are the heart of terahertz imaging systems. They generate electromagnetic waves in the 0.1 to 10 THz range, bridging the gap between microwaves and infrared light. Understanding these sources is crucial for building effective imaging systems.
Various types of terahertz sources exist, each with unique characteristics. From pulsed to continuous wave, broadband to narrowband, and high-power to low-power, the choice of source depends on the specific imaging application and desired performance.
Types of terahertz sources
Terahertz sources generate electromagnetic radiation in the terahertz frequency range (0.1 to 10 THz) which is essential for terahertz imaging systems
Different types of terahertz sources exist, each with their own unique characteristics and advantages for specific applications in terahertz imaging
Understanding the various types of terahertz sources is crucial for selecting the appropriate source for a given terahertz imaging system and optimizing its performance
Pulsed vs continuous wave
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generate short bursts of terahertz radiation (picosecond to nanosecond duration) which are useful for and imaging
Continuous wave (CW) terahertz sources emit a constant stream of terahertz radiation and are suitable for frequency-domain spectroscopy and real-time imaging
Pulsed sources offer high peak power and broad bandwidth, while CW sources provide higher average power and narrower linewidth
Broadband vs narrowband
emit radiation over a wide range of frequencies (several THz) which enables spectroscopic analysis and depth resolution in imaging
have a limited frequency range (typically < 1 THz) but offer higher spectral brightness and coherence
Broadband sources are used for material characterization and tomography, while narrowband sources are preferred for high-resolution imaging and sensing
High-power vs low-power
can generate output powers in the milliwatt to watt range, enabling long-range imaging and deep tissue penetration
(microwatt to milliwatt range) are more compact, energy-efficient, and suitable for short-range imaging and spectroscopy
The choice between high-power and low-power sources depends on the specific application requirements such as imaging distance, sample absorption, and signal-to-noise ratio
Optically-pumped terahertz lasers
use optical excitation (usually from another laser) to generate terahertz radiation through various physical mechanisms
These lasers offer high , narrow linewidth, and tunability, making them attractive for terahertz imaging applications
Different types of optically-pumped terahertz lasers exist, each with their own pumping scheme and active medium
CO2 pumped gas lasers
use a high-power CO2 laser to excite a gas medium (such as methanol or ammonia) and generate terahertz radiation
The pumping occurs through a rotational-vibrational transition in the gas molecules, resulting in population inversion and lasing
These lasers can achieve high output powers (>100 mW) and narrow linewidths (<1 MHz) but are bulky and require cryogenic cooling
Quantum cascade lasers
(QCLs) are semiconductor devices that emit terahertz radiation through intersubband transitions in a periodic heterostructure
QCLs are electrically pumped and can be designed to operate at specific frequencies by engineering the layer thicknesses and compositions
They offer compact size, high power (>1 mW), and room-temperature operation but have limited tuning range and require complex fabrication
P-type germanium lasers
use optical excitation of holes in heavily doped p-type germanium to generate terahertz radiation
The pumping is achieved using a pulsed near-infrared laser, and the emission occurs through direct interband transitions
These lasers can provide high peak powers (>1 W) and broad tuning range (1-4 THz) but require strong magnetic fields and cryogenic cooling
Terahertz semiconductor sources
are compact, solid-state devices that generate terahertz radiation through various optoelectronic mechanisms
These sources offer the advantage of room-temperature operation, low power consumption, and potential for integration with other electronic components
Different types of terahertz semiconductor sources have been developed, each with their own operating principle and performance characteristics
Photoconductive antennas
(PCAs) consist of a semiconductor substrate (GaAs or InGaAs) with metallic electrodes forming an antenna structure
A femtosecond laser pulse excites charge carriers in the semiconductor, which are accelerated by an applied electric field and radiate terahertz waves
PCAs can generate broadband terahertz pulses (0.1-5 THz) with high peak power (>1 mW) but have limited average power and require precise laser alignment
Photomixers
are based on the nonlinear mixing of two continuous-wave laser beams in a semiconductor (LT-GaAs or ErAs:GaAs) to generate a terahertz beat frequency
The mixing occurs in a small active area between two metal electrodes, which also serve as an antenna to radiate the terahertz waves
Photomixers can provide narrow-linewidth (<1 MHz), frequency-tunable terahertz radiation but have limited output power (<1 μW) and bandwidth
