Reliability of BCB passivated InAlAs/InGaAs HEMTs under thermal stress

D. Kim, M. Yoon, T. Kim, K. Yang
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In this study, the photosensitiveBCB layer was applied to InAlAsiInGaAs HEMTs for passivation and their thermal reliability characteristics were investigated and compared with the S i N x and polyimidepassivated devices for the first time. The designed HEMT layer structure is shown in Table I. For device fabrication, the mesa was defined by wet chemical etching. For ohmic contacts, AuGeiNiiAu were evaporated and alloyed resulting in a contact resistance of 0.085C2mm The thickness of Ni layer was optimized to have a minimum resistance variation during the thermal stress [4]. The conventional succinic acidHZOz solution was used for mesa-sidewall and gate recess etching. The Schottky gate was formed by evaporation of TUAu metal. The fabricated unpassivated-HEMTs with a 1.2pm gatelength showed good pinch-off characteristics with V, of -0.W and a maximum DC-transconductance g, of 398 mS/mm as shown in Fig. 1. The peak fr and f, measured at Vb=2.5V, estimated 60m -2OdB/decade extrapolation, were 25.7GHz and 53.1GH2, respectively. For fair comparison, the devices having I . , and g, variations within 5% were chosen and passivated by S N X (SiN-HEMT), polyimide (PI-HEMT) and BCB (BCB-HEMT). A 9Onm SiN. was deposited with Si”H,/He gas mixtures using an RPCVD for the SiN-HEMT. For the PIand BCB-HEMT, the polyimide and photosensitive-BCB were spin coated and cured at 200°C during 3Omin in nitrogen atmosphere, respectively. The devices were fmt characterized prior to thermal stressing, and during thermal stressing at 200°C for a period of 1006rs. The devices were not biased and were exposed to air in a closed oven during thermal stress. As shown in Fig. 1, g, is reduced by 5.6% in the BCB-HEMT and that of PI-HEMT is reduced by 4.5% after passivation. Compared to the PIand BCB-HEMT, the g, degadation in the SWHEMT (25%) at a high V, is significant due to the surface modification by the inherent CVD RF damage [5]. In all cases, some degradation of DC-characteristics was observed after passivation due to the increase of access resistance as shown in Fig. 3. Id and g, variation during thermal stress are shown in Fig. 2. Id and degradation of the SiN-HEMT were recovered by stabilition bake [I], whereas the PI-HEMT showed most severe degradation. The BCB-HEMT showed most stable DC-characteristics during thermal stress. In order to investigate the effect on thermal stability, parameter extraction was performed and analyzed based on the measured S-parameters. As shown in Fig. 3, the variation of increased ohmic resistance in the BCB-HEMT is minimal due to the low moisture uptakeand low barrier oxidationcharacteristics of BCB. Cutoff 6quencies of the fabricated devices were also characterized to determine the impact on the microwave performance as shown in Fig. 4. The fr of devices showed a similar behavior to that of &during thermal stress according to its relation to &. The f,, of the PI-HEMT is dramatically degraded after thermal stress, so polyimide is thought to be inadequate for passivation of InAlAslInGaAs HEMT. In an initial stage of thermal test, the BCBand SN-HEMT, having suppressed leakage path, showed enhanced f , , values resulting from the increased output resistance of rb by 33% and 43% for 24hrs’ test, respectively. After thermal stress of lOOhrs, degradation off& was observed for both devices and it was affected by g, rather than r&. In summary, JnAIAs/lnGaAs HEMTs passivated by different dielectric materials were fabricated and their performances were investigated prior to thermal stress and during thermal stress. The SiNxand BCB-passivated HEMTs show good device characteristics during reliability test. However, the BCB-passivated HEMTs have distinct advantages of much simpler fabrication process and reduced surface damages together with good thermal stability, sufficient for consideration as an attractive alternative to the conventional SiNx passivation technique.","PeriodicalId":404065,"journal":{"name":"2003 International Symposium on Compound Semiconductors","volume":"1 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"2003-10-27","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"2","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"2003 International Symposium on Compound Semiconductors","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1109/ISCS.2003.1239990","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 2

