CN101470458B - Bandgap Reference Voltage Reference Circuit - Google Patents

Bandgap Reference Voltage Reference Circuit Download PDF

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CN101470458B
CN101470458B CN2007103038918A CN200710303891A CN101470458B CN 101470458 B CN101470458 B CN 101470458B CN 2007103038918 A CN2007103038918 A CN 2007103038918A CN 200710303891 A CN200710303891 A CN 200710303891A CN 101470458 B CN101470458 B CN 101470458B
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CN101470458A (en
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王晗
叶青
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Ruili Flat Core Microelectronics Guangzhou Co Ltd
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Institute of Microelectronics of CAS
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Abstract

The invention discloses a band gap reference voltage reference circuit, which comprises: a VBEA voltage generator (11), the VBEThe voltage generator (11) comprises a self-bias current source (111) for generating a two-branch reference circuit, and a circuit coupled to the self-bias current source (111) for generating two paths VBEA bias generator (112) of voltage; a reference voltage regulator (12), the reference voltage regulator (12) comprising an operational transconductance amplifier (121) and a reference voltage regulating unit (122) for generating a constant reference voltage. The invention uses the transistor of the sub-threshold working region to replace a resistor to amplify the voltage with positive temperature coefficient, thereby reducing the power consumption and the cost of the band-gap reference voltage reference circuit.

Description

带隙基准电压参考电路 Bandgap Reference Voltage Reference Circuit

技术领域technical field

本发明涉及模拟电路设计技术领域,特别是一种无需任何电阻元件的低功耗带隙基准电压参考电路。The invention relates to the technical field of analog circuit design, in particular to a low-power consumption bandgap reference voltage reference circuit without any resistance element.

背景技术Background technique

在模拟电路设计中,基准电压参考电路是许多重要功能模块必不可少的组成单元之一。电压基准的目的是建立一个与温度、工艺和电源电压变化无关的直流电压源。In analog circuit design, the reference voltage reference circuit is one of the essential components of many important functional modules. The purpose of a voltage reference is to create a DC voltage source that is independent of temperature, process, and supply voltage variations.

目前公认的电压基准技术为带隙电压基准。一种带隙电压基准利用与绝对温度成正比的电路,来抵消双极型晶体管基区-发射区电压的负温度特性,从而得到恒定的输出基准电压,输出电压值一般为硅的带隙电压1.25V左右。而且带隙电压基准可以在不同的电源电压和工艺条件以及较宽的工作温度范围下保持稳定。The currently recognized voltage reference technology is a bandgap voltage reference. A bandgap voltage reference uses a circuit proportional to absolute temperature to offset the negative temperature characteristic of the base-emitter voltage of a bipolar transistor, thereby obtaining a constant output reference voltage, which is typically the bandgap voltage of silicon 1.25V or so. Moreover, the bandgap voltage reference can remain stable under different supply voltages and process conditions as well as a wide operating temperature range.

双极型晶体管的基区-发射区电压具有负温度系数,一般情况下,此温度系数大约为-1.5mV/℃。当两个双极型晶体管工作在不相等的电流密度下,它们的基区-发射区电压的差值就与绝对温度成正比。一般情况下,差值的温度系数是单个双极型晶体管基区-发射区电压温度系数的三分之一到六分之一。The base-emitter voltage of bipolar transistors has a negative temperature coefficient. Generally, this temperature coefficient is about -1.5mV/°C. When two bipolar transistors are operated at unequal current densities, the difference in their base-emitter voltages is proportional to the absolute temperature. Typically, the temperature coefficient of the difference is one third to one sixth of the temperature coefficient of the base-emitter voltage of a single bipolar transistor.

在传统的带隙基准电路中,一般采用两个不同的电阻值之比来放大两个双极型晶体管的基区-发射区电压的差值,使其和单个双极型晶体管基区-发射区电压的温度系数相抵消,这样得到了具有零温度系数的基准电压。In traditional bandgap reference circuits, the ratio of two different resistor values is generally used to amplify the difference in the base-emitter voltages of two bipolar transistors so that it is comparable to the base-emitter voltage of a single bipolar transistor. The temperature coefficient of the zone voltage cancels out, thus obtaining a reference voltage with zero temperature coefficient.

