Semiconductor Devices

Chapter 14
Reliability, Failure Physics, and Qualification

Post Graduate Program in Electronics and Communication Engineering
Semiconductor Devices   •   Post Graduate

Reliability, Failure Physics, and Qualification

Introduction and Context

Semiconductor devices are expected to perform predictable electrical functions for years while being exposed to electrical stress, temperature variation, humidity, vibration, radiation, contamination, and manufacturing variability. Reliability engineering addresses the probability that a device or system will perform its specified function for a stated time, under stated conditions. Failure physics explains the mechanisms by which performance degrades or functionality is lost. Qualification establishes, through structured testing and evidence, whether a technology, process, package, or product is sufficiently robust for its intended application.

These three ideas are related but not interchangeable. Reliability is a probabilistic property; failure physics is a causal and physical explanation; qualification is an evidence-generation and decision process. A device can pass a qualification test without its field reliability being fully known, and a statistically reliable device can still fail if it is operated outside its specified conditions.

In advanced semiconductor manufacturing, reliability is no longer limited to package cracking or gross contamination. It includes bias-temperature instability, hot-carrier degradation, time-dependent dielectric breakdown, electromigration, stress-induced voiding, dielectric damage, random telegraph noise, single-event effects, thermal cycling, interfacial delamination, corrosion, and aging of compound-semiconductor and wide-bandgap structures.

Learning Objectives

After completing this chapter, the student should be able to:

  1. Define reliability, failure rate, lifetime, maintainability, and availability.
  2. Distinguish intrinsic, extrinsic, random, wear-out, and catastrophic failure mechanisms.
  3. Explain the physical origins of major semiconductor failure mechanisms.
  4. Apply exponential, Weibull, Arrhenius, and Eyring-type models within their assumptions.
  5. Design and interpret accelerated life, qualification, and reliability-monitoring tests.
  6. Relate electrical degradation data to physical failure analysis.
  7. Evaluate qualification evidence, confidence limits, and limitations of extrapolation.
  8. Integrate reliability engineering into semiconductor design, manufacturing, and field-return analysis.

1. Reliability as a Quantitative Engineering Concept

For a non-repairable device, the lifetime is represented by a random variable T. The reliability function is the probability that failure has not occurred by time t:

R(t) = P(T > t) = 1 − F(t)

Here, F(t) is the cumulative distribution function of failure time. The probability density is f(t) = dF(t)/dt. The hazard rate, or instantaneous failure rate conditional on survival to time t, is:

λ(t) = f(t) / R(t)

The units of λ(t) are inverse time, commonly failures per hour. The mean time to failure is:

MTTF = E[T] = ∫₀∞ R(t) dt

These expressions apply to statistically defined populations and require a clearly specified failure criterion. The criterion may be catastrophic failure, parametric drift beyond a limit, leakage-current increase, threshold-voltage shift, gain loss, or inability to meet a system function.

1.1 Important reliability measures

QuantityMeaningTypical use
MTTFMean time to failure for non-repairable itemsSemiconductor lifetime estimates
MTBFMean time between failures for repairable systemsEquipment and system reliability
FITFailures in 10⁹ device-hoursLow failure-rate reporting
R(t)Probability of survival to time tMission reliability
AvailabilityFraction of time a repairable system is operationalCommunication and computing systems
B10 lifeTime by which 10% of a population has failedWear-out and qualification analysis

For a constant failure rate λ, the lifetime distribution is exponential:

R(t) = e^(−λt)

The exponential model assumes a constant hazard rate and is therefore most suitable for a useful-life region in which failures occur randomly and wear-out is negligible. Under this model, MTTF = 1/λ. If failure rate is reported in FIT:

λ = FIT × 10⁻⁹ h⁻¹

For example, 100 FIT corresponds to λ = 1.0 × 10⁻⁷ h⁻¹ and an exponential MTTF of 10⁷ h. This does not imply that every device lasts 10⁷ h; it is a population mean under the model.

