EP0913029A1 - A method and device for continuous-time filtering in digital cmos process - Google Patents

A method and device for continuous-time filtering in digital cmos process

Info

Publication number
EP0913029A1
EP0913029A1 EP97932096A EP97932096A EP0913029A1 EP 0913029 A1 EP0913029 A1 EP 0913029A1 EP 97932096 A EP97932096 A EP 97932096A EP 97932096 A EP97932096 A EP 97932096A EP 0913029 A1 EP0913029 A1 EP 0913029A1
Authority
EP
European Patent Office
Prior art keywords
continuous
pole
cmos process
digital cmos
current
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Withdrawn
Application number
EP97932096A
Other languages
German (de)
English (en)
French (fr)
Inventor
Nianxiong Tan
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Telefonaktiebolaget LM Ericsson AB
Original Assignee
Telefonaktiebolaget LM Ericsson AB
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Telefonaktiebolaget LM Ericsson AB filed Critical Telefonaktiebolaget LM Ericsson AB
Publication of EP0913029A1 publication Critical patent/EP0913029A1/en
Withdrawn legal-status Critical Current

Links

Classifications

    • HELECTRICITY
    • H03ELECTRONIC CIRCUITRY
    • H03FAMPLIFIERS
    • H03F3/00Amplifiers with only discharge tubes or only semiconductor devices as amplifying elements
    • H03F3/34DC amplifiers in which all stages are DC-coupled
    • H03F3/343DC amplifiers in which all stages are DC-coupled with semiconductor devices only
    • H03F3/345DC amplifiers in which all stages are DC-coupled with semiconductor devices only with field-effect devices
    • HELECTRICITY
    • H03ELECTRONIC CIRCUITRY
    • H03HIMPEDANCE NETWORKS, e.g. RESONANT CIRCUITS; RESONATORS
    • H03H11/00Networks using active elements
    • H03H11/02Multiple-port networks
    • H03H11/04Frequency selective two-port networks
    • HELECTRICITY
    • H03ELECTRONIC CIRCUITRY
    • H03HIMPEDANCE NETWORKS, e.g. RESONANT CIRCUITS; RESONATORS
    • H03H11/00Networks using active elements
    • H03H11/02Multiple-port networks
    • H03H11/04Frequency selective two-port networks
    • H03H11/0422Frequency selective two-port networks using transconductance amplifiers, e.g. gmC filters
    • H03H11/0427Filters using a single transconductance amplifier; Filters derived from a single transconductor filter, e.g. by element substitution, cascading, parallel connection
    • HELECTRICITY
    • H03ELECTRONIC CIRCUITRY
    • H03FAMPLIFIERS
    • H03F2200/00Indexing scheme relating to amplifiers
    • H03F2200/331Sigma delta modulation being used in an amplifying circuit

