The document discusses the use of Rietveld refinement for analyzing powder X-ray diffraction data. Rietveld refinement allows for the determination of phase purity, identification of crystal structures, refinement of structural parameters, quantitative phase analysis, and calculation of properties like lattice parameters, atomic positions, thermal vibrations, grain size, and magnetic moments. The document provides examples of Rietveld refinement output and parameters that can be refined.
EMRS 2018 Replacing rare earth ions in LEDs (?)Philippe Smet
Two decades after the development of the blue light-emitting diode (LED), LEDs have quickly established themselves as the lighting technology of the future. The high efficiency, spectral tunability, lack of toxic compounds and a small footprint makes them far more attractive than other lighting technologies. The high efficiency, now well exceeding 100 lum/W in commercial products, has still the margin to double, promising a strong reduction in electricity consumption.
White LEDs are commonly based on a blue LED, combined with luminescent materials, or phosphors, which convert part of the blue light to longer wavelengths, the mixture providing white light. Besides the workhorse Y3Al5O12:Ce (YAG:Ce, yielding yellow emission), europium doped phosphors are used to provide e.g. the red emission required for warm-white LEDs.
Six main requirements for LED phosphors are discussed and used to explain the discrepancy between the high number of compositions described in literature and the handful of actually used compounds, being almost uniquely based on rare earth ions as luminescent center [1]. Alternative materials avoiding the use of rare earth ions are discussed, including Mn4+ doped fluorides phosphors (e.g. K2SiF6:Mn4+ [2]) and quantum dots. Finally, the impact of phosphor geometries on phosphor use, including remote phosphor applications, are discussed.
[1] Smet PF and Joos JJ, Nat. Mater. 16 (2017) 500.
[2] Sijbom H et al, Opt. Mater. Exp. 7 (2017) 3332.
Optical band gap measurement by diffuse reflectance spectroscopy (drs)Sajjad Ullah
Introduction to Optical band gap measurement
by electronic spectroscopy and diffuse reflectance spectroscopy (DRS) with comparison of the results obtained suing different equation and measurement techniques.
The role of scattering in extinction of light as it passes through media is briefly discussed.
EMRS 2018 Replacing rare earth ions in LEDs (?)Philippe Smet
Two decades after the development of the blue light-emitting diode (LED), LEDs have quickly established themselves as the lighting technology of the future. The high efficiency, spectral tunability, lack of toxic compounds and a small footprint makes them far more attractive than other lighting technologies. The high efficiency, now well exceeding 100 lum/W in commercial products, has still the margin to double, promising a strong reduction in electricity consumption.
White LEDs are commonly based on a blue LED, combined with luminescent materials, or phosphors, which convert part of the blue light to longer wavelengths, the mixture providing white light. Besides the workhorse Y3Al5O12:Ce (YAG:Ce, yielding yellow emission), europium doped phosphors are used to provide e.g. the red emission required for warm-white LEDs.
Six main requirements for LED phosphors are discussed and used to explain the discrepancy between the high number of compositions described in literature and the handful of actually used compounds, being almost uniquely based on rare earth ions as luminescent center [1]. Alternative materials avoiding the use of rare earth ions are discussed, including Mn4+ doped fluorides phosphors (e.g. K2SiF6:Mn4+ [2]) and quantum dots. Finally, the impact of phosphor geometries on phosphor use, including remote phosphor applications, are discussed.
[1] Smet PF and Joos JJ, Nat. Mater. 16 (2017) 500.
[2] Sijbom H et al, Opt. Mater. Exp. 7 (2017) 3332.
Optical band gap measurement by diffuse reflectance spectroscopy (drs)Sajjad Ullah
Introduction to Optical band gap measurement
by electronic spectroscopy and diffuse reflectance spectroscopy (DRS) with comparison of the results obtained suing different equation and measurement techniques.
The role of scattering in extinction of light as it passes through media is briefly discussed.
In concrete module, the basic properties of concrete are investigated. The design project is to design and make a bowling ball made of concrete and its various component. It should have the ability to roll for a maximum distance of three meters and should weigh less than 5.5 Kg. The project is done by group Engineers form Al-Wakra Secondary School for boys.
Customer Centred Business Decisions in the EnterpriseJake Causby
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In concrete module, the basic properties of concrete are investigated. The design project is to design and make a boat made of concrete and its various component. It should have the ability to float and carry maximum load.
