The document discusses heterostructures, heterojunction bipolar transistors (HBTs), and thyristors. It begins by explaining homojunctions and heterojuctions, how they differ in material composition and resulting energy band structures. It then describes HBTs, noting they can achieve higher speeds than bipolar junction transistors (BJTs) due to reduced injection of minority carriers into the emitter. Finally, it discusses thyristors, four-layer pnpn semiconductor devices that can operate in either conducting or blocking states, and diacs, bidirectional thyristor variants used in alternating current switching applications.
Basic of semiconductors and optical propertiesKamran Ansari
This presentation explains the band structure, intrinsic semiconductor, extrinsic semiconductor, electrical conductivity, mobility, hall effect, p-n junction diode, tunnel diode and optical properties of the semiconductor.
Basic of semiconductors and optical propertiesKamran Ansari
This presentation explains the band structure, intrinsic semiconductor, extrinsic semiconductor, electrical conductivity, mobility, hall effect, p-n junction diode, tunnel diode and optical properties of the semiconductor.
Hello, I am Subhajit Pramanick. I and my classmate, Anannya Sahaw, both presented this ppt in seminar of our Institute, Indian Institute of Technology, Kharagpur. The topic of this presentation is on exchange interaction and their consequences. It includes the basic of exchange interaction, the origin of it, classification of it and their discussions etc. We hope you will all enjoy by reading this presentation. Thank you.
Super conductors,properties and its application and BCS theorysmithag7
superconductors:-Introduction, definition, type1,type2 and atypical. Preparation of high temperature super conductor-Y1 Ba2Cu3Ox±δ, BCS theory and general application of high temperature super conductors.
Superconductivity is the ability of certain materials to conduct electric current with practically zero resistance. This capacity produces interesting and potentially useful effects. For a material to behave as a superconductor, low temperatures are required.
This presentation is the introduction to Density Functional Theory, an essential computational approach used by Physicist and Quantum Chemist to study Solid State matter.
Hello, I am Subhajit Pramanick. I and my classmate, Anannya Sahaw, both presented this ppt in seminar of our Institute, Indian Institute of Technology, Kharagpur. The topic of this presentation is on exchange interaction and their consequences. It includes the basic of exchange interaction, the origin of it, classification of it and their discussions etc. We hope you will all enjoy by reading this presentation. Thank you.
Super conductors,properties and its application and BCS theorysmithag7
superconductors:-Introduction, definition, type1,type2 and atypical. Preparation of high temperature super conductor-Y1 Ba2Cu3Ox±δ, BCS theory and general application of high temperature super conductors.
Superconductivity is the ability of certain materials to conduct electric current with practically zero resistance. This capacity produces interesting and potentially useful effects. For a material to behave as a superconductor, low temperatures are required.
This presentation is the introduction to Density Functional Theory, an essential computational approach used by Physicist and Quantum Chemist to study Solid State matter.
Introduction
How a transistor works - the basics
Summary of transistor junction bias scenarios
Bipolar Transistor Configurations
Bipolar Transistor Summary
NPN Transistor
PNP Transistor
Output Characteristics Curves of a BJT
Application of BJT - as a Switch
Cut-off Regio
Saturation Region
Here you find the information about Transistors. And know about
-> Type Of Transistor:
->Region of Transistor:
->P-N Junction Diodes
->Transistor application
->Transistor Connections
Limitation:
->Future of transistor:
This presentation aims at introducing the concepts of soliton propagation. The solitons are a result of nonlinear optical interaction of light pulses within optical fibers.
Earliest Galaxies in the JADES Origins Field: Luminosity Function and Cosmic ...Sérgio Sacani
We characterize the earliest galaxy population in the JADES Origins Field (JOF), the deepest
imaging field observed with JWST. We make use of the ancillary Hubble optical images (5 filters
spanning 0.4−0.9µm) and novel JWST images with 14 filters spanning 0.8−5µm, including 7 mediumband filters, and reaching total exposure times of up to 46 hours per filter. We combine all our data
at > 2.3µm to construct an ultradeep image, reaching as deep as ≈ 31.4 AB mag in the stack and
30.3-31.0 AB mag (5σ, r = 0.1” circular aperture) in individual filters. We measure photometric
redshifts and use robust selection criteria to identify a sample of eight galaxy candidates at redshifts
z = 11.5 − 15. These objects show compact half-light radii of R1/2 ∼ 50 − 200pc, stellar masses of
M⋆ ∼ 107−108M⊙, and star-formation rates of SFR ∼ 0.1−1 M⊙ yr−1
. Our search finds no candidates
at 15 < z < 20, placing upper limits at these redshifts. We develop a forward modeling approach to
infer the properties of the evolving luminosity function without binning in redshift or luminosity that
marginalizes over the photometric redshift uncertainty of our candidate galaxies and incorporates the
impact of non-detections. We find a z = 12 luminosity function in good agreement with prior results,
and that the luminosity function normalization and UV luminosity density decline by a factor of ∼ 2.5
from z = 12 to z = 14. We discuss the possible implications of our results in the context of theoretical
models for evolution of the dark matter halo mass function.
