High Temperature Characterization Of Ni, W And Al Contacts To 3C-Silicon Carbide Thin Films

1997 ◽  
Vol 483 ◽  
Author(s):  
C Jacob ◽  
P Pirouz ◽  
H-I Kuo ◽  
M Mehregany

AbstractWith the current availability of large-area 3C-SiC films, it is imperative that stable high temperature contacts be developed for high power devices. By comparing the existing data in the literature, we demonstrate that the contact behavior on each of the different polytypes of SiC will vary significantly. In particular, we demonstrate this for 6H-SiC and 3C-SiC. The interface slope parameter, S, which is a measure of the Fermi-level pinning in each system varies between 0.4–0.5 on 6H-SiC, while it is 0.6 on 3C-SiC. This implies that the barrier heights of contacts to 3C-SiC will vary more significantly with the choice of metal than for 6H-SiC.Aluminum, nickel and tungsten were deposited on 3C-SiC films and their specific contact resistance measured using the circular TLM method. High temperature measurements (up to 400°C) were performed to determine the behavior of these contacts at operational temperatures. Aluminum was used primarily as a baseline for comparison since it melts at 660°C and cannot be used for very high temperature contacts. The specific contact resistance (ρc) for nickel at room temperature was 5 × 10−4 Ω-cm2, but increased with temperature to a value of 1.5 × 10−3 Ω-cm2 at 400°C. Tungsten had a higher room temperature × 10−3 Ω-cm2, which remained relatively constant with increasing temperature up to 400°C. This is related to the fact that there is hardly any reaction between tungsten and silicon carbide even up to 900°C, whereas nickel almost completely reacts with SiC by that temperature. Contact resistance measurements were also performed on samples that were annealed at 500°C.

1999 ◽  
Vol 572 ◽  
Author(s):  
Frank Erler ◽  
Henry Romanus ◽  
Jörg K. N. Lindner ◽  
Lothar Spiess

ABSTRACTAmorphous tungsten-silicon layers were deposited by DC co-sputtering and subsequently annealed in an argon atmosphere up to 1325 K to form tetragonal crystalline WSi2. Al-implanted p-6H-SiC exhibits a small depletion area forming an ohmic contact with low specific contact resistance. A modified Circular Transmission Line Model (CTLM), introduced by Marlow & Das [1] and Reeves [2], was used to characterize the electrical properties of the prepared contacts in the range between 300 K and 650 K. Deviations between calculated fieldemission contact resistances and measured contact resistances (ρc=2·10−2 Ωcm2, T=650 K) could be explained by TEM-cross section investigations. These deviations are caused by inhomogeneous contact interfaces originating from technological difficulties during contact preparation.


2018 ◽  
Vol 924 ◽  
pp. 385-388 ◽  
Author(s):  
Roberta Nipoti ◽  
Maurizio Puzzanghera ◽  
Maria Concetta Canino ◽  
Giovanna Sozzi ◽  
Paolo Fedeli

This study shows that a thin Ni film on Al/Ti/4H-SiC metal pads allows to preserve the pad form factor during a 1000 °C/2 min treatment, provided that the Al and Ti film thicknesses are sufficiently thin. Moreover, by reducing the Al to Ti thickness ratio, droplet formation in the contact area is avoided and a mirror-like appearance is obtained. This optimal contact morphology corresponds to a specific contact resistance of few 10-4Ωcm2at room temperature on p-type 4H-SiC with resistivity in the range 0.1 – 1 Ωcm.


2019 ◽  
Vol 58 (11) ◽  
pp. 116501 ◽  
Author(s):  
Vuong Van Cuong ◽  
Seiji Ishikawa ◽  
Tomonori Maeda ◽  
Hiroshi Sezaki ◽  
Satoshi Yasuno ◽  
...  

