1986 steyaert novel cmos schmitt trigger.pdf

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  • 8/18/2019 1986 steyaert novel CMOS Schmitt trigger.pdf

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    tions (3 /im and 5 /im) and three electrode widths (1 /im, 2 /im

    and 3  fitn),  the device areas were adjusted to obtain the target

    capacitance values. A typical frequency response is depicted in

    Fig.

      2

      I/V characteristic of MIL PIN device

    Fig. 3. The 3 dB roll-off frequency n ear 8 G H z ap pears to be

    limited by the carrier transit time rather than the electrode

    capacitance. This observation is also consistent with the

    anticipated roll-off frequency of our largest detectors. (With

    220 fF capacitances and 50 Q load resistances, the theoretical,

    RC

      time-con stant-limited ba ndw idth is 14 GH z.) Althou gh it

    is possible to attain even larger detector geometries without

    affecting ou r observe d 3 dB roll-off po int, th e limited real

    estate available on an IC chip tends to discourage the devel-

    opment of extremely large detector areas

    (> 200 ;im x 200/^m).

    Fig.  3

      Typical frequency response from 2 G Hz to 8 GHz

    Lo g of am plitud e response is 5 dB/d iv and reference level is set at

    —10 dB. 5 dB fluctuations app aren t in res ponse curve between

    3 GH z and 7 GH z are believed present because packaging has not

    been optimised

    In summary, a detector design which can be implemented

    on a substrate in common with other IC components allows

    the fabrication of detector/amplifier ICs. We have demon-

    strated than an interdigitated MIL PIN device meets this

    requirement without sacrificing the desirable features of high

    speed and large detection area.

    D.

      J. JACKSON

      16th

     December

      1985

    D.  L. PERSECHINI

    Hughes Research Laboratories

    Malibu, CA 90265, USA

    References

    1   SLAYMAN,  c. w., and   FIGUEROA, L. :

      IEEE Electron Device L ett.,

    1981,  EDL-2 p. 112; SUGETA, T.,  an d   URISU, T.:

      IEEE Transactions

    Electron Devices,

     ED-26 1979, 1855

    2   FORREST,  s. R.:

      J. Lightwave Technol.,

      1985,  LT3 p. 347

    3   DIADIUK,   v., and  GROVES, S. H.:

      Appl. Phys. Lett.,

      1985, 46, p. 157

    NOVEL CMOS SCHMITT TRIGGER

    Indexing terms: Semicondu ctor devices and materials, MOS

    structures and devices

    A novel CMOS Schmitt trigger circuit has been realised,

    using only five MOS transistors. The circuit always guar-

    antees hysteresis, even with very large process variations. The

    switching speed of the new Schmitt trigger is higher, com-

    pared to previously reported CMOS Schmitt triggers.

    Introduction:  The Sch mitt trigger is a circuit that converts a

    varying voltage into a stable logical signal (one or zero). The

    DC transfer characteristic needs hysteresis to reduce the sensi-

    tivity to noise and disturbances. In many applications it is

    necessary to control the hysteresis width from a few tens of

    millivolts, up to volts. In the new Schmitt trigger circuit, this

    hysteresis voltage is controlled by the dimension of only one

    transistor. Even if the hysteresis voltage has been chosen very

    small, the hysteresis is always guaranteed even under large

    process variations.

    The Schmitt trigger circuit:   The integration of a CMOS

    Schmitt trigger requires special circuits to cancel the resistors

    commonly used in discrete Schmitt triggers.

    1

      In Fig. la a

    commonly used CMOS Schmitt trigger is shown,

    2

     

    3

      and in

    Fig.  \b  the new CMOS Schmitt trigger. The new Schmitt

    out

    rfC

     d d

     int

    M,M,

     o ut

    4

    Fig.  1

    a

      Commonly used Schmitt trigger circuit

    b

      New Schmitt trigger circuit

    trigger consists of two invertors (M

    1 ;

      M

    2

      and M

    4

    , M

    5

    ) and an

    extra feedback transistor (M

    3

    ). It is this extra transistor that

    always guarantees the hysteresis of the Schmitt trigger.

