Semiconductor Detectors and Their Applications

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Questions and Answers

Match the semiconductor detectors with their primary application:

Silicon Diode Detectors = Gamma spectroscopy Germanium Gamma-ray Detectors = Energy measurement of charged particles Lithium Drifted Silicon Detectors = Tracking and vertexing Scintillation Counters = Tracking, particle identification

Match the semiconductor property with its description:

Valence Band = Electrons bound to specific lattice sites Conduction Band = Electrons free to move through the crystal Bandgap = Determines the type of semiconductor material Electron-Hole Pairs = Information carriers in semiconductor detectors

Match the characteristics of semiconductor diode detectors with their features:

Superior Energy Resolution = Best energy resolution in routine use Compact Size = Small detector dimensions Fast Timing Characteristics = Relatively quick response Radiation-Induced Damage = High susceptibility in small sizes

Match the materials with their impurity levels:

<p>Ge = Several cm Si = Several mm with higher impurity level than Ge Si (high purity) = Lower impurity than Si (higher level) Ge (high purity) = Low impurity compared to Ge</p> Signup and view all the answers

Match the type of detection to its description:

<p>Solid-state Detectors = Use electron-hole pairs as information carriers Gas Detectors = Detection medium with lower density than solids Scintillation Detectors = Based on photoelectric effect with statistical fluctuations Semiconductor Detectors = Yield larger number of charge carriers</p> Signup and view all the answers

Match the solid-state detector applications with their fields:

<p>Nuclear Physics = Gamma spectroscopy and energy measurement Particle Physics = Tracking and beam condition monitoring Satellite Experiments = Particle identification and tracking Security and Medicine = Applications in health and safety monitoring</p> Signup and view all the answers

Match the fabrication techniques with their descriptions:

<p>Ion implantation = Newer method for fabricating silicon junction detectors Photolithography = Used in combination with ion implantation Complex electrode geometries = Achievable through modern fabrication methods Planar fabrication = Junction edges buried within wafer</p> Signup and view all the answers

Match the limitations of semiconductor detectors with their descriptions:

<p>Limitation to Small Sizes = Restricted dimensions for effective use Radiation-Induced Damage = Susceptibility due to environmental exposure Cost = Higher expense compared to alternative detectors Statistical Fluctuations = Energy resolution affected by number of carriers</p> Signup and view all the answers

Match the factors influencing leakage current:

<p>Minority carrier current = Roughly proportional to junction area Thermal generation = Electron-hole pairs within depletion region Surface leakage effects = Depending on encapsulation and humidity Voltage supply = Via large-value series resistor</p> Signup and view all the answers

Match the semiconductor terms with their meanings:

<p>Band Structure = Arrangement of energy levels in solids Discrete Electron Energy Levels = Isolated atom energy configuration Periodic Lattice = Crystalline structure regulating energy bands Allowed Energy Bands = Regions where electrons can exist in solids</p> Signup and view all the answers

Match the terms with their effects on detector operation:

<p>Low bias voltage = Pulse height rises with applied voltage High electric fields = Induces multiplication effects Saturation region = Pulse height no longer changes with voltage Incomplete charge collection = Trapping and recombination effects</p> Signup and view all the answers

Match the following types of semiconductors with their characteristics:

<p>Intrinsic Semiconductors = Pure semiconductor materials Extrinsic Semiconductors = Doped semiconductors to alter properties n-type Semiconductors = Doping with electron donors p-type Semiconductors = Doping with electron acceptors</p> Signup and view all the answers

Match the pulse characteristics with their details:

<p>Pulse rise time = Generally about 10ns or less Charge transit time = Critical for fast detection Detector speed = Among the fastest radiation detectors Signal integration = Involves large resistor for bias voltage</p> Signup and view all the answers

Match the sources of leakage current with their origins:

<p>Bulk volume = Main contributor to leakage Detector surface = Affects overall leakage Planar fabrication = Reduces surface leakage effects Cooling methods = Helpful in reducing thermal generation</p> Signup and view all the answers

Match the electrical characteristics with their effects:

<p>Increasing electric field = Decreases fraction of collected charge Voltage integration circuit = Used to manage leakage currents Pulse height = Continues to rise until saturation is reached Multiplication effects = Similar to gas-filled chambers</p> Signup and view all the answers

