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A New 8T SRAM Circuit with Low Leakage and High Data Stability Idle Mode at 70nm Technology

P. Raikwal1*, V. Neema1 and A.Verma2

1Department of Electronics and Telecommunication Engineering, IET, Devi Ahilya University, Indore, India

2IDepartment of Electronics and Instrumentation Engineering, IET, Devi Ahilya University, Indore, India

 

 

DOI : http://dx.doi.org/10.13005/ojcst/10.01.12

Article Publishing History
Article Received on : February 16, 2017
Article Accepted on : March 10, 2017
Article Published : 22 Mar 2017
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ABSTRACT:

Memory has been facing several problems in which the leakage current is the most severe. Many techniques have been proposed to withstand leakage control such as power gating and ground gating.  In this paper a new 8T SRAM cell, which adopts a single bit line scheme has been proposed to limit the leakage current as well as to gain high hold static noise margin. The proposed cell with low threshold voltage, high threshold voltage and dual threshold voltage are used to effectively reduce leakage current, and delay. Additionally, the comparison has been performed between conventional 6T SRAM cell and the new 8T SRAM cell. The proposed circuit consumes 671.22 pA leakage current during idle state of the circuit which is very less as compare to conventional 6T SRAM cell with sleep and hold transistors and with different β ratio. The proposed new 8T SRAM cell shows highest noise immunity 0.329mv during hold state. Furthermore, the proposed new 8T SRAM circuit represents minimum read and write access delays 114.13ps and 38.56ps respectively as compare to conventional 6T SRAM cell with different threshold voltages and β ratio.

KEYWORDS: SRAM; static noise margin; single bit line; threshold voltage; leakage current; β ratio

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Raikwal P, Neema V, Verma A. A New 8T SRAM Circuit with Low Leakage and High Data Stability Idle Mode at 70nm Technology. Orient.J. Comp. Sci. and Technol;10(1)


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Raikwal P, Neema V, Verma A. A New 8T SRAM Circuit with Low Leakage and High Data Stability Idle Mode at 70nm Technology. Orient.J. Comp. Sci. and Technol;10(1). Available from: http://www.computerscijournal.org/?p=4973


Introduction

It has always been a great challenge to fabricate a circuit using transistors. To design a big circuit the size of transistor is becoming small [1]. SRAM utilizes minimum sized transistors to fulfill the requirement of high packing density. SRAM is facing severe difficulties after scaling the dimensions of transistor, such as degraded data stability and increased power consumption at advanced technology nodes [2]. The dynamic power dissipation can be reduced by supply voltage scaling [3] [4]. But scaling the supply voltage has adverse effect on static noise margin [5]. So to improve throughout performance of the SRAM cell is a great challenge for the designers [6].

Additionally, leakage current contributes a large proportion for the total power dissipation. Leakage current flows through the circuits during idle mode [7]. MTCMOS and power and ground gating are the most widely utilized circuit techniques for suppressing the leakage current [8] [9]. In this paper a new single ended 8T SRAM is explored. The proposed cell utilizes an extra transistor (CS) to disconnect the feedback loop during active mode. A new read circuitry is introduced to read the stored content. 

Previously proposed Conventional 6T SRAM cell with ground gated technique:

Already published ground gated technique is reviewed in this part of the paper. Fig.2 shows conventional 6T SRAM cell with ground gated circuit. Fig.1 presents the conventional 6T SRAM cell. As conventional 6T SRAM cell is not reliable to perform the operation at low voltage because of voltage division between the access transistors and the pull-down transistors in cross coupled inverters [10]. That affects the data stability of the cell. Therefore, the widths of the pull down transistors are changed to improve the data stability as well as for low power dissipation. The ratio of W/L ratio of pull up transistor to the W/L ratio of pull down transistor is known as beta ratio (β) [11].

In ground gated 6T SRAM circuit a high threshold PMOS hold (HLD) transistor is connected in parallel with high threshold NMOS sleep (SLP) transistor shown in fig.2. This circuitry is connected between the memory cell and ground [12]. During the active mode sleep transistor (N_5) is kept ON while hold transistor (P_3) is OFF. That maintains the ground level approximately at 0 volts. During the idle mode sleep transistor is off whereas hold is on [13]. This particular state of the sleep and hold transistors suppress the leakage current when the circuit is in idle mode [11] [14]. In sleep mode the on state of the hold transistor helps to preserve the stored content of the cell [15].

