Low temperature epitaxy of tensile-strained Si:P

•550 °C epitaxy of tensile SiP. with disilane and phosphine.•Various strategies evaluated to obtain low resistivities and high [P]subst.•High phosphine to disilane mass-flow, low H2 carrier flow and high pressure.•Smooth and uniform t-Si:P layers with a substitutional P concentration of 6.3%.•Electr...

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Veröffentlicht in:Journal of crystal growth 2022-03, Vol.582, p.126543, Article 126543
Hauptverfasser: Hartmann, J.M., Kanyandekwe, J.
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description •550 °C epitaxy of tensile SiP. with disilane and phosphine.•Various strategies evaluated to obtain low resistivities and high [P]subst.•High phosphine to disilane mass-flow, low H2 carrier flow and high pressure.•Smooth and uniform t-Si:P layers with a substitutional P concentration of 6.3%.•Electrical resistivity much lower than with a chlorinated chemistry. Our long-term aim was to explore the Low Temperature Cyclic Deposition/Etch (CDE) of tensile-Si:P, in order to engineer the Sources and Drains of n-type Field Effect Transistors. We wanted to have high amounts of tensile strain and low resistivities in tensile Si:P layers grown at 550 °C, with (i) mainstream Si2H6 + PH3 gases for the non-selective deposition of t-Si:P and (ii) HCl + GeH4 for the selective etches of amorphous-Si:P versus monocrystalline Si:P (to have selectivity on patterned wafers). In the current study, we have focused on the deposition in such processes, having shown beforehand that, indeed, t-Si:P could be etched at 550 °C with HCl + GeH4 if the process conditions were right (Hartmann J.M. and Veillerot M., 2020 Semicond. Sci. Technol. 35 015015). Thanks to (i) high F(PH3)/(2*F(Si2H6)) Mass-Flow Ratios (MFR), (ii) a reduction of the H2 carrier flow, from the reference value of a few tens of standard liters per minute down to 1/5th of it and (iii) a chamber pressure increase, from 20 Torr up to 90 Torr, we succeeded in dramatically increasing the “substitutional” P concentration. and reaching values as high as 7.9%. 40 Torr was the best pressure in order to simultaneously have (i) a high “substitutional” P concentration (6.3%), (ii) a reasonable t-Si:P growth rate (5.5 nm min−1) and (iii) a low electrical resistivity (0.41 mOhm·cm), without being hampered by a layer uniformity that would be too degraded to be of use in actual devices. Those t-Si:P layers, grown with a MFR of 0.46, were of superior crystalline quality (in X-Ray Diffraction) and smooth (from haze measurements).
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Our long-term aim was to explore the Low Temperature Cyclic Deposition/Etch (CDE) of tensile-Si:P, in order to engineer the Sources and Drains of n-type Field Effect Transistors. We wanted to have high amounts of tensile strain and low resistivities in tensile Si:P layers grown at 550 °C, with (i) mainstream Si2H6 + PH3 gases for the non-selective deposition of t-Si:P and (ii) HCl + GeH4 for the selective etches of amorphous-Si:P versus monocrystalline Si:P (to have selectivity on patterned wafers). In the current study, we have focused on the deposition in such processes, having shown beforehand that, indeed, t-Si:P could be etched at 550 °C with HCl + GeH4 if the process conditions were right (Hartmann J.M. and Veillerot M., 2020 Semicond. Sci. Technol. 35 015015). Thanks to (i) high F(PH3)/(2*F(Si2H6)) Mass-Flow Ratios (MFR), (ii) a reduction of the H2 carrier flow, from the reference value of a few tens of standard liters per minute down to 1/5th of it and (iii) a chamber pressure increase, from 20 Torr up to 90 Torr, we succeeded in dramatically increasing the “substitutional” P concentration. and reaching values as high as 7.9%. 