figure 3. The potentials of the nodes INT1 and INT2 are close to vdd + av. Such a potential will cause the gate oxide layer of N1 or ^ to be electrically broken down. Therefore, in order to improve the stability and operation speed of the circuit, a new level shift device is urgently needed to replace the conventional level shift device. _ Purpose and summary of the invention: The purpose of the present invention is to use the transistor (thick gate oxide layer) and an operating speed to replace the thick gate oxide device of the conventional technology. A pair of zero-threshold metal-oxygen half-field-effects A pair of N-type transistors (thin gate oxide) N-type transistors to enhance the level shift level in Device, which includes an inverter and an offset latch. An inversion transistor and a group of p-type transistors, where the power-on has a relatively thin gate oxide layer, and the electric current of the P-type transistor is positively biased, and the-pole of the N-type transistor is connected to —Electricity = One and the said partial material 1 includes-the corresponding M electricity is = type

第9頁 510022 五、發明說明(7) I ^ ^t t ^ ^ ^ ^ !電曰曰體八有相對厚的閘極氧化層,其中一極連接 里_型電晶體具有相對薄的閘極氧化層, ϊ之ΐ ίίί一電位通常為接地,閘極分別連接於反相 i 。另外,具有零臨界電壓Ν型電晶 ㈣ίί 厚之間極氧化層,其閉極分別連接於該反 i f^ 端’其它兩極分別與相互麵科型電 、:桎遠接m體連接,也就是’零臨界電編型電晶體之 及極連接於PM0S之汲極,其源極連接於肫⑽之汲極。 發明詳細說明 次微 圖五 本發明所要揭示的為一種電 米互補金氧半場效電晶體, ’以及詳細說明將敘述如下 平位移裝置,應用於超深 其電路架構請參閱圖四及 圖一為各種不同類型金氧半場效電晶體的符號❶圖四 所不為本發明之具零臨界電壓金氧半場效電晶體之電平位 移裝置電路架構,其包含一反相器由電晶體(N、N〇)及 P型電晶體(P、P〇)所組成,以及包含一偏移閃。偏移問由籲 一對N型電晶體(N1、N2)、一對零臨界電壓之N型電晶體 (ΝΑΙ、NA2)以及一相互耦合之p型電晶體(ρι、p2)所構 成’也就疋P型電晶體(P2)之閘極連接到n型電晶體(ναι) 之汲極,同理,Ρ型電晶體(Pl)之閘極也連接到N型電晶體Page 9 510022 V. Description of the invention (7) I ^ ^ tt ^ ^ ^ ^! The electric body has a relatively thick gate oxide layer, of which the _-type transistor in one pole connection has relatively thin gate oxide Layer, ϊ 之 ΐ ί a potential is usually grounded, the gates are connected to the reverse phase i respectively. In addition, the N-type transistor with zero critical voltage has a thick interlayer oxide layer, and its closed electrodes are respectively connected to the inverse if terminal. The other two poles are respectively connected to the mutual surface-type electrical and: 'The sum of the zero-critical electro-transistor transistor is connected to the drain of PMOS, and its source is connected to the drain of 肫 ⑽. Detailed description of the invention: Sub-micrograph 5. The present invention is to disclose an electric meter complementary metal-oxide half-field effect transistor, and the detailed description will describe the following translational displacement device, which is applied to ultra-deep circuit structure. Please refer to Figure 4 and Figure 1. Symbols of various types of metal-oxide-semiconductor half-field-effect transistors. Figure 4 does not show the circuit structure of the level-shifting device of the metal-oxide-semiconductor half-field-effect transistor with zero critical voltage according to the present invention. No.) and P-type transistors (P, P0), and includes an offset flash. The offset problem consists of a pair of N-type transistors (N1, N2), a pair of zero-voltage N-type transistors (NAI, NA2), and a mutually coupled p-type transistor (ρ, p2). As for the gate of the P-type transistor (P2) is connected to the drain of the n-type transistor (ναι), the gate of the P-type transistor (Pl) is also connected to the N-type transistor.