The transistors sizes are in nanometer 70nm CMOS technology. WL represents wordline, BL and BBAR represent bitline and bitline bar respectively. Fig. 3(a) represents ground gated 6T SRAM cell using low threshold voltage transistors (LVT), where analysis has been performed for  β=1 and β=3. SLP and HLD utilize high threshold voltage transistors. Fig. 3(b) represents ground gated 6T SRAM cell using dual threshold voltage transistors (DVT), where β=1 and β=5 is taken for analysis. In this figure all transistors are high threshold voltage except access transistors. Fig. 3(c) shows ground gated 6T SRAM cell using high threshold voltage transistors (HVT), where analysis has been performed for  β=1 and β=2. In the figures transistors with thin line represent low threshold voltage whereas transistors with thick line represent high threshold voltage.

Fig. 1 Conventional 6T SRAM circuit

Figure 1: Conventional 6T SRAM circuit

 

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Fig. 2 6T SRAM with ground gated circuit

Figure 2 6T SRAM with ground gated circuit

 

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Fig. 3 (a) 6T SRAM (LVT) with ground gated circuit

Figure 3(a): 6T SRAM (LVT) with ground gated circuit 

 

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Fig. 3 (b) 6T SRAM (DVT) with ground gated circuit

Figure 3(b): 6T SRAM (DVT) with ground gated circuit  

 

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 Fig. 3 (c) 6T SRAM (HVT) with ground gated circuit

Figure 3(c): 6T SRAM (HVT) with ground gated circuit



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New 8T SRAM Circuit

In this paper a new single ended 8T SRAM cell is presented for providing low leakage current and high data stability during sleep mode of the circuit. The proposed cell is shown in fig.4 utilizes 70nm technology. The cell is composed of two cross coupled inverters P_1, P_2, N_1 and N_2. Data is stored on Q and QBAR. An extra charge storage transistor CS (N_4) is used to disconnect the feedback loop during active mode of the circuit [16] [17]. Hence this eliminates flipping of content which occurs suddenly in conventional 6T SRAM cell. All transistors have minimum width and length except P_3 has width of 700nm to make read operation easier. A new read port is presented here, composed of bit line access transistor P_3 and NMOS transistor N_5 to which read word line is connected.

 Fig. 4 New 8T SRAM cell

Figure 4: New 8T SRAM cell

 

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Data Preserving Sleep Mode with Low Leakage Current

 In idle mode of the cell write word line WWL, read word line RWL and charge storage transistor CS all are maintained at ground level. The hold operation CS is kept turned off to suppress the leakage current. During sleep mode of the cell strong data stability is reflected as well as with low leakage current.

Write Operation

Prior to write operation BL is charged to VDD or discharged to 0v depending on what is to be written ‘0’ or ‘1’ on the storing node Q. Before initiating single ended write operation WWL is charged to VDD.  Charge storage transistor CS is kept at 0v, to enhance the write stability of the cell during write state.  CS kept the stored content RWL is maintained at 0v. Data is written from bit line to on the node ‘Q’ through the WWL. Due to separate word lines data is stability is improved [18]. The chance of data distortion is eliminated by keeping CS turned off.

Read Operation

Before initiating single ended read operation BL is charged to VDD. RWL and CS are transitions to VDD while WWL is discharged to 0v. In this cell the storing node Q is directly connected to the PMOS (P_3) transistor. Assume that ‘1’ is stored on node Q, BL will not get discharged because the P_3 transistor is in cut off state. Therefore the charge stored at BL is directly access by the sense amplifier and will be read as ‘1’.  Alternatively, when ‘0’ is stored at node Q, the P_3 will turn on. RWL is activated, BL is discharged through P_3 and N_5 and ‘0’ is sensed by the sense amplifier.

Simulation Result and Analysis

In this section the newly proposed single ended SRAM cell and conventional 6T SRAM cell are analyzed and evaluated. The circuit is characterized by using the 70nm technology with the supply voltage of 1.2 volt. Circuit verification is done on the Tanner tool. Schematic of the SRAM cell is designed on the S-Edit and net list simulation done by using T-spice.

In this section conventional  6T SRAM cell and proposed new 8T SRAM cell are compared through different parameters such as read delay, write delay, leakage current, write ability and read and hold static noise margin.

