A Study of an Organic Bottom Antireflective Coating for 157-nm Lithography
In 157-nm lithography, an organic bottom-antireflective-coating (BARC), which has been mainly used as an antireflective technology in KrF or ArF lithography, is needed to reduce reflection from the substrate under the resist. To apply a conventional BARC to 157-nm lithography, the BARC thickness mus...
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Veröffentlicht in: | Journal of Photopolymer Science and Technology 2003, Vol.16(4), pp.565-572 |
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description | In 157-nm lithography, an organic bottom-antireflective-coating (BARC), which has been mainly used as an antireflective technology in KrF or ArF lithography, is needed to reduce reflection from the substrate under the resist. To apply a conventional BARC to 157-nm lithography, the BARC thickness must be less than that used in KrF or ArF lithography. This is because conventional BARCs have a lower dry-etching rate than resists with a fluorinated polymer resist for 157-nm lithography and the thickness of the remaining resist after BARC dry-etching may be greatly reduced. Moreover, the substrate reflection under a conventional thin BARC cannot be completely controlled since the k-value of the extinction coefficient at a 157-nm wavelength is small. Therefore, a BARC material for 157-nm lithography must have a higher k-value at the 157-nm wavelength, a higher dry-etching rate than resists with a fluorinated polymer, good matching between the fluorinated resist and the BARC material to ensure a good resist pattern shape, and low outgassing from the BARC material during exposure. In this paper, we evaluate newly developed BARC materials for 157-nm lithography. We found that the k-value of one new BARC material (NCA660) was 0.41 (1.6 times that of a conventional BARC (DUV30J; Brewer Science, Inc)), and the ratio of the dry-etching rate to that of a KrF resist was 2.0 (twice that of DUV30J). These improvements were achieved by introducing a chromophore containing an I-atom of halogen into a heterocyclic polymer. Furthermore, the film thickness loss (used to evaluate outgassing from this BARC material when irradiated by 157-nm light) was close to 0 nm (irradiation condition: 100 mJ/cm2), and a resist pattern with no footing was obtained in four typical kinds of fluorinated resist on this BARC material. We concluded that this BARC material was suitable for 157-nm lithography. |
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To apply a conventional BARC to 157-nm lithography, the BARC thickness must be less than that used in KrF or ArF lithography. This is because conventional BARCs have a lower dry-etching rate than resists with a fluorinated polymer resist for 157-nm lithography and the thickness of the remaining resist after BARC dry-etching may be greatly reduced. Moreover, the substrate reflection under a conventional thin BARC cannot be completely controlled since the k-value of the extinction coefficient at a 157-nm wavelength is small. Therefore, a BARC material for 157-nm lithography must have a higher k-value at the 157-nm wavelength, a higher dry-etching rate than resists with a fluorinated polymer, good matching between the fluorinated resist and the BARC material to ensure a good resist pattern shape, and low outgassing from the BARC material during exposure. In this paper, we evaluate newly developed BARC materials for 157-nm lithography. We found that the k-value of one new BARC material (NCA660) was 0.41 (1.6 times that of a conventional BARC (DUV30J; Brewer Science, Inc)), and the ratio of the dry-etching rate to that of a KrF resist was 2.0 (twice that of DUV30J). These improvements were achieved by introducing a chromophore containing an I-atom of halogen into a heterocyclic polymer. Furthermore, the film thickness loss (used to evaluate outgassing from this BARC material when irradiated by 157-nm light) was close to 0 nm (irradiation condition: 100 mJ/cm2), and a resist pattern with no footing was obtained in four typical kinds of fluorinated resist on this BARC material. We concluded that this BARC material was suitable for 157-nm lithography.