Page 44 - Power Electronics Handbook
P. 44

The IGBT   37

                      The on-resistance (T~s(~~)) the device is given by  equation (1.13),
                                               of
                    where Rfb is the  resistance of  the channel beneath the gate; Re, is  the
                    resistance of  the substrate, solder connections, leads and package; and Rbk
                    is the resistance between the two p layers and the drain, through the body
                    of the vertical transistor.
                      TDS(ON)  = Rbk  -I- Rch + Rex                            (1.13)
                      The channel and external resistances are constant but the bulk resistance
                    increases  with  the  breakdown  voltage  of  the  device.  Therefore  the
                    on-resistance will also increase as the breakdown voltage capability of  the
                    transistor increases. To avoid this, large chips are constructed using many
                    identical  parallel  cells,  which  give  a  low  on-resistance  and  a  high
                    breakdown voltage.
                      The  shorter  the  gate  channel  in  a  unipolar  device,  the  higher  the
                    transconductance and the lower the parasitic capacitance. The maximum
                    frequency of operation cfmu) is given by equation (1.14), where W, is the
                    length of  the channel in micrometres and V, is the camer velocity in cds.

                                                                               (1.14)
                      Figure 1.21(b) shows a short-chamel arrangement which is formed byp
                    and  n diffusions,  hence  it  is  often  called  a  double-diffused (DMOS)
                    transistor. As  the  drain-source voltage  is  increased the depletion layer
                    spreads into the drain drift region since it is lightly doped. Since the drain
                    drift  region  is  increased  the  breakdown  voltage  is  higher,  but  the
                    drain-source resistance also increases. This can be reduced by using several
                    parallel cells on the semiconductor die.
                      Figure  1.21(c) shows part  of the  short-channel transistor  of  Figure
                    1.21(b), with an illustration of the parasitic components. The action of the
                    parasitic transistor is usually avoided by a metal contact which bridges the
                    source  and  the  body,  i.e.  the  base  and  the  emitter  of  the  parasitic
                    transistor. Therefore theoretically this transistor should be off, but since
                    the ohmic p layer puts a resistance into the base of this transistor it is
                    possible to turn it on, for example via the parasitic capacitance (C,) which
                    can destroy the device. The parasitic capacitance is formed by the p base
                    and  the  n drift  region.  The  parasitic  diode  is  useful  when  switching
                    inductive loads.
                      The V-groove MOSFET or VMOS device, is shown in Figure 1.21(e). Its
                    operation is  identical to  the DMOS structure except  that  it  is  a  vertical
                    structure, and there are now two parallel paths down to the drain. The metal
                    gate shown in the figure is also usually replaced by  a silicon gate.

                    1.7 The IGBT
                    The insulated gate bipolar transistor (IGBT) is a hybrid device which aims to
                    combine the benefits of  power MOSFETs, such as low input current drive
                    and wide safe operating area, with the advantages of bipolar transistors, such
                    as low saturation voltage (IR, 1992; Goodenough, 1994; Bush, 1996). Figure
                    1.22 shows the basic construction of  this device, with its equivalent circuit
                    and symbol.
   39   40   41   42   43   44   45   46   47   48   49