US20020100947A1 - Method for forming variable-K gate dielectric - Google Patents

Method for forming variable-K gate dielectric Download PDF

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US20020100947A1
US20020100947A1 US09/769,811 US76981101A US2002100947A1 US 20020100947 A1 US20020100947 A1 US 20020100947A1 US 76981101 A US76981101 A US 76981101A US 2002100947 A1 US2002100947 A1 US 2002100947A1
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Prior art keywords
dielectric layer
gate
dielectric
low
gate electrode
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US6436774B1 (en
Inventor
James Lee
Ying Leung
Yelehanka Pradeep
Jia Zheng
Lap Chan
Elgin Quek
Ravi Sundaresan
Yang Pan
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GlobalFoundries Singapore Pte Ltd
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Chartered Semiconductor Manufacturing Inc
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Priority to US09/769,811 priority Critical patent/US6436774B1/en
Priority to TW090111539A priority patent/TW510013B/en
Priority to SG200504604-0A priority patent/SG137692A1/en
Priority to SG200200222A priority patent/SG108291A1/en
Priority to JP2002016958A priority patent/JP4255235B2/en
Priority to DE60211396T priority patent/DE60211396T2/en
Priority to AT02368011T priority patent/ATE326768T1/en
Priority to EP02368011A priority patent/EP1227513B1/en
Priority to US10/196,111 priority patent/US6709934B2/en
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    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01LSEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
    • H01L21/00Processes or apparatus adapted for the manufacture or treatment of semiconductor or solid state devices or of parts thereof
    • H01L21/02Manufacture or treatment of semiconductor devices or of parts thereof
    • H01L21/04Manufacture or treatment of semiconductor devices or of parts thereof the devices having at least one potential-jump barrier or surface barrier, e.g. PN junction, depletion layer or carrier concentration layer
    • H01L21/18Manufacture or treatment of semiconductor devices or of parts thereof the devices having at least one potential-jump barrier or surface barrier, e.g. PN junction, depletion layer or carrier concentration layer the devices having semiconductor bodies comprising elements of Group IV of the Periodic System or AIIIBV compounds with or without impurities, e.g. doping materials
    • H01L21/28Manufacture of electrodes on semiconductor bodies using processes or apparatus not provided for in groups H01L21/20 - H01L21/268
    • H01L21/28008Making conductor-insulator-semiconductor electrodes
    • H01L21/28017Making conductor-insulator-semiconductor electrodes the insulator being formed after the semiconductor body, the semiconductor being silicon
    • H01L21/28158Making the insulator
    • H01L21/28167Making the insulator on single crystalline silicon, e.g. using a liquid, i.e. chemical oxidation
    • H01L21/28194Making the insulator on single crystalline silicon, e.g. using a liquid, i.e. chemical oxidation by deposition, e.g. evaporation, ALD, CVD, sputtering, laser deposition
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01LSEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
    • H01L29/00Semiconductor devices adapted for rectifying, amplifying, oscillating or switching, or capacitors or resistors with at least one potential-jump barrier or surface barrier, e.g. PN junction depletion layer or carrier concentration layer; Details of semiconductor bodies or of electrodes thereof  ; Multistep manufacturing processes therefor
    • H01L29/40Electrodes ; Multistep manufacturing processes therefor
    • H01L29/41Electrodes ; Multistep manufacturing processes therefor characterised by their shape, relative sizes or dispositions
    • H01L29/423Electrodes ; Multistep manufacturing processes therefor characterised by their shape, relative sizes or dispositions not carrying the current to be rectified, amplified or switched
    • H01L29/42312Gate electrodes for field effect devices
    • H01L29/42316Gate electrodes for field effect devices for field-effect transistors
    • H01L29/4232Gate electrodes for field effect devices for field-effect transistors with insulated gate
    • H01L29/42372Gate electrodes for field effect devices for field-effect transistors with insulated gate characterised by the conducting layer, e.g. the length, the sectional shape or the lay-out
    • H01L29/42376Gate electrodes for field effect devices for field-effect transistors with insulated gate characterised by the conducting layer, e.g. the length, the sectional shape or the lay-out characterised by the length or the sectional shape
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01LSEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
    • H01L29/00Semiconductor devices adapted for rectifying, amplifying, oscillating or switching, or capacitors or resistors with at least one potential-jump barrier or surface barrier, e.g. PN junction depletion layer or carrier concentration layer; Details of semiconductor bodies or of electrodes thereof  ; Multistep manufacturing processes therefor