Match the detector behavior with monitoring practices:

<p>Monitoring leakage current = Detects abnormal behavior or damage Reduction of leakage = Achieved by cooling methods Series resistor usage = Can lead to large leakage currents Thermal generation effects = Can be minimized but not eliminated</p> Signup and view all the answers

Match the terms related to semiconductor behavior with their correct descriptions:

<p>Drift velocity = Velocity due to an electric field Saturation velocity = Maximum drift velocity in high fields Intrinsic semiconductor = Completely pure semiconductor Diffusion = Spread in arrival position and collection time</p> Signup and view all the answers

Match the semiconductor types with their definitions:

<p>Electrons = Negatively charged charge carriers Holes = Positively charged charge carriers Intrinsic = Defined solely by thermal excitation Doped = Modified by impurities to alter properties</p> Signup and view all the answers

Match the equations to their relevant contexts in semiconductors:

<p>$vh = , , , \mu_h , E$ = Drift velocity of holes $\rho = \frac{1}{eni(\mu_e + \mu_h)}$ = Resistivity formula $I = Ani_e(\nu_e + \nu_h)$ = Net current in semiconductors $ni = pi$ = Intrinsic carrier density equality</p> Signup and view all the answers

Match the factors influencing conductivity in semiconductors:

<p>Carrier density = Number of charge carriers per unit volume Mobility = Speed of charge carriers in an electric field Surface area = Size of the conducting area Thickness = Distance charge carriers travel in the material</p> Signup and view all the answers

Match the semiconductor characteristics with their typical values:

<p>Saturation velocity = ~$10^7$ cm/s Carrier density in Si = $1.5 , \cdot , 10^{10}/cm^3$ Carrier density in Ge = $2.4 , \cdot , 10^{13}/cm^3$ Typical diffusion spread = &lt; 100 µm</p> Signup and view all the answers

Match the terms to the effects observed in semiconductors:

<p>Thermal excitation = Generates electron-hole pairs Recombination = Decreases charge carrier density Mobility = Response to the applied electric field Impurities = Modify electrical properties</p> Signup and view all the answers

Match the mathematical principles with their correct applications in semiconductors:

<p>$\mu = \frac{vh}{E}$ = Mobility definition $I = V/\rho$ = Ohm's law for semiconductors $\rho = R , A / L$ = Resistivity formula relationship $ni = p_i$ = Equality of electron and hole densities in intrinsic semiconductors</p> Signup and view all the answers

Match the semiconductor conditions with their behaviors:

<p>Low to moderate electric fields = Drift velocity proportional to electric field High electric fields = Drift velocity reaches saturation Doped semiconductors = Altered intrinsic properties Intrinsic state = Only thermal excitation causes charge carriers</p> Signup and view all the answers

Match the following semiconductor types with their characteristics:

<p>Intrinsic Semiconductors = Undoped and have equal electron and hole concentration N-type Semiconductors = Doped with pentavalent impurities providing extra electrons P-type Semiconductors = Doped with trivalent impurities creating holes Compound Semiconductors = Consist of two or more atomic elements</p> Signup and view all the answers

Match the following III-V compounds with their advantages and drawbacks:

<p>GaAs = Faster and more radiation resistant than Si GaP = Used in LED applications InP = High electron mobility GaSb = Less industrial experience than Si</p> Signup and view all the answers

Match the following II-VI compounds with their specific properties:

<p>CdTe = Efficient at detecting photons ZnSe = Used in blue light applications ZnS = Good for white LEDs CdS = Often used in solar cells</p> Signup and view all the answers

Match the following terms with their definitions related to semiconductors:

<p>Donor Impurities = Pentavalent atoms providing extra conduction electrons Fermi Level (EF) = Energy level indicating the probability of occupancy by electrons Breaking Voltage = The voltage at which a semiconductor begins to conduct Electron Mobility = The speed at which electrons move through a semiconductor material</p> Signup and view all the answers

Match the following factors with their effect on semiconductor properties:

<p>Bandgap = Determines the energy required for electron excitation Thermal Stability = Influences the operational temperature range Electron Mobility = Affects current flow efficiency Recombination = Decreases the number of free charge carriers</p> Signup and view all the answers

Match the following semiconductors with their doping types:

<p>Silicon (Si) = Can be intrinsic or extrinsic Gallium Arsenide (GaAs) = Best used in high-speed electronics Cadmium Telluride (CdTe) = Promising for photovoltaic applications Tin Dioxide (SnO2) = Commonly used as a transparent conducting oxide</p> Signup and view all the answers

Match the following semiconductor applications with their corresponding materials:

<p>LEDs = GaP and InP Solar Cells = CdTe and CdS High-Power Electronics = Si and III-V compounds Opto-electronics = ZnSe and InGaN</p> Signup and view all the answers

Match the following intrinsic semiconductor characteristics with their values:

<p>Resistance = $230,000 , ext{Ω cm}$ Carrier Concentration = $1.5 \times 10^{10} , ext{cm}^{-3}$ Electric Field Strength = $1350 + 480 , ext{cm}^2/Vs$ Temperature = Room Temperature (~300K)</p> Signup and view all the answers

Match the following types of semiconductor detector configurations with their descriptions:

<p>Diffused junction detectors = Treatment with n-type vapor to create a region near surface Ion implanted layers = Surface of semiconductor exposed to accelerator produced ions Surface barrier detectors = High density of electron traps at the surface of n-type crystal Partially depleted detectors = Variable active volume depending on reverse bias</p> Signup and view all the answers

Match the following terms related to semiconductor detectors with their meanings:

<p>Depletion region = Active volume of detector where charge carriers are collected Breakdown voltage = Maximum operating voltage before failure occurs Dead layer = Surface layer outside the depletion region that hinders detection Reverse bias = Voltage applied to enhance charge carrier collection</p> Signup and view all the answers

Match the following features of junction detectors with their roles:

<p>Width of depletion area = Represents the active detector volume Small detector capacitance = Needed for good energy resolution Max E-field = Occurs at the transition between p- and n-material Sensitivity to light = Causes high noise levels in thin entrance windows</p> Signup and view all the answers

Match the following processes with their characteristics:

<p>Diffusion = Creating n-type areas in p-type crystals Ion implantation = Controlling concentration profile through ion energy Etching = Procedure to prepare the surface of semiconductor detectors Evaporation = Method to deposit thin metal layers for electrical contact</p> Signup and view all the answers

Match the following types of radiation detection issues with their corresponding effects:

<p>Dead layer = Reducing efficiency of particle detection High noise levels = Resulting from light sensitivity Charge carrier collection = Efficiency dependent on depletion region Capacitance variation = Influenced by applied voltage in partially depleted detectors</p> Signup and view all the answers

Match the following semiconductor detector characteristics with their typical values:

<p>Max E-field = Typically $10^6 - 10^7$ V/m Depth of diffused layer = Ranges from 0.1 to 2.0 µm Thickness of gold layer = Approximately 20 nm Operating voltage = Must be below breakdown voltage</p> Signup and view all the answers

Match the following effects related to semiconductor p-n junctions with their outcomes:

<p>Reversed biased p-n junction = Attractive for radiation detection Creation of charge carriers = Occurs within the depletion region Active detector volume = Dependent on the reverse bias Variable capacitance = Resulting from applied voltage changes</p> Signup and view all the answers

Match the following terms in semiconductor detector technology with their relevance:

<p>Capacitance = Impacts charge collection efficiency Active volume = Determined by depletion region width Depletion region width = Varies with reverse bias voltage Sensitivity = Critical for detector performance and noise control</p> Signup and view all the answers

Match the features of Ge detectors with their descriptions:

<p>Cryostat = Inhibits thermal conductivity between crystal and surrounding air Dewar = Houses liquid nitrogen for cooling Interlock mechanism = Prevents high voltage application before low temperature is reached Preamplifier = Reduces electronic noise by being cooled</p> Signup and view all the answers

Match the configurations of Germanium detectors with their advantages:

<p>Closed-ended coaxial = Avoids surface leakage current Well configuration = Allows access to central hole for additional sources Rectifying contact on outer surface = Lower depletion voltage and higher electric field Thin end window = Minimizes gamma ray attenuation before entering the detector</p> Signup and view all the answers

Match the factors affecting energy resolution in Ge detectors:

<p>Statistical spread in charge carriers = Inherent variability in charge collection Charge collection efficiency = Influences the response of the detector Electronic noise = Contributes to overall energy measurement uncertainty Radiation energy = Affects how factors dominate energy resolution</p> Signup and view all the answers

Match the properties of charge collection in Ge detectors with their implications:

<p>Drift velocity = Increases linearly with electric field for low fields Saturation of drift velocity = Occurs at high electric fields Time constant in measuring electronics = Influences the leading edge of signal pulse Limiting factors for time resolution = Charge collection is inherently slow</p> Signup and view all the answers

Match the operational characteristics of Ge detectors with their required conditions:

<p>Ge(Li) detectors = Must maintain low temperature continuously HPGe detectors = Can be kept at room temperature between uses Room temperature operation = Impossible due to small bandgap Vacuum-tight housing = Prevents thermal conductivity issues</p> Signup and view all the answers

Match the aspects of germanium crystal characteristics with their implications:

<p>Limited size of crystal = Results in smaller wafer and volume Purity level of 99.99999999999% = Indicates high quality of germanium Cylindrical crystal = Allows for larger volumes of crystal Surface configuration = Impacts the electric field's radial perfection</p> Signup and view all the answers

Match the different types of Ge detectors with their cooling strategies:

<p>Ge(Li) detector = Requires continuous low temperature HPGe detector = Can be warmed up in between usages Traditional Ge detector = Requires cooling to 77 K Liquid nitrogen reservoir = Essential for efficient cooling of Ge detectors</p> Signup and view all the answers

Match the components involved in the design of Germanium detectors with their roles:

<p>Input stages of preamplifier = Cooled to reduce electronic noise Liquid nitrogen = Maintains low operational temperature Crystal configuration = Affects the planar front entrance window Electric field application = Influences overall detector performance</p> Signup and view all the answers

Match the issues faced by Ge detectors with their solutions:

<p>Surface leakage current = Addressed by closed-ended coaxial design Drifting of lithium = Avoided in HPGe detectors Thermal conductivity = Minimized with vacuum-tight cryostat Signal pulse timing = Managed by the equivalent circuit's time constant</p> Signup and view all the answers

Match the environmental conditions with their impacts on Ge detectors:

<p>High temperature = May cause catastrophic redistribution of lithium Low temperature = Necessary for stable operation of Ge(Li) Vacuum conditions = Help prevent thermal conductivity Gamma ray detection = Impacted by thin end window location</p> Signup and view all the answers

Flashcards

Band Gap

The difference in energy between the valence band and the conduction band, crucial for determining the behavior of a material as a conductor, insulator, or semiconductor.

Energy Bands

In a solid material, the energy levels available for electrons to occupy. These levels are grouped into bands, with the valence band representing electrons bound to atoms, and the conduction band representing free-moving electrons.

Conductor

A material where electrons can move freely, with a small or nonexistent energy gap between the valence and conduction bands. This allows for easy flow of electric current.

Insulator

A material where electrons are tightly bound and do not easily move, possessing a large energy gap between the valence and conduction bands. This prevents the flow of electric current.

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Semiconductor

A material with a moderate energy gap between the valence and conduction bands. This allows for controlled conductivity, making them useful for electronic devices.

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Valence band

The outermost electrons within an atom, which are involved in chemical bonding and electrical conductivity.

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Conduction band

The higher energy band where electrons can move freely, allowing for electrical conductivity. This is the band achieved when electrons gain enough external energy to jump the gap.

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Ionizing Radiation in Semiconductors

When incident ionizing radiation interacts with semiconductor material, it creates electron-hole pairs, contributing to the material's ability to detect radiation.

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Semiconductors as Radiation Detectors

The ability for a semiconductor material to register the presence of radiation and generate a corresponding signal, often by creating electron-hole pairs.

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Drift Velocity

The velocity of a charge carrier in a semiconductor due to the influence of an electric field. It is the average velocity of the charge carriers in the direction of the field.

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Mobility

A measure of how easily charge carriers move through a material. It is defined as the ratio of the drift velocity to the electric field strength.

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Saturation Velocity

The maximum drift velocity that a charge carrier can attain in a semiconductor. This occurs when the electric field is very strong.

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Intrinsic Semiconductor

A semiconductor material that is completely pure, with no impurities. The number of electrons in the conduction band is equal to the number of holes in the valence band.

