Electronics Guide

mm-Wave Packaging

Millimeter-wave packaging represents one of the most challenging aspects of high-frequency circuit design, where the package transitions from a passive housing to an active component of the RF system. At frequencies from 30 GHz to 300 GHz, conventional packaging approaches fail catastrophically as parasitic elements become resonant structures, bond wires act as inefficient antennas, and package dimensions approach or exceed a quarter-wavelength. The package must simultaneously provide electrical transitions with minimal loss and reflection, mechanical protection, thermal management, hermetic sealing for reliability, and electromagnetic shielding—all while maintaining consistent performance across temperature and throughout the product lifetime.

Modern mm-wave packaging demands a multidisciplinary approach that integrates electromagnetic design, materials science, thermal engineering, and manufacturing process control. The package architecture must address fundamental physical challenges: the need for extremely low-loss transitions from chip to board, the suppression of unwanted resonant modes and surface waves, the management of power dissipation in compact volumes, and the achievement of hermetic sealing without introducing RF discontinuities. Each packaging decision—from material selection to assembly process—directly impacts the electrical performance, thermal behavior, reliability, and manufacturability of the final product.

Fundamental Packaging Challenges at mm-Wave Frequencies

The millimeter-wave frequency regime transforms packaging from a relatively benign mechanical and thermal function into a critical RF design element. At 100 GHz, a wavelength of 3 mm means that package features measuring just 0.75 mm represent a quarter-wavelength—the characteristic dimension at which standing waves, resonances, and reflections become severe. Physical structures that appear microscopically small at lower frequencies now behave as distributed electromagnetic components with complex frequency-dependent behavior.

Traditional wire bonding, which provides adequate performance below 10 GHz, becomes essentially unusable above 30-40 GHz. The inductance of even a short 0.5 mm bond wire creates significant impedance at mm-wave frequencies, while the wire itself radiates power and couples to nearby structures. Similarly, conventional lead frames and standard IC packages introduce parasitics, discontinuities, and cavity resonances that completely dominate circuit performance. The package can easily contribute more loss and distortion than the active circuitry it contains.

Thermal management grows increasingly difficult as power densities increase and package sizes shrink. Modern mm-wave integrated circuits may dissipate several watts in die areas of just a few square millimeters, creating power densities exceeding 1 kW/cm². The packaging solution must extract this heat efficiently while maintaining electrical performance—a challenging requirement since good thermal conductors like metals create grounded planes and shielding structures that can disturb field distributions and introduce unwanted modes.

Package Resonances and Mode Control

Package cavities and enclosures inevitably support electromagnetic resonances when their dimensions approach half-wavelength multiples. These resonances can occur in the space between the chip and package lid, in the region between substrate layers, or in the air gaps created by assembly tolerances. When excited by the circuit, these resonant modes create dramatic peaks and nulls in the frequency response, generate spurious signals, reduce isolation between circuit elements, and can even lead to oscillation in amplifier circuits.

The resonant frequencies of a rectangular cavity are determined by its dimensions according to f = (c/2)√[(m/a)² + (n/b)² + (p/d)²], where a, b, and d are the cavity dimensions and m, n, p are integer mode numbers. For a typical mm-wave package with dimensions of 5 mm × 3 mm × 0.5 mm, the fundamental cavity resonance occurs near 30 GHz, with higher-order modes filling the spectrum at regular intervals. These resonances must be carefully characterized during design and their excitation minimized through proper circuit layout and mode suppression techniques.

Mode suppression strategies include the use of absorptive materials placed strategically within the package cavity, the introduction of metallic vias or posts that disrupt field patterns and raise resonant frequencies, and the deliberate design of cavity dimensions to push resonances outside the operating band. Absorptive materials must be lossy enough to damp resonances without being so lossy that they degrade the desired signal paths. Resistive films, magnetic materials loaded with carbonyl iron, and dielectric materials with controlled loss tangents can all serve this purpose.

Surface wave modes, which propagate along dielectric interfaces rather than being confined to transmission lines, present another form of unwanted mode that becomes problematic in mm-wave packages. Thin substrates with high dielectric constants readily support surface waves, which can carry energy away from intended signal paths and create coupling between supposedly isolated circuits. Suppression techniques include the use of via fences to create boundaries that reflect surface waves, graded dielectric profiles that reduce the field concentration at interfaces, and substrate thinning to push surface wave cutoff frequencies above the operating range.