</description><identifier>ISSN: 0914-9244</identifier><identifier>EISSN: 1349-6336</identifier><identifier>DOI: 10.2494/photopolymer.16.565</identifier><language>eng</language><publisher>Hiratsuka: The Society of Photopolymer Science and Technology(SPST)</publisher><subject>157-nm lithography ; Bottom-antireflective-coating ; dry-etching rate ; fluorinated resist ; halogen atom ; optical constants ; outgassing ; resist pattern shape</subject><ispartof>Journal of Photopolymer Science and Technology, 2003, Vol.16(4), pp.565-572</ispartof><rights>2003 The Society of Photopolymer Science and Technology (SPST)</rights><rights>Copyright Japan Science and Technology Agency 2003</rights><oa>free_for_read</oa><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c533t-109a6130a363a3dd16c5eb95c4e1dfd33a488763d55338466a5864407190b9413</citedby><cites>FETCH-LOGICAL-c533t-109a6130a363a3dd16c5eb95c4e1dfd33a488763d55338466a5864407190b9413</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>314,776,780,1877,27901,27902</link.rule.ids></links><search><creatorcontrib>Irie, Shigeo</creatorcontrib><creatorcontrib>Shigematsu, Masato</creatorcontrib><creatorcontrib>Sakamoto, Rikimaru</creatorcontrib><creatorcontrib>Mizusawa, Kenichi</creatorcontrib><creatorcontrib>Nakajima, Yasuyuki</creatorcontrib><creatorcontrib>Itani, Toshiro</creatorcontrib><title>A Study of an Organic Bottom Antireflective Coating for 157-nm Lithography</title><title>Journal of Photopolymer Science and Technology</title><addtitle>J. Photopol. Sci. Technol.</addtitle><description>In 157-nm lithography, an organic bottom-antireflective-coating (BARC), which has been mainly used as an antireflective technology in KrF or ArF lithography, is needed to reduce reflection from the substrate under the resist. To apply a conventional BARC to 157-nm lithography, the BARC thickness must be less than that used in KrF or ArF lithography. This is because conventional BARCs have a lower dry-etching rate than resists with a fluorinated polymer resist for 157-nm lithography and the thickness of the remaining resist after BARC dry-etching may be greatly reduced. Moreover, the substrate reflection under a conventional thin BARC cannot be completely controlled since the k-value of the extinction coefficient at a 157-nm wavelength is small. Therefore, a BARC material for 157-nm lithography must have a higher k-value at the 157-nm wavelength, a higher dry-etching rate than resists with a fluorinated polymer, good matching between the fluorinated resist and the BARC material to ensure a good resist pattern shape, and low outgassing from the BARC material during exposure. In this paper, we evaluate newly developed BARC materials for 157-nm lithography. We found that the k-value of one new BARC material (NCA660) was 0.41 (1.6 times that of a conventional BARC (DUV30J; Brewer Science, Inc)), and the ratio of the dry-etching rate to that of a KrF resist was 2.0 (twice that of DUV30J). These improvements were achieved by introducing a chromophore containing an I-atom of halogen into a heterocyclic polymer. Furthermore, the film thickness loss (used to evaluate outgassing from this BARC material when irradiated by 157-nm light) was close to 0 nm (irradiation condition: 100 mJ/cm2), and a resist pattern with no footing was obtained in four typical kinds of fluorinated resist on this BARC material. We concluded that this BARC material was suitable for 157-nm lithography.</description><subject>157-nm lithography</subject><subject>Bottom-antireflective-coating</subject><subject>dry-etching rate</subject><subject>fluorinated resist</subject><subject>halogen atom</subject><subject>optical constants</subject><subject>outgassing</subject><subject>resist pattern shape</subject><issn>0914-9244</issn><issn>1349-6336</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2003</creationdate><recordtype>article</recordtype><recordid>eNplkEFLwzAUx4MoOKefwEvAc2ey95I1xznUKYMd1HPI0rTraJuaZkK_vZXKELz83-X_e4_3I-SWs9kcFd63ex9966u-dmHG5UxIcUYmHFAlEkCekwlTHBM1R7wkV113YAxACDUhr0v6Fo9ZT31OTUO3oTBNaemDj9HXdNnEMri8cjaWX46uvIllU9DcB8rFImlquinj3hfBtPv-mlzkpurcze-cko-nx_fVOtlsn19Wy01iBUBMOFNGcmAGJBjIMi6tcDslLDqe5RmAwTRdSMjEUE9RSiNSicgWXLGdQg5TcjfubYP_PLou6oM_hmY4qTkiSmDzIaYExpYNvuuGJ3QbytqEXnOmf6Tpv9I0l3qQNlDrkTp00RTuxJgQS1u5fwyOMaCnit2boF0D3-z9fJA</recordid><startdate>20030101</startdate><enddate>20030101</enddate><creator>Irie, Shigeo</creator><creator>Shigematsu, Masato</creator><creator>Sakamoto, Rikimaru</creator><creator>Mizusawa, Kenichi</creator><creator>Nakajima, Yasuyuki</creator><creator>Itani, Toshiro</creator><general>The Society of Photopolymer Science and Technology(SPST)</general><general>Japan Science and Technology Agency</general><scope>AAYXX</scope><scope>CITATION</scope><scope>7SP</scope><scope>7SR</scope><scope>7U5</scope><scope>8FD</scope><scope>JG9</scope><scope>L7M</scope></search><sort><creationdate>20030101</creationdate><title>A