TW200810331A - Circuit of charge pump - Google Patents

Circuit of charge pump Download PDF

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TW200810331A
TW200810331A TW095128383A TW95128383A TW200810331A TW 200810331 A TW200810331 A TW 200810331A TW 095128383 A TW095128383 A TW 095128383A TW 95128383 A TW95128383 A TW 95128383A TW 200810331 A TW200810331 A TW 200810331A
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Taiwan
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circuit
boost
boosting
charge
turned
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TW095128383A
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Chinese (zh)
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TWI321892B (en
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Che-Ming Wu
Ying-Feng Wu
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G Time Electronic Co Ltd
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Abstract

A circuit of charge pump includes a plurality of diode equivalent networks, at least a boost capacitance network, and at least a reverse current cut-off circuit. The diode equivalent networks are electrically connected in series. A node is formed between two diode equivalent networks. Each node corresponds to a voltage-boosting step, in which the low voltage side of the diode equivalent network with a lowest voltage-boosting step is an input end of the circuit of charge pump. The input end receives an input voltage signal. One end of each of the boost capacitance network is separately connected electrically to one of the nodes. Another end of each of the boost capacitance network is separately connected electrically to a clock signal. Each of the reverse current cut-off circuits is separately connected electrically to the diode equivalent networks, in which the reverse current cut-off circuits include at least two conductive paths, which form a closed loop according to the switching of clock signal in each voltage-boosting step.

Description

200810331 九、發明說明: - 【發明所屬之技術領域】 、日本發嗎關於-種電荷增壓電路,尤指由逆電流截止電路 以提升電路效率以及可靠度之電荷增壓電路。 【先前技術】 電荷增壓電路(Charge Pump)是一種通過電容上 電荷累積效應以實現升降壓的電路。隨著各類可攜式以 及快閃記憶體裝置及應用的發展,系統所需工作^壓高 2電源供應電壓的狀況也日趨普見,其中所衍生的電源 官理問題,適可利用升壓型電荷增壓電路作為解決方 法。一個升壓型電荷增壓電路能夠穩定遞降電壓或產生 高於電源電壓的輸出,請見第1圖,為一習知之雙時向 (Dual Phase)電荷增壓電路100示意圖,該電荷增壓 電路100包含一組以二極體方式串接型金氧半導體 電晶體(Diode-connected NMOS Transistor)以及複數 電容,其中該等N型金氧半導體電晶體之結構具有臨界 電壓Vt,該等電容分別電連接於兩n型金氧半導體電 曰日m間之郎點。其工作原理係利用一對反相時脈信號p 1以及p 2,對該等電容進行交替充電而達成增壓的目 的,依照電流路徑的不同,其電路工作週期(cl〇ck cycle) 可分為設定週期(setup peri〇d)以及升壓週期(pumping period )’在設定階段時,該時脈信號% 1為低位準 (low ),該雙時向電荷增壓電路丨〇〇開啟一第一充電路 徑110,該第一充電路徑110上之N型金氧半導體電晶 體導通直到一第一節點120上之電壓值到達vin-vt,此 k 一笔谷C1之電壓亦充電至Vin_vt。接著,於升壓階 5 200810331 &纣,忒犄脈信號$ i為高位準(),本實施例中, =時脈信號之電壓值於升壓階段到達,將會使得電 备c 1電壓也因此提升ν φ,而使得該第一節點1 上 之電壓值到達vin+(v(^vt),當節點120電壓值大於η 型金氧半導體電晶體的臨界電壓值Vt,此時也開啟第 二充電路徑H0並使得一第二節點13〇上之電壓值到達 =ιη一+(J p _Vt)-Vt。同理可得,於下一個設定週期時,該 第一節點130上之電壓值到達Vin + 2(v % 。 總結來說,一個包含n個節點的雙時向電荷增壓電 路之輸出電壓值可表示為:200810331 IX. Description of the invention: - [Technical field to which the invention pertains], Japanese-made charge-charge circuit, especially a charge boost circuit that improves the efficiency and reliability of the circuit by a reverse current cut-off circuit. [Prior Art] A charge pump is a circuit that realizes buck-boost by a charge accumulation effect on a capacitor. With the development of various portable and flash memory devices and applications, the system requires a high voltage 2 power supply voltage, and the power supply policy is derived from the power supply. A type of charge boost circuit is used as a solution. A boost type charge boost circuit capable of stabilizing the voltage drop or generating an output higher than the power supply voltage, see FIG. 1 , is a schematic diagram of a conventional dual phase charge boost circuit 100, the charge boost circuit 100 includes a set of diode-connected MOS transistors and a plurality of capacitors, wherein the structures of the N-type MOS transistors have a threshold voltage Vt, and the capacitors are respectively charged Connected to the two n-type MOS semiconductors. The working principle is to use a pair of inverted clock signals p 1 and p 2 to alternately charge the capacitors to achieve supercharging. According to the current path, the circuit cycle (cl〇ck cycle) can be divided. In order to set the period (setup peri〇d) and the pumping period (in the setting phase), the clock signal %1 is at a low level (low), and the dual-time charge boost circuit is turned on. In a charging path 110, the N-type MOS transistor on the first charging path 110 is turned on until the voltage value on the first node 120 reaches vin-vt, and the voltage of the k-cell C1 is also charged to Vin_vt. Then, in the boosting stage 5 200810331 & 纣, the pulse signal $ i is a high level (), in this embodiment, = the voltage value of the clock signal arrives in the boosting phase, which will cause the voltage of the power supply c 1 Therefore, ν φ is raised, so that the voltage value on the first node 1 reaches vin+(v(^vt), and when the voltage value of the node 120 is greater than the threshold voltage value Vt of the n-type MOS transistor, the same is also turned on. The second charging path H0 causes the voltage value on a second node 13 to reach = ηη + (J p _Vt) - Vt. Similarly, the voltage value at the first node 130 at the next set period is obtained. Reach Vin + 2 (v %. In summary, the output voltage value of a dual-time charge boost circuit with n nodes can be expressed as:

Vout = Vin+N*(V(p .Vt)-Vt ........ ( 1-1 )。 曰由1 -1式之關係中可以發現,受限於金氧半導體電 晶體結構中,臨界電壓vt (thresh〇][d v〇hage)效應的 存在,該電荷增壓電路i 00的增壓效率因而下降,造成 系統效率不彰,尤其在低電源電壓狀況下,臨界電壓效 應對系統效能造成的影響將十分明顯,使得該電荷增壓 電路100並不適用於低電壓操作,而一般的電路應用上 其增壓的效率不佳造成必須有更多的功率消耗來彌補 更是其很大的缺點。 々為此,許多對電荷增壓電路的改良相繼被提出。請 見第2圖,為美國專利證號·· 6,670,884 B2所揭露之一 種改良式電荷增壓電路2〇〇,該改良式電荷增壓電路 200之結構與該電荷增壓電路1 〇〇大致相同,唯該改良 式電荷增壓電路200中之二極體連接金氧半導體電晶 體係以空乏型金氧半導體電晶體(Depleti〇n-type MQS Transistor )實施。其優點以空乏型N通道金氧半導體 電晶體(Depleti〇n-type N.channel M〇s Transist〇r)舉例 200810331 之,其臨界電壓值為負值,其特性使得空乏型N通道金 氧半導體電晶體之通道持續維持導通狀態,除非其閘源 級間電壓(Vgs )被施加一低於臨界電壓之電壓值。利 用上述空乏型金氧半‘體電晶體的特性,該改良式電荷 增壓電路200得以避免臨界電壓Vt效應所造成的系統 效能下降的影響,使該改良式電荷增壓電路2〇〇的輸出 電壓較同階之該電荷增壓電路100為高。但是,於此同 曰守,上述空乏型金氧半導體電晶體的特性亦使得該改良 式電荷增壓電路200於工作時脈切換時,當節點a的電 壓已經被增壓後,該等空乏型N通道金氧半導體電晶體 仍無法截止(turn off),因而沿一路徑21〇產生一反向 漏電流Iq,該反向漏電流Iq與電荷增壓電路1〇〇中採 用 J曰強型 N 通道電晶體(Enhancement_type N_channel Transistor)之臨界電壓vt所造成增壓的效率不佳之效 應相同,都將造成系統效能的低下,尤有甚者,該反向 漏電流Iq於該改良式電荷增壓電路2〇〇中溢流更可能 使系統損毀,降低可靠度,為了防止可靠度下降,系统 常需增加保護電路,這樣的措施又使得系統的成本上 升’更不利於產品的應用與銷售。 為J減少該反向漏電流Iq,該改良式電荷增壓電路 =〇揭露了利用改變該等空乏型金氧半導體電晶體之長 寬比(W/L)參數以降低該反向漏電流Iq的方法,但這 樣0方法僅此降低卻無法完全避免該反向漏電流Iq的 產生過度麦化的電晶體長寬比除了增加製程的難度 ^ ^可此產生设計時所無法察覺的電性干擾,總結而 這樣的作法首先無法完全截止反向逆電流,再者製 程難度的增加亦可能增加生產成本,其次可能發生的電 性干擾亦使得電路之可靠度下降。 200810331 為此,一種於完全截止反向逆電流的同時,亦得以 維持電路可靠性之電荷增壓電路,是十分有其需要的。 【發明内容】 本發明之一目的在於提供一種升壓電荷增壓電 路,該升壓電荷增壓電路利用空乏型電晶體 (Depletion_type M〇s心⑽仏化。組成等效串接二極 體’使該升壓電荷增壓電路無臨界電壓損耗以增加升壓 效率。 本心月之另目的在於提供一種升壓電荷增壓電 路:該升壓電荷增壓電路包含至少一逆電流截止電路, 该逆電流截止電路截止反向漏電流以增加升壓效率。 本發明之另一目的在於提供一種升壓電荷增壓電 路,該升壓電荷增壓電路包含至少―逆電流截止電路, 該升壓電荷增壓電路無須使用特殊製程,得以節省成 奉戬月之另一目的在於提供一種升壓電荷增屙雷 路’該升壓電荷增壓電路包含至少—逆電流戴止電^, 該逆電流截止電路截止反向漏電流,以減少電性 , 增加系統可靠度。 欠亚 本發明之另一目的在於提供一種升壓電荷擗厣雷 路,該升壓電荷增壓電路包含至少―穩壓電路,^ 定的輸出電壓。 fe 路,::現上述目的,本發明提供一種升壓電荷增壓電 複數二極體等效網路,其中 該 極體等效網路係 8 200810331 以串聯方式電诖姑 卜 節點,每一兮,母兩該等二極體等效網路間具有一 該二極體等效網路之屙中农低升壓階之 輸入端,該輪入浐桩你 為该升壓電荷增壓電路之一 而接收一輸入電壓信號; 至少一升壓電容網路, 端點分別與該等節點 〇、升1電谷、,罔路之一 路之另一端 ”, 電連接,每一該等升壓電容網 號具有至少::電:::脈信號電連接,其中該時脈信 脈信號位準之準堅位準,藉由該時 ph ^ Γ 使δ亥輸入电壓信號於每一升壓 I白开问忒该電壓位準值;以及 至〆 逆電流截止電路,各一兮楚、ν' + ★必,a 分別寺1^電流截止電路 止電路控制對應之-該等二極體等效網路之致: (enable)與失能(disable),其中該等逆電流截止電路 具有至少兩導通路徑。 藉由單純示範最適於實施本發明的模式中之一,熟 習此項技術人士將可自以下說明瞭解本發明的特點及優 勢中之一或部分或全部,因此,附圖及說明書基本上可 視為範例性而非限制性。 【實施方式】 弟3圖所示為本發明貫施例之一中所揭露之一種 四階升壓電荷增壓電路(4-order Charge_pump Circuit)3 00之示意圖,該四階升壓電荷增壓電路3〇〇包 含一第一逆電流截止電路3 1 0a、一第二逆電流截止電 路310b、一第三逆電流截止電路310c、一第四逆電流 截止電路31 0d、一第一等效二極體320a、一第二等效 9 200810331 二極體32〇b、一第三等效二極體32〇c、一第四等致一 極體32〇d、一第一升壓電容33 0a、一第二升壓電容 330b、一第三升壓電容330c以及一第四升壓電容 3 3 0d,其中每一該等逆電流截止電路31〇包含一開^ 對’本實施例中,該等逆電流截止電路3丨〇係分別由— 增強型N通道金氧半導體電晶體Vout = Vin+N*(V(p .Vt)-Vt ........ ( 1-1 ). 曰 From the relationship of 1-1, it can be found that it is limited by the MOS transistor structure. In the presence of the threshold voltage vt (thresh〇][dv〇hage) effect, the boosting efficiency of the charge boosting circuit i 00 is thus reduced, resulting in inefficient system efficiency, especially in the case of low supply voltage conditions, the critical voltage effect is The impact of system performance will be very obvious, making the charge boost circuit 100 not suitable for low voltage operation, and the poor efficiency of boosting in general circuit applications necessitates more power consumption to compensate. A large number of shortcomings. 々 For this reason, many improvements to the charge booster circuit have been proposed. See Figure 2, an improved charge booster circuit disclosed in U.S. Patent No. 6,670,884 B2, The structure of the improved charge boosting circuit 200 is substantially the same as that of the charge boosting circuit 1 , except that the diode in the improved charge boosting circuit 200 is connected to the MOS semiconductor crystal system to the vacant metal oxide semiconductor. The crystal (Depleti〇n-type MQS Transistor) was implemented. The advantage is as follows: Depleti〇n-type N.channel M〇s Transist〇r is exemplified by 200810331, whose threshold voltage value is a negative value, and its characteristics make the depleted N-channel MOS semiconductor The channel of the crystal is continuously maintained in conduction state unless the voltage between the gate source stages (Vgs) is applied with a voltage lower than the threshold voltage. The improved charge boosting circuit is utilized by the characteristics of the above-described depleted gold-oxygen half-body transistor. 200 can avoid the influence of the system performance degradation caused by the threshold voltage Vt effect, so that the output voltage of the improved charge boosting circuit 2〇〇 is higher than that of the charge boosting circuit 100 of the same order. The characteristics of the above-mentioned depleted MOS transistor also cause the improved charge boosting circuit 200 to switch between the operating clocks, and when the voltage of the node a has been boosted, the depleted N-channel MOS transistors Still unable to turn off, thus generating a reverse leakage current Iq along a path 21 ,, the reverse leakage current Iq and the charge boosting circuit 1 采用 using a J-type N-channel transistor Enhancement_type N_channel Transistor) The threshold voltage vt causes the same effect of poor boost efficiency, which will cause the system performance to be low. In particular, the reverse leakage current Iq is in the improved charge boost circuit 2〇〇 Overflow is more likely to damage the system and reduce reliability. In order to prevent the reliability from declining, the system often needs to increase the protection circuit. Such measures increase the cost of the system, which is more detrimental to the application and sales of the product. Reducing the reverse leakage current Iq for J, the improved charge boosting circuit=〇 discloses the use of changing the aspect ratio (W/L) parameter of the vacant MOS transistors to reduce the reverse leakage current Iq The method, but the 0 method is only reduced, but the reverse leakage current Iq cannot be completely avoided. The excessively grown transistor aspect ratio is difficult to increase the process. ^^ This can cause electrical interference that cannot be detected during design. In summary, such a method cannot first completely reverse the reverse reverse current, and the increase in the difficulty of the process may increase the production cost. Secondly, the electrical interference that may occur also causes the reliability of the circuit to decrease. For this reason, a charge booster circuit that maintains circuit reliability while completely turning off the reverse reverse current is very desirable. SUMMARY OF THE INVENTION An object of the present invention is to provide a boost charge boost circuit that utilizes a depletion transistor (Depletion_type M〇s core (10) deuteration. Composition equivalent series diodes' The boost charge boosting circuit has no threshold voltage loss to increase the boosting efficiency. Another object of the present invention is to provide a boost charge boosting circuit: the boosting charge boosting circuit includes at least one reverse current blocking circuit, The reverse current cutoff circuit turns off the reverse leakage current to increase the boosting efficiency. Another object of the present invention is to provide a boost charge boosting circuit including at least an "inverse current cutoff circuit, the boosted charge The booster circuit does not need to use a special process, and the other purpose is to save a boost charge. Another purpose is to provide a boost charge booster circuit. The boost charge boost circuit includes at least - reverse current wear voltage, and the reverse current cutoff The circuit cuts off the reverse leakage current to reduce the electrical property and increase the system reliability. Another object of the present invention is to provide a boosted charge 擗厣 Ray Road, which The piezoelectric charge boosting circuit comprises at least a voltage stabilizing circuit, and the output voltage is determined. Fe, :: For the above purpose, the present invention provides a boosted charge boosting electrical complex diode equivalent network, wherein the pole The body-equivalent network system 8 200810331 is a series-connected electric nucleus node, each of which has a diode-equivalent network between the equivalent network of the two poles. At the input end, the wheel enters the pile and you receive an input voltage signal for one of the boost charge boosting circuits; at least one boost capacitor network, and the end points respectively rise with the nodes, and rise to 1 valley, The other end of one of the roads is electrically connected. Each of the boost capacitor network numbers has at least::::: pulse signal electrical connection, wherein the clock signal signal level is accurate and accurate. From this time, ph ^ Γ causes the δ hai input voltage signal to open the voltage level value for each boost I; and to the reverse current cut-off circuit, each one, ν' + ★ must, a separate temple 1^ Current cut-off circuit is controlled by the circuit control - the equivalent network of these diodes: And enable, wherein the reverse current cutoff circuit has at least two conduction paths. By simply demonstrating one of the modes most suitable for implementing the present invention, those skilled in the art will be able to understand this from the following description. The drawings and the description are to be regarded as illustrative and not restrictive. FIG. 3 is a diagram showing one of the embodiments of the present invention. A schematic diagram of a fourth-order charge-pump circuit 3 00, the fourth-order boost charge boost circuit 3 〇〇 includes a first reverse current cut-off circuit 3 1 0a, a second inverse The current cut-off circuit 310b, a third reverse current cut-off circuit 310c, a fourth reverse current cut-off circuit 31 0d, a first equivalent diode 320a, a second equivalent 9 200810331 diode 32〇b, a first a three-equivalent diode 32〇c, a fourth-equivalent body 32〇d, a first boosting capacitor 33 0a, a second boosting capacitor 330b, a third boosting capacitor 330c, and a fourth Boost capacitor 3 3 0d, each of these reverse current cuts 31〇 circuit comprises a pair of open ^ 'the present embodiment, the reverse current blocking circuit 3 such Shu square lines were made - the enhancement N-channel metal oxide semiconductor transistor