传统的CMOS工艺流程中采用硅化工艺来减小多晶硅和扩散区的薄膜电阻,从而增大了所需的电阻的长度和面积。部分工艺流程可以采用硅化阻挡层来增大电阻值,与此同时增加了工艺的成本。而在传统带隙基准电压参考电路中,一般采用大电阻来达到低功耗的要求,这样也使得电路的成本大大增加。In the traditional CMOS process flow, the silicide process is used to reduce the sheet resistance of the polysilicon and the diffusion region, thereby increasing the length and area of the required resistance. Part of the process flow can use the silicide barrier layer to increase the resistance value, and at the same time increase the cost of the process. However, in traditional bandgap reference voltage reference circuits, large resistors are generally used to meet the requirements of low power consumption, which also greatly increases the cost of the circuit.

基准电压电路设计须考虑的一个因素是其电路所需的尺寸或者芯片面积。通常,基准电压电路的尺寸由集成电路的主电路设计来决定。减小基准电压电路所需的面积,有助于使得电路芯片面积最小化或增加供主电路设计所用的面积,从而减小芯片成本。One factor that must be considered in the design of a voltage reference circuit is the size or chip area required for its circuit. Usually, the size of the reference voltage circuit is determined by the main circuit design of the integrated circuit. Reducing the required area of the reference voltage circuit helps to minimize the chip area of the circuit or increase the area used for the main circuit design, thereby reducing chip cost.

此外,CMOS工艺中提供的电阻具有一定的温度系数,从而影响输出基准电压的性能,而工艺厂商提供的电阻模型往往精度较低,因此传统的带隙基准电压参考电路性能往往受限于电阻的性能和模型的精确程度。In addition, the resistance provided in the CMOS process has a certain temperature coefficient, which affects the performance of the output reference voltage, and the resistance model provided by the process manufacturer is often of low accuracy, so the performance of the traditional bandgap reference voltage reference circuit is often limited by the resistance. performance and accuracy of the model.

随着深亚微米集成电路工艺和手持移动设备产业的飞速发展,低功耗的模拟电路设计正成为研究的热点。在传统的基准电路里,为了降低功耗,往往会采用大面积的电阻。如果能够作出无需电阻元件的基准电路,则可以大大降低其功耗和成本。With the rapid development of deep submicron integrated circuit technology and handheld mobile device industry, low-power analog circuit design is becoming a research hotspot. In traditional reference circuits, in order to reduce power consumption, large-area resistors are often used. If a reference circuit without resistive components can be made, its power consumption and cost can be greatly reduced.

发明内容Contents of the invention

(一)要解决的技术问题(1) Technical problems to be solved

有鉴于此,本发明的主要目的在于提供一种无需任何电阻元件的低功耗带隙基准电压参考电路,以降低带隙基准电压参考电路的功耗和成本。In view of this, the main purpose of the present invention is to provide a low power consumption bandgap reference voltage reference circuit without any resistance element, so as to reduce the power consumption and cost of the bandgap reference voltage reference circuit.

(二)技术方案(2) Technical solution

为了达到上述目的,本发明的技术方案是这样实现的:In order to achieve the above object, the technical solution of the present invention is achieved in that:

一种带隙基准电压参考电路,该电路包括:A bandgap reference voltage reference circuit, the circuit comprising:

一VBE电压产生器11,该VBE电压产生器11包括一个用于产生两支路参考电路的自偏置电流源111,以及耦合于该自偏置电流源111的用于产生两路VBE电压的偏置发生器112;A V BE voltage generator 11, the V BE voltage generator 11 includes a self-bias current source 111 for generating two-way reference circuits, and a self-bias current source 111 coupled to the self-bias current source 111 for generating two-way V Bias generator 112 for BE voltage;

一基准电压调节器12,该基准电压调节器12包括运算跨导放大器121和基准电压调节单元122,用于产生一个恒定的基准电压;其中:A reference voltage regulator 12, which includes an operational transconductance amplifier 121 and a reference voltage adjustment unit 122 for generating a constant reference voltage; wherein:

自偏置电流源111包括PMOS晶体管M1、M2和NMOS晶体管M3、M4,其中M1和M2的源极与参考电源相连接,M1的栅极、M2的栅极和漏极以及M4的漏极直接耦合,而M1的漏极、M3的栅极和漏极以及M4的栅极直接耦合,M3、M4的源极分别与所述偏置发生器112中pnp晶体管D1和D2的发射区相连接;The self-bias current source 111 includes PMOS transistors M1, M2 and NMOS transistors M3, M4, wherein the sources of M1 and M2 are connected to the reference power supply, the gate of M1, the gate and drain of M2 and the drain of M4 are directly coupled, and the drain of M1, the gate and drain of M3 and the gate of M4 are directly coupled, and the sources of M3 and M4 are respectively connected to the emitter regions of pnp transistors D1 and D2 in the bias generator 112;