    • H01L29/40Electrodes ; Multistep manufacturing processes therefor
    • H01L29/43Electrodes ; Multistep manufacturing processes therefor characterised by the materials of which they are formed
    • H01L29/49Metal-insulator-semiconductor electrodes, e.g. gates of MOSFET
    • H01L29/51Insulating materials associated therewith
    • H01L29/511Insulating materials associated therewith with a compositional variation, e.g. multilayer structures
    • H01L29/512Insulating materials associated therewith with a compositional variation, e.g. multilayer structures the variation being parallel to the channel plane
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01LSEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
    • H01L29/00Semiconductor devices adapted for rectifying, amplifying, oscillating or switching, or capacitors or resistors with at least one potential-jump barrier or surface barrier, e.g. PN junction depletion layer or carrier concentration layer; Details of semiconductor bodies or of electrodes thereof  ; Multistep manufacturing processes therefor
    • H01L29/40Electrodes ; Multistep manufacturing processes therefor
    • H01L29/43Electrodes ; Multistep manufacturing processes therefor characterised by the materials of which they are formed
    • H01L29/49Metal-insulator-semiconductor electrodes, e.g. gates of MOSFET
    • H01L29/51Insulating materials associated therewith
    • H01L29/517Insulating materials associated therewith the insulating material comprising a metallic compound, e.g. metal oxide, metal silicate
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01LSEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
    • H01L29/00Semiconductor devices adapted for rectifying, amplifying, oscillating or switching, or capacitors or resistors with at least one potential-jump barrier or surface barrier, e.g. PN junction depletion layer or carrier concentration layer; Details of semiconductor bodies or of electrodes thereof  ; Multistep manufacturing processes therefor
    • H01L29/66Types of semiconductor device ; Multistep manufacturing processes therefor
    • H01L29/66007Multistep manufacturing processes
    • H01L29/66075Multistep manufacturing processes of devices having semiconductor bodies comprising group 14 or group 13/15 materials
    • H01L29/66227Multistep manufacturing processes of devices having semiconductor bodies comprising group 14 or group 13/15 materials the devices being controllable only by the electric current supplied or the electric potential applied, to an electrode which does not carry the current to be rectified, amplified or switched, e.g. three-terminal devices
    • H01L29/66409Unipolar field-effect transistors
    • H01L29/66477Unipolar field-effect transistors with an insulated gate, i.e. MISFET
    • H01L29/66568Lateral single gate silicon transistors
    • H01L29/66575Lateral single gate silicon transistors where the source and drain or source and drain extensions are self-aligned to the sides of the gate
    • H01L29/66583Lateral single gate silicon transistors where the source and drain or source and drain extensions are self-aligned to the sides of the gate with initial gate mask or masking layer complementary to the prospective gate location, e.g. with dummy source and drain contacts
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01LSEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
    • H01L29/00Semiconductor devices adapted for rectifying, amplifying, oscillating or switching, or capacitors or resistors with at least one potential-jump barrier or surface barrier, e.g. PN junction depletion layer or carrier concentration layer; Details of semiconductor bodies or of electrodes thereof  ; Multistep manufacturing processes therefor
    • H01L29/40Electrodes ; Multistep manufacturing processes therefor
    • H01L29/43Electrodes ; Multistep manufacturing processes therefor characterised by the materials of which they are formed
    • H01L29/49Metal-insulator-semiconductor electrodes, e.g. gates of MOSFET
    • H01L29/51Insulating materials associated therewith
    • H01L29/518Insulating materials associated therewith the insulating material containing nitrogen, e.g. nitride, oxynitride, nitrogen-doped material

Definitions

  • This invention relates generally to fabrication of a semiconductor device and more particularly to a method for forming a gate dielectric with areas having different dielectric constants.
  • a lightly doped drain region LDD is formed between the channel and the source/drain, lowering the electric field.
  • the reduced impurity concentration in the LDD causes parasitic resistance, reducing drive current and slowing down the transistor.
  • U.S. Pat. No. 5,952,700 shows a process for forming a two-layer gate dielectric on one side of the gate.
  • U.S. Pat. No. 5,677,217 shows a gate process where a LDD structure is formed only on the drain side of a gate, and a two-layer insulator is formed only at the drain side of a gate using an opening in an insulator layer or an offset mask.
