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1.
Rapid thermal annealing (RTA) technology offers potential advantages for GaAs MESFET device technology such as reducing dopant
diffusion and minimizing the redistribution of background impurities. LEC semi-insulating GaAs substrates were implanted with
Si at energies from 100 to 400 keV to doses from 1 × 1012 to 1 × 1014/cm2. The wafers were encapsulated with Si3N4 and then annealed at temperatures from 850-1000° C in a commercial RTA system. Wafers were also annealed using a conventional
furnace cycle at 850° C to provide a comparison with the RTA wafers. These implanted layers were evaluated using capacitance-voltage
and Hall effect measurements. In addition, FET’s were fabricated using selective implants that were annealed with either RTA
or furnace cycles. The effects of anneal temperature and anneal time were determined. For a dose of 4 × 1012/cm2 at 150 keV with anneal times of 5 seconds at 850, 900, 950 and 1000° C the activation steadily increased in the peak of the
implant with overlapping profiles in the tail of the profiles, showing that no significant diffusion occurs. In addition,
the same activation could be obtained by adjusting the anneal times. A plot of the equivalent anneal times versus 1/T gives
an activation energy of 2.3 eV. At a higher dose of 3 × 1013 an activation energy of 1.7 eV was obtained. For a dose of 4 × 1012 at 150 keV both the RTA and furnace annealing give similar activations with mobilities between 4700 and 5000 cm2/V-s. Mobilities decrease to 4000 at a dose of 1 × 1013 and to 2500 cm2/V-s at 1 × 1014/cm2. At doses above 1 × 1013 the RTA cycles gave better activation than furnace annealed wafers. The MESFET parameters for both RTA and furnace annealed
wafers were nearly identical. The average gain and noise figure at 8 GHz were 7.5 and 2.0, respectively, for packaged die
from either RTA or furnace annealed materials. 相似文献
2.
Rapid thermal annealing of ion implantedn-type CdTe has been investigated. Samples were implanted with 60 keV Ar+ and As+ ions to a dose of 1 × 1014 cm−2 and subjected to anneal sequences of 5-100s at temperatures of 350-650° C. Photoluminescence measurements have indicated
that the implantation completely quenches the photoluminescence; however, anneals for only 5s at 350° C are sufficient to
recover most of the features of the photoluminescence spectrum to that equivalent of unimplanted material. Luminescence spectral
features associated with thermal annealing damage and substitutional As in inferred. Type conversion of the As+ implanted layer is observed and it has been shown that good diodes can be made, with the best behaviour resulting from a
5s anneal at 450° C.
Research supported by the Natural Sciences and Engineering Research Council of Canada 相似文献
3.
Rapid thermal annealing (RTA) of neutron transmutation doped Si wafers is shown to be an alternative to conventional furnace
annealing. Measurements of resistivity and deep level transient spectroscopy (DLTS), demonstrated annealing on wafers with
diameters up to 75 mm. A 4.5 kW incoherent-light RTA furnace was used. Evidence for crystalline slip was found but this did
not appear to affect the results. The slip was more severe for the larger diameter wafers. Some results from a DLTS examination
of a partially rapid-thermal-annealed wafer are presented. 相似文献
4.
The electrical characteristics of thermally nitrided gate oxides on n-type 4H-SiC, with and without rapid thermal annealing processes, have been investigated and compared in this paper. The effects of annealing time (isothermal annealing) and annealing temperature (isochronal annealing) on the gate oxide quality have also been systematically investigated. After rapid isothermal and isochronal annealings, there has been a significant increase in positive oxide-charge density and in oxide-breakdown time. A correlation between the density of the positive oxide charge and the oxide breakdown reliability has been established. We proposed that the improvement in the oxide-breakdown reliability, tested at electric field of 11 MV/cm, is attributed to trapping of injected electron by the positive oxide charge and not solely due to reduction of SiC-SiO2 interface-trap density. 相似文献
5.
The physical and electrical properties of BF
2
+
implanted polysilicon films subjected to rapid thermal annealing (RTA) are presented. It is found that the out diffusion
ofF and its segregation at polysilicon/silicon oxide interface during RTA are the major causes ofF anomalous migration. Fluorine bubbles were observed in BF
2
+
implanted samples at doses of 1×1015 and 5×1015 cm−2 after RTA. 相似文献
6.