1.2 The bathtub curve

The classical bathtub curve contains three regions: early failures, useful life, and wear-out. Early failures arise from manufacturing defects and screening escapes; the useful-life region is approximately random; wear-out results from cumulative physical damage. Modern semiconductor products may not display a clean bathtub curve because multiple mechanisms overlap and field conditions are non-stationary.

Reliability block diagrams are useful at system level. For independent components in series, where every component must operate, system reliability is:

Rseries(t) = ∏ᵢ Rᵢ(t)

For independent, identical components in a one-out-of-n parallel configuration:

Rparallel(t) = 1 − [1 − R(t)]ⁿ

Independence is a strong assumption. Shared thermal environments, common power supplies, common process defects, and correlated overstress can invalidate these simple expressions.

2. Failure Distributions and Statistical Interpretation

The Weibull distribution is especially useful for semiconductor failure populations because its shape parameter can represent infant mortality, random failure, or wear-out:

F(t) = 1 − exp[−(t/η)^β]

where β > 0 is the shape parameter and η > 0 is the characteristic life, the time at which 63.2% of the population has failed. Its reliability is:

R(t) = exp[−(t/η)^β]

The hazard rate increases when β > 1, is constant when β = 1, and decreases when β < 1. Thus β is physically informative, but it should not be interpreted without examining censoring, competing failure modes, sample selection, and test conditions.

The B10 life is obtained by setting F(t) = 0.10:

B10 = η[−ln(0.90)]^(1/β)

Worked Example 1: Weibull life

Suppose a population has β = 2 and η = 10,000 h. The reliability at 5,000 h is:

R(5000) = exp[−(5000/10000)²] = exp(−0.25) ≈ 0.7788.

Thus approximately 77.9% survive to 5,000 h under the stated conditions. The B10 life is:

B10 = 10000[−ln(0.90)]^(1/2) ≈ 10000(0.3246) ≈ 3,246 h.

This estimate is model-dependent and should not be reported without confidence bounds.

2.1 Censoring and confidence

Reliability tests commonly end before all units fail. Such observations are right-censored: the unit is known to have survived at least to the censoring time. Ignoring censored observations biases lifetime estimates. Maximum-likelihood estimation, Kaplan–Meier methods, and confidence intervals are therefore important.

A zero-failure demonstration test does not prove zero failure probability. If n independent units are tested for duration t under constant failure rate and zero failures occur, an approximate one-sided upper confidence bound at confidence level 1 − α is:

λupper = −ln(α) / (nt)

For α = 0.10, this is a 90% upper confidence bound. The formula assumes independent identical units, constant hazard, and an appropriate failure definition.

3. Physics of Semiconductor Failure

Failure physics links stress, material response, defect evolution, and functional failure. The most useful engineering chain is:

Applied stress → local physical damage → parameter degradation → specification violation → functional failure.

The same electrical symptom may have different physical causes. For example, increased leakage can result from junction damage, dielectric defects, contamination, edge termination breakdown, or thermal damage. Consequently, electrical testing should be combined with physical analysis such as microscopy, cross-sectioning, emission microscopy, secondary-ion mass spectrometry, focused-ion-beam preparation, and spectroscopy.

3.1 Electromigration

Electromigration is the transport of metal atoms caused by momentum transfer from conducting electrons and by temperature-dependent atomic diffusion. It can produce voids, which increase resistance or open a line, and hillocks, which can short adjacent conductors.

A commonly used empirical relationship is Black’s equation:

MTTF = A J^(−n) exp(Ea / kT)

A is a process-dependent constant, J is current density, n is an empirical current-density exponent, Ea is activation energy, k is Boltzmann’s constant, and T is absolute temperature. The equation assumes a dominant thermally activated electromigration mechanism and a defined metallization system. It should not be extrapolated across mechanism changes, different microstructures, or different current-direction conditions without validation.