偏置发生器112包括pnp晶体管D1和D2,D1和D2的基区和集电区接地,发射区与所述自偏置电流源111中M3和M4的源极分别相连接;The bias generator 112 includes pnp transistors D1 and D2, the base area and the collector area of D1 and D2 are grounded, and the emitter area is respectively connected to the sources of M3 and M4 in the self-bias current source 111;

运算跨导放大器121包括一路正输入端、一路负输入端和一路输出端,其中正输入端与所述基准电压调节单元122中的晶体管M7的栅极相连接,负输入端与所述自偏置电流源111中M3的源极相连接,输出与晶体管M5的栅极相连接;所述晶体管M5用于为所述基准电压调节单元122提供直流偏置;The operational transconductance amplifier 121 includes one positive input terminal, one negative input terminal and one output terminal, wherein the positive input terminal is connected to the gate of the transistor M7 in the reference voltage adjustment unit 122, and the negative input terminal is connected to the self-biased The source of M3 in the current source 111 is connected, and the output is connected to the gate of the transistor M5; the transistor M5 is used to provide a DC bias for the reference voltage adjustment unit 122;

基准电压调节单元122包括PMOS晶体管M6、M7和M8,该晶体管M6、M7和M8是工作中亚阈值的晶体管,其中晶体管M6和M7的栅极与漏极相连接,M8的栅极与所述自偏置电流源111中M4的源极相连接;所述M6、M7和M8的衬底与各自的源极相连接。The reference voltage adjustment unit 122 includes PMOS transistors M6, M7 and M8, the transistors M6, M7 and M8 are sub-threshold transistors in operation, wherein the gates of the transistors M6 and M7 are connected to the drain, and the gate of M8 is connected to the The source of M4 in the self-bias current source 111 is connected; the substrates of M6, M7 and M8 are connected to their respective sources.

上述方案中,所述偏置发生器112产生的第一路偏置和第二路偏置共同耦合到所述自偏置电流源111上产生两路参考电压。In the above solution, the first bias and the second bias generated by the bias generator 112 are jointly coupled to the self-bias current source 111 to generate two reference voltages.

(三)有益效果(3) Beneficial effects

从上述技术方案可以看出,本发明具有以下有益效果:As can be seen from the foregoing technical solutions, the present invention has the following beneficial effects:

1、传统的带隙基准电路利用电阻将电流转变成电压形式,并且提供正温度系数电压的增益。工作在亚阈值区的MOS晶体管的栅源电压随着温度的升高而在一定范围内近似线性降低。基于该特性,传统带隙基准电路中的电阻可以被工作在亚阈值区的晶体管套筒形式代替来产生正温度系数电压的增益,用于抵消负温度系数的双极型晶体管基极-发射极电压,输出一个低温度系数的基准源,从而避免了电阻的使用,减小了电路的功耗和面积。1. Traditional bandgap reference circuits use resistors to convert current into voltage form and provide positive temperature coefficient voltage gain. The gate-source voltage of a MOS transistor operating in the subthreshold region decreases approximately linearly within a certain range as the temperature increases. Based on this characteristic, the resistors in the traditional bandgap reference circuit can be replaced by transistor sleeves operating in the subthreshold region to generate a positive temperature coefficient voltage gain, which is used to offset the negative temperature coefficient of the bipolar transistor base-emitter Voltage, outputting a reference source with a low temperature coefficient, thus avoiding the use of resistors and reducing the power consumption and area of the circuit.

2、本发明利用亚阈值工作区的晶体管来代替电阻放大具有正温度系数的电压,从而得到低功耗,高集成度的带隙基准电压参考电路,达到了降低带隙基准电压参考电路的功耗和成本的目的。2, the present invention utilizes the transistor of sub-threshold value work area to replace the voltage with positive temperature coefficient of resistance amplification, thereby obtains low power consumption, the bandgap reference voltage reference circuit of high integration degree, has reached and reduced the function of bandgap reference voltage reference circuit consumption and cost purposes.