The project is done by group Scientists from Nasser Al-Attiya Secondary School for Boys
OPTIMIZED RATE ALLOCATION OF HYPERSPECTRAL IMAGES IN COMPRESSED DOMAIN USING ...Pioneer Natural Resources
This paper studies the application of bit allocation using JPEG2000 for compressing multi-dimensional remote sensing data. Past experiments have shown that the Karhunen- Lo
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ve transform (KLT) along with rate distortion optimal(RDO) bit allocation produces good compression perfor-mance. However, this model has the unavoidable disadvan-tage of paying a price in terms of implementation complex-ity. In this research we address this complexity problem byusing the discrete wavelet transform (DWT) instead of theKLT as the decorrelator. Further, we have incorporated amixed model (MM) to find the rate distortion curves instead of the prior method of using experimental rate distortioncurves for RDO bit allocation. We compared our results tothe traditional high bit rate quantizer bit allocation modelbased on the logarithm of variances among the bands. Our comparisons show that by using the MM-RDO bit rate al-location method result in lower mean squared error (MSE)compared to the traditional bit allocation scheme. Our ap- proach also has an additional advantage of using DWT asa computationally efficient decorrelator when compared tothe KLT
Designed and manufactured an edge-coupled bandpass filter, with a required bandwidth of 900MHz at a center frequency of 3.8GHz experiencing 0.5dB pass-band ripple within Keysight ADS.
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A REVIEW OF LOW POWERAND AREA EFFICIENT FSM BASED LFSR FOR LOGIC BISTjedt_journal
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The French Revolution, which began in 1789, was a period of radical social and political upheaval in France. It marked the decline of absolute monarchies, the rise of secular and democratic republics, and the eventual rise of Napoleon Bonaparte. This revolutionary period is crucial in understanding the transition from feudalism to modernity in Europe.
For more information, visit-www.vavaclasses.com
The Indian economy is classified into different sectors to simplify the analysis and understanding of economic activities. For Class 10, it's essential to grasp the sectors of the Indian economy, understand their characteristics, and recognize their importance. This guide will provide detailed notes on the Sectors of the Indian Economy Class 10, using specific long-tail keywords to enhance comprehension.
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We all have good and bad thoughts from time to time and situation to situation. We are bombarded daily with spiraling thoughts(both negative and positive) creating all-consuming feel , making us difficult to manage with associated suffering. Good thoughts are like our Mob Signal (Positive thought) amidst noise(negative thought) in the atmosphere. Negative thoughts like noise outweigh positive thoughts. These thoughts often create unwanted confusion, trouble, stress and frustration in our mind as well as chaos in our physical world. Negative thoughts are also known as “distorted thinking”.
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This presentation provides a briefing on how to upload submissions and documents in Google Classroom. It was prepared as part of an orientation for new Sainik School in-service teacher trainees. As a training officer, my goal is to ensure that you are comfortable and proficient with this essential tool for managing assignments and fostering student engagement.
Model Attribute Check Company Auto PropertyCeline George
In Odoo, the multi-company feature allows you to manage multiple companies within a single Odoo database instance. Each company can have its own configurations while still sharing common resources such as products, customers, and suppliers.
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Bills have a main role in point of sale procedure. It will help to track sales, handling payments and giving receipts to customers. Bill splitting also has an important role in POS. For example, If some friends come together for dinner and if they want to divide the bill then it is possible by POS bill splitting. This slide will show how to split bills in odoo 17 POS.
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This slides describes the basic concepts of ICT, basics of Email, Emerging Technology and Digital Initiatives in Education. This presentations aligns with the UGC Paper I syllabus.
2024.06.01 Introducing a competency framework for languag learning materials ...Sandy Millin
http://sandymillin.wordpress.com/iateflwebinar2024
Published classroom materials form the basis of syllabuses, drive teacher professional development, and have a potentially huge influence on learners, teachers and education systems. All teachers also create their own materials, whether a few sentences on a blackboard, a highly-structured fully-realised online course, or anything in between. Despite this, the knowledge and skills needed to create effective language learning materials are rarely part of teacher training, and are mostly learnt by trial and error.
Knowledge and skills frameworks, generally called competency frameworks, for ELT teachers, trainers and managers have existed for a few years now. However, until I created one for my MA dissertation, there wasn’t one drawing together what we need to know and do to be able to effectively produce language learning materials.
This webinar will introduce you to my framework, highlighting the key competencies I identified from my research. It will also show how anybody involved in language teaching (any language, not just English!), teacher training, managing schools or developing language learning materials can benefit from using the framework.
Read| The latest issue of The Challenger is here! We are thrilled to announce that our school paper has qualified for the NATIONAL SCHOOLS PRESS CONFERENCE (NSPC) 2024. Thank you for your unwavering support and trust. Dive into the stories that made us stand out!
