NIGA Flashcards

1
Q

Principles of laser printer

A

Laser printers operate on the electrophotography principle. The process involves charging a photosensitive drum, exposing it to a laser beam that creates an electrostatic latent image, developing the image with toner, transferring it to paper, and fusing it using heat. This process allows precise and fast image reproduction

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2
Q

Requirements for the lasers used in laser printers

A

Lasers in laser printers must:
-Emit wavelengths that are in the sensitivity range of the photoconductor.
-Be stable, reliable, compact, not expensive, short time increasing temperature and possibility to modulate the intensity with high speed

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3
Q

Advantages and disadvantages of barcodes

A

Advantages: fast, accurate, cost-effective data encoding, reduces errors and enables automation
Disadvantages: requires barcode scanners, lacks read/write capabilities, relies on line-of-sight scanning, and is sensitive to physical damage

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4
Q

How speed could be increased in laser printers

A

Printing speed increases with higher laser power, multi-beam systems, or higher rotation speeds of mirrors. However, these approaches might increase cost, noise or heating issues

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5
Q

Linear barcodes: advantages and disadvantages

A

Advantages: simple to generate, easy to decode, low-cost equipment, mature technology
Disadvantages: Limited data storage, sensitive to damage (scratches or distortion), and prone to errors if damaged

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6
Q

Main standards of barcodes

A

Standards include:
UPC-A 12 digits, common in retail.
UPC-E 6-digit compressed version for small packages
EAN-13 13-digit European standard, a superset of UPC-A
EAN-8 8-digit version for small packages
UPC-universal product code, EAN - European article numbering.

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7
Q

How is the information read from a barcode

A

Barcode scanners read reflected light from the black and white bars. The dark bars absorb light, while the white spaces reflect it. Photodetectors convert the reflected light into electrical signals, corresponding to the encoded data.

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8
Q

Principle of barcode reader

A

The scanner uses a laser beam deflected by a rotating polygon mirror. The reflected light scatters off the barcode and is collected by a photodetector. Intensity variations (due to black and white bars) are converted into electrical signals, corresponding to the encoded data

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9
Q

Optical communication systems compared to electrical communication

A

Advantages of optical systems over electrical systems:
-Extremely wide bandwidth (over 100GHz)
-Immunity to electromagnetic interference.
-smaller size and lighter weight.
-Lower cost and enhanced security.
-Longer lifespan and resistance to corrosion.

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10
Q

Main components of the optical fiber systems

A

Compact light source: LEDs for short distances; laser diodes for long distances
Low-loss optical fibers: enable efficient signal transmission.
Photo detectors: convert optical signals into electrical signals.

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11
Q

Types of light sources used in optical communication systems

A

LEDs - used for short distances and low data rates
Laser diodes - Preferred for long distances and high data rates due to high power, speed and narrow spectral width

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12
Q

Wavelengths of light used in optical fibers

A

Short wavelength: 0.85um
Long wavelength: 1.3um and 1.55um, with the latter offering the lowest attenuation (0.2 dB/km)

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13
Q

Numerical aperture of graded-index fiber

A

The numerical aperture (NA) is the sine of the largest angle of incident light that can undergo total internal reflection. It measures the light-gathering ability of the fiber.

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14
Q

“V-parameter” or fiber parameter

A

The V-parameter determines the number of modes in a fiber. For single-mode operation, V must be less than 2.405
V=2pi(a/lamda)*NA
a-radius of the fiber
lamda-input wavelength
number of modes ~V^2

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15
Q

What does dispersion cause in the optical fiber

A

Dispersion causes temporal spreading of light pulses, leading to signal overlap and reduced clarity at the receiver. This limits data transmission rates over long distances.

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16
Q

Types of dispersion in optical fibers

A

Modal dispersion: Occurs in multimode fibers due to varying path lengths of modes
Material dispersion: results from wavelength dependence of refractive index
Waveguide dispersion: arises from the fibers core and cladding geometry

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17
Q

Intermodal dispersion in optical fiber

A

Intermodal dispersion is significant in multimode fibers and occurs when different modes propagate at different velocities, causing pulse broadening.

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18
Q

Dispersion in single-mode fibers

A

Single-mode fibers are free from intermodal dispersion but experience material and waveguide dispersion. These types can still cause pulse broadening over long distances.

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19
Q

What is the cut-off wavelength in optical fibers, and how is it measured

A

The cut-off wavelength is the longest wavelength at which a fiber remains single-mode. It is measured by analyzing transmitted power as a function of wavelength.

