Connector contact resistance may become unstable if fretting occurs. Such motions result in the formation of insulating oxides on the surface of base metal contacts or organic polymers on contacts made of platinum group metals. These degradations are termed fretting corrosion and frictional polymerization, respectively. Motion may be caused by external vibration or fluctuating temperature. The lower the frequency of movement, the fewer the number of cycles to contact failure. Increasing the contact normal load or reducing the amplitude of movement may stabilize the connection. Tin and palladium and many of their alloys are especially prone to fretting failure. Tin mated to gold is worse than all-tin contacts. Gold and high gold-silver alloys that are softer when mated to palladium stabilize contact resistance since these metals transfer to the palladium during fretting; but flash gold coatings on palladium and palladium nickel offer marginal improvement for the gold often quickly wears out. Dissimilar metal contact pairs show behaviors like that of the metal which predominates on the surface by transfer. Contact lubricants can often prevent fretting failures and may even restore unlubricated failed contacts to satisfactory service.

Contact resistance of nickel hardened gold electroplate (NiHG) deposited on nickel-underplated phosphor bronze disk coupons (substrate) after thermal aging was measured with a hard gold-plated beryllium copper alloy pin probe by means of a four-point probe technique, compared to that of cobalt-hardened gold electroplate (CoHG). Surface of NiHG plated coupons after aging was analyzed by X-ray photoelectron spectroscopy (XPS) to investigate the influence of the oxide film formation during thermal aging on contact resistance of NiHG electroplate, compared to that of CoHG. Initial contact resistance of the NiHG coupons was less than 10 mΩ at a contact forces more than 0.05 N, increased to 10 mΩ at a contact force of 0.05 N after 100 hours aging at 200. In contrast, contact resistance of the CoHG coupons progressively increased with increase in aging time, reached 1000 mΩ even at a contact force of 0.05 N after 52 hours aging. XPS analysis for the NiHG coupons demonstrated that nickel oxide film was formed on the NiHG surface in conformity with parabolic growth kinetics, as cobalt oxide film formed on CoHG surface. However, a thickness of the latter film was approximately 4-fold larger than that of former after 100 hours aging at 200. The small increase in contact resistance of NiHG coupons after aging suggested to be due to inhibitory of nickel oxide film growth on the surface. The cause of relatively low and steady contact resistance of NiHG during thermal aging was discussed.

The applicability of composite materials containing laminar solid lubricants to sliding contacts was studied. Performances of several composite materials prepared by incorporating solid lubricants with the basic alloys of the Cu-Nb system and Cu-Sn system were investigated to test the suitability of the composite materials as sliding contacts. As a result, it was clarified that the composite materials based on Cu-Sn alloy were superior to those based on Cu-Nb alloy and those containing only WS₂ and not MoS₂ were more effective in reducing both the contact resistance and the coefficient of friction. Based on the relationship between the contact resistance and the coefficient of friction obtained in this experimental study, the author proposed a new model for electric contact of composite materials.

Simple expressions for constriction resistance of multitude conducting spots were analytically formulated by Greenwood. These expressions, however, include some approximations. Nakamura presented that the constriction resistance of one circular spot computed using the BEM is closed to Maxwell's exact value. This relative error is only e=0. 00162 [%]. In this study, the constriction resistances of two, five and ten conducting spots are computed using the boundary element method (BEM), and compared with those obtained using Greenwood's expressions. As the conducting spots move close to each other, the numerical deviations between constriction resistances computed using Greenwood's expressions and the BEM increase. As a result, mutual resistance computed by the BEM is larger than that obtained from Greenwood's expressions. The numerical deviations between the total resistances computed by Greenwood's expressions and that by the BEM are small. Hence, Greenwood's expressions are valid for the total constriction resistance calculation and can be applied to problems where only the total resistance of two contact surfaces, such as a relay and a switch, is required. However, the numerical deviations between the partial resistances computed by Greenwood's expression and that by the BEM are very large. The partial resistance calculations of multitude conducting spots are beyond the applicable range of Greenwood's expression, since Greenwood's expression for constriction resistance of two conducting spots is obtained by assuming that the conducting spots are equal size. In particular, the deviation between resistances of conducting spots, which are close to each other, is very large. In the case of partial resistances which are significant in semiconductor devices, Greenwood's expressions cannot be used with high precision.