  • U.S. Pat. No. 4,196,507 shows a process for forming a transistor gate using a lateral etch to undercut the oxide over the channel region to provide a mask for a threshold adjust implant.
  • U.S. Pat. No. 5,920,103 shows a method to modify the gate dielectric on the drain side edge using an RTA.
  • the present invention provides a method for forming a gate dielectric having regions with different dielectric constants.
  • a low-K dielectric layer is formed over a semiconductor structure.
  • a dummy dielectric layer is formed over the low-K dielectric layer.
  • the dummy dielectric layer and low-K dielectric layer are patterned to form an opening.
  • the dummy dielectric layer is isentropically etched selectively to the low-K dielectric layer to form a stepped gate opening.
  • a high-K dielectric layer is formed over the dummy dielectric and in the stepped gate opening.
  • a gate electrode is formed on the high-K dielectric layer.
  • FIGS. 1 through 6 illustrate sequential sectional views of a process for forming a gate dielectric having regions with different dielectric constants according to the present invention.
  • the present invention provides a method for forming a gate dielectric having regions with different dielectric constants.
  • the gate dielectric comprises both a high-K and a low-K dielectric region.
  • the gate dielectric comprises only a high-K dielectric region allowingdrive current with reduced overlap capacitance.
  • the present invention begins by providing a semiconductor structure ( 11 ).
  • Semiconductor structure ( 11 ) should be understood to possibly include a wafer or substrate of semiconducting material, such as monocrystalline silicon, or a similar structure now known or later developed, such as a silicon-on-insulator (SOI) structure.
  • Semiconductor structure ( 11 ) should be further understood to possibly include one or more conductive and or insulating layers formed over the substrate or like structure, and one or more active and/or passive devices formed on or over the substrate or like structure.
  • a low-K dielectric layer ( 20 ) layer is formed over the semiconductor structure ( 11 ), and a dummy dielectric layer ( 40 ) is formed over the low-K dielectric layer ( 20 ).
  • the low-K dielectric layer ( 20 ) will be used to form low-K regions at the edges of a gate dielectric.
  • the low-K dielectric layer ( 20 ) preferably has a thickness of between about 30 angstroms and 100 angstroms and can comprise any low-K material that can be formed in such a thin layer, preferably fluorinated silicon dioxide, carbon doped silicon dioxide, or a low-K polymer.
  • Low-K material should be understood to be a material having a dielectric constant less than 3.9.
  • the dummy dielectric layer ( 40 ) can comprise any dielectric material that can be etched selectively to the low-K dielectric layer ( 20 ).
  • the dummy dielectric layer ( 40 ) can comprise silicon nitride.
  • the dummy dielectric layer should have a sufficient thickness for an intended gate electrode.
  • the dummy dielectric layer ( 40 ) and the low-K dielectric layer ( 20 ) are patterned to form a first gate opening ( 45 ) in the dummy dielectric layer ( 40 ) and a second gate opening ( 25 ) in the low-K dielectric layer ( 20 ).
  • the first gate opening ( 45 ) and the second gate opening ( 25 ) are narrower than the desired width of the intended gate electrode.
  • the second gate opening ( 25 ) preferably has a width of between about 0.06 microns and 0.48 microns.
  • the dummy dielectric layer ( 40 ) is isotropically etched selectively to the low-K dielectric layer ( 20 ) to open the first gate opening ( 45 ).
  • the selective, isotropic etch forms a stepped gate opening ( 55 ).
  • the selective, isotropic etch can be performed with hot phosphoric acid.
  • the stepped opening ( 55 ) preferably has an stepped opening width ( 59 ) of between about 0.08 microns and 0.50 microns with a step width ( 51 ) of between about 0.01 microns and 0.02 microns.
  • a high-K dielectric layer ( 60 ) is formed over the dummy dielectric layer ( 40 ) and in the stepped gate opening ( 55 ).
  • the high-K dielectric layer ( 60 ) can comprise any of a the presently-known or later-developed high-K materials, including but not limited to: ZrO 2 , Ta 2 O 5 , TiO 2 , Si 3 N 4 ,ZrSiO 4 , or Al 2 O 3 , and most preferably ZrSiO 4 .
  • the high-K dielectric layer ( 60 ) is preferably formed to a thickness of between about 10 angstroms and 100 angstroms by sputtering.