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20
Q

Principles of polarization-maintaining optical fiber

A

Polarization-maintaining fibers (e.g., Panda fibers) maintain the polarization state of light by inducing stress in the core using asymmetrical cladding designs. They are used in high-precision applications like sensing and interferometry

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21
Q

What materials are used to increase the refractive index of the core in optical fibers

A

Materials like titanium dioxide TiO2, aluminum oxide Al2O3, and germanium dioxide GeO2 are used to increase the refractive index of the fiber core.

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22
Q

Benefits and drawbacks of plastic fiber

A

Benefits: cost-effective and flexible, can bend without cracking, immune to electromagnetic noise, lightweight and easy to install, can withstand stress.
Drawbacks: high attenuation and dispersion limit its use for long distances, Core and cladding refractive indexes vary at high temperature, affecting performance, low quality compared to glass fiber, it is flammable

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23
Q

Formation of plastic fiber

A

Plastic fibers are made using polystyrene as the core material and polymethil methacrylate PMMA for cladding. The fibers are drawn using a specialized tower.

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24
Q

Types of losses in junctions of optical fibers

A

Fresnel reflection - due to reflection in the intermedia of air and fused silica
Misalignment losses - axial, angular or radial misalignments can cause power loss. Bigger loss in single mode fibers due to much smaller diameter.
Radial shift - lateral displacement between fibers.
Defects