Hermetic Sealing Considerations

Hermetic sealing protects sensitive mm-wave circuits from moisture, contaminants, and atmospheric corrosion while maintaining reliable electrical performance over the product lifetime. However, the requirements for hermetic integrity often conflict with those for optimal RF performance. Traditional sealing techniques like metal seam welding, glass frit bonding, and eutectic die attachment must be adapted to minimize their impact on electromagnetic behavior while still achieving leak rates below 10⁻⁸ atm·cc/sec of helium, the typical requirement for military and aerospace applications.

Metal lid attachment through soldering or welding can introduce problematic discontinuities unless carefully designed. The seal ring must be positioned to avoid creating resonant cavities or altering the impedance of nearby transmission lines. The lid-to-body interface must provide consistent electrical contact to maintain shielding effectiveness and prevent slot antenna radiation. Compression seals using metal gaskets or O-rings can provide hermiticity with minimal RF impact but require precise flatness and surface finish on the mating surfaces—typically better than a few micrometers over the seal perimeter.

Glass-to-metal seals offer excellent hermetic integrity and high-temperature capability but introduce dielectric interfaces that can support unwanted modes or create reflections. The glass composition must be matched to the thermal expansion of the metal parts to prevent cracking during temperature cycling, typically requiring matching to within a few ppm/°C. Kovar alloy (Fe-Ni-Co) is commonly used as the metal component due to its thermal expansion match to borosilicate glasses, though its moderate electrical conductivity requires plating with copper or gold for RF applications.

Epoxy-based seals provide lower cost and simpler processing than metal or glass seals but generally cannot achieve true hermetic performance. Moisture permeation through polymer seals limits their use to less demanding applications or requires protective conformal coatings on the internal circuitry. For mm-wave packages requiring both hermiticity and cost-effectiveness, hybrid approaches may be employed: a glass or metal hermetic seal for the primary cavity, with epoxy used only for non-hermetic closures or to attach external components.

Thermal Management Architecture

Effective thermal management in mm-wave packages requires careful integration of heat spreading structures, thermal conduction paths, and heat removal mechanisms without compromising electrical performance. The thermal resistance from junction to ambient must be minimized to maintain acceptable operating temperatures, typically requiring junction-to-case thermal resistances below 10-20°C/W for multi-watt circuits and sometimes below 5°C/W for high-power applications.

Die attachment techniques critically affect thermal performance. Eutectic die attach using gold-silicon or gold-tin solders provides excellent thermal conductivity (60-80 W/m·K for AuSn) with hermetic integrity and reliable high-temperature performance. The die attach layer must be kept thin—ideally below 10 μm—to minimize thermal resistance, requiring highly planar mounting surfaces and controlled process parameters. Silver-filled epoxies offer easier processing and lower stress but provide inferior thermal conductivity (2-4 W/m·K) and have temperature limitations around 150-200°C.

Heat spreading structures distribute localized heat sources across larger areas to reduce thermal resistance. Copper or molybdenum heat spreaders attached to the backside of the chip can effectively distribute heat laterally before it enters the package substrate. For GaN devices operating at very high power densities, diamond heat spreaders offer exceptional thermal conductivity (>1000 W/m·K) though at substantial cost. The interface between die and heat spreader must minimize thermal resistance through thin, high-quality bonding layers.

Package-level thermal paths typically conduct heat through the substrate to a metal baseplate or directly to a heat sink. Thick metal layers, thermal vias through dielectric substrates, and minimization of high-resistance interfaces all contribute to lower thermal resistance. For the highest power applications, microchannel cooling or direct liquid cooling may be integrated into the package structure, though these approaches add significant complexity and potential reliability concerns from fluid leakage or pump failures.

Thermal simulation during the design phase has become essential for modern mm-wave packages. Finite element analysis tools can predict temperature distributions, identify hot spots, and evaluate different heat spreading strategies before committing to expensive prototypes. These simulations must account for the three-dimensional geometry, material properties including temperature-dependent thermal conductivity, power dissipation maps from the circuit design, and boundary conditions representing the external cooling environment.

