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  • 1
    In: IEEE Journal of Solid-State Circuits, Institute of Electrical and Electronics Engineers (IEEE), Vol. 45, No. 9 ( 2010-09), p. 1678-1686
    Materialart: Online-Ressource
    ISSN: 0018-9200 , 1558-173X
    Sprache: Unbekannt
    Verlag: Institute of Electrical and Electronics Engineers (IEEE)
    Publikationsdatum: 2010
    ZDB Id: 240580-5
    ZDB Id: 2040287-9
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  • 2
    In: ECS Transactions, The Electrochemical Society, Vol. 86, No. 7 ( 2018-07-20), p. 373-383
    Materialart: Online-Ressource
    ISSN: 1938-6737 , 1938-5862
    Sprache: Englisch
    Verlag: The Electrochemical Society
    Publikationsdatum: 2018
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  • 3
    In: ECS Transactions, The Electrochemical Society, Vol. 109, No. 4 ( 2022-09-30), p. 35-46
    Kurzfassung: In this work we present the progress in regard to the integration of a surface plasmon resonance refractive index sensor into a CMOS compatible 200 mm wafer silicon-based technology. Our approach pursues the combination of germanium photodetectors with metallic nanohole arrays. The paper is focused on the technology development to fabricate large area photodetectors based on a modern design concept. In a first iteration we achieved a leakage current density of 82 mA/cm 2 at reverse bias of 0.5 V and a maximum optical responsivity of 0.103 A/W measured with TE polarized light at λ = 1310 nm and a reversed bias of 1 V. For the realization of nanohole arrays we used thin Titanium nitride (TiN) layers deposited by a sputtering process. We were able to produce very homogenous TiN layers with a thickness deviation of around 10 % and RMS of 1.413 nm for 150 nm thick TiN layers.
    Materialart: Online-Ressource
    ISSN: 1938-5862 , 1938-6737
    Sprache: Unbekannt
    Verlag: The Electrochemical Society
    Publikationsdatum: 2022
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  • 4
    Online-Ressource
    Online-Ressource
    The Electrochemical Society ; 2011
    In:  ECS Transactions Vol. 35, No. 2 ( 2011-04-25), p. 95-104
    In: ECS Transactions, The Electrochemical Society, Vol. 35, No. 2 ( 2011-04-25), p. 95-104
    Kurzfassung: The formation of TSVs includes a deep Si trench etching and a formation of a dielectric layer along the high-aspect-ratio Si trench to isolate the filling conductive material from the bulk Si. The isolation of the filling conductor from the silicon substrate becomes more important for higher frequencies due to the high coupling to the silicon. The importance of the oxide thickness on the wall can be verified using electromagnetic simulators, such as HFSS®. A SA-CVD with a pulsed flow of ozone is developed and used to deposit an isolation oxide to the walls of deep silicon trenches. The technique provides a good coating of the 100µm depth silicon trenches with the high aspect ratio of 20. Developed technique allows covering the deep silicon trenches by oxide and makes the high isolation of TSVs from silicon substrate feasible which is the key for performance of TSVs for mm-wave 3D packaging.
    Materialart: Online-Ressource
    ISSN: 1938-5862 , 1938-6737
    Sprache: Unbekannt
    Verlag: The Electrochemical Society
    Publikationsdatum: 2011
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  • 5
    In: ECS Transactions, The Electrochemical Society, Vol. 92, No. 4 ( 2019-07-03), p. 211-221
    Materialart: Online-Ressource
    ISSN: 1938-6737 , 1938-5862
    Sprache: Englisch
    Verlag: The Electrochemical Society
    Publikationsdatum: 2019
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  • 6
    In: physica status solidi c, Wiley, Vol. 14, No. 12 ( 2017-12)
    Kurzfassung: We use a wide variety of analytical methods to characterize nanometer‐sized oxygen precipitates in highly B‐doped Czochralski (CZ) silicon. Due to the enhanced precipitation of oxygen in this type of wafer, the precipitate density reaches a value of 1 × 10 13  cm −3 already after short annealing. On the one hand, this provides an excellent possibility for testing the detection limits of different methods and on the other hand the knowledge on oxygen precipitation in p + material can be broadened. In order to study density, size, and morphology of oxygen precipitates, we exploit scanning transmission microscopy (STEM), reactive ion etching (RIE), and preferential etching. STEM is also used to determine size distribution and energy dispersive X‐ray spectroscopy (EDX) and electron energy loss spectroscopy (EELS) are used to investigate the composition of oxygen precipitates. In annealed samples, oxygen precipitates, dislocation loops, and stacking faults are found. The dislocation loops disappear after long annealing in contrast to the stacking faults which are detected in all samples annealed at 1000 °C. It is found that the long anneal at 1000 °C leads to the formation of two size fractions of precipitates. This process is similar to Ostwald ripening. The precipitates are octahedral, consist of SiO 2 and the B concentration is below the detection limit of the methods used here. The obtained results are in good agreement with the nucleation model of highly doped wafers proposed by Sueoka.
