Influence of the magnetron on the growth of aluminum nitride thin films deposited by reactive sputtering
Aluminum nitride (AlN) thin films deposited on high-vacuum systems without substrate heating generally exhibit a poor degree of c -axis orientation. This is due to the nonequilibrium conditions existing between the energy of the sputtered particles and the energy at the substrate surface. The applic...
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Published in: | Journal of vacuum science & technology. A, Vacuum, surfaces, and films Vol. 28; no. 2; pp. 193 - 198 |
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American Vacuum Society
01-03-2010
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Abstract | Aluminum nitride (AlN) thin films deposited on high-vacuum systems without substrate heating generally exhibit a poor degree of
c
-axis orientation. This is due to the nonequilibrium conditions existing between the energy of the sputtered particles and the energy at the substrate surface. The application of substrate bias or substrate temperature is known to improve the adatom mobility by delivering energy to the substrate; both are hence well-established crystal growth promoting factors. It is well known that low sputtering pressures can be used as a parameter improving the growth of highly
c
-axis oriented aluminum nitride films at room temperature even without applying bias voltage to the substrate. Generally, the use of high pressures implies thermalization of particles within the gas phase and is considered to increase the energy gap between these and the substrate surface. However, in later experiments we have learned that the use of high processing pressures does not necessarily implies a detriment of crystallographic orientation in the films. By measuring (for the first time to the author’s knowledge) the full width at half maximum value of the rocking curve of the 0002-AlN peak at several positions along the
100
mm
diameter (100)-silicon wafers on which aluminum nitride thin films were deposited by reactive sputtering, a new effect was observed. Under certain processing conditions, the growth of the AlN thin films is influenced by the target magnetron. More precisely, their degree of
c
-axis orientation varies at wafer areas locally coincident under the target magnetron. This effect should be considered, especially where large area substrates are employed such as in silicon wafer foundry manufacturing processes. |
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AbstractList | Aluminum nitride (AlN) thin films deposited on high-vacuum systems without substrate heating generally exhibit a poor degree of
c
-axis orientation. This is due to the nonequilibrium conditions existing between the energy of the sputtered particles and the energy at the substrate surface. The application of substrate bias or substrate temperature is known to improve the adatom mobility by delivering energy to the substrate; both are hence well-established crystal growth promoting factors. It is well known that low sputtering pressures can be used as a parameter improving the growth of highly
c
-axis oriented aluminum nitride films at room temperature even without applying bias voltage to the substrate. Generally, the use of high pressures implies thermalization of particles within the gas phase and is considered to increase the energy gap between these and the substrate surface. However, in later experiments we have learned that the use of high processing pressures does not necessarily implies a detriment of crystallographic orientation in the films. By measuring (for the first time to the author’s knowledge) the full width at half maximum value of the rocking curve of the 0002-AlN peak at several positions along the
100
mm
diameter (100)-silicon wafers on which aluminum nitride thin films were deposited by reactive sputtering, a new effect was observed. Under certain processing conditions, the growth of the AlN thin films is influenced by the target magnetron. More precisely, their degree of
c