510022 五、發明說明(8) -----— — (NA2)之汲極。 零臨界電壓金氧半場效電晶體的vt例如為〇伏, 來保護N型電晶體(Νι) 型電晶體(N2)免於高壓的應力 5( = reSS),N型電晶體(…^以型電晶體^2)的以例:為〇· 本發明與習知技術所不同之處有兩點(1 )N型電晶體 (Nl、N2)為薄閘極氧化層之電晶體,與傳統之厚閘:氧化 層電晶體不同,其源極則連接到一電位通常為接地,N型 電晶體(N1、NA1)之閘極連接於反相器之輸入端,而1^型_ 晶體(N2、NA2)之閘極則連接於反相器之輸出端。(2)本發 明加入一對零臨界電壓之金氧半場效N型電晶體“^、 X NA2),其汲極連接於P型電晶體之汲極,其源極連接於1^型 電晶體之沒極’閘極則分別連接於反相器之輸入端、輸出 端,也就是說’ N型電晶體(ΝΑΙ、NA2)的閘極是接到一個 可變動的電位訊號(signal)。除此之外,對於元件可靠度 而言,所有VDDQ只偏壓到具有厚閘極氧化層之p型電晶 體,而具有薄閘極氧化層之P型電晶體及N型電晶體只受到 VDD偏壓。 · 所述反相器藉由輸入端(IN)接收一輸入訊號之電壓位 準,經由偏移閂將電平位移輸出一預定範圍位準之輸出訊 號。,般,輸入的低電位訊號約介於VDD-VSS之間,經由510022 V. Description of invention (8) ------(NA2) The drain. The vt of the zero critical voltage metal-oxide half field effect transistor is, for example, 0 volts to protect the N-type transistor (Nι) -type transistor (N2) from high-voltage stress 5 (= reSS), and the N-type transistor (... ^ to An example of the type transistor ^ 2) is: The difference between the present invention and the conventional technology is two points (1) the N-type transistor (Nl, N2) is a thin-gate oxide transistor, and the traditional Thick gate: the oxide transistor is different, its source is connected to a potential which is usually ground, the gate of the N-type transistor (N1, NA1) is connected to the input of the inverter, and the type 1_ crystal ( The gates of N2 and NA2) are connected to the output of the inverter. (2) The present invention adds a pair of zero-critical metal-oxide half-field-effect N-type transistors "^, X NA2", whose drain is connected to the drain of the P-type transistor, and its source is connected to the 1 ^ -type transistor. The "Zhi pole" gate is connected to the input and output terminals of the inverter, which means that the gate of the "N-type transistor (NAI, NA2) is connected to a variable potential signal. In addition In addition, for device reliability, all VDDQs are biased only to p-type transistors with thick gate oxide layers, while P-type transistors and N-type transistors with thin gate oxide layers are only biased by VDD. · The inverter receives a voltage level of an input signal through an input terminal (IN), and outputs a level shift output signal of a predetermined range level through an offset latch. Generally, an input low-potential signal Between VDD-VSS, via

510022 五、發明說明(9) 偏移裝偏移置處理後之電位位準約介於VDDQ_VSS之間。本 發明之訊號輸入端只連結到電晶體(N1、n A1、P、P 〇、N、 NO)之閘極’且反相器之輸出接到n型電晶體(N2、NA2)之 閘極,對於輸入訊號沒有DC漏電流路徑。因為只有電晶體 (P、NO)及電晶體(N、P0)之一會開啟,所以從VDD到vss沒 有短路電流。另外,只有電晶體(pi、N2)或電晶體(P2、 N1)之一同時開啟,因此介於VDDq到vss之間也沒有短路電 流之路徑。 圖四所述裝置之操作條件如下,在訊號輸入端(丨N )輸· 入一較低電位訊號(如VSS)時,p型電晶體(p)開啟,n型電 晶體(N)關閉,則將IN-bar電位提升為較高之電位VDD,因 而N型電晶體(NO)開啟,p型電晶體(P〇)關閉。此時,因為510022 5. Description of the invention (9) Offset device The potential level after the offset processing is approximately between VDDQ_VSS. The signal input terminal of the present invention is only connected to the gates of the transistors (N1, n A1, P, P 0, N, NO), and the output of the inverter is connected to the gates of the n-type transistors (N2, NA2). There is no DC leakage current path for input signals. Because only one of the transistors (P, NO) and transistors (N, P0) will turn on, there is no