Design responses include reducing current density, improving barrier and liner integrity, using redundant vias, controlling line temperature, and avoiding severe current crowding at contacts and corners.

3.2 Time-dependent dielectric breakdown

A gate or interlayer dielectric can accumulate defects under electric field and temperature until a conductive path forms. Breakdown may be hard, causing abrupt leakage, or soft, causing a progressive increase in leakage and noise. The measured lifetime depends strongly on field distribution, dielectric thickness, polarity, area, defect generation, and failure criterion.

Common lifetime models include empirical field-acceleration forms such as:

tBD = A exp(−γE)

and temperature-augmented forms. Here tBD is breakdown time, E is electric field, γ is a fitted field-acceleration parameter, and A is a fitted constant. The model is valid only over the calibrated field and temperature range and for a consistent dielectric and failure definition.

3.3 Bias-temperature instability

Bias-temperature instability causes threshold-voltage shift and transconductance degradation in MOS devices. Positive bias-temperature instability is particularly important for p-channel devices with positive gate bias, while negative bias-temperature instability affects n-channel devices under corresponding stress conditions. Charge trapping and interface-state generation contribute to the shift, and recovery may occur after stress removal.

A simplified empirical representation is:

∆VT = A tⁿ

where ∆VT is threshold-voltage shift, t is stress time, and A and n depend on voltage, temperature, device geometry, and process. Because recovery is important, measurement delay and readout protocol must be controlled. A permanent-shift interpretation may overestimate degradation if transient trapping is included.

3.4 Hot-carrier degradation

High-energy carriers near the drain can generate interface states and oxide-trapped charge. This reduces transconductance, changes threshold voltage, and may increase substrate current. Hot-carrier stress is sensitive to drain voltage, gate voltage, channel length, temperature, and device architecture. Short-channel scaling and lightly doped drain structures have altered the dominant conditions but have not eliminated the mechanism.

3.5 Thermal and mechanical failure

Temperature accelerates diffusion, reaction, defect generation, and many chemical processes. Thermal expansion mismatch between silicon, die attach, mold compound, substrate, solder, and board can generate cyclic mechanical stress. Repeated thermal cycling may cause solder fatigue, bond-wire heel cracking, die cracking, delamination, and package warpage.

A useful first-order measure of thermal mismatch is:

∆ε ≈ (α₁ − α₂)∆T

where ∆ε is differential strain, α₁ and α₂ are coefficients of thermal expansion, and ∆T is the temperature excursion. This relation assumes small strain and approximately uniform materials; real packages require finite-element analysis because geometry, viscoelasticity, plasticity, and interfaces strongly influence stress.

3.6 Moisture, corrosion, and contamination

Moisture can plasticize mold compounds, promote corrosion, cause popcorning during reflow, and reduce insulation resistance. Ionic contaminants can migrate under bias and humidity, creating leakage paths or dendrites. Corrosion is controlled through materials selection, passivation, clean processing, package design, humidity control, and electrical spacing.

3.7 Radiation and single-event effects

Ionizing radiation creates electron–hole pairs and trapped charge, while displacement damage alters semiconductor lattices. Single-event effects occur when a single energetic particle deposits sufficient charge to cause a transient, upset, latch-up, or destructive burnout. Space, nuclear, avionics, and high-altitude applications require technology-specific radiation qualification.

4. Stress, Acceleration, and Lifetime Models

Reliability testing often accelerates failure by increasing temperature, voltage, current density, humidity, or mechanical cycling. The central requirement is mechanism preservation: the accelerated test must activate the same dominant failure mechanism as the use condition.

4.1 Arrhenius temperature acceleration

For a thermally activated process, the rate is often represented as:

r(T) = A exp(−Ea / kT)

The acceleration factor from use temperature Tu to stress temperature Ts is:

AF = exp[(Ea/k)(1/Tu − 1/Ts)]

Temperatures must be in kelvin, Ea in joules per particle or equivalently electron-volts with a consistent value of k, and Ts > Tu for acceleration. The model assumes one dominant thermally activated mechanism and constant activation energy over the range. Excessively high stress temperature may activate a different mechanism, making extrapolation invalid.