-axis orientation varies at wafer areas locally coincident under the target magnetron. This effect should be considered, especially where large area substrates are employed such as in silicon wafer foundry manufacturing processes. Aluminum nitride (AlN) thin films deposited on high-vacuum systems without substrate heating generally exhibit a poor degree of c-axis orientation. This is due to the nonequilibrium conditions existing between the energy of the sputtered particles and the energy at the substrate surface. The application of substrate bias or substrate temperature is known to improve the adatom mobility by delivering energy to the substrate; both are hence well-established crystal growth promoting factors. It is well known that low sputtering pressures can be used as a parameter improving the growth of highly c-axis oriented aluminum nitride films at room temperature even without applying bias voltage to the substrate. Generally, the use of high pressures implies thermalization of particles within the gas phase and is considered to increase the energy gap between these and the substrate surface. However, in later experiments we have learned that the use of high processing pressures does not necessarily implies a detriment of crystallographic orientation in the films. By measuring (for the first time to the author’s knowledge) the full width at half maximum value of the rocking curve of the 0002-AlN peak at several positions along the 100mm diameter (100)-silicon wafers on which aluminum nitride thin films were deposited by reactive sputtering, a new effect was observed. Under certain processing conditions, the growth of the AlN thin films is influenced by the target magnetron. More precisely, their degree of c-axis orientation varies at wafer areas locally coincident under the target magnetron. This effect should be considered, especially where large area substrates are employed such as in silicon wafer foundry manufacturing processes. |
Author | Iriarte, G. F. |
Author_xml | – sequence: 1 givenname: G. F. surname: Iriarte fullname: Iriarte, G. F. email: gonzalo.fuentes@upm.es organization: ISOM-Universidad Politécnica de Madrid, Ciudad Universitaria s/n, E-28040 Madrid, Spain |
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CitedBy_id | crossref_primary_10_1088_1674_4926_43_2_022801 crossref_primary_10_1016_j_mssp_2020_105567 crossref_primary_10_1088_1674_4926_40_12_121801 crossref_primary_10_1088_1742_6596_1517_1_012104 crossref_primary_10_1007_s11664_017_5924_8 crossref_primary_10_1088_1361_6641_abe3c5 crossref_primary_10_1002_pssb_201700506 crossref_primary_10_1016_j_tsf_2012_10_015 crossref_primary_10_1016_j_jallcom_2024_174330 crossref_primary_10_1088_0256_307X_31_12_124302 |
Cites_doi | 10.1016/S0040-6090(00)01914-3 10.1063/1.356105 10.1016/j.jcrysgro.2004.11.421 10.1016/S0040-6090(95)06530-X 10.1103/PhysRevLett.60.112 10.1007/BF00324324 10.1557/JMR.2002.0218 10.1016/S0040-6090(99)00130-3 10.1016/j.tsf.2005.12.250 10.1063/1.111553 10.1116/1.580053 10.1063/1.1791753 10.1016/j.jcrysgro.2008.09.046 10.1080/00150199908210573 |
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Growth doi: 10.1016/j.jcrysgro.2008.09.046 – volume: 54–55 start-page: 167 year: 1992 ident: 2023062903251316600_c7 publication-title: Surf. Coat. Technol. – volume: 75 start-page: 3446 year: 1994 ident: 2023062903251316600_c13 publication-title: J. Appl. Phys. doi: 10.1063/1.356105 – volume: 18 start-page: 1733 year: 2003 ident: 2023062903251316600_c12 publication-title: J. Mater. Res. – volume: 276 start-page: 525 year: 2005 ident: 2023062903251316600_c16 publication-title: J. Cryst. Growth doi: 10.1016/j.jcrysgro.2004.11.421 – volume: 96 start-page: 4166 year: 2004 ident: 2023062903251316600_c20 publication-title: J. Appl. Phys. doi: 10.1063/1.1791753 – volume: 54 start-page: 481 year: 1992 ident: 2023062903251316600_c18 publication-title: Appl. Phys. A: Mater. Sci. Process. doi: 10.1007/BF00324324 – volume: 64 start-page: 166 year: 1994 ident: 2023062903251316600_c4 publication-title: Appl. Phys. Lett. doi: 10.1063/1.111553 – volume: 31 start-page: 513 year: 1994 ident: 2023062903251316600_c5 publication-title: Eur. J. Solid State Inorg. Chem. – volume: 515 start-page: 421 year: 2006 ident: 2023062903251316600_c11 publication-title: Thin Solid Films doi: 10.1016/j.tsf.2005.12.250 – volume: 17 start-page: 1469 year: 2002 ident: 2023062903251316600_c14 publication-title: J. Mater. Res. doi: 10.1557/JMR.2002.0218 – volume: 14 start-page: 2238 year: 1996 ident: 2023062903251316600_c8 publication-title: J. Vac. Sci. Technol. A doi: 10.1116/1.580053 – volume: 388 start-page: 62 year: 2001 ident: 2023062903251316600_c9 publication-title: Thin Solid Films doi: 10.1016/S0040-6090(00)01914-3 |
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Snippet | Aluminum nitride (AlN) thin films deposited on high-vacuum systems without substrate heating generally exhibit a poor degree of
c
-axis orientation. This is... Aluminum nitride (AlN) thin films deposited on high-vacuum systems without substrate heating generally exhibit a poor degree of c-axis orientation. This is due... |
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Title | Influence of the magnetron on the growth of aluminum nitride thin films deposited by reactive sputtering |
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