Uni-traveling carrier photodiodes
(UTC-PDs) are based on a modified p-i-n photodiode structure with a special absorber layer that favors electron transport
UTC-PDs can generate terahertz radiation through photomixing or pulsed operation, offering high output power (>1 mW), wide bandwidth (>1 THz), and high efficiency
They require a high-frequency antenna and matching circuit for efficient terahertz emission and have limited frequency tunability
Nonlinear optical sources
generate terahertz radiation through the interaction of intense laser beams with nonlinear optical crystals
These sources exploit the second-order or third-order nonlinear susceptibility of the crystal to achieve frequency conversion or mixing
Nonlinear optical sources offer the advantage of room-temperature operation, high peak power, and broad bandwidth but require powerful laser pumps and phase-matching conditions
Optical rectification
is a second-order nonlinear process where a femtosecond laser pulse generates a DC polarization in a nonlinear crystal (ZnTe, GaP, or LiNbO3)
The time-varying polarization acts as a source of broadband terahertz radiation, which is emitted in a direction determined by the phase-matching condition
Optical rectification can generate terahertz pulses with high peak power (>1 kW) and ultra-broad bandwidth (>10 THz) but has limited conversion efficiency (<0.1%)
Difference frequency generation
(DFG) is a second-order nonlinear process where two laser beams at different frequencies mix in a nonlinear crystal to generate a terahertz wave at their difference frequency
DFG can be achieved using either pulsed or continuous-wave lasers and provides narrow-linewidth, frequency-tunable terahertz radiation
The conversion efficiency of DFG is typically low (<0.01%) but can be enhanced using waveguide geometries or resonant cavities
Optical parametric oscillators
(OPOs) are based on a second-order nonlinear process called parametric amplification, where a pump laser beam amplifies a signal beam in a nonlinear crystal and generates an idler beam
By placing the nonlinear crystal in a resonant cavity and selecting the appropriate signal and idler frequencies, a terahertz OPO can be realized
Terahertz OPOs can provide high output power (>10 mW), narrow linewidth (<1 MHz), and wide tuning range (1-5 THz) but require a high-power pump laser and precise cavity alignment
Vacuum electronic devices
are a class of terahertz sources that rely on the interaction between electrons and electromagnetic fields in a vacuum environment
These devices can generate high-power, coherent terahertz radiation by exploiting the bunching and acceleration of electron beams
Different types of vacuum electronic devices have been developed for terahertz generation, each with their own operating principle and performance characteristics
Gyrotrons
are based on the cyclotron resonance maser instability, where a high-energy electron beam interacts with a strong magnetic field in a resonant cavity
The electrons gyrate around the magnetic field lines and emit coherent radiation at the cyclotron frequency or its harmonics, which can be in the terahertz range
Gyrotrons can generate high-power (>1 kW), narrow-linewidth (<1 MHz) terahertz radiation but require superconducting magnets and high-vacuum conditions
Backward wave oscillators
(BWOs) are based on the interaction between an electron beam and a slow-wave structure (helix or corrugated waveguide) in a vacuum tube
The electrons transfer their kinetic energy to the electromagnetic wave, which propagates in the opposite direction to the electron beam, leading to oscillation and amplification
BWOs can provide frequency-tunable, moderately high-power (>10 mW) terahertz radiation but have limited bandwidth and require high-voltage power supplies
Free electron lasers
(FELs) are based on the interaction between a relativistic electron beam and a periodic magnetic field (undulator) in a vacuum chamber
The electrons oscillate in the undulator and emit synchrotron radiation, which can be amplified by synchronizing the electron bunches with the radiation field
FELs can generate high-power (>1 kW), widely tunable terahertz radiation with excellent coherence properties but are large, complex, and expensive facilities
Comparison of terahertz sources
The choice of a terahertz source for a specific imaging system depends on various factors such as the required frequency range, output power, , and system complexity
Each type of terahertz source has its own strengths and limitations, and a comparative analysis can help in selecting the most suitable source for a given application
The following criteria can be used to compare and evaluate different terahertz sources:
Frequency range and tunability
The frequency range of a terahertz source determines the spectral coverage and resolution of the imaging system
Some sources (photoconductive antennas, optical rectification) provide broadband emission, while others (quantum cascade lasers, photomixers) offer narrow-linewidth, tunable radiation
The required frequency range depends on the spectroscopic signatures and penetration depth of the target materials
Output power and efficiency