  • High-K material should be understood to be material having a dielectric constant of greater than 3.9, and preferably greater than 8.0.
  • a gate electrode layer ( 80 ) is formed over the high-K dielectric layer ( 60 ).
  • the gate electrode layer can comprise a metal, polysilicon, or a stack of metal and/or polysilicon films, as is known in the art.
  • the gate electrode layer has a sufficient thickness to overfill the stepped opening ( 55 ).
  • the gate electrode layer ( 80 ) and the high-K dielectric layer ( 60 ) are planarized stopping on the dummy dielectric layer ( 40 ) to form a gate electrode ( 80 A).
  • the planarization is most preferably performed using a chemical-mechanical polishing (CMP) process as is known in the art.
  • CMP chemical-mechanical polishing
  • the dummy dielectric layer ( 40 ) preferably acts as a CMP stop.
  • the dummy dielectric layer (not shown) is removed, preferably using an etch which etches the dummy dielectric selectively to the high-K dielectric layer ( 60 ).
  • a dummy dielectric layer comprising silicon nitride can be etched selectively to a high-K dielectric layer comprising ZrO 2 (zirconium dioxide).
  • Lightly doped source and drain regions (LDDs) ( 91 ) can be formed in the semiconductor structure ( 11 ) adjacent the gate electrode ( 80 A) by an impurity ion implant and diffuision anneal as is known in the art.
  • Spacers ( 92 ) can be formed adjacent the gate electrode ( 80 A) as is known in the art.
  • Source and drain regions can then be formed in the semiconductor structure ( 11 ) adjacent the spacers ( 92 ).
  • the low-K dielectric layer ( 20 ) extends over at least a portion of the lightly doped source and drain regions.
  • the low-K dielectric layer ( 20 ) extends a distance of within 10% of the length of the lightly doped source and drain regions.
  • the low-K dielectric layer ( 20 ) extends a distance of about the length of the lightly doped source and drain regions.
  • the key advantages of the present invention are that a gate dielectric is formed having regions with different dielectric constants.
  • the gate dielectric of the present invention provides a method for increasing drive current in a gate channel while reducing hot carrier effects and overlap capacitance.

Abstract

A method for forming a gate dielectric having regions with different dielectric constants. A low-K dielectric layer is formed over a semiconductor structure. A dummy dielectric layer is formed over the low-K dielectric layer. The dummy dielectric layer and low-K dielectric layer are patterned to form an opening. The dummy dielectric layer is isontropically etched selectively to the low-K dielectric layer to form a stepped gate opening. A high-K dielectric layer is formed over the dummy dielectric and in the stepped gate opening. A gate electrode is formed on the high-K dielectric layer.

Description

    BACKGROUND OF INVENTION
  • 1) Field of the Invention [0001]
  • This invention relates generally to fabrication of a semiconductor device and more particularly to a method for forming a gate dielectric with areas having different dielectric constants. [0002]
  • 2) Description of the Prior Art [0003]
  • In MOS (metal on silicon) transistor technology, a gate dielectric is formed on a silicon substrate, and a gate electrode is formed over the gate dielectric. Source and drain regions are formed adjacent the gate electrode and the gate dielectric. When a voltage is applied to the gate electrode, electrons (NMOS) or holes (PMOS) flow across the region of the silicon substrate under the gate dielectric, known as the channel. As the channel length decreases, the electrons in an NMOS transistor gain sufficient energy from the electric field to enter the gate dielectric layer where they become trapped, changing the gate threshold voltage (e.g. hot carrier effect). [0004]
  • To reduce the hot carrier effect, a lightly doped drain region LDD is formed between the channel and the source/drain, lowering the electric field. However, the reduced impurity concentration in the LDD causes parasitic resistance, reducing drive current and slowing down the transistor. [0005]
  • Another problem with LDD structured MOS transistors is that the overlap of the gate electrode over the LDD regions with a thin gate dielectric between them causes capacitance, called overlap capacitance, which further slows the transistor. [0006]
  • The importance of overcoming the various deficiencies noted above is evidenced by the extensive technological development directed to the subject, as documented by the relevant patent and technical literature. The closest and apparently more relevant technical developments in the patent literature can be gleaned by considering the following patents. [0007]
  • U.S. Pat. No. 5,952,700 (Yoon) shows a process for forming a two-layer gate dielectric on one side of the gate. [0008]
  • U.S. Pat. No. 5,677,217 (Tseng) shows a gate process where a LDD structure is formed only on the drain side of a gate, and a two-layer insulator is formed only at the drain side of a gate using an opening in an insulator layer or an offset mask. [0009]