2006 ◽  
Vol 911 ◽  
Author(s):  
Kirk Hofeling ◽  
Loren Rieth ◽  
Florian Solzbacher

AbstractTiW(40 nm)/TiWN(80 nm)/Pt(500nm) was investigated as a new high-temperature compatible contact stack to 3C-SiC for harsh environment applications. Performance of TiW/TiWN/Pt contacts deposited on unintentionally doped (8.85×1018 cm-3) 3C-SiC grown by LPCVD to a thickness of ~1μm on (100) Si are reported. The linear transmission line method was used to determine specific contact resistance (ρc) at room temperature and for long-term tests at 300 °C. As deposited contacts were Ohmic with a ρc range of 1×10-4 to 1×10-3 cm2. These contacts were annealed for five minutes in forming gas (8% H2 92% Ar), at temperatures from 450 to 950 °C and all retained Ohmic character. Annealing samples at 450, 550 and 950 °C decreased ρc while anneling between 650 and 850 °C generally increased ρc.Auger Electron Spectroscopy (AES) analysis was performed on a sample annealed at 750 °C. The as-received surface was composed of Si and O; after a brief sputter etch a characteristic Pt peak became visible and the O peak decreased substantially. Depth profiles detected Si throughout the Pt capping layer but not in the TiW layers. We suspect that Si diffuses from the SiC substrate into the Pt capping layer and surface Si also reacts with O2 to from an oxide. These reactions, in combination with incomplete SiC/TiW interface reactions, are suspected to cause the increase of ρc for samples annealed between 650 and 850 °C. Annealing at 950 °C gave the lowest contact resistance of 2.3×10-5. Long-term testing at 300 °C for 190 hours, in atmosphere, was performed on contacts annealed at 450 °C. When heated, the contacts initial ρc of 2.1×10-4 cm2 increased to ~4×10-3 cm2 which remained stable for the test duration. After long-term testing the sample ρc measured at room temperature decreased to 9.8×10-5 cm2.


2011 ◽  
Vol 679-680 ◽  
pp. 193-196 ◽  
Author(s):  
Xi Song ◽  
Anne Elisabeth Bazin ◽  
Jean François Michaud ◽  
Frédéric Cayrel ◽  
Marcin Zielinski ◽  
...  

Two electrical characterization methods were used to study 3C-SiC epilayers doped by nitrogen implantation: circular Transfer Length Method (c­TLM) which allows extracting the specific contact resistance and Scanning Spreading Resistance Microscopy (SSRM) used to measure activated doping concentration. 3C-SiC samples were implanted at room temperature with different energies (ranging from 30 to 150keV) and doses (from 1 to 5.4x1015cm-2) in order to obtain a 300nm thick box-like profile at 5x1020cm-3. To activate the dopant, the samples were then annealed from 1150°C to 1350°C for 1h to 4h. Titanium-nickel c-TLM contacts annealed at 1000°C under argon showed the best results in terms of specific contact resistance (8x10-6.cm2) after a 1350°C–1h annealing. For this annealing condition, the activation rate was assessed by SSRM around 13%. This value confirms the difficulty to activate the dopants introduced into the 3C-SiC as the temperature is limited by the silicon substrate. However, this work demonstrates that low resistance values can be achieved on 3C-SiC, using nitrogen implantation at room temperature.


2013 ◽  
Vol 740-742 ◽  
pp. 581-584 ◽  
Author(s):  
Jean François Michaud ◽  
X. Song ◽  
J. Biscarrat ◽  
F. Cayrel ◽  
E. Collard ◽  
...  

For this study, 4H SiC samples were implanted with aluminum at room temperature, 200°C and 600°C with different energies, ranging from 30 to 380 keV, for a total dose of 4x1015 cm 2, to create a “box-like” profile. To activate dopants, samples were then isochronally annealed from 1650°C to 1850°C during 30min. The lowest specific contact resistance achieved, evaluated to 1.3x10-5 Ω.cm2, has been obtained for the 200°C implanted sample annealed at 1850°C. For this condition, Scanning Capacitance Microscopy study has proved that the dopant activity is quite homogeneous in opposition with the samples implanted at RT and 600°C.


