This application claims the priority benefit of Taiwan application serial no. 112119698, filed on May 26, 2023. The entirety of the above-mentioned patent application is hereby incorporated by reference herein and made a portion of this specification.
The embodiments of the present disclosure relate to an integrated circuit and a method of fabricating the same, and particularly to a semiconductor device and a method of fabricating the same.
Transistors are indispensable electronic devices in integrated circuits. Depending on different applied voltages, various transistors with different voltages are provided. High-voltage (HV) transistors, such as laterally diffused metal-oxide-semiconductor (LDMOS) field-effect transistors, can be used as high-voltage switching regulators and high-voltage switches in power management integrated circuits (ICs). In order to handle the high voltages involved in these and other high voltage applications, it is desirable to have a high voltage transistor with high breakdown voltage and low on-resistance.
The disclosure provides a semiconductor device and a manufacturing method thereof, so as to reduce the influence of the hot carrier effect and therefore improve the breakdown voltage and the performance of the semiconductor device.
In an embodiment of the present disclosure, a semiconductor device includes a gate structure, a first doped region, a second doped region, an isolation structure, an insulating layer and a field plate. The gate structure is located on the substrate. The first doped region and the second doped region are located at two sides of the gate structure. The isolation structure is located in the substrate between the first doped region and the second doped region, and is separated from the gate structure by a non-zero distance. The insulating layer extends continuously from a portion of a top surface of the gate structure to a portion of a top surface of the isolation structure. The field plate is located on the insulating layer and has the same potential as the gate structure.
In an embodiment of the present disclosure, a method of fabricating a semiconductor device includes the following steps. An isolation structure is formed in the substrate. A gate structure is formed on the substrate. A first doped region and a second doped region are formed at two sides of the gate structure. An isolation structure is formed in the substrate between the first doped region and the second doped region, and is separated from the gate structure by a non-zero distance. An insulating layer is formed extending continuously from a portion of a top surface of the gate structure to a portion of a top surface of the isolation structure. A field plate is formed on the insulating layer. The field plate is electrically connected to the gate structure, so the field plate and the gate structure are equipotential.
Based on the above, the semiconductor device and the manufacturing method thereof according to the embodiments of the present disclosure can reduce the influence of the hot carrier effect and therefore improve the breakdown voltage and the performance of the semiconductor device.
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In the embodiment of the present disclosure, the gate structure 20 is separated from the isolation structure 14a, and an insulating layer 32 is located between the gate structure 20 and the isolation structure 14a. The thickness of the insulating layer 32 is greater than the thickness of the gate dielectric layer 22 of the gate structure 20. Therefore, the electric field can be released, the ionization impact on the top surface at the corner of the isolation structure 14a can be reduced, and the breakdown voltage and the performance of the device can be accordingly improved.
In the embodiment of the present disclosure, the insulating layer 32 covers a portion of the top surface of the gate structure 20 and the sidewall of the spacer 26, a portion of the top surface of the well region 18 between the gate structure 20 and the isolation structure 14a, and a portion of the top surface of the isolation structure 14a. The width Lc of the isolation structure 14a covered by the insulating layer 32 is about 30% to 80% of the top width Ld of the isolation structure 14a.
The insulating layer 32 may include silicon oxide. The insulating layer 32 can be integrated with the existing manufacturing process. For example, the insulating layer 32 can be a salicide block (SAB) layer in a self-aligned silicide process. Therefore, it can be integrated with the existing manufacturing process without an additional process step.
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Thereafter, a deep well region 12, well regions 16a, 18, 16b and isolation structures 14a and 14b are formed in substrate 10. The well region 16a is located in deep well region 12. The well region 16b is located in the substrate 10 outside the deep well region 12. The well region 18 is located within the deep well region 12 in the substrate 10, and the sidewall of the well region 18 is aligned with (as shown in
Each of the deep well region 12 and the well region 18 may have a dopant of a second conductivity type. The dopant of the second conductivity type is different from the dopant of the first conductivity type. The dopant of the second conductivity type can be an N-type dopant, such as phosphorus or arsenic. The dopant of the second conductivity type a P-type dopant, such as boron or boron trifluoride. Each of the well regions 16a, 16b may have a dopant of the first conductivity type. The dopant of the first conductivity type can be a P-type dopant, such as boron or boron trifluoride. The dopant of the first conductivity type can be an N-type dopant, such as phosphorus or arsenic. The deep well region 12, the well regions 16a, 18, 16b can be formed by ion implantation processes. The isolation structures 14a and 14b may include silicon oxide, silicon nitride or a combination thereof. The isolation structures 14a and 14b may be shallow trench isolation structures. In other words, the isolation structures 14a and 14b can be formed by a shallow trench isolation method.