    Materialart: Online-Ressource
    ISSN: 1862-6351 , 1610-1642
    URL: Issue
    Sprache: Englisch
    Verlag: Wiley
    Publikationsdatum: 2017
    ZDB Id: 2105580-4
    ZDB Id: 2102966-0
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  • 7
    In: Micro and Nano Engineering, Elsevier BV, Vol. 14 ( 2022-04), p. 100102-
    Materialart: Online-Ressource
    ISSN: 2590-0072
    Sprache: Englisch
    Verlag: Elsevier BV
    Publikationsdatum: 2022
    ZDB Id: 2965612-6
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  • 8
    In: ECS Meeting Abstracts, The Electrochemical Society, Vol. MA2022-02, No. 32 ( 2022-10-09), p. 1174-1174
    Kurzfassung: During the last decade optical sensor technologies have attracted increased attention for various applications. Plasmon-based optical sensor concepts for the detection of refractive index changes that rely on propagating surface-plasmon polaritons at metal-dielectric interfaces or on localized plasmons in metallic nanostructures prove their potential for these application due to their fast detection speed, high specificity and sensitivities [1, 2]. Combining plasmonic structures directly with optoelectronic devices could enable a high level of integration, however, it represents a significant technological challenge to develop an on-chip solution for these concepts including the integration of sensor and detector components. Previous works demonstrated first approaches mainly for the integration of refractive index sensor components on wafer level [3, 4] . In [5] and [6] a proof-of-concept of a fully integrated on-chip solution with high sensitivities was presented, which can be easily combined with microfluidics [7] for potential applications in biosensing. In this concept, a nanohole array (NHA) was structured in a 100 nm thick aluminum layer on top of a vertical PIN germanium photodetector (GePD) with an intrinsic germanium sheet of 480 nm. This sensor concept relies on extraordinary optical transmission through the NHA [8] : Light transmission is only possible for narrow wavelength ranges determined by the NHA geometry which determine the transmission peaks at the resonance wavelength of the NHA. Thus, the NHA acts as a high quality wavelength filter. Due to the change in the refractive index, a material under test (MUT) contacting directly the surface of the NHA, provokes a shift of the wavelength maximum, which can be detected by measuring the photocurrent spectra of the GePD. While responsivities and sensitivities of (0 V) = 0.075 A/W and = 1200 nm/RIU could be attained in this proof-of-concept device [6, 7], the semiconductor device layers were deposited using molecular beam epitaxy (MBE). Furthermore the vertical PIN GePD was realized by a mesa procedure to enable large areas for top illuminated operations. These techniques are unsuitable for an industrial CMOS fabrication process with high throughput. Therefore, the development of a CMOS compatible technology process with low costs and high yields is an important step towards large-scale fabrication of this sensor concept. In this work we present the progress for the realization of a surface plasmon resonance (SPR) refractive index sensor in a 200 mm wafer Silicon based technology. One main challenge is the fabrication of a large area photodetector for top illuminated sensor devices. We developed a process, which is mainly based on the IHP electronic photonic integrated circuits (ePIC) technology [9]. This ePIC technology enables the production of waveguide coupled lateral PIN GePDs with high bandwidth and high responsivities [10] . However, these PDs are unsuitable for top illuminated applications because of their small germanium areas. Due to certain process conditions with respect to chemical mechanical polishing procedures there are limits for feasible large detector areas. Furthermore, large detector areas for lateral PIN GePDs would result in very low electric fields in the intrinsic zone where carriers are generated by photon absorption. Thus, very high voltages for reversed bias are necessary for sufficient carrier drifts. For the first time we have developed a modern detector design concept which is compatible to the IHP ePIC technology. This concept allows the realization of large area detectors of 1600µm² (40µm x 40µm) with optimized optical responsivities for top illuminated applications. The detector consists of several parallel connected lateral PIN GePDs. We designed different variations and varied Ge width and distance between neighboring GePDs in order to investigate process limits. The p- and n-doped regions were defined by dopant implantation using a photo resist mask. We used a finger-like design as implantation masks to enable one contact area for each p-doped and each n-doped region (Fig. 1). This contacting approach differs from the standard GePD offered in the IHP ePIC technology. We analyzed I-V characteristics in dependence of detector design and contacting scheme (Fig. 2). In addition, process adjustments for the optimization of the germanium quality were investigated to reduce dark currents and to improve optical responsivities (Fig.3). Titanium nitride (TiN) is very promising metallic alloy with respect to thickness homogeneity and low surface roughness. Therefore we used titanium nitride which was deposited by a sputtering process to develop plasmonic active NHA layers. Various process development runs were done to evaluate the NHA performance. Ellipsometry and atomic force microscope measurements were performed to characterize the quality of the TiN layer (Fig.4). Figure 1