The Roman Empire A Historical Colossus.pdfkaushalkr1407
The Roman Empire, a vast and enduring power, stands as one of history's most remarkable civilizations, leaving an indelible imprint on the world. It emerged from the Roman Republic, transitioning into an imperial powerhouse under the leadership of Augustus Caesar in 27 BCE. This transformation marked the beginning of an era defined by unprecedented territorial expansion, architectural marvels, and profound cultural influence.
The empire's roots lie in the city of Rome, founded, according to legend, by Romulus in 753 BCE. Over centuries, Rome evolved from a small settlement to a formidable republic, characterized by a complex political system with elected officials and checks on power. However, internal strife, class conflicts, and military ambitions paved the way for the end of the Republic. Julius Caesar’s dictatorship and subsequent assassination in 44 BCE created a power vacuum, leading to a civil war. Octavian, later Augustus, emerged victorious, heralding the Roman Empire’s birth.
Under Augustus, the empire experienced the Pax Romana, a 200-year period of relative peace and stability. Augustus reformed the military, established efficient administrative systems, and initiated grand construction projects. The empire's borders expanded, encompassing territories from Britain to Egypt and from Spain to the Euphrates. Roman legions, renowned for their discipline and engineering prowess, secured and maintained these vast territories, building roads, fortifications, and cities that facilitated control and integration.
The Roman Empire’s society was hierarchical, with a rigid class system. At the top were the patricians, wealthy elites who held significant political power. Below them were the plebeians, free citizens with limited political influence, and the vast numbers of slaves who formed the backbone of the economy. The family unit was central, governed by the paterfamilias, the male head who held absolute authority.
Culturally, the Romans were eclectic, absorbing and adapting elements from the civilizations they encountered, particularly the Greeks. Roman art, literature, and philosophy reflected this synthesis, creating a rich cultural tapestry. Latin, the Roman language, became the lingua franca of the Western world, influencing numerous modern languages.
Roman architecture and engineering achievements were monumental. They perfected the arch, vault, and dome, constructing enduring structures like the Colosseum, Pantheon, and aqueducts. These engineering marvels not only showcased Roman ingenuity but also served practical purposes, from public entertainment to water supply.
1. PXRD AND RIETVELD REFINEMENT
By Saurav Chandra Sarma and Dundappa Mumbaraddi
Solid State and Inorganic Chemistry Lab, NCU,
JNCASR
2. What Rietveld can do..???
• Analysis of the whole diffraction pattern.
• Phase purity and identification.
• Refinement of the structure parameters from diffraction data.
• Quantitative phase analysis.
• Lattice parameters.
• Atomic positions and Occupancies.
• Isotropic and anisotropic thermal vibrations.
• Grain size and micro-strain calculation.
• Magnetic moments (Neutron diffraction).
7. What Rietveld can do..???
• Analysis of the whole diffraction pattern.
• Phase purity and identification.
• Refinement of the structure parameters from diffraction data.
• Quantitative phase analysis.
• Lattice parameters.
• Atomic positions and Occupancies.
• Isotropic and anisotropic thermal vibrations.
• Grain size and micro-strain calculation.
• Magnetic moments (Neutron diffraction).
8. QUANTITATIVE PHASE ANALYSIS
With high quality data, you can determine how much of
each phase is present
The ratio of peak intensities varies linearly as a function
of weight fractions for any two phases in a mixture.
10. CRYSTALLITE SIZE
Crystallites smaller than ~120nm create broadening of
diffraction peaks. (scherrer’s equation)
Where,
D-Size of ordered domains
K-dimentionless Shape factor
Lamda-X-ray wavelength
β-Line broading at FWHM
Theta-Brage angle
11. MICROSTRAIN
Ref:A. Khorsand Zak et al. / Solid State Sciences 13 (2011) 251-256
Microstrain may also create peak broadening (analyzing the peak
widths over a long range of 2theta using a Williamson-Hull plot can let
you separate microstrain and crystallite size)
12. PREFERRED ORIENTATION (TEXTURE)
Preferred orientation of crystallites can create a systematic
variation in diffraction peak intensities.
DOI: 10.1038/srep03679
37. Nph:Number of phases
Nba: Background type
0 Refine with polynomial
1 Read from CODFIL.bac
N >1Linear interpolation
-1 Refine with Debye+polynomial
-2 Treated iteratively with Fourier filtering
-3 Read addition 6 additional polynomial coeffs.