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Intrinsic Carrier Density (ni)

The number of charge carriers (electrons and holes) per unit volume in an intrinsic semiconductor. It is determined by the material's properties and temperature.

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Conductivity

The ability of a material to conduct electricity. In a semiconductor, it is determined by the number of charge carriers and their mobility.

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Resistivity

The inverse of conductivity, it represents the resistance to the flow of electricity in a material.

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Thermal Velocity

The random motion of charge carriers in a semiconductor due to thermal energy. This motion is independent of the applied electric field.

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Resistivity (ρ)

The ability of a material to resist the flow of electric current. In semiconductors, resistivity is measured in ohm-centimeters (Ω.cm).

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n-type Semiconductor

A semiconductor material where the majority of charge carriers are electrons, usually due to the presence of donor impurities.

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p-type Semiconductor

A semiconductor material where the majority of charge carriers are holes, usually due to the presence of acceptor impurities.

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Donor Impurities

Impurities that donate extra electrons to the conduction band in a semiconductor material. These atoms have more valence electrons than the semiconductor atoms they replace.

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Acceptor Impurities

Impurities that accept electrons from the valence band, creating holes in a semiconductor material. These atoms have fewer valence electrons than the semiconductor atoms they replace.

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Fermi Level (EF)

The energy level within the forbidden gap of a semiconductor that represents the average energy of electrons. It shifts closer to the conduction band in n-type semiconductors and closer to the valence band in p-type semiconductors.

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Compound Semiconductors

Semiconductors made from two or more different elements. Examples include GaAs (Gallium Arsenide) and SiGe (Silicon Germanium).

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III-V Semiconductors

A semiconductor composed of two or more elements, specifically those from Group III and Group V of the periodic table. Examples include GaAs and InP.

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Semiconductor Diode Detectors

A type of radiation detector that utilizes the properties of semiconductors to detect radiation. These detectors are known for their high sensitivity and fast response times.

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Doping

The process of selectively introducing impurities (dopants) into a semiconductor material to modify its electrical conductivity and create a junction with specific electrical properties.

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PN Junction

A region within a semiconductor where the material is doped with both positive and negative impurities, resulting in a boundary layer with a built-in electric field.

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Reverse Bias

The process of applying an external voltage to a PN junction to control the flow of charge carriers across the junction and create a depletion region free of charge carriers.

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Leakage Current

The microscopic current that flows through a reverse-biased PN junction due to the small, thermally generated electron-hole pairs.

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Charge Collection Saturation

The phenomenon where the charge collected from ionizing radiation increases with higher applied bias voltage until a saturation point is reached, where further increasing the bias voltage no longer affects the amount of collected charge.

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Pulse Rise Time

The time it takes for the signal from a radiation interaction to rise to its peak value in a semiconductor detector. It is typically very fast, usually in the range of 10 nanoseconds or less.

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Passivated Planar Detector Fabrication

The process of creating complex electrode geometries on silicon detectors using ion implantation and photolithography, allowing for more sophisticated detector designs.

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Maximum Electric Field Strength (Emax) in a Detector

The maximum electric field strength within a semiconductor detector, usually occurring at the transition between the p-type and n-type materials. It is typically in the range of 106 to 107 V/m.

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Dead Layer in Semiconductor Detectors

A thin layer at the surface of a semiconductor detector that acts as an entrance window for incident radiation. It can be a disadvantage for particle detection because it may absorb some of the radiation before it reaches the active region.

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Diffused Junction Semiconductor Detector

A type of semiconductor detector where a thin, heavily doped layer is created on the surface of the semiconductor material. This layer creates a depletion region that extends primarily into the bulk material, forming the active detection area.

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Ion Implantation in Semiconductor Detectors

A method of creating thin, heavily doped layers on the surface of a semiconductor material by bombarding the surface with ions, like phosphorus or boron. The ions create a controlled concentration profile, defining the depth and properties of the doped layer.

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Surface Barrier Detector

A type of semiconductor detector where a thin layer of gold provides a Schottky contact to an n-type semiconductor material. The junction between the metal and the semiconductor creates a depletion region, functioning as the sensitive detection area.

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Depletion Region in Semiconductor Detectors

The area within a semiconductor detector where an electric field exists, collecting charge carriers generated by incident radiation. The size of this area directly affects the detector's sensitivity and resolution.