M. Rabus A. T. Fiory N. M. Ravindra P. Frisella A. Agarwal T. Sorsch J. Miner E. Ferry F. Klemens R. Cirelli W. Mansfield 《Journal of Electronic Materials》2006,35(5):877-891
Fabrication of devices and circuits on silicon wafers creates patterns in optical properties, particularly the thermal emissivity
and absorptivity, that lead to temperature nonuniformity during rapid thermal processing (RTP) by infrared heating methods.
The work reported in this paper compares the effect of emissivity test patterns on wafers heated by two RTP methods: (1) a
steadystate furnace or (2) arrays of incandescent lamps. Method I was found to yield reduced temperature variability, attributable
to smaller temperature differences between the wafer and heat source. The temperature was determined by monitoring test processes
involving either the device side or the reverse side of the wafer. These include electrical activiation of implanted dopants
after rapid thermal annealing (RTA) or growth of oxide films by rapid thermal oxidation (RTO). Temperature variation data
are compared with a model of radiant heating of patterned wafers in RTP systems. 相似文献
7.
Youn Tae Kim Chi Hoon Jun Jong-Tae Baek Hyung Joun Yoo Sang-Koo Chung 《Journal of Electronic Materials》1995,24(10):1413-1417
In this study, we have investigated sensitivities of the ion implanted silicon wafers processed by rapid thermal annealing
(RTA), which can reveal the variation of sheet resistance as a function of annealing temperature as well as implantation parameters.
All the wafers were sequentially implanted by the arsenic or phosphorous implantations at 40, 80, and 100 keV with the dose
level of 1014 to 2 × 1016 ions/cm2. Rapid thermal annealing was carried out for 10 s by the infrared irradiation at a temperature between 850 and 1150°C in
the nitrogen ambient. The activated wafer was characterized by the measurements of the sheet resistance and its uniformity
mapping. The values of sensitivities are determined from the curve fitting of the experimental data to the fitting equation
of correlation between the sheet resistance and process variables. From the sensitivity values and the deviation of sheet
resistance, the optimum process conditions minimizing the effects of straggle in process parameters are obtained. As a result,
a strong dependence of the sensitivity on the process variables, especially annealing temperatures and dose levels is also
found. From the sensitivity analysis of the 10 s RTA process, the optimum values for the implant dose and annealing temperature
are found to be in the range of 1016 ions/cm2 and 1050-1100°C, respectively. The sensitivity analysis of sheet resistance will provide valuable data for accurate activation
process, offering a guideline for dose monitoring and calibration of ion implantation process. 相似文献
8.
N. H. Beltrán C. Balocchi X. Errazu R. E. Avila G. Piderit 《Journal of Electronic Materials》1998,27(2):L9-L11
Zirconia (8 mol% yttria) (YSZ) amorphous layers were deposited by spray pyrolysis on Si oxidized substrates and crystallized
by rapid thermal treatment in a home-made halogen lamps furnace. Uniform films were obtained by depositing up to six layers,
followed by the thermal treatment. X-ray analysis showed that the cubic phase is obtained during the initial stage of the
annealing process. No significant differences with increasing annealing time nor interaction between the YSZ film and the
substrate were observed. Ionic conduction in air, with activation energies comparable to those of bulk YSZ ceramics, was observed.
The electrical characteristics of the films make them suitable for microelectronics applications. 相似文献
9.
The structural characterization of hole patterns on GaAs cap layers grown on GaInNAs quantum wells (QWs) created by rapid thermal annealing is shown in this work. The effect of annealing temperature on the hole size, as well as the impact of the ion density present during the growth of the QW on the formation of this hole pattern, is presented. Structural (atomic force, scanning electron and transmission electron microscopy) and optical characterization (cathodoluminescence) of the samples is presented. The structure of the planes forming the walls and base of these holes is proposed. 相似文献
10.