Transistor)以及一增強型p通道金氧半導體電晶體 (Enhancement-type P-channd Transistor)組成,但亦不以此 ^ 限事貝上,本發明中,該等開關對可由導通特性相^子 之任何開關組成,除了半導體元件形成之電子開關外, 諸如電磁開關等,應視為已於本發明中所揭露。 ^ ΤΓ心电ML戰儿电吟I增強 型N通道金氧半導體電晶體與增強型p通道金氧半 體電晶體間,係利用該等電晶體各自之源極(⑽咖 gate )與另一電晶體之源極,或各自之汲極(心也$ 與另-電晶體之汲極進行電性連接。此外,级成每一组 逆電流截止電路31〇之該等電晶體之間極可聯接至^ ;本實施例中’每一該等等效二極體320 ^ 工 1 Ν 通道 M0S 電晶體(DePletion_type 〇S =ansistor)舆組成該截止電路3i〇之該增強型p 電晶體所組成’該增強型P通道金氧半 導體電晶體是否導:二制二增強型p通道金氧半 P通道金氧半導體電曰二2 310中之該增強型Transistor) and an enhanced p-channel CMOS transistor (Enhancement-type P-channd Transistor), but this is not limited to the case, in the present invention, the switch pairs can be turned on by the characteristics Any switch composition, other than an electronic switch formed by a semiconductor component, such as an electromagnetic switch, etc., should be considered as disclosed in the present invention. ^ ΤΓ ΤΓ ML ML ML 增强 增强 增强 增强 增强 增强 增强 增强 增强 增强 增强 增强 增强 增强 增强 增强 增强 增强 增强 增强 增强 增强 增强 增强 增强 增强 增强 增强 增强 增强 增强 增强 增强 增强 增强 增强 增强 增强 增强 增强 增强 增强 增强 增强 增强 增强The source of the transistor, or the respective drain (the core is also electrically connected to the drain of the other-transistor). In addition, each of the sets of reverse current cutoff circuits 31 is electrically connected between the transistors. Connected to ^; in this embodiment, 'each of the equivalent diodes 320 ^ 1 Ν channel M0S transistor (DePletion_type 〇 S = ansistor) 舆 constitutes the cut-off circuit 3i 〇 the enhanced p-crystal 'Whether the enhanced P-channel MOS transistor is conductive: the enhanced version of the two-system two-enhanced p-channel MOS half-channel MOS transistor 2 2 2 310

iH乳半導體電晶體截止時,該等空乏型N 〇之本貝施例猎由組成該等逆電 10 200810331When the iH milk semiconductor transistor is turned off, the depletion type N 〇 本 施 施 猎 猎 猎 组成 10 10 10 10 10 10 10 10 10 10 10 10 10

之該等開關對,控制對應之該等空乏型N I〜电日日租以及該等逆電流截止電路 通道金氧半導體電晶體所形之強型p ienaM、t 成之寺效二極體之致能 等空乏mf(disabie)。事實上,本實施例中,該 1電M體之閘極端以及汲極端間之迴路僅需等 件即可實施,除利用—p通道電晶體外, 曰強i Ν通這電晶體亦可實現前述結構。 此外,本實施例中,該等逆電流截止電路31〇之一 知舁一接地端(GND)電連接,以使 止電路盥每一兮笙笙崎-托础兩 邊寺逆電肌截 ,,0i r :' ^忒寻寺效—極體電路組成之迴路得以依 太二 的控制分別導通以及關閉。值得注意的是, 地端電麼得以調整至任何適合的數值 以零電壓為限。 下 該四階㈣電荷增壓電4 3⑽之連接關係敛述如 該第一等效二極體32〇a與該第二等效二極體32肋 =此串聯(eGnneeted in sedal),其連接端點為一第 一即』Nodel,該第二等效二極體32〇b與該第三等效 一極體32〇c係彼此串聯,其連接端點為一第二節點 〇de2,該第三等效二極體32〇c與該第四等效二極體 =〇d係彼此串聯,其連接端點為一第三節點N〇de3,該 弟=等效二極體320d之源極端點為第四階之一電壓輸 出郎點Vout。 μ、,每一該等逆電流截止電路中,組成該等開關對之該 等牦強型金氧半導體電晶體之閘極彼此電連接,該等連 接= ,、、、占刀別形成一第4節點N〇de4、一第5節點Node5、 一第6節點Node6以及一第7節點N〇de7。 11 200810331 組成該等逆電流截止電路3 1 0之該兩增強型金氧 半導體電晶體間之兩没極或兩源極彼此電連接,該等連 接立而點分別形成一第8節點Node8、一第9節點Node9、 一第10節點NodelO以及一第11節點Nodell。 該第一升壓電容33 0a與Nodel電連接,該第二升 壓電容330b與Node2電連接,該第三升壓電容33〇c 與Node3電連接,該第四升壓電容33〇d與該第四階電 壓輸出Vout點連接。本實施例中,該等升壓電容33〇 係利用源極與汲極彼此電連接之空乏型N通道金氧半 導體電晶體實現,但亦不以此為限。事實上,任何足以 等效:具有適合電容值之電子元件或電路組合,均可視 為該等升壓電容之變化實施。其中該第一升壓電容3 之源極與汲極間連接為一第12節點Nodel2,同理類 推,该第二升壓電容33〇b之源極與汲極間之連 -第η節點N〇del3,該第三升厂堅電容330c之源極: =極間之連接點與N〇del2為同一節點。該第四升壓電 谷330d之源極與汲極間之連接點與N〇dei3為同一節 點,而Nodel2與N〇del3分別連接至一第一時脈信號 源P 1以及一第二時脈信號源p 2 , p 1與p 2為反相 脈信號源’該等信號源之高低位準係交互出現,本, 例中,表示低位準之電壓值為〇,高位準為^亦 不以此為限,其尚低位準變化可依系統需要調節。誃 升壓電容之閘極分別與該第一節點Nodel、該第二節點 第二即點N〇de3以及第四階電壓輸出節點v〇ut 下 該四階升壓電荷增麼電4 3GG之工作原理敎述如 12 200810331 弟4圖所示,係為本發明所揭露之該 :於二路3〇0於一第—輪入狀態時之等效電路 兮升芦;Γ/—輸人狀“,—輸人電壓信號Vin輸入 ^ 何增壓電路挪’此時"為G(亦可為接地位 準或Low準位)或低電壓準位而少2為Vp,則逆電流 截乂電路因受其控制而分別將該等逆電流戴止電路中L 之該等開關對依其導通特性,分別導通(比⑺〇n )以及 關斷(turn off),因而形成不同的導通路徑,使得嗲等等 :二級體32〇a以及320c間之空乏型Nit道電晶:間極 Μ源極間之回路導通以形成二極體連接 (D1〇de-connected),該等等效二級體32补以及32〇d間 之空乏型N通道電晶體閘極與源極間之回路斷開,故 320b與320d的空乏型N通道電晶體在此時並非二極體 連接,亦即該等等效二極體於該第一輸入狀態時處於失 能狀態。 此時,由於320a中之空乏型N通道電晶體導通, 因此輸入端Vin將產生一充電電流j工對電容3 3 充 電,直到Nodel之電壓Vnodel=Vin。 請見第5圖所示,係為本發明所揭露之該升壓電荷 增壓電路300於一第二輸入狀態時之等效電路5〇〇。於 該第二輸入狀態時,一輸入電壓信號Vin輸入該升壓電 荷增壓電路300,此時% ;[為v $而p 2為〇(接地或L〇w 準位),則逆電流截止電路因受其控制而使該等逆電流 截止電路中之該等開關對依其導通特性,分別被導通 (turn on )以及斷開(turn 〇ff),因而形成不同的導通路 徑’該等等效二級體320b以及320d間之空乏型N通道 電晶體閘極與源極間之回路導通成形成二極體連接,該 專專效一級體320a以及320c間之空乏型N通道電晶體 13 200810331 閘極與源極間之回路關斷,故32〇a與32〇c的空乏型n 通道電晶體在此時並非二極體連接,亦即該等等效二極 體於該第一輸入狀態時處於失能狀態。以此,於N〇de工2 處輸入該第一時脈信號源φ卜第一升壓電容33〇a電壓 被提升一 vp的準位,而nodel之電壓Vn〇dei也隨之 提升至Vin+Vp。該第二等效二極體32〇b因為二極體 連接而導通,透過回路產生之一電流12對電容33〇b充 電,Vnode2也隨之充電提升至vin+v 是’於習知技術中,此時0Vodel大於Vin,:產^ ^向電流Iq,而於該升壓電荷增壓電路3〇〇中,由於此 % 3 20a中之空乏型N通道電晶體之閘極因為3丨的開 關對而導通到接地,而若此時有反向電流產生3施中 =空乏型N通道電晶體的源極依照逆電流iq方向將是 郎點Viη ’以此,士卜α α 此岭320a中之空乏型Ν通道電晶體 的問源極電壓Vgsl=_Vin,故若t此時該空乏型n通道 電晶體的閘,極電壓相較於空乏㉟N通道電晶體的臨 界電壓Vt還要/J、,也就是說Vgsl<Vt,則將不會產生 反向電流,該升壓電荷增壓電路300以此達成增加增壓 效率以及降低成本的目的。 請^第6圖所示,隨後該等時脈信號回復至該第一 輸入狀態’此時該帛二時脈信號以此,Ν_2 將如上述相同原理被提升一個V φ準位,使得The switch pairs control the corresponding depletion type NI~Electric daily rent and the strong type of p ienaM, t into the temple effect diode of the reverse current cutoff circuit channel MOS transistor Can wait for the lack of mf (disabie). In fact, in this embodiment, the circuit between the gate terminal and the gate terminal of the one-electron M body can be implemented only by the same piece, and in addition to using the p-channel transistor, the transistor can be realized by reluctantly i-passing the transistor. The foregoing structure. In addition, in this embodiment, one of the reverse current cutoff circuits 31 is electrically connected to the ground (GND), so that the circuit is reversed from each of the two sides of the Sakizaki-Tokyo, 0i r : ' ^ 忒 寺 效 — — — — — — — — — — — 极 极 极 极 极 极 极 回路 回路 回路 回路 回路It is worth noting that the ground power can be adjusted to any suitable value to the zero voltage. The connection relationship of the fourth-order (four) charge booster 4 3 (10) is as follows: the first equivalent diode 32 〇 a and the second equivalent diode 32 rib = this is connected in series (eGnneeted in sedal), which is connected The endpoint is a first, ie, Nodel, the second equivalent diode 32〇b and the third equivalent pole 32〇c are connected in series with each other, and the connection end point is a second node 〇de2, The third equivalent diode 32〇c and the fourth equivalent diode=〇d are connected in series with each other, and the connection end point is a third node N〇de3, which is the source of the equivalent diode 320d The extreme point is the voltage output of the fourth order, the point Vout. μ, in each of the reverse current-cutting circuits, the gates of the bare-type MOS transistors constituting the pair of switches are electrically connected to each other, and the connections = , , , and 4 nodes N〇de4, a 5th node Node5, a 6th node Node6, and a 7th node N〇de7. 11 200810331 The two non-polar or two sources of the two enhanced MOS transistors constituting the reverse current cut-off circuit 310 are electrically connected to each other, and the points are respectively connected to form an eighth node Node8, one The 9th node Node9, a 10th node Node1O, and an 11th node Node11. The first boosting capacitor 33 0a is electrically connected to Node1, the second boosting capacitor 330b is electrically connected to Node2, and the third boosting capacitor 33〇c is electrically connected to Node3, and the fourth boosting capacitor 33〇d and the The fourth-order voltage output Vout is connected. In this embodiment, the boost capacitors 33 are implemented by a depleted N-channel MOS transistor whose source and drain are electrically connected to each other, but are not limited thereto. In fact, anything that is equivalent: an electronic component or combination of circuits with a suitable capacitance value can be considered as a variation of these boost capacitors. The source and the drain of the first boosting capacitor 3 are connected to a 12th node Nodel2, and so on, the source and the drain of the second boosting capacitor 33〇b are connected to the nth node N. 〇del3, the source of the third liter factory capacitor 330c: = The connection point between the poles is the same node as N〇del2. The connection point between the source and the drain of the fourth boosting electric valley 330d is the same node as N〇dei3, and Nodel2 and N〇del3 are respectively connected to a first clock signal source P1 and a second clock. The signal source p 2 , p 1 and p 2 are the inverted pulse signal sources. The high and low levels of the signal sources appear alternately. In this example, the low level voltage value is 〇, and the high level is ^. This is limited, and its low level change can be adjusted according to system needs. The gate of the boost capacitor and the first node Node1, the second node second, the point N〇de3, and the fourth-order voltage output node v〇ut, the fourth-order boost charge increase power 4 3GG work The principle description is as shown in Fig. 12 200810331, which is the invention disclosed in the following figure: the equivalent circuit of the second road 3〇0 in a first-wheel-in state, the ascending reed; Γ / - input human form" , - input voltage signal Vin input ^ What is the boost circuit shift 'this time' is G (can also be ground level or Low level) or low voltage level and 2 is Vp, then the reverse current paraplegic circuit Because of the control, the switch pairs of L in the reverse current blocking circuit are respectively turned on (by (7) 〇 n ) and turned off according to their conduction characteristics, thereby forming different conduction paths, so that different conduction paths are formed.嗲 and so on: the depleted Nit channel crystal between the 32u and 32c diodes: the loop between the source and the source is connected to form a diode connection (D1〇de-connected), the equivalent level The cavity between the body 32 and the 32-d-d-type N-channel transistor is disconnected from the source, so the depleted N-channel electron crystals of 320b and 320d At this time, it is not a diode connection, that is, the equivalent diodes are in a disabled state in the first input state. At this time, since the depleted N-channel transistor in 320a is turned on, the input terminal Vin will A charging current is generated to charge the capacitor 3 3 until the voltage of Nodel Vnodel=Vin. As shown in FIG. 5, the boosting charge boosting circuit 300 disclosed in the present invention is in a second input state. The equivalent circuit is 5. In the second input state, an input voltage signal Vin is input to the boost charge boost circuit 300, at this time %; [is v $ and p 2 is 〇 (ground or L〇w The level of the reverse current cut-off circuit is controlled by the switch, and the switch pairs in the reverse current cut-off circuit are turned on and off (turn 〇 ff) according to their turn-on characteristics, thereby forming Different conduction paths' loops between the gates of the depleted N-channel transistors and the source between the equivalent diodes 320b and 320d are connected to form a diode connection between the special-purpose primary bodies 320a and 320c. Depleted N-channel transistor 13 200810331 Back between gate and source Turned off, so the 32 n and 32 〇 c of the depleted n-channel transistors are not connected to the diode at this time, that is, the equivalent diodes are disabled in the first input state. Input the first clock signal source φ at the N〇de2, and the voltage of the first boost capacitor 33〇a is raised by a level of vp, and the voltage Vn〇dei of the nodel is also raised to Vin+Vp. The second equivalent diode 32〇b is turned on because of the diode connection, and a current 12 is generated through the loop to charge the capacitor 33〇b, and the Vnode2 is also charged to vin+v. In this case, 0Vodel is greater than Vin, and the current is supplied to the current Iq, and in the boosted charge boosting circuit 3〇〇, since the gate of the depleted N-channel transistor in the % 3 20a is 3 丨The switch is turned on to ground, and if there is reverse current generated at this time, the source of the depleted N-channel transistor will be the point of the reverse current iq, which is the point of the point Viη ', thus, the αα α ridge 320a In the middle of the space-deficient Ν channel transistor, the source voltage Vgsl=_Vin, so if t is the gate of the depleted n-channel transistor, the pole voltage is compared with The threshold voltage Vt of the depleted 35N channel transistor is still /J, that is, Vgsl < Vt, then no reverse current will be generated, and the boosting charge boosting circuit 300 achieves an increase in boosting efficiency and a reduction in cost. purpose. Please, as shown in Fig. 6, then the clock signals return to the first input state'. At this time, the second clock signal is used, and Ν_2 will be raised by a Vφ level according to the same principle as described above, so that