The output power of a terahertz source affects the signal-to-noise ratio, imaging speed, and penetration depth of the system
High-power sources (gyrotrons, free electron lasers) are suitable for long-range imaging and deep tissue penetration, while low-power sources (photomixers, UTC-PDs) are adequate for short-range, surface-level imaging
The power efficiency of the source (ratio of terahertz output power to input power) is important for portable, battery-operated imaging systems
Spectral purity and coherence
The spectral purity (linewidth, phase noise) and coherence (temporal, spatial) of a terahertz source determine the spectral resolution and imaging quality of the system
Narrow-linewidth, highly coherent sources (quantum cascade lasers, photomixers) are preferred for high-resolution spectroscopy and interferometric imaging, while broadband, incoherent sources (photoconductive antennas, optical rectification) are suitable for time-domain spectroscopy and tomography
The coherence properties also affect the ability to perform phase-sensitive measurements and coherent signal processing
Size, cost, and complexity
The size, cost, and complexity of a terahertz source are practical considerations for the development and deployment of imaging systems
Compact, low-cost sources (photoconductive antennas, photomixers) are attractive for portable, field-deployable systems, while larger, expensive sources (free electron lasers, gyrotrons) are more suitable for laboratory-based, high-performance systems
The complexity of the source (number of components, alignment requirements, cooling needs) affects the ease of use, reliability, and maintainability of the imaging system
Applications of terahertz sources
Terahertz sources find diverse applications in various fields, ranging from fundamental science to industrial quality control and biomedical diagnostics
The unique properties of terahertz radiation (penetration depth, spectral fingerprints, non-ionizing nature) make it suitable for non-destructive testing, chemical analysis, and biological imaging
The following are some of the key applications of terahertz sources in imaging and sensing:
Terahertz spectroscopy and imaging
Terahertz spectroscopy involves measuring the absorption or transmission spectrum of a sample in the terahertz frequency range, which provides information about its chemical composition, molecular structure, and dynamics
Terahertz imaging uses the spatial variation of the terahertz spectral response to create 2D or 3D maps of the sample, revealing its internal structure, defects, or inhomogeneities
Applications include material characterization (polymers, ceramics, semiconductors), quality control (pharmaceutical tablets, food products), and art conservation (paintings, manuscripts)
Wireless communications and networking
Terahertz wireless communications exploit the large bandwidth and high directivity of terahertz waves to achieve high data rates (>100 Gbps) and secure, short-range links
Terahertz sources can be used as transmitters or local oscillators in wireless communication systems, enabling applications such as high-definition video streaming, wireless data centers, and chip-to-chip communication
Challenges include the high atmospheric absorption, limited output power, and the need for line-of-sight propagation
Non-destructive testing and evaluation
Terahertz non-destructive testing (NDT) uses the penetration and reflection properties of terahertz waves to detect defects, voids, or delaminations in materials without causing damage
Terahertz NDT can be applied to a wide range of materials, including polymers, composites, ceramics, and semiconductors, and is particularly useful for inspecting layered or coated structures
Applications include quality control in manufacturing (automotive, aerospace), structural health monitoring (buildings, bridges), and packaging inspection (food, pharmaceuticals)
Medical diagnostics and therapy
Terahertz medical imaging exploits the sensitivity of terahertz radiation to water content and tissue structure to differentiate between healthy and diseased tissues
Terahertz sources can be used for non-invasive, label-free imaging of skin cancer, breast tumors, and dental caries, as well as for monitoring wound healing and burn assessment
Terahertz radiation has also shown potential for therapeutic applications, such as targeted drug delivery, photodynamic therapy, and non-thermal tissue ablation
Challenges include the limited penetration depth in biological tissues, the need for compact, portable imaging systems, and the potential health effects of long-term exposure
Key Terms to Review (37)
Backward Wave Oscillators: Backward wave oscillators (BWOs) are specialized electronic devices that generate microwaves and terahertz radiation by exploiting the backward wave phenomenon, where the wave propagates in the opposite direction to the electron beam. These oscillators play a crucial role in producing high-frequency signals needed for various applications, including imaging, spectroscopy, and material characterization. Their unique mechanism allows for the generation of tunable frequencies, making them valuable sources in terahertz systems.