short-circuit current from VDD to vss. In addition, only one of the transistors (pi, N2) or transistors (P2, N1) is turned on at the same time, so there is no short-circuit current path between VDDq and vss. The operating conditions of the device described in Figure 4 are as follows. When a lower potential signal (such as VSS) is input to the signal input terminal (丨 N), the p-type transistor (p) is turned on and the n-type transistor (N) is turned off. The IN-bar potential is increased to a higher potential VDD, so the N-type transistor (NO) is turned on and the p-type transistor (P0) is turned off. At this time, because

IN-bar之拉升(pull up),所以開啟n型電晶體(N1),而N 型電晶體(N2)關閉。由於n型電晶體(NA1)為開啟狀態, LDSR1的電壓位準會低於VDDq減去臨界電壓之值,N型電晶 體(N A 2 )為關閉狀態’因此,I n τ 1的電位接近〇伏,造成p 型電晶體(P2)開啟,而ουτ-bar之LDSR處電位變為VDDQ, 使得P型電晶體(P1)關閉,接著,N型電晶體(N3)開啟,而 P型電晶體(P3)關閉,此時輸出端(〇υτ)完全被下拉到電位春 為零或接地(ground)。 一 反之’倘若在訊號輸入端(IN)由VSS轉換為輸入一較 兩之電位訊號,例如VDD時,N型電晶體(N)開啟,p型電晶The IN-bar pulls up, so the n-type transistor (N1) is turned on, and the n-type transistor (N2) is turned off. Because the n-type transistor (NA1) is on, the voltage level of LDSR1 will be lower than VDDq minus the threshold voltage, and the N-type transistor (NA 2) is off. Therefore, the potential of I n τ 1 is close to 0. Voltage, causing the p-type transistor (P2) to turn on, and the potential at the LDSR of ουτ-bar becomes VDDQ, so that the P-type transistor (P1) is turned off, then the N-type transistor (N3) is turned on, and the P-type transistor is turned on (P3) is turned off. At this time, the output terminal (0υτ) is completely pulled down to the potential spring to zero or ground. "Conversely" If the signal input terminal (IN) is converted from VSS to a potential signal of one to two, for example, VDD, the N-type transistor (N) is turned on, and the p-type transistor

第12頁 510022Page 510022

體(P)關閉’則將IN-bar從VDD拉為較低之電位(接地),因 而P型電晶體(P0)開啟,而N型電晶體(N0)關閉。因為 IN-bar之下拉所以開型電晶體(]^2),N型電晶體(N1)關 閉’由於N型電晶體(NA1)為開啟狀態,n型電晶體(NA2)為 關閉狀態,因此,ιΝΤ1的電位接近0伏,此時LDSR1的電壓 低於VDDQ減掉臨界電壓之值,造成p型電晶體(p2)開啟, 而OUT-bar之LDSR1處電位變為VDDQ,使得P型電晶體(P2) 關閉,接著,P型電晶體(P3)開啟,而N型電晶體〇3)關 閉’因此輸出端(OUT)之電位為VDDQ。 m 本發明除了接面電流(junct i〇n ieakage)及次臨界電 流(sub-threshold leakage)之外不會有電流之損失,也 不會產生DC靜電流以及短路電流。 因為N型電晶體(ΝΑΙ、NA2),原先厚閘極氧化層之電 晶體將被具有較薄閘極氧化層之電晶體取代且執行相同之 功能。此薄的閘極氧化層之臨界電壓較低,以及具有較高 之飽和電流。此較低之臨界電壓造成本發明可以將較低g 位之VDD轉換為VDDQ。藉由N型電晶體(ΝΑΙ、NA2)之保護可 以使得薄閘極氧化層之Ν型電晶體〇1、Ν2)不會被高 _ 接偏壓。 當VDD=1.0V時’習知技術無法正常運作,因為 極氧化層之N型電晶體(N1、N2)無法提供足夠大的電流。Body (P) OFF 'pulls IN-bar from VDD to a lower potential (ground), so the P-type transistor (P0) is turned on and the N-type transistor (N0) is turned off. Because the IN-bar is pulled down, the on-type transistor (] ^ 2) is turned on, and the N-type transistor (N1) is off. Because the N-type transistor (NA1) is on and the n-type transistor (NA2) is off, so The potential of ιΝΤ1 is close to 0 volts. At this time, the voltage of LDSR1 is lower than VDDQ minus the threshold voltage value, causing the p-type transistor (p2) to turn on, and the potential at LDSR1 of OUT-bar becomes VDDQ, making the P-type transistor (P2) is turned off, then the P-type transistor (P3) is turned on, and the N-type transistor (03) is turned off ', so the potential of the output terminal (OUT) is VDDQ. m In addition to the junction current (junct ion) and sub-threshold leakage, the present invention does not cause current loss, nor does it generate DC static current and short-circuit current. Because of the N-type transistor (NAI, NA2), the original transistor with a thicker gate oxide layer will be replaced by a transistor with a thinner gate oxide layer and perform the same function. This thin gate oxide layer has a lower threshold voltage and a higher saturation current. This lower threshold voltage causes the present invention to convert the lower g-bit VDD to VDDQ. The protection of the N-type transistor (NAI, NA2) can prevent the N-type transistor (01, N2) of the thin gate oxide layer from being biased by a high voltage. When VDD = 1.0V, the conventional technique cannot work normally because the N-type transistors (N1, N2) of the polar oxide layer cannot provide a sufficient current.

第13頁 510022 發明說明(11) 然而,在相同條件之下本發明仍然可以正常操作,因為本 發明之薄閘極氧化層電晶體之飽合電流較高於習知技術。 因此’具有零臨界電壓之金氧半場效電晶體是〇· 13微米 (um)以下之雙閘極氧化層CM〇s製造之關鍵元件。當n型電 晶體NA1(NA2)的次臨界電流(sub-threshold leakage)等 於N型電晶體NA1+N1 (NA2 + N2)之接面反偏壓電流,Δν即 為平衡電壓,並且Ρ型電晶體?1(!>2)拉升時,關掉Ν型電晶 體ΝΑ1(ΝΑ2)能隔離來自節點(n〇(je)LSDRl(LSDR)之寄生 (parasitic)電容C1(C2),而導致速度之提升。此方法並 不需要額外的製程(no extra process),且於數百萬。頻馨 率的運用上只需要花費約卜ns的時間。 圖五為本發明具有零臨界電壓之金氧半場效電晶體之 電平位移電路示意圖。圖五與圖四之差別為於N型電晶體 (ΝΑΙ、NA2)與N型電晶體(Nl、N2)間多加了一對n型電晶體 (N3、N4),其中上述N型電晶體(N3、N4)閘極連接電位 VDD ’其係用來更佳地保護n型電晶體(Ni、N2),使得薄閘 極氧化層之N型電晶體(Nl、N2)不會被高壓直接偏壓。 對於邏輯電路而言,根據Sp i c e模型的模擬結果估計_ INT1與INT2的電位有一些困難性,並且n型電晶體(ναι 、ΝΑ2)的次臨界電流模型也無法精確估算,因此,可藉由 增加一對Ν型電晶體(Ν3、Ν4)來進一步保護Ν型電晶體曰 (Nl、Ν2)。此方法並不需要額外的製程(n〇 extraPage 13 510022 Description of the invention (11) However, the present invention can still operate normally under the same conditions, because the saturation current of the thin gate oxide transistor of the present invention is higher than that of the conventional technology. Therefore, a metal-oxide-semiconductor field-effect transistor with a zero critical voltage is a key element for manufacturing a double-gate oxide layer CMos below 0.1 micron (um). When the sub-threshold leakage of the n-type transistor NA1 (NA2) is equal to the reverse bias current of the junction of the N-type transistor NA1 + N1 (NA2 + N2), Δν is the equilibrium voltage, and the P-type transistor Crystal? 1 (! ≫ 2) When pulled up, turning off the N-type transistor NA1 (NA2) can isolate the parasitic capacitor C1 (C2) from the node (n0 (je) LSDR1 (LSDR), resulting in speed Enhancement. This method does not require no extra process, and it is in the millions. The use of frequency rate only takes about ns time. Figure 5 shows the metal-oxygen half field with zero critical voltage in the present invention. Schematic diagram of the level shift circuit of an effect transistor. The difference between Figure 5 and Figure 4 is that an additional pair of n-type transistors (N3, N3, N3, N2, N2, N2, N2, N2, N2) N4), where the above N-type transistor (N3, N4) gate connection potential VDD 'is used to better protect the n-type transistor (Ni, N2), so that the N-type transistor with a thin