Introduction:
RNA interference (RNAi) or Post-Transcriptional Gene Silencing (PTGS) is an important biological process for modulating eukaryotic gene expression.
It is highly conserved process of posttranscriptional gene silencing by which double stranded RNA (dsRNA) causes sequence-specific degradation of mRNA sequences.
dsRNA-induced gene silencing (RNAi) is reported in a wide range of eukaryotes ranging from worms, insects, mammals and plants.
This process mediates resistance to both endogenous parasitic and exogenous pathogenic nucleic acids, and regulates the expression of protein-coding genes.
What are small ncRNAs?
micro RNA (miRNA)
short interfering RNA (siRNA)
Properties of small non-coding RNA:
Involved in silencing mRNA transcripts.
Called “small” because they are usually only about 21-24 nucleotides long.
Synthesized by first cutting up longer precursor sequences (like the 61nt one that Lee discovered).
Silence an mRNA by base pairing with some sequence on the mRNA.
Discovery of siRNA?
The first small RNA:
In 1993 Rosalind Lee (Victor Ambros lab) was studying a non- coding gene in C. elegans, lin-4, that was involved in silencing of another gene, lin-14, at the appropriate time in the
development of the worm C. elegans.
Two small transcripts of lin-4 (22nt and 61nt) were found to be complementary to a sequence in the 3' UTR of lin-14.
Because lin-4 encoded no protein, she deduced that it must be these transcripts that are causing the silencing by RNA-RNA interactions.
Types of RNAi ( non coding RNA)
MiRNA
Length (23-25 nt)
Trans acting
Binds with target MRNA in mismatch
Translation inhibition
Si RNA
Length 21 nt.
Cis acting
Bind with target Mrna in perfect complementary sequence
Piwi-RNA
Length ; 25 to 36 nt.
Expressed in Germ Cells
Regulates trnasposomes activity
MECHANISM OF RNAI:
First the double-stranded RNA teams up with a protein complex named Dicer, which cuts the long RNA into short pieces.
Then another protein complex called RISC (RNA-induced silencing complex) discards one of the two RNA strands.
The RISC-docked, single-stranded RNA then pairs with the homologous mRNA and destroys it.
THE RISC COMPLEX:
RISC is large(>500kD) RNA multi- protein Binding complex which triggers MRNA degradation in response to MRNA
Unwinding of double stranded Si RNA by ATP independent Helicase
Active component of RISC is Ago proteins( ENDONUCLEASE) which cleave target MRNA.
DICER: endonuclease (RNase Family III)
Argonaute: Central Component of the RNA-Induced Silencing Complex (RISC)
One strand of the dsRNA produced by Dicer is retained in the RISC complex in association with Argonaute
ARGONAUTE PROTEIN :
1.PAZ(PIWI/Argonaute/ Zwille)- Recognition of target MRNA
2.PIWI (p-element induced wimpy Testis)- breaks Phosphodiester bond of mRNA.)RNAse H activity.
MiRNA:
The Double-stranded RNAs are naturally produced in eukaryotic cells during development, and they have a key role in regulating gene expression .
This presentation explores a brief idea about the structural and functional attributes of nucleotides, the structure and function of genetic materials along with the impact of UV rays and pH upon them.
Observation of Io’s Resurfacing via Plume Deposition Using Ground-based Adapt...Sérgio Sacani
Since volcanic activity was first discovered on Io from Voyager images in 1979, changes
on Io’s surface have been monitored from both spacecraft and ground-based telescopes.
Here, we present the highest spatial resolution images of Io ever obtained from a groundbased telescope. These images, acquired by the SHARK-VIS instrument on the Large
Binocular Telescope, show evidence of a major resurfacing event on Io’s trailing hemisphere. When compared to the most recent spacecraft images, the SHARK-VIS images
show that a plume deposit from a powerful eruption at Pillan Patera has covered part
of the long-lived Pele plume deposit. Although this type of resurfacing event may be common on Io, few have been detected due to the rarity of spacecraft visits and the previously low spatial resolution available from Earth-based telescopes. The SHARK-VIS instrument ushers in a new era of high resolution imaging of Io’s surface using adaptive
optics at visible wavelengths.
Seminar of U.V. Spectroscopy by SAMIR PANDASAMIR PANDA
Spectroscopy is a branch of science dealing the study of interaction of electromagnetic radiation with matter.
Ultraviolet-visible spectroscopy refers to absorption spectroscopy or reflect spectroscopy in the UV-VIS spectral region.