  • U.S. Pat. No. 4,196,507 (Baptiste) shows a process for forming a transistor gate using a lateral etch to undercut the oxide over the channel region to provide a mask for a threshold adjust implant. [0010]
  • U.S. Pat. No. 5,920,103 (Fulford et al.) shows a method to modify the gate dielectric on the drain side edge using an RTA. [0011]
  • SUMMARY OF THE INVENTION
  • It is an object of the present invention to provide a method for forming a gate dielectric having regions of varying dielectric constant. [0012]
  • It is another object of the present invention to provide a method for increasing drive current in a gate channel while reducing hot carrier effects and overlap capacitance. [0013]
  • It is yet another object of the present invention to provide a method for reducing channel length without causing detrimental short channel effects and overlap capacitance. [0014]
  • To accomplish the above objectives, the present invention provides a method for forming a gate dielectric having regions with different dielectric constants. A low-K dielectric layer is formed over a semiconductor structure. A dummy dielectric layer is formed over the low-K dielectric layer. The dummy dielectric layer and low-K dielectric layer are patterned to form an opening. The dummy dielectric layer is isentropically etched selectively to the low-K dielectric layer to form a stepped gate opening. A high-K dielectric layer is formed over the dummy dielectric and in the stepped gate opening. A gate electrode is formed on the high-K dielectric layer. [0015]
  • The present invention provides considerable improvement over the prior art. A gate dielectric can be formed having regions with different dielectric constants. The high-K dielectric region allows the drive current in a gate channel to be increased. The low-K dielectric regions at the edges of the gate electrode reduce hot carrier effects and overlap capacitance. The gate dielectric of the present invention provides a method for reducing channel length without causing detrimental short channel effects and overlap capacitance. [0016]
  • The present invention achieves these benefits in the context of known process technology. However, a further understanding of the nature and advantages of the present invention may be realized by reference to the latter portions of the specification and attached drawings.[0017]
  • BRIEF DESCRIPTION OF THE DRAWINGS
  • The features and advantages of a semiconductor device according to the present invention and further details of a process of fabricating such a semiconductor device in accordance with the present invention will be more clearly understood from the following description taken in conjunction with the accompanying drawings in which like reference numerals designate similar or corresponding elements, regions and portions and in which: [0018]
  • FIGS. 1 through 6 illustrate sequential sectional views of a process for forming a gate dielectric having regions with different dielectric constants according to the present invention.[0019]
  • DETAILED DESCRIPTION OF THE INVENTION
  • The present invention will be described in detail with reference to the accompanying drawings. The present invention provides a method for forming a gate dielectric having regions with different dielectric constants. At the edges of the channel, where hot carrier effects are most likely to occur, the gate dielectric comprises both a high-K and a low-K dielectric region. In the middle of the channel, the gate dielectric comprises only a high-K dielectric region allowingdrive current with reduced overlap capacitance. [0020]
  • Referring to FIG. 1, the present invention begins by providing a semiconductor structure ([0021] 11). Semiconductor structure (11) should be understood to possibly include a wafer or substrate of semiconducting material, such as monocrystalline silicon, or a similar structure now known or later developed, such as a silicon-on-insulator (SOI) structure. Semiconductor structure (11) should be further understood to possibly include one or more conductive and or insulating layers formed over the substrate or like structure, and one or more active and/or passive devices formed on or over the substrate or like structure.
  • Still referring to FIG. 1, a low-K dielectric layer ([0022] 20) layer is formed over the semiconductor structure (11), and a dummy dielectric layer (40) is formed over the low-K dielectric layer (20). The low-K dielectric layer (20) will be used to form low-K regions at the edges of a gate dielectric. The low-K dielectric layer (20) preferably has a thickness of between about 30 angstroms and 100 angstroms and can comprise any low-K material that can be formed in such a thin layer, preferably fluorinated silicon dioxide, carbon doped silicon dioxide, or a low-K polymer. Low-K material should be understood to be a material having a dielectric constant less than 3.9.
  • The dummy dielectric layer ([0023] 40) can comprise any dielectric material that can be etched selectively to the low-K dielectric layer (20). For example, over a flourinated silicon dioxide low-K dielectric layer (20), the dummy dielectric layer (40) can comprise silicon nitride. The dummy dielectric layer should have a sufficient thickness for an intended gate electrode.