In〇de2 = Vin + 2VP。該第三等效二極體網路320c中之 ,乏^ N通道電晶體也因為3 1 0c的開關分別被導通 j turnon)/及斷開(tum〇ff),因而形成不同的導通路 钇而开y成一極體連接而導通,透過該回路形成一充電電 流13對電容330c充電至%〇以3=^+2^。此外,In〇de2 = Vin + 2VP. In the third equivalent diode network 320c, the N-channel transistors are also turned on and turned off (tum〇ff) because the switches of the 3 1 0c are respectively turned on, thereby forming different conduction paths. The open y is connected to the one body and turned on, and a charging current 13 is formed through the loop to charge the capacitor 330c to % 〇 to 3 = ^ + 2^. In addition,

Vnodel之電墨回庙不V ^ 土 U设至Vln,使得Vgs2=-Vin,此時該空 14 200810331 乏型N通道電晶體的閘源極電壓相較於空乏型N通道 電晶體的臨界電壓vt還要小,也就是說Vgs2<Vt,則 將不會產生反向電流’則該第二等效二極體320b關閉 (turnoff),使Node2以及Node3之電壓得以維持。 請見第7圖所示’隨後該等時脈信號回復至該第2 輸入狀態,同上所述,此時該第一時脈信號p 1=V p。 以此,於N 〇 d e 1 2處輸入該第一時脈信號p 1之該第3 升壓電容330a電壓被提升一個Vp之準位,而n〇de3 之電壓Vnode3也隨之提升至Vin + 3 V φ。該第四等效二 極體320d中之空乏型Ν通道電晶體亦在此時為實際二 極體連接而導通,透過回路形成之一充電電流14對電 容330d充電,Vout也隨之被該電流14充電,直到提升 至 Vin + 3V p。 同理,當該等時脈信號再次回復到第二時脈信號 時,電容330d又被提昇一個γφ之電壓值使得 Vout=Vin+4V ρ而達到增壓輸出之電路功能。 值得注意的是,該等逆電流截止電路可以利用任何 其導通特性相對之電子元件或電路組合而成,其作用在 於利用輸入時脈信號的變化改變導通路徑,以避免前述 之逆向漏電流現象的發生。因此,習知該項技術之人應 可瞭解,本貫施例中利用一增強型N通道金氧半導體電 晶體與一增強型N通道金氧半導體電晶體實現該等逆 包流截止電路的方法,為實施逆電流截止電路所例舉的 方法之一,而非本發明的限制。 ^發明藉由電性相對之開關形成逆電流截止電 路,藉以防止升壓所產生之逆電流造成能源消耗以及影 響升壓效率,並且增加系統之可靠度。 15 200810331 電 該㈣升壓電荷Vnodel's electro-ink back to temple is not V ^ soil U is set to Vln, so that Vgs2 = -Vin, at this time the empty 14 200810331 the source voltage of the spent N-channel transistor is compared with the threshold voltage of the depleted N-channel transistor Vt is still small, that is, Vgs2 < Vt, then no reverse current will be generated'. Then the second equivalent diode 320b is turned off, so that the voltages of Node2 and Node3 are maintained. Please refer to Fig. 7, and then the clock signals return to the second input state, as described above, at which time the first clock signal p 1 = V p . Therefore, the voltage of the third boosting capacitor 330a that inputs the first clock signal p1 at N 〇de 1 2 is raised by a level of Vp, and the voltage Vnode3 of n〇de3 is also raised to Vin + 3 V φ. The depleted germanium channel transistor in the fourth equivalent diode 320d is also turned on for the actual diode connection at this time, and a charging current 14 is formed through the loop to charge the capacitor 330d, and Vout is also used by the current. 14 Charge until it is raised to Vin + 3V p. Similarly, when the clock signals return to the second clock signal again, the capacitor 330d is boosted by a voltage value of γφ such that Vout=Vin+4V ρ to achieve the circuit function of the boost output. It should be noted that the reverse current cut-off circuit can be combined with any electronic component or circuit whose on-characteristic characteristics are opposite to each other, and its function is to change the conduction path by using the change of the input clock signal to avoid the aforementioned reverse leakage current phenomenon. occur. Therefore, those skilled in the art should be able to understand that the method for realizing the reverse packet cut-off circuit by using an enhanced N-channel MOS transistor and an enhanced N-channel MOS transistor in the present embodiment One of the methods exemplified for implementing the reverse current cutoff circuit, and not the limitation of the present invention. The invention forms a reverse current cut-off circuit by electrically opposing the switch, thereby preventing the reverse current generated by the boosting from causing energy consumption and affecting the boosting efficiency, and increasing the reliability of the system. 15 200810331 Electricity (4) boost charge