3、本发明提供的带隙基准电压参考电路,消除了电阻的使用,采用亚阈值区的晶体管减小了电路的工作电流和面积,与传统的带隙基准电压参考电路相比具有更低的功耗和成本。3. The bandgap reference voltage reference circuit provided by the present invention eliminates the use of resistors, and adopts transistors in the subthreshold region to reduce the operating current and area of the circuit. Compared with traditional bandgap reference voltage reference circuits, it has a lower power consumption and cost.

附图说明Description of drawings

图1是本发明提供的带隙基准电压参考电路的电路图;Fig. 1 is the circuit diagram of the bandgap reference voltage reference circuit provided by the present invention;

图2是图1所示电压基准电路输出基准电压的温度特性曲线图;Fig. 2 is a temperature characteristic curve diagram of the output reference voltage of the voltage reference circuit shown in Fig. 1;

图3是图1所示电压基准电路输出基准电压随电源电压变化曲线图。FIG. 3 is a graph showing the variation of the output reference voltage of the voltage reference circuit shown in FIG. 1 with the power supply voltage.

具体实施方式Detailed ways

为使本发明的目的、技术方案和优点更加清楚明白,以下结合具体实施例,并参照附图,对本发明进一步详细说明。In order to make the object, technical solution and advantages of the present invention clearer, the present invention will be described in further detail below in conjunction with specific embodiments and with reference to the accompanying drawings.

如图1所示,图1是本发明提供的带隙基准电压参考电路的电路图,该电路包括VBE电压产生器11和基准电压调节器12。其中,该VBE电压产生器11包括一个用于产生两支路参考电路的自偏置电流源111,以及耦合于该自偏置电流源111的用于产生两路VBE电压的偏置发生器112。该基准电压调节器12包括运算跨导放大器121和基准电压调节单元122,用于产生一个恒定的基准电压。As shown in FIG. 1 , FIG. 1 is a circuit diagram of a bandgap reference voltage reference circuit provided by the present invention, and the circuit includes a V BE voltage generator 11 and a reference voltage regulator 12 . Wherein, the V BE voltage generator 11 includes a self-bias current source 111 for generating two-branch reference circuits, and a bias generator coupled to the self-bias current source 111 for generating two V BE voltages device 112. The reference voltage regulator 12 includes an operational transconductance amplifier 121 and a reference voltage adjustment unit 122 for generating a constant reference voltage.

所述VBE电压产生器11产生第一路VBE电压和第二路VBE电压,所述第一路VBE电压直接耦合到所述基准电压调节单元122上,所述第二路VBE电压通过所述运算跨导放大器121耦合到所述基准电压调节单元122上。The V BE voltage generator 11 generates a first V BE voltage and a second V BE voltage, the first V BE voltage is directly coupled to the reference voltage adjustment unit 122, and the second V BE voltage is directly coupled to the reference voltage adjustment unit 122. The voltage is coupled to the reference voltage adjustment unit 122 through the operational transconductance amplifier 121 .

所述自偏置电流源111包括PMOS晶体管M1、M2和NMOS晶体管M3、M4,其中M1和M2的源极与参考电源相连接,M1的栅极、M2的栅极和漏极以及M4的漏极直接耦合,而M1的漏极、M3的栅极和漏极以及M4的栅极直接耦合,M3、M4的源极分别与所述偏置发生器112中pnp晶体管D1和D2的发射区相连接。The self-bias current source 111 includes PMOS transistors M1, M2 and NMOS transistors M3, M4, wherein the sources of M1 and M2 are connected to the reference power supply, the gate of M1, the gate and drain of M2 and the drain of M4 pole is directly coupled, and the drain of M1, the gate and drain of M3 and the gate of M4 are directly coupled, and the sources of M3 and M4 are respectively in phase with the emitter regions of pnp transistors D1 and D2 in the bias generator 112 connect.

所述用于产生两路VBE电压的偏置发生器112包括pnp晶体管D1和D2,D1和D2的基区和集电区接地,发射区与所述自偏置电流源111中M3和M4的源极分别相连接。所述晶体管D1的导电区为所述晶体管D2导电区的N倍。The bias generator 112 for generating two-way V BE voltages includes pnp transistors D1 and D2, the base and collector regions of D1 and D2 are grounded, and the emitter region is connected to M3 and M4 in the self-bias current source 111 The sources are connected separately. The conduction area of the transistor D1 is N times the conduction area of the transistor D2.

所述偏置发生器112产生的第一路偏置和第二路偏置共同耦合到所述自偏置电流源111上产生两路参考电压。The first bias and the second bias generated by the bias generator 112 are jointly coupled to the self-bias current source 111 to generate two reference voltages.