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25
What are the main requirements for an ideal optical detector
High sensitivity, low noise(high signal to noise ratio), wide spectral range, fast response time, rugged and cost-effective.
26
Types of optical detectors
Photon detectors: phototubes, photodiodes, photomultipliers and charge-coupled devices (CCDs) Thermal detectors: bolometers, thermocouples and pyroelectric detectors
27
What is the detectivity of an optical detector
D* represents the signal to noise ratio for a certain electrical frequency and bandwidth if 1 watt of radiation power reaches a detector surface of 1cm2. The higher D* value is, the better the detector is D*=sqrt(active detector area)/NEP NEP (noise equivalent power) is defined as the signal power that gives a signal to noise ratio of one in a one hertz output bandwidth
28
Main properties of photon transducers.
-Convert photon energy into electrical signals -Exhibit high sensitivity and fast response times -Operate in the UV-VIS range and are unsuitable for far-IR detection -single or multi channel (1-D or 2-D) - Highly variable spectral response
29
Photon transducers: principle of phototube
A phototube comprises a cathode and anode in a vacuum. Incident photons eject electrons from the cathode, creating a photocurrent proportional to the light intensity. The wavelength range depends on the cathode material.
30
Principle of silicon photodiode transducers
Silicon photodiodes are reverse-biased pn junctions. Incident light creates electron-hole pairs in the depletion region, producing a photocurrent proportional to the light intensity
31
Types of multichannel photon transducers
Photodiode arrays (PDAs) - linear arrays of diodes for simultaneous detection across a spectrum. Charge-coupled devices (CCDs) - high sensitivity and resolution for capturing entire spectra
32
Multichannel photon transducers: principles of photodiode arrays (PDA)
PDAs are linear arrays of reverse-biased silicon diodes. Each diode measures incident light at specific wavelengths. They are commonly used in spectroscopy.
33
Multichannel photon transducers: principles of Charge-transfer devices CTD
CTDs, such as CCDs and CIDs, store photon-induced charges in silicon elements. These charges are transferred sequentially to amplifiers for measurement. They offer high sensitivity and spatial resolution.
34
Main properties of thermal transducers
Thermal transducers absorb radiant energy, causing temperature changes that are measured. They have a flat spectral response, operate in the IR range, and are slower than photon detectors.
35
Thermal transducers: principle of thermocouple
A thermocouple uses 2 dissimilar metals joined at a junction. Radiation absorption causes a temperature difference, generating a voltage proportional to the radiant energy.
36
Thermal transducers: principle of bolometer
Bolometers measure changes in resistance caused by absorbed radiation. They are highly sensitive and operate by detecting temperature in blackened materials.
37
Why are semiconductor bolometers more sensitive than metallic bolometers
Semiconductor bolometers have higher thermal coefficients of resistance, making them more sensitive to temperature changes compared to metals.
38
For what reason is the cooling of bolometers used
Cooling reduces thermal noise enhancing sensitivity and allowing the detection of weak signals
39
Thermal transducers: principle of pyroelectric transducers
Pyroelectric transducers use temperature-dependent polarization in crystals. Radiation absorption alters the polarization, generating a measurable current. Materials like LiTaO₃ and TGS are common.
40
Laser application in length measurement: interference method
The interference method uses coherent laser light. As a mirror moves, interference fringes form, allowing precise measurements of displacement by counting fringe shifts. Michelson interferometers are common for this application.
41
What distances could be measured by interference method
Distances up to the laser's coherence length (often 100m or more) can be measured with micrometer accuracy using stabilized lasers.
42
Distance measurement using laser interferometers: Michelson interferometer. Principle setup
The michelson interferometer splits laser beam into 2 paths. Reflected beams recombine to form interference fringes, with fringe shifts indicating distance changes.
43
Distance measurement using laser interferometers: polarization interferometer. Principle setup
The polarization interferometer uses polarized beams and measures phase shifts due to displacement
44
Distance measurement using laser interferometers: Dual-Frequency interferometer. Principle setup.
Dual-frequency interferometer uses 2 laser frequencies. Doppler shifts caused by motion are measured to determine displacement.
45
Testing the quality of optical imaging components: Tywan-Green Interferometer. Principle setup.
This interferometer, a modified Michelson, assesses optical surface quality by observing interference fringes caused by slight mirror tilts.
46
Measurement of length by laser: Time of flight method. principle
This method measures the time taken for a laser pulse to travel to a target and back. Accuracy depends on pulse duration and timing resolution.
47
Measurement of length by laser: triangulation methods
Triangulation uses a laser beam to create a spot on the target. A camera captures the spot's position, and geometric calculations determine the distance. 300nm to 10m range. 0.05% accuracy.
48
Measurement of length by laser: Beam modulation telemetry method. Principle
Continuous-wave lasers modulated with sine waves are used. The phase delay between transmitted and received signals determines the range.
49
Laser Doppler velocimeter. Principle
Measures velocity using Doppler shifts in reflected light. The frequency change corresponds to the object's speed.
50
Angle measurements by laser. Principle