VoutVout

Vin + N*V φ ........ ( 3-1 ) 該^㈣電荷„電路彻之串接級數可 调整’直到電荷辦舉掏^ r . 要 & 日应(Pumping Voltage Gain)趨 二巳π止。換言之,直到電荷增壓增益趨於飽 她電路之級數可以依需要調整,該升“ 電路300揭露之4級升壓電路僅為實施方式之 ’不可視為本發明之限制。 德备tI明所揭&之該升壓電荷増壓電路於升壓時可 ==荷增壓電路中臨界電厂堅以及逆向漏電;; 不良影響’並無須對元件尺寸進行任何 ‘導通路"殊°又计’利用系統中既有的時脈信號即可操 以避免逆向漏電流。以此,本發明所揭露之 本以及高可靠性的優點,更適合應用於諸:ΐ 土置等電源有限,電壓較低而需要 低電壓系統中。 山值得一提的是,該升壓電荷增壓電路3〇"透過輸 穩壓電路(RegulatGO電連接,透過該穩壓電 定的輸人電壓值,以於輸人電源衰減或變動 守仍犯提供一穩定的輸出電壓。 例二’前述之各種電路以及元件僅為示意,除實施 所“之組合外,該等電路以及元件之等效電路以 16 200810331 =均應視為已為本發 各種電路以及元件之私口 牛例;5兄,刖述之 數元件所構成之等效網:::為:發明之限制,由複 露。另外,孰應視為已為本發明所揭 電路拓樸,二 體間組成元件之配合n止^以及該等等效二極 能,但於相同的電 ^月存在终多替代實施的可 所揭露。舉例而言,實施空 (jfeT),此/,體m可利用接面場效電晶體 (GND)之升㈣荷;^ 於相對於接地 壓輸入Vin負辦壓W 、、輸出電壓為將一負電 體替代實施。J至更負㈣亦可用空乏型p通道電晶 之本::ΐ=:二士 9應瞭解上述圖式及說明中所示 月豆貝知例/、疋範例性且非限制。 ^ ^ ί t m # ^ ^ ^ 例性具體,Li :該精確形式或已揭示之範 制性。顯二二1 *此,先珂說明應視為示範性而非限 把明二 正及變化對於熟習此項技術人士將是 =顯的°具體實施例之選擇及描述是為了更佳解釋= ㈣Γ原理及其實際應用之最佳模式,從而允許孰習此 、商人士理解用於各種具體實施例之本發明,且、且有 ::於特定使用或所涵蓋實作之各種修 : ;吏其範傳由在此所附之申請專利範圍及其等同月 泛之2ΪΓΠΓ否則所有請求項均包含其最廣 Pm Γ 可由熟f此項技術者對於具 ί::二ΐ仃改變,而不脫離由以下申請專利範圍所定 I月的砣疇。再者,本揭露書中沒有任何元件及 17 200810331 ^件係意以用於公眾,不管該元件或組件是否在以下 請專利範圍中明確地提及。此外,本揭露書的摘 =用以順應摘要規則之要求,其允許搜尋者迅速地確定 從此揭露書發布的任何專利之技術揭露主題。應要瞭2 到其非用於解釋或限制申請專利範圍的範疇或意涵 【圖式簡單說明】 第1圖為一習知之雙時相(dual phase )電荷增题雷 1⑽示意圖。 土 第2圖為一種改良式電荷增壓電路200。 第3圖為本發明實施例之一中所揭露之一種 增壓電路30。之示意圖。 土電何 第4圖為本發明實施例之一中所揭露之一種升壓電荷 增壓電路300之於一第一輸入狀態時之等效電路4〇〇示 意圖。 第5圖為本發明實施例之一中所揭露之一種升壓電荷 增壓電路300之於一第二輸入狀態時之等效電路500示 意圖。 第6圖為本發明實施例之一中所揭露之一種升壓電荷 增壓電路300之時脈信號回復至該第一輸入狀態時之 等效電路示意圖。 第7圖為本發明實施例之一中所揭露之一種升壓電荷 增壓電路300之時脈信號回復至該第二輸入狀態時之 等效電路示意圖。 【主要元件符號說明】 18 200810331 p 1時脈信號 p 2時脈信號 100雙時向電荷增壓電路 11 0充電路徑 120第一節點 1 3 0第二節點 140第二充電路徑 C1電容 C2電容 C3電容 C4電容 Cout電容 200改良式電荷增壓電路 2 1 0路徑 Iq反向漏電流 Vt臨界電壓 3 00四階升壓電荷增壓電路 310a第一逆電流截止電路 310b第二逆電流截止電路 310c第三逆電流截止電路 3 10d第四逆電流截止電路 320a第一等效二極體 320b第二等效二極體 320c第三等效二極體 320d第四等效二極體 330a第一升壓電容 330b第二升壓電容 19 200810331 330c第三升壓電容 330d第四升壓電容Vin + N*V φ ........ ( 3-1 ) The ^ (four) charge „the circuit can be adjusted in series until the charge 掏^ r. want & day should (Pumping Voltage Gain) tends to 巳π。 In other words, until the charge boosting gain tends to saturate the number of stages of her circuit can be adjusted as needed, the rise of the "four-stage boost circuit disclosed by circuit 300 is only an embodiment" can not be regarded as the present invention The limit. Debu's tI Ming revealed that the boost charge voltage circuit can be used to boost the critical power plant and reverse leakage in the booster circuit; the adverse effect does not require any guidance on the component size. The path " is also considered to use the existing clock signal in the system to avoid reverse leakage current. Therefore, the advantages disclosed in the present invention and the advantages of high reliability are more suitable for applications in which the power supply is limited, the voltage is low, and the low voltage system is required. It is worth mentioning that the boosting charge boosting circuit 3〇" is transmitted through the voltage regulator circuit (RegulatGO electrical connection, through the voltage input voltage value of the voltage regulator, in order to reduce or change the input power supply Provided to provide a stable output voltage. Example 2 'The various circuits and components mentioned above are only schematic, except for the combination of the implementation, the circuit and the equivalent circuit of the components are 16 200810331 = both should be regarded as the same The private network of various circuits and components; 5 brothers, the equivalent network of the components described in the following::: is the limitation of the invention, by the re-exposed. In addition, 孰 should be regarded as the circuit disclosed in the present invention. Topology, the combination of the components between the two bodies, and the equivalent two-pole energy, but there are many alternative implementations in the same electricity month. For example, the implementation of empty (jfeT), this /, body m can use the junction field effect transistor (GND) rise (four) charge; ^ relative to the ground pressure input Vin negative voltage W, the output voltage is to replace a negative body. J to more negative (four) The available space of p-type p-channel electron crystal::ΐ=:Two people 9 should understand the above pattern And the description of the Bean Beans in the description /, 疋 exemplary and non-limiting. ^ ^ ί tm # ^ ^ ^ Instance-specific, Li: the exact form or the revealed system. Show two two 1 * This First, the description should be regarded as exemplary rather than limiting. The change will be obvious to those skilled in the art. The choice and description of the specific embodiment is for better explanation. (4) Principle and practical application The best mode, thus allowing the business person to understand the invention for various specific embodiments, and with:: various modifications to the specific use or covered practice: Included in the scope of the patent application and its equivalent month 2 otherwise all claims contain their most extensive Pm Γ can be changed by the skilled person, without departing from the scope of the following patent application In addition, there are no components in this disclosure and it is intended to be used by the public, regardless of whether the component or component is explicitly mentioned in the scope of the following patent. In addition, the disclosure of this document Excerpt = to comply with the requirements of the summary rules, The searcher quickly determines the subject of the technology disclosure of any patents issued from this disclosure. It should be 2 to the scope or meaning of the patent application that is not used to explain or limit the scope of the patent application. A schematic diagram of a dual phase charge increase 1 (10) is shown. Fig. 2 is an improved charge boost circuit 200. Fig. 3 is a boost circuit 30 disclosed in one embodiment of the present invention. FIG. 5 is a schematic diagram of an equivalent circuit 4 升压 of a boost charge booster circuit 300 according to one embodiment of the present invention in a first input state. FIG. A schematic diagram of an equivalent circuit 500 of a boost charge boost circuit 300 in a second input state disclosed in one of the embodiments. FIG. 6 is a schematic diagram showing an equivalent circuit when the clock signal of the boost charge boost circuit 300 is restored to the first input state according to one embodiment of the present invention. FIG. 7 is a schematic diagram showing an equivalent circuit when the clock signal of the boost charge boost circuit 300 is restored to the second input state according to one embodiment of the present invention. [Major component symbol description] 18 200810331 p 1 clock signal p 2 clock signal 100 dual time charge boost circuit 11 0 charging path 120 first node 1 3 0 second node 140 second charging path C1 capacitor C2 capacitor C3 Capacitor C4 Capacitor Cout Capacitor 200 Improved Charge Boost Circuit 2 1 0 Path Iq Reverse Leakage Current Vt Threshold Voltage 3 00 Fourth-Order Boost Charge Boost Circuit 310a First Reverse Current Shutdown Circuit 310b Second Reverse Current Shutdown Circuit 310c Three reverse current cutoff circuit 3 10d fourth reverse current cutoff circuit 320a first equivalent diode 320b second equivalent diode 320c third equivalent diode 320d fourth equivalent diode 330a first boost Capacitor 330b second boosting capacitor 19 200810331 330c third boosting capacitor 330d fourth boosting capacitor

