I. Mack, Kawa Rosta, U. Quliyeva, J. Ott, T. Pasanen, V. Vähänissi, Zahra Sadat Jahanshah Rad, J. Lehtiö, P. Laukkanen, C. Soldano, H. Savin
{"title":"量化Al沉积方法对Al2O3/Si界面质量的影响","authors":"I. Mack, Kawa Rosta, U. Quliyeva, J. Ott, T. Pasanen, V. Vähänissi, Zahra Sadat Jahanshah Rad, J. Lehtiö, P. Laukkanen, C. Soldano, H. Savin","doi":"10.1002/pssa.202200653","DOIUrl":null,"url":null,"abstract":"Oxide–semiconductor interface quality has often a direct impact on the electrical properties of devices and on their performance. Traditionally, the properties are characterized through metal–oxide–semiconductor (MOS) structures by depositing a metal layer and measuring the capacitance–voltage (C–V) characteristics. However, metal deposition process itself may have an impact on the oxide and the oxide–semiconductor interface. The impact of magnetron sputtering, e‐beam evaporation, and thermal evaporation on an A l 2 O 3 / S i interface is studied, where atomic layer deposited (ALD) A l 2 O 3 is used, by MOS C–V and corona oxide characterization of semiconductors (COCOS) measurements. The latter allows characterization of the interface also in its original state before metallization. The results show that sputtering induces significant damage at the underlying A l 2 O 3 / S i interface as the measured interface defect density D it increases from 10 11 to 10 13 cm−2 eV. Interestingly, sputtering also generates a high density of positive charges Q tot at the interface as the charge changes from − 2 × 10 12 to + 7 × 10 12 cm − 2 . Thermal evaporation is found to be a softer method, with modest impact on D it and Q tot . Finally, Alnealing heals the damage but has also a significant impact on the charge of the film recovering the characteristic negative charge of A l 2 O 3 (∼−4 × 1012 cm − 2 ).","PeriodicalId":87717,"journal":{"name":"Physica status solidi (A): Applied research","volume":"1 1","pages":""},"PeriodicalIF":0.0000,"publicationDate":"2023-08-31","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Quantifying the Impact of Al Deposition Method on Underlying Al2O3/Si Interface Quality\",\"authors\":\"I. Mack, Kawa Rosta, U. Quliyeva, J. Ott, T. Pasanen, V. Vähänissi, Zahra Sadat Jahanshah Rad, J. Lehtiö, P. Laukkanen, C. Soldano, H. Savin\",\"doi\":\"10.1002/pssa.202200653\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"Oxide–semiconductor interface quality has often a direct impact on the electrical properties of devices and on their performance. Traditionally, the properties are characterized through metal–oxide–semiconductor (MOS) structures by depositing a metal layer and measuring the capacitance–voltage (C–V) characteristics. However, metal deposition process itself may have an impact on the oxide and the oxide–semiconductor interface. The impact of magnetron sputtering, e‐beam evaporation, and thermal evaporation on an A l 2 O 3 / S i interface is studied, where atomic layer deposited (ALD) A l 2 O 3 is used, by MOS C–V and corona oxide characterization of semiconductors (COCOS) measurements. The latter allows characterization of the interface also in its original state before metallization. The results show that sputtering induces significant damage at the underlying A l 2 O 3 / S i interface as the measured interface defect density D it increases from 10 11 to 10 13 cm−2 eV. Interestingly, sputtering also generates a high density of positive charges Q tot at the interface as the charge changes from − 2 × 10 12 to + 7 × 10 12 cm − 2 . Thermal evaporation is found to be a softer method, with modest impact on D it and Q tot . Finally, Alnealing heals the damage but has also a significant impact on the charge of the film recovering the characteristic negative charge of A l 2 O 3 (∼−4 × 1012 cm − 2 ).\",\"PeriodicalId\":87717,\"journal\":{\"name\":\"Physica status solidi (A): Applied research\",\"volume\":\"1 1\",\"pages\":\"\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"2023-08-31\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Physica status solidi (A): Applied research\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.1002/pssa.202200653\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Physica status solidi (A): Applied research","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1002/pssa.202200653","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
Quantifying the Impact of Al Deposition Method on Underlying Al2O3/Si Interface Quality
Oxide–semiconductor interface quality has often a direct impact on the electrical properties of devices and on their performance. Traditionally, the properties are characterized through metal–oxide–semiconductor (MOS) structures by depositing a metal layer and measuring the capacitance–voltage (C–V) characteristics. However, metal deposition process itself may have an impact on the oxide and the oxide–semiconductor interface. The impact of magnetron sputtering, e‐beam evaporation, and thermal evaporation on an A l 2 O 3 / S i interface is studied, where atomic layer deposited (ALD) A l 2 O 3 is used, by MOS C–V and corona oxide characterization of semiconductors (COCOS) measurements. The latter allows characterization of the interface also in its original state before metallization. The results show that sputtering induces significant damage at the underlying A l 2 O 3 / S i interface as the measured interface defect density D it increases from 10 11 to 10 13 cm−2 eV. Interestingly, sputtering also generates a high density of positive charges Q tot at the interface as the charge changes from − 2 × 10 12 to + 7 × 10 12 cm − 2 . Thermal evaporation is found to be a softer method, with modest impact on D it and Q tot . Finally, Alnealing heals the damage but has also a significant impact on the charge of the film recovering the characteristic negative charge of A l 2 O 3 (∼−4 × 1012 cm − 2 ).