Nex:Number of regions to exclude
Nsc:Number of user defined scattering factors
Nor:Preferred orientation function type
0 Function No. 1
1 Function No. 2
38. Dum:Control of divergence
1 If some phases are treated in Profile Matching,
convergence criterion with stand. dev. not applied
2 Program stopped for local divergence: chi2(i-
cycle+1)>chi2(i-cycle)
3 Reflections near excluded regions excluded from
Bragg R-factor
Iwg:Refinement weighting scheme
0 Standard least squares
1 Maximum likelihood
2 Unit weights
Ilo: Lorentz and polarization corrections
0 Standard Debye-Scherrer or Bragg Brentano
1 Flat plate PSD geometry
-1 Lorentz-polarization correction not performed
2 Transmission geometry
3 Special polarization correction
39. Ias: Reflections reordering
0 Reordering performed only at first cycle
1 Reordering at each cycle
Res: Resolution function
0 Not given
1—4 For CW data, profile is Voigt function and different
functions available
Ste: Number of data points reduction factor
1,2..N If Ste>1, number of data points and therefore step
size reduced by factor Ste
Nre: Number of constrained parameters
Cry: Single crystal job
0 Only integrated intensity given, no profile parameters
1 Refinement with single crystal data or int. intensities
2 Montecarlo search for starting configuration, no least
squares
3 Simulated annealing optimization method
40. Uni:Scattering variable unit
0 2θ in degrees
1 TOF in sec
2 Energy in keV
Cor:Intensity correction
0 No correction is applied
1 File with intensity corrections
2 File with empirical function
Opt:Calculation optimization
0 General procedures used
1 Optimizes calculations to proceed faster
Aut: Automatic mode for refinement codes
numbering
0 Codewords treated as usual.
1 Codewords treated automatically by program
41. REFINEMENT OUTPUT CONTROLS (LINE 7)
Ipr: Profile integrated intensities
0 No action
1 Observed and calculated profiles in .out file
2 Calculated profiles for each phase in n.sub
files
3 Like 2 but background added to each profile
Ppl: Types of calc output-I
0 No action
1 Line printer plot in .out file
2 Generates background file
3 Difference pattern included in .bac file
42. Ioc: Types of calc output-II
0 No action
1 List of observed and calculated integrated
intensities in .out file
2 Reflection from 2nd wavelength if different
Mat:Correlation matrix
0 No action
1 Correlation matrix written in .out file
2 Diagonal of LS matrix printed before inversion
at every cycle
43. Pcr: Update of .pcr
0 after refinement
1 .pcr re-written with updated parameters
2 New input file generated called .new
Ls1:Types of calc output-III
0 No action
1 Reflection list before starting cycles written in
.out file
Ls2:Types of calc output-IV
0 No action
1 Corrected data list written in .out file
4 Plot of diffraction pattern displayed on the
screen at each cycle
44. LS3:Types of calc output-V
0 No action
1 Merged reflection list written in .out file
Prf: Output format of Rietveld plot file
0
1 For WinPLOTR
2 For IGOR
3 For KaleidaGraph and WinPLOTR
4 For Picsure, Xvgr
45. Ins: Data file format
0 Free format, 7 comments ok
= 1 D1A/D2B, original Rietveld
= 2 D1B old format
= 3 ILL instruments D1B, D20
= 4 Brookhaven, pairs of lines with 10 items
= -4 DBWS program
= 5 GENERAL FORMAT for TWO AXIS
= 6 D1A/D2B format prepared by SUM, ADDET or
MPDSUM
= 7 From D4 or D20L
= 8 DMC at Paul-Scherrer Inst.
= 10X, Y, sigma format
= 11 Variable time XRD
= 12 GSAS
47. Fou:Output of CODEFIL.fou
= 0 No action
= 1 Cambridge format
= 2 SHELXS format
= 3 FOURIER format
= 4 GFOURIER
Sho:Reduced output during refinement
= 0
= 1 Suppress out from each cycle, only last printed
48. EXPERIMENTAL SET UP CONTROLS (LINE 8)
Lamda1:wavelength 1
Lamda2:wavelength 2
Ratio:I2/I1
If <0, parameters U,V,W for l2 read separately
Bkpos: Origin of polynomial for background
Wdt:Cut off for peak profile tails in FWHM units
~4 for Gaussian
~20-30 for Lorentzian
~4—5 for TOF
Cthm:Monochromator polarization correction
49. muR: Absorption correction
m = effective absorption coeff.