Biomedical imaging: Biomedical imaging is the process of visualizing the internal structures and functions of biological systems, primarily for diagnostic, therapeutic, or research purposes. This field plays a crucial role in understanding diseases, guiding medical procedures, and developing new treatments through various imaging techniques.
Broadband terahertz sources: Broadband terahertz sources are devices capable of generating terahertz radiation over a wide range of frequencies, typically spanning from 0.1 to several THz. These sources are essential for various applications in imaging, spectroscopy, and communications, as they enable the probing of materials and systems with high temporal and spatial resolution. The versatility and efficiency of broadband terahertz sources make them crucial in advancing terahertz technology for both scientific research and practical applications.
CO2 Pumped Gas Lasers: CO2 pumped gas lasers are a type of laser that utilizes carbon dioxide as the primary lasing medium, with a specific configuration designed for efficient pumping and laser generation. These lasers operate by exciting the CO2 molecules using electrical energy, allowing them to emit coherent light in the infrared range, which is particularly useful for various applications, including terahertz imaging and material processing.
Coherence Length: Coherence length is the distance over which a coherent wave, such as a light wave, maintains a specified degree of coherence. This concept is crucial in understanding the behavior of terahertz sources, as it determines how well the waves can interfere with each other and influence imaging systems. The coherence length can significantly impact the resolution and quality of imaging, as it influences how the terahertz radiation interacts with materials and produces detailed images.
Continuous Wave Terahertz Sources: Continuous wave terahertz sources are devices that generate electromagnetic radiation in the terahertz frequency range using a continuous output rather than pulsed signals. These sources provide a stable and consistent beam of terahertz radiation, which is essential for various applications such as spectroscopy, imaging, and communication. Continuous wave terahertz sources enable real-time analysis and measurement, making them invaluable in fields like materials science and biomedical research.
Continuous-wave vs Pulsed Sources: Continuous-wave (CW) and pulsed sources are two types of signal generation used in terahertz imaging systems. CW sources emit a constant wave of electromagnetic radiation, providing a steady signal that is useful for certain applications, while pulsed sources generate short bursts of energy, allowing for time-domain measurements and improved resolution. Understanding the differences between these two types of sources is essential for effectively selecting the appropriate method for various terahertz imaging tasks.
David G. Stinson: David G. Stinson is a notable figure in the field of terahertz technology, particularly recognized for his contributions to terahertz sources and their applications. His work has helped advance the understanding of how terahertz waves can be generated and utilized in various fields, including imaging and spectroscopy. Stinson's research has had a significant impact on improving the efficiency and effectiveness of terahertz systems, contributing to both theoretical advancements and practical implementations.
Difference Frequency Generation: Difference frequency generation is a nonlinear optical process where two waves at different frequencies interact in a medium to produce a new wave at a frequency equal to the difference between the original frequencies. This technique is crucial in producing terahertz radiation, which has applications in various imaging and spectroscopic techniques, making it essential for understanding how terahertz optics, sources, and Raman spectroscopy work.
Fourier Transform Spectroscopy: Fourier Transform Spectroscopy (FTS) is a technique that analyzes the spectral content of signals by transforming data from the time domain to the frequency domain using the Fourier transform. This method allows for the collection of spectral information over a wide range of frequencies, making it especially useful in terahertz applications where high-resolution spectral analysis is crucial.
Free Electron Lasers: Free electron lasers (FELs) are advanced light sources that utilize relativistic electrons moving through a magnetic structure to produce coherent electromagnetic radiation across a wide range of wavelengths, including terahertz frequencies. These lasers are particularly significant for terahertz imaging systems, as they provide tunable, high-power radiation that can be adjusted to target specific applications, such as spectroscopy or material characterization.
Frequency Multiplication: Frequency multiplication refers to the process of generating a signal at a frequency that is an integer multiple of a lower frequency signal. This technique is crucial in various applications, especially in terahertz imaging systems where high-frequency signals are necessary for effective imaging. By utilizing frequency multiplication, devices can produce the terahertz waves required for detailed imaging, enhancing the capabilities of terahertz sources and their associated detectors.