Leakage Power Consumption

In this part the evaluation of the leakage current is performed during the idle state of the memory cell. Here, asymmetrical cell structure of 6T SRAM cell shown in fig. 3(a), 3(b), and 3(c) is considered.  HVT is used for high threshold voltage, LVT is for low threshold voltage and DVT is for dual threshold voltage. Generally, HVT transistor is utilized to suppress leakage current when the circuit is in idle state. LVT is used for high performance applications. DVT is also adopted to get some variation in performance parameters [19].

In this section β is varied for the conventional 6T SRAM cell and then all performance parameters are evaluated. Table 1 and fig.5 show the simulation results of leakage current and leakage power consumption for new 8T SRAM cell and conventional 6T SRAM cell with different threshold voltage and β ratio.

Table 1: Simulation results of leakage power consumption

Cell

Leakage current (nA)

Leakage power consumption(nW)

C6T_Lβ1

349.104

418.8

C6T_Lβ3

476.45

571.2

C6T_Hβ1

11.354

13.624

C6T_Hβ2

14.074

16.88

C6T_Dβ1

13.784

27.568

C6T_Dβ5

18.916

22.699

New8T SRAM

0.671

0.805

 

        Fig.5. Leakage current and Leakage power consumption with different threshold voltages and β ratio

Figure 5: Leakage current and Leakage power consumption with different threshold voltages and β ratio



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Read Access Delay and Write Access Delay

Read delay of 6T SRAM cell is the maximum time interval from the 50% low to high transition of word line to the 50% high to low transition of sense amplifier output. In the proposed 8T SRAM cell there is separate word line for read operation (RWL). The read access time of 8T SRAM cell is evaluated by the maximum time interval from the 50% low to high transition of read word line RWL to the 50% high to low transition of sense amplifier output.

Write delay of 6T SRAM cell and 8T SRAM cell is the longest time interval from the 50% low to high transition of word line to the 50% high to low transition of storing node (Q or QBAR). Table 2 shows the values of read and write access delay and fig.6 shows the graph.

Table 2: Simulation results of read and write access delay

Cell

Read access delay (pS)

Write access delay (pS)

C6T_Lβ1

92.87

234.10

C6T_Lβ3

54.43

115.76

C6T_Hβ1

312.60

940.21

C6T_Hβ2

349.3

891.10

C6T_Dβ1

315.08

539.8

C6T_Dβ5

301.96

535

New8T SRAM

38.56

114.13

 

Fig.6. Read and write access delay with different threshold voltages and β ratio

Figure 6: Read and write access delay with different threshold voltages and β ratio



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Data stability in terms of read and hold static noise margin is evaluated and analyzed in this section. These two parameters estimate the stability of the cell during read and hold state. Data stability of the cell is highly considerable constraint during read operation and hold state of the cell at nanometers technology nodes. At advanced technology data stability reduces because of the supply voltage minimization. Stability is generally defined by the static noise margin (SNM) of the cell [20]. SNM is the maximum value of DC noise voltage that is tolerable by the cell without affecting the stored data of the SRAM cell [1]. In this paper the SNM is calculated using butterfly curve. SNM is calculated graphically by estimating the length of maximum possible square fitted between the voltage transfer characteristics of the cross coupled inverters [7]. In ground gated 6T SRAM cell the RSNM and HSNM are calculated at different β ratio and by utilizing LVT, HVT and DVT transistors. The RSNM of the proposed 8T SRAM cell is estimated by keeping the RWL, WWL and CS at VDD, 0v and VDD respectively.

Hold stability is calculated when the cell is in hold state. At this state the word lines are off, so the whole cell is totally disconnected from the bit lines. Table 3 and fig. 7 represent the stability in terms of RSNM and HSNM.

Table 3: Simulation results of RSNM and HSNM

Cell

RSNM (mv)

HSNM (mv)

C6T_Lβ1

0.182

0.23

C6T_Lβ3

0.436

0.215

C6T_Hβ1

0.465

0.284

C6T_Hβ2

0.495

0.294

C6T_Dβ1

0.436

0.284

C6T_Dβ5

0.509

0.275

New8T SRAM

0.343

0.329

 

 Fig.7. Data stability in terms of read and hold static noise margin with different threshold voltages                           and β ratioq

Figure 7: Data stability in terms of read and hold static noise margin with different threshold voltages and β ratio



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Write voltage margin is the measure of write ability. The maximum noise voltage necessary to flip the stored bit of the cell, defines the write voltage margin. In this paper the write ability is measured using write trip point. It shows how difficult it is to write to the storing nodes of the cell [7]. The bit-line voltage is swept from 0v to VDD, and the flipping voltage of the cell, when Q and QBAR flip their data is noticed. The value of bit-line voltage at the crossing point of internal storage nodes Q and QBAR represents the write trip point [16]. Table 4 and fig.8 represent the write voltage margin for new 8T SRAM cell and conventional 6T SRAM cell with different threshold voltage and β ratio.