R= radius or thickness of sample
AsyLim: Limit angle for asymmetry correction
Rpolarz:Polarization factor
Iabscor:Absorption correction for TOF data
= 1 Flat plate perp. to inc. beam
= 2 Cylindrical
50. REFINEMENT CONTROLS (LINE 9)
NCY:Number of refinement cycles
Eps:Control of convergence precisionForced termination
when shifts < EPS x e.s.d
R_at Relaxation factor of shifts of atomic parameters:
coordinates, moments, occupancies, Uiso’s
R_anRelaxation factor for shifts of anisotropic displacement
parameters
R_pr: Relaxation factor of profile parameters,
asymmetry, overall displacement, cell constants, strains, size,
propagation vectors, user-supplied parameters
R_gl:Relaxation factor of Global parameters, zero-shift,
background, displacement and transparency
Thmin:Starting scattering variable value (2θ/TOF/Energy)
Step:Step in scattering variable
Thmax: Last value of scattering variable
PSD: Incident beam angle
Sent0: Maximum angle at which primary beam
completely enlightens sample
51. NUMBER OF REFINED PARAMETERS
Maxs: Number of refined parameters (one
integer, one line)
52. REFINEMENT CONTROLS II (LINE 14, REFINABLE)
Zero: Zero point for T
Sycos: Systematic shift with cosθ dependence
Sysin:Systematic 2 shift with sin2θ dependence
Lambda:Wavelength to be refined
More: Flag to read micro-absorption
coefficients
≠ 0 Line 15 is read to define microabsorption
53. JASON-HODGES FORMULATION FOR TOF DATA (LINE
16)
Zerot: Zero shift for thermal neutrons
Dtt1t: Coeff. #1 for d-spacing calc
Dtt2t: Coeff. #2 for d-spacing calculation
x-cross:Position of the center of the crossover
region
Width:Width of crossover region
54. REFINEMENT PARAMETERS FOR EACH PHASE (LINE
19)
Nat: Number of atoms in asymmetric unit
Dis: Number of distance constraints
Mom:Number of angle constraints or number of magnetic
moment constraints
Jbt: Structure factor model and refinement method
= 0 Rietveld Method
= 1 Rietveld Method but purely magnetic phases
= -1 Like 1 but with extra parameters in spherical coordinates
= 2 Profile matching mode with constant scale factor
= -2 Like 2 but modulus instead of intensity given in .hkl file
= 3 Profile matching with constant relative intensities
= -3 Like 3 but modulus instead of intensity given in .hkl file
= 4 Intensities of nuclear reflections are calculated from Rigid
body groups
= 5 Intensities of magnetic reflections calculated from conical
magnetic structures in real space
= 10 Phase can contain nuclear and magnetic contributions
= 15 Phase is treated as commensurate modulated crystal
structure
55. Pr1, Pr2, Pr3:
Preferred orientation in reciprocal space for all
three directions
Irf: Method of reflection generation
= 0 List of reflections for the phase generated by
space group
= 1 h, k, l, mult read from .hkl file
= 2 h, k, l, mult, intensity read from .hkl file
= 3 h,k,l, mult, F_real, F_imag read from .hkl file
= 4 list of integrated intensities given as
observations
56. Isy: Symmetry operators reading control code
= 0 Operators automatically generated from Space
Group
= 1 Symmetry operators read below (use for
magnetism)
= 2 Basis functions of irreducible representations of
propagation vector group instead of symmetry operators
Str: Size-strain reading control
= 0 Strain/size parameters correspond to selected
models
= 1 Generalized formulation of strain used
= 2 Generalized formulation of size used
= -1 Options 1 and 2 simultaneously, size read before
strain
= 3 Generalized formulation of size and strain
parameters
Furth:Number of user defined parameters (only when
Jbt=4)
57. ATZ:Quantitative phase analysis coefficient
ATZ = ZMwf2/t
Z: Formula units per cell
Mw: Molecular weight
f: Site multiplicity
t: Brindley coefficient for microabsorption
Nvk: Number of propagation vectors
Npr Specific profile function for the phase
More: If not 0, then line 19-1 read
58. ATOMIC PARAMETERS (LINE 25)
Atom:Atom name
Typ:Atom type
X, Y, Z:Coordinates
Biso:Isotropic B factor
Occ:Occupancy
In/Fin:Ordinal number of first and last symmetry
operator applied to the atom (when users supply own list
of reflections)
N_t: Atom type
= 0 Isotropic atom
= 2 Anisotropic atom
= 4 Form-factor of atom is calculated
Spc:Number of chemical species
(For bond valence calcs.)
betaij:6 numbers (i,j =1,2) for anisotropic factors (line
25b)