Gyrotrons: Gyrotrons are high-frequency vacuum tubes that generate microwave radiation through the interaction of a beam of electrons with a magnetic field. These devices are essential for producing terahertz radiation, enabling a range of applications in imaging, spectroscopy, and communications. The ability of gyrotrons to operate at frequencies in the terahertz range makes them vital sources for advanced imaging systems, particularly in fields like materials science and medical diagnostics.
High-power terahertz sources: High-power terahertz sources are devices or systems that generate terahertz radiation with significant output power, typically in the range of milliwatts to watts. These sources are crucial in advancing terahertz imaging and spectroscopy applications, enabling the investigation of materials and biological samples with greater sensitivity and resolution.
Low-power terahertz sources: Low-power terahertz sources are devices that generate terahertz radiation with relatively low output power, typically in the range of microwatts to milliwatts. These sources are crucial for various applications such as imaging, spectroscopy, and communications because they enable non-destructive testing and analysis without damaging the sample being studied. Their significance lies in providing a balance between power efficiency and the ability to perform high-resolution measurements in a range of scientific and industrial fields.
Narrowband Terahertz Sources: Narrowband terahertz sources are devices that generate terahertz radiation within a limited frequency range, typically exhibiting high spectral purity and stability. These sources are crucial in various applications, such as spectroscopy, imaging, and communications, as they enable precise measurements and analyses of materials and biological samples. The ability to focus on specific frequency bands allows for enhanced resolution and sensitivity in terahertz imaging systems.
Nonlinear optical processes: Nonlinear optical processes refer to interactions between light and matter that occur when the intensity of the light is so high that it alters the material's response. This can lead to phenomena such as frequency mixing, second harmonic generation, and self-focusing. These processes are essential for generating terahertz waves, which are critical in imaging and spectroscopy applications, as they enhance the capabilities of terahertz sources.
Nonlinear optical sources: Nonlinear optical sources are devices or materials that exploit nonlinear optical effects to generate or manipulate light, particularly in the terahertz (THz) frequency range. These sources play a crucial role in various applications, allowing the conversion of laser light into THz radiation through processes such as difference frequency generation, optical rectification, or four-wave mixing. Their ability to produce high-intensity THz waves makes them essential for advanced imaging techniques and spectroscopic methods.
Optical Parametric Oscillators: Optical parametric oscillators (OPOs) are devices that convert a single input photon into two lower-energy photons through a non-linear optical process, typically using a non-linear crystal. They are crucial in generating tunable wavelengths of light, making them valuable for various applications, particularly in spectroscopy and imaging systems. OPOs can provide a wide range of frequencies, including terahertz waves, by adjusting the pump wavelength and exploiting the unique properties of the non-linear medium.
Optical Rectification: Optical rectification is a nonlinear optical process where incident light is converted into a direct current (DC) electric field, generating terahertz (THz) radiation. This process is crucial for producing THz waves from laser sources and plays a vital role in various applications, including spectroscopy and imaging techniques.
Optically-pumped terahertz lasers: Optically-pumped terahertz lasers are specialized devices that generate terahertz radiation through the excitation of a gain medium using optical pumping techniques. These lasers utilize a high-energy light source, like a laser, to stimulate the gain medium, which then emits coherent terahertz waves. The unique operating principle allows for the generation of continuous-wave or pulsed terahertz radiation, making them valuable tools in various applications such as imaging and spectroscopy.
Output Power: Output power refers to the amount of energy emitted by a terahertz source, typically measured in watts or milliwatts. This parameter is crucial as it influences the effectiveness of imaging systems and the overall quality of the terahertz signals produced, impacting applications such as material characterization and security scanning.
P-type germanium lasers: P-type germanium lasers are semiconductor lasers that use p-type doping in germanium to create a population inversion necessary for laser action. This type of laser operates in the infrared range and is significant for its potential applications in terahertz imaging and communication technologies. They are crucial in developing compact and efficient sources of terahertz radiation, which is essential for various imaging systems.
Passive vs Active Terahertz Sources: Passive terahertz sources are devices that do not require an external power supply to generate terahertz radiation; instead, they rely on natural processes or phenomena. Active terahertz sources, on the other hand, use external energy to produce terahertz waves, often resulting in higher output power and tunability. Understanding these two categories is crucial as they have different applications, operational mechanisms, and performance characteristics in terahertz imaging systems.