所述运算跨导放大器121包括一路正输入端、一路负输入端和一路输出端,其中正输入端与所述基准电压调节单元122中的晶体管M7的栅极相连接,负输入端与所述自偏置电流源111中M3的源极相连接,输出与晶体管M5的栅极相连接。所述晶体管M5用于为所述基准电压调节单元122提供直流偏置。The operational transconductance amplifier 121 includes one positive input terminal, one negative input terminal and one output terminal, wherein the positive input terminal is connected to the gate of the transistor M7 in the reference voltage adjustment unit 122, and the negative input terminal is connected to the gate of the transistor M7 in the reference voltage adjustment unit 122. The source of M3 in the self-bias current source 111 is connected, and the output is connected to the gate of transistor M5. The transistor M5 is used to provide a DC bias for the reference voltage adjustment unit 122 .

所述基准电压调节单元122包括PMOS晶体管M6、M7和M8,所述晶体管M6和M7的栅极与漏极相连接,M8的栅极与所述自偏置电流源111中M4的源极相连接;所述M6、M7和M8的衬底与各自的源极相连接。The reference voltage adjustment unit 122 includes PMOS transistors M6, M7 and M8, the gates of the transistors M6 and M7 are connected to the drain, and the gate of M8 is connected to the source of M4 in the self-bias current source 111. connection; the substrates of M6, M7 and M8 are connected to their respective sources.

再参照图1,pnp双极型晶体管D1和D2用来产生两个具有负温度系数的电压31和32,所述节点的温度系数A可以表示为下式:Referring to FIG. 1 again, pnp bipolar transistors D1 and D2 are used to generate two voltages 31 and 32 with negative temperature coefficients, and the temperature coefficient A of the nodes can be expressed as the following formula:

A=(VBE-2.5×VT-Eg/q)/T                               (1)A=(V BE -2.5×V T -E g /q)/T (1)

所述公式(1)中,VBE表示双极型晶体管D1和D2发射极电压,Eg为硅的带隙能量,T为绝对温度。因此当VBE约等于750mV,T=300K时,VBE的温度系数约为-1.5mV/℃。In the formula (1), V BE represents the emitter voltage of the bipolar transistors D1 and D2, E g is the bandgap energy of silicon, and T is the absolute temperature. Therefore, when V BE is approximately equal to 750mV and T=300K, the temperature coefficient of V BE is approximately -1.5mV/°C.

所述节点31通过运算跨导放大器121耦合到节点33,而运算跨导放大器的输出端口控制基准电压调节单元122的直流偏置,因此有:The node 31 is coupled to the node 33 through an operational transconductance amplifier 121, and the output port of the operational transconductance amplifier controls the DC bias of the reference voltage adjustment unit 122, so:

V31=V33                                              (2)V 31 =V 33 (2)

由所述(2)式,得:From the (2) formula, get:

V33-V32=VT×ln(n)                                    (3)V 33 −V 32 =V T ×ln(n) (3)

所述(3)式中VT为热电压,在常温下约等于26mV,N为双极型晶体管D2和D1导电区面积之比。而由于直流电流流过MOS晶体管M6、M7和M8,当所述晶体管的漏极到源极的电压大于4倍VT时,可以得到以下三式:In the formula (3), V T is the thermal voltage, which is approximately equal to 26mV at normal temperature, and N is the ratio of the conductive areas of the bipolar transistors D2 and D1. Since the direct current flows through the MOS transistors M6, M7 and M8, when the voltage from the drain to the source of the transistor is greater than 4 times V T , the following three formulas can be obtained:

IM6=uCdVT 2WM6/LM6exp((V35-V34-|Vth,M6|)/(r×VT))    (4)I M6 =uC d V T 2 W M6 /L M6 exp((V 35 -V 34 -|V th, M6 |)/(r×V T )) (4)

IM7=uCdVT 2WM7/LM7exp((V34-V33-|Vth,M7|)/(r×VT))    (5)I M7 =uC d V T 2 W M7 /L M7 exp((V 34 −V 33 −|V th, M7 |)/(r×V T )) (5)

IM8=uCdVT 2WM8/LM8exp((V33-V32-|Vth,M8|)/(r×VT))    (6)I M8 =uC d V T 2 W M8 /L M8 exp((V 33 -V 32 -|V th, M8 |)/(r×V T )) (6)