  • Still referring to FIG. 1, the dummy dielectric layer ([0024] 40) and the low-K dielectric layer (20) are patterned to form a first gate opening (45) in the dummy dielectric layer (40) and a second gate opening (25) in the low-K dielectric layer (20). The first gate opening (45) and the second gate opening (25) are narrower than the desired width of the intended gate electrode. The second gate opening (25) preferably has a width of between about 0.06 microns and 0.48 microns.
  • Referring now to FIG. 2, the dummy dielectric layer ([0025] 40) is isotropically etched selectively to the low-K dielectric layer (20) to open the first gate opening (45). The selective, isotropic etch forms a stepped gate opening (55). For a dummy dielectric layer (40) comprising silicon nitride and a low-K dielectric layer (20) comprising fluorinated silicon dioxide, the selective, isotropic etch can be performed with hot phosphoric acid. The stepped opening (55) preferably has an stepped opening width (59) of between about 0.08 microns and 0.50 microns with a step width (51) of between about 0.01 microns and 0.02 microns.
  • Referring now to FIG. 3, a high-K dielectric layer ([0026] 60) is formed over the dummy dielectric layer (40) and in the stepped gate opening (55). The high-K dielectric layer (60) can comprise any of a the presently-known or later-developed high-K materials, including but not limited to: ZrO2, Ta2O5, TiO2, Si3N4,ZrSiO4, or Al2O3, and most preferably ZrSiO4. The high-K dielectric layer (60) is preferably formed to a thickness of between about 10 angstroms and 100 angstroms by sputtering. High-K material should be understood to be material having a dielectric constant of greater than 3.9, and preferably greater than 8.0.
  • Referring now to FIG. 4, a gate electrode layer ([0027] 80) is formed over the high-K dielectric layer (60). The gate electrode layer can comprise a metal, polysilicon, or a stack of metal and/or polysilicon films, as is known in the art. The gate electrode layer has a sufficient thickness to overfill the stepped opening (55).
  • As shown in FIG. 5, the gate electrode layer ([0028] 80) and the high-K dielectric layer (60) are planarized stopping on the dummy dielectric layer (40) to form a gate electrode (80A). The planarization is most preferably performed using a chemical-mechanical polishing (CMP) process as is known in the art. The dummy dielectric layer (40) preferably acts as a CMP stop.
  • Referring now to FIG. 6, the dummy dielectric layer (not shown) is removed, preferably using an etch which etches the dummy dielectric selectively to the high-K dielectric layer ([0029] 60). For example, a dummy dielectric layer comprising silicon nitride can be etched selectively to a high-K dielectric layer comprising ZrO2 (zirconium dioxide).
  • Lightly doped source and drain regions (LDDs) ([0030] 91) can be formed in the semiconductor structure (11) adjacent the gate electrode (80A) by an impurity ion implant and diffuision anneal as is known in the art. Spacers (92) can be formed adjacent the gate electrode (80A) as is known in the art. Source and drain regions can then be formed in the semiconductor structure (11) adjacent the spacers (92). Following lightly doped source and drain region formation, the low-K dielectric layer (20) extends over at least a portion of the lightly doped source and drain regions. Preferably the low-K dielectric layer (20) extends a distance of within 10% of the length of the lightly doped source and drain regions. Most preferably, the low-K dielectric layer (20) extends a distance of about the length of the lightly doped source and drain regions.
  • The key advantages of the present invention are that a gate dielectric is formed having regions with different dielectric constants. The gate dielectric of the present invention provides a method for increasing drive current in a gate channel while reducing hot carrier effects and overlap capacitance. [0031]
  • While the invention has been particularly shown and described with reference to the preferred embodiments thereof, it will be understood by those skilled in the art that various changes in form and details may be made without departing from the spirit and scope of the invention. [0032]

Claims (20)

What is claimed is:
1. A method for forming a gate dielectric, comprising the steps of:
a. forming a low-K dielectric layer over a semiconductor structure;
b. forming a dummy dielectric layer over said low-K dielectric layer;
c. patterning said dummy dielectric layer and low-K dielectric layer to form a first gate opening in said dummy dielectric layer and a second gate opening in said low-K dielectric layer;
d. isotropically etching said dummy dielectric layer selectively to said low-K dielectric layer to open said first gate opening, forming a stepped gate opening;
e. forming a high-K dielectric layer over said dummy dielectric and in said stepped gate opening; and
f. forming a gate electrode on said high-K dielectric layer.