2013 ◽  
Vol 4 ◽  
pp. 234-242 ◽  
Author(s):  
Gabriele Fisichella ◽  
Salvatore Di Franco ◽  
Patrick Fiorenza ◽  
Raffaella Lo Nigro ◽  
Fabrizio Roccaforte ◽  
...  

Chemical vapour deposition (CVD) on catalytic metals is one of main approaches for high-quality graphene growth over large areas. However, a subsequent transfer step to an insulating substrate is required in order to use the graphene for electronic applications. This step can severely affect both the structural integrity and the electronic properties of the graphene membrane. In this paper, we investigated the morphological and electrical properties of CVD graphene transferred onto SiO2 and on a polymeric substrate (poly(ethylene-2,6-naphthalene dicarboxylate), briefly PEN), suitable for microelectronics and flexible electronics applications, respectively. The electrical properties (sheet resistance, mobility, carrier density) of the transferred graphene as well as the specific contact resistance of metal contacts onto graphene were investigated by using properly designed test patterns. While a sheet resistance R sh ≈ 1.7 kΩ/sq and a specific contact resistance ρc ≈ 15 kΩ·μm have been measured for graphene transferred onto SiO2, about 2.3× higher R sh and about 8× higher ρc values were obtained for graphene on PEN. High-resolution current mapping by torsion resonant conductive atomic force microscopy (TRCAFM) provided an insight into the nanoscale mechanisms responsible for the very high ρc in the case of graphene on PEN, showing a ca. 10× smaller “effective” area for current injection than in the case of graphene on SiO2.


2017 ◽  
Vol 897 ◽  
pp. 391-394 ◽  
Author(s):  
P. Fedeli ◽  
Maurizio Puzzanghera ◽  
Francesco Moscatelli ◽  
Renato Amaral Minamisawa ◽  
Giovanni Alfieri ◽  
...  

This study shows that an Al-Ti bilayer with an Al to Ti atomic ratio suitable forohmic contacts on p-type 4H-SiC can be covered by a Ni film during the high temperature alloying process, without altering the ohmic nature, while eliminating a detrimental contact morphology caused by the presence of molten Al-Si during alloying. On 1×1020 cm-3 Al-implanted 4H-SiC layer, the RT specific contact resistance of this Ni-Al-Ti contact measured by TLM-C method is (3 ± 1)×10-6 Ωcm2.


1997 ◽  
Vol 468 ◽  
Author(s):  
D. J. King ◽  
L. Zhang ◽  
J. C. Ramer ◽  
S. D. Hersee ◽  
L. F. Lester

ABSTRACTOhmic contacts to Mg-doped p-GaN grown by MOCVD [1] are studied using a circular transmission line model (TLM) to avoid the need for isolation. For samples which use a p-dopant activation anneal before metallization, no appreciable difference in the specific contact resistance, rc, as a function of different capping options is observed. However, a lower rc is obtained when no pre-metallization anneal is employed, and the post-metallization anneal simultaneously activates the p-dopant and anneals the contact. This trend is shown for Pt/Au, Pt, Pd/Pt/Au, and Ni/Au contacts to p-GaN. The rc 's for these metal contacts are in the range of 1.4–7.6 × 10-3 ohm-cm2 at room temperature at a bias of 10mA. No particular metallization formula clearly yields a consistently superior contact. Instead, the temperature of the contact has the strongest influence.Detailed studies of the electrical properties of the Pt/Au contacts reveal that the I-V linearity improves significantly with increasing temperature. At room temperature, a slightly rectified I-V characteristic curve is obtained, while at 200°C and above, the I-V curve is linear. For all the p-GaN samples, it is also found that the sheet resistance decreases by an order of magnitude with increasing temperature from 25°C to 350°C. The specific contact resistance is also found to decrease by nearly an order of magnitude for a temperature increase of the same range. A minimum rc of 4.2 × 10-4 ohm-cm2 was obtained at a temperature of 350°C for a Pt/Au contact. This result is the lowest reported rc for ohmic contacts to p-GaN.


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