gate oxide layer ( Nl, N2) will not be directly biased by high voltage. For logic circuits, it is difficult to estimate the potential of INT1 and INT2 according to the simulation results of the Sp ice model, and the subcriticality of n-type transistors (ναι, ΝΑ2) The current model cannot be accurately estimated either. Therefore, the N can be further protected by adding a pair of N-type transistors (N3, N4). Said transistors (Nl, Ν2). This method does not require an additional process (extra n〇

第14頁 510022 五、發明說明(12) process),且於數百萬Hz頻率 的時間。 千幻連用上^、而要花費約卜ns 因此,本發明之優點為:本發明電平位移裝 =外的製程’即能使其運作速度比傳統電平位移裝置= 成,、,並且不會消耗DC電流;另外,本發明的電路設計甚 至能運作於設計規則(design rule )0· 1微米以下(um)的電 路° 對熟悉此領域技藝者,本發明雖以一較佳實例闡明如 上’然其並非用以限定本發明精神。在不脫離本發明之精 神與範圍内所作之修改與類似的安排,均應包含在下述之 中請專利範圍内,這樣的範圍應該與覆蓋在所有修改與類 似結構的最寬廣的詮釋一致。因此,闡明如上的本發明一 較佳實例’可用來鑑別不脫離本發明之精神與範圍内所作 之各種改變。Page 14 510022 V. Description of the invention (12) process), and the time at the frequency of millions of Hz. Thousands of magic are used together, and it takes about ns. Therefore, the advantages of the present invention are: the level shift device of the present invention = an external process, that is, it can make its operation speed faster than that of a traditional level shift device, and does not DC current will be consumed; in addition, the circuit design of the present invention can even operate on circuits with a design rule of less than 1 micron (um) ° For those skilled in the art, the present invention is illustrated by a better example as above 'But it is not intended to limit the spirit of the invention. Modifications and similar arrangements made without departing from the spirit and scope of the present invention should be included in the scope of the following patents, and such scope should be consistent with the broadest interpretation covering all modifications and similar structures. Therefore, the description of a preferred embodiment of the present invention as described above can be used to identify various changes made without departing from the spirit and scope of the present invention.

510022 圖式簡單說明 本發明的較佳實施例將於往後之說明文字中輔以下列圖 形做更詳細的闡述: 圖一為各種不同類型金氧半場效電晶體示意圖。 圖二為習知技術之電平位移之電路示意圖。 圖三為習知技術具有零臨界電壓之金氧半場效電晶體之電 平位移電路示意圖。 圖四為本發明具有零臨界電壓之金氧半場效電晶體之電平 位移電路示意圖。 圖五為本發明具有零臨界電壓之金氧半場效電晶體之電平· 位移電路不意圖。510022 Brief description of the drawings The preferred embodiment of the present invention will be described in more detail in the following explanatory text with the following figures: Figure 1 is a schematic diagram of various types of metal-oxide half-field effect transistors. FIG. 2 is a schematic diagram of a level shift circuit of the conventional technology. Figure 3 is a schematic diagram of a level shift circuit of a conventional metal-oxide-semiconductor half field-effect transistor with zero critical voltage. FIG. 4 is a schematic diagram of a level shift circuit of a metal-oxide half-field-effect transistor with zero critical voltage according to the present invention. FIG. 5 is a schematic diagram of the level and displacement circuit of the metal-oxide-semiconductor half field-effect transistor with zero critical voltage according to the present invention.