Transition Design for Minimal Loss and Reflection

Transitions between the integrated circuit, package substrate, and external transmission lines represent critical points where signal integrity can be compromised. Each interface introduces potential impedance discontinuities, parasitic reactances, and coupling to unwanted modes. Well-designed transitions maintain return loss better than 15-20 dB across the operating band while adding minimal insertion loss—typically targeting less than 0.5 dB per transition at the high end of the frequency range.

Chip-to-package transitions have evolved from wire bonding to more sophisticated approaches that maintain controlled impedance and minimal inductance. Flip-chip attachment using solder bumps or copper pillars provides the shortest electrical path—typically 50-150 μm in height—with inductances of just a few pH per bump. The bump pitch must be fine enough to accommodate required I/O density while maintaining sufficient mechanical integrity. Ground-signal-ground (GSG) bump patterns are commonly employed for high-frequency signals, with the ground returns providing shielding and a well-defined return current path.

Wafer-level ball grid array (WLBGA) and fan-out wafer-level packaging extend the flip-chip concept by redistributing the die I/Os to a larger area while maintaining very short electrical paths. These approaches can achieve transitions with less than 0.3 dB of loss up to 100 GHz when properly designed. The redistribution layer design requires careful electromagnetic simulation to ensure that the trace routing does not create resonances or couple to substrate modes.

Package-to-board transitions typically employ either surface-mount connectorized approaches or direct-attach methods like ball grid arrays. For frequencies above 60-70 GHz, standard rectangular coaxial connectors become lossy and dimensionally critical. Compact board-mount connectors designed specifically for mm-wave applications, such as 1.85 mm (67 GHz), 1.0 mm (110 GHz), or even smaller geometries, provide controlled impedance transitions with repeatability sufficient for production applications.

Waveguide transitions offer an alternative for the highest frequency applications, transitioning from planar transmission lines within the package to rectangular or circular waveguide for board or system-level interconnection. These transitions can be implemented using probe launches, ridge waveguide adapters, or antipodal fin-line structures. While waveguides provide lower loss than coaxial cables at mm-wave frequencies, the physical size of the waveguide and the precision required for the transition make this approach suitable primarily for fixed installations rather than portable or mobile applications.

Material Selection for mm-Wave Performance

Package substrate materials must satisfy competing electrical, thermal, and mechanical requirements. At mm-wave frequencies, the dielectric loss tangent becomes a dominant source of signal attenuation, with conductor losses also increasing substantially due to skin effect and surface roughness. The material must also provide adequate thermal conductivity, mechanical strength, coefficient of thermal expansion (CTE) matching to the semiconductor die, and compatibility with the chosen assembly processes.

Ceramic materials, particularly alumina (Al₂O₃) and aluminum nitride (AlN), serve as workhorse substrates for high-performance mm-wave packages. Alumina provides moderate dielectric constant (εr ≈ 9.8), low loss tangent (tan δ ≈ 0.0001 at mm-wave frequencies), good mechanical strength, and mature processing technology at reasonable cost. Aluminum nitride offers significantly better thermal conductivity (170-200 W/m·K vs. 20-30 W/m·K for alumina) with similar electrical properties, making it preferred for high-power applications despite higher material cost.

Low-temperature co-fired ceramic (LTCC) technology enables the fabrication of multilayer ceramic substrates with embedded passive components, transmission lines, and vias. LTCC materials typically have dielectric constants between 5 and 8 and loss tangents around 0.001-0.003. While the loss is higher than bulk alumina, LTCC provides substantial design flexibility through its multilayer capability and integrated component features. Careful material selection and process control can achieve acceptable performance through 100 GHz.

Organic substrates including high-frequency laminates like Rogers RO3000 or RO4000 series materials offer lower dielectric constants (εr ≈ 3-4) and reasonable loss tangents (tan δ ≈ 0.002-0.004) at significantly lower cost than ceramics. However, their thermal conductivity is poor (typically 0.5-0.8 W/m·K), limiting their use to lower power applications. The CTE mismatch between organic materials and silicon or GaAs die also creates reliability concerns, requiring underfill or other stress-relief approaches.

Metallization materials must provide high conductivity, good adhesion, and resistance to oxidation and electromigration. Gold plating over a thin nickel or titanium-tungsten barrier layer provides excellent conductivity and surface stability. Silver offers even better conductivity than gold but requires protective coatings to prevent tarnishing. Aluminum and copper are used in some applications where cost is paramount, though they require careful surface treatment to maintain long-term reliability. The metal thickness must exceed several skin depths at the operating frequency—typically requiring 3-5 μm or more at 100 GHz for gold metallization.