A dual-frequency interferometer measures angular rotation by detecting differences in Doppler shifts between beams reflected from 2 retroreflectors
51
Straightness measurements by laser. Principle
A modified dual-frequency interferometer splits the laser beam using a Wollaston prism. Deviations in reflected beams measure the straightness of a surface.
52
Measurement of surface finish by laser. Principle setup
Laser beam comes at the surface at an angle, only scattered light reaches diode (Caused by surface irregularities). By analyzing intensity and distribution of scattered light, surface texture and roughness can be assessed
53
Main applications of lasers for agriculture
For poultry farming - to prevent male chicken killing (after 9 days of incubation laser burns a tiny hole in the eggs shell, from it drop of allantois fluid is taken) this allows detection of chicken gender. Using NIR-Raman spectroscopy after 3 days of incubation the formed blood vessel systems reflects light and gender is determined from its hemoglobin spectrum. Weed control - lasers are being developed to distinguish weeds from crops using imaging techniques and to weaken weed's growth centers with precise, high-energy pulses, reducing the need for chemical herbicides( could be used in high-quality vegetable growth) Laser leveling - for even soil surface (less water needed, improves crop establishment, faster work, reduced weed problem, uniformity of crop maturity)
54
Main components of laser leveling system
Drag scrapper/bucket - mounted or pulled by a tractor. Laser transmitter - mounted on tripod, emits infrared beam that travels up to 500m in a straight line. Laser receiver - senses infrared beam and converts it to electrical signal, multi-directional receiver directs the position of the laser reference plane, transmits signal to the control box. Control box - accepts, processes signals from the receiver, indicates drag buckets position relative to the finished grade. Hydraulic system - supplies oil to raise and lower leveling bucket, several times a second it raises and lowers blades of a grader to follow the infrared beam.
55
Benefits of laser land leveling over conventional land leveling
Reduction of time and water for irrigation, uniform water distribution, smoother soil surface, uniform moisture environment for crops, less weeds in the fields, uniformity in crop maturity, reduced seed rate, fertilizers, chemicals and fuel requirements, better germination and growth of a crop
56
What are benefits of 3D laser scanning
Laser surveying helps avoid assumptions, generalizations, errors in interpretation, problems by having the original data set to refer back to
57
The principles of laser scanning
Scanner emits a laser beam that is reflected from the object. To measure a point's position, the scanner records inclined distance and 2 angles: horizontal (a) and vertical (b). Measurements are converted from polar coordinates to a cartesian coordinate system to determine the point's precise location. The collected data forms a "point cloud" representing the object's surface. Accuracy depends on distance to the object, the angle of incidence, reflective properties of the surface.
58
Basics of laser medicine: at which spectral region the absorption of chromophores in biological soft tissue are the highest
Highest absorption of chromophores occurs in the UV and VIS spectral regions, particularly below 1000nm. This is where key chromophores such as hemoglobin, melanin, and other biomolecules exhibit strong absorption. Water strongly absorbs light in the IR spectral regions, particularly beyond 1000nm.
59
Basics of laser medicine: what type of scattering is observed during light propagation in soft tissue
Rayleigh scattering, d << lambda (mitochondria), and Mie scattering, d >= lambda (macromolecules, membrane structures). Scattering of tissue is always a combination of Rayleigh and Mie scattering, depending on what structures are dominant.
60
Models of laser-tissue interactions: the electromechanical (photomechanical or photodisruptive) mode. Principle
Relies on extremely short laser pulses(ns or shorter), high photon spatial density and coherent light. It generates micro-plasma through optical breakdown (intense electric fields tear molecules apart). Micro-plasma expansion creates supersonic shockwaves, leading to mechanical rupture of the tissue
61
Models of laser-tissue interactions: Ablation. Principle
It's evaporation followed by expulsion of evaporated material. Depending on the laser type (e.g. UV lasers), the process can be clean and localized, with minimal heat diffusion, while the interaction volume is determined by the spot size and optical penetration depth. If energy is smaller than needed for evaporation it results in thermal effects.
62
Models of laser-tissue interactions: photothermal (coagulative and vaporizing) processes
Rely on selective heating of highly absorbing regions, such as microvessels. Achieved when laser pulse duration is shorter than the thermal diffusion time accross the region ((τ < L²/4D), ensuring thermal energy is confined before diffusing, leading to coagulative or vaporizing effects. L-diffusion length, D-diffusion constant.
63
What are the applications of new photothermal sensitizers (nanoparticles) heated with short laser pulses
Selective cancer-cell targeting by conjugation of absorbing particles; localized tumor destruction; absorption of radiation at longer wavelengths.
64
Models of laser-tissue interactions: photochemical (photodynamic) heated with short laser pulses.
Activates photosensitizer by light to produce reactive oxygen species (ROS), primarily singlet oxygen (1O₂) it induces cytotoxic effects in tissues with high photosensitizer concentrations, makes it effective for tumor-targeted therapies.
65
Principles of photodynamic therapy (PDT)
Uses photodynamic reaction, steps: photosensitizer administration, photosensitizer distribution in body, tumor irradiation, tumor ablation & cure.
66