Worked Example 2: Arrhenius acceleration

Let Ea = 0.7 eV, Tu = 85 °C = 358.15 K, Ts = 125 °C = 398.15 K, and k = 8.617 × 10⁻⁵ eV/K.

AF = exp[(0.7/(8.617 × 10⁻⁵))(1/358.15 − 1/398.15)]

The reciprocal-temperature difference is approximately 2.806 × 10⁻⁴ K⁻¹. Therefore the exponent is approximately 2.28 and AF ≈ 9.8. A 1,000 h stress test would correspond to approximately 9,800 h at the use temperature only if the mechanism, failure criterion, and thermal history remain comparable.

4.2 Voltage and humidity acceleration

Voltage acceleration may be modeled with an inverse-power law:

tf = B V^(−n)

where tf is time to failure, V is applied voltage, and B and n are fitted constants. Field acceleration may instead be exponential. Humidity effects are often represented by empirical temperature–humidity models, such as the Peck model, but parameters are technology- and package-specific. These models should be fitted from designed experiments rather than assumed universally.

4.3 Eyring-type models

When more than one stress variable matters, an Eyring-type model may be used:

ln(L) = a + b/T + cS + dS/T

where L is a lifetime or characteristic-life measure, T is absolute temperature, S is another stress variable, and a, b, c, d are fitted coefficients. The model is useful for planned multifactor experiments but can be misleading if interactions, mechanism transitions, or non-linear damage accumulation are ignored.

5. Qualification and Reliability Demonstration

Qualification is a formal assessment that a product or technology is robust enough for a defined application. It usually combines design review, process audits, environmental stress tests, electrical characterization, sample inspection, and failure analysis. Qualification is not identical to production screening. Qualification challenges a design or process using representative samples; screening examines individual units to remove defective items.

A typical qualification flow is:

  1. Define mission profile, operating limits, failure criteria, and sample plan.
  2. Identify likely failure mechanisms using design and process analysis.
  3. Select stresses that accelerate relevant mechanisms without creating artifacts.
  4. Characterize pre-stress electrical and physical parameters.
  5. Apply environmental, electrical, mechanical, and endurance stresses.
  6. Perform intermediate and final electrical measurements.
  7. Analyze failures and determine root cause.
  8. Document statistical confidence, deviations, corrective actions, and release decision.

Common stress categories include high-temperature operating life, high-temperature storage, temperature cycling, thermal shock, humidity-bias testing, highly accelerated stress testing, electrostatic discharge, latch-up, package integrity, solderability, vibration, mechanical shock, and radiation tests where applicable.

Industry standards provide test methods and acceptance structures. Examples include JEDEC semiconductor reliability standards, AEC-Q100 for automotive integrated circuits, MIL-STD methods for military environments, and IEC or other sector-specific standards. A standard does not remove the need for engineering judgment: the selected grade, mission profile, failure criteria, and sample plan must match the product application.

5.1 Qualification versus production monitoring

Qualification is normally performed at technology introduction, major process change, package change, or design change. Reliability monitoring continues through production and field life. Monitoring includes parametric control charts, defect-density tracking, wafer-level reliability, lot acceptance, early-life failure analysis, customer-return analysis, and periodic requalification.

5.2 Wafer-level reliability

Wafer-level tests isolate process and structure weaknesses before full packaging. Examples include capacitor dielectric breakdown, transistor bias-temperature instability, electromigration test structures, contact resistance, and metal line continuity. Such tests reduce cost and improve physical correlation, but they may not capture package-induced stress, assembly defects, board interactions, or system-level thermal behavior.