The results of a study of the electrical and metallurgical properties of thin metallic layers deposited on InP for use as an ohmic contact are presented. A rapid thermal annealing system was used to alloy AuGe/Ni/Au contacts ton-type ion implanted InP. Rutherford backscattering and contact resistivity measurement were used to evaluate the structural and electrical characteristics of these rapid thermal alloyed thin films. Varying degrees of mixing between the metals and the semiconductor were found depending on the temperature and temperature-time cycle. These results were compared to furnace and graphite strip-heater alloying techniques. A correlation between the interface structure and the contact resistance was found. Temperatures between 430 and 450° C and alloying time of 2 sec have produced the best electrical results, with specific contact resistance as low as 2*10?7 Ω cm2 on semi-insulating InP which was Siimplanted with a peak concentration about 2*1018 cm?3. The optimum alloy temperature is marked by the onset of substantial wrinkling of the contact surface, whereas essentially smooth surfaces are obtained at temperatures below optimum. The depth of the alloyed ohmic contact is controlled by the time of heating and could be less than 1000Å. 相似文献
11.
Rapid thermal annealing (RTA) with incoherent light from tungsten lamps shows high potential relative to the conventional
furnace annealing (FA) to activate the implanted dopant. Due to the short time annealing, it could completely eliminate the
re-diffusion of dopant and host atom. For the Si implantation with dose of 2 × 1014 cm2, the electrical activity of 78% for RTA was higher than that of the FA. But for this short time, some defects measured by
deep level transient spectroscopy (DLTS) were hard to remove. A two-step annealing was suggested by the combination of high
temperature RTA (1000° C) and FA (700° C). After the post-FA, the defects would be removed to a great extent, and the electrical
activity of dopant also increased. With the dose of 2 x 1013 cm-2, the activity attained after the two step annealing was 92.5%, which may be the highest value according to our knowledge
for rapid thermal annealing on Si ion implanted GaAs. 相似文献
12.
YANG Hong-guan WEN Li-qun DAI Da-kang YU Biao 《半导体光子学与技术》2006,12(4):265-269
The relationship between the arrangement of tungsten-halogen lamps and the uniformity of irradiance received by the wafer is discussed, and a sort of axial-symmetrical lamps-array is designed to guarantee that the irradiation on the edge is approximately the same as the one on the center of the wafer. The magnitude of temperature on the wafer vs. the power of tungsten-halogen lamps is calculated numerically. 相似文献
13.
In this study we evaluate the effects of dual implantation with different doses of Si and P on dopant activation efficiency
and carrier mobility in InP:Fe. The implants were activated by a rapid thermal annealing step carried out in an optimized
phosphoruscontaining ambient. For high dose implants (1014–1015 cm−2), which are typically employed for source/drain regions in FETs, dual implantation of equal doses of Si and P results in
a higher sheet carrier concentration and lower sheet resistance. For 1014 cm−2 Si implants at 150 keV, the optimal P co-implant dose is equal to the Si dose for most anneal temperatures. We obtain an
activation efficiency of ∼70% for dual implanted samples annealed at 850° C for 10 sec. The high activation efficiencies and
low sheet resistances obtained in this study emphasize the importance of stoichiometry control through the use of P co-implants
and a phosphorus-containing ambient during the thermal processing of InP. 相似文献
14.
Activation of nitrogen implants in 6H-SiC 总被引:1,自引:0,他引:1
We have studied the effect of anneal time and temperature on activation of high-dose nitrogen implants into 6H-SiC. At a fixed
anneal temperature, a strong dependence on anneal time is seen. For short anneals, the resistivity initially decreases with
anneal time. After a minimum resistivity is reached, resistivity increases with further anneal. The optimum anneal time for
minimum resistiv-ity increases as anneal temperature is reduced. Successful activation has been achieved at temperatures as
low as 900°C. 相似文献
15.
The use of rapid thermal annealing (RTA) techniques to anneal ion implanted GaAs compounds is expected to have a significant
impact on device technology. Due to the short duration of the heat treatment, the implanted impurities may be activated without
significant diffusion. For heterojunction bipolar transistor (HBT) applications, high doses of p-type impurities are required
to compensate the doping levels of N-GaAlAs emitter and n+ GaAs contact layers. Multi-implantations were chosen to maintain a flat profile down to the base layer. Energies of 30, 60,
150, and 340 keV with doses of 6 × 1013, 9 × 1013,6 × 1014, and 9 × 1014 cm−2, respectively, have been used. Annealing cycles with time durations of a few seconds and temperature in the range of 850–950°C
are described. Electrical properties of the annealed samples have been investigated using an electrochemical measurement technique.