Definitions

  • the present invention relates to a method for continuous-time filtering in digital CMOS process and a device for continuous- time filtering in digital CMOS process .
  • US-A-4 , 839, 542 there are disclosed active transconductance .filters, which belong to a filter type which is called a transconductance-capacitance (gm-C) filter.
  • the basic idea is to create poles by using linear capacitors and transconductors.
  • current mirrors are used as active loads for the transconductors and current mirrors are not utilized to create poles for any filtering purposes .
  • the invention relates preferably to the design of continuous- time filters for sampled data systems in digital CMOS processes.
  • a digital CMOS process neither resistors nor linear capacitors are available. Therefore it is not possible or simply not practical to design continuous-time filters using traditional methods.
  • the pole frequency is therefore determined by the transconductance of an MOS transistor and the capacitance seen at its gate.
  • a generalized method of designing continuous-time filters in digital CMOS process and methods of cascading have been proposed to reduce the spread of the pole frequencies.
  • Fig. 1 " is a circuit showing a basic current mirror as a single- pole filter.
  • Fig. ' 2 is a graph showing SPICE simulation results of fig. 1, wherein cascode current mirrors and cascode current sources are used and the capacitor is realized by NMOS transistors.
  • Fig. 3 a and b are circuits showing cascading techniques according to the invention.
  • Fig. 4 is a graph showing SPICE simulation results of fig. 3b, wherein cascode current mirrors and cascode current sources are used and the capacitors are realized by NMOS transistors.
  • the capacitor C 0 1 can be realized by a gate capacitor on chip, or realized by an off-chip capacitor, if the cut-off frequency of the filter is required to be very low.
  • a scaling factor can also be realized within this filter.
  • the pole frequency of the single-pole filter shown in fig. 1 is given by
  • g m0 is the transconductance of the diode-connected transistor M 0 2 and C p0 represents all the parasitics at the gate of transistor M 0 2.
  • the nonlinearities in the transconductances do not introduce distortion in the output current as long as the transconductances of M 0 2 and M x 3 are matched or constantly rationed.
  • nonlinearities in the capacitance can introduce error in the output current .
  • the gate capacitance is highly nonlinear across the whole operation region, in a current mirror configuration as shown in fig. 1, the gate voltage change is quite limited, making the transistors operate in a well specified region all the time. Therefore, the gate capacitance does not vary dramatically and the linearity is acceptable. When external capacitors are used, linearity can also be guaranteed.
  • the transconductance of a transistor is dependent of the drain current, i.e.,
  • ⁇ n is the channel charge mobility
  • C ox is the unit gate capacitance
  • W/L is the transistor size
  • i D is the drain current. Therefore, when the drain current in transistor M 0 2 changes accommodating input current I 0 , the transconductance g ra0 changes, making the pole frequency change.
  • the SPICE simulation results when the input current changes between ⁇ 0 , 5 I bias0 .
  • circuit of fig. 1 is a single-pole system, having 20 dB/dec frequency roll-off. And the change in the 3-dB frequency is well in line with the prediction given by the equation of transconductance. The change in the pole frequency also introduces distortion, when the input signal frequency approaches the cut-off frequency, in that a different input amplitude experiences a different attenuation.
  • the simulated total harmonic distortion is about -50 dB, when the input is a 100 Khz sinusoidal with amplitude equal to one- fourth of the bias current. When the input frequency decreases to 10 Khz, the total harmonic distortion is less than -70 dB . When the input frequency is larger than the cut-off frequency, the total harmonic distortion is attenuated by the filter itself .
  • the change in the drain current is needed to be as small as possible.
  • One way to do so is to limit the input current compared with the bias current. This is very power consuming.
  • proper cascading realizing higher-order filters can reduce the variation in the pole frequencies.
  • cascading of current mirrors can be used.
  • a single- pole system only gives a 20-dB/dec roll-off. In many applications, sharper cut-off is needed.
  • Cascading two single- pole systems realizes a two-pole system having a 40-dB/dec roll- off. Sharper cut-off can be realized by cascading more stages. There are two possibilities of cascading as shown in fig. 3a and b.
  • the use of cascading shown in fig. 3a results in lower power consumption due to the use of the p-type branch.
  • the n-type branch "1" consists of n-type transistors M0 6 and Ml 7, capacitor C 0 8 and bias current IbiasO 9 for transistor M0 6.
  • the p-type branch "2" consists of p-type transistors M2 10 and M3 11 capacitor C 1 12 and bias current Ibiasl 13 for M3 11.
  • the n-type branch is similar to the one shown in fig. 1 except that the bias current for Ml 7 is omitted due to the use of the p- type branch.
  • Transistors Ml 7 and M2 10 bias each other.
  • the p- type branch is the same as the n-type except p-type transistors are used.
  • this kind of cascading influences the pole frequencies.
  • input current I 0 is positive
  • the drain current in M 0 6 increases making its transconductance to increase. Therefore, the pole frequency determined by the transconductance of M 0 6 and capacitor C 0 8 will increase.
  • the drain current in M 2 10 equal to the drain current of M 7, increases as well making its transconductance to increase. Therefore, the pole frequency determined by the transconductance of M 2 10 and the capacitance of C ⁇ 12 will increase as well .
  • the combined effect is that the pole frequencies vary more rapidly as the input current varies.
  • the cascading technique shown in fig. 3 b results in more power consumption due to an extra n-type branch. It consists of two n- type branches "1" and "2" , which are exactly the same as the one shown in fig. 1.
  • it has a big advantage stabilizing the pole frequencies.
  • input current I 0 is positive
  • the drain current in M0 6 increases making its transconductance increase. Therefore, the pole frequency determined by g m0 /C 0 will increase.
  • the drain current in M 2 10 decreases making its transconductance decrease. Therefore, the pole frequency determined by will decrease.
  • the combined effect is that the variations in the two pole frequencies tend to reduce the total variation.
  • the circuit of fig. 3b is a two-pole system, having 40-dB/dec frequency roll-off. And the change in the variation in the 3-dB frequency is reduced considerably.
  • the simulated total harmonic distortion is less than - 60 dB, when the input is a 100 Khz sinusoidal with amplitude equal to one-fourth of the bias current.
  • the total harmonic distortion is less than -80 dB.
  • the total harmonic distortion is attenuated by the filter itself.