The distributions of a spectral intensity of the breaking arc between silver contacts in DC 45-66 V/2.5-5.0 A circuits have been measured using a high-speed color video. As a result, a cathode brightening spot, which has a high spectral intensity, exists near the cathode surface. The cathode brightening spot expands with the increase of the contact gap, but its length expands until about 18µm. When the contact gap spreads over about 180 µm, a dark positive column appears and grows between the cathode brightening spot and the anode surface. The higher the interrupted current is, the larger the diameter of the cathode brightening spot will be. The maximum diameter of cathode brightening spot is 500 µm under these experiments.

In a DC 50 V/3.3 A circuit, the spatial distributions of the spectral intensities of breaking arcs near the cathode for silver contacts were measured on the contact surfaces of three different shapes: flat and spherical (1 mm radius and 2 mm radius) and the arc temperature and the metal-vapor quantity were calculated from the spectral intensities. The influence of the contact shape on the arc temperature and the metal-vapor quantity were also examined, as well as the arc tracks on the contact surfaces and the gain and loss of the contacts. Findings show the distributions of spectral intensities are non-symmetrical from the beginning to the extinction of the breaking arc for the flat contact: However, they are symmetrical in the latter half of the breaking in spite of the number of breaking arcs and the shape of contact surface for the spherical contact. The relationship between the area of the arc tracks on the cathode and the shape of contact surface is the same as the relationship between the existent areas of measured spectra and the shape of the contact surface. For the spherical contacts, the arc temperature and the metal-vapor quantity are affected a little by the radius of the curved of contact surface and the number of breaking arcs. However, the longer the arc duration, the higher the metal-vapor quantity is in the latter period of the breaking arc. For the flat contacts, the metal-vapor quantity is lower than those for the spherical contacts. The gain and loss of the contacts are less and the arc duration is shorter for the flat contact than for the spherical contact.

The authors observed the correlation between electromagnetic noise and trace of discharge on surface for various surface areas of Cu in opening copper (Cu)-carbon (C) electrodes. In the case of Cu (anode)-C (cathode), the duration of sporadic burst noise generated by discharge becomes longer when Cu surface area is increased, and trace of discharge (melting area) distribute widely on electrodes. Also the forms of the burst noise in the start of arc are classified, and the traces of discharge correspond to each forms. The forms of the burst noise depend on the pattern which the trace of discharge are formed. As these results, the authors showed the correlation between form of burst noise and trace of discharge on electrode surface.

This paper proposed the method as an estimation on the size of discharge spots through observation on traces after the discharge arose in circumstances gases mixed hydrocarbon gas. Namely, the circular carbonaceous deposit and the carbonaceous heap are observed on cathode and anode surface, respectively, after the short gap discharge arises in N₂+NO+CH₄ gases. The current density, which is the normal conversion current density, is calculated from the size of the trace of discharge and its value is about 1.010^-9 A/(cm² Pa²) in case that the concentration of CH₄ is 0.6%. The value is about 1/5 of values that are reported in the former articles and is reasonable one.

We propose and experimentally confirm two approaches to improve the sensitivity of the H-type piezoelectric crystal gyroscope of LiTaO₃. One is to adjust the resonant frequencies of the f_z mode through additional mass control; the other is to change the driving mode from f_x mode to f_z mode, while the driving frequency is the resonant frequency of the f_x mode. The sensitivity of the unit driving voltage is almost the same, but the threshold driving voltage level may increase more than 1,000 times, because it is far from the mechanical resonance. The high sensitivity of 0.11 pC (deg/sec) was obtained at a driving voltage of 30 V_pp.

The static fatigue parameters of plastic sleeves are determined by dynamic fatigue and destructive tests. The failure probability and lifetime of the plastic sleeve are estimated by using these parameters. No failure is expected for 20 years if the plastic sleeve is used in a normal atmosphere (23, 60%RH) and hot water (50).