6. Failure Analysis and Root-Cause Methodology

Failure analysis begins with failure verification. The analyst must reproduce the reported symptom, preserve the unit, and avoid introducing damage during handling. A robust workflow is:

  • confirm electrical failure and operating history;
  • compare with a known-good control;
  • localize the failing node using non-destructive methods;
  • use optical, thermal, emission, acoustic, X-ray, or electrical localization;
  • prepare a physical cross-section only after evidence is preserved;
  • identify the defect and its initiating mechanism;
  • determine escape point and corrective action;
  • verify correction through a targeted experiment.

Root cause should be distinguished from failure site. A cracked bond wire is a failure site; excessive loop height, mold-flow stress, or an assembly-tool defect may be the root cause. Similarly, a gate-oxide breakdown site is not necessarily the root cause if contamination, voltage overshoot, or a process excursion initiated the defect.

Useful analytical tools include fault-tree analysis, failure-mode and effects analysis, design of experiments, Pareto analysis, fishbone diagrams, statistical process control, and physics-of-failure modeling. A failure mode and effects analysis should rank severity, occurrence, and detectability, but numerical risk-priority scores should not replace engineering judgment.

7. Applied Case Study: Illustrative Automotive Power Module Failure

Background

Consider an illustrative silicon-carbide power module used in an electric-vehicle inverter. The module passes initial production tests but exhibits intermittent open-circuit behavior after 600 thermal cycles between −40 °C and 175 °C.

Problem

Field returns show increased on-state voltage followed by complete loss of conduction in one phase leg. The failure rate is low but unacceptable because the consequence is loss of propulsion torque.

Analysis

Electrical characterization reveals increased resistance before open-circuit failure. X-ray imaging shows no gross die fracture, but acoustic microscopy indicates localized delamination near a die-attach region. Cross-sectional analysis finds voiding and a crack propagating from a die-attach edge toward a metallized contact. The measured temperature profile also shows a local hot spot caused by current crowding.

The initial hypothesis was bond-wire fatigue. However, microscopy shows intact bond wires in most failed samples. Finite-element analysis indicates that the combination of coefficient-of-thermal-expansion mismatch, die-attach voids, and local temperature gradients produces cyclic shear stress at the attach perimeter.

Approach and solution

The manufacturer implements four changes: improved die-attach void control, rounded metallization corners, reduced current crowding through layout modification, and an expanded thermal-cycle test using a representative power mission profile. In addition, an in-line acoustic inspection limit is introduced, and resistance is measured at intermediate cycle intervals to detect progressive degradation.

Outcome

The revised module shows no open-circuit failures in the expanded qualification sample, while the distribution of on-state resistance remains stable. The conclusion is not simply that one test was passed; rather, the evidence supports a causal chain from thermal mission profile to local stress, damage accumulation, parametric drift, and final failure.

Learning points

  1. A qualification test is most valuable when linked to a physical failure model.
  2. Intermediate parametric measurements can reveal degradation before catastrophic failure.
  3. Screening for a visible defect is not a substitute for correcting the design margin.
  4. Field reliability requires package, assembly, thermal, electrical, and system analysis together.

8. Design-for-Reliability and Best Practice

Reliability should be designed in rather than tested into a finished product. Best practice includes:

  • define realistic voltage, current, temperature, humidity, vibration, and duty-cycle margins;
  • identify physics-of-failure mechanisms during architecture and layout;
  • use guard bands based on distributions, not only nominal values;
  • control hotspots and current density;
  • design package interfaces for thermal and mechanical compatibility;
  • include electrostatic-discharge and electrical-overstress protection;
  • separate qualification, screening, and monitoring objectives;
  • use statistically justified sample sizes and confidence limits;
  • preserve failed units and document chain of custody;
  • correlate accelerated tests with field data;
  • requalify after material, process, mask, package, or supplier changes;
  • track reliability indicators across the entire supply chain.