Surface roughness of conductors becomes increasingly important at mm-wave frequencies where the skin depth shrinks to submicron dimensions. Rough surfaces created by electroplating or chemical etching can significantly increase loss compared to smooth deposited films. The roughness can be characterized by RMS or peak-to-valley measurements, with smoother surfaces consistently providing better performance. Polishing, lapping, or specialized deposition techniques may be required to achieve the necessary surface quality.

Assembly Processes and Manufacturing Considerations

The assembly of mm-wave packages requires precise control of dimensional tolerances, material properties, and process parameters. Variations that would be insignificant at lower frequencies can dramatically affect performance at mm-wave. Process capability must be sufficient to maintain critical dimensions within a few percent of their nominal values, often requiring statistical process control and 100% inspection of critical parameters.

Die attachment processes must achieve high yield while maintaining electrical, thermal, and mechanical integrity. Eutectic die attach processes require careful control of peak temperature, time at temperature, bonding pressure, and atmosphere to achieve complete wetting and uniform bond line thickness. The process window is often narrow—temperature variations of more than ±5-10°C or timing variations of more than ±30 seconds can result in weak bonds or excessive voiding. Automated die bonders with precision temperature control and force feedback ensure consistent results.

Flip-chip assembly introduces additional challenges in solder bump formation, flux application, reflow profile control, and underfill dispensing. The solder bumps must be uniform in height and composition to achieve simultaneous bonding of all interconnects. Flux residues must be minimal and non-corrosive since they remain trapped under the die. The reflow profile must melt all solder bumps without overheating the die or substrate, requiring precise control and sometimes multiple temperature zones. Underfill material flows into the narrow gap between die and substrate to provide mechanical reinforcement and stress relief, but must not create voids or contaminate adjacent areas.

Wire bonding, when used for lower-frequency control signals or DC power connections in mm-wave packages, requires optimization for the specific materials and geometries involved. Ball bonding onto gold or aluminum pads requires appropriate deformation to achieve reliable metallurgical bonds without cracking the underlying structures. Ribbon bonding can provide lower inductance than wire bonding for certain applications, though the bonding process is more sensitive to surface planarity and contamination.

Lid attachment must create the required hermetic seal while maintaining dimensional tolerances that affect cavity resonances and electromagnetic shielding. Seam welding requires precise control of welding current, speed, and electrode force. Solder sealing demands temperature profiles that melt the solder preform completely while avoiding reflow of the die attach or other previously bonded assemblies—sometimes necessitating step-solder approaches with different melting points. Compression seals require controlled clamping force and uniform seal contact.

Quality control throughout assembly includes visual inspection for defects, X-ray inspection for hidden voids or misalignment in die attach and flip-chip bonds, hermeticity testing using fine-leak helium mass spectrometry or gross-leak fluorocarbon detection, and electrical testing to verify RF performance. High-value mm-wave packages may undergo 100% electrical screening rather than statistical sampling to ensure that every shipped unit meets specifications.

Reliability Testing and Qualification

Reliability testing validates that mm-wave packages will survive and maintain performance throughout their intended service life under expected environmental stresses. Military and aerospace applications follow rigorous qualification standards such as MIL-STD-883 or MIL-PRF-38534, requiring hundreds or thousands of test hours across multiple stress conditions. Commercial applications may adopt similar but less extensive protocols based on JEDEC standards or custom test plans addressing specific application requirements.

Thermal cycling tests subject packages to repeated temperature excursions between temperature extremes (typically -55°C to +125°C or wider) to induce thermomechanical fatigue in materials with mismatched thermal expansion. The cycling creates stresses in die attach interfaces, bond wires, solder joints, and package seals that accumulate over hundreds or thousands of cycles. Failures typically manifest as cracking in die attach, bond wire fatigue, or loss of hermeticity. High-performance packages must survive 500-1000 cycles without failure, with periodic electrical testing to detect degradation before complete failure occurs.