Ultraviolet-visible spectroscopy is an analytical method that can measure the amount of light received by the analyte.
THE IMPORTANCE OF MARTIAN ATMOSPHERE SAMPLE RETURN.Sérgio Sacani
The return of a sample of near-surface atmosphere from Mars would facilitate answers to several first-order science questions surrounding the formation and evolution of the planet. One of the important aspects of terrestrial planet formation in general is the role that primary atmospheres played in influencing the chemistry and structure of the planets and their antecedents. Studies of the martian atmosphere can be used to investigate the role of a primary atmosphere in its history. Atmosphere samples would also inform our understanding of the near-surface chemistry of the planet, and ultimately the prospects for life. High-precision isotopic analyses of constituent gases are needed to address these questions, requiring that the analyses are made on returned samples rather than in situ.
A brief information about the SCOP protein database used in bioinformatics.
The Structural Classification of Proteins (SCOP) database is a comprehensive and authoritative resource for the structural and evolutionary relationships of proteins. It provides a detailed and curated classification of protein structures, grouping them into families, superfamilies, and folds based on their structural and sequence similarities.
3. Heterostructures
Heterojunction Bipolar Transistor
Thyristors
Introduction
Homojunction
Heterojunction
Like and Unlike
Homojunction
Semiconductor material is homogeneous through out the structure.
Heterojunction
Two different SC materials form junction
Different Energy Band Gaps
Energy Band Discontinuity at the junction interface
Narrow Band gap to wide band gap – Abrupt Junction
Lattice Constant matching must be done
Shuvan Prashant Heterostructures, HBTs and Thyristors
4. Heterostructures
Heterojunction Bipolar Transistor
Thyristors
Introduction
Homojunction
Heterojunction
Energy Band Diagram Construction
Assumption
There are negligible number of traps or generation-recombination
centers at the interface of two dissimilar SCs
Validity: SCs have matched Lattice Constants
Requirements
The Fermi Level must be same on both sides of the interface
The vacuum Level must be continuous and parallel to the band
edges
Discontinuity in band edges is unaffected because of doping
Materials Used III-V Compound Semiconductors
GaAs Eg = 1.42eV Lattice Constant = 5.6533 Ao
Alx Ga1−x As where x can vary from 0 to 1
Eg = 2.17eV Lattice Constant = 5.6605 Ao
Shuvan Prashant Heterostructures, HBTs and Thyristors
6. Heterostructures
Heterojunction Bipolar Transistor
Thyristors
Introduction
Homojunction
Heterojunction
Energy band Edge Picture
Band Edge energies
The band edge energies
relative to the Vacuum Ref
are the property of SC
Electron Affinity,χ, CB end
to Vacuum Ref
Energy Gap Eg , Valence
Band Edge to Conduction
Band Edge
Fermi Level
Depends on doping level
Work Function,Φ: Fermi Level to Vacuum ref
Shuvan Prashant Heterostructures, HBTs and Thyristors
12. Heterostructures
Heterojunction Bipolar Transistor
Thyristors
Introduction
Homojunction
Heterojunction
2D electron gas
Electrons from wide gap
AlGaAs flow into GaAs
Form an accumulation layer
of electrons in Potential well
2d Electron Gas – electrons
have quantized energy levels
in one spatial direction
but are free in other two So
What?
Electron Mobility increases
in the low impurity doping
region (abrupt
heterojunction)
Shuvan Prashant Heterostructures, HBTs and Thyristors
13. Heterostructures
Heterojunction Bipolar Transistor
Thyristors
Introduction
Homojunction
Heterojunction
2D electron gas
Electrons from wide gap
AlGaAs flow into GaAs
Form an accumulation layer
of electrons in Potential well
2d Electron Gas – electrons
have quantized energy levels
in one spatial direction
but are free in other two So
What?
Electron Mobility increases
in the low impurity doping
region (abrupt
heterojunction)
Shuvan Prashant Heterostructures, HBTs and Thyristors
14. Heterostructures
Heterojunction Bipolar Transistor
Thyristors
Introduction
Homojunction
Heterojunction
2D electron gas
Electrons from wide gap
AlGaAs flow into GaAs
Form an accumulation layer
of electrons in Potential well
2d Electron Gas – electrons
have quantized energy levels
in one spatial direction
but are free in other two So
What?
Electron Mobility increases
in the low impurity doping
region (abrupt
heterojunction)
Shuvan Prashant Heterostructures, HBTs and Thyristors
15. Heterostructures
Heterojunction Bipolar Transistor
Thyristors
Introduction
Homojunction
Heterojunction
2D electron gas
Electrons from wide gap
AlGaAs flow into GaAs
Form an accumulation layer
of electrons in Potential well
2d Electron Gas – electrons
have quantized energy levels
in one spatial direction
but are free in other two So
What?