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Capacitance of a Partially Depleted Semiconductor Detector

The capacitance of a semiconductor detector that varies with the applied voltage. This variation is a characteristic feature of partially depleted detectors, where the size of the depletion region and hence the detector's active volume, changes.

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Energy Resolution of Semiconductor Detectors

A key parameter of semiconductor detectors that determines their capability to separate closely spaced energy peaks in radiation spectra. A higher energy resolution allows for better differentiation between different types of radiation.

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Germanium Crystal Growth

The process of growing large, high-purity germanium crystals for use in detectors.

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Rectifying Contact Configuration

The configuration of a germanium detector where the electrical contact is on the outer surface, leading to a higher electric field in the detector's outer regions where most of the detector volume is.

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Detector Cooling

The cooling of germanium detectors to 77K (liquid nitrogen temperature) to reduce thermal noise and enable operation.

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HPGe Detector

A type of germanium detector where lithium is drifted into the detector material during fabrication. This results in a higher purity and improved resolution.

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Detector Cryostat

A sealed container that houses the germanium detector and provides a vacuum environment to minimize thermal conductivity and increase efficiency.

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Energy Resolution

The ability of a detector to distinguish between different energy levels of radiation.

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Statistical Spread in Charge Carriers

The inherent spread in the number of charge carriers generated by radiation interaction, contributing to the overall energy resolution.

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Charge Collection Time

The time it takes for a charge carrier to travel through a certain distance in a semiconductor.

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Charge Collection as a Time Resolution Limitation

The inherent slowness in the charge collection process in germanium detectors, leading to a limitation in their ultimate time resolution.

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Study Notes

Semiconductor Diode Detectors

  • Semiconductor properties are essential to radiation detection
  • Ionizing radiation in semiconductors creates electron-hole pairs
  • Semiconductor detector configurations vary in design
  • Operational characteristics of detectors are significant
  • Applications of silicon diode detectors include high-energy physics
  • Germanium gamma-ray detectors are used for nuclear physics
  • Lithium-drifted silicon detectors are useful for applications requiring high energy resolution

Solid Detection Medium

  • Solid detection medium density is ~1000x higher than gas
  • Smaller detector dimensions are possible
  • Scintillation counters (solid) require ~100 eV for one carrier
  • Statistical fluctuations limit energy resolution
  • Semiconductor diode detectors provide high charge carrier numbers for incident radiation events
  • High energy resolution in routine use

Features of Semiconductor Diode Detectors

  • Information carriers are electron-hole pairs (similar to electron-ion pairs)
  • Superior energy resolution
  • Compact size
  • Relatively fast timing characteristics
  • Effective thickness can be varied
  • Limitations include small size, relative high susceptibility to radiation-induced damage, and cost

Use of Solid State Detectors

  • Used in Nuclear Physics for energy measurement of charged particles
  • Used in Nuclear Physics for gamma spectroscopic precission measurement of photon energies
  • Used in Particle Physics for tracking and vertexing measurements
  • Used in Particle Physics for beam condition monitoring
  • Used in Satellite Experiments for tracking and particle identification
  • Used in Security, medicine, and biology

Semiconductor Properties-Band Structure

  • Isolated atoms have discrete electron energy levels
  • In solids, discrete levels merge to form energy bands (periodic lattice of crystal material establishes allowed bands)
  • Valence band: outer shell electrons bound to lattice sites
  • Conduction band: electrons free to move through the crystal

Properties of Semiconductor Materials

  • Size of bandgap determines material type (metals, insulators, semiconductors)
  • Metals have overlapping valence and conduction bands
  • Insulators have large bandgaps (>5 eV)
  • Semiconductors have bandgaps (~eV)
  • Without thermal excitation, valence band is full and conduction band empty
  • Electrons can easily migrate in metals due to partially filled bands

Elemental Semiconductors

  • Silicon is the standard material for vertex and tracking detectors in high-energy physics
  • Germanium is used in nuclear physics due to its small bandgap (~0.66 eV), requiring cooling
  • Diamond has a large bandgap (~5.5 eV) and is very radiation-hard