    If  V

    in

     = V

    ss

    in t

      is high and 

    ou t

      is low. It means that tran-

    sistor M

    3

      is off. If   V

    in

      increases, the first invertor (M,, M

    2

    ) will

    switch with a threshold voltage  V

    Oi

    )  defined by the transistors

    M, and M

    2

    :

    1 +  m

    (1)

    with

    l k

    p

     W/L)l\

    where l^

    n

    , ^

    p

      are the threshold voltages and

      k

    n

    , k

    p

      are the

    transconductance parameters of the  NMOS   and   PMOS   t ran-

    sistors, respectively. If the first inverter is switching, the second

    inverter (M

    4

    , M

    5

    ) will be switching as well. It means that M

    3

    ELECTRONICS LETTERS  13th February 1986 Vol. 22 No. 4

    20 3

  • 8/18/2019 1986 steyaert novel CMOS Schmitt trigger.pdf

    2/3

    is switched on, and will generate positive feedback

      V

    int

    decrease—> 

    ou t

      increase—• M

    3

      is more on—• V

    im

      decreases

    more—* ..

     .)•

     From this moment on the Schmitt trigger is in the

    other state.

    If  v

    in

     =  V

    dd

    in t

      is low and 

    ou t

      is high. It means that tran-

    sistor M

    3

     is now switched on, and works as a current source.

    To switch the first inverter the threshold voltage  V

    l0

      has to be

    lower than  V

    01

      to compensate for this extra current sink from

    transistor M

    3

    , or

    k

    p

     = 15-2

    v  —  v —

    2(1 + m)

     2)

    with

    n  =

    k

    n

     W/L)3\

    UW QlJ

    As soon as the input voltage is lower than  V

    l0

    ,  again positive

    feedback switches the Schmitt trigger to the other state.

    The hysteresis voltage of this Schmitt trigger is given by the

    second part of eqn. 2 and can be controlled by  W/L)  of tran-

    sistor M

    3

    . As can be seen, there is always a hysteresis even

    with large variations in dimensions  {W/L  ratio) or process

    variations  k

    n

    , k

    p

    tn

     and

      V

    tp

    ).

     If, for example, the parameter of

    transistor  M

    3

     k

    n

     W/L)3)  is reduced by 50%, the hysteresis

    width will be 30% reduced, but the hysteresis is still present

    even if the hysteresis width is designed to be few tens of milli-

    volts.  In the previously reported CMOS Schmitt trigger, such

    a large variation in one of the transistors M

    l 5

      M

    3

    , M

    5

      or M

    6

    would cause the hysteresis to disappear if this is designed to

    be smaller than 500 mV.

    The advantage of this new circuit, compared with pre-

    viously reported Schmitt triggers, is the higher switching

    speed. This switching speed is limited to the slew rate of the

    internal node  V

    int

    ).  The slew rate is defined by the current

    available divided by the load capacitor (C

    t

    ). In this circuit

      C

    l

    is only the gate-source capacitor

      C

    gs

    )

      of the next inverter

    (only two transistors) and the drain-bulk capacitor

      C

    db

    ),

    which in this case is negligible. In the Schmitt trigger of

    Fig.

      la  C

    x

      is given by four  C

    gs

      values, whereby the extra two

    transistors need to be very large for practical use, which

    causes large values of C

    gs

    .  It means that in the first order the

    switching speed of the new circuit is more than two times

    higher for the same current consumption.

    CMOS realisation and measurements: The new circuit has been

    designed in a 3 /zm CMOS process. The design specifications

    for the threshold voltages were: K

    01

      = 2-5 V and

      V

    l0

      = 2 V.

    The transistor dimensions are given in Table

      1.

     The circuit has

    Table 1

      DIMENSIONS OF TRANSISTORS IN

    DESIGNED NEW SCHMITT TRIGGER

    W/L

    M

    t

    M

    2

    M

    3

    M

    4

    M

    5

    5/7

    5/18

    5/40

    5/7

    5/18

    been extensively simulated in SPICE level 2. In Fig. 2 the DC

    transfer and the AC transfer curve of 

    in t

     and 

    ou t

     are given. As

    can be seen, the threshold voltages are  V

    Ql

     = 2-5 V and  V

    l0

      =

    21 V. The delay with a load of 200 fF is about 65 ns. In

    Fig.  3 a microphotograph of the circuit is given. The Schmitt

    trigger is used to realise a PDM- PPM convertor. In Fig. 4

    measurement results of the integrated Schmitt trigger are

    shown. The input signal is a triangular wave. Out of this

    measurement, the threshold voltages were deduced to be

    V

    0l

      = 2-48 V and  V

    l0

      = 1-8 V (spread  a = 50 mV). The differ-

    ences between measurements and the simulations are mainly

    found in the used threshold voltages. The results of a SPICE

    simulation using the extracted transistor parameters and

    threshold voltages of that run are:  V

    0l

      = 2-56 V and  V

    l0

      =

    1-82 V  V

    tn

      = 0-7 V,  V

    tp

     = 0-78 V,  k

    n

     = 40-7

      p

    /iA/V). The measured performance of the new Schmitt trigger

    compares very well with the simulation.