Landscapes

  • Engineering & Computer Science (AREA)
  • Power Engineering (AREA)
  • Networks Using Active Elements (AREA)
  • Amplifiers (AREA)
EP97932096A 1996-07-19 1997-06-27 A method and device for continuous-time filtering in digital cmos process Withdrawn EP0913029A1 (en)

Applications Claiming Priority (3)

Application Number Priority Date Filing Date Title
SE9602824A SE508697C2 (sv) 1996-07-19 1996-07-19 Förfarande och anordning för tidskontinuerlig filtrering i digital CMOS-process
SE9602824 1996-07-19
PCT/SE1997/001169 WO1998004038A1 (en) 1996-07-19 1997-06-27 A method and device for continuous-time filtering in digital cmos process

Publications (1)

Publication Number Publication Date
EP0913029A1 true EP0913029A1 (en) 1999-05-06

Family

ID=20403437

Family Applications (1)

Application Number Title Priority Date Filing Date
EP97932096A Withdrawn EP0913029A1 (en) 1996-07-19 1997-06-27 A method and device for continuous-time filtering in digital cmos process

Country Status (10)

Country Link
EP (1) EP0913029A1 (zh)
JP (1) JP2000514980A (zh)
KR (1) KR20000065251A (zh)
CN (1) CN1108658C (zh)
AU (1) AU3563797A (zh)
CA (1) CA2260915A1 (zh)
HK (1) HK1021595A1 (zh)
SE (1) SE508697C2 (zh)
TW (1) TW349264B (zh)
WO (1) WO1998004038A1 (zh)

Families Citing this family (7)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
WO2011004512A1 (ja) * 2009-07-08 2011-01-13 パナソニック株式会社 フィルタ回路及びこれを備えた光ディスク装置
US8502597B2 (en) * 2009-10-21 2013-08-06 Qualcomm, Incorporated Low-pass filter design
US20140010783A1 (en) 2012-07-06 2014-01-09 Hoffmann-La Roche Inc. Antiviral compounds
KR20150109451A (ko) 2013-01-23 2015-10-01 에프. 호프만-라 로슈 아게 항바이러스성 트라이아졸 유도체
RU2015136256A (ru) 2013-03-05 2017-04-10 Ф. Хоффманн-Ля Рош Аг Противовирусные соединения
CN104679095A (zh) * 2015-02-15 2015-06-03 格科微电子(上海)有限公司 电流源及其阵列、读出电路及其控制方法、放大电路
US11296678B1 (en) * 2020-12-29 2022-04-05 Qualcomm Incorporated Complementary current-mode biquad with high linearity

Family Cites Families (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US4839542A (en) * 1984-08-21 1989-06-13 General Datacomm Industries, Inc. Active transconductance filter device
US4686487A (en) * 1986-07-28 1987-08-11 Commodore Business Machines, Inc. Current mirror amplifier
EP0600141B1 (en) * 1992-10-30 1997-03-05 SGS-THOMSON MICROELECTRONICS S.p.A. Transconductor stage
WO1995006977A1 (en) * 1993-09-02 1995-03-09 National Semiconductor Corporation Active impedance termination

Non-Patent Citations (1)

* Cited by examiner, † Cited by third party
Title
See references of WO9804038A1 *

Also Published As

Publication number Publication date
JP2000514980A (ja) 2000-11-07
WO1998004038A1 (en) 1998-01-29
HK1021595A1 (en) 2000-06-16
SE9602824L (sv) 1998-01-20
CN1225759A (zh) 1999-08-11
SE9602824D0 (sv) 1996-07-19
SE508697C2 (sv) 1998-10-26
KR20000065251A (ko) 2000-11-06
AU3563797A (en) 1998-02-10
CN1108658C (zh) 2003-05-14
TW349264B (en) 1999-01-01
CA2260915A1 (en) 1998-01-29

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