Insulated gate bipolar transistor

Active solid-state devices (e.g. – transistors – solid-state diode – Field effect device – Having insulated electrode

Reexamination Certificate

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Details

C257S328000, C257S133000, C257S139000

Reexamination Certificate

active

06563170

ABSTRACT:

This application relies for priority upon Korean Patent Application No. 97-54216, filed on Oct. 22, 1997, the contents of which are herein incorporated by reference in their entirety.
BACKGROUND OF THE INVENTION
1. Field of the Invention
The present invention relates to a semiconductor device and a method of manufacturing the same, and more particularly, to an insulated gate bipolar transistor (IGBT) and a method of manufacturing the same.
2. Description of the Related Art
Recently, demands have rapidly increased for an inverter used in a logic circuit for a robot or machine tool, an inverter used in industrial electronics as a power device without power failure for office supplies, and an inverter used in a small power converter for the public. In the specific case of a power converter, together with any extension of this application field, the need has increased for a small and light power converter with low noise that provides a high efficiency. However, conventional semiconductor devices such as bipolar junction transistors (BJTs) or a high-power MOS field effect transistors (MOSFETs) cannot satisfy such requirements. Thus, a new semiconductor device has been developed that has both the high-speed switching characteristic of a MOSFET and the high power characteristic of the BJT. This device, an insulated gate bipolar transistor (IGBT), has now become the object of much attention.
The IGBT has a latch-up phenomenon in that the current cannot be controlled by the gate voltage if the current increases. Such latch-up phenomenon is the primary factor for limiting the level of current that enables operation of the IGBT.
In an IGBT having a thyristor structure, if a hole current flowing beneath an n
+
source region formed on a p

well increases, the voltage between the well and the source region is decreased by the resistance of the p

well. If this difference in voltage is over a predetermined level, a parasitic npnp thyristor comes into operation. When the thyristor operates, it provides an electron current to a pnp transistor. Thus, even if the gate voltage is blocked, the current level is increased via the pnp transistor, rather than the pnp transistor turning off. As a result, the temperature of the IGBT increases, leading to the breakdown of the IGBT.
These serial operations refer to the latch-up phenomenon. In order to prevent this latch-up phenomenon, the controllable current level is increased and an accumulated carrier is rapidly removed at the same time for a high-speed operation. This is a key for making the IGBT practical.
On the other hand, when a power semiconductor device is used to drive a motor, a saturation current, which is about 4~5 times higher than the actual operation current, flows if the motor is overloaded. Because of the heat generated by this much current, the efficiency of the emitter in a power semiconductor device increases. As a result, many holes are injected into the semiconductor device, resulting in a latch-up phenomenon. This phenomenon is called a “short circuit current” or a “thermal latch-up”.
Many suggestions have been provided to supply a large current by preventing the above latch-up phenomenon. Particularly, a structure has been widely used in which a p
+
well is formed in a p

well using an ion implantation method. A conventional IGBT having such a structure will be described briefly with reference to
FIGS. 1 through 3
.
FIG. 1
is a layout of a conventional IGBT capable of preventing the latch-up phenomenon.
As shown in
FIG. 1
, reference numeral
100
represents a first mask pattern for forming a gate electrode; reference numeral
110
represents a second mask pattern for forming a p
+
well region to remove the latch-up; reference numeral
120
represents a third mask pattern for forming a n
+
source region; and reference numeral
130
represents a mask pattern for forming a contact hole that connects a metal electrode with the source region and well region formed in a semiconductor substrate, respectively.
FIGS. 2 and 3
are section views of the conventional IGBT shown in
FIG. 1
, cut along line II-II′ and line III-III′, respectively.
Referring to
FIGS. 2 and 3
, an n
+
buffer layer
4
with a high concentration is formed over a p
+
semiconductor substrate
2
. Also, an n

semiconductor layer
6
with a low concentration is grown over the n
+
buffer layer
4
by an epitaxial growth method. A gate electrode
10
made of a polysilicon layer is formed over the n

semiconductor layer
6
while a gate dielectric film
8
is interposed between the gate electrode
10
and the n

semiconductor layer.
A p

well region
12
is formed by impurity ion implantation and thermal diffusion beneath the surface of the n

semiconductor layer
6
, between the gate electrodes
8
. Also, in order to prevent the latch-up, a p
+
well region
14
with a high concentration is formed by ion implantation and thermal diffusion, passing through the center of the p

well region
12
(see
FIG. 2
) and extended to a part of the n

semiconductor layer
6
.
Also, an n
+
source region
16
is formed beneath the surface of the p

well region
12
and the p
+
well region
14
using a mask for the source. A metal electrode
20
used as a cathode is formed on the surface of the n
+
source region
16
and p
+
well region
14
. Here, reference numeral
18
represents a dielectric film for electrical insulation between the metal electrode
20
and the gate electrode
10
.
In the conventional IGBT described above, the resistance between the p

well region
12
and the n
+
source region
16
is decreased by the p
+
well region
14
, which is formed to pass through the p

well region
12
. Thus, the difference in voltage between the source region
16
and the well regions
12
and
14
is decreased, thereby improving the latch-up phenomenon.
However, according to the above conventional IGBT, electron current and hole current both flow in the same direction, collecting in an emitter contact where the metal electrode
20
contacts the n
+
source region (see FIG.
3
). Thus, if the concentration of the p

well region
12
is low, the hole current is multiplied by the resistance of the p

well region, thereby causing a voltage drop in the p

well region
12
beneath the n
+
source region
16
. As a result, it is difficult to prevent the latch-up of the IGBT, and the short circuit current characteristics of this circuit are deteriorated.
SUMMARY OF THE INVENTION
To solve the above problems, it is a first object of the present invention to provide an insulated gate bipolar transistor (IGBT) that is capable of improving the control of latch-up and short circuit current characteristics.
It is a second object of the present invention to provide a method for manufacturing this IGBT.
To achieve the first object, there is provided an insulated gate bipolar transistor (IGBT). In the IGBT, a semiconductor layer of a second conductive type is formed over the semiconductor substrate. A well of the first conductive type is then formed beneath the surface of the semiconductor layer. A source region of the second conductive type is formed in the well and doped with a high concentration. And a gate electrode is formed over the semiconductor layer. The gate electrode only contacts the source region outside of a cathode region in which a contact between the source region and a cathode electrode is formed.
Preferably the IGBT also comprises an impurity region of the first conductive type for controlling latch-up, the impurity region being extended to a part of the primary semiconductor layer via the well. The IGBT may also comprise a highly-doped semiconductor layer of the second semiconductor type, formed over the semiconductor substrate. The IGBT may also comprise an impurity region of the first conductive type for controlling latch-up, the impurity region bei

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