40 Torr was the best pressure in order to simultaneously have (i) a high “substitutional” P concentration (6.3%), (ii) a reasonable t-Si:P growth rate (5.5 nm min−1) and (iii) a low electrical resistivity (0.41 mOhm·cm), without being hampered by a layer uniformity that would be too degraded to be of use in actual devices. 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Our long-term aim was to explore the Low Temperature Cyclic Deposition/Etch (CDE) of tensile-Si:P, in order to engineer the Sources and Drains of n-type Field Effect Transistors. We wanted to have high amounts of tensile strain and low resistivities in tensile Si:P layers grown at 550 °C, with (i) mainstream Si2H6 + PH3 gases for the non-selective deposition of t-Si:P and (ii) HCl + GeH4 for the selective etches of amorphous-Si:P versus monocrystalline Si:P (to have selectivity on patterned wafers). In the current study, we have focused on the deposition in such processes, having shown beforehand that, indeed, t-Si:P could be etched at 550 °C with HCl + GeH4 if the process conditions were right (Hartmann J.M. and Veillerot M., 2020 Semicond. Sci. Technol. 35 015015). Thanks to (i) high F(PH3)/(2*F(Si2H6)) Mass-Flow Ratios (MFR), (ii) a reduction of the H2 carrier flow, from the reference value of a few tens of standard liters per minute down to 1/5th of it and (iii) a chamber pressure increase, from 20 Torr up to 90 Torr, we succeeded in dramatically increasing the “substitutional” P concentration. and reaching values as high as 7.9%. 40 Torr was the best pressure in order to simultaneously have (i) a high “substitutional” P concentration (6.3%), (ii) a reasonable t-Si:P growth rate (5.5 nm min−1) and (iii) a low electrical resistivity (0.41 mOhm·cm), without being hampered by a layer uniformity that would be too degraded to be of use in actual devices. Those t-Si:P layers, grown with a MFR of 0.46, were of superior crystalline quality (in X-Ray Diffraction) and smooth (from haze measurements).</description><subject>A1. Crystal morphology</subject><subject>A1. Doping</subject><subject>A1. Stresses</subject><subject>A3. Chemical vapor deposition processes</subject><subject>B1. Germanium silicon alloys</subject><subject>B3. Field effect transistors</subject><subject>Deposition</subject><subject>Field effect transistors</subject><subject>Haze</subject><subject>Low temperature</subject><subject>Mass flow</subject><subject>Selectivity</subject><subject>Semiconductor devices</subject><subject>Tensile strain</subject><issn>0022-0248</issn><issn>1873-5002</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2022</creationdate><recordtype>article</recordtype><recordid>eNqFkE9LxDAQxYMouK5-BSl4bk0mbZp6Uhb_wYKCeg7ZdCopu01Nsup-e7NUz15mYHjvDe9HyDmjBaNMXPZFb_wuvHtXAAUoGIiq5AdkxmTN84pSOCSzNCGnUMpjchJCT2lyMjojdOm-soibEb2OW48Zjjbq713munQegl1jHqLXdsA2e7FXz6fkqNPrgGe_e07e7m5fFw_58un-cXGzzA2XMuarFddGy44zsdKN1MCNaHRdl8gNCJRCVrI0vDSikpIL2ZVNJbRs2hZqCrzhc3Ix5Y7efWwxRNW7rR_SSwWiprwBDiypxKQy3oXgsVOjtxvtd4pRtaejevVHR-3pqIlOMl5PRkwdPi16FYzFwWBrPZqoWmf_i_gB3Txvhg</recordid><startdate>20220315</startdate><enddate>20220315</enddate><creator>Hartmann, J.M.</creator><creator>Kanyandekwe, J.</creator><general>Elsevier B.V</general><general>Elsevier BV</general><scope>AAYXX</scope><scope>CITATION</scope><scope>7SR</scope><scope>7U5</scope><scope>8BQ</scope><scope>8FD</scope><scope>JG9</scope><scope>L7M</scope></search><sort><creationdate>20220315</creationdate><title>Low temperature epitaxy of tensile-strained Si:P</title><author>Hartmann, J.M. ; Kanyandekwe, J.