第16頁Page 16

Claims (1)

1 t月2利乾圍 飞rrT,V^ .二^有零臨界電壓元件之高速電平位ixiH 一為移閂(shlft latch),該偏移閂包含·· L 3 卜、十、P ,互耦合(crossed_couple)之P型電晶體,复Φ 第二電晶體之一極連接於第二正偏壓;/、 诚坌一.型電晶體’具有第-厚度的閘極氧化層,其Φ " 對N型電晶體之源極連接到一電位通常為接地上 操作速度Ί A 以增進該電平位移裝置之 ί〗;:型體,係為零臨界電壓之N型電晶體,閘極分 對相器之輸入端與輸出端’其它兩極分別與該 對㈣带曰:1電晶體、該第一對Ν型電晶體連接,該第二 厚於該ya_體具有第二厚度之問極氧化層’該第二厚度較 該第二對電:::其中上述之第二對N型電晶體用以保護 2. ί! ϊ ί::圍第1項之具有零臨界電壓之金氧半場效 /dd曰曰脰 移裝置,其中上述之第一正偏壓為 3,==圍第1項之具有零臨界電壓之金氧半場效 二: 裝置,其中上述第二正偏壓為1 month and 2 months, rrT, V ^. Two high-speed level ixiH with zero critical voltage element. One is a shlft latch. The offset latch contains ... L 3 BU, X, P, Cross-coupled P-type transistor, complex Φ One of the second transistor is connected to the second positive bias voltage; / 、 Since the first type transistor has a gate oxide layer of the first thickness, its Φ " When the source of N-type transistor is connected to a potential, the operating speed is usually Ί A to increase the level shift device. 型: The body is an N-type transistor with zero critical voltage, gate The input and output ends of the phase splitter's other poles are respectively connected to the pair of bands: 1 transistor, the first pair of N-type transistors are connected, the second thicker than the ya_body has a second thickness Extremely oxidized layer 'The second thickness is greater than the second pair of electricity ::: where the second pair of N-type transistors described above are used to protect 2. ί! Ϊ ί :: metal oxide with zero critical voltage around item 1 Half-field-effect / dd-shift device, where the first positive bias voltage is 3, == metal-oxygen half-field-effect with zero critical voltage around item 1 Wherein said second positive bias 510022510022 4. 一種電平位移裝置,該電平位移裝置包含·· 一偏移閃(shift latch),包含一對相互耦合(cr〇ssed — couple)之p型電晶體,第一對~型電晶體,係為具 有零臨界電壓之〜型電晶體,以及第二對N型電晶 體★ f用以增進該電平位移裝置之操作速度,其中該第二 對電晶體之閘極氧化層相對於該第一對電晶體之閘極氧化 層為薄,且該第二對N型電晶體之源極連接到一電位通常 為接地,而其閘極分別連接於一反相器之輸入端與輸出 端0 5· —種具‘有零臨界電壓元件之高速電平位移裝置,該電 位 移器裝置包含: 一偏移問(shi ft latch),該偏移閂包含: 一對相互耦合(crossed —c〇upU)之?型電晶體,其中上述p 型電晶體之一極連接於第二正偏壓; 第對^型黾晶體,具有第一厚度的閘極氧化層,其中上 f第、,對N型電晶體之源極連接到一電位通常為接地,該 第對N型電晶體之閘極分別連接於一反相器之輪入端與 輸出端,該第一對N型電晶體用以增進該電平位移裝置之 操作速度; 又 第一對N型電晶體,系為零臨界電壓之N型電晶體,閘極分 別連接於反相為之輸入端與輸出端,其它兩極分別與該對 相互耦合p型電晶體、該第一對N型電晶體連接,該第二對4. A level shifting device comprising a shift latch, including a pair of p-type transistors coupled to each other (cr0ssed — couple), a first pair of ~ type transistors Is a ~ -type transistor with a zero critical voltage, and a second pair of N-type transistors. F is used to increase the operating speed of the level shift device, wherein the gate oxide layer of the second pair of transistors is opposite to the The gate oxide layer of the first pair of transistors is thin, and the source of the second pair of N-type transistors is usually connected to a potential, and the gates are respectively connected to the input terminal and the output terminal of an inverter. 0 5 · —A kind of high-speed level shifting device with a zero critical voltage element. The electric shifter device includes: a shift latch (shi ft latch), the shift latch includes: a pair of cross-coupled (c 〇upU)? Type transistor, in which one of the p-type transistors is connected to a second positive bias voltage; the second pair of 黾 -type 黾 crystals has a gate oxide layer of a first thickness, where the fth and the n-type transistors are The source is usually connected to a potential, and the gate of the second pair of N-type transistors is connected to the input and