It was found that hole concentrations as high as 4 × 1019 cm−3 and electrical activities near to 75 percent can be obtained. There is no evident indiffusion and no significant outdiffusion
at the optimal annealing conditions. Simulation of multilayer implantations are also carried out by an accurate model available
in TITAN 2D process simulator using Pearson IV laws and taking into account the diffusion effects on profile distribution
caused by RTA. A first approximation using a simple model allows a rapid evaluation of the data fitting operation. In a second
approach, concentration dependent diffusivity and the contribution of the electric field at the interface are covered to perform
an improved data fitting of ion implanted and annealed dopant profiles. A comparative study shows a good agreement between
experimental and simulated distributions. 相似文献
16.
An overview is given of modelling issues in rapid thermal processing. Firstly, the influence of surface and bulk properties on wafer emissivity is discussed. Secondly, the influence of back-side layers, wafer transparency and back-side roughness on temperature measurement is discussed. Thirdly, several causes of temperature non-uniformity are mentioned. 相似文献
17.
J. A. López-Rubio J. Sangrador M. Clement T. Rodríguez 《Journal of Electronic Materials》1994,23(11):1245-1249
In this work, we are reporting the use of a two-step rapid thermal annealing (RTA) process (250°C, 100s+340°C, 30s) for the
annealing of Hg1−xCdxTe (MCT) implanted layers over p-type (x=0.22) substrates. We report a high value of electrical activation (70%) of the indium
implants after this short RTA treatment in inert Ar atmosphere. The need of two RTA steps in the annealing recipe is shown,
and so the role played by each of them: the first step annihilates the implantation damage, while the second one produces
the impurity electrical activation. However, for the boron case, no electrical activity was found after several annealing
processes, behaving as an inert species for the case of this bulk MCT material. We also point out the change on the substrate
electrical characteristics induced by the thermal treatments, and report the convenience of a subsequent low temperature furnace
annealing (200°C, 72 h) to reduce back the bulk carrier concentration to values low enough to achieve an n+-p IR detector structure. 相似文献
18.
Deep level traps are observed in silicon that has been implanted with high doses of arsenic and subsequently annealed by rapid
thermal annealing. The doses studied create enough damage to form a surface amorphous layer. Annealing temperatures, implant
fluence, and the presence of a surface amorphous layer contribute to the type of trap observed. These results show evidence
for a clustering/declustering mechanism of arsenic in silicon during rapid thermal annealing. 相似文献
19.
The impact of the heating rate (HR) of a Rapid Thermal Annealing (RTA) on the crystallinity and on the morphology of CeO2 thin films has been investigated by Raman Spectroscopy (RS), Photoluminescence (PL), Scanning Electron Microscopy (SEM), Energy Dispersive Spectroscopy (EDS), and tapping mode Atomic Force Microscopy (AFM). The electrical properties of CeO2 thin films have also been studied with the Conductive AFM mode. This paper highlights the importance of the heating rate value used during an RTA on crystalline quality, morphology and on the electrical properties of the CeO2 layer. In fact, the best crystallinity with a good morphology and a high resistivity has been obtained for a CeO2 layer sputtered on (111) Si substrate and post-annealed at 1000 °C for 30 s with an HR of 25 °C/s. 相似文献
20.
A P-layer can be formed on a SiC wafer surface by using multiple Al ion implantations and post-implantation annealing in a low pressure CVD reactor.The Al depth profile was almost box shaped with a height of 1×1019cm-3 and a depth of 550 nm.Three different annealing processes were developed to protect the wafer surface.Variations in RMS roughness have been measured and compared with each other.The implanted SiC, annealed with a carbon cap,maintains a high-quality surface with an RMS roughness as low as 3.8 nm.Macrosteps and terraces were found in the SiC surface,which annealed by the other two processes(protect in Ar/protect with SiC capped wafer in Ar).The RMS roughness is 12.2 nm and 6.6 nm,respectively. 相似文献