Reliability allocation at system level should reflect mission importance. Safety-critical automotive, medical, aerospace, and infrastructure applications require traceability, change control, independent review, and documented evidence. Ethical responsibility is central: suppressing adverse test results, redefining failure criteria after observing failures, or claiming field reliability from unrepresentative stress tests can create unacceptable safety risks.

9. Contemporary Developments and Research Directions

Advanced nodes introduce new geometries, materials, and variability sources. Gate-all-around transistors, backside power delivery, three-dimensional integration, hybrid bonding, chiplets, advanced packaging, and high-bandwidth memory create reliability interactions that are not captured by isolated transistor tests. Thermal resistance, power density, interface integrity, and interconnect fatigue increasingly dominate system reliability.

Wide-bandgap devices such as SiC and GaN enable high temperature and high frequency operation but introduce challenges involving dynamic on-resistance, gate reliability, trapping, threshold-voltage instability, avalanche behavior, and package parasitics. Reliability models must reflect switching waveforms rather than only static voltage and current.

Machine learning can assist anomaly detection, predictive maintenance, defect classification, and lifetime estimation. However, AI models require representative data, physical interpretability, drift monitoring, and safeguards against confounding process changes. A model trained on one product generation should not automatically be used for another. Physics-informed machine learning is promising because it combines measured degradation with constraints from known mechanisms.

Challenges and Limitations

Reliability prediction is limited by scarce failures, competing mechanisms, non-constant field conditions, sample-to-sample variation, and uncertainty in acceleration parameters. Extrapolation over several decades of time is especially sensitive to small errors in activation energy or fitted exponents. Qualification samples may not represent all process corners or supplier variation. Zero observed failures provide evidence, not certainty. Finally, a device may be reliable under its specified mission but unsafe when subjected to electrical overstress, inadequate cooling, or uncontrolled environmental exposure.

Chapter Summary

Reliability is the probability of successful operation for a specified time and condition, whereas failure physics explains how stress produces degradation and qualification provides structured evidence of robustness. Reliability functions, hazard rates, MTTF, FIT, Weibull distributions, and confidence bounds provide the statistical foundation. Major semiconductor failure mechanisms include electromigration, dielectric breakdown, bias-temperature instability, hot-carrier degradation, thermal-mechanical fatigue, moisture-induced corrosion, contamination, and radiation effects.

Arrhenius, inverse-power, Black’s, Weibull, and Eyring-type models are useful only within their assumptions and calibrated ranges. Accelerated testing must preserve the dominant field mechanism. Qualification should combine electrical characterization, environmental stress, physical inspection, statistical analysis, and root-cause failure analysis. Design-for-reliability, process control, package engineering, mission-profile analysis, and ethical reporting are essential for dependable semiconductor products.

Key Terms

Reliability: Probability that a device performs its specified function for a stated time and condition.

Failure rate: Instantaneous conditional rate of failure among surviving units.

Hazard function: Failure rate expressed as a function of elapsed time.

MTTF: Mean time to failure for a non-repairable item.

FIT: Expected failures per 10⁹ device-hours.

Weibull distribution: Lifetime distribution characterized by shape and scale parameters.

Characteristic life: Weibull time at which 63.2% of units have failed.

B10 life: Time by which 10% of a population has failed.

Censoring: Observation in which a unit has survived beyond the test endpoint.

Qualification: Formal evidence that a design or process meets defined reliability requirements.

Screening: Testing intended to remove defective individual units.

Electromigration: Current-induced atomic transport in conducting materials.

Time-dependent dielectric breakdown: Progressive dielectric damage leading to leakage or breakdown.

Bias-temperature instability: Electrical degradation caused by electrical bias and temperature.

Hot-carrier degradation: Damage caused by energetic carriers in a semiconductor device.

Arrhenius model: Thermally activated acceleration model.

Physics of failure: Causal analysis connecting stress, damage, degradation, and failure.

Mission profile: Time-dependent description of environmental and operating conditions.

Failure analysis: Investigation used to localize, identify, and explain a failure.

Confidence bound: Statistical limit expressing uncertainty in a reliability estimate.

Review Questions

Short Answer Questions

  1. Define reliability and distinguish it from qualification.
  2. What physical meaning is assigned to the Weibull shape parameter β?
  3. State two assumptions required for use of an Arrhenius acceleration model.
  4. Explain the difference between a failure site and a root cause.
  5. Why are intermediate electrical measurements useful during qualification?

Long Answer Questions

  1. Explain the bathtub curve and discuss why it may not accurately represent a modern semiconductor product.
  2. Describe electromigration, including its physical mechanism, electrical consequences, and design controls.
  3. Compare qualification testing, production screening, and reliability monitoring.
  4. Explain how thermal expansion mismatch can produce package failure during temperature cycling.
  5. Discuss the limitations of accelerated life testing and statistical extrapolation.

Analytical / Application Questions

  1. A device population follows a Weibull distribution with β = 2.5 and η = 8,000 h. Calculate its reliability at 4,000 h and its B10 life. State the assumptions of your calculation.
  2. A qualification test has zero failures among 2,000 devices, each tested for 1,000 h. Using a 90% one-sided confidence bound, estimate the upper failure-rate bound in FIT.
  3. An automotive power device shows increasing on-state resistance after thermal cycling. Propose a complete failure-analysis plan that distinguishes die degradation, bond failure, die-attach fatigue, and measurement artefacts.

Multiple Choice Questions with Answers

Question 1

Which quantity is defined as the probability that a device survives beyond time t?

A. Failure density

B. Reliability function

C. Hazard rate

D. Activation energy

Correct Answer: B. Reliability function

Question 2

For a Weibull distribution, a shape parameter β greater than 1 generally indicates:

A. Decreasing hazard rate

B. Constant hazard rate

C. Increasing hazard rate

D. Zero failure probability

Correct Answer: C. Increasing hazard rate

Question 3

Which mechanism is directly associated with current-induced atomic transport in metal interconnects?

A. Electromigration

B. Bias-temperature instability

C. Radiation displacement damage

D. Moisture absorption

Correct Answer: A. Electromigration

Question 4

In an Arrhenius acceleration model, temperature must be expressed in:

A. Degrees Celsius

B. Degrees Fahrenheit

C. Kelvin

D. Relative humidity percentage

Correct Answer: C. Kelvin

Question 5

A qualification test primarily provides evidence about:

A. The color uniformity of a package

B. The robustness of a design or process under defined stresses

C. The exact lifetime of every fielded unit

D. The market price of a device

Correct Answer: B. The robustness of a design or process under defined stresses

Question 6

If β = 1 in a Weibull model, the hazard rate is:

A. Constant

B. Always increasing quadratically

C. Always zero

D. Undefined

Correct Answer: A. Constant

Question 7

Which observation is an example of right censoring?

A. A unit fails at the start of the test

B. A unit survives until the test ends without failing

C. A unit is deliberately destroyed before testing

D. A unit has a measured nominal parameter

Correct Answer: B. A unit survives until the test ends without failing

Question 8

For independent components connected in series, system reliability is generally:

A. The sum of component reliabilities

B. The average of component reliabilities

C. The product of component reliabilities

D. One minus the product of component reliabilities

Correct Answer: C. The product of component reliabilities

Question 9

Which practice best supports a valid accelerated life test?

A. Changing the failure criterion during the test

B. Using stresses that preserve the dominant field failure mechanism

C. Ignoring censored observations

D. Testing only the single best-performing unit

Correct Answer: B. Using stresses that preserve the dominant field failure mechanism

Question 10

A bond-wire crack is best described as what in a root-cause investigation?

A. Necessarily the ultimate root cause

B. A possible failure site requiring causal investigation

C. A statistical confidence limit

D. An acceleration factor

Correct Answer: B. A possible failure site requiring causal investigation

Semiconductor Devices
Chapter 14 of 14