2. The method of claim 1 wherein said low-K dielectric layer comprises fluorinated silicon dioxide.
3. The method of claim 1 wherein said high-K dielectric comprises ZrSiO4.
4. The method of claim 1 wherein said high-K dielectric comprises ZrO2, Ta2O5, TiO2, Si3N4, or A2O3.
5. The method of claim 1 wherein lightly doped source and drain regions are formed adjacent said gate electrode such that said high-K dielectric layer extends a distance of within 10% of the length of said lightly doped source and drain regions.
6. The method of claim 1 wherein lightly doped source and drain regions are formed adjacent said gate electrode such that said high-K dielectric layer extends a distance of about the length of the comprises Si3N4.
7. The method of claim 1 wherein said low-K dielectric layer has a thickness of between about 30 angstroms and 100 angstroms and said high-K dielectric has a thickness of between about 10 angstroms and 100 angstroms.
8. The method of claim 1 wherein said stepped opening has a width of between about 0.08 microns and 0.50 microns with a step width of between about 0.01 microns and 0.02 microns.
9. The method of claim 1 which further comprise the steps of:
(g) removing the dummy dielectric layer;
(h) forming lightly doped source and drain regions in said semiconductor structure adjacent said gate electrode;
(i) forming spacers adjacent said gate electrode; and
(j) forming source and drain regions in said semiconductor structure adjacent said spacers.
10. The method of claim 9 wherein said low-K dielectric layer extends over at least a portion of said lightly doped source and drain regions.
11. A semiconductor gate having a gate dielectric with regions having different dielectric constants, comprising:
(a) a stepped gate electrode having a co-planer top surface with a greater thickness in its center than at its edges;
(b) a low-K dielectric region underlying the gate electrode at each edge of the gate; and
(c) a high-K dielectric region overlying the low-K dielectric regions and contacting the bottom and sides of said gate electrode.
12. The semiconductor gate of claim 11 wherein said low-K dielectric layer comprises fluorinated silicon dioxide.
13. The semiconductor gate of claim 11 wherein said high-K dielectric comprises ZrSiO4.
14. The semniconductor gate of claim 11 wherein said high-K dielectric comprises ZrO2, Ta2O5, TiO2, Si3N4, or Al2O3.
15. The semiconductor gate of claim 11 wherein said low-K dielectric layer has a thickness of between about 30 angstroms and 100 angstroms and said high-K dielectric has a thickness of between about 10 angstroms and 100 angstroms.
16. The semiconductor gate of claim 11 wherein said stepped gate electrode has a width of between about 0.08 microns and 0.50 microns with a step width of between about 0.01 microns and 0.02 microns.
17. The semiconductor gate of claim 11 which further comprises:
(d) lightly doped source and drain regions adjacent said gate electrode;
(e) spacers adjacent said gate electrode; and
(f) source and drain regions adjacent said spacers.
18. The semiconductor gate of claim 11 wherein said low-K dielectric layer extends over at least a portion of said lightly doped source and drain regions.
19. The semiconductor gate of claim 17 wherein said high-K dielectric layer extends a distance of within 10% of the length of said lightly doped source and drain regions
20. The semiconductor gate of claim 17 wherein said high-K dielectric layer extends a distance of about the length of said lightly doped source and drain regions.
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SG200504604-0A SG137692A1 (en) 2001-01-26 2002-01-10 Method for forming variable-k gate dielectric
SG200200222A SG108291A1 (en) 2001-01-26 2002-01-10 Method for forming variable-k gate dielectric
AT02368011T ATE326768T1 (en) 2001-01-26 2002-01-25 METHOD FOR PRODUCING A GATE DIELECTRIC WITH A VARIABLE DILECTRIC CONSTANT
DE60211396T DE60211396T2 (en) 2001-01-26 2002-01-25 A method of fabricating a variable dielectric constant gate dielectric
JP2002016958A JP4255235B2 (en) 2001-01-26 2002-01-25 Method for manufacturing gate dielectric
EP02368011A EP1227513B1 (en) 2001-01-26 2002-01-25 Method for forming variable-K gate dielectric
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EP1227513B1 (en) 2006-05-17
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DE60211396T2 (en) 2007-05-03

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