WO2005052992A2 - Semiconductor device with silicided source/drains - Google Patents

Semiconductor device with silicided source/drains Download PDF

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Publication number
WO2005052992A2
WO2005052992A2 PCT/US2004/035546 US2004035546W WO2005052992A2 WO 2005052992 A2 WO2005052992 A2 WO 2005052992A2 US 2004035546 W US2004035546 W US 2004035546W WO 2005052992 A2 WO2005052992 A2 WO 2005052992A2
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WO
WIPO (PCT)
Prior art keywords
source
drain
implanting
atoms
activating
Prior art date
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Ceased
Application number
PCT/US2004/035546
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English (en)
French (fr)
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WO2005052992A3 (en
Inventor
Dharmesh Jawarani
Nigel G. Cave
Michael Renden
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NXP USA Inc
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Freescale Semiconductor Inc
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Priority to JP2006541193A priority Critical patent/JP2007512704A/ja
Publication of WO2005052992A2 publication Critical patent/WO2005052992A2/en
Publication of WO2005052992A3 publication Critical patent/WO2005052992A3/en
Anticipated expiration legal-status Critical
Ceased legal-status Critical Current

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Classifications

    • 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 potential barriers, e.g. a PN junction, depletion layer or carrier concentration layer
    • H01L21/18Manufacture or treatment of semiconductor devices or of parts thereof the devices having potential barriers, e.g. a PN junction, depletion layer or carrier concentration layer the devices having semiconductor bodies comprising elements of Group IV of the Periodic Table or AIIIBV compounds with or without impurities, e.g. doping materials
    • H01L21/26Bombardment with radiation
    • H01L21/263Bombardment with radiation with high-energy radiation
    • H01L21/265Bombardment with radiation with high-energy radiation producing ion implantation
    • H01L21/26506Bombardment with radiation with high-energy radiation producing ion implantation in group IV semiconductors
    • 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 potential barriers, e.g. a PN junction, depletion layer or carrier concentration layer
    • H01L21/18Manufacture or treatment of semiconductor devices or of parts thereof the devices having potential barriers, e.g. a PN junction, depletion layer or carrier concentration layer the devices having semiconductor bodies comprising elements of Group IV of the Periodic Table or AIIIBV compounds with or without impurities, e.g. doping materials
    • H01L21/24Alloying of impurity materials, e.g. doping materials, electrode materials, with a semiconductor body
    • 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 potential barriers, e.g. a PN junction, depletion layer or carrier concentration layer
    • H01L21/18Manufacture or treatment of semiconductor devices or of parts thereof the devices having potential barriers, e.g. a PN junction, depletion layer or carrier concentration layer the devices having semiconductor bodies comprising elements of Group IV of the Periodic Table or AIIIBV compounds with or without impurities, e.g. doping materials
    • 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 potential barriers, e.g. a PN junction, depletion layer or carrier concentration layer
    • H01L21/18Manufacture or treatment of semiconductor devices or of parts thereof the devices having potential barriers, e.g. a PN junction, depletion layer or carrier concentration layer the devices having semiconductor bodies comprising elements of Group IV of the Periodic Table or AIIIBV compounds with or without impurities, e.g. doping materials
    • H01L21/26Bombardment with radiation
    • H01L21/263Bombardment with radiation with high-energy radiation
    • H01L21/265Bombardment with radiation with high-energy radiation producing ion implantation
    • H01L21/2658Bombardment with radiation with high-energy radiation producing ion implantation of a molecular ion, e.g. decaborane
    • HELECTRICITY
    • H10SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
    • H10DINORGANIC ELECTRIC SEMICONDUCTOR DEVICES
    • H10D30/00Field-effect transistors [FET]
    • H10D30/01Manufacture or treatment
    • H10D30/021Manufacture or treatment of FETs having insulated gates [IGFET]
    • H10D30/0223Manufacture or treatment of FETs having insulated gates [IGFET] having source and drain regions or source and drain extensions self-aligned to sides of the gate
    • H10D30/0227Manufacture or treatment of FETs having insulated gates [IGFET] having source and drain regions or source and drain extensions self-aligned to sides of the gate having both lightly-doped source and drain extensions and source and drain regions self-aligned to the sides of the gate, e.g. lightly-doped drain [LDD] MOSFET or double-diffused drain [DDD] MOSFET
    • HELECTRICITY
    • H10SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
    • H10DINORGANIC ELECTRIC SEMICONDUCTOR DEVICES
    • H10D30/00Field-effect transistors [FET]
    • H10D30/01Manufacture or treatment
    • H10D30/021Manufacture or treatment of FETs having insulated gates [IGFET]
    • H10D30/0212Manufacture or treatment of FETs having insulated gates [IGFET] using self-aligned silicidation
    • HELECTRICITY
    • H10SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
    • H10DINORGANIC ELECTRIC SEMICONDUCTOR DEVICES
    • H10D64/00Electrodes of devices having potential barriers
    • H10D64/01Manufacture or treatment
    • H10D64/021Manufacture or treatment using multiple gate spacer layers, e.g. bilayered sidewall spacers

