This application claims the priority benefit of Taiwan application serial no. 103143498, filed on Dec. 12, 2014. The entirety of the above-mentioned patent application is hereby incorporated by reference herein and made a part of specification.
1. Field of Invention
The present invention relates to a semiconductor technology, and more particularly to a termination structure and a method of forming the same and a semiconductor device including the termination structure.
2. Description of Related Art
In recent years, high-voltage MOS devices have been widely used in all types of power integrated circuits or smart power integrated circuits. In order to enhance the performance of a device, the operation of a high-voltage MOS device requires a high breakdown voltage and a low on-state resistance (Ron).
The design of a termination structure plays a very important role in improving the breakdown voltage of a semiconductor device. As the level of integration of semiconductor devices is getting increased, the dimension of the same is getting reduced. Therefore, how to maintain or even improve the original breakdown voltage with decreasing the device dimension has become an important topic in the industry.
Accordingly, the present invention provides a termination structure and a method of forming the same and a semiconductor device including the termination structure, in which a single bulk isolation structure is disposed on an epitaxial layer in a termination area, and the profile of the doped region below the single bulk isolation structure can be effectively controlled by the method herein described. Therefore, the breakdown voltage of the device can be easily improved.
The present invention provides a termination structure including a substrate of a first conductivity type, an epitaxial layer of the first conductivity type, a single bulk isolation structure and a bulk doped region of a second conductivity type. The epitaxial layer is disposed on the substrate. The single bulk isolation structure, is disposed on the epitaxial layer. The bulk doped region is disposed in the epitaxial layer below the single bulk isolation structure, wherein a doping depth of the bulk doped region has a graded distribution.
According to an embodiment of the present invention, the doping depth of the bulk doped region is gradually increased toward an active area.
According to an embodiment of the present invention, the single bulk isolation structure has a thickness of about 100 angstroms to 10,000 angstroms.
According to an embodiment of the present invention, the substrate includes silicon, silicon carbide or gallium nitride.
According to an embodiment of the present invention, the single bulk isolation structure is a field oxide layer.
According to an embodiment of the present invention, the first conductivity type is N-type and the second conductivity type is P-type; or the first conductivity type is P-type and the second conductivity type is N-type.
The present invention further provides a method of forming a termination structure. An epitaxial layer of a first conductivity type is formed on a substrate of the first conductivity type. A single bulk isolation structure is formed on the epitaxial layer. A photoresist layer is formed on the single bulk isolation structure, wherein the photoresist layer has a plurality of openings with different widths. An ion implantation process is performed by using the photoresist layer as a mask, so as to form a plurality of doped regions of a second conductivity type in the epitaxial layer below the single bulk isolation structure, wherein doping depths of the doped regions have a graded distribution.
According to an embodiment of the present invention, the doped regions are separate from each other, an i-th doped region is more away from the active area than an (i+1)-th doped region, a doping depth of the i-th doped region is less than a doping depth of the (i+1)-th doped region, and i is a positive integer.
According to an embodiment of the present invention, the method further includes performing an annealing process, so that the doped regions are connected to one another to form a bulk doped region.
According to an embodiment of the present invention, the ion implantation process has a doping energy of about 30 KeV to 1,000 KeV and a doping dose of about 1×1012/cm2 to 100×1012/cm2.
According to an embodiment of the present invention, the widths of the openings in the photoresist layer are gradually increased toward the active area.
According to an embodiment of the present invention, the single bulk isolation structure has a thickness of about 100 angstroms to 10,000 angstroms.
According to an embodiment of the present invention, the single bulk isolation structure is a field oxide layer.
According to an embodiment of the present invention, the first conductivity type is N-type and the second conductivity type is P-type; or the first conductivity type is P-type and the second conductivity type is N-type.
The present invention also provides a semiconductor device including a substrate of a first conductivity type, an epitaxial layer of the first conductivity type, a single bulk isolation structure and a bulk doped region of a second conductivity type. The substrate has a first area and a second area. The epitaxial layer is disposed on the substrate. The single bulk isolation structure is disposed on the epitaxial layer in the first area. The bulk doped region is disposed in the epitaxial layer below the single bulk isolation structure, wherein a doping depth of the bulk doped region is gradually decreased toward the second area.
According to an embodiment of the present invention, the single bulk isolation structure has a thickness of about 100 angstroms to 10,000 angstroms.
According to an embodiment of the present invention, the substrate includes silicon, silicon carbide or gallium nitride.
According to an embodiment of the present invention, the single bulk isolation structure is a field oxide layer.
According to an embodiment of the present invention, the substrate further includes a third area, and the first area is located between the second area and the third area.
According to an embodiment of the present invention, the first area is a termination area, the second area is a seal ring area, and the third area is an active area.
In view of the above, in the method of the invention, a photoresist layer serves as a mask, and ions penetrate through a single bulk isolation structure and into an epitaxial layer to create an ion distribution with gradually changed doping depth. Since the opening sizes of the photoresist layer can be precisely defined, the process window can be widened and the doping profile can be easily controlled, and thus, the breakdown voltage of the device can be significantly improved.
In order to make the aforementioned and other objects, features and advantages of the present invention comprehensible, a preferred embodiment accompanied with figures is described in detail below.
The accompanying drawings are included to provide a further understanding of the invention, and are incorporated in and constitute a part of this specification. The drawings illustrate embodiments of the invention and, together with the description, serve to explain the principles of the invention.
Reference will now be made in detail to the present preferred embodiments of the invention, examples of which are illustrated in the accompanying drawings. Wherever possible, the same reference numbers are used in the drawings and the description to refer to the same or like parts.