A high-density multi-port optical connector that exploits the flexibility of bare optical fibers has been developed for use as an optical interface of a parallel optical interconnection module. In the BF (Bare-Fiber) connector, 24 multimode-fibers are mated by direct physical contact in micro-glass-capillaries with a 250-µm pitch. The buckling forces of the optical fibers themselves secure the physical contact. Optical fiber buckling is investigated theoretically and experimentally. A new design method to optimize the span length l and the longitudinal displacement ΔL for the buckling is also proposed based on the requirements afor optical characteristics, mechanical reliability, and dimensional tolerances, etc. A prototype BF connector with l 10 mm and ΔL of 50 µm was designed and fabricated for multimode fiber connections. This connector provides high optical performance: an average insertion loss of 0.05 dB and a return loss of over 35 dB at 850 nm. The optical performance remained stable after a durability test with ten connection-repetitions.

Peculiar patterns of SiO₂ contamination around the periphery of the contact trace caused by silicone vapor under switching at the boundary of 1.6 W were confirmed. For micro relays, the electrical power conditions are restricted to lower level. Therefore, it is important to ascertain the upper limit of the electrical power conditions for normal operation. The peculiar pattern is important as it is recognized as the first stage of the origination of contact failure. Causes of this pattern were discussed from the viewpoints of temperature distribution in the contact trace, molten metallic bridge, micro arc discharge, and supply of silicone vapor with oxygen. It is proposed that during the closing contacts, as maximum Joule heating occurs at the periphery of the true contact area and silicone vapor with oxygen is easily supplied at the periphery, SiO₂ grows around the contact trace. For the opening contacts, as the bridge or micro arc appears, silicone vapor with oxygen is supplied only outside of the contacts. Thus SiO₂ is formed mainly around the periphery of the trace. Moreover, SiO₂ was scattered radially depending on the sputtering of molten metal under rupture of the bridge. Therefore, the peculiar pattern forms as a result.

we evaluate the effect of express lots on production dispatching rule scheduling and cost in VLSI manufacturing final test process. In the assignment of express lots, we make comparisons of two rules, First In First Out (FIFO) rule which is widely used and WEIGHT+RPM rule which considers the time required for jig and temperature exchanges, the remaining processing time of the machine in use and the lot waiting time in queue. When using FIFO rule, the test efficiency begins to deteriorate and the test cost per chip begins to increase, if the content of express lots exceeds 15%. Furthermore, for 30% of express lots' content, the number of total processed lots decreases by 19% and the test cost per chip increases by 22% in comparison to the cases including no express lots. For WEIGHT+RPM rule, however, the test efficiency does not deteriorate and the test cost per chip does not increase even if the content of express lots is increased up to 50%. When we use WEIGHT+RPM rule, Express Lots Tolerances (ELTs), defined as the maximum content of express lots which permits the deterioration of the system characteristics by 5%, are about three times as high as ones when using FIFO rule. It is also found that WEIGHT+RPM rule maintains higher ELTs against the changes in the numbers of planned chips and prepared jigs as compared with FIFO rule.

High-speed and low-power techniques are described for megabit-class size-configurable CMOS SRAM macrocells. To shorten the design turn-around-time, the methodology of abutting nine kinds of leaf cells is employed; two-level via-hole programming and the array-address decoder embedded in each control leaf cell present a divided-memory-array structure. A new squashed-memory-cell architecture using trench isolation and stacked-via-holes is proposed to reduce access times and power dissipation. To shorten the time for writing data, per-bitline architecture is proposed, in which every bitline has a personal writing driver. Also, read-out circuitry using a current-sense-type two-stage sense amplifier is designed. The effect of the non-multiplexed bitline scheme for fast read-out is shown in a simulation result. To reduce the noise from the second- to first-stage amplifier due to a feedback loop, current paths are separated so as not to cause common impedance. To confirm the techniques described in this paper, a 1-Mb SRAM test chip was fabricated with an advanced 0.35-µm CMOS/bulk process. The SRAM has demonstrated 250-MHz operation with a 2.5-V typical power supply. Also, 100-mW power dissipation was obtained at a practical operating frequency of 150-MHz.

This paper describes a new floating-point divider (FDIV), in which the key features of redundant binary circuits and an asynchronous clock scheme reduce the delay time and area penalty. The redundant binary representation of +1 = (1, 0), 0 = (0, 0), -1 = (0,1) is applied to the all mantissa division circuits. The simple and unified representation reduces circuit delay for the quotient determination. Additionally, the local clock generator circuit for the asynchronous clock scheme eliminates clock margin overhead. The generator circuit guarantees the worst delay-time operation by the feedback loop of the replica delay paths via a C-element. The internal iterative operation by the asynchronous scheme and the modified redundant-binary addition/subtraction circuit keep the area small. The architecture design avoids extra calculation time for the post processes, whose main role is to produce the floating-point status flags. The FDIV core using proposed technologies operates at 42. 1 ns with 0.35 µm CMOS technology and triple metal interconnections. The small core of 13.5 k transistors is laid-out in a 730µm 910 µm area.