Vin輸入電壓信號Vin input voltage signal

Vout輸出電壓信號 φ 1第一時脈信號源或一時脈信號 ρ 2第二時脈信號源或一時脈信號 400四階升壓電荷增壓電路於第一輸入狀態時之等效電 路 500四階升壓電荷增壓電路於第二輸入狀態時之等效電 路 20Vout output voltage signal φ 1 first clock signal source or a clock signal ρ 2 second clock signal source or a clock signal 400 fourth-order boost charge boost circuit in the first input state of the equivalent circuit 500 fourth order Equivalent circuit 20 for boosting charge boost circuit in second input state

Claims (1)

200810331 十、申請專利範圍: 1.一種升壓電荷增壓電路,包含·· 複數二極體等效網且 聯方式# j 1卜/、中°亥寻—極體寺效網路係以奉 i't接’每兩該等二極體等效網路間具有 ..沾母-该寺節點對應_升麼階,其中 :即 二極體等效網路之低壓側為該㈣之= 入:二該輸入端接收一輪入電麼信號;…路之-輸 5二升壓電容網路’每一該等升壓電容網路之-端點 :別與該等節點之一電連接,每一 :: 有至少其巾料脈信號具 號位準之交替蠻化,佶兮认不广千精由"亥日π脈k 向該該電廢位準值;以及 # 白升 ”流截止電路,每一該等逆電流截止電路分 與4寺二極體等效網路電連接,每一該 =制對應之一該等二極體等效網路之致能(二電 〇失月巨(disable)’其中該等逆電流截止電路具有至少兩 導通路經。 2·如請求項丨所述之該升壓電荷增壓電路,其中該等導 L路位依據母一升壓階中時脈信號之切換交替開啟,以 避免該升壓電荷增壓電路出現反向逆電流。 3 .如請求項i所述之該升壓電荷增壓電路,其中每兩相 鄰節點間之該時脈信號相位相反。 4·如請求項1所述之該升壓電荷增壓電路,其中該等逆 電流截止電路包含兩電子開關網路,該等電子開關網路 之導通特性相對,以於該時脈信號切換時分別開啟該等 電子開關網路之一者。 5·如請求項丨所述之該升壓電荷增壓電路,其中每一該 21 200810331 專二極體等效網路係由-空乏型電晶體以及該等逆電流 ?止電路中該兩電子開關網路之一者組成,當該二極體 寺效網路内之該電子開關網路導通時,對應之該空乏 電晶體係為二極體連接。 6如明求項2所述之該升壓電荷增壓電路,其中每一兮 =二極體等效網路係由一空乏型電晶體以及該等逆電= 5止電路中該兩電子開關網路之一者組成,當該二極體 寺效網路内之該電子開關網路導通時’對應之該空乏型 電晶體係為二極體連接。 7. 如請求項1所述之該升壓電荷增壓電路,1中該等逆 =截止電路包含兩電子開關網路’該等電子開關網路 ==特性相對’以㈣時脈信號切換時分別開啟該等 黾子開關網路之一者。 8. 如請求項2所述之該升壓電荷增壓電路,其中該等逆 2截止電路包含兩電子開關網路,該等電子開關網路 性相對’以於該時脈信號切換時分別開啟 電子開關網路之一者。 9 ·如明求項4所述之該升壓電荷增壓電路,1中哼 ::截止電路包含兩電子開關網路,該等電;開關網路 性相對,以於該時脈信號切換時分別開啟 電子開關網路之一者。 項1所述之該升壓電荷增壓電路,其中該等逆 广截止電路包含一增強Μ通道金氧半導體電晶體以 =增強型Ρ通道金氧半導體電晶體,#對應之升壓階 所輸入之該時脈信號為低電壓位準時,該增強型p通首 ί 體電晶體導通且該增強型㈣道金氧半導體ΐ 日日體截止,當對應之升壓階所輸入之該時脈信號 堡位準時’該增_ Ρ通道金氧半導體電晶體截止且二 22 200810331 增強型N通道金氧半導體電晶體導通。 士叫求項2所述之該升壓電荷增壓電路,1 、, 電流戴止電路包含一辦強 ,Y咸寻逆 及-氧半導體電晶體以 3自盂Ρ通迢金氧半導體電晶體,當對應之升壓階 八二:t 4時脈信號為低電壓位準時,該增強型Ρ通道 ::截T體電晶體導通且該增強型N通道金氧半導體電 ,當對應之升壓階所輸人之該時脈信號為高電 該增強型ρ通道金氧半導體電晶體截止且該 曰強i Ν通道金氧半導體電晶體導通。 1 2.如睛求項4所述之該升壓電荷增壓電路,豆 電路包含一增強型Nii道金氧半導體電:曰:體以 9強型P通道金氧半導體電晶體,當對應之升壓階 二f ^之該時脈信號為低電壓位準時,該增強型P通道 至氧半導體電晶體導通且該增強型N通道金 兩 SI ΐ,當對應之升壓階所輸入之該時脈信號為高ΐ ,:,該增強型Ρ通道金氧半導體電晶體截止且該 七強型Ν通道金氧半導體電晶體導通。 1 3 ·如明求項8所述之該升壓電荷增壓電路,其中該增強 L道至氧半導體電日日體之源極端接收該輸入電壓信 號、、’該增強型Ρ通道金氧半導體電晶體以及該增強型^ 通迢金氧半導體電晶體之閘極端分別接收對應之升壓階 所輸入之該時脈信號。 1 4 ·如明求項9所述之该升壓電荷增壓電路,其中該增強 里Ρ通道金氧半導體電晶體之源極端接收該輸入電壓信 號,該增強型Ρ通道金氧半導體電晶體以及該增強型Ν 通道金氧半導體電晶體之閉極端分別接收對應之升壓階 所輸入之該時脈信號。 如請求項10所述之該升壓電荷增壓電路,其中該增 23 200810331 = 電壓 N通道金氧半導體電:曰曰體以及该增強型 階所輸入之該時脈信號。 °而刀別接收對應之升壓 16. —種升壓電荷增壓電路,包含: 複數二極體等效網路,其中該等二極 聯方式雷遠接,— 豆專放、、,罔路係以串 點,每-該等節點對應一升壓階 :^有-即 入端; 塔之域側為㈣壓電荷增壓電路之一輸 -穩壓電路’包含—輸入端以及 該升壓電荷增壓電路之該輸入端電輸出端與 一輸入電m俨缺#丄 而电連接,该輪入端接收 二既定電塵位準,並由該輸出端輸出至 壓電路之該輸入端; /升壓電何增 至少一升壓電容網路,每一該等 分別與-該等節點電連接,每之-端點 一媸》;八w也士 口κ等升^电各網路之另 至:::,一時脈信號電連接’其中該時脈信號具有 至乂 一尚電壓位準以及一低電壓位 位乘夕六祛料稽田5亥日T脈j吕號 又曰,交化,使該輸入電壓信號於每一升壓階升古 该该電壓位準值;以及 复I自开呵 逆;:?止電路,每一該等逆電流截止電路分別 q寺一極體寺效網路電連接,每一該 :控:對應之一該等二極體等效網路之致能=止】 中忒電流截止電路具有至少兩導通路徑。 '、 ^如請求項16所述之該升壓電荷增壓電路,其中 、通路#依據每一升昼):皆中時脈信冑之切換交替開啟, 以避免該升壓電荷增壓電路出現反向逆電流。 24 200810331 18·如請求項16所述之該升壓電荷增壓電路,其中每兩 相鄰節點間之該時脈信號相位相反。 1 9.如請求項1 6所述之該升壓電荷增壓電路,其中該等 逆電流截止電路包含兩電子開關網路,該等電子開關網 路之導通特性相對,以於該時脈信號切換時分別開啟該 等電子開關網路之一者。 2〇·如請求項16所述之該升壓電荷增壓電路,其中每一 f等二極體等效網路係由一空乏型電晶體以及該等逆電 流截止電路中該兩電子開關網路之一者組成,當該二極 體等效網路内之該電子開關網路導通時,對應之該空乏 型電晶體與對應之該等逆電流截止電路之一組成二二體 連接。 ▲〕如請求項17所述之該升壓電荷增壓電路,其中每一 =等二極體等效網路係由一空乏型電晶體以及該等逆電 二止電路中該兩電子開關網路之一者組成,當該二極 ^二、文、、、罔路内之戒電子開關網路導通時,對應之該空乏 體係與對應之該等逆電流截止電路之一組成二極 項16所述之該升壓電荷增壓電路,其中該等 路:,電路包含兩電子開關網路,該等電子開關網 等雷i ^寺性相對,以於該時脈信號切換時分別開啟該 寺電子開關網路之一者。 逆^/7所述之該升壓電荷增壓電路,其中該等 路之導通特:路包含兩電子開關網路,該等電子開關網 等電=性相對,以於該時脈信號切換時分別開啟該 卞电千開關網路之一者。 κ 逆:所述之該升壓電荷增壓電路,其中該等 ;,L电路包含兩電子開關網路,等電子開關網 25 200810331 路之導通特性相對,以於姑士 等電子開關網路之一者;^ 4脈化號切換時分別開啟該 25·如請求項16所、十、 逆電流截止電路包人㈣墨電荷增麼電路,其中該等 以及-增強型p 3二增強型N通道金氧半導體電晶體 道金氧半導體電曰蝴 -監位卓訏,该增強型P通 電晶體截止,=該增強❹通道金氧半導體 電1位準時,升壓階所輸人之該時脈信號為高 該增強型N、甬二二/ P通遏金氧半導體電晶體截止且 26:i/通逼金氧半導體電晶體導通。 逆電^截1\17所述之該升壓電荷增壓電路,其中該等 包含一增強型Nii道金氧半導體電晶體 二:=:通道金氧半導體電晶體,當對應之升壓 、輸入之该日寸脈信號為低電壓位準時,該增強型p 導體電晶體導通且該增強型_道金氧半導體 體截止,當對應之升壓階所輸入之該時脈信號為高 電壓位準時,該增強型P通道金氧半導體電晶體截止且 该增強型N通道金氧半導體電晶體導通。 27·如請求項19所述之該升壓電荷增壓電路,其中該等 逆電流截止電路包含一增強型N通道金氧半導體電晶體 以及一增強型P通道金氧半導體電晶體,當對應之升壓 階所輸入之該時脈信號為低電壓位準時,該增強型P通 道金氧半導體電晶體導通且該增強型N通道金氧半導體 電晶體截止,當對應之升壓階所輸入之該時脈信號為高 電壓位準時,該增強蜇p通道金氧半導體電晶體截止且 該增強型N通道金氧半導體電晶體導通。 2 8 ·如請求項2 3所述之该升壓電荷增壓電路,其中該增 強型P通道金氧半導體電晶體之源極端接收該輸入電壓 26 200810331 信號’該增強型p通道金氧半 N通道金氧半導體 :體%曰曰體以及該增強型 階所輸入之該時端分別接收對應之升壓 29.如請求項24所述之該升壓電荷辦 、, 強型P it道金氧半導體電 : 二°玄增 信號,該增強型原極&接收錢入電壓 M、s言人& 通i虱+導體電晶體以及該妗強都 、、五氣半導體電晶體之閘極g & f+曰 階所輸入之該時脈信號。 而刀別接收對應之升壓 =青求項25所述之該升墨電荷 氧半導體電晶體之源極端接收該輸:電; 型ρ通道金氧半導體電晶體以及該增強型 氧半導體電晶體之間極端分別接收對應之升壓 I5白所輸入之該時脈信號。 項26所述之該升壓電荷增壓電路,其中每一該 :1、包各網路由一空乏型電晶體構成,該等空乏型電晶 體之源極以及汲極間電連接。 >·々二求項29所述之該升壓電荷增壓電路,其中每一 f升壓電容網路由一空乏型電晶體構成,該等空乏型電 晶體之源極以及汲極間電連接。 33·^二求項} 6所述之該升壓電荷增壓電路,其中每一該 升壓,容網路由一接面場效電晶體(JFET)構成,該等 接面場效電晶體之源極以及汲極間電連接。 34.如請求項29所述之該升壓電荷增壓電路,其中每一 ,升壓電容網路由一接面場效電晶體(JFET )構成,該 等接面場效電晶體之源極以及汲極間電連接。 35·如請求項16所述之該升壓電荷增壓電路,其中每一該 等二極體等效網路係由一接面場效電晶體(JFET)組成, 每一該等接面場效電晶體(JFET )與對應之該等逆電流 27 200810331 截止電路之一組成二極體連接。 $·如明求項29所述之該升壓電荷增壓電路,其中每一該 ,一極=等效網路係由一接面場效電晶體()組成, 母一該等接面場效電晶體(JFET)與對應之該等逆電流 截止電路之一組成二極體連接。 37·—種用於電荷增壓電路之升壓單元,包含·· 一等效二極體網路,接收一輸入電壓; -電容網路,魅等效二極體網路錢接,藉由—時脈錢輸出高於該 輸入電壓之一電壓;以及 一開關對,與該等效二極體網路電連接,控制該等效二極 體網路是否形成二極體連接之啟動(enabl (disable) 〇 /、天月匕 38. 如請求項37所述之該升壓單元,其中該開關對藉由該時脈 信號控制該輸入電壓之傳導,該開關對具有至少兩導通 路徑,該時脈信號具有至少兩信號狀況。 、、 39. 如請求項38所述之該升壓單元,其中該等導通路徑依 據該時脈信號之變化交替地開啟。 該等導通路徑之交替 其中該開關對之一端 其中該接地蠕之電壓 40·如請求項38所述之該升壓單元, 變化阻斷反向電流之產生。 41 ·如請求項37所述之該升壓單元, 與一接地端電連接。 42·如請求項4 1所述之該升壓單元, 值不限於〇。 43.如請求項38所述之該升壓單元,其中該時脈信穿呈 高電壓狀態以及/低電壓狀態。 °有 28200810331 X. Patent application scope: 1. A boosting charge boosting circuit, including ················································· Ii't connect 'Every two of these diode equivalent networks have .. dip--the temple node corresponds to _ liter level, where: the low-voltage side of the diode equivalent network is the (four) = In: 2, the input receives a round of incoming signal; ... the road - the 5 5 boost capacitor network 'each of the boost capacitor networks - the end point: not electrically connected to one of the nodes, Each:: There are at least the alternate barbarism of the signal of the material of the towel, and the arbitrarily arbitrarily arbitrarily arbitrarily arbitrarily arbitrarily arbitrarily arbitrarily arbitrarily arbitrarily arbitrarily arbitrarily arbitrarily The cut-off circuit, each of the reverse current cut-off circuits is electrically connected to an equivalent network of the 4 temples, each of which corresponds to one of the equivalent networks of the diodes (second power loss) "月" (disable) wherein the reverse current cutoff circuits have at least two conduction paths. 2. The boost charge boost circuit as recited in claim ,, wherein the The L-channel is alternately turned on according to the switching of the clock signal in the parent-boost step to avoid reverse reverse current of the boosting charge boosting circuit. 3. The boosting charge boosting circuit as claimed in claim i, The clock signal of each of the two adjacent nodes is opposite in phase. 4. The boost charge boost circuit of claim 1, wherein the reverse current cutoff circuit comprises two electronic switch networks, and the electronic switches The continuity characteristic of the network is opposite, so that one of the electronic switch networks is respectively turned on when the clock signal is switched. 