Abstract

InP-based HEMTs have been regarded as promising devices for ultra-high speed applications [I]. For practical system applications, the device reliability is one of the most critical issues. Extensive works have been done on the reliability of AIGaAs/(In)GaAs pHEMTs and InP-based HEMTs [I-21. Recently, the device performance improvement of benzocyclobutene (BCB) passivated GaAs pHEMT has been reported demonstrating the advantages of its low dielectric constant and a low loss tangent of BCB [3]. But, up to date, there has been no report on the reliability study on BCB passivated InP-based HEMTs to our knowledge. In this study, the photosensitiveBCB layer was applied to InAlAsiInGaAs HEMTs for passivation and their thermal reliability characteristics were investigated and compared with the S i N x and polyimidepassivated devices for the first time. The designed HEMT layer structure is shown in Table I. For device fabrication, the mesa was defined by wet chemical etching. For ohmic contacts, AuGeiNiiAu were evaporated and alloyed resulting in a contact resistance of 0.085C2mm The thickness of Ni layer was optimized to have a minimum resistance variation during the thermal stress [4]. The conventional succinic acidHZOz solution was used for mesa-sidewall and gate recess etching. The Schottky gate was formed by evaporation of TUAu metal. The fabricated unpassivated-HEMTs with a 1.2pm gatelength showed good pinch-off characteristics with V, of -0.W and a maximum DC-transconductance g, of 398 mS/mm as shown in Fig. 1. The peak fr and f, measured at Vb=2.5V, estimated 60m -2OdB/decade extrapolation, were 25.7GHz and 53.1GH2, respectively. For fair comparison, the devices having I . , and g, variations within 5% were chosen and passivated by S N X (SiN-HEMT), polyimide (PI-HEMT) and BCB (BCB-HEMT). A 9Onm SiN. was deposited with Si”H,/He gas mixtures using an RPCVD for the SiN-HEMT. For the PIand BCB-HEMT, the polyimide and photosensitive-BCB were spin coated and cured at 200°C during 3Omin in nitrogen atmosphere, respectively. The devices were fmt characterized prior to thermal stressing, and during thermal stressing at 200°C for a period of 1006rs. The devices were not biased and were exposed to air in a closed oven during thermal stress. As shown in Fig. 1, g, is reduced by 5.6% in the BCB-HEMT and that of PI-HEMT is reduced by 4.5% after passivation. Compared to the PIand BCB-HEMT, the g, degadation in the SWHEMT (25%) at a high V, is significant due to the surface modification by the inherent CVD RF damage [5]. In all cases, some degradation of DC-characteristics was observed after passivation due to the increase of access resistance as shown in Fig. 3. Id and g, variation during thermal stress are shown in Fig. 2. Id and degradation of the SiN-HEMT were recovered by stabilition bake [I], whereas the PI-HEMT showed most severe degradation. The BCB-HEMT showed most stable DC-characteristics during thermal stress. In order to investigate the effect on thermal stability, parameter extraction was performed and analyzed based on the measured S-parameters. As shown in Fig. 3, the variation of increased ohmic resistance in the BCB-HEMT is minimal due to the low moisture uptakeand low barrier oxidationcharacteristics of BCB. Cutoff 6quencies of the fabricated devices were also characterized to determine the impact on the microwave performance as shown in Fig. 4. The fr of devices showed a similar behavior to that of &during thermal stress according to its relation to &. The f,, of the PI-HEMT is dramatically degraded after thermal stress, so polyimide is thought to be inadequate for passivation of InAlAslInGaAs HEMT. In an initial stage of thermal test, the BCBand SN-HEMT, having suppressed leakage path, showed enhanced f , , values resulting from the increased output resistance of rb by 33% and 43% for 24hrs’ test, respectively. After thermal stress of lOOhrs, degradation off& was observed for both devices and it was affected by g, rather than r&. In summary, JnAIAs/lnGaAs HEMTs passivated by different dielectric materials were fabricated and their performances were investigated prior to thermal stress and during thermal stress. The SiNxand BCB-passivated HEMTs show good device characteristics during reliability test. However, the BCB-passivated HEMTs have distinct advantages of much simpler fabrication process and reduced surface damages together with good thermal stability, sufficient for consideration as an attractive alternative to the conventional SiNx passivation technique.