We examine crossing waveguides with three channels consisting of nonlinear material by means of FD-BPM (Finite Difference Beam Propagation Method). Specifically, we investigate how the insertion of a multimode waveguide into the crossing section of both 13 and 23 structures influences the switching characteristics of output power. We then confirm that these structures can be favorably applied to a wide variety of all-optical devices for integrated optics such as intensity-dependent optical switches, optical power distributors and so on.

A new electromagnetic coupling structure has been proposed for a millimeter wave DR-VCO. The structure consists of a microstrip substrate placed on a planar type dielectric resonator and provides a strongly confined electromagnetic field and a high Q. The resonator used in this structure is a TE₀₁₀ mode dielectric resonator composed of a dielectric substrate and electrodes on both sides of the substrate. Each electrode has a circular hollow patch. A microstrip circuit substrate with an aperture on the ground electrode is stacked on the resonator. The resonator is magnetically coupled to the transmission line through the aperture. The coupling structure has advantages as follows: (a) The electromagnetic field is strongly confined at the hollow patch, and (b) unloaded Q reduction is only 18% under a strong coupling. When the structure is used as a resonant circuit for a DR-VCO, the circuit can be small because the transmission lines to be isolated from the resonator are able to be placed near the resonator. Both a large loaded Q and a large reflection coefficient of a resonant circuit are obtained with the structure. Fabricated DR-VCO has following performances. The oscillation center frequency is 30. 242 GHz and the frequency tuning range is 91 MHz when the control voltage varies 2 to 10 V. An output power of more than 7.3 dBm and a C/N of 90 dBc/Hz at 100 kHz offset are obtained at the frequency range.

Basic characteristics of a short-ended coplanar waveguide (CPW) resonator of good spurious suppression property is studied. The resonator is loaded with open tubs at its middle position and makes a fully planar structure. The length of the resonator is shortened almost by half and the first spurious resonance goes up to more than 3 times of the fundamental resonant frequency without degradation of unloaded Q(Q₀). The origin and property of spurious response is thoroughly investigated to show the advantage and the limit of this configuration. The external Q(Q_e) and fundamental resonant frequency of the resonator are also clarified theoretically and experimentally. Using those result, a bandpass filter (BPF) is designed on the basis of the narrow band approximation is realized and its transmission characteristics are examined theoretically and experimentally. The spurious suppression characteristics have been realized by the present filter in accordance with the expectation.

The presence of a new surface-wave-like mode on CPWs of infinite width produces a complex transition region at the onset of leakage, involving the unusual simultaneous combination of a coupling region and a spectral gap. An examination of this region leads to a clear physical explanation of why sharp minima occur in the leakage behavior.

We investigated a radio interferometer for geodetic use that incorporates commercially available fiber-optic links modulated in the radio-frequency range, and a method for compensating for the delay occurring in the links. With this type of radio interferometer, we can perform baseline analysis without the need for estimating the clock difference between observation stations, which causes a relatively large error in the vertical component of the estimated position of the station. Another advantage of the interferometer is utilization of phase delay, which improves the accuracy of delay determination considerably. By analyzing the interferometer's signal-to-noise ratio, we estimated the practicable cable length to be 58.0 km. The results of preliminary experiments with short optical fiber links show that the differences in the cable delays of the fiber-optic links can be compensated for by calibration signals which make a round trip between the analysis station and the observation sites, and that phase delay can be measured successfully.

Resonant coupling type microstrip line interconnects using a bonding ribbon and dielectric pad have been designed and fabricated. The basic concept of this interconnect is the LC serial resonance of the pad capacitor and ribbon inductor. Both numerical simulation and experiment reveal low return loss and high efficiency connection at the predicted resonant frequency region, which can be readily shifted to higher frequencies by tuning the structural parameters. Improvement in bandwidth of the interconnect is demonstrated by using a pad with higher dielectric constant. Furthermore, it is also shown that a slight modification allows DC connection in addition to efficient coupling at the resonant frequency.