    Materialart: Online-Ressource
    ISSN: 2151-2043
    Sprache: Unbekannt
    Verlag: The Electrochemical Society
    Publikationsdatum: 2022
    ZDB Id: 2438749-6
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  • 9
    Online-Ressource
    Online-Ressource
    Wiley ; 1997
    In:  Surface and Interface Analysis Vol. 25, No. 9 ( 1997-08), p. 660-666
    In: Surface and Interface Analysis, Wiley, Vol. 25, No. 9 ( 1997-08), p. 660-666
    Materialart: Online-Ressource
    ISSN: 0142-2421 , 1096-9918
    URL: Issue
    RVK:
    Sprache: Englisch
    Verlag: Wiley
    Publikationsdatum: 1997
    ZDB Id: 2023881-2
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  • 10
    Online-Ressource
    Online-Ressource
    The Electrochemical Society ; 2019
    In:  ECS Meeting Abstracts Vol. MA2019-02, No. 25 ( 2019-09-01), p. 1194-1194
    In: ECS Meeting Abstracts, The Electrochemical Society, Vol. MA2019-02, No. 25 ( 2019-09-01), p. 1194-1194
    Kurzfassung: The demand for the high-density integrated memories is growing along with the scaling of the transistor technology nodes. To fabricate the reliable devices in advanced technologies, optimization of several process steps is necessary [1]. The capacitor, which is commonly a MIM (Metal-Insulator-Metal) module finds its application as a basic storage device in memories, filters, voltage limiters etc. The MIM module is also considered as an integral part of memory technologies such as DRAM, FeRAM, and RRAM. The MIM modules should demonstrate reliable operation through better performance and efficiency. And, it is realized through the parameters related to MIM module such as, low leakage current, less variability with respect to capacitance, high quality factor Q, lower defect density, low parasitic capacitance and many others [2] . Reactive-ion-etching plays a very important role in BEOL integration of MIM devices. The MIM module is created by dry etching through the MIM stack. Related to RRAM (Resistive Random Access Memory) applications the MIM stack consists of an additional buffer layer such as Ti or Hf [3]. These layers are easily oxidizable and the etching step could oxidize them from the sidewalls. Also, the residuals of the metal if remain on the sidewall could lead to leaky devices. Hence, an etch process which is not well optimized could damage the devices and in turn pose a threat to their functionality and reliability [4] . An improved MIM stack etch process is beneficial to reduce the above-mentioned damages. Several techniques were used in the past to cover the MIM devices with dielectric materials like SiO 2 and SiN, which protects the devices from further process steps involved in the fabrication procedure [5]. In this work we demonstrate the effect of the improved etch process with a combination of SiNO spacers and encapsulation techniques for TiN/Ti/HfO 2 /TiN stacks. This stack is most popularly used in RRAM and, in this work, it is integrated into the BEOL of the 250 nm CMOS technology at IHP. To test the performance of the devices, the MIM stack was fabricated in three different approaches. In the first approach, photoresist is used as a mask to etch the MIM stack, the second one uses TiN hard mask and the third one uses TiN hard mask etch in addition to creation of SiNO spacers after the TiN/Ti etch. The encapsulation of MIM modules with SiNO is implemented in all the three approaches mentioned above. Special device structures with the TiN/Ti/HfO 2 /TiN stack are fabricated to test the variability of the MIM parameters on the entire wafer. Additionally, the switching operation was tested by means of DC voltage sweeps on the MIM RRAM devices which includes, forming, reset and set steps followed by 50 cycles of reset and set processes. The devices associated with the improved fabrication process steps exhibited less variability in terms of leakage current, capacitance and Q-factor values along the entire wafer. This reduction in the variability of the parameters corresponding to the MIM devices could be used for emerging applications. References G.S. Kar, A.Fantini, Y.Y. Chen, V. Paraschiv, B. Govorenau, H. Hody, N. Jossart, H.Tielens, S. Brus, O. Richard, T. Vandeweyer, D.J. Wouters, L. Altimime, M. Jurczak, i n Symposium on VLSI Technology (VLSIT), 2012 IEEE , pp. 157-158 E. Pérez, A. Grossi, C. Zambelli, M. K. Mahadevaiah, P. Olivo, and Ch. Wenger, in MTT-S International Microwave Workshop Series on Advanced Materials and Processes for RF and THz Applications (IMWS-AMP), 2018 IEEE , pp. 1-3 E. Pérez, M. K. Mahadevaiah, C. Zambelli, P. Olivo, and Ch. Wenger, Solid-State Electronics, (2019) V. B. Naik, J. H. Lim, K. Yamane, D. Zeng, H. Yang, N. Thiyagarajah, J. Kwon, N. L. Chung, R. Chao, T. Ling, K. Lee, in International Reliability Physics Symposium (IRPS) , 2019 IEEE, pp. 2C-2 Y.S. Chen, H.Y. Lee, P.S. Chen, P.Y. Gu, W.H. Liu, W.S. Chen, Y.Y. Hsu, C.H. Tsai, F. Chen, M.J. Tsai, and C. Lien, Electron Device Letters , Vol. 32 , Issue: 3, pp 390-392 (2011)
    Materialart: Online-Ressource
    ISSN: 2151-2043
    Sprache: Unbekannt
    Verlag: The Electrochemical Society
    Publikationsdatum: 2019
    ZDB Id: 2438749-6
    Standort Signatur Einschränkungen Verfügbarkeit
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