High-temperature storage testing exposes packages to elevated temperatures (typically +150°C or higher) for extended periods (500-1000 hours or more) to accelerate chemical degradation mechanisms including diffusion, oxidation, intermetallic compound growth, and electromigration. The temperature is chosen based on the Arrhenius equation to provide reasonable acceleration factors without introducing failure modes that would not occur at operating temperatures. Hermetic packages generally show excellent high-temperature stability if properly sealed, while non-hermetic packages may exhibit corrosion or contamination-related failures.

Temperature-humidity-bias testing combines elevated temperature (typically +85°C) with high relative humidity (85% RH) and applied voltage bias to accelerate corrosion and electrochemical migration mechanisms. This test is particularly important for non-hermetically sealed packages or packages with exposed bond wires or solder joints. Hermetic packages usually do not require extensive humidity testing unless the hermetic seal integrity is questionable.

Mechanical shock and vibration testing verifies structural integrity under handling, shipping, and operational mechanical stresses. Military applications may require survival of shocks up to 1500 G or more with millisecond duration pulses, and vibration profiles spanning 20 Hz to 2000 Hz with significant acceleration levels. Wire bonds are often the most vulnerable element, requiring optimization of bond loop height, wire diameter, and bonding profiles to achieve adequate mechanical robustness.

Power cycling testing applies electrical power in a cyclic fashion to create temperature changes from internal heating rather than external temperature forcing. This test stresses the thermal interfaces and the regions of maximum temperature gradient more severely than conventional thermal cycling. It is particularly important for power amplifiers and high-power circuits where junction temperatures may rise 50-100°C above ambient during operation. The test typically runs for thousands or tens of thousands of power cycles.

Electrical performance must be verified before and after each reliability stress to detect degradation. At mm-wave frequencies, key parameters include insertion loss, return loss, output power, gain, noise figure, and frequency stability. Even small changes—such as 0.5 dB increase in insertion loss or 2 dB degradation in return loss—can indicate developing failure mechanisms. Trend analysis across multiple test intervals enables early detection of failure modes before they cause complete device failure.

Advanced Packaging Architectures

System-in-package (SiP) approaches integrate multiple die, passive components, and interconnecting substrate technologies into a single package to achieve functionality that would previously require board-level assembly. At mm-wave frequencies, SiP architectures can minimize interconnection lengths between RF circuits, convert between transmission line types within the protected package environment, and embed filtering or matching networks directly in the substrate. The integration reduces overall size and potentially improves performance by eliminating board-level transitions and routing.

Antenna-in-package (AiP) takes integration one step further by incorporating the antenna elements within the package structure itself. This approach is particularly attractive for phased array applications at mm-wave where hundreds or thousands of antenna elements must be fed from corresponding RF circuits. The package substrate or a separate antenna layer contains the radiating elements—often patch antennas, slot antennas, or dipoles—connected to the driving circuitry through very short low-loss transitions. AiP dramatically simplifies system assembly and enables compact form factors for automotive radar, 5G communications, and imaging applications.

3D packaging using through-silicon vias (TSVs) enables vertical stacking of multiple die with extremely short interconnections between layers. TSV-based 3D packages can achieve hundreds of GB/s of bandwidth between stacked chips using thousands of vertical interconnects with capacitances and inductances orders of magnitude smaller than wire bonds or flip-chip bumps. While primarily developed for digital circuits, 3D packaging is beginning to find applications in mm-wave systems where heterogeneous integration of different process technologies (e.g., SiGe BiCMOS for RF with advanced CMOS for digital control) provides system advantages.

Wafer-level packaging (WLP) performs package assembly operations at the wafer scale before die singulation, enabling extremely small form factors and potentially lower cost through parallel processing. Fan-out wafer-level packaging (FOWLP) redistributes die I/Os to a larger area while maintaining wafer-level processing, providing flexibility for I/O placement and thermal enhancement. These approaches are being adapted for mm-wave applications with careful attention to the packaging-induced parasitics and mode control challenges.

Measurement and Characterization

Characterizing mm-wave package performance requires specialized measurement techniques and equipment capable of operating at the relevant frequencies with sufficient accuracy. Vector network analyzers (VNAs) form the primary tool for measuring S-parameters, which fully characterize the linear electrical behavior of package transitions, transmission lines, and complete packaged circuits. At mm-wave frequencies, VNA calibration becomes critical due to the short wavelengths and high frequencies involved. Multiple calibration standards must be measured to remove systematic errors from cables, connectors, and test fixtures.

