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Microelectronic Circuits, Sixth Edition Sedra/Smith Copyright © 2011 by Oxford University Press, Inc. C H A P T E R 15 Advanced MOS (and Bipolar) Logic Circuits

Capitolo 15 Advanced MOS 2015 - unipv MOS_2015.pdf · 2015-06-03 · For pseudo-NMOS logic inverter, only one additional transistor wil l be needed for each additional gate input

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Page 1: Capitolo 15 Advanced MOS 2015 - unipv MOS_2015.pdf · 2015-06-03 · For pseudo-NMOS logic inverter, only one additional transistor wil l be needed for each additional gate input

Microelectronic Circuits, Sixth Edition Sedra/Smith Copyright © 2011 by Oxford University Press, Inc.

C H A P T E R 15

Advanced MOS (and Bipolar) Logic Circuits

Page 2: Capitolo 15 Advanced MOS 2015 - unipv MOS_2015.pdf · 2015-06-03 · For pseudo-NMOS logic inverter, only one additional transistor wil l be needed for each additional gate input

Microelectronic Circuits, Sixth Edition Sedra/Smith Copyright © 2011 by Oxford University Press, Inc.

Figure 15.1 (a) The pseudo-NMOS logic inverter. (b) The enhancement-load (or saturated-load) NMOS inverter. (c) The depletion-load NMOS inverter.

15.1.1 The pseudo-NMOS Inverter

Page 3: Capitolo 15 Advanced MOS 2015 - unipv MOS_2015.pdf · 2015-06-03 · For pseudo-NMOS logic inverter, only one additional transistor wil l be needed for each additional gate input

Microelectronic Circuits, Sixth Edition Sedra/Smith Copyright © 2011 by Oxford University Press, Inc.

nMOS amplifier with depletion load VTC transfer characteristic

Depletion nMOS always ON

Page 4: Capitolo 15 Advanced MOS 2015 - unipv MOS_2015.pdf · 2015-06-03 · For pseudo-NMOS logic inverter, only one additional transistor wil l be needed for each additional gate input

4

Pseudo-NMOS Logic Circuits

!  Despite many advantages, CMOS suffers from the increased area, and correspondingly increased capacitance and delay as the logic gates becomes more complex.

!  For pseudo-NMOS logic inverter, only one additional transistor will be needed for each additional gate input.

This structure is similar to depleted-load NMOS but with rather improved characteristics. It also has the advantage of being directly compatible with CMOS circuits. PMOS always ON

Figure 15.1 (a) The pseudo-NMOS logic inverter

Page 5: Capitolo 15 Advanced MOS 2015 - unipv MOS_2015.pdf · 2015-06-03 · For pseudo-NMOS logic inverter, only one additional transistor wil l be needed for each additional gate input

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Static Operation of A Pseudo-NMOS Logic Inverter (1)

!  The obvious disadvantage of the inverter is the non-zero VOL for VI=VDD (point E). It causes the static power dissipation to be PD= Istat x VDD.

These 2 parameters approach zero for conventional CMOS inverter.

Figure 15.2 Graphical construction to determine the VTC of the inverter in Fig. 15.1(a).

15.1.2 Static characteristics

kn > kp

Page 6: Capitolo 15 Advanced MOS 2015 - unipv MOS_2015.pdf · 2015-06-03 · For pseudo-NMOS logic inverter, only one additional transistor wil l be needed for each additional gate input

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!  VTC for the pseudo-NMOS inverter.

Figure 15.3 VTC for the pseudo-NMOS inverter. This curve is plotted for VDD = 5 V,

Vtn = −Vtp = 1 V, and r = 9.

Static Operation of A Pseudo-NMOS Logic Inverter (2) 15.1.3 Derivation of the VTC

r =kpkn

=µ pWp

µnWn

same channel length L

Page 7: Capitolo 15 Advanced MOS 2015 - unipv MOS_2015.pdf · 2015-06-03 · For pseudo-NMOS logic inverter, only one additional transistor wil l be needed for each additional gate input

7

Gate Circuit of A Pseudo-NMOS Logic

! 4-input pseudo-NMOS NOR and NAND gates are shown below. Note that each requires only 5 transistors compared to 8 used in complementary CMOS.

! NOR type consumes less area than NAND type. ! Pseudo-NMOS is suited for applications in which the output remains high most of the time.

Figure 15.4 NOR and NAND gates of the pseudo-NMOS type.

NOR NAND

Page 8: Capitolo 15 Advanced MOS 2015 - unipv MOS_2015.pdf · 2015-06-03 · For pseudo-NMOS logic inverter, only one additional transistor wil l be needed for each additional gate input

8

Pass-Transistor Logic Circuits (1)

!  A simple approach for implementing logic functions utilizes series and parallel combinations of switches that are controlled by input variables to connect the input and output nodes.

!  Each of the switches can be implemented either by a single NMOS transistor or by a pair of CMOS transistors connected in CMOS transmission gate configuration.

CMOS transmission gate

Y=AC

Figure 15.5 Conceptual pass-transistor logic gates. (a) Two switches, controlled by the input variables B and C, when connected in series in the path between the input node to which an input variable A is applied and the output node (with an implied load to ground) realize the

function Y = ABC. (b) When the two switches are connected in parallel, the function realized is Y = A(B + C).