Definitions

  • This invention relates to semiconductor devices, and more particularly, to semiconductor devices with suicided source/drains.
  • semiconductor devices are made with lightly-doped drains at the junction with the channel and a relatively higher doped drain region used for making contact.
  • the sources are made in the same way.
  • the contact to the drain is made using a metal silicide. This contact is achieved by depositing the metal layer then reacting the metal layer with the silicon of the heavily-doped drain contact region to form a metal silicide contact region.
  • the unreacted metal which is located in the regions where there is no silicon, is then etched away with an etchant that is selective to the metal silicide. This metal silicide is then the contact point for the source and the drain of the semiconductor device.
  • One effective metal has been found to be cobalt.
  • Cobalt is effective but has been found to be difficult to use for very small poly silicon dimensions. Thus, with cobalt there have been problems with achieving reliable and continuous cobalt silicide formed on narrow poly silicon lines. This is even called the "line width effect.” Thus, other metals have been studied to overcome this problem.
  • One promising metal is nickel.
  • the use of nickel to form nickel silicide is effective for narrower line widths than have been found to be achievable for cobalt silicide.
  • a difficulty with nickel silicide has been the spiking of the nickel silicide to below the targeted depth in the form of inverted pyramids. The nickel atoms tend to continue to extend along a downward path that may extend below the drain.
  • the silicide structure is nickel disilicide.
  • the formation of this nickel disilicide has been particularly difficult to control for the semiconductor devices that are P channel transistors.
  • Dopant atoms, such as boron that are smaller than silicon atoms induce contraction of the silicon lattice. This causes the silicon substrate lattice to match with the lattice of the nickel disilicide thus causing nucleation of the nickel disilicide phase instead of the nickel monosilicide phase that would have formed had there been no lattice contraction.
  • there is a need for a technique for forming nickel silicide on source/drains that has improved manufacturability for P channel transistors.
  • FIGs. 1-7 are cross sections of a semiconductor device at sequential stages in processing according to an embodiment of the invention. Skilled artisans appreciate that elements in the figures are illustrated for simplicity and clarity and have not necessarily been drawn to scale. For example, the dimensions of some of the elements in the figures may be exaggerated relative to other elements to help improve the understanding of the embodiments of the present invention. Detailed Description of the Drawings In one aspect a relatively deep germanium implant and activation thereof precedes deposition of the nickel that is used to form nickel silicide.
  • the activation of the germanium causes the lattice constant in the region of the implant to be increased over the lattice constant of the background substrate, which is preferably silicon.
  • the effect is that the lattice so altered avoids formation of nickel disilicide.
  • the result is that nickel silicide spiking is avoided.
  • FIG. 1 Shown in FIG. 1 is a semiconductor device 10 comprising a semiconductor substrate 12, a gate 14 on a gate dielectric 16, and a liner 18 around gate 14 receiving a germanium implant.
  • the result of the implant and subsequent anneal is the formation of modified lattice regions 20 and 22.
  • Semiconductor device 10 is, in this example, being made into a P channel transistor.
  • Substrate 12 is preferably silicon doped to N- so as to form an N well region. This may be achieved by starting with a bulk P- substrate and selectively doping active regions to N- for formation of P channel transistors in which case substrate 12 is a well region within a larger substrate. Liner 18 is formed by an oxidation step. An antireflective coating (ARC), which is present for other reasons, prevents oxidation on the top of gate 14 and is then removed. Regions 20 and 22 are adjacent to gate 14, since gate 14 acts as a mask during germanium implant that forms regions 20 and 22. The region in substrate 12 between regions 20 and 22 is where the channel of the P channel transistor is to be located.
  • ARC antireflective coating
  • the stretched lattice has a spacing that is larger than that of nickel disilicide, which makes formation of nickel disilicide difficult.
  • the germanium implant in the present embodiment is preferably at least 3Kev at a dose of at least 10 to the 13 th (1E13) atoms per centimeter squared.
  • One example is lOKev at 1E15 atoms per centimeter square.
  • the energy should not exceed 50Kev, but it could be higher.
  • the dose preferably does not exceed 1E17 atoms per centimeter square but could be greater than that.
  • the anneal which causes the activation of the germanium, is preferably between 900 and 1400 degrees Celsius.
  • the activation can occur at an even lower temperature, such as 550 degrees Celsius.
  • One example of an effective anneal is 1050 degrees Celsius for 5 seconds.
  • Shown in FIG. 2 is device 10 after formation of sidewall spacer 24 around gate 14 and a source/drain implant of boron to form source/drain regions 26 and 28 using gate 14 and sidewall spacer 24 as a mask.
  • a boron implant may be in the form of boron difluoride. Most of the boron remains and most of the fluorine outgases during subsequent thermal processes. This implant is sometimes referred to as an extension implant.
  • extension source/drain regions 26 and 28 that are at the interface with the channel of the ultimate P channel transistor that is formed.
  • This formation of source/drain regions 26 and 28 are within modified lattice regions 20 and 22, respectively. But for the presence of regions 20 and 22, this formation of extension regions 26 and 28 is well known in the art of semiconductor processing.