    Fig.

     2

      Simulated DC and AC transfer curve of Schmitt trigger

    Fig.

     3

      Microphotograph of designed Schmitt trigger

     

    Fig.

     4

      Measured transfer curve of designed Schmitt trigger

    Conclusion: A new CMOS Schmitt trigger has been designed

    and measured. The relations to calculate the threshold volt-

    ages and the hysteresis width are described. The hysteresis of

    this new Schmitt trigger is always guaranteed, even with very

    large process variations. From the measurements, it is shown

    that the new structure has a very excellent performance with a

    very simple circuit.

    M. STEYAERT*

    W.

      SANSEN

    Katholieke Universiteit Leuven

    Departement Elektrotechniek-Ajdeling

      E.S.A.T.

    Kardinaal Mercierlaan 94

    B-3030

      Heverlee, Belgium

      Supported by the Belgium IWONL

    6th December

     1985

    204

    ELECTRONICS LETTERS

      13th

     February

     1986 Vol. 22 No. 4

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     eferen es

    1  RIDDERS,  'Accurate determination of threshold voltage levels of a

    Schmitt  trigger',

     IEEE Trans.,

      1985,

     CAS-32

    2

      BRANKO,

      'Modified CMOS

     invertors , Microelectron. J.,

      1983, 14

    3

      NAGARAJ, SATYAM,

      'Multistage monostable multivibrator using

    load coupled  regenerative feedback',

     Electron. Lett.,

      1981, 17, pp.

    159 160

    EFFICIENT

      RQ TECHNIQUE USING SOFT

    DEMODULATION

    Indexing  terms:

      Codes,

     Demodulation

    In

      the letter a new technique for increas ing the efficiency of

    an  automatic-repeat-request communication system is

    described.

      This technique uses all the received versions of a

    codeword,

      and also those versions containing

      errors.

      Such a

    strategy,  together with a soft demodulation of each received

    symbol ,  is particularly efficient when applied to ARQ

    schemes

      in which each block erroneously received is

    retransmitted

      many

      times.

    Automatic-repeat-request (ARQ) techniques are widely used

    to improve the reliability of communication systems using

    many types of practical channel. 'Stop-and-wait', 'go-back-JV'

    and 'selective ARQ' schemes are the best known methods.

    1

    '

    2

    Stop-and-wait and go-back-iV schemes present a lower imple-

    mentation cost with respect to the selective scheme; on the

    other hand, their efficiency falls rapidly with the increase in

    the channel error probability.

    Sastry

    3

      proposed a modification of the classical stop-and-

    wait and go-back-N schemes to increase the throughput by

    reducing the wasted time spent in the waiting or in the

    retransmission state. Each new codeword

      c

     is first transmitted

    only once, while it is repeated  i  times when a repeat request is

    received. Recently, a continuous ARQ scheme has been pro-

    posed by Moeneclaey and Bruneel,

    4

      in which each block is

    always transmitted  N  times, where N  is the number of blocks

    which can be transmitted during the round-trip delay.

    In this letter it is shown that the performance of the

    previous ARQ schemes, in which the same codeword is

    retransmitted many times, can be significantly improved by

    introducing a soft decision demodulation.

    5

    A signal having amplitude  d

    m

    A  is used to transmit the

    binary symbol  d

    m

      d

    m

     — ±

      1).

      Each information-bearing

    sequence of k symbols is encoded into a codeword  c through a

    code of type (n, k).  The positive signal region (0 — A)  is lin-

    early quantised in  n

    L

      levels; the quantisation step is  d =

    2A/ 2n

    L

      —  1); the upper level lies between  A  —  d/2) and

      +00.

    Similarly,  n

    L

      levels are defined for the negative signal region.

    With the /th quantisation positive level, the integer / is associ-

    ated, and with the /th negative level, the integer —/. We

    denote by r

    jt

     m

      t), for 1