Figure 15.6 Two possible implementations of a voltage-controlled switch connecting nodes A and Y: (a) single NMOS transistor and (b) CMOS transmission gate.

Page 9: Capitolo 15 Advanced MOS 2015 - unipv MOS_2015.pdf · 2015-06-03 · For pseudo-NMOS logic inverter, only one additional transistor wil l be needed for each additional gate input

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Operation with NMOS as Switches (1) (IT IS NOT AN INVERTER!!!!)

!  Although switches with single NMOS transistor is a simple circuit, there are serious shortcomings in both static and dynamic performance.

!  For dynamic operation (poor “1”):

The high output voltage (VOH) will not be equal to VDD; rather, it will be lower by Vt, and to make matters worse, the value of Vt can be as high as 1.5 to 2 times Vto (due to body effect).

!  For static consideration, the low value of VOH can cause the Qp of the next CMOS inverter stage to conduct and thus has a finite static current and static power dissipation.

Figure 15.8

Q (NMOS) will stop conducting when vo= VDD-Vt

Page 10: Capitolo 15 Advanced MOS 2015 - unipv MOS_2015.pdf · 2015-06-03 · For pseudo-NMOS logic inverter, only one additional transistor wil l be needed for each additional gate input

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!  Operation of the NMOS switch as the input goes low is shown below.

!  It results in a “good 0”. Note that the drain of an NMOS transistor is always higher in voltage than the source; correspondingly, the drain and source terminals interchange roles in comparison to previous case.

Operation with NMOS as Switches (2) (IT IS NOT AN INVERTER!!!!)

Page 11: Capitolo 15 Advanced MOS 2015 - unipv MOS_2015.pdf · 2015-06-03 · For pseudo-NMOS logic inverter, only one additional transistor wil l be needed for each additional gate input

Operation with CMOS Transmission Gate as Switches (1)

!  Great improvement in static and dynamic performance are obtained when the switches are implemented with CMOS transmission gate.

" Qn will stop conducting when vo= VDD-Vtn # Qp will enter triode region at vo= |Vtp|, but will continue to

conduct until C is fully charged and vo= VDD. $  Qp provides the gate with a good “1”. %  tPLH will be lower than that in the case of single NMOS switch

due to additional current available from Qp. & Additional Qp, however, increases the value of C.

VSG-P=VDD

Page 12: Capitolo 15 Advanced MOS 2015 - unipv MOS_2015.pdf · 2015-06-03 · For pseudo-NMOS logic inverter, only one additional transistor wil l be needed for each additional gate input

Operation with CMOS Transmission Gate as Switches (2)

!  With vI goes from high to low, the output waveform is shown below.

" Qp will cease conduction when vo falls to |Vtp|. # Qn, however, will continue to conduct until C is fully discharged

and vo = VOL = 0V.

! The transmission gates provide far superior performance than single NMOS switches. The price paid is increased circuit complexity, area and capacitance.

Page 13: Capitolo 15 Advanced MOS 2015 - unipv MOS_2015.pdf · 2015-06-03 · For pseudo-NMOS logic inverter, only one additional transistor wil l be needed for each additional gate input

Fig.  5.64    The  CMOS  transmission  gate  with  analog  signal.  

Carico

Segnale  ananalogico  

di  uscita

Segnale  analogico  di  ingresso

vC

Page 14: Capitolo 15 Advanced MOS 2015 - unipv MOS_2015.pdf · 2015-06-03 · For pseudo-NMOS logic inverter, only one additional transistor wil l be needed for each additional gate input

Fig.  5.65    Equivalent  circuits  for  visualizing  the  operaBon  of  the  transmission  gate  in  the  closed  (on)  posiBon:    (a)  vA  is  posiBve;    (b)  vA  is  negaBve.    

NMOS

NMOS

PMOS

PMOS

Page 15: Capitolo 15 Advanced MOS 2015 - unipv MOS_2015.pdf · 2015-06-03 · For pseudo-NMOS logic inverter, only one additional transistor wil l be needed for each additional gate input

vA RL

vo

Switch closed

vA RL

vo

vo =RL

REQ + RLvA

REQ < RL vo – vA Piccola differenza

Tensioni di comando sui gate vGN = +vC vGP = -vC

IP: vA>0; NMOS e PMOS in triodo (NMOS spento Se vo> vC-VTN )

iN ≈ KN 2(vC-vo-VTN) (vA-vo) RonN=(vA-vo)/iN 1/RonN=2KN (vC-vo-VTN)

iP ≈ KP 2(vA+vC-|VTP|) (vA-vo) RonP=(vA-vo)/ip 1/RonP=2KP (vA+vC-|VTP|)

REQ = RonN//RonP =[2KN (vC-vo-VTN) + 2KP (vA+vC-|VTP|)]-1

Se KN=KP=K VTN=|VTP|=VT allora REQ = [4K (vC-VT+vA-vo)]-1

REQ = RonN//RonP

Page 16: Capitolo 15 Advanced MOS 2015 - unipv MOS_2015.pdf · 2015-06-03 · For pseudo-NMOS logic inverter, only one additional transistor wil l be needed for each additional gate input

Variation in the REQ of a Transmission Gate as input signal is varied. (NMOS and PMOS un-matched)

REQ

vA(vo)

REQ = RonN//RonP