Electron Mobility increases
in the low impurity doping
region (abrupt
heterojunction)
Shuvan Prashant Heterostructures, HBTs and Thyristors
16. Heterostructures
Heterojunction Bipolar Transistor
Thyristors
Structure
Application
Limitations of BJT
1 Limit on Current Gain-
Emitter Injection Efficiency
γ
2 γ - accounts for minority
carrier hole diffusion current
in the emitter
3 Doesn’t contribute to
transistor action
4 Increase in emitter doping -
bandgap narrowing offsets
the improvement
5 Solution: Use wideband
gap material to minimise
carrier injection from base
to emitter
n*GaAs
n*GaAs
nGaAlAs
Emitter
nGaAs
nGaAlAs
pGaAs
Collector
Base
nGaAlAs Emitter and p GaAs Base Junc
Energy Band Diagram
Shuvan Prashant Heterostructures, HBTs and Thyristors
18. Heterostructures
Heterojunction Bipolar Transistor
Thyristors
Structure
Application
What made the difference?
The holes and electrons see a different barrier
The holes are not allowed to go back into emitter
Drastic reduction in Hole Injection – high emitter doping
needn’t be done
Reduction in band narrowing effect too..
So What’s the use ?
High Frequency Device
Lower emitter Doping⇒ Smaller junction Capacitance⇒
Higher Speed
Electron Mobility for npn GaAs is 5 times that of Si⇒ Shorter
Base transit Time
Cutoff Frequencies of the order of 40 GHz
Shuvan Prashant Heterostructures, HBTs and Thyristors
19. Heterostructures
Heterojunction Bipolar Transistor
Thyristors
pnpn Junction
Diac
Thyristors
Three pn junctions in series - pnpn diode
With a gate terminal – Semiconductor Controlled Rectifier or
Thyristor
Switching from an OFF or blocking state to an ON or conducting
state
Wider range of current and voltage handling capabilities than
transistors
Shuvan Prashant Heterostructures, HBTs and Thyristors
20. Heterostructures
Heterojunction Bipolar Transistor
Thyristors
pnpn Junction
Diac
Basic Characteristics
Figure: Thyristor in forward region
Regions
1 Forward Blocking - OFF
State with high impedance
Forward Breakover
(switching) dV/dI = 0 V=
VBF I= Is
2 Negative Resistance Region
3 Forward Conducting - ON
State with low impedance
dV/dI = 0 V= Vh I= Ih
4 Reverse Blocking State
5 Reverse Breakdown region
Shuvan Prashant Heterostructures, HBTs and Thyristors
21. Heterostructures
Heterojunction Bipolar Transistor
Thyristors
pnpn Junction
Diac
Basic Characteristics
Figure: Thyristor in forward region
Regions
1 Forward Blocking - OFF
State with high impedance
Forward Breakover
(switching) dV/dI = 0 V=
VBF I= Is
2 Negative Resistance Region
3 Forward Conducting - ON
State with low impedance
dV/dI = 0 V= Vh I= Ih
4 Reverse Blocking State
5 Reverse Breakdown region
Shuvan Prashant Heterostructures, HBTs and Thyristors
22. Heterostructures
Heterojunction Bipolar Transistor
Thyristors
pnpn Junction
Diac
Basic Characteristics
Figure: Thyristor in forward region
Regions
1 Forward Blocking - OFF
State with high impedance
Forward Breakover
(switching) dV/dI = 0 V=
VBF I= Is
2 Negative Resistance Region
3 Forward Conducting - ON
State with low impedance
dV/dI = 0 V= Vh I= Ih
4 Reverse Blocking State
5 Reverse Breakdown region
Shuvan Prashant Heterostructures, HBTs and Thyristors
23. Heterostructures
Heterojunction Bipolar Transistor
Thyristors
pnpn Junction
Diac
Understanding pnpn as coupled transistors
Bistable device
pnpn diode in forward region is Bistable device
high impedance low current OFF
low impedance high current ON
Shuvan Prashant Heterostructures, HBTs and Thyristors
24. Heterostructures
Heterojunction Bipolar Transistor
Thyristors
pnpn Junction
Diac
Bidirectional Thyristor Diac
Diac Diode for Alternating current
Diac diode as an ac switch
ON OFF States for positive and negative anode voltages
Shuvan Prashant Heterostructures, HBTs and Thyristors
25. Heterostructures
Heterojunction Bipolar Transistor
Thyristors
pnpn Junction
Diac
Bibliography
Thank You
References
Semiconductor Devices S M Sze I edition
Semiconductor Devices D A Neamann Third Edition
MIT Lectures OCW 6.772 Compound Semiconductor Devices
As taught in: Spring 2003 by Clifton Fonstad Jr.
Pictures for thyristors from www.wikipedia.com
Shuvan Prashant Heterostructures, HBTs and Thyristors