Referring to
Thereafter, a single bulk isolation structure 104 is formed on the epitaxial layer 102 in the first area 10. More specifically, the first area 10 merely has a single isolation structure therein, and this isolation structure is a bulk structure without openings or a single-ring structure from a top view. The single bulk isolation structure 104 includes silicon oxide and has a thickness of about 100 angstroms to 10,000 angstroms, e.g. about 1,000 angstroms to 9,000 angstroms, 2,000 angstroms to 8,000 angstroms, 3,000 angstroms to 7,000 angstroms, 4,000 angstroms to 6,000 angstroms, or 5,000 angstroms to 5,500 angstroms. In an embodiment, the single bulk isolation structure 104 includes a field oxide layer. The method of forming the single bulk isolation structure 104 includes forming a mask layer (not shown) on the epitaxial layer 102, and the mask layer has an opening exposing a portion of the epitaxial layer 102. Thereafter, an oxidation process is conducted to grow a field oxide layer in the opening. The mask layer is then removed. In such manner, the surface of the epitaxial layer 102 in the first area 10 is lower than that in the second area 20 or in the third area 30.
Afterwards, a blanket ion implantation process is optionally performed by using the single bulk isolation structure 104 as a mask, so as to form doped regions 105a and 105b of a second conductivity type in the epitaxial layer 102 respectively in the second area 20 and in the third area 30. The doped regions 105a and 105b can be P-type doped regions. In an embodiment, the doped regions 105a and 105b can serve as JFET doped regions for reducing the on-state resistance below the device gate.
Referring to
Referring to
Referring to
As shown in
It is noted that, the method of the invention is relatively competitive since the opening sizes of the photoresist layer and therefore the profile of the formed doped regions can be effectively controlled with the method herein described. In the conventional method, a field oxide layer with openings is used as a mask, but it is difficult to control the opening sizes of the field oxide layer with an etching process. For example, a wet etching may laterally etch so the opening sizes are deviated from targets, and a dry etching may have polymer residues. However, in the present invention, a photoresist layer is used as a VLD mask, and ions then penetrate through the single bulk field oxide layer and into the epitaxial layer to create a VLD ion distribution. The opening sizes of the photoresist layer can be precisely defined, so a wider process window can be provided for mass production.
The termination structure of the invention in the first area 10 is illustrated with reference to
The devices in the second and third areas 20 and 30 are then fabricated. Continue referring to
Referring to
Thereafter, a blanket ion implantation process is performed by using the single bulk isolation structure 104 and the conductive layer 116a and 116b as a mask, so as to form doped regions 118a and 118b of the second conductivity type in the epitaxial layer 102 respectively in the second area 20 and in the third area 30. The doped regions 118a and 118b can serve as P-type body (PB) doped regions. In an embodiment, since the bulk doped region 112 and the body doped regions 118a/118b have different doping concentrations, the conventional method requires to fabricate a photomask and a photoresist layer, and the photoresist layer covers the termination area (i.e. first area 10) to prevent the doping concentration/profile of the bulk doped region 112 from being affected by the doping step of the body doped regions 118a/118b. However, with the method of the invention, the termination area (i.e. first area 10) has been covered by the single bulk isolation structure 104, so a blanket ion implantation process can be conducted to form P-type body doped regions 118a/118b without additional photomask and photoresist layer.
Afterwards, a doped region 120 of the first conductivity type is formed in the doped region 118b in the third area 30. The doped region 120 can be an N-type heavily doped region, serving as the source region of the device.
Referring to
Thereafter, a blanket ion implantation process is preformed, so as to form doped regions 126a and 126b of the second conductivity type respectively in the doped regions 118a and 118b below the openings 124a and 124b. The doped regions 126a and 126b can be P-type heavily doped regions, for reducing the Ohmic resistance of the subsequently formed conductive plugs.
Afterwards, metal layers 128a and 128b are formed on the dielectric layer 122 respectively in the second and third areas 20 and 30. Each of the metal layers 128a and 128b extends onto a portion of the dielectric layer 122 in the first area 10. The metal layers 128a and 128b respectively fill in the openings 124a and 124b and therefore constitute conductive plugs 127a and 127b. The conductive plugs 127a and 127b are electrically connected to the doped regions 126a and 126b, respectively. In such manner, the seal ring structure in the second area 20 is short-circuited to the substrate 100. The semiconductor device of the present invention is thus completed.
The semiconductor device of the invention is illustrated with reference to
The said embodiment in which the first conductivity type is N-type and the second conductivity type is P-type is provided for illustration purposes, and is not construed as limiting the present invention. In another embodiment, the first conductivity type can be P-type and the second conductivity type can be N-type.
In summary, in the method of the invention, a photoresist layer serves as a VLD mask, and ions penetrate through a single bulk field oxide layer and into an epitaxial layer to create a VLD ion distribution. Since the opening sizes of the photoresist layer can be precisely defined, a wider process window can be provided for mass production. The method of the invention can easily control the VLD forming profile and therefore effectively improve the breakdown voltage. In the case of maintaining the same breakdown voltage, a smaller termination area and therefore a smaller device size can be easily obtained.
The present invention has been disclosed above in the preferred embodiments, but is not limited to those. It is known to persons skilled in the art that some modifications and innovations may be made without departing from the spirit and scope of the present invention. Therefore, the scope of the present invention should be defined by the following claims.
Number | Date | Country | Kind |
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103143498 | Dec 2014 | TW | national |