Photoconductive Antennas: Photoconductive antennas are devices that convert optical signals into terahertz radiation by utilizing the photoconductive effect, where the absorption of light generates free charge carriers in a semiconductor material. This mechanism allows them to generate terahertz pulses, making them essential for various terahertz imaging applications and systems.
Photomixers: Photomixers are devices that generate terahertz radiation by mixing two optical signals from different sources, producing a beat frequency that falls within the terahertz range. This process allows for the efficient production of terahertz waves, which are crucial for various imaging and sensing applications in science and technology.
Pulsed Terahertz Sources: Pulsed terahertz sources are devices that generate terahertz radiation in short bursts, allowing for the exploration of materials and biological samples with high temporal resolution. These sources are vital for terahertz imaging and spectroscopy applications, providing insights into the dynamics of various processes by capturing information at picosecond time scales. Their capability to deliver high peak power in short durations makes them ideal for probing the properties of materials and biological tissues non-destructively.
Quantum Cascade Lasers: Quantum cascade lasers (QCLs) are semiconductor lasers that produce coherent light in the terahertz and infrared range by exploiting quantum mechanical effects in low-dimensional structures. They are essential in various applications, particularly in the realm of terahertz imaging and spectroscopy, due to their ability to emit specific wavelengths tailored for distinct tasks.
R. A. McKinnon: R. A. McKinnon is a prominent figure in the field of terahertz science and technology, known for his contributions to terahertz sources and imaging systems. His work has significantly advanced the understanding and development of various terahertz generation techniques, which are crucial for applications in imaging, spectroscopy, and material characterization.
Security screening: Security screening refers to the process of inspecting individuals, their belongings, or environments to detect any potential threats or prohibited items. This practice is crucial in various settings, including airports and public venues, and relies heavily on advanced imaging technologies to ensure safety while minimizing inconvenience.
Spectral Purity: Spectral purity refers to the degree to which a signal contains only a single frequency or a narrow range of frequencies, minimizing the presence of unwanted harmonics or noise. This concept is critical when discussing the performance and quality of terahertz sources, as high spectral purity ensures clearer and more precise imaging results in various applications such as material characterization and biological sensing.
Terahertz semiconductor sources: Terahertz semiconductor sources are devices that generate electromagnetic radiation in the terahertz frequency range, typically between 0.1 to 10 THz. These sources utilize semiconductor materials to produce terahertz waves, which have unique properties that make them suitable for various applications, including imaging, spectroscopy, and communications. Their ability to create coherent and tunable terahertz radiation is crucial for advancing technologies in areas such as medical diagnostics and security screening.
Terahertz sources: Terahertz sources are devices or systems that generate electromagnetic waves in the terahertz frequency range, which spans from 0.1 to 10 THz. These sources are crucial for various applications, including imaging, spectroscopy, and sensing, as they provide the necessary radiation to probe materials and biological samples effectively.
Time-domain spectroscopy: Time-domain spectroscopy is a technique used to analyze the properties of materials by measuring their response to terahertz pulses over time. It allows for the capture of transient phenomena and provides detailed information about the electronic, vibrational, and rotational dynamics of substances, making it essential for various imaging and spectroscopic applications.
Uni-traveling carrier photodiodes: Uni-traveling carrier photodiodes (UTC-PDs) are specialized semiconductor devices that generate photocurrent by allowing only one type of carrier, usually electrons, to travel through the device while the other carrier, holes, is restricted. This design helps improve speed and efficiency, making UTC-PDs particularly suitable for applications in terahertz imaging systems where high-speed response is crucial. They are often used in conjunction with terahertz sources to detect and measure terahertz radiation effectively.
Vacuum Electronic Devices: Vacuum electronic devices are components that use vacuum as the medium for electron flow and are essential in generating, amplifying, or controlling microwave and terahertz signals. These devices exploit the behavior of electrons in a vacuum to achieve high-frequency operations, making them vital sources for terahertz applications in communication and imaging systems. Their ability to handle high power levels and operate at various frequencies enables advancements in both scientific research and practical applications.
Wavelength range: Wavelength range refers to the span of wavelengths that a particular source can emit or detect, which is crucial in applications like terahertz imaging. This range determines the capabilities and limitations of terahertz sources, impacting how they interact with different materials and their effectiveness in various imaging applications. Understanding the wavelength range is essential for selecting appropriate terahertz sources for specific tasks.