所述式(4)-(6)中,I为流过晶体管的电流,u为少数载流子的迁移率,Cd为栅下的耗尽层电容,W和L分别为MOS晶体管的沟道宽度和长度,Vth为MOS晶体管的阈值电压,r为亚阈值坡度因子,式(4)-(6)可以变换成式(7)-(8):In the formulas (4)-(6), I is the current flowing through the transistor, u is the mobility of the minority carriers, C d is the depletion layer capacitance under the gate, W and L are the channel of the MOS transistor respectively The width and length of the track, V th is the threshold voltage of the MOS transistor, r is the subthreshold slope factor, and formulas (4)-(6) can be transformed into formulas (7)-(8):

r×VT×ln(IM6/(uCdVT 2WM6/LM6))=V35-V34-|Vth,M6|    (7)r×V T ×ln(I M6 /(uC d V T 2 W M6 /L M6 ))=V 35 -V 34 -|V th,M6 | (7)

r×VT×ln(IM7/(uCdVT 2WM7/LM7))=V34-V33-|Vth,M7|    (8)r×V T ×ln(I M7 /(uC d V T 2 W M7 /L M7 ))=V 34 -V 33 -|V th, M7 | (8)

r×VT×ln(IM8/(uCdVT 2WM8/LM8))=V33-V32-|Vth,M8|    (9)r×V T ×ln(I M8 /(uC d V T 2 W M8 /L M8 ))=V 33 -V 32 -|V th,M8 | (9)

由于晶体管M6、M7和M8的衬底分别与各自的源极相连,消除了体效应,因此有:Since the substrates of transistors M6, M7, and M8 are connected to their respective sources, the body effect is eliminated, so there are:

|Vth,M6|=|Vth,M7|=|Vth,M8|                      (10)|Vth , M6 |=|Vth , M7 |=|Vth , M8 | (10)

将(9)×2-(7)-(8),同时根据(10),则有:Put (9)×2-(7)-(8), and according to (10), there are:

V35=V32+3×(V33-V32)+r×VT×ln((WM8/LM8)2/((WM6/LM6)×(WM7/LM7)))V 35 =V 32 +3×(V 33 −V 32 )+r×V T ×ln((W M8 /L M8 ) 2 /((W M6 /L M6 )×(W M7 /L M7 )))

                                                     (11)(11)

将(3)式带入(11)式可得:Bring (3) into (11) to get:

V35=V32+3×VT×ln(n)+r×VT×ln((WM8/LM8)2/((WM6/LM6)×(WM7/LM7)))V 35 =V 32 +3×V T ×ln(n)+r×V T ×ln((W M8 /L M8 ) 2 /((W M6 /L M6 )×(W M7 /L M7 )))

                                                     (12)(12)

在(12)式中,节点35即为输出基准电压。所述式中等式右边第一项为负温度系数电压,第二项为正温度系数电压,第三项则为正温度系数电压的调节项。通过选择合适的参数可以使得输出节点35具有零温度系数。In (12) formula, node 35 is the output reference voltage. The first item on the right side of the equation in the above formula is the negative temperature coefficient voltage, the second item is the positive temperature coefficient voltage, and the third item is the adjustment item of the positive temperature coefficient voltage. The output node 35 can be made to have a zero temperature coefficient by selecting appropriate parameters.

采用真实数值的例子有助于说明电压基准电路的设计。假定双极型晶体管发射极的温度系数为-1.5mV/℃,n为24,VT等于26mV,则为了使输出基准电压具有零温度系数,则有下式:Examples using real numerical values help illustrate the design of voltage reference circuits. Assuming that the temperature coefficient of the emitter of the bipolar transistor is -1.5mV/°C, n is 24, and V T is equal to 26mV, in order to make the output reference voltage have a zero temperature coefficient, the following formula is given:

ln((WM8/LM8)2/((WM6/LM6)×(WM7/LM7)))=(-V32-3×VT×ln(n))/(r×VT)ln((W M8 /L M8 ) 2 /((W M6 /L M6 )×(W M7 /L M7 )))=(-V 32 -3×V T ×ln(n))/(r×V T )

                                                     (13)(13)

将式(13)等式两边取微分,再带入具体的数值,则可以得到:Differentiate both sides of the equation (13), and then bring in specific values, you can get:

(WM8/LM8)2/((WM6/LM6)×(WM7/LM7))=180               (14)(W M8 /L M8 ) 2 /((W M6 /L M6 )×(W M7 /L M7 ))=180 (14)