In some embodiments, a deep well region 12 may be first formed in substrate 10. Thereafter, isolation structures 14a and 14b are formed in the substrate 10. Afterwards, well regions 16a, 16b are formed in the substrate 10. A well region 18 is then formed. However, the embodiments of the present disclosure are not limited thereto.
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The gate structure 20 covers a portion of the well region 16a, a portion of the deep well region 12 and a portion of the well region 18. The gate structure 20 does not extend to cover the isolation structure 14a. The gate structure 20 exposes a portion of the surface of the well region 18 and the entire surface of the isolation structure 14a. There is a non-zero distance d1 between the gate dielectric layer 22 of the gate structure 20 and the isolation structure 14a. The distance d1 may be about 0.1 μm to 1 μm, for example.
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Thereafter, doped regions 28a, 28b and doped regions 30a, 30b are formed in the substrate 10 at two sides of the gate structure 20 and the isolation structure 14a. The doped regions 28a and 28b are located in the well region 16a and the well region 18, respectively. The doped regions 30a and 30b are located in the well regions 16a and 16b, respectively. There is a channel region 60 below the gate structure 20. The channel region 60 is located in the well region 16a between the doped region 28a and the deep well region 12. Each of the doped regions 28a and 28b may have a dopant of the second conductivity type. The dopant of the second conductivity type is different from the dopant of the first conductivity type. The dopant of the second conductivity type can be an N-type dopant, such as phosphorus or arsenic. The dopant of the second conductivity type can be a P-type dopant, such as boron or boron trifluoride. Each of the doped regions 30a, 30b may have a dopant of the first conductivity type. The dopant of the first conductivity type can be a P-type dopant, such as boron or boron trifluoride. The dopant of the first conductivity type can be an N-type dopant, such as phosphorus or arsenic.
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Thereafter, contacts 44a, 44b, 44c, 44d, and 44e are formed in the dielectric layer 42. The contacts 44a, 44b, 44c, 44d, 44e can be formed according to the method described below. For example, multiple contact openings are formed in the dielectric layer 42 by lithography and etching processes, and a conductive material is then formed in the multiple contact openings and on the dielectric layer 42. The conductive material may include tungsten, for example. A barrier material (e.g., tantalum, tantalum nitride, titanium, titanium nitride, or a combination thereof) may be formed prior to the formation of the conductive material. Afterwards, the barrier material and the conductive material on the dielectric layer 42 are removed by a chemical mechanical polishing process or an etch-back process.
Afterwards, conductive lines 48a, 48b, 48c and 48d are formed on the dielectric layer 42. The conductive lines 48a, 48b, 48c and 48d are formed by forming a conductive material on the dielectric layer 42, and then patterning the conductive material through lithography and etching processes, for example. After that, a dielectric layer 46 is formed on the dielectric layer 42 and the conductive lines 48a, 48b, 48c, and 48d. The material of the dielectric layer 46 may include silicon oxide or undoped silicon glass. The method of forming the dielectric layer 46 may include forming a dielectric material on the dielectric layer 42 and the conductive lines 48a, 48b, 48c, and 48d, and then performing a chemical mechanical polishing process or an etching back process to remove the dielectric material on the conductive lines 48a, 48b, 48c, and 48d.