Models of laser-tissue interactions: Bistimulation and wound healing.
Involves low-fluence light, also called low-level laser therapy (LLLT), aimed at promoting cellular repair and recovery, though its efficacy is unclear and not scientifically proven
67
Laser-tissue interactions: During thermal reactions, according to the degree of heating, what type of thermal damage can be achieved.
42-45C start of hyperthermia, collagen shrinkage. 50C Enzyme activity decreases 60C Protein denaturation, collagen coagulation, membrane permeabilization. 100C Tissue drying, vacuole formation. >100C Vaporization, tissue carbonization 300-1000C thermoablation, photoablation, tissue disruption.
68
Laser-tissue interaction: on what parameters depends the temperature increase in the tissue due to laser irradiation. Please provide an equation.
delta T - temperature increase Q(J/cm^3) - absorbed thermal energy per unit volume ro (g/cm^3) - density c [J/g*K] - specific heat delta T = Q/(ro*c)[K]
69
Main fields of applications of lasers in dermatology
Hair removal, vascular and pigmented lesion treatment (various skin diseases and abnormalities), tatoo removal, skin resurfacing, acne treatment, and scar revision.
70
How is phenomenon of photoacoustics used in photorejuvenation
Pigment is broken down by shock waves generated in the tissue by very short light pulses from Q switched lasers operating with pulse durations of 2-50ns. Longer pulse duration can be used by targeting entire pigmented lesions.
71
Laser vision correction: principles of photorefractive Karatectomy
Uses excimer laser to decrease nearsightness, removes precise amount of tissue from cornea to reduce its curvature using "cold" UV laser. It brings the focal point closer to retina.
72
Lasers in Opthalmology: principle of LASIK ("LAser in SItu Keratomileusis")
Procedure utilizes excimer laser and the microkeratome to alter the degree of near-sightedness in an eye. Creates a flap from cornea, folds it back, then laser removes precise amount of tissue from cornea, folds the flap back.
73
Lasers in Opthalmology: principles of radial keratectomy.
Reduces nearsightness, radial incisions are made in cornea, with a diamond blade. Incisions flatten the central portion of cornea, brings the focal point closer to the retina, improves distance vision.
74
Lasers in Opthalmology: Hyperopic correction
Excimer laser is used to reshape cornea to correct farsightedness. Farsighted (hyperopic) cornea is flatter than is required given the length of your eye. Surgery improves vision by reshaping the front surface of the eye and making it more curved.
75
Principles of femtosecond laser assisted cataract surgery
Uses a laser to make very precise cuts in the eye: creating an opening in the lens capsule and breaking up the cataract. The laser is guided by detailed images of the eye, improving the safety and accuracy of the procedure.
76
Application of ocular photodynamic therapy method.
Treatment of neovascular (wet) age-related macular degeneration, choroidal neovascularization. IT targets abnormal blood vessels or tumors with light-activated drugs, reducing fluid and improving retinal health.
77
Main application fields of lasers in dentistry
Surgical management of oral hard/soft tissue, non-surgical application, antibacterial applications. Restorative dentistry, laser assisted diagnosis, surgical applications, oral diagnosis/oral medicine, oral surgery, periodontics, pediatric, endodontics, biostimulation.
78
Types of lasers used in dentistry
Neodymium YAG; Erbium (Er:YAG and Er,Cr:YSGG) and diode group of semiconductor based technology.
79
What are the most popular non-surgical, low level laser applications in dentistry
Photo-biomodulation, diagnostics, photo-activated anti-bacterial processes, laser tooth whitening and laser scanning of tooth cavity preparations.
80
What are the advantages of laser use with oral hard tissue in comparison to conventional rotary instrumentation
Precise ablation of hard tissue, selective ablation of diseased tissue, less risk of injury, less risk of thermal and mechanical cracking of tooth structure, reduction in bacterial contamination of tooth cavity, less discomfort for patient.
81
Main purposes of the use of surgical lasers in periodontology
Removal of diseased pocket lining epithelium, bactericidal effect of lasers on pocket organisms, removal of calculus deposits and root surface detoxification.
82
Main laser applications in otolaryngology
Treatments for nasal polyps, sinus surgery and turbinate hypertrophy. Also used for vascular malformations, tumor removal, glottis/subglottis procedures, and cosmetic treatments such as rhinophyma correction. Used lasers vary in wavelength and penetration depth to target specific tissues effectively (CO2 and Erbium:YAG)
83
Lasers in gastroenterology. Main applications.
Used for hemostasis, tumor debulking, palliation of inoperable cancers, treatments of dysphagia, interstitial photocoagulation of liver metastases, treatment of small gastrointestinal tumors.
84
Lasers in the cardiovascular system. Main applications.
Lasers in the cardiovascular system are used to treat blocked arteries, remove blood clots, improve blood flow in heart muscle, and treat irregular heartbeats by precisely targeting and removing or reshaping tissue, though further research is needed to address some challenges.
85
Lasers in neurosurgery. Main applications
Used to treat brain and spinal tumors, vascular issues, and deep-seated lesion with precision and minimal damage, often through techniques like stereotactic surgery and minimally invasive laser therapies
86
Principle of optical coherence tomography
Using low-coherence light to capture high resolution cross-sectional images of tissues. Light is split into 2 beams: one reflects from the sample and the other from a reference mirror. By analyzing the interference of the reflected beams, detailed depth-resolved images of the sample are generated.
87
Principle of diffuse optical tomography