De-embedding techniques mathematically remove the effects of test fixtures, probe pads, and access transmission lines to extract the intrinsic performance of the package structure itself. This process requires additional measurements of calibration standards or test structures with known properties. TRL (Thru-Reflect-Line), SOLT (Short-Open-Load-Thru), and multiline TRL calibration methods each have advantages depending on the specific geometry and frequency range. Proper de-embedding enables accurate comparison between simulation predictions and measured results.

Time-domain analysis can reveal the location of discontinuities and impedance variations along package signal paths. Time-domain reflectometry (TDR) measurements show reflected energy as a function of position, allowing identification of specific transitions or features that create reflections. Time-domain transmission (TDT) measurements reveal the transmitted signal including the effects of loss, dispersion, and multiple reflections. Modern VNAs can perform these time-domain transformations from frequency-domain S-parameter data.

Thermal characterization includes both steady-state junction-to-case thermal resistance measurements and transient thermal response testing. Thermal resistance is typically measured by operating the device at known power dissipation while monitoring junction temperature (via forward voltage drop, infrared imaging, or embedded temperature sensors) and case temperature. Transient measurements reveal the thermal time constants and thermal capacitance of the package structure, providing insight into the package's response to pulsed operation.

Non-destructive analysis techniques including acoustic microscopy can detect voids, delamination, and cracks in die attach, encapsulants, and package seals without destroying the package. X-ray imaging reveals wire bond positioning, solder joint integrity, and die placement. Cross-sectioning and microscopic examination provide the most detailed information about package construction but destroy the sample in the process—this technique is reserved for failure analysis and process development.

Emerging Trends and Future Directions

The push toward higher frequencies, higher integration levels, and more complex functionality continues to drive innovation in mm-wave packaging. Development of materials with lower loss tangents and better thermal properties, advances in assembly processes enabling finer features and tighter tolerances, and improvements in simulation tools allowing more accurate prediction of package behavior all contribute to enhanced package performance.

Additive manufacturing techniques including 3D printing of dielectric and metallic structures may enable package geometries and features impossible with conventional processes. Direct metal laser sintering can create complex three-dimensional metallic features with resolution approaching 50 μm, potentially enabling monolithic integration of waveguide components, heat sinks, and mechanical structures. Aerosol jet printing and other direct-write approaches can deposit conductors and dielectrics in arbitrary patterns without lithographic masking.

Advanced thermal interface materials including carbon nanotube arrays, graphene films, and phase-change materials promise dramatic reductions in thermal resistance between die and package or package and heat sink. These materials may achieve thermal conductivities exceeding conventional approaches by 2-10×, enabling higher power densities or reduced cooling requirements.

Optical interconnects are beginning to supplement or replace electrical interconnects in packages requiring very high data rates. Silicon photonic circuits can integrate laser sources, modulators, and photodetectors with CMOS control circuitry, with optical fibers or waveguides carrying the signals between package locations or between packages. While the technology is currently expensive and primarily used in data center applications, continued development may extend optical packaging to broader mm-wave systems where electrical interconnect bandwidth becomes limiting.

Machine learning and artificial intelligence applied to package design and optimization can explore design spaces too large for manual investigation, potentially discovering novel configurations that achieve superior performance. AI-driven process control in manufacturing can adapt process parameters in real-time to maintain quality despite variation in incoming materials or environmental conditions. Predictive reliability modeling using physics-based models enhanced by machine learning from field return data may enable more accurate lifetime predictions and proactive maintenance.

Conclusion

mm-Wave packaging represents a critical enabling technology for the deployment of millimeter-wave systems in communications, radar, imaging, and sensing applications. Success requires simultaneous optimization of electrical performance, thermal management, reliability, and cost through careful material selection, transition design, mode suppression, hermetic sealing when required, and well-controlled assembly processes. The package must be viewed not as a passive container but as an integral component of the RF system whose design is as critical as the circuits it houses.

As operating frequencies continue to increase and performance requirements become more demanding, packaging technologies must evolve to meet these challenges. The integration of multiple functions within single packages, the use of advanced materials and processes, and the application of sophisticated simulation and characterization tools all contribute to advancing the state of the art. Engineers working in this field must combine deep understanding of electromagnetics, materials science, thermal engineering, and manufacturing processes to create packages that enable the next generation of mm-wave systems.