</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c388t-bb3aca8f316ba98a23c69a774e3c26e868584c34c6588368f4956a89dd2702393</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2022</creationdate><topic>A1. Crystal morphology</topic><topic>A1. Doping</topic><topic>A1. Stresses</topic><topic>A3. Chemical vapor deposition processes</topic><topic>B1. Germanium silicon alloys</topic><topic>B3. Field effect transistors</topic><topic>Deposition</topic><topic>Field effect transistors</topic><topic>Haze</topic><topic>Low temperature</topic><topic>Mass flow</topic><topic>Selectivity</topic><topic>Semiconductor devices</topic><topic>Tensile strain</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Hartmann, J.M.</creatorcontrib><creatorcontrib>Kanyandekwe, J.</creatorcontrib><collection>CrossRef</collection><collection>Engineered Materials Abstracts</collection><collection>Solid State and Superconductivity Abstracts</collection><collection>METADEX</collection><collection>Technology Research Database</collection><collection>Materials Research Database</collection><collection>Advanced Technologies Database with Aerospace</collection><jtitle>Journal of crystal growth</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Hartmann, J.M.</au><au>Kanyandekwe, J.</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Low temperature epitaxy of tensile-strained Si:P</atitle><jtitle>Journal of crystal growth</jtitle><date>2022-03-15</date><risdate>2022</risdate><volume>582</volume><spage>126543</spage><pages>126543-</pages><artnum>126543</artnum><issn>0022-0248</issn><eissn>1873-5002</eissn><abstract>•550 °C epitaxy of tensile SiP. with disilane and phosphine.•Various strategies evaluated to obtain low resistivities and high [P]subst.•High phosphine to disilane mass-flow, low H2 carrier flow and high pressure.•Smooth and uniform t-Si:P layers with a substitutional P concentration of 6.3%.•Electrical resistivity much lower than with a chlorinated chemistry. Our long-term aim was to explore the Low Temperature Cyclic Deposition/Etch (CDE) of tensile-Si:P, in order to engineer the Sources and Drains of n-type Field Effect Transistors. We wanted to have high amounts of tensile strain and low resistivities in tensile Si:P layers grown at 550 °C, with (i) mainstream Si2H6 + PH3 gases for the non-selective deposition of t-Si:P and (ii) HCl + GeH4 for the selective etches of amorphous-Si:P versus monocrystalline Si:P (to have selectivity on patterned wafers). In the current study, we have focused on the deposition in such processes, having shown beforehand that, indeed, t-Si:P could be etched at 550 °C with HCl + GeH4 if the process conditions were right (Hartmann J.M. and Veillerot M., 2020 Semicond. Sci. Technol. 35 015015). Thanks to (i) high F(PH3)/(2*F(Si2H6)) Mass-Flow Ratios (MFR), (ii) a reduction of the H2 carrier flow, from the reference value of a few tens of standard liters per minute down to 1/5th of it and (iii) a chamber pressure increase, from 20 Torr up to 90 Torr, we succeeded in dramatically increasing the “substitutional” P concentration. and reaching values as high as 7.9%. 40 Torr was the best pressure in order to simultaneously have (i) a high “substitutional” P concentration (6.3%), (ii) a reasonable t-Si:P growth rate (5.5 nm min−1) and (iii) a low electrical resistivity (0.41 mOhm·cm), without being hampered by a layer uniformity that would be too degraded to be of use in actual devices. Those t-Si:P layers, grown with a MFR of 0.46, were of superior crystalline quality (in X-Ray Diffraction) and smooth (from haze measurements).</abstract><cop>Amsterdam</cop><pub>Elsevier B.V</pub><doi>10.1016/j.jcrysgro.2022.126543</doi><oa>free_for_read</oa></addata></record>
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subjects A1. Crystal morphology
A1. Doping
A1. Stresses
A3. Chemical vapor deposition processes
B1. Germanium silicon alloys
B3. Field effect transistors
Deposition
Field effect transistors
Haze
Low temperature
Mass flow
Selectivity
Semiconductor devices
Tensile strain
title Low temperature epitaxy of tensile-strained Si:P
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