Table 4: Simulation results of write voltage margin

Cell

Write voltage margin (mv)

C6T_Lβ1

600.33

C6T_Lβ3

627.29

C6T_Hβ1

560.59

C6T_Hβ2

571.54

C6T_Dβ1

532.13

C6T_Dβ5

543.07

New8T SRAM

462.93

 

Fig.8. Write voltage margin with different threshold voltages and β ratio

Figure 8: Write voltage margin with different threshold voltages and β ratio

 

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Characterization of New 8T SRAM using MTCMOS Techniques

In this section the new 8T SRAM cell is examined under different β ratio and on different threshold voltages. The parameters taken for the analysis are shown in table 6 and fig. (9 and 10) depicts the pictorial analysis of different parameters.

Table 5: Simulation results on different parameters for new 8T SRAM cell on different threshold voltages and β ratio

Cell

Leakage current   (in amperes)

Leakage power consumption (in watts)

Read access delay (ps)

Write access delay (ps)

RSNM (mv)

HSNM (mv)

Write voltage margin (mv)

New8T_Lβ1

671.22p

805.46p

114.13

38.56

0.343

0.329

462.93

New8T_Lβ3

1.701n

2.041n

113.92

11.56

0.351

0.342

381.05

New8T_Dβ1

3.688µ

4.425µ

114.03

15.87

0.505

0.512

536.51

New8T_Dβ5

5.910µ

7.092µ

114.01

23.31

0.382

0.382

525.56

New8T_Hβ1

2.842p

3.410p

115.20

41.64

0.485

0.484

518.99

 

Fig.9. Simulation results on different parameters for new 8T SRAM cell on different threshold voltages                     and β ratio

Figure 9: Simulation results on different parameters for new 8T SRAM cell on different threshold voltages and β ratio



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Fig.10. Simulation results on leakage current and leakage power consumption for new 8T SRAM                              cell on different threshold voltages and β ratio

Figure 10: Simulation results on leakage current and leakage power consumption for new 8T SRAM cell on different threshold voltages and β ratio

 

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It is noticed here that new 8T SRAM cell using HVT represents less leakage power dissipation as compare to other threshold voltage transistors. The LVT new 8T SRAM circuit at β=3 achieves the fastest write speed due to the low threshold transistors and using pull down transistor width 420nm. The DVT new 8T SRAM circuit with β=1 shows lowest read access delay due to low threshold voltage access transistor. DVT 8T SRAM circuit with β=1 achieves the highest RSNM, HSNM and write voltage margin.

The abbreviations used in table 5 are:

 New8T_Lβ1: low threshold and β ratio is 1,      

New8T _Lβ3: low threshold and β ratio is 3                                                                                     

New8T _Hβ1: high threshold and β ratio is 1,                                                                                

New8T_Dβ1: Dual threshold and β ratio is 1,    

New8T_Dβ5: Dual threshold and β ratio is 5.

Conclusions

The new single ended 8T SRAM cell with low leakage power and high data stability is explored in this paper. The proposed circuit consumes 805.46pW leakage power during idle state of the circuit which is very less as compare to conventional 6T SRAM cell with sleep and hold transistors. The proposed new 8T SRAM cell shows highest noise immunity 0.329mv in hold state. Furthermore, the proposed circuit represents minimum read and write access delays 114.13ps and 38.56ps respectively as compare to conventional 6T SRAM cell. Alternatively proposed single ended 8T SRAM cell with different threshold voltages and β ratio is also evaluated in section 5. That shows some further improvement is possible in terms of leakage current, data stability (RSNM and HSNM) and write voltage margin. The proposed 8T SRAM cell with HVT represents less leakage power dissipation. The LVT new 8T SRAM circuit at β=3 achieves the fastest write speed due to the low threshold transistors and pull down transistor. The DVT new 8T SRAM circuit with β=1 shows lowest read access delay. DVT 8T SRAM circuit with β=1 achieves the highest RSNM, HSNM and write voltage margin.

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