5. The boost charge boost circuit as described in the request item, wherein each of the 21 200810331 The special diode equivalent network is composed of a depleted transistor and one of the two electronic switching networks in the reverse current stopping circuit, and the electronic switching network in the diode network When the road is conducting, the corresponding vacant cell system is a diode connection. 6 The boost charge boost circuit of claim 2, wherein each 兮=diode equivalent network is depleted Type of transistor and the two electrons in the reverse circuit One of the switch networks is composed of a diode connection when the electronic switch network in the diode network is turned on. 7. The request is as described in claim 1. The boosting charge boosting circuit, wherein the inverse=cutting circuit comprises two electronic switching networks, and the electronic switching network==characteristics are respectively turned on when the (four) clock signals are switched respectively. 8. The boost charge boost circuit of claim 2, wherein the inverse 2 cutoff circuit comprises two electronic switch networks, the electronic switches being networked relative to the clock signal One of the electronic switch networks is turned on when switching. 9 · The boost charge boost circuit as described in Item 4, 1: The cut-off circuit includes two electronic switch networks, the same; The directionality is opposite, so that one of the electronic switch networks is turned on when the clock signal is switched. The boost charge boosting circuit of item 1, wherein the inverse wide cutoff circuit comprises a boosted germanium channel MOS transistor to be an reinforced germanium channel MOS transistor, #corresponding to a boost step input When the clock signal is at a low voltage level, the enhanced p-channel is turned on and the enhanced (four) MOS transistor is turned off, and the clock signal is input when the corresponding boost step is input. The bunker is on time 'this increase _ Ρ channel MOS transistor cut-off and the second 22 200810331 enhanced N-channel MOS transistor is turned on. The boosting charge boosting circuit described in claim 2, wherein the current wearing circuit comprises a strong, Y-salt and -oxy semiconductor transistor with a self-contained through-metal oxide semiconductor transistor When the corresponding boosting step VIII: t 4 clock signal is a low voltage level, the enhanced Ρ channel:: the T-shaped transistor is turned on and the enhanced N-channel MOS is electrically connected, when the corresponding boost The clock signal of the step input is high. The enhanced p-channel MOS transistor is turned off and the bare i channel MOS transistor is turned on. 1 2. According to the boosting charge boosting circuit described in Item 4, the bean circuit comprises an enhanced Nii channel MOS semiconductor: 曰: body is a 9-type P-channel MOS transistor, when corresponding When the clock signal of the boosting step two f ^ is a low voltage level, the enhanced P-channel to the oxygen semiconductor transistor is turned on and the enhanced N-channel gold is two SI ΐ, when the corresponding boosting step is input The pulse signal is high, :: the enhanced germanium channel MOS transistor is turned off and the seven strong germanium channel MOS transistors are turned on. The boost charge boosting circuit of claim 8, wherein the source of the enhanced L-to-oxygen semiconductor electric solar cell receives the input voltage signal, 'the enhanced germanium channel MOS semiconductor The transistor and the gate terminal of the enhanced MOS transistor respectively receive the clock signal input by the corresponding boost step. The boost charge booster circuit of claim 9, wherein the source terminal of the enhanced drain channel MOS transistor receives the input voltage signal, the enhanced germanium channel MOS transistor and The closed terminals of the enhanced germanium channel MOS transistors respectively receive the clock signals input by the corresponding boost steps. The boost charge boost circuit of claim 10, wherein the increase is 2008-10-331 = voltage N-channel MOS semiconductor: the body and the clock signal input by the enhanced step. ° The knife does not receive the corresponding boost 16. A boost charge boost circuit, comprising: a complex diode equivalent network, wherein the two poles are connected remotely, - the bean special, The circuit is a series of points, each of which corresponds to a boosting step: ^ has - the input end; the domain side of the tower is (four) one of the charge-charge boosting circuits, the input-regulator circuit' contains the input terminal and the The input electrical output end of the boost charge boosting circuit is electrically connected to an input power, and the wheel receiving end receives two predetermined electric dust levels, and the output terminal outputs the voltage to the voltage circuit. The input terminal; / boosting power to increase at least one boost capacitor network, each of which is electrically connected to - the nodes, each of which - the end point of a"; eight w also Shikou κ, etc. Another network:::, a clock signal electrical connection 'where the clock signal has a voltage level to a 以及 and a low voltage position by 夕 祛 稽 稽 5 5 5 亥 亥 亥 亥 亥 亥 亥曰, cross-linking, so that the input voltage signal rises to the voltage level value at each boosting step; and the complex I self-opening; The circuit, each of the reverse current-cutting circuits are electrically connected to each other, and each of the controls: corresponding to one of the diode-equivalent networks. The current cutoff circuit has at least two conduction paths. ', ^, as described in claim 16, the boost charge boost circuit, wherein the path # is based on each boost): the switching of the clock signals is alternately turned on to avoid the boost charge boost circuit Reverse reverse current. The boost charge boost circuit of claim 16, wherein the clock signal is opposite in phase between every two adjacent nodes. 1 9. The boost charge boost circuit of claim 18, wherein the reverse current cutoff circuit comprises two electronic switch networks, the conductive characteristics of the electronic switch networks being opposite to the clock signal One of the electronic switch networks is turned on when switching. 