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Analog Integrated Circuits Fundamental Building Blocks Fundamental Building Blocks Current mirrors Faculty of Electronics Telecommunications and Information Technology Information Technology Gabor Csipkes Bases of Electronics Department


  1. Analog Integrated Circuits Fundamental Building Blocks Fundamental Building Blocks Current mirrors Faculty of Electronics Telecommunications and Information Technology Information Technology Gabor Csipkes Bases of Electronics Department

  2. Outline  current source biasing – voltage sources  MOS transistor current mirrors  fundamental current mirror  fundamental current mirror  cascode current mirror  low swing cascode current mirror  unbalanced and symmetrical Wilson current mirrors  bipolar transistor current mirrors  fundamental current mirror  fundamental current mirror with β compensation  fundamental current mirror with resistive emitter degeneration  fundamental current mirror with resistive emitter degeneration  cascode current mirror  unbalanced and symmetrical Wilson current mirrors Analog Integrated Circuits – Fundamental building blocks – Current mirrors 2

  3. Current mirrors – principles of operation  integrated current sources with transistors need bias voltages → voltage sources 1 g R R m in out 1: n Is this a voltage Current mirror source?  key parameters to consider:  input resistance → must be as small as possible → current input  input resistance → must be as small as possible → current input  output resistance → must be as large as possible → current output  minimum required output voltage  required input voltage  current gain → precision imposed by the application Analog Integrated Circuits – Fundamental building blocks – Current mirrors 3

  4. The fundamental MOS current mirror NMOS PMOS Small signal model V 1 V     R in R out r    V V V V V in out DS 2 I g I in DSat 1 Th o min DSat 2 in m 1 out         1 V     V V 1 V I I   n n out out     2 2 GS GS Th Th 2 2 DS DS 2 2 n n out out  current gain :  current gain :      1 V     I V V 1 V in in 1 GS Th 1 DS 1    2 V  Δ β – geometry mismatch    n 1 Th  2 V  Δ V Th – threshold voltage mismatch DSat Analog Integrated Circuits – Fundamental building blocks – Current mirrors 4

  5. The MOS cascode current mirror NMOS PMOS     V V V V V in DSat 3 Th 3 DSat 1 Th 1   f V BS 3    V V V V (!) o min DSat 4 DSat 2 Th 2 1 1 1 1   R in g g m 1 m 3       R r r g g r r out DS 2 DS 4 m 4 mb 4 DS 2 DS 4 Small signal model Analog Integrated Circuits – Fundamental building blocks – Current mirrors 5

  6. The MOS cascode current mirror  the V GS voltages of M 3 and M 4 balance the fundamental mirror M 1 -M 2 → n is accurately defined    V V V V in in out out DS DS 1 1 DS DS 2 2 V V DS 2 DS 1 The current gain is very close to unity even when the input- output voltage imbalance Δ V is significant Analog Integrated Circuits – Fundamental building blocks – Current mirrors 6

  7. The MOS low swing cascode current mirror  the cascode current mirror is not optimal in terms of V omin → the gate voltage of M 4 must be decreased by V Th 2 1  V 2 V o min DSat V G 4 V G 4  V V DS 1 DS 2 4 3   V V V DS 1 DS 2 R R triode region Analog Integrated Circuits – Fundamental building blocks – Current mirrors 7

  8. The MOS low swing cascode current mirror NMOS PMOS   V V V in DSat 1 Th 1   V V V o min DSat 4 DSat 2 1 R   R in g m 1       R r r g g r r out DS 2 DS 4 m 4 mb 4 DS 2 DS 4 Small signal model Analog Integrated Circuits – Fundamental building blocks – Current mirrors 8

  9. The Wilson current mirror NMOS PMOS     V V V V V in DSat 3 Th 3 DSat 2 Th 2    V V V V o min DSat 3 DSat 2 Th 2   g g g g   R R m m 2 2 m m 3 3 in g g m 1 m 3 g g r r  R m 1 m 3 DS 1 DS 3 out g m 2 Small signal V in and V out create voltage imbalance model model between V between V DS 1 and V DS 2 and V Accuracy issues for the current gain n Analog Integrated Circuits – Fundamental building blocks – Current mirrors 9