output ends of an inverter. The first pair of N-type transistors is used to enhance the level shift. The operating speed of the device; and the first pair of N-type transistors are N-type transistors with zero critical voltage. The gates are connected to the input and output terminals of the opposite phase, and the other two poles are coupled to the pair. The transistor, the first pair of N-type transistors are connected, and the second pair 第18頁 六、申請專利範圍 N型電晶體具有第二厚度 於該第一厚度,其中上述第二對^型該第二厚度較厚 一對電晶體;以及 、 缝晶體用以保護該第 第三對N型電晶體,具有第二 厚度較薄於該第二厚度;其子广、)一極氧化層,該第三 極連接到該第一對N型電a顺 处弟二對N型電晶體之源 之没極連接到該第一對::的及極1第三對N型電晶體 曰㈣之H I ” 電晶體的及極,該第三對N型電 曰日體之閘極分別連接於第一 ^ 用以保護該第一對電晶體。偏£ ’該第三對Ν型電晶體 6·如申請專利範圍第5 電晶體之電平位移裝置,其、有令?電壓之金氧半場效 VDD。 、中上述弟一正偏壓為 7·如申請專利範圍第5項之星 電晶體之電平位移裝置,其、有令二界笔壓之金氧半場效 VDDQ。 、Τ上述弟一正偏壓為 8. -:二平位移裝置’該電平位移袭置包含: 偏私問(shi f t lat_ch),勺人批丄 couple)之p型電晶體,第 包3 一對相互耦合(crossed- 電平位移裝置之操作速ΓΓ第型電二體’係用以增進該 接到-電位通常為接地,而電晶體之源極連 輸入端與輪出端’第 而厂間極7刀別連接於一反相器之 以# 型f晶體’係為具有零臨界電Page 18 VI. Patent application scope The N-type transistor has a second thickness over the first thickness, wherein the second pair of the second-thickness and the second-thicker pair of transistors; and Three pairs of N-type transistors, having a second thickness that is thinner than the second thickness; a second electrode, an oxide layer, and the third electrode connected to the first pair of N-type transistors. The source electrode of the transistor is connected to the first pair of :: and the pole 1 and the third pair of N-type transistors called the HI of the transistor, and the third pair of N-type transistors. Connected to the first ^ to protect the first pair of transistors. The third pair of N-type transistors 6. If the level shifting device of the fifth transistor in the patent application scope, the order of voltage Metal-oxygen half-field effect VDD. The positive bias voltage of the above-mentioned brother is 7. If the level shift device of the star transistor of item 5 of the patent application is applied, it has metal-oxygen half-field effect VDDQ which enables the pressure of the second boundary. ΤThe above-mentioned positive bias voltage is 8.-: Two-level displacement device 'This level shifting device includes: partial bias (shi ft lat_ch ), A p-type transistor approved by a couple of people, the first package 3 a pair of mutually-coupled (level-shift device operating speed ΓΓ-type electric two-body) is used to improve the connection-the potential is usually grounded The source of the transistor is connected to the input terminal and the wheel output terminal, and the inter-factory pole 7 is connected to an inverter. The # type f crystal is a system with zero critical voltage. 第19頁 510022 ij 六、申請專利範圍 壓之N型電晶體,該第二對電晶體之閘極氧化層相對於該 第一對電晶體之閘極氧化層為厚,該第二對N型電晶體係 用以保護該第一對電晶體,以及第三對N型電晶,該第三 對電晶體之閘極氧化層相對於該第二對電晶體之閘極氧化 層為薄,該第三對N型電晶體係用以保護該第一對電晶 體0Page 19 510022 ij 6. For the N-type transistor with a patent application range, the gate oxide layer of the second pair of transistors is thicker than the gate oxide layer of the first pair of transistors, and the second pair of N-type transistors The transistor system is used to protect the first pair of transistors and the third pair of N-type transistors. The gate oxide layer of the third pair of transistors is thin compared to the gate oxide layer of the second pair of transistors. A third pair of N-type transistor systems is used to protect the first pair of transistors. 第20頁Page 20
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