2. The boost charge boosting circuit of claim 16, wherein each of the f-equivalent equivalent networks is a depleted transistor and the two electronic switching networks of the reverse current cutoff circuits One of the paths is formed. When the electronic switch network in the diode equivalent network is turned on, the depleted transistor is connected to one of the corresponding reverse current cutoff circuits to form a diode connection. ▲] The boost charge boosting circuit of claim 17, wherein each equal-equivalent equivalent network is composed of a depleted transistor and the two electronic switching networks One of the roads is composed of one of the two poles 16 and one of the reverse current cutoff circuits corresponding to the two-pole item 16 when the electronic switch network of the two poles, the second, the second, the middle, the middle, and the second circuit are turned on. The boosting charge boosting circuit, wherein the circuit comprises: two electronic switching networks, and the electronic switching network is opposite to each other, so that the temple is turned on when the clock signal is switched One of the electronic switch networks. The step-up charge boosting circuit described in the above paragraph, wherein the circuit of the circuit comprises two electronic switch networks, and the electronic switch network is electrically opposite, so that when the clock signal is switched Open one of the ones of the electric switch network respectively. κ inverse: the boosted charge boosting circuit, wherein the L circuit comprises two electronic switching networks, and the electrical switching network 25 200810331 has a conductive characteristic opposite to the electronic switching network of the aunt and the like. One; ^ 4 pulse number switching respectively to turn on the 25. If the request item 16, the tenth, the reverse current cutoff circuit package (four) ink charge increase circuit, wherein the same - enhanced p 3 two enhanced N channel The MOS semiconductor transistor MOS transistor 监 监 监 监 监 监 监 监 监 监 监 訏 訏 訏 訏 訏 訏 訏 訏 訏 訏 增强 增强 增强 增强 增强 增强 增强 增强 增强 增强 增强 增强 增强 增强 增强 增强 增强 增强 增强 增强 增强 增强 增强 增强 增强To be high, the enhanced N, 甬22/P pass MOS transistor is turned off and the 26:i/command MOS transistor is turned on. The step-up charge boosting circuit described in FIG. 1/17, wherein the enhanced Nii channel MOS transistor 2:=: channel MOS transistor, when corresponding boost, input When the pulse signal of the day is a low voltage level, the enhanced p-conductor transistor is turned on and the enhanced-type gold-oxide semiconductor body is turned off, when the clock signal input by the corresponding boost step is a high voltage level. The reinforced P-channel MOS transistor is turned off and the reinforced N-channel MOS transistor is turned on. The boost charge boost circuit of claim 19, wherein the reverse current cutoff circuit comprises an enhancement type N-channel MOS transistor and an enhancement type P-channel MOS transistor, corresponding to When the clock signal input by the boosting step is a low voltage level, the enhanced P-channel MOS transistor is turned on and the enhanced N-channel MOS transistor is turned off, and the corresponding boost step is input. When the clock signal is at a high voltage level, the enhanced 蜇p-channel MOS transistor is turned off and the enhanced N-channel MOS transistor is turned on. The boost charge boosting circuit of claim 2, wherein the source terminal of the enhanced P-channel MOS transistor receives the input voltage 26 200810331 signal 'the enhanced p-channel MOS half N The channel MOS: body % steroid and the input terminal of the enhanced step respectively receive a corresponding boost 29. The boost charge as described in claim 24, the strong P it gold oxide Semiconductor power: two-degree Xuanzeng signal, the enhanced original pole & receiving money into the voltage M, s people & pass i虱 + conductor crystal and the bare, the five gas semiconductor transistor gate g & f + the input of the clock signal. And the sigma receives the corresponding boost voltage = the source terminal of the liter charge oxygen semiconductor transistor described in claim 25, and receives the input: the ρ channel MOS transistor and the reinforced oxygen semiconductor transistor The inter-terminal receives the corresponding clock signal input by the corresponding boost I5 white. The boost charge boosting circuit of item 26, wherein each of the packets: 1 comprises a depleted transistor, and the source and the drain of the depleted transistor are electrically connected. The boost charge boosting circuit of claim 29, wherein each f-boost capacitor network is routed to a depletion transistor, and the source and the drain of the depletion transistor are electrically connected. . 33·^二求项} The boosted charge boosting circuit described in 6, wherein each of the boosting, the network routing is formed by a junction field effect transistor (JFET), and the junction field effect transistor The source and the drain are electrically connected. 34. The boost charge boost circuit of claim 29, wherein each boost capacitor network is routed to a junction field effect transistor (JFET), the source of the junction field effect transistor and The bungee is electrically connected. 35. The boost charge boost circuit of claim 16, wherein each of the diode equivalent networks is comprised of a junction field effect transistor (JFET), each of the junction fields The effect transistor (JFET) is connected to one of the corresponding reverse current 27 200810331 cut-off circuits to form a diode. $. The boost charge boosting circuit of claim 29, wherein each of the one poles = equivalent network is composed of a junction field effect transistor (), and the mating field A utility transistor (JFET) is connected to one of the corresponding reverse current cutoff circuits to form a diode. 37·- a boosting unit for a charge boosting circuit, comprising: an equivalent diode network, receiving an input voltage; - a capacitor network, the enchant equivalent binary network money connection, by - the clock money output is higher than a voltage of the input voltage; and a switch pair electrically connected to the equivalent diode network to control whether the equivalent diode network forms a diode connection (enabl) The voltage boosting unit of claim 37, wherein the switch pair controls conduction of the input voltage by the clock signal, the switch pair having at least two conduction paths, the switch pair The clock signal has at least two signal conditions. The boosting unit of claim 38, wherein the conduction paths are alternately turned on according to the change of the clock signal. For one of the voltages of the grounding voltage 40, the boosting unit as described in claim 38, the change blocks the generation of the reverse current. 41. The boosting unit, as described in claim 37, and a ground. Electrical connection 42. As requested in item 4 1 Boosting of the cell, the value is not limited to square 43. The request entry of the said booster unit 38, wherein the channel clock as a high voltage state, and wear / low voltage state. 28 [deg.]
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Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
TWI494730B (en) * 2009-12-17 2015-08-01 Magnachip Semiconductor Ltd Circuit for generating boosted voltage and method for operating the same

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
TWI494730B (en) * 2009-12-17 2015-08-01 Magnachip Semiconductor Ltd Circuit for generating boosted voltage and method for operating the same

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