  • Shown in FIG. 3 is device 10 after formation of sidewall spacer 30 around sidewall spacer 24 and a source/drain implant of boron to form source/drain contact regions 34 and 36 using gate 14, sidewall spacer 24, and sidewall spacer 30 as a mask.
  • Sidewall spacer 30 may be a composite of more than one layer. For example this could be an oxide layer followed by a nitride layer.
  • regions 34 and 36 extend below modified lattice regions 20 and 22.
  • the contact source/drain implant and the germanium implant will terminate at the interface of the semiconductor layer and the insulating layer that is below the semiconductor layer.
  • These source/drain contact regions 34 and 36 are also known as deep source/drains and, but for the presence of modified lattice regions 20 and 22, the formation of source/drain contact regions 34 and 36 is well known in the art of semiconductor processing. Shown in FIG. 4 is semiconductor device 10 after annealing the source/drain implants as shown in FIGs. 2 and 3. This activates these implants and has the effecting of expanding regions 26, 28, 34, and 36.
  • the extension regions, source/drain regions 26 and 28, expand to be at least aligned to the edges of gate 14.
  • the anneal will cause regions 28 and 36 and regions 26 and 34 to have a gradual change, if any, in doping concentration so they effectively merge into single regions.
  • FIG. 4 Shown in FIG. 5 is semiconductor device 10 after deposition of metal layer 38 that, in this example, is nickel. This layer 38 is in direct contact with source/drain regions 34 and 36, gate 14, and sidewall spacer 30.
  • semiconductor device 10 Shown in FIG. 6 is semiconductor device 10 after a heating step to cause the formation of nickel silicide where nickel layer 38 is in contact with silicon.
  • silicide region 40 over and in source/drain region 34, a silicide region 42 over and in source/drain region 36, and a silicide region 44 over and in gate 14.
  • These silicide regions 40, 42, and 44 are contacts that are effective for making an electrical connection as desired.
  • semiconductor device 10 after removal of the portion of layer 38 that was not suicided. This is achieved using an etchant, such as piranha, that is selective between the metal, which is nickel in this case, and the metal silicide, which is nickel silicide in this case. The device may then be subjected to an additional anneal to complete the silicide formation if so desired.
  • An alternative embodiment is to wait to perform the germanium implant until after the formation of the sidewall spacer that is used for the deep source/drain implant for making contacts.
  • the extension implant is performed prior to the germanium implant that forms the extension source/drain regions, the sidewall spacer for the deep source/drain implant is formed, and then the germanium implant is performed. This results in the germanium implant region being offset further from the channel than for regions 20 and 22 of FIG. 2.
  • the germanium implant is activated with a very short but high temperature anneal, which can be considered a non-diffusing anneal.
  • exemplary anneals are flash anneal and laser annealing. Flash annealing utilizes an arc lamp that provides very fast ramp rates for the heat. The intent is to increase the lattice constant in the area of the germanium implant without causing the extension regions to diffuse toward each other in the channel region.
  • the deep source/drain implant is performed. The lightly-doped and heavily-doped regions can then be activated using standard techniques for that.
  • the subsequent silicide formation is thus over a region in which the lattice constant has been increased to avoid the nickel silicide spiking.
  • the regions of increased lattice constant such as regions 20 and 22 which at least have portions in the source/drain contact regions, are useful in preventing spiking of nickel silicide and may be effective for preventing the spiking or the encroachment of other metal silicides such as cobalt silicide.
  • the increased lattice constant regions in this described example are about 400 angstroms deep. It is preferred that the depth be greater than the silicide depth. Thus, the preferred smallest depth is at least the depth of the silicide. A greater depth than 400 angstroms should be effective as well.
  • Activation of the germanium to form modified lattice regions 20 and 22 may occur at any time prior to formation of the silicide regions, but it is preferred that it occur before the implanting of the source/drain regions 26, 28, 34, and 36. Delaying the activation of the modified lattice regions 20 and 22 until after the source/drain implants causes competition with the source/drain implant dopants for the lattice sites. This can result in the lattice not being sufficiently modified to achieve the desired effect. Germanium has been found to be effective in avoiding spiking but other implanted materials may be effective as well.
  • other materials that may be effective include gallium, arsenic, indium, tin, antimony, thallium, lead, bismuth, zinc, cadmium, mercury, selenium, tellurium, and polonium. These materials all have a larger atomic radius than silicon and are in group II, III, IV, V, or VI, which are known to be able to be activated and occupy substitutional sites in a silicon lattice. In order to increase the lattice constant, any of these species or any combination of these species can be used to achieve the desired result.
  • the invention has been described with reference to specific embodiments.
  • the source/drain contact regions may be in a region that is elevated above the plane of the substrate. These are called elevated source/drains. In such case the implant into the source/drain contact region to increase the lattice constant will be into the elevated region and the silicide will be formed on the elevated regions as well. Accordingly, the specification and figures are to be regarded in an illustrative rather than a restrictive sense, and all such modifications are intended to be included within the scope of the present invention.