The dielectric layers 42, 46, the conductive lines 48a, 48b, 48c, and 48d in the above-mentioned interconnect structure 50 can also be formed by another method, such as a single damascene process. The single damascene process includes forming a dielectric layer 46, forming a trench in the dielectric layer 46 through lithography and etching processes, forming a conductive material on the dielectric layer 46 and in the trench, and performing a chemical mechanical polishing process or an etching back process to removes the excess conductive material on the dielectric layer 46 and therefore form the conductive lines 48a, 48b, 48c and 48d. In other embodiments, the conductive lines 48a, 48b, 48c, and 48d and the contacts 44a, 44b, 44c, 44d, and 44e may be formed by a dual damascene process.
The conductive line 48a is electrically connected to the doped regions 30a and 28a through the contact 44a and the metal silicide layer 36a. The conductive line 48b is electrically connected to the gate conductive layer 24 through the contact 44b and the metal silicide layer 36b. The conductive line 48b is further electrically connected to the field plate 34 through the contact 44c and the metal silicide layer 36c. That is, the gate conductive layer 24 and the field plate 34 are electrically connected to each other and have the same potential. The conductive line 48c is electrically connected to the doped region 28b through the contact 44d and the metal silicide layer 36d. The conductive line 48d is electrically connected to the doped region 30b through the contact 44e and the metal silicide layer 36e.
In this embodiment, the gate conductive layer 24 and the field plate 34 are electrically connected to each other through the conductive line 48b of a first metal layer. However, the embodiment of the present disclosure is not limited thereto. In other embodiments, the gate conductive layer 24 and the field plate 34 can be electrically connected to each other through a conductive line of a second metal layer, a third metal layer or a higher-level metal layer, as long as the gate conductive layer 24 and the field plate 34 can be equipotential.
The thickness of gate dielectric layer 22 is about 120 angstroms, and the thickness of insulating layer (e.g., salicide block layer) 32 is about 300 angstroms. The width Ld of the isolation structure 14a is about 2.7 μm. The distance d1 between the gate dielectric layer 24 of the gate structure 20 and the isolation structure 14a is about 0.27 μm.
The thickness of gate dielectric layer 22 is about 120 angstroms, and the thickness of insulating layer (e.g., salicide block layer) 32 is 300 angstroms. The width Ld of the isolation structure 14a is about 2 μm. The distance d1 between the gate dielectric layer 24 of the gate structure 20 and the isolation structure 14a is about 0.27 μm.
The thickness of gate dielectric layer 22 is about 120 angstroms, and the thickness of insulating layer (e.g., salicide block layer) 32 is 300 angstroms. The width Ld of the isolation structure 14a is about 2.7 μm. The gate dielectric layer 24 of the gate structure 20 extends to cover the isolation structure 14a, and the distance d1 is about zero.
Table 1 shows the breakdown voltage BV, the turn-on resistance Rdson and the performance (i.e., the ratio of breakdown voltage BV to turn-on resistance Rdson) FOM of each of Example 1, Example 2 and Comparative Example 1. The results of Example 1 and Comparative Example 1 in Table 1 show that: under the same isolation structure width Ld, Example 1 and Comparative Example 1 have substantially the same turn-on resistance Rdson, but the breakdown voltage of Example 1 can be greatly improved. The performance FOM of Comparative Example 1 is 0.98, while the performance FOM of Example 1 can be increased to 1.16.
The results of Example 2 and Comparative Example 1 in Table 1 show that: under substantially the same breakdown voltage BV, the performance FOM of Comparative Example 1 having a larger isolation structure width Ld is 0.98, but the performance FOM of Example 2 having a smaller isolation structure width Ld can be increased to 1.32. The performance FOM can be increased by 34.8%.
In the method of the embodiments of the present disclosure, the electric field at the corner of the isolation structure can be greatly dispersed by separating a gate structure from an isolation structure, disposing an insulating layer (having a thickness greater than that of a gate dielectric layer of the gate structure) between the gate structure and the isolation structure, and disposing a field plate on the insulating layer. By such configuration, the influence of the hot carrier effect can be reduced, the breakdown voltage and the performance of the device can be greatly improved. On the other hand, with the method of the embodiment of the present disclosure, the performance of the device can be improved while shrinking the isolation structure. Therefore, the chip area occupied by the isolation structure can be reduced.
Number | Date | Country | Kind |
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112119698 | May 2023 | TW | national |