当输出基准电压为零温度系数时,其值等于硅的带隙电压约1.2V,这样再根据初始条件:When the output reference voltage is zero temperature coefficient, its value is equal to the bandgap voltage of silicon about 1.2V, so according to the initial conditions:

V35|T=T0=1.2V                        (15)V 35 | T =T 0 =1.2V (15)

利用亚阈值工作区的晶体管M6、M7和M8的工作方程(4)-(6),可以确定晶体管M6、M7和M8的长度为0.4u,宽度分别为40u,10u和1u。这样,一个具有零温度系数的基准电压参考电路得以实现。Using the working equations (4)-(6) of the transistors M6, M7 and M8 in the subthreshold working region, it can be determined that the length of the transistors M6, M7 and M8 is 0.4u, and the widths are 40u, 10u and 1u respectively. In this way, a reference voltage reference circuit with zero temperature coefficient is realized.

由于晶体管M6、M7和M8工作在亚阈值区,因此流过的电流可以为纳安培级,而运算跨导放大器的输入管也可以工作在亚阈值区来提供一定的增益,这样大大减小了基准电压电路的功耗。Since the transistors M6, M7 and M8 work in the sub-threshold region, the current flowing through them can be at the nanoampere level, and the input tube of the operational transconductance amplifier can also work in the sub-threshold region to provide a certain gain, which greatly reduces the power consumption of the reference circuit.

图2是图1所示电压基准电路输出基准电压的温度特性曲线图。图2所示的曲线图是采用与所述例子相似的元件值下,利用SMIC提供的0.18um CMOS混合信号工艺BSIM3V3 SPICE模型下模拟得出的。该图以40℃为中心,温度范围为-40℃~120℃。在该温度范围内,电压在1.210V与1.216V之间变化,变化幅度为6mV,温度系数为31ppm/℃,ppm表示百万分之一,电路的总电流小于3微安培。FIG. 2 is a temperature characteristic graph of the output reference voltage of the voltage reference circuit shown in FIG. 1 . The graph shown in Figure 2 is simulated under the 0.18um CMOS mixed-signal process BSIM3V3 SPICE model provided by SMIC with component values similar to the above example. The graph is centered on 40°C and the temperature range is from -40°C to 120°C. In this temperature range, the voltage varies between 1.210V and 1.216V, the variation range is 6mV, the temperature coefficient is 31ppm/℃, ppm means one millionth, and the total current of the circuit is less than 3 microamperes.

图3是图1所示电压基准电路输出基准电压随电源电压变化曲线图。采用的工艺同图2中所述。该图表示输出基准电压随电源电压从0V到5V变化时的响应。当电源电压从0V上升,输出基准电压也随着升高;当电源电压升高到1.5V时,输出基准电压升至1.2V,并随后保持基本恒定,一直到电源电压升至5V。在该电源电压变化范围内,电压在1.211V与1.233V之间(室温下)变化,变化幅度为22mV,电源电压抑制系数为6mV/V。FIG. 3 is a graph showing the variation of the output reference voltage of the voltage reference circuit shown in FIG. 1 with the power supply voltage. The process used is the same as that described in Figure 2. This graph shows the response of the output reference voltage as the supply voltage varies from 0V to 5V. When the supply voltage increases from 0V, the output reference voltage also increases; when the supply voltage increases to 1.5V, the output reference voltage rises to 1.2V, and then remains basically constant until the supply voltage rises to 5V. Within the power supply voltage variation range, the voltage varies between 1.211V and 1.233V (at room temperature), the variation range is 22mV, and the power supply voltage suppression coefficient is 6mV/V.

至此,可以理解,本发明提供的这种无电阻的电压基准电路。对于MOS晶体管,当漏电流保持不变时,工作在弱反型区的晶体管的栅源电压随着温度的升高而在一定范围内近似线性降低。利用多个套筒结构的工作在亚阈值区的晶体管可以代替电阻来放大具有正温度系数的电压,使其与具有负温度系数的双极型晶体管基区-发射区电压相抵消,从而产生了与温度无关的基准电压。由于消除了电阻的使用,从而减小了电路的功耗和面积。So far, it can be understood that the non-resistor voltage reference circuit provided by the present invention. For MOS transistors, when the leakage current remains constant, the gate-source voltage of the transistor operating in the weak inversion region decreases approximately linearly within a certain range as the temperature increases. Transistors operating in the subthreshold region using multiple sleeve structures can replace resistors to amplify voltages with positive temperature coefficients to cancel out the base-emitter voltages of bipolar transistors with negative temperature coefficients, resulting in Temperature Independent Reference Voltage. Since the use of resistors is eliminated, the power consumption and area of the circuit are reduced.