  10. The balanced Wilson current mirror NMOS PMOS     V V V V V in DSat 3 Th 3 DSat 2 Th 2    V V V V o min DSat 3 DSat 2 Th 2   g g g g   R R m m 2 2 m m 3 3 in g g m 1 m 3 g g r r  R m 1 m 3 DS 1 DS 3 out g m 2 Small signal model Analog Integrated Circuits – Fundamental building blocks – Current mirrors 10

  11. The fundamental bipolar current mirror NPN PNP   V V V V in BE 1 o min CE 2 1   R R r in out CE 2 g m 1             I I V V V V I I V V 2 1       S S 2 2 1 1 CE CE 2 2 CE CE 1 1     n n S S 2 1    I V V  I V V      S 1 CE 1 EA  current gain : n S 1 in EA    1 I V V    1 S 2 1 CE 2 CE 1       I I V V     n S 2 S 1 CE 1 EA   I 2  Δ V – input-output voltage imbalance S 1 Analog Integrated Circuits – Fundamental building blocks – Current mirrors 11

  12. The fundamental current mirror with β compensation NPN PNP 1    V V V V V  R  R r o min CE 2 in BE 1 BE 3 in g out CE 2 m 1  current gain → β replaced by β ( β +1) → n much closer to the ideal value when the  current gain → β replaced by β ( β +1) → n much closer to the ideal value when the input and the output are balanced in voltage        1  I I V     n S 2 S 2 n 1          I 1 2 I V V   S 1 S 1 in EA Analog Integrated Circuits – Fundamental building blocks – Current mirrors 12

  13. The degenerated fundamental current mirror NPN PNP 1   R R    R r R g r R     in 1 V V I R V V I R out CE 2 2 m 2 CE 2 2 g in BE 1 in 1 o min CE 2 out 2 m 1 R  n 1       V V I R I R V V I I R R  current gain :  current gain : R R BE BE 1 1 in in 1 1 BE BE 2 2 out out 2 2 2  remember to adjust the emitter areas of Q 1 and Q 2 A I R    2 S 2 1 n proportionally with the current in each branch !!! A I R 1 S 1 2  n is still affected by the finite β and by Δ V Analog Integrated Circuits – Fundamental building blocks – Current mirrors 13

  14. The bipolar cascode current mirror NPN PNP g r r r  1 1 R m 4 CE 4 CE 2 BE 4   R     out   V V V V V V g in in BE 1 BE 3 o min CE 4 BE 2 g g   r r 1 m 2   m 1 m 3 BE 4 CE 2 g   m 1  current gain → β influences the accuracy while the  2 I   n S 2 fundamental mirror Q 1 -Q 2 is balanced by the cascode     2 I 4 2 transistors Q 3 -Q 4 S 1 Analog Integrated Circuits – Fundamental building blocks – Current mirrors 14

  15. The bipolar Wilson current mirror asymmetrical balanced     V V V V V V  current gain → β influences the accuracy o min CE 4 BE 2 in BE 1 BE 3 while the fundamental mirror Q 1 -Q 2 is    r g g balanced by the cascode transistors Q 3 -Q 4   BE 3 m 2 m 3 R R in in   g g g g g g r r m 2 m 1 m 3 BE 3    2 I 2   n S 2 r  g g r r CE 1     2 I 4 2 m 1 m 3 CE 1 CE 3 S 1 r  R BE 3 out   r r   g 1 CE 1 g CE 1   m 2 m 1 r r   BE 3 BE 3 Analog Integrated Circuits – Fundamental building blocks – Current mirrors 15

  16. Bibliography  P.E. Allen, D.R. Holberg, CMOS Analog Circuit Design , Oxford University Press, 2002  B. Razavi, Design of Analog CMOS Integrated Circuits , McGraw-Hill, 2002  D. Johns, K. Martin, Analog Integrated Circuit Design , Wiley, 1996  P.R.Gray, P.J.Hurst, S.H.Lewis, R.G, Meyer, Analysis and Design of Analog Integrated Circuits , Wiley,2009  R.J. Baker, CMOS Circuit Design, Layout and Simulation , 3 rd edition, IEEE Press, 2010 Analog Integrated Circuits – Fundamental building blocks – Current mirrors 16

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