Study of an Organic Bottom Antireflective Coating for 157-nm Lithography</title><author>Irie, Shigeo ; Shigematsu, Masato ; Sakamoto, Rikimaru ; Mizusawa, Kenichi ; Nakajima, Yasuyuki ; Itani, Toshiro</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c533t-109a6130a363a3dd16c5eb95c4e1dfd33a488763d55338466a5864407190b9413</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2003</creationdate><topic>157-nm lithography</topic><topic>Bottom-antireflective-coating</topic><topic>dry-etching rate</topic><topic>fluorinated resist</topic><topic>halogen atom</topic><topic>optical constants</topic><topic>outgassing</topic><topic>resist pattern shape</topic><toplevel>online_resources</toplevel><creatorcontrib>Irie, Shigeo</creatorcontrib><creatorcontrib>Shigematsu, Masato</creatorcontrib><creatorcontrib>Sakamoto, Rikimaru</creatorcontrib><creatorcontrib>Mizusawa, Kenichi</creatorcontrib><creatorcontrib>Nakajima, Yasuyuki</creatorcontrib><creatorcontrib>Itani, Toshiro</creatorcontrib><collection>CrossRef</collection><collection>Electronics & Communications Abstracts</collection><collection>Engineered Materials Abstracts</collection><collection>Solid State and Superconductivity Abstracts</collection><collection>Technology Research Database</collection><collection>Materials Research Database</collection><collection>Advanced Technologies Database with Aerospace</collection><jtitle>Journal of Photopolymer Science and Technology</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Irie, Shigeo</au><au>Shigematsu, Masato</au><au>Sakamoto, Rikimaru</au><au>Mizusawa, Kenichi</au><au>Nakajima, Yasuyuki</au><au>Itani, Toshiro</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>A Study of an Organic Bottom Antireflective Coating for 157-nm Lithography</atitle><jtitle>Journal of Photopolymer Science and Technology</jtitle><addtitle>J. Photopol. Sci. Technol.</addtitle><date>2003-01-01</date><risdate>2003</risdate><volume>16</volume><issue>4</issue><spage>565</spage><epage>572</epage><pages>565-572</pages><issn>0914-9244</issn><eissn>1349-6336</eissn><abstract>In 157-nm lithography, an organic bottom-antireflective-coating (BARC), which has been mainly used as an antireflective technology in KrF or ArF lithography, is needed to reduce reflection from the substrate under the resist. To apply a conventional BARC to 157-nm lithography, the BARC thickness must be less than that used in KrF or ArF lithography. This is because conventional BARCs have a lower dry-etching rate than resists with a fluorinated polymer resist for 157-nm lithography and the thickness of the remaining resist after BARC dry-etching may be greatly reduced. Moreover, the substrate reflection under a conventional thin BARC cannot be completely controlled since the k-value of the extinction coefficient at a 157-nm wavelength is small. Therefore, a BARC material for 157-nm lithography must have a higher k-value at the 157-nm wavelength, a higher dry-etching rate than resists with a fluorinated polymer, good matching between the fluorinated resist and the BARC material to ensure a good resist pattern shape, and low outgassing from the BARC material during exposure. In this paper, we evaluate newly developed BARC materials for 157-nm lithography. We found that the k-value of one new BARC material (NCA660) was 0.41 (1.6 times that of a conventional BARC (DUV30J; Brewer Science, Inc)), and the ratio of the dry-etching rate to that of a KrF resist was 2.0 (twice that of DUV30J). These improvements were achieved by introducing a chromophore containing an I-atom of halogen into a heterocyclic polymer. Furthermore, the film thickness loss (used to evaluate outgassing from this BARC material when irradiated by 157-nm light) was close to 0 nm (irradiation condition: 100 mJ/cm2), and a resist pattern with no footing was obtained in four typical kinds of fluorinated resist on this BARC material. We concluded that this BARC material was suitable for 157-nm lithography.</abstract><cop>Hiratsuka</cop><pub>The Society of Photopolymer Science and Technology(SPST)</pub><doi>10.2494/photopolymer.16.565</doi><tpages>8</tpages><oa>free_for_read</oa></addata></record> |
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subjects | 157-nm lithography Bottom-antireflective-coating dry-etching rate fluorinated resist halogen atom optical constants outgassing resist pattern shape |
title | A Study of an Organic Bottom Antireflective Coating for 157-nm Lithography |
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