热应力下BCB钝化InAlAs/InGaAs hemt的可靠性
基于inp的hemt被认为是超高速应用的有前途的器件[I]。在实际系统应用中,器件可靠性是最关键的问题之一。在AIGaAs/(In)GaAs phemt和基于inp的hemt的可靠性方面已经做了大量的工作。最近,有报道称苯并环丁烯(BCB)钝化GaAs pHEMT的器件性能得到了改善,表明其具有低介电常数和BCB低损耗正切的优点[3]。但是,据我们所知,目前还没有关于BCB钝化inp基hemt可靠性研究的报道。在本研究中,光敏bcb层应用于InAlAsiInGaAs hemt进行钝化,并首次研究了其热可靠性特性,并与nsx和聚酰亚胺钝化器件进行了比较。所设计的HEMT层结构如表1所示。对于器件制造,台面由湿化学蚀刻确定。对于欧姆接触,将AuGeiNiiAu蒸发并合金化,得到0.085 5c2mm的接触电阻。优化Ni层的厚度,使其在热应力过程中电阻变化最小[4]。采用常规琥珀酸hzoz溶液进行台面、侧壁和栅极凹槽刻蚀。肖特基栅极是由TUAu金属蒸发形成的。制备的栅极长度为1.2pm的未钝化hemt在V = -0时表现出良好的掐断特性。W和最大直流跨导g,为398 mS/mm,如图1所示。在Vb=2.5V处测得的峰值fr和f分别为25.7GHz和53.1GH2,估计为60m -2OdB/ 10年外推。为了公平比较,带有I的设备。选择5%以内的变化,分别用sn X (SiN-HEMT)、聚酰亚胺(PI-HEMT)和BCB (BCB- hemt)钝化。A 9m SiN。使用RPCVD沉积Si”H,/He气体混合物,用于sinhemt。对于pib - hemt和BCB-HEMT,分别对聚酰亚胺和光敏- bcb进行自旋包覆,并在200℃、3Omin的氮气气氛中进行固化。器件在热应力之前和在200°C的1006rs的热应力期间进行了fmt表征。这些装置没有偏置,并且在热应力期间暴露在封闭的烤箱中。如图1所示,钝化后,BCB-HEMT的g降低了5.6%,PI-HEMT的g降低了4.5%。与pib - hemt和BCB-HEMT相比,SWHEMT在高电压下的g衰减(25%)非常明显,这是由于CVD固有的射频损伤对表面进行了修饰[5]。在所有情况下,钝化后由于接入电阻的增加,都观察到一些直流特性的退化,如图3所示。热应力过程中Id和g的变化如图2所示。稳定焙烧可恢复SiN-HEMT的Id和降解[1],而PI-HEMT的降解最为严重。BCB-HEMT在热应力作用下表现出最稳定的直流特性。为了研究其对热稳定性的影响,根据测量的s参数进行了参数提取和分析。如图3所示,由于BCB的低吸湿性和低屏障氧化特性,BCB- hemt中增加的欧姆电阻变化很小。还对所制备器件的截止频率进行了表征,以确定其对微波性能的影响,如图4所示。根据其与&的关系,在热应力作用下,器件的电流表现出与&相似的行为。PI-HEMT的f,在热应力后急剧降解,因此聚酰亚胺被认为不足以钝化InAlAslInGaAs HEMT。在热测试的初始阶段,由于bband SN-HEMT抑制了泄漏路径,在24hrs的测试中,由于rb的输出电阻分别增加了33%和43%,其f,,值有所提高。在lohrs的热应力作用下,两种器件都出现了退化现象,其影响因素是g而不是r。综上所述,制备了不同介电材料钝化的JnAIAs/lnGaAs hemt,并对其在热应力前和热应力过程中的性能进行了研究。在可靠性测试中,SiNxand bcb钝化hemt表现出良好的器件特性。然而,bcb钝化hemt具有明显的优点,制造工艺简单,表面损伤少,热稳定性好,足以作为传统SiNx钝化技术的有吸引力的替代方案。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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