基于图1所示的带隙基准电压参考电路,本发明还提供了一种应用带隙基准电压参考电路产生基准电压的方法,该方法包括以下步骤:Based on the bandgap reference voltage reference circuit shown in Figure 1, the present invention also provides a method for applying the bandgap reference voltage reference circuit to generate a reference voltage, the method comprising the following steps:

产生两个具有负温度系数的参考电压;Generate two reference voltages with negative temperature coefficients;

将产生的这两个参考电压相减得到具有正温度系数的电压;Subtracting these two generated reference voltages yields a voltage with a positive temperature coefficient;

放大该具有正温度系数的电压;amplifying the voltage with a positive temperature coefficient;

将相等的具有正负温度系数的两个电压相加,得到基准电压。The reference voltage is obtained by adding two equal voltages with positive and negative temperature coefficients.

所述放大该具有正温度系数的电压是由处于亚阈值工作区的晶体管完成的;所述基准电压由一个基区-发射区电压降和经过放大的具有相等正温度系数的电压之和产生。The amplification of the voltage with a positive temperature coefficient is accomplished by transistors in the subthreshold operating region; the reference voltage is generated by the sum of a base-emitter voltage drop and the amplified voltage with an equal positive temperature coefficient.

以上所述的具体实施例,对本发明的目的、技术方案和有益效果进行了进一步详细说明,所应理解的是,以上所述仅为本发明的具体实施例而已,并不用于限制本发明,凡在本发明的精神和原则之内,所做的任何修改、等同替换、改进等,均应包含在本发明的保护范围之内。The specific embodiments described above have further described the purpose, technical solutions and beneficial effects of the present invention in detail. It should be understood that the above descriptions are only specific embodiments of the present invention and are not intended to limit the present invention. Any modifications, equivalent replacements, improvements, etc. made within the spirit and principles of the present invention shall be included within the protection scope of the present invention.

Claims (2)

1. a bandgap voltage reference circuit is characterized in that, this circuit comprises:
One V BEVoltage generator (11), this V BEVoltage generator (11) comprises a self-bias current source (111) that is used to produce two branch road reference circuits, and be coupled in this self-bias current source (111) be used to produce two-way V BEThe bias generator of voltage (112);
One reference voltage regulator (12), this reference voltage regulator (12) comprise operation transconductance amplifier (121) and reference voltage regulon (122), are used to produce a constant reference voltage; Wherein:
Self-bias current source (111) comprises PMOS transistor M1, M2 and nmos pass transistor M3, M4, wherein the source electrode of M1 and M2 is connected with reference power source, the drain electrode of the grid of M1, the grid of M2 and drain electrode and M4 directly is coupled, and the grid of the grid of the drain electrode of M1, M3 and drain electrode and M4 directly is coupled, and the source electrode of M3, M4 is connected with the launch site of middle pnp transistor D1 of described bias generator (112) and D2 respectively;
Bias generator (112) comprises pnp transistor D1 and D2, the base of D1 and D2 and collecting zone ground connection, and the launch site is connected respectively with the source electrode of middle M3 of described self-bias current source (111) and M4;
Operation transconductance amplifier (121) comprises one road positive input terminal, one road negative input end and one road output terminal, wherein the grid of the transistor M7 in positive input terminal and the described reference voltage regulon (122) is connected, negative input end is connected with the source electrode of M3 in the described self-bias current source (111), and output is connected with the grid of transistor M5; Described transistor M5 is used to described reference voltage regulon (122) that direct current biasing is provided;
Reference voltage regulon (122) comprises PMOS transistor M6, M7 and M8, this transistor M6, M7 and M8 are the transistors of subthreshold value in the work, wherein the grid of transistor M6 and M7 is connected with drain electrode, and the grid of M8 is connected with the source electrode of M4 in the described self-bias current source (111); The substrate of described M6, M7 and M8 is connected with source electrode separately.
2. bandgap voltage reference circuit according to claim 1 is characterized in that, the first via biasing that described bias generator (112) produces and the second tunnel biasing coupled in common go up to described self-bias current source (111) and produce the two-way reference voltage.
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