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  • Physics & Mathematics (AREA)
  • Engineering & Computer Science (AREA)
  • High Energy & Nuclear Physics (AREA)
  • Microelectronics & Electronic Packaging (AREA)
  • Condensed Matter Physics & Semiconductors (AREA)
  • General Physics & Mathematics (AREA)
  • Manufacturing & Machinery (AREA)
  • Computer Hardware Design (AREA)
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  • Spectroscopy & Molecular Physics (AREA)
  • Electrodes Of Semiconductors (AREA)
  • Insulated Gate Type Field-Effect Transistor (AREA)
PCT/US2004/035546 2003-11-21 2004-10-26 Semiconductor device with silicided source/drains Ceased WO2005052992A2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP2006541193A JP2007512704A (ja) 2003-11-21 2004-10-26 シリサイドをソース/ドレインに用いた半導体素子

Applications Claiming Priority (2)

Application Number Priority Date Filing Date Title
US10/718,892 US7262105B2 (en) 2003-11-21 2003-11-21 Semiconductor device with silicided source/drains
US10/718,892 2003-11-21

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WO2005052992A2 true WO2005052992A2 (en) 2005-06-09
WO2005052992A3 WO2005052992A3 (en) 2005-10-20

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US (1) US7262105B2 (enExample)
JP (1) JP2007512704A (enExample)
KR (1) KR20060126972A (enExample)
CN (1) CN1883042A (enExample)
WO (1) WO2005052992A2 (enExample)

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JP2005294360A (ja) * 2004-03-31 2005-10-20 Nec Electronics Corp 半導体装置の製造方法
US7253071B2 (en) * 2004-06-02 2007-08-07 Taiwan Semiconductor Manufacturing Company Methods for enhancing the formation of nickel mono-silicide by reducing the formation of nickel di-silicide
US20090162966A1 (en) * 2007-12-21 2009-06-25 The Woodside Group Pte Ltd Structure and method of formation of a solar cell
US20090159111A1 (en) * 2007-12-21 2009-06-25 The Woodside Group Pte. Ltd Photovoltaic device having a textured metal silicide layer
JP2009182089A (ja) * 2008-01-30 2009-08-13 Panasonic Corp 半導体装置の製造方法
US8178430B2 (en) 2009-04-08 2012-05-15 International Business Machines Corporation N-type carrier enhancement in semiconductors
CN102867748B (zh) 2011-07-06 2015-09-23 中国科学院微电子研究所 一种晶体管及其制作方法和包括该晶体管的半导体芯片
US8648412B1 (en) 2012-06-04 2014-02-11 Semiconductor Components Industries, Llc Trench power field effect transistor device and method
CN117712162A (zh) * 2022-09-08 2024-03-15 联华电子股份有限公司 N型金属氧化物半导体晶体管及其制作方法

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JP2947654B2 (ja) * 1990-10-31 1999-09-13 キヤノン株式会社 Mis型トランジスタ
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JP3156436B2 (ja) * 1993-04-05 2001-04-16 日本電気株式会社 ヘテロ接合バイポーラトランジスタ
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Also Published As

Publication number Publication date
KR20060126972A (ko) 2006-12-11
US20050112829A1 (en) 2005-05-26
WO2005052992A3 (en) 2005-10-20
US7262105B2 (en) 2007-08-28
CN1883042A (zh) 2006-12-20
JP2007512704A (ja) 2007-05-17

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