Using near-infrared light to measure the scattering and absorption properties of tissues. By analyzing how light propagates through the tissue, DOT reconstructs 3D images of internal structures, used for examination of biological tissues at a macroscopic scale.
88
Main advantages of lasers in spectroscopy
Ability to achieve high spectral resolution and detection sensitivity by providing strong, stable radiation sources, enabling the detection of very small absorption levels and low concentrations of molecules.
89
Principle of absorption spectroscopy. Main advantages of using tunable lasers.
It is based on measuring the amount of light absorbed by a sample at specific wavelengths, which provides information about the sample's composition and concentration of molecules. Advantages: Extremely high spectral resolution, enhanced detection sensitivity, the ability to use long absorption paths for detecting weak absorptions, precise calibration of absorption lines and rapid wavelength tuning for studying short-lived molecular species.
90
What is laser induced fluorescence (LIF) ?
Laser excites molecules to a higher energy state, undergoes possible collisional change, and after some delay, they emit fluorescence as they return to a lower energy state. The emitted light is typically observed at a 90deg. angle to the excitation beam, it provides high sensitivity for detecting specific molecules on a dark background.
91
Principle of Optic emission spectroscopy (OES)
Sample is excited using external energy source (plasma), it causes them to emit light at characteristic wavelengths. By analyzing this emitted light, the elemental composition of the sample can be determined.
92
Laser induced breakdown spectroscopy (LIBS). Principles.
Laser pulses vaporize solid sample, causes breakdown in gas and create a plasma, plasma emits light at characteristic wavelengths, and can be used for elemental analysis.
93
Laser induced plasma emission versus temporal delay with respect to laser.
Early delays dominated by intense continuum emission, intermediate delays show atomic emissions and long delays showing reduced intensity due to plasma cooling. Optimal timing is crucial for capturing desired spectral features.
94
Typical optical setups used in LIBS practice.
Laser beam --> focussing objective --> collection lens --> entrance slit of the spectrometer Laser beam --> focusing objective --> collection lenses --> optical fiber to the spectrometer Laser beam --> focussing objective <-- Schwarzschild objective or Cassegrain telescope <-- Optical fiber to the spectrometer Laser beam --> Dichroic mirror -->/--> Focussing and collection objective -->/--> Collection lens --> optical fiber to the spectrometer
95
Basics of laser scattering spectroscopy.
It uses light scattering to study gases: Rayleigh scattering helps measure density and temperature, while Raman scattering identifies molecules and their energy levels. Rayleigh is stronger and cleaner, but Raman gives more detailed chemical information
96
Compare Rayleigh and Raman scattering
Rayleigh scattering is elastic, strong, and ideal for imaging density and temperature with minimal background, while Raman scattering is inelastic, weaker, and used for identifying multiple molecular species and temperature but often suffers from background interference.
97
Surface-enhanced Raman scattering (SERS). Principles.
It amplifies Raman signals by placing analyte molecules near metal nanoparticles, where localized surface plasmons create "hot spots" that enhance the electromagnetic field, significantly increasing sensitivity for molecular detection.
98
Time resolved fluorescence techniques: time correlated single photon counting. Principle scheme with explanation.
Laser > photodiode > discriminator > time-to-voltage converter /> multichannel analyzer /> discriminator > photomultiplier > sample It splits laser pulse, one part starting a timer and the other exciting the sample. The timer runs until it is stopped by a fluorescence photon emitted from the sample, detected by a photon counting device. Repeating this process many times creates a histogram of fluorescence decay, provides sample's fluorescence lifetime.
99
Time-resolved fluorescence techniques: Streak camera. Principle scheme with explanation.
Light --- Electrions --- light Entrance slit > Entrance optics > photocathode > acceleration grid > deflection electrodes > microchannel plate > phosphor screen > Exit optics > CCD camera Fluorescence photons are converted into electrons at a photocathode. Electrons are accelerated and deflected by a sweeping voltage, it converts their arrival time into position in space. Process is synchronized with the laser pulse, and the deflected electrons create an image on a phosphor screen, which is then captured by a CCD camera.
100
Time-resolved fluorescence techniques: fluorescence upconversion. Principle scheme with explanation
BS /> RR > BBO2 > CCD BS /> BBO1 > BPF > 400nm > sample > LPF > BBO2 > CCD Pulse is split into 2, gate is delayed by the optical delay line, other is used to excite sample. Emitted fluorescence is collected using parabolic reflectors and focused into BBO2 crystal together with delayed gate pulse. BBO2 generates sum frequency between gate and fluorescence, its spectrum is spread by monochromator and recorded by CCD detector
101
Time-resolved fluorescence techniques: optical Kerr shutter. Principle scheme with explanation
Gate pulse + fluorescence > polarizer > nonlinear medium > polarizer > spectrograph > CCD Fluorescence passes 2 crossed polarizers and nonlinear medium, the gate pulse hits medium, polarization of fluorescence light is rotated and the light overlapping with gate pulse is transmitted through second polarizer.
102
Principle of Pump-probe spectroscopy
Pump pulse excites the sample, while a probe pulse measures how the sample's transmittance changes over time. By varying the delay between the pump and probe pulses, the time-dependent absorption signal is recorded.