Charge Carriers

  • At nonzero temperatures, valence electrons gain thermal energy, leave their covalent bonding sites, and drift (creating electrons in conduction band and holes in valence band)
  • The probability of electron-hole pair generation depends on temperature and bandgap energy
  • In the absence of electrical fields, electron-hole pairs recombine, establishing an equilibrium proportional to the rate of formation with strong temperature dependence.
  • Distribution of charges (for single point of origin): σ=√2Dt (D = μD, diffusion constant; kT/e=0.0253V at 20°C)

Migration of Charge Carriers in Electric Field

  • When an electric field is applied to a semiconductor, electrons and holes experience a net migration parallel to the electric field.
  • At moderate fields, drift velocity is proportional to applied field (mobility)
  • In semiconductors, electron and hole mobilities are roughly similar to those of electrons and ions in gases.
  • At higher fields, drift velocity reaches saturation velocity.
  • Charge collection times in typical semiconductor detectors are <10 ns.
  • Diffusion causes spread in arrival position (<100 μm) and collection time (<1 ns)

Intrinsic Semiconductors

  • Intrinsic semiconductors have completely pure semiconductors, with electron-hole pairs produced only by thermal excitation
  • Electrical properties are determined if very well purified impurities are present

Impurity (Extrinsic) Semiconductors

  • Extrinsic semiconductors have properties arising from small levels of impurities
  • Impurities (e.g., donors or acceptors) create energy levels near the band edges, making electrons easily excited into the conduction band (n-type), or holes in the valence band (p-type)

Conductivity

  • Conductivity (resistivity) depends on charge carrier densities and their mobilities.
  • The formula is given as I = AV/pt; p = AV/It(with A = area, t = thickness, and V = voltage)
  • Resistivity is p ≈ (1/en₁)(μe+μh).

Compound Semiconductor

  • Compound semiconductors (e.g., GaAs, CdTe) are used; they can have suitable properties for radiation detection
  • Differing properties allow a wide range of applications

n-type Semiconductors

  • Pentavalent (Group V) impurities substitute for silicon atoms, creating excess electrons that act as charge carriers
  • Extra electrons reside in the band gap but are loosely bound and can move into the conduction bands with little energy input
  • Fermi energy level moves up slightly

p-Type Semiconductors

  • Trivalent (Group III) impurities substitute for silicon atoms, creating "holes" that act as positive charge carriers
  • The holes serve as positive charge carriers when electrons fill the vacancies (acceptors) resulting in fewer electrons, and hence creating holes
  • Fermi energy level moves down slightly

Compensated and Heavily Doped Materials

  • Compensated materials contain equal numbers of donor and acceptor impurities
  • Heavily doped materials have high impurity concentrations

Trapping and Recombination

  • Electrons and holes in a semiconductor tend to migrate or recombine
  • Deep impurities (Au, Zn, Cd) can introduce energy levels in the band gap and act as trapping centers, leading to carrier delay before collection
  • Recombination centers capture both majority and minority carriers, causing them to annihilate, leading to a time delay.

Ionizing Radiation in Semiconductors

  • Ionization energy, often 3 eV for silicon, (energy of incident radiation has little effect in number of electron-hole pairs formed)
  • Slight dependence on incident radiation (proton, alpha, heavy ions, fissions)
  • Doping atoms in normal concentrations have negligible effect on interaction probabilities.
  • Statistical fluctuations lead to variations in the number of carriers per pulse.

The Fano Factor

  • Fluctuations in the number of charge carriers affect energy resolution.
  • For semiconductors, observed fluctuations are smaller than predicted by a Poisson process
  • Good energy resolution is obtained with small values of the Fano factor

Pulse Formation

  • Equal numbers of electrons and holes are generated.
  • Charge carriers drift in opposite directions due to an electric field
  • Charge collection times are close to each other, with hole mobility generally within a factor of 2–3 of electron mobility

Leakage Current

  • Leakage current is due to both bulk volume and detector surface
  • Small minority carriers across a junction roughly proportional to junction area.
  • Thermal electron-hole generation depends on material & temperature.
  • Surface leakage effects depends on contamination, edges.
  • Bias voltage is frequently provided through high-value resistors for signal integration.
  • Monitoring of leakage current helps detect detector problems.

Changes with Detector Bias Voltage

  • For low bias voltage and electric field, pulse height increases and is due to incomplete charge collection (trapping and recombination)
  • Increasing electric field decreases charge loss and pulse height becomes constant once saturation region is reached.
  • High field triggers electron and hole multiplication
  • Multiplication effects are similar to gas-filled chambers.

Pulse Rise Time

  • Semiconductor diode detectors are generally fast
  • Charge transit time (time of migration) depends on the depletion region.
  • Fully depleted detectors decrease transit time with increasing bias voltage
  • Partially depleted detectors have more complex behaviors due to variable electric field and distance.
  • Plasma time is significant for heavy charged particles producing plasma clouds.

Entrance Window/Dead Layer

  • Particle energy loss before reaching active volume can be significant
  • Dead layer thickness can be determined by varying incident angle of particles
  • Energy loss can depend on angle of incidence due to recombination w.r.t. electric field

Channeling

  • Particles travelling parallel to crystalline planes experience a lower rate of energy loss
  • To minimize channeling, silicon wafers are cut perpendicular to the <111> crystal orientation to the wafer surface

Energy Calibration

  • Semiconductor diode detectors have high sensitivity to electrons and light ions
  • Calibration sources are routinely used, such as 241 Am, with standard energies.

Pulse Height Defect

  • Pulse height defect observed for heavy ions; less than that for light ions of the same energy
  • Energy loss of ions in entrance window and dead layers is significant
  • Other energy loss mechanisms (e.g. nuclear collisions) contribute
  • High rate of recombination in dense plasma along ion track could be lowered by higher bias voltage
  • Radiation damage increases pulse defect due to enhanced trapping and recombination

Applications of Silicon Diode Detectors

  • Used in general charged particle spectroscopy for heavy particle detection
  • Detectors offer advantages such as stability, good energy resolution, excellent timing characteristics, and thin entrance windows.
  • Commercially available devices range up to ~20 cm²
  • Depletion depth can be up to 5 mm

Alpha Particle Spectroscopy

  • Silicon diodes at room temperature are good for a's and light ions
  • Pre-amplifier noise can be a limiting factor for resolutions
  • Calculations can be made for FWHM resolution (2.35√FEɛ

Energy Loss Measurements (Particle Identification)

  • Thin detectors are useful for energy loss identification, as compared to full energy.
  • Semiconductor detectors are useful in coincidence with other detectors (telescopes)
  • Bethe's formula describes energy loss for non-relativistic particles due to factors in mZ2.

Germanium Gamma-Ray Detectors

  • Using Si or Ge, depletion depth is limited to a few mm or less for normal semiconductor purities
  • Reducing N levels (<10^10 atoms/cm³), can increase detection depth up to ~ 1cm

Germanium Detector Configurations

  • High-purity Ge (HPGe) fabrication employs zone refining to achieve the high purity
  • Planar configuration: p-type HPGe + n⁺ contact
  • Coaxial configuration avoids surface leakage current, for a better configuration.

Germanium Detector Operational Characteristics

  • Ge(Li) detectors need to be cooled to low temperatures to prevent catastrophic Li distributions.
  • Detector cryostats and dewars provide insulation and cooling for these detectors
  • Thermal conductivity between crystal and air is minimized in vacuum-tight cryostats.
  • Thin end windows minimize gamma-ray attenuation.

Germanium Detector Energy Resolution

  • Ge detectors have superior energy resolution due to their inherent statistical spread, charge carrier variations and collection efficiency variations.
  • Detector size and radiation energy affect the dominant factors.

Pulse Shape and Timing Properties

  • Charge collection is inherently slow, as 100 ns required for 1 cm travel
  • Pulse rise times from Ge detectors can vary from event to event

Gamma-Ray Spectroscopy

  • Lower atomic number Z of Ge, smaller active volume compared to NaI lead to differences in pulse height spectrum
  • Full-energy peak is more likely to consist of multiple interactions.

Fully Depleted Detectors

  • Fully depletion with high reverse bias extends depletion region over entire wafer thickness
  • Suitable for high purity detectors
  • Used as transmission detectors for energy loss measurement
  • Active volume and capacitance are independent from applied voltage

Passivated Planar Detectors

  • Newest method of fabricating silicon junction detectors: